Skip to content

AP Precalculus β€” Practice

All practice problems and solutions for AP Precalculus, organized by unit. Worked examples stay on the unit pages.

Auto-collected from the practice sections of each unit’s notes (scripts/build_practice.py). Edit the source notes, not this page.

Full notes β†’

  1. The taxicab distance between points (x1,y1)(x_1, y_1) and (x2,y2)(x_2, y_2) in the coordinate plane is given by ∣x1βˆ’x2∣+∣y1βˆ’y2∣\lvert x_1 - x_2 \rvert + \lvert y_1 - y_2 \rvert. For how many points PP with integer coordinates is the taxicab distance between PP and the origin less than or equal to 2020? (2022 AMC 12A)
  2. Solve for xx: x4βˆ’13x2+36=0x^4 - 13x^2 + 36 = 0.
  3. Simplify x4256+x332+5x216+x+4+16xβˆ’84xβˆ’7βˆ’24+2(x216+x4+2)(βˆ’2+24xβˆ’7)\sqrt{\frac{x^4}{256} + \frac{x^3}{32} + \frac{5x^2}{16} + x + 4 + 16x - 8\sqrt{4x-7} - 24 + 2(\frac{x^2}{16} + \frac{x}{4} + 2)(-2 + 2\sqrt{4x-7})}. (Hint: Use factor by grouping.)
  4. Solve for xx and discard any extraneous solutions: 1xβˆ’1+2x2βˆ’1=3x+1\dfrac{1}{x-1} + \dfrac{2}{x^2-1} = \dfrac{3}{x+1}.
  5. Solve for xx in R\mathbb{R}: 9xβˆ’10β‹…3x+9=09^x - 10\cdot 3^x + 9 = 0.
  6. Solve for xx in R\mathbb{R} and check every candidate in the original equation: 2x+3+x+1=3\sqrt{2x+3} + \sqrt{x+1} = 3.
  7. Solve for xx in R\mathbb{R} and write the answer in interval notation: 3x+1xβˆ’2>2\dfrac{3x+1}{x-2} > 2.
  8. Solve for xx in R\mathbb{R} and write the answer in interval notation: ∣xβˆ’2∣+∣x+4βˆ£β‰€10\lvert x - 2\rvert + \lvert x + 4\rvert \le 10.
  9. Solve for xx in R\mathbb{R} and write the answer in interval notation: ∣x2βˆ’9βˆ£β‰€5\lvert x^{2} - 9\rvert \le 5.
  10. Solve in R\mathbb{R}: (xβˆ’1)2(xβˆ’4)(x+2)<0(x-1)^{2}(x-4)(x+2) < 0. Explain how repeated roots change the sign chart compared with all simple roots.
  11. Solve in R\mathbb{R}: x3βˆ’5x2+6xβ‰₯0x^{3} - 5x^{2} + 6x \ge 0.
  12. Solve in R\mathbb{R}: x2βˆ’4x2+x≀0\dfrac{x^{2} - 4}{x^{2} + x} \le 0. Give the domain, a single rational inequality of the form R(x)Q(x)≀0\dfrac{R(x)}{Q(x)} \le 0 with no common factors, and the solution in interval notation.
  13. Solve in R\mathbb{R}: 4βˆ’x2β‰₯x\sqrt{4 - x^{2}} \ge x. Find the radical domain first, then split into x<0x < 0 and xβ‰₯0x \ge 0 before squaring where legal.
  14. Solve in R\mathbb{R}: x2+5≀x+2\sqrt{x^{2} + 5} \le x + 2. Impose all conditions needed before and after squaring.
  15. Determine the symmetries of both graphs: f(x)=x2x2+1f(x)=\dfrac{x^2}{x^2+1} and g(x)=x∣x∣g(x)=x\lvert x\rvert. For each, decide whether the graph has yy-axis symmetry, xx-axis symmetry, origin symmetry, or none.
  16. (Bonus, Markov equations)

Our goal is to find all positive integer solutions (x,y)(x,y) to

x2+y2+1=3xy.x^2+y^2+1=3xy.

This is a small version of a famous family of Diophantine equations (equations with positive integer solutions) known as Markov equations.

(A)(A) Find the solutions with y=1y=1.

(B)(B) Treat the equation as a quadratic in xx. If xx is one root, use Vieta’s formulas to find the other root xβ€²x'.

(C)(C) Suppose (x,y)(x,y) is a positive integer solution with xβ‰₯yβ‰₯2x\ge y\ge 2. Prove that the other root xβ€²x' is a positive integer and that xβ€²<yx'<y.

(D)(D) Explain why repeatedly replacing the larger coordinate by the smaller Vieta root must eventually reach a solution with one coordinate equal to 11.

(E)(E) Reverse the process to describe all positive integer solutions.


We want integer points (x,y)(x,y) satisfying

∣x∣+∣yβˆ£β‰€20.\lvert x \rvert +\lvert y \rvert \le 20.

For distance 00, there is only the origin: 11 point.

For each distance rβ‰₯1r\ge 1, the equation

∣x∣+∣y∣=r\lvert x \rvert +\lvert y \rvert =r

has 4r4r integer points. Therefore the total number of points is

1+βˆ‘r=1204r=1+4(20β‹…212)=1+840=841.1+\sum_{r=1}^{20}4r =1+4\left(\frac{20\cdot 21}{2}\right) =1+840 =841.

Thus

841.\boxed{841}.

Let u=x2u=x^2. Then

x4βˆ’13x2+36=0x^4-13x^2+36=0

becomes

u2βˆ’13u+36=0.u^2-13u+36=0.

Factor:

(uβˆ’9)(uβˆ’4)=0.(u-9)(u-4)=0.

So u=9u=9 or u=4u=4. Since u=x2u=x^2,

x2=9orx2=4.x^2=9 \quad\text{or}\quad x^2=4.

Therefore

x=βˆ’3,βˆ’2,2,3.\boxed{x=-3,-2,2,3}.

Let

A=x216+x4+2andB=βˆ’2+24xβˆ’7.A=\frac{x^{2}}{16}+\frac{x}{4}+2 \qquad\text{and}\qquad B=-2+2\sqrt{4x-7}.

The first five terms under the square root are exactly A2A^2:

(x216+x4+2)2=x4256+x332+5x216+x+4.\left(\frac{x^{2}}{16}+\frac{x}{4}+2\right)^2 =\frac{x^4}{256}+\frac{x^3}{32}+\frac{5x^2}{16}+x+4.

The next three terms are exactly B2B^2:

(βˆ’2+24xβˆ’7)2=16xβˆ’84xβˆ’7βˆ’24.\left(-2+2\sqrt{4x-7}\right)^2 =16x-8\sqrt{4x-7}-24.

The remaining term is 2AB2AB, so the expression under the radical is

A2+B2+2AB=(A+B)2.A^2+B^2+2AB=(A+B)^2.

Thus the original expression is

(A+B)2=∣A+B∣.\sqrt{(A+B)^2}=\lvert A+B\rvert.

Now

A+B=x216+x4+24xβˆ’7.A+B=\frac{x^2}{16}+\frac{x}{4}+2\sqrt{4x-7}.

The domain requires 4xβˆ’7β‰₯04x-7\ge 0, so xβ‰₯74x\ge \frac74. On this domain, A+Bβ‰₯0A+B\ge 0, so

x216+x4+24xβˆ’7.\boxed{\frac{x^2}{16}+\frac{x}{4}+2\sqrt{4x-7}}.

The denominators show that

xβ‰ 1,xβ‰ βˆ’1.x\ne 1,\qquad x\ne -1.

Start with

1xβˆ’1+2x2βˆ’1=3x+1.\frac{1}{x-1}+\frac{2}{x^2-1}=\frac{3}{x+1}.

Factor x2βˆ’1=(xβˆ’1)(x+1)x^2-1=(x-1)(x+1) and multiply both sides by (xβˆ’1)(x+1)(x-1)(x+1):

x+1+2=3(xβˆ’1).x+1+2=3(x-1).

Solve:

x+3=3xβˆ’3⟹6=2x⟹x=3.x+3=3x-3 \quad\Longrightarrow\quad 6=2x \quad\Longrightarrow\quad x=3.

Since 33 is allowed in the original equation,

x=3.\boxed{x=3}.

Let

u=3x.u=3^x.

Then 9x=(3x)2=u29^x=(3^x)^2=u^2, so

9xβˆ’10β‹…3x+9=09^x-10\cdot 3^x+9=0

becomes

u2βˆ’10u+9=0.u^2-10u+9=0.

Factor:

(uβˆ’1)(uβˆ’9)=0.(u-1)(u-9)=0.

Thus u=1u=1 or u=9u=9. Returning to u=3xu=3^x:

3x=1⟹x=0,3^x=1 \quad\Longrightarrow\quad x=0,

or

3x=9⟹x=2.3^x=9 \quad\Longrightarrow\quad x=2.

Therefore

x=0,2.\boxed{x=0,2}.

The domain requires

2x+3β‰₯0andx+1β‰₯0,2x+3\ge 0 \qquad\text{and}\qquad x+1\ge 0,

so xβ‰₯βˆ’1x\ge -1. Start with

2x+3+x+1=3.\sqrt{2x+3}+\sqrt{x+1}=3.

Isolate one radical:

2x+3=3βˆ’x+1.\sqrt{2x+3}=3-\sqrt{x+1}.

Square both sides:

2x+3=9βˆ’6x+1+x+1.2x+3=9-6\sqrt{x+1}+x+1.

Simplify:

xβˆ’7=βˆ’6x+1.x-7=-6\sqrt{x+1}.

Then

7βˆ’x=6x+1.7-x=6\sqrt{x+1}.

Square again:

(7βˆ’x)2=36(x+1).(7-x)^2=36(x+1).

Expand and solve:

x2βˆ’14x+49=36x+36x^2-14x+49=36x+36 x2βˆ’50x+13=0.x^2-50x+13=0.

By the quadratic formula,

x=50Β±2500βˆ’522=25Β±617.x=\frac{50\pm\sqrt{2500-52}}{2} =25\pm 6\sqrt{17}.

Check candidates in the original equation. The value 25+61725+6\sqrt{17} is extraneous because it makes 7βˆ’x<07-x<0 in the equation 7βˆ’x=6x+17-x=6\sqrt{x+1}. The value 25βˆ’61725-6\sqrt{17} works. Therefore

x=25βˆ’617.\boxed{x=25-6\sqrt{17}}.

Move everything to one side:

3x+1xβˆ’2>2⟹3x+1xβˆ’2βˆ’2>0.\frac{3x+1}{x-2}>2 \quad\Longrightarrow\quad \frac{3x+1}{x-2}-2>0.

Combine into one rational expression:

3x+1βˆ’2(xβˆ’2)xβˆ’2>0.\frac{3x+1-2(x-2)}{x-2}>0.

Simplify:

x+5xβˆ’2>0.\frac{x+5}{x-2}>0.

The critical values are x=βˆ’5x=-5 and x=2x=2. A sign chart gives positive values on (βˆ’βˆž,βˆ’5)(-\infty,-5) and (2,∞)(2,\infty). Since the inequality is strict, x=βˆ’5x=-5 is not included, and x=2x=2 is never allowed.

Thus

(βˆ’βˆž,βˆ’5)βˆͺ(2,∞).\boxed{(-\infty,-5)\cup(2,\infty)}.

The expression

∣xβˆ’2∣+∣x+4∣\lvert x-2\rvert+\lvert x+4\rvert

is the sum of the distances from xx to 22 and from xx to βˆ’4-4. Break at x=βˆ’4x=-4 and x=2x=2.

If x<βˆ’4x<-4, then

∣xβˆ’2∣+∣x+4∣=βˆ’(xβˆ’2)βˆ’(x+4)=βˆ’2xβˆ’2.\lvert x-2\rvert+\lvert x+4\rvert=-(x-2)-(x+4)=-2x-2.

So

βˆ’2xβˆ’2≀10⟹xβ‰₯βˆ’6.-2x-2\le 10 \quad\Longrightarrow\quad x\ge -6.

This gives [βˆ’6,βˆ’4)[-6,-4).

If βˆ’4≀x≀2-4\le x\le 2, then

∣xβˆ’2∣+∣x+4∣=(2βˆ’x)+(x+4)=6,\lvert x-2\rvert+\lvert x+4\rvert=(2-x)+(x+4)=6,

which is always at most 1010. This gives [βˆ’4,2][-4,2].

If x>2x>2, then

∣xβˆ’2∣+∣x+4∣=(xβˆ’2)+(x+4)=2x+2.\lvert x-2\rvert+\lvert x+4\rvert=(x-2)+(x+4)=2x+2.

So

2x+2≀10⟹x≀4.2x+2\le 10 \quad\Longrightarrow\quad x\le 4.

This gives (2,4](2,4]. Combining all pieces,

[βˆ’6,4].\boxed{[-6,4]}.

Start with

∣x2βˆ’9βˆ£β‰€5.\lvert x^2-9\rvert\le 5.

Rewrite this as a compound inequality:

βˆ’5≀x2βˆ’9≀5.-5\le x^2-9\le 5.

Add 99 to all parts:

4≀x2≀14.4\le x^2\le 14.

Thus x2x^2 must be at least 44 and at most 1414. Therefore

[βˆ’14,βˆ’2]βˆͺ[2,14].\boxed{[-\sqrt{14},-2]\cup[2,\sqrt{14}]}.

The inequality is already factored:

(xβˆ’1)2(xβˆ’4)(x+2)<0.(x-1)^2(x-4)(x+2)<0.

The critical values are

x=βˆ’2,x=1,x=4.x=-2,\quad x=1,\quad x=4.

The root x=1x=1 has even multiplicity because of (xβˆ’1)2(x-1)^2, so the sign does not change when crossing x=1x=1. Simple roots, like x=βˆ’2x=-2 and x=4x=4, do change the sign.

A sign chart gives:

  • positive on (βˆ’βˆž,βˆ’2)(-\infty,-2),
  • negative on (βˆ’2,1)(-2,1),
  • negative on (1,4)(1,4),
  • positive on (4,∞)(4,\infty).

Because the inequality is strict, none of the zeros are included. Thus

(βˆ’2,1)βˆͺ(1,4).\boxed{(-2,1)\cup(1,4)}.

Factor:

x3βˆ’5x2+6x=x(x2βˆ’5x+6)=x(xβˆ’2)(xβˆ’3).x^3-5x^2+6x=x(x^2-5x+6)=x(x-2)(x-3).

Solve

x(xβˆ’2)(xβˆ’3)β‰₯0.x(x-2)(x-3)\ge 0.

The critical values are 00, 22, and 33. A sign chart gives:

  • negative on (βˆ’βˆž,0)(-\infty,0),
  • positive on (0,2)(0,2),
  • negative on (2,3)(2,3),
  • positive on (3,∞)(3,\infty).

Since the inequality is β‰₯0\ge 0, include the zeros. Therefore

[0,2]βˆͺ[3,∞).\boxed{[0,2]\cup[3,\infty)}.

The domain comes from the denominator:

x2+x=x(x+1)β‰ 0.x^2+x=x(x+1)\ne 0.

So

xβ‰ 0,xβ‰ βˆ’1.x\ne 0,\qquad x\ne -1.

Factor the rational expression:

x2βˆ’4x2+x=(xβˆ’2)(x+2)x(x+1).\frac{x^2-4}{x^2+x} =\frac{(x-2)(x+2)}{x(x+1)}.

There are no common factors, so the rational inequality is

(xβˆ’2)(x+2)x(x+1)≀0.\frac{(x-2)(x+2)}{x(x+1)}\le 0.

The critical values are βˆ’2,βˆ’1,0,2-2,-1,0,2. Remember that βˆ’1-1 and 00 cannot be included because they make the denominator zero. A sign chart gives nonpositive values on

[βˆ’2,βˆ’1)and(0,2].[-2,-1) \quad\text{and}\quad (0,2].

Thus

domain:Β xβ‰ βˆ’1,0;(xβˆ’2)(x+2)x(x+1)≀0;[βˆ’2,βˆ’1)βˆͺ(0,2].\boxed{\text{domain: }x\ne -1,0;\quad \frac{(x-2)(x+2)}{x(x+1)}\le 0;\quad [-2,-1)\cup(0,2]}.

First find the domain:

4βˆ’x2β‰₯0βŸΉβˆ’2≀x≀2.4-x^2\ge 0 \quad\Longrightarrow\quad -2\le x\le 2.

Now solve

4βˆ’x2β‰₯x.\sqrt{4-x^2}\ge x.

If x<0x<0, the right side is negative and the left side is nonnegative, so the inequality is automatically true on the domain. This gives [βˆ’2,0)[-2,0).

If xβ‰₯0x\ge 0, both sides are nonnegative, so we can square:

4βˆ’x2β‰₯x2.4-x^2\ge x^2.

Then

4β‰₯2x2⟹x2≀2.4\ge 2x^2 \quad\Longrightarrow\quad x^2\le 2.

With xβ‰₯0x\ge 0, this gives 0≀x≀20\le x\le \sqrt2. Combining both cases,

[βˆ’2,2].\boxed{[-2,\sqrt2]}.

The radical is always defined because

x2+5>0x^2+5>0

for all real xx. But since

x2+5β‰₯0,\sqrt{x^2+5}\ge 0,

we also need the right side to be nonnegative:

x+2β‰₯0⟹xβ‰₯βˆ’2.x+2\ge 0 \quad\Longrightarrow\quad x\ge -2.

Now square both sides:

x2+5≀(x+2)2.x^2+5\le (x+2)^2.

Expand:

x2+5≀x2+4x+4.x^2+5\le x^2+4x+4.

Cancel x2x^2:

5≀4x+4⟹xβ‰₯14.5\le 4x+4 \quad\Longrightarrow\quad x\ge \frac14.

This already satisfies xβ‰₯βˆ’2x\ge -2, so

[14,∞).\boxed{\left[\frac14,\infty\right)}.

For

f(x)=x2x2+1,f(x)=\frac{x^2}{x^2+1},

test f(βˆ’x)f(-x):

f(βˆ’x)=(βˆ’x)2(βˆ’x)2+1=x2x2+1=f(x).f(-x)=\frac{(-x)^2}{(-x)^2+1} =\frac{x^2}{x^2+1} =f(x).

So ff has yy-axis symmetry. It does not have origin symmetry because f(βˆ’x)β‰ βˆ’f(x)f(-x)\ne -f(x) in general, and it does not have xx-axis symmetry because reflecting a nonzero function value across the xx-axis would not stay on the graph of the same function.

For

g(x)=x∣x∣,g(x)=x\lvert x\rvert,

test g(βˆ’x)g(-x):

g(βˆ’x)=(βˆ’x)βˆ£βˆ’x∣=βˆ’x∣x∣=βˆ’g(x).g(-x)=(-x)\lvert -x\rvert=-x\lvert x\rvert=-g(x).

So gg has origin symmetry. It does not have yy-axis symmetry because g(βˆ’x)β‰ g(x)g(-x)\ne g(x) in general, and it does not have xx-axis symmetry for the same reason ordinary nonzero functions usually do not.

Therefore

fΒ hasΒ y-axisΒ symmetryΒ only,Β andΒ gΒ hasΒ originΒ symmetryΒ only.\boxed{f\text{ has }y\text{-axis symmetry only, and }g\text{ has origin symmetry only}}.

We solve

x2+y2+1=3xyx^2+y^2+1=3xy

in positive integers.

For part (A), set y=1y=1. Then

x2+2=3x.x^2+2=3x.

So

x2βˆ’3x+2=0⟹(xβˆ’1)(xβˆ’2)=0.x^2-3x+2=0 \quad\Longrightarrow\quad (x-1)(x-2)=0.

Thus the solutions with y=1y=1 are

(1,1)Β andΒ (2,1).\boxed{(1,1)\text{ and }(2,1)}.

By symmetry, (1,2)(1,2) is also a solution.

For part (B), treat the equation as a quadratic in xx:

x2βˆ’3yx+(y2+1)=0.x^2-3yx+(y^2+1)=0.

If xx is one root, let xβ€²x' be the other root. By Vieta’s formulas,

x+xβ€²=3yx+x'=3y

and

xxβ€²=y2+1.xx'=y^2+1.

From the sum formula,

xβ€²=3yβˆ’x.x'=\boxed{3y-x}.

Because xx and yy are integers, xβ€²x' is also an integer. The pair (xβ€²,y)(x',y) satisfies the same equation because xβ€²x' is the other root of the same quadratic.

For part (C), suppose (x,y)(x,y) is a positive integer solution with

xβ‰₯yβ‰₯2.x\ge y\ge 2.

We first show xβ€²>0x'>0. Since

xβ€²=3yβˆ’x,x'=3y-x,

it is enough to show x<3yx<3y. If xβ‰₯3yx\ge 3y, then

x2βˆ’3xy+y2+1>0,x^2-3xy+y^2+1>0,

which contradicts the equation rewritten as

x2βˆ’3xy+y2+1=0.x^2-3xy+y^2+1=0.

Therefore x<3yx<3y, so xβ€²>0x'>0.

Now show xβ€²<yx'<y. Since xβ‰₯yβ‰₯2x\ge y\ge 2, the larger root is

x=3y+5y2βˆ’42.x=\frac{3y+\sqrt{5y^2-4}}{2}.

Because yβ‰₯2y\ge 2,

5y2βˆ’4>y2,5y^2-4>y^2,

so

5y2βˆ’4>y.\sqrt{5y^2-4}>y.

Thus

x>3y+y2=2y.x>\frac{3y+y}{2}=2y.

Therefore

xβ€²=3yβˆ’x<3yβˆ’2y=y.x'=3y-x<3y-2y=y.

So every solution with xβ‰₯yβ‰₯2x\ge y\ge 2 creates a smaller positive integer solution

(xβ€²,y)(x',y)

with 0<xβ€²<y≀x0<x'<y\le x.

For part (D), repeat this step. Each time, the larger coordinate decreases to a smaller positive integer. A strictly decreasing sequence of positive integers cannot continue forever, so the descent must eventually stop.

It can only stop when the smaller coordinate is 11. By part (A), the terminal solutions are (1,1)(1,1), (2,1)(2,1), and by symmetry (1,2)(1,2).

For part (E), reverse the descent. Starting with (1,1)(1,1), repeatedly replace the smaller coordinate by

newΒ coordinate=3(largerΒ coordinate)βˆ’(smallerΒ coordinate).\text{new coordinate}=3(\text{larger coordinate})-(\text{smaller coordinate}).

This gives

(1,1),Β (1,2),Β (2,5),Β (5,13),Β (13,34),…(1,1),\ (1,2),\ (2,5),\ (5,13),\ (13,34),\ldots

and the swapped pairs.

Equivalently, define a sequence by

a0=1,a1=1,an+1=3anβˆ’anβˆ’1.a_0=1,\qquad a_1=1,\qquad a_{n+1}=3a_n-a_{n-1}.

Then all positive integer solutions are

(an,an+1)Β andΒ (an+1,an)forΒ nβ‰₯0.\boxed{(a_n,a_{n+1})\text{ and }(a_{n+1},a_n)\quad\text{for }n\ge 0}.

The first few values are

a0=1,a1=1,a2=2,a3=5,a4=13,a5=34.a_0=1,\quad a_1=1,\quad a_2=2,\quad a_3=5,\quad a_4=13,\quad a_5=34.

It remains to check that this sequence really gives solutions. If (u,v)(u,v) satisfies

u2+v2+1=3uv,u^2+v^2+1=3uv,

then (v,3vβˆ’u)(v,3v-u) also satisfies the equation because uu and 3vβˆ’u3v-u are the two Vieta roots of

X2βˆ’3vX+(v2+1)=0.X^2-3vX+(v^2+1)=0.

Since (1,1)(1,1) works, every pair generated by the recurrence works. The descent argument shows there are no others.

AllΒ positiveΒ integerΒ solutionsΒ areΒ (1,1),(1,2),(2,1),(2,5),(5,2),(5,13),(13,5),…\boxed{\text{All positive integer solutions are }(1,1),(1,2),(2,1),(2,5),(5,2),(5,13),(13,5),\ldots}

Full notes β†’

  1. Find the domain and range of f(x)=9βˆ’(xβˆ’2)2xβˆ’2f(x)=\frac{\sqrt{9-(x-2)^2}}{x-2}.
  2. Let f(x)={x2βˆ’4x+1,x<1,ax+b,1≀x<4,x+c,xβ‰₯4.f(x)=\begin{cases}x^2-4x+1, & x<1,\\ax+b, & 1\le x<4,\\\sqrt{x+c}, & x\ge 4.\end{cases}. Find aa, bb, and cc so that the pieces connect at x=1x=1 and x=4x=4, and so that the middle piece has average rate of change 33 on [1,4][1,4].
  3. Find the explicit form(s) for the relation (x2+y2)2=4(x2βˆ’y2)(x^2+y^2)^2=4(x^2-y^2).
  4. Find the explicit form(s) for the relation y2βˆ’2xy+x2=4x+4y^2-2xy+x^2=4x+4. State the domain of each branch.
  5. Let f(x)=(xβˆ’3)2+2f(x)=(x-3)^2+2 with domain xβ‰₯3x\ge 3. Find fβˆ’1(x)f^{-1}(x), and state the domain and range of fβˆ’1f^{-1}.
  6. Let f:[βˆ’2,∞)β†’[βˆ’4,∞)f:[-2,\infty)\to[-4,\infty) be defined by f(x)=(x+2)2βˆ’4f(x)=(x+2)^2-4. Determine whether ff is injective, surjective, bijective, or none.
  7. Simplify the difference quotient for f(x)=2xβˆ’1f(x)=\frac{2}{x-1}. That is, simplify f(x+h)βˆ’f(x)h.\frac{f(x+h)-f(x)}{h}.
  8. The graph of y=f(x)y=f(x) has domain [βˆ’4,6][-4,6] and range [βˆ’2,5][-2,5]. Find the domain and range of g(x)=βˆ’3f(xβˆ’2x+1)+7g(x)=-3f(\frac{x-2}{x+1})+7.
  9. Find fβˆ’1(3)f^{-1}(3) given that f(x)=3x+12x+f(x)f(x)=\frac{3x+1}{2x+f(x)}.
  10. Let h(x)=4βˆ’βˆ£xβˆ’1∣.h(x)=\sqrt{4-\lvert x-1 \rvert}. Find the domain and range of hh, and describe the transformations from y=xy=\sqrt{x} as clearly as possible.
  11. Let f(x)=2x+5f(x)=\sqrt{2x+5} and g(x)=1xβˆ’3g(x)=\frac{1}{x-3}. Find formulas and domains for (f∘g)(x)(f\circ g)(x) and (g∘f)(x)(g\circ f)(x).
  12. Let f(x)=∣xβˆ’2∣+1f(x)=\lvert x-2\rvert+1. If the domain is restricted to [2,∞)[2,\infty) and the codomain is [1,∞)[1,\infty), determine whether ff is bijective and find fβˆ’1(x)f^{-1}(x). Then explain what goes wrong if the domain is all real numbers.
  13. Let f(x)={2x+a,x<1,x2+b,1≀x<3,cxβˆ’1,xβ‰₯3.f(x)=\begin{cases}2x+a, & x<1,\\x^2+b, & 1\le x<3,\\cx-1, & x\ge 3.\end{cases} Find aa, bb, and cc so that ff is continuous everywhere and f(0)=5f(0)=5.
  14. Suppose ff is an odd function with domain [βˆ’5,5][-5,5], range [βˆ’3,3][-3,3], and f(2)=βˆ’1f(2)=-1. Define g(x)=2f(xβˆ’1)βˆ’4g(x)=2f(x-1)-4. Find the domain and range of gg, and find g(3)g(3) and g(βˆ’1)g(-1).
  15. Suppose f:Aβ†’Bf:A\to B and g:Bβ†’Cg:B\to C. Prove that if ff and gg are both injective, then g∘fg\circ f is injective. Also prove that if g∘fg\circ f is surjective onto CC, then gg must be surjective onto CC.
  16. (Bonus, Cauchy’s Functional Equation)

Consider a function Q⟢Q\mathbb{Q} \longrightarrow \mathbb{Q} (basically taking rational inputs and giving rational outputs) such that f(x+y)=f(x)+f(y)f(x+y)=f(x)+f(y) (basically for any two rational numbers, this equation holds true for f(x)f(x)).

(A) Show that f(0)=0f(0) = 0 and f(βˆ’x)=βˆ’f(x)f(-x) = -f(x). What does this show about f(x)f(x)?

(B) Prove that f(nx)=nf(x)f(nx) = nf(x) for all n∈Zn \in \mathbb{Z} (for all integer nn).

(C) Prove that f(xn)=f(x)nf(\frac{x}{n}) = \frac{f(x)}{n}.

(D) Determine all such functions f(x)f(x) that satisfy Cauchy’s Functional Equation. Remember you not only need to find all such solutions, but prove that each one is a valid solution to the equation.

(E) The solution in part (D) is the only solution for the rationals, but there exist infinitely more solutions for the reals! Why can’t your proof in steps (A) - (D) extend to real numbers?

The square root requires

9βˆ’(xβˆ’2)2β‰₯0.9-(x-2)^2\ge 0.

Thus

βˆ’3≀xβˆ’2≀3βŸΉβˆ’1≀x≀5.-3\le x-2\le 3 \quad\Longrightarrow\quad -1\le x\le 5.

The denominator also requires x≠2x\ne 2, so

domain=[βˆ’1,2)βˆͺ(2,5].\boxed{\text{domain}=[-1,2)\cup(2,5]}.

Let t=xβˆ’2t=x-2. Then

f(x)=9βˆ’t2t,t∈[βˆ’3,0)βˆͺ(0,3].f(x)=\frac{\sqrt{9-t^2}}{t}, \qquad t\in[-3,0)\cup(0,3].

For t>0t>0, the outputs cover [0,∞)[0,\infty). For t<0t<0, the outputs cover (βˆ’βˆž,0](-\infty,0]. Therefore

range=(βˆ’βˆž,∞).\boxed{\text{range}=(-\infty,\infty)}.

The average rate of change of the middle piece ax+bax+b is its slope, so

a=3.a=3.

The pieces connect at x=1x=1, so

12βˆ’4(1)+1=3(1)+b.1^2-4(1)+1=3(1)+b.

This gives

βˆ’2=3+b⟹b=βˆ’5.-2=3+b \quad\Longrightarrow\quad b=-5.

The pieces connect at x=4x=4, so

3(4)βˆ’5=4+c.3(4)-5=\sqrt{4+c}.

Thus

7=4+c⟹49=4+c⟹c=45.7=\sqrt{4+c} \quad\Longrightarrow\quad 49=4+c \quad\Longrightarrow\quad c=45.

Therefore

a=3,b=βˆ’5,c=45.\boxed{a=3,\qquad b=-5,\qquad c=45}.

Let

u=y2.u=y^2.

Then

(x2+u)2=4(x2βˆ’u).(x^2+u)^2=4(x^2-u).

Expand and collect terms:

x4+2x2u+u2=4x2βˆ’4ux^4+2x^2u+u^2=4x^2-4u u2+(2x2+4)u+x4βˆ’4x2=0.u^2+(2x^2+4)u+x^4-4x^2=0.

Using the quadratic formula,

u=βˆ’(2x2+4)Β±(2x2+4)2βˆ’4(x4βˆ’4x2)2.u=\frac{-(2x^2+4)\pm\sqrt{(2x^2+4)^2-4(x^4-4x^2)}}{2}.

The discriminant simplifies:

(2x2+4)2βˆ’4(x4βˆ’4x2)=16(2x2+1).(2x^2+4)^2-4(x^4-4x^2)=16(2x^2+1).

So

u=βˆ’(x2+2)Β±22x2+1.u=-(x^2+2)\pm 2\sqrt{2x^2+1}.

Since u=y2u=y^2,

y2=βˆ’(x2+2)+22x2+1y^2=-(x^2+2)+2\sqrt{2x^2+1}

or

y2=βˆ’(x2+2)βˆ’22x2+1.y^2=-(x^2+2)-2\sqrt{2x^2+1}.

The second expression is always negative, so it gives no real branches. The real explicit forms are

y=βˆ’(x2+2)+22x2+1\boxed{y=\sqrt{-(x^2+2)+2\sqrt{2x^2+1}}}

and

y=βˆ’βˆ’(x2+2)+22x2+1.\boxed{y=-\sqrt{-(x^2+2)+2\sqrt{2x^2+1}}}.

For these branches to be real,

βˆ’(x2+2)+22x2+1β‰₯0.-(x^2+2)+2\sqrt{2x^2+1}\ge 0.

This simplifies to x2≀4x^2\le 4, so both branches have domain

[βˆ’2,2].\boxed{[-2,2]}.

Start with

y2βˆ’2xy+x2=4x+4.y^2-2xy+x^2=4x+4.

This equation is quadratic in yy. Move everything to one side:

y2βˆ’2xy+(x2βˆ’4xβˆ’4)=0.y^2-2xy+(x^2-4x-4)=0.

Using the quadratic formula with

a=1,b=βˆ’2x,c=x2βˆ’4xβˆ’4,a=1,\qquad b=-2x,\qquad c=x^2-4x-4,

we get

y=βˆ’(βˆ’2x)Β±(βˆ’2x)2βˆ’4(1)(x2βˆ’4xβˆ’4)2.y=\frac{-(-2x)\pm\sqrt{(-2x)^2-4(1)(x^2-4x-4)}}{2}.

Simplify the discriminant:

(βˆ’2x)2βˆ’4(x2βˆ’4xβˆ’4)=4x2βˆ’4x2+16x+16=16(x+1).(-2x)^2-4(x^2-4x-4) =4x^2-4x^2+16x+16 =16(x+1).

So

y=2xΒ±16(x+1)2=2xΒ±4x+12.y=\frac{2x\pm\sqrt{16(x+1)}}{2} =\frac{2x\pm 4\sqrt{x+1}}{2}.

Thus the explicit branches are

y=x+2x+1y=x+2\sqrt{x+1}

and

y=xβˆ’2x+1.y=x-2\sqrt{x+1}.

Both branches require

x+1β‰₯0,x+1\ge 0,

so each branch has domain

[βˆ’1,∞).\boxed{[-1,\infty)}.

Therefore the relation is not one function of xx on most of its domain; it splits into

y=x+2x+1\boxed{y=x+2\sqrt{x+1}}

and

y=xβˆ’2x+1\boxed{y=x-2\sqrt{x+1}}

each with domain [βˆ’1,∞)[-1,\infty).

Start with

y=(xβˆ’3)2+2.y=(x-3)^2+2.

Switch xx and yy:

x=(yβˆ’3)2+2.x=(y-3)^2+2.

Then

xβˆ’2=(yβˆ’3)2.x-2=(y-3)^2.

Since the original domain is xβ‰₯3x\ge 3, use the positive square-root branch:

yβˆ’3=xβˆ’2.y-3=\sqrt{x-2}.

Therefore

fβˆ’1(x)=3+xβˆ’2.\boxed{f^{-1}(x)=3+\sqrt{x-2}}.

The domain of fβˆ’1f^{-1} is the range of ff:

[2,∞).\boxed{[2,\infty)}.

The range of fβˆ’1f^{-1} is the domain of ff:

[3,∞).\boxed{[3,\infty)}.

On [βˆ’2,∞)[-2,\infty), the parabola starts at its vertex and increases. Therefore it passes the horizontal line test, so it is injective.

Also,

f(βˆ’2)=βˆ’4,f(-2)=-4,

and as xβ†’βˆžx\to\infty, f(x)β†’βˆžf(x)\to\infty. Therefore the range is

[βˆ’4,∞),[-4,\infty),

which matches the codomain. So ff is surjective.

Since ff is both injective and surjective,

fΒ isΒ bijective.\boxed{f\text{ is bijective}}.

First,

f(x+h)=2x+hβˆ’1.f(x+h)=\frac{2}{x+h-1}.

So

f(x+h)βˆ’f(x)h=2x+hβˆ’1βˆ’2xβˆ’1h.\frac{f(x+h)-f(x)}{h} = \frac{\frac{2}{x+h-1}-\frac{2}{x-1}}{h}.

Use a common denominator:

2(xβˆ’1)βˆ’2(x+hβˆ’1)(x+hβˆ’1)(xβˆ’1)h.\frac{\frac{2(x-1)-2(x+h-1)}{(x+h-1)(x-1)}}{h}.

The numerator simplifies:

2(xβˆ’1)βˆ’2(x+hβˆ’1)=βˆ’2h.2(x-1)-2(x+h-1)=-2h.

Thus

f(x+h)βˆ’f(x)h=βˆ’2h(x+hβˆ’1)(xβˆ’1)h=βˆ’2(x+hβˆ’1)(xβˆ’1).\frac{f(x+h)-f(x)}{h} =\frac{\frac{-2h}{(x+h-1)(x-1)}}{h} =\boxed{\frac{-2}{(x+h-1)(x-1)}}.

For the domain, the input to ff must lie in [βˆ’4,6][-4,6]:

βˆ’4≀xβˆ’2x+1≀6,xβ‰ βˆ’1.-4\le \frac{x-2}{x+1}\le 6, \qquad x\ne -1.

Solve the two inequalities separately:

xβˆ’2x+1β‰₯βˆ’4⟹5x+2x+1β‰₯0,\frac{x-2}{x+1}\ge -4 \quad\Longrightarrow\quad \frac{5x+2}{x+1}\ge 0,

so

x<βˆ’1orxβ‰₯βˆ’25.x<-1\quad\text{or}\quad x\ge -\frac25.

Also,

xβˆ’2x+1≀6βŸΉβˆ’5xβˆ’8x+1≀0,\frac{x-2}{x+1}\le 6 \quad\Longrightarrow\quad \frac{-5x-8}{x+1}\le 0,

so

xβ‰€βˆ’85orx>βˆ’1.x\le -\frac85\quad\text{or}\quad x>-1.

Intersecting these gives

domain=(βˆ’βˆž,βˆ’8/5]βˆͺ[βˆ’2/5,∞).\boxed{\text{domain}=(-\infty,-8/5]\cup[-2/5,\infty)}.

The range cannot be determined from only the information given. The inner function

xβˆ’2x+1\frac{x-2}{x+1}

takes values in [βˆ’4,6][-4,6] except it never equals 11. Since we only know the domain and range of ff, we do not know whether removing the input 11 changes the outputs of ff. If the graph of ff still hits every value in [βˆ’2,5][-2,5] away from input 11, then the range would be

[βˆ’8,13],[-8,13],

but that is an extra assumption. Therefore the correct conclusion from the stated information is

theΒ rangeΒ isΒ notΒ determinedΒ byΒ theΒ givenΒ data.\boxed{\text{the range is not determined by the given data}}.

We want fβˆ’1(3)f^{-1}(3), meaning we want the input xx for which

f(x)=3.f(x)=3.

Use the given relation:

f(x)=3x+12x+f(x).f(x)=\frac{3x+1}{2x+f(x)}.

Substitute f(x)=3f(x)=3:

3=3x+12x+3.3=\frac{3x+1}{2x+3}.

Then

3(2x+3)=3x+13(2x+3)=3x+1 6x+9=3x+16x+9=3x+1 3x=βˆ’8.3x=-8.

So

fβˆ’1(3)=βˆ’83.\boxed{f^{-1}(3)=-\frac83}.

For the domain, require

4βˆ’βˆ£xβˆ’1∣β‰₯0.4-\lvert x-1\rvert\ge 0.

Then

∣xβˆ’1βˆ£β‰€4,\lvert x-1\rvert\le 4,

so

βˆ’4≀xβˆ’1≀4.-4\le x-1\le 4.

Thus

domain=[βˆ’3,5].\boxed{\text{domain}=[-3,5]}.

The largest value occurs when ∣xβˆ’1∣=0\lvert x-1\rvert=0:

h(1)=4=2.h(1)=\sqrt4=2.

The smallest value occurs when ∣xβˆ’1∣=4\lvert x-1\rvert=4:

h(βˆ’3)=h(5)=0.h(-3)=h(5)=0.

Therefore

range=[0,2].\boxed{\text{range}=[0,2]}.

This is not a single basic transformation of y=xy=\sqrt{x}. It is better viewed as two square-root pieces:

h(x)={x+3,βˆ’3≀x≀1,5βˆ’x,1≀x≀5.h(x)= \begin{cases} \sqrt{x+3}, & -3\le x\le 1,\\ \sqrt{5-x}, & 1\le x\le 5. \end{cases}

The graph is symmetric about x=1x=1, has endpoints (βˆ’3,0)(-3,0) and (5,0)(5,0), and reaches its maximum at (1,2)(1,2).

First,

(f∘g)(x)=f(g(x))=2(1xβˆ’3)+5=2xβˆ’3+5.(f\circ g)(x)=f(g(x)) =\sqrt{2\left(\frac{1}{x-3}\right)+5} =\sqrt{\frac{2}{x-3}+5}.

Combine the expression under the radical:

2xβˆ’3+5=2+5xβˆ’15xβˆ’3=5xβˆ’13xβˆ’3.\frac{2}{x-3}+5 =\frac{2+5x-15}{x-3} =\frac{5x-13}{x-3}.

So

(f∘g)(x)=5xβˆ’13xβˆ’3.(f\circ g)(x)=\sqrt{\frac{5x-13}{x-3}}.

For the domain, require x≠3x\ne 3 and

5xβˆ’13xβˆ’3β‰₯0.\frac{5x-13}{x-3}\ge 0.

The critical values are x=135x=\frac{13}{5} and x=3x=3. A sign chart gives

domainΒ ofΒ f∘g=(βˆ’βˆž,135]βˆͺ(3,∞).\boxed{\text{domain of }f\circ g=\left(-\infty,\frac{13}{5}\right]\cup(3,\infty)}.

Now

(g∘f)(x)=g(f(x))=12x+5βˆ’3.(g\circ f)(x)=g(f(x)) =\frac{1}{\sqrt{2x+5}-3}.

For the domain, require

2x+5β‰₯02x+5\ge 0

and also

2x+5βˆ’3β‰ 0.\sqrt{2x+5}-3\ne 0.

The first condition gives xβ‰₯βˆ’52x\ge -\frac52. The second condition gives

2x+5β‰ 3⟹2x+5β‰ 9⟹xβ‰ 2.\sqrt{2x+5}\ne 3 \quad\Longrightarrow\quad 2x+5\ne 9 \quad\Longrightarrow\quad x\ne 2.

Therefore

(g∘f)(x)=12x+5βˆ’3\boxed{(g\circ f)(x)=\frac{1}{\sqrt{2x+5}-3}}

with

domainΒ ofΒ g∘f=[βˆ’52,∞)βˆ–{2}.\boxed{\text{domain of }g\circ f=\left[-\frac52,\infty\right)\setminus\{2\}}.

On the restricted domain [2,∞)[2,\infty),

f(x)=∣xβˆ’2∣+1=xβˆ’2+1=xβˆ’1.f(x)=\lvert x-2\rvert+1=x-2+1=x-1.

This function is increasing on [2,∞)[2,\infty), so it is injective.

Also, if xβ‰₯2x\ge 2, then

f(x)=xβˆ’1β‰₯1.f(x)=x-1\ge 1.

Every output yβ‰₯1y\ge 1 is reached by choosing x=y+1x=y+1, which is at least 22. Therefore ff is surjective onto [1,∞)[1,\infty).

So f:[2,∞)β†’[1,∞)f:[2,\infty)\to[1,\infty) is bijective.

To find the inverse, write

y=xβˆ’1.y=x-1.

Then

x=y+1.x=y+1.

Thus

fβˆ’1(x)=x+1\boxed{f^{-1}(x)=x+1}

with domain [1,∞)[1,\infty) and range [2,∞)[2,\infty).

If the domain is all real numbers, the function is not injective. For example,

f(1)=2andf(3)=2.f(1)=2 \qquad\text{and}\qquad f(3)=2.

Since two different inputs give the same output, the function does not have an inverse function on all of R\mathbb{R}.

Since f(0)=5f(0)=5 and 0<10<1, use the first piece:

f(0)=2(0)+a=a.f(0)=2(0)+a=a.

Thus

a=5.a=5.

For continuity at x=1x=1, the left-hand value must match the value from the middle piece:

2(1)+a=12+b.2(1)+a=1^2+b.

Substitute a=5a=5:

2+5=1+b.2+5=1+b.

So

b=6.b=6.

For continuity at x=3x=3, the value from the middle piece must match the value from the last piece:

32+b=3cβˆ’1.3^2+b=3c-1.

Substitute b=6b=6:

9+6=3cβˆ’1.9+6=3c-1.

Then

16=3c,16=3c,

so

c=163.c=\frac{16}{3}.

Therefore

a=5,b=6,c=163.\boxed{a=5,\qquad b=6,\qquad c=\frac{16}{3}}.

The expression f(xβˆ’1)f(x-1) requires

xβˆ’1∈[βˆ’5,5].x-1\in[-5,5].

So

βˆ’5≀xβˆ’1≀5.-5\le x-1\le 5.

Add 11 throughout:

βˆ’4≀x≀6.-4\le x\le 6.

Thus

domainΒ ofΒ g=[βˆ’4,6].\boxed{\text{domain of }g=[-4,6]}.

Since ff has range [βˆ’3,3][-3,3], the expression 2f(xβˆ’1)2f(x-1) has range

[βˆ’6,6].[-6,6].

Subtracting 44 gives

rangeΒ ofΒ g=[βˆ’10,2].\boxed{\text{range of }g=[-10,2]}.

Now

g(3)=2f(3βˆ’1)βˆ’4=2f(2)βˆ’4.g(3)=2f(3-1)-4=2f(2)-4.

Since f(2)=βˆ’1f(2)=-1,

g(3)=2(βˆ’1)βˆ’4=βˆ’6.g(3)=2(-1)-4=-6.

So

g(3)=βˆ’6.\boxed{g(3)=-6}.

Also,

g(βˆ’1)=2f(βˆ’1βˆ’1)βˆ’4=2f(βˆ’2)βˆ’4.g(-1)=2f(-1-1)-4=2f(-2)-4.

Because ff is odd,

f(βˆ’2)=βˆ’f(2)=1.f(-2)=-f(2)=1.

Therefore

g(βˆ’1)=2(1)βˆ’4=βˆ’2.g(-1)=2(1)-4=-2.

So

g(βˆ’1)=βˆ’2.\boxed{g(-1)=-2}.

First suppose ff and gg are both injective. To prove that g∘fg\circ f is injective, start by assuming two inputs give the same output:

(g∘f)(a)=(g∘f)(b).(g\circ f)(a)=(g\circ f)(b).

This means

g(f(a))=g(f(b)).g(f(a))=g(f(b)).

Since gg is injective,

f(a)=f(b).f(a)=f(b).

Since ff is injective,

a=b.a=b.

Therefore

g∘f is injective.\boxed{g\circ f\text{ is injective}}.

Now suppose g∘fg\circ f is surjective onto CC. This means that for every c∈Cc\in C, there is some a∈Aa\in A such that

(g∘f)(a)=c.(g\circ f)(a)=c.

Equivalently,

g(f(a))=c.g(f(a))=c.

But f(a)f(a) is an element of BB. So for every c∈Cc\in C, we have found an element of BB, namely f(a)f(a), that maps to cc under gg.

Therefore

gΒ isΒ surjectiveΒ ontoΒ C.\boxed{g\text{ is surjective onto }C}.

We are given

f(x+y)=f(x)+f(y)f(x+y)=f(x)+f(y)

for rational inputs.

For part (A), set x=0x=0 and y=0y=0:

f(0)=f(0+0)=f(0)+f(0).f(0)=f(0+0)=f(0)+f(0).

Thus

f(0)=0.\boxed{f(0)=0}.

Now use 0=x+(βˆ’x)0=x+(-x):

0=f(0)=f(x+(βˆ’x))=f(x)+f(βˆ’x).0=f(0)=f(x+(-x))=f(x)+f(-x).

So

f(βˆ’x)=βˆ’f(x).\boxed{f(-x)=-f(x)}.

This shows that ff is an odd function.

For part (B), if nn is a positive integer, then

f(nx)=f(x+x+β‹―+x⏟nΒ times)=f(x)+f(x)+β‹―+f(x)⏟nΒ times=nf(x).f(nx)=f(\underbrace{x+x+\cdots+x}_{n\text{ times}}) =\underbrace{f(x)+f(x)+\cdots+f(x)}_{n\text{ times}} =nf(x).

For n=0n=0, this says f(0)=0f(0)=0. For negative nn, use part (A):

f(nx)=f(βˆ’(∣n∣x))=βˆ’f(∣n∣x)=βˆ’βˆ£n∣f(x)=nf(x).f(nx)=f(-(\lvert n\rvert x))=-f(\lvert n\rvert x)=-\lvert n\rvert f(x)=nf(x).

Therefore

f(nx)=nf(x)for all n∈Z.\boxed{f(nx)=nf(x)\quad\text{for all }n\in\mathbb{Z}}.

For part (C), apply part (B) to x/nx/n:

f(x)=f(nβ‹…xn)=nf(xn).f(x)=f\left(n\cdot\frac{x}{n}\right)=n f\left(\frac{x}{n}\right).

Therefore

f(xn)=f(x)n.\boxed{f\left(\frac{x}{n}\right)=\frac{f(x)}{n}}.

For part (D), let

c=f(1).c=f(1).

For any rational number r=mnr=\frac{m}{n},

f(r)=f(mn)=f(m)n.f(r)=f\left(\frac{m}{n}\right)=\frac{f(m)}{n}.

By part (B),

f(m)=mf(1)=mc.f(m)=mf(1)=mc.

So

f(r)=mcn=cr.f(r)=\frac{mc}{n}=cr.

Thus every solution must have the form

f(x)=cx\boxed{f(x)=cx}

for some rational constant cc. Conversely, every function of the form f(x)=cxf(x)=cx works because

f(x+y)=c(x+y)=cx+cy=f(x)+f(y).f(x+y)=c(x+y)=cx+cy=f(x)+f(y).

For part (E), the proof works over Q\mathbb{Q} because every rational number is a rational multiple of 11. It does not extend to all real numbers because not every real number can be built from 11 using only integer multiplication and division. Over R\mathbb{R}, there are many wild additive functions if no conditions like continuity, monotonicity, or boundedness are required.

Unit 4 & 13: Polynomial & Rational Functions and Applications to Optimization

Section titled β€œUnit 4 & 13: Polynomial & Rational Functions and Applications to Optimization”

Full notes β†’

  1. Let f(x)=mx+bf(x)=mx+b. Suppose f(a+b)=f(a)+f(b)βˆ’6f(a+b)=f(a)+f(b)-6 for all real numbers a,ba,b and f(4)=10f(4)=10. Find f(x)f(x), its xx-intercept, and the equation of the line perpendicular to ff through (4,10)(4,10).
  2. A quadratic function has xx-intercepts βˆ’1-1 and 55 and passes through (0,10)(0,10). Find the function, its vertex, maximum/minimum value, and range.
  3. For h(x)=βˆ’2x2+8x+10h(x)=\sqrt{-2x^2+8x+10}, find the domain, range, and maximum value of hh.
  4. Find the lowest-degree polynomial p(x)p(x) with real coefficients such that x=βˆ’3x=-3 is a zero of multiplicity 22, x=1x=1 is a zero of multiplicity 33, and p(0)=βˆ’18p(0)=-18. Give the end behavior.
  5. For f(x)=βˆ’12(x+4)(xβˆ’1)2(xβˆ’3)3f(x)=-\dfrac12(x+4)(x-1)^2(x-3)^3, give the degree, leading coefficient, end behavior, zeros with multiplicities, crossing/bouncing behavior, yy-intercept, and maximum possible number of turning points. Give a rough graph of the function.
  6. Find the lowest-degree polynomial with real coefficients, leading coefficient positive, zeros 22 with multiplicity 22, βˆ’1-1, and 3+i3+i, and f(0)=100f(0)=100.
  7. Factor P(x)=x4βˆ’3x3βˆ’11x2+39xβˆ’18P(x)=x^4-3x^3-11x^2+39x-18 completely over the real numbers, given that P(3)=0P(3)=0.
  8. Use the Rational Root Theorem to list the possible rational zeros of f(x)=2x4βˆ’x3βˆ’20x2+13x+30f(x)=2x^4-x^3-20x^2+13x+30, then find all real zeros.
  9. A polynomial f(x)f(x) leaves remainder 55 when divided by xβˆ’2x-2 and remainder βˆ’4-4 when divided by x+1x+1. Find the remainder when f(x)f(x) is divided by (xβˆ’2)(x+1)(x-2)(x+1).
  10. Find the monic polynomial with rational coefficients whose zeros include 1+i1+i and 2βˆ’32-\sqrt3.
  11. For R(x)=(xβˆ’2)(x+1)2(x+1)(xβˆ’3)R(x)=\dfrac{(x-2)(x+1)^2}{(x+1)(x-3)}, state the domain, hole, vertical asymptote, slant asymptote, and intercepts. Give a rough graph of this function.
  12. Solve in R\mathbb{R}: (xβˆ’4)(x+1)2(xβˆ’2)(x+1)≀0\dfrac{(x-4)(x+1)^2}{(x-2)(x+1)}\le 0.
  13. A box with no top is made by cutting squares of side length xx from each corner of a 24Β in24\text{ in} by 18Β in18\text{ in} sheet and folding up the sides. Write the volume function, state the practical domain, and use a graph or calculator to approximate the value of xx that maximizes the volume.
  14. A machine’s output is modeled by M(x)=150xx2+25M(x)=\dfrac{150x}{x^2+25} for xβ‰₯0x\ge 0. Use an algebraic method to find the maximum possible output and the input where it occurs.
  15. A farmer has 240240 feet of fencing to build three identical rectangular pens side-by-side, sharing interior fences. If the pens together form one large rectangle split by two parallel dividers, find the dimensions of the large rectangle that maximize the total area.
  16. (Bonus, Rational Root Theorem)

In this unit, we have introduced the Rational Root Theorem as a quick way of finding rational roots. We will now get a chance to prove this theorem.

Let

f(x)=anxn+anβˆ’1xnβˆ’1+β‹―+a1x+a0f(x)=a_nx^n+a_{n-1}x^{n-1}+\cdots+a_1x+a_0

have integer coefficients. Suppose pq\frac{p}{q} is a rational zero in lowest terms. Note that a∣ba \mid b means aa divides bb and gcdgcd means greatest common divisor.

(A)(A) Substitute pq\frac{p}{q} into f(x)=0f(x)=0 and multiply by qnq^n and rearrange your equation to show that p∣a0qnp\mid a_0q^n. Also explain why gcd⁑(p,q)=1\gcd(p,q)=1 implies p∣a0p\mid a_0.

(B)(B) Rearrange the equation from part (A)(A) in a different way to show that q∣anpnq\mid a_np^n and explain why gcd⁑(p,q)=1\gcd(p,q)=1 implies q∣anq\mid a_n.

(C)(C) State the Rational Root Theorem in words.


Let f(x)=mx+bf(x)=mx+b. Then

f(a+b)=m(a+b)+b=ma+mb+b,f(a+b)=m(a+b)+b=ma+mb+b,

while

f(a)+f(b)βˆ’6=(ma+b)+(mb+b)βˆ’6=ma+mb+2bβˆ’6.f(a)+f(b)-6=(ma+b)+(mb+b)-6=ma+mb+2b-6.

Since these are equal for all a,ba,b,

b=2bβˆ’6,b=2b-6,

so b=6b=6. Use f(4)=10f(4)=10:

4m+6=10,4m+6=10,

so m=1m=1. Therefore

f(x)=x+6.\boxed{f(x)=x+6}.

The xx-intercept satisfies x+6=0x+6=0, so it is

(βˆ’6,0).\boxed{(-6,0)}.

The slope of ff is 11, so a perpendicular line has slope βˆ’1-1. Through (4,10)(4,10):

yβˆ’10=βˆ’(xβˆ’4),y-10=-(x-4),

so

y=βˆ’x+14.\boxed{y=-x+14}.

Since the zeros are βˆ’1-1 and 55,

q(x)=a(x+1)(xβˆ’5).q(x)=a(x+1)(x-5).

Use (0,10)(0,10):

10=a(1)(βˆ’5),10=a(1)(-5),

so a=βˆ’2a=-2. Thus

q(x)=βˆ’2(x+1)(xβˆ’5).\boxed{q(x)=-2(x+1)(x-5)}.

Expanding,

q(x)=βˆ’2x2+8x+10.q(x)=-2x^2+8x+10.

The axis of symmetry is halfway between the zeros:

x=βˆ’1+52=2.x=\frac{-1+5}{2}=2.

Then

q(2)=βˆ’2(3)(βˆ’3)=18.q(2)=-2(3)(-3)=18.

The vertex is

(2,18).\boxed{(2,18)}.

Since a<0a<0, this is a maximum. The maximum value is 1818 and the range is

(βˆ’βˆž,18].\boxed{(-\infty,18]}.

The square root requires

βˆ’2x2+8x+10β‰₯0.-2x^2+8x+10\ge 0.

Factor:

βˆ’2(x2βˆ’4xβˆ’5)β‰₯0-2(x^2-4x-5)\ge 0

so

βˆ’2(xβˆ’5)(x+1)β‰₯0.-2(x-5)(x+1)\ge 0.

This is true for

βˆ’1≀x≀5.\boxed{-1\le x\le 5}.

Thus the domain is

[βˆ’1,5].\boxed{[-1,5]}.

The inside quadratic has maximum at the midpoint of the roots:

x=2.x=2.

Its maximum value is

βˆ’2(2)2+8(2)+10=18.-2(2)^2+8(2)+10=18.

Since square root is increasing, the maximum of hh is

18=32.\boxed{\sqrt{18}=3\sqrt2}.

At the endpoints, h(x)=0h(x)=0, so the range is

[0,32].\boxed{[0,3\sqrt2]}.

The lowest-degree polynomial must have factors

(x+3)2and(xβˆ’1)3.(x+3)^2 \qquad\text{and}\qquad (x-1)^3.

So

p(x)=a(x+3)2(xβˆ’1)3.p(x)=a(x+3)^2(x-1)^3.

Use p(0)=βˆ’18p(0)=-18:

βˆ’18=a(3)2(βˆ’1)3=βˆ’9a.-18=a(3)^2(-1)^3=-9a.

Thus a=2a=2, so

p(x)=2(x+3)2(xβˆ’1)3.\boxed{p(x)=2(x+3)^2(x-1)^3}.

The degree is 55 and the leading coefficient is 22. Therefore

xβ†’βˆ’βˆžβ‡’p(x)β†’βˆ’βˆž,xβ†’βˆžβ‡’p(x)β†’βˆž.x\to -\infty \Rightarrow p(x)\to -\infty, \qquad x\to \infty \Rightarrow p(x)\to \infty.

For

f(x)=βˆ’12(x+4)(xβˆ’1)2(xβˆ’3)3,f(x)=-\frac12(x+4)(x-1)^2(x-3)^3,

the degree is

1+2+3=6.1+2+3=6.

The leading coefficient is

βˆ’12.\boxed{-\frac12}.

Even degree with negative leading coefficient means

xβ†’βˆ’βˆžβ‡’f(x)β†’βˆ’βˆž,xβ†’βˆžβ‡’f(x)β†’βˆ’βˆž.x\to -\infty \Rightarrow f(x)\to -\infty, \qquad x\to \infty \Rightarrow f(x)\to -\infty.

The zeros are:

  • x=βˆ’4x=-4, multiplicity 11, crosses.
  • x=1x=1, multiplicity 22, bounces.
  • x=3x=3, multiplicity 33, crosses with flattening.

The yy-intercept is

f(0)=βˆ’12(4)(1)(βˆ’27)=54,f(0)=-\frac12(4)(1)(-27)=54,

so it is

(0,54).\boxed{(0,54)}.

The maximum possible number of turning points is

5.\boxed{5}.

This graph is shown below:

parent functions

Because the polynomial has real coefficients, 3βˆ’i3-i must also be a zero. The lowest-degree polynomial has the form

f(x)=a(xβˆ’2)2(x+1)(xβˆ’(3+i))(xβˆ’(3βˆ’i)).f(x)=a(x-2)^2(x+1)\bigl(x-(3+i)\bigr)\bigl(x-(3-i)\bigr).

The complex pair multiplies to

(xβˆ’(3+i))(xβˆ’(3βˆ’i))=(xβˆ’3)2+1.\bigl(x-(3+i)\bigr)\bigl(x-(3-i)\bigr)=(x-3)^2+1.

So

f(x)=a(xβˆ’2)2(x+1)((xβˆ’3)2+1).f(x)=a(x-2)^2(x+1)\bigl((x-3)^2+1\bigr).

Use f(0)=100f(0)=100:

100=a(4)(1)(10)=40a.100=a(4)(1)(10)=40a.

Thus a=52a=\dfrac52, and

f(x)=52(xβˆ’2)2(x+1)((xβˆ’3)2+1).\boxed{f(x)=\frac52(x-2)^2(x+1)\bigl((x-3)^2+1\bigr)}.

Since P(3)=0P(3)=0, xβˆ’3x-3 is a factor. Synthetic division gives

31βˆ’3βˆ’1139βˆ’1830βˆ’331810βˆ’1160\begin{array}{r|rrrrr} 3 & 1 & -3 & -11 & 39 & -18\\ & & 3 & 0 & -33 & 18\\ \hline & 1 & 0 & -11 & 6 & 0 \end{array}

So

P(x)=(xβˆ’3)(x3βˆ’11x+6).P(x)=(x-3)(x^3-11x+6).

Test x=3x=3 again:

310βˆ’11639βˆ’613βˆ’20\begin{array}{r|rrrr} 3 & 1 & 0 & -11 & 6\\ & & 3 & 9 & -6\\ \hline & 1 & 3 & -2 & 0 \end{array}

Thus

P(x)=(xβˆ’3)2(x2+3xβˆ’2).P(x)=(x-3)^2(x^2+3x-2).

The quadratic formula gives

x=βˆ’3Β±9+82=βˆ’3Β±172.x=\frac{-3\pm\sqrt{9+8}}{2} =\frac{-3\pm\sqrt{17}}{2}.

Therefore

P(x)=(xβˆ’3)2(xβˆ’βˆ’3+172)(xβˆ’βˆ’3βˆ’172).\boxed{P(x)=(x-3)^2\left(x-\frac{-3+\sqrt{17}}{2}\right)\left(x-\frac{-3-\sqrt{17}}{2}\right)}.

By the Rational Root Theorem, possible rational zeros are

Β±1,Β Β±2,Β Β±3,Β Β±5,Β Β±6,Β Β±10,Β Β±15,Β Β±30,\pm1,\ \pm2,\ \pm3,\ \pm5,\ \pm6,\ \pm10,\ \pm15,\ \pm30,

and

Β±12,Β Β±32,Β Β±52,Β Β±152.\pm\frac12,\ \pm\frac32,\ \pm\frac52,\ \pm\frac{15}{2}.

Factor by grouping:

2x4βˆ’x3βˆ’20x2+13x+30=(x2+xβˆ’6)(2x2βˆ’3xβˆ’5).2x^4-x^3-20x^2+13x+30 =(x^2+x-6)(2x^2-3x-5).

Then

(x2+xβˆ’6)(2x2βˆ’3xβˆ’5)=(x+3)(xβˆ’2)(2xβˆ’5)(x+1).(x^2+x-6)(2x^2-3x-5) =(x+3)(x-2)(2x-5)(x+1).

So the real zeros are

βˆ’3,Β βˆ’1,Β 2,Β 52.\boxed{-3,\ -1,\ 2,\ \frac52}.

When dividing by (xβˆ’2)(x+1)(x-2)(x+1), the remainder must be linear:

R(x)=ax+b.R(x)=ax+b.

Since the remainder after division by xβˆ’2x-2 is 55,

R(2)=5.R(2)=5.

Since the remainder after division by x+1x+1 is βˆ’4-4,

R(βˆ’1)=βˆ’4.R(-1)=-4.

Thus

2a+b=5,βˆ’a+b=βˆ’4.2a+b=5, \qquad -a+b=-4.

Subtract:

3a=9,3a=9,

so a=3a=3. Then b=βˆ’1b=-1. The remainder is

3xβˆ’1.\boxed{3x-1}.

For rational coefficients, conjugate pairs are required:

1+i,Β 1βˆ’i,Β 2βˆ’3,Β 2+3.1+i,\ 1-i,\ 2-\sqrt3,\ 2+\sqrt3.

The polynomial is

(xβˆ’(1+i))(xβˆ’(1βˆ’i))(xβˆ’(2βˆ’3))(xβˆ’(2+3)).\bigl(x-(1+i)\bigr)\bigl(x-(1-i)\bigr)\bigl(x-(2-\sqrt3)\bigr)\bigl(x-(2+\sqrt3)\bigr).

Since

(xβˆ’(1+i))(xβˆ’(1βˆ’i))=(xβˆ’1)2+1=x2βˆ’2x+2\bigl(x-(1+i)\bigr)\bigl(x-(1-i)\bigr)=(x-1)^2+1=x^2-2x+2

and

(xβˆ’(2βˆ’3))(xβˆ’(2+3))=(xβˆ’2)2βˆ’3=x2βˆ’4x+1,\bigl(x-(2-\sqrt3)\bigr)\bigl(x-(2+\sqrt3)\bigr)=(x-2)^2-3=x^2-4x+1,

we get

(x2βˆ’2x+2)(x2βˆ’4x+1).(x^2-2x+2)(x^2-4x+1).

Expanding:

x4βˆ’6x3+11x2βˆ’10x+2.\boxed{x^4-6x^3+11x^2-10x+2}.

Start with

R(x)=(xβˆ’2)(x+1)2(x+1)(xβˆ’3).R(x)=\frac{(x-2)(x+1)^2}{(x+1)(x-3)}.

The original denominator is zero at x=βˆ’1x=-1 and x=3x=3, so the domain is

xβ‰ βˆ’1,3.\boxed{x\ne -1,3}.

Cancel the common factor:

R(x)=(xβˆ’2)(x+1)xβˆ’3,xβ‰ βˆ’1,3.R(x)=\frac{(x-2)(x+1)}{x-3}, \qquad x\ne -1,3.

The canceled factor creates a hole at x=βˆ’1x=-1. Its yy-value is

(βˆ’1βˆ’2)(βˆ’1+1)βˆ’1βˆ’3=0,\frac{(-1-2)(-1+1)}{-1-3}=0,

so the hole is

(βˆ’1,0).\boxed{(-1,0)}.

The uncanceled denominator gives the vertical asymptote:

x=3.\boxed{x=3}.

There is no horizontal asymptote because the numerator degree is one more than the denominator degree. For the slant asymptote, simplify the numerator:

(xβˆ’2)(x+1)=x2βˆ’xβˆ’2.(x-2)(x+1)=x^2-x-2.

Divide:

x2βˆ’xβˆ’2xβˆ’3=x+2+4xβˆ’3.\frac{x^2-x-2}{x-3} =x+2+\frac{4}{x-3}.

Thus the slant asymptote is

y=x+2.\boxed{y=x+2}.

The true xx-intercept comes from the simplified numerator and must be in the original domain. Since x=βˆ’1x=-1 is a hole, the only xx-intercept is

(2,0).\boxed{(2,0)}.

The yy-intercept is

R(0)=(βˆ’2)(1)2(1)(βˆ’3)=23,R(0)=\frac{(-2)(1)^2}{(1)(-3)}=\frac23,

so it is

(0,23).\boxed{\left(0,\frac23\right)}.

The graph is shown below:

parent functions
(xβˆ’4)(x+1)2(xβˆ’2)(x+1)\frac{(x-4)(x+1)^2}{(x-2)(x+1)}

has original domain restrictions

xβ‰ βˆ’1,Β 2.x\ne -1,\ 2.

Cancel one factor of x+1x+1:

(xβˆ’4)(x+1)xβˆ’2≀0,xβ‰ βˆ’1,2.\frac{(x-4)(x+1)}{x-2}\le 0, \qquad x\ne -1,2.

The critical numbers are

βˆ’1,Β 2,Β 4.-1,\ 2,\ 4.

Test intervals:

  • On (βˆ’βˆž,βˆ’1)(-\infty,-1), the expression is negative.
  • At x=βˆ’1x=-1, the original expression is undefined.
  • On (βˆ’1,2)(-1,2), the expression is positive.
  • At x=2x=2, the expression is undefined.
  • On (2,4)(2,4), the expression is negative.
  • At x=4x=4, the expression is zero.
  • On (4,∞)(4,\infty), the expression is positive.

Therefore the solution is

(βˆ’βˆž,βˆ’1)βˆͺ(2,4].\boxed{(-\infty,-1)\cup(2,4]}.

The dimensions of the box are:

length=24βˆ’2x,\text{length}=24-2x, width=18βˆ’2x,\text{width}=18-2x, height=x.\text{height}=x.

So

V(x)=x(24βˆ’2x)(18βˆ’2x).V(x)=x(24-2x)(18-2x).

The practical domain is

0<x<9.\boxed{0<x<9}.

Expanding,

V(x)=4x3βˆ’84x2+432x.V(x)=4x^3-84x^2+432x.

Using a graph or calculator on 0<x<90<x<9, the maximum occurs at approximately

xβ‰ˆ3.39Β in.\boxed{x\approx 3.39\text{ in}}.

The maximum volume is approximately

V(3.39)β‰ˆ655.0Β in3.V(3.39)\approx 655.0\text{ in}^3.

Let

y=150xx2+25.y=\frac{150x}{x^2+25}.

Then

y(x2+25)=150x.y(x^2+25)=150x.

Rearrange as a quadratic in xx:

yx2βˆ’150x+25y=0.yx^2-150x+25y=0.

For real xx, the discriminant must be nonnegative:

(βˆ’150)2βˆ’4(y)(25y)β‰₯0.(-150)^2-4(y)(25y)\ge 0.

Thus

22500βˆ’100y2β‰₯0⟹y2≀225.22500-100y^2\ge 0 \quad\Longrightarrow\quad y^2\le 225.

Since M(x)β‰₯0M(x)\ge 0 for xβ‰₯0x\ge 0, the maximum possible output is

15.\boxed{15}.

Find where it occurs:

15=150xx2+25.15=\frac{150x}{x^2+25}.

Then

15x2+375=150x⟹x2βˆ’10x+25=0⟹(xβˆ’5)2=0.15x^2+375=150x \quad\Longrightarrow\quad x^2-10x+25=0 \quad\Longrightarrow\quad (x-5)^2=0.

So the maximum occurs at

x=5.\boxed{x=5}.

Let the large rectangle have length yy and width xx, where the two interior dividers are each parallel to the width. Then the fencing uses four widths and two lengths:

4x+2y=240.4x+2y=240.

So

y=120βˆ’2x.y=120-2x.

The total area is

A(x)=xy=x(120βˆ’2x)=120xβˆ’2x2.A(x)=xy=x(120-2x)=120x-2x^2.

This parabola opens downward, so its maximum occurs at

x=βˆ’1202(βˆ’2)=30.x=-\frac{120}{2(-2)}=30.

Then

y=120βˆ’2(30)=60.y=120-2(30)=60.

Thus the large rectangle should be

30Β ftΒ byΒ 60Β ft.\boxed{30\text{ ft by }60\text{ ft}}.

The maximum total area is

1800Β ft2.\boxed{1800\text{ ft}^2}.

For part (A), since pq\frac{p}{q} is a zero,

an(pq)n+anβˆ’1(pq)nβˆ’1+β‹―+a1(pq)+a0=0.a_n\left(\frac{p}{q}\right)^n +a_{n-1}\left(\frac{p}{q}\right)^{n-1} +\cdots +a_1\left(\frac{p}{q}\right)+a_0=0.

Multiplying by qnq^n gives

anpn+anβˆ’1pnβˆ’1q+β‹―+a1pqnβˆ’1+a0qn=0.a_np^n+a_{n-1}p^{n-1}q+\cdots+a_1pq^{n-1}+a_0q^n=0.

Move the constant-term part:

anpn+anβˆ’1pnβˆ’1q+β‹―+a1pqnβˆ’1=βˆ’a0qn.a_np^n+a_{n-1}p^{n-1}q+\cdots+a_1pq^{n-1}=-a_0q^n.

Every term on the left has a factor of pp, so

p∣a0qn.p\mid a_0q^n.

Since pq\frac{p}{q} is in lowest terms, gcd⁑(p,q)=1\gcd(p,q)=1. Therefore pp is relatively prime to qnq^n. If pp divides a0qna_0q^n and shares no factor with qnq^n, then

p∣a0.\boxed{p\mid a_0}.

For part (B), now move the leading-term part instead:

anβˆ’1pnβˆ’1q+β‹―+a1pqnβˆ’1+a0qn=βˆ’anpn.a_{n-1}p^{n-1}q+\cdots+a_1pq^{n-1}+a_0q^n=-a_np^n.

Every term on the left has a factor of qq, so

q∣anpn.q\mid a_np^n.

Since gcd⁑(p,q)=1\gcd(p,q)=1, qq is relatively prime to pnp^n. If qq divides anpna_np^n and shares no factor with pnp^n, then

q∣an.\boxed{q\mid a_n}.

For part (C), the theorem statement is this: If a polynomial with integer coefficients has a rational zero pq\frac{p}{q} in lowest terms, then the numerator must divide the constant term and the denominator must divide the leading coefficient.

p∣a0andq∣an.\boxed{p\mid a_0\quad\text{and}\quad q\mid a_n}.

Full notes β†’

  1. Let f(x)=3βˆ’2β‹…5x+1f(x)=3-2\cdot 5^{x+1}. State the domain, range, horizontal asymptote, intercepts, intervals of increase/decrease, and find an explicit formula for fβˆ’1(x)f^{-1}(x) with the domain and range of the inverse.
  2. The points (βˆ’1,17)(-1,17) and (2,1)(2,1) lie on the graph of g(x)=aβ‹…bxβˆ’h+kg(x)=a\cdot b^{x-h}+k. The horizontal asymptote is y=βˆ’1y=-1, and h=1h=1. Find aa and bb, then determine whether gg represents exponential growth or decay.
  3. Find all real solutions to 4x+1βˆ’10β‹…2x+1=04^{x+1}-10\cdot 2^x+1=0. Give exact answers.
  4. Solve in R\mathbb{R}: 32xβˆ’28β‹…3x+27≀03^{2x}-28\cdot 3^x+27\le 0. Write the answer in interval notation.
  5. Solve for xx exactly: 2x+1=52xβˆ’3.2^{x+1}=5^{2x-3}.
  6. Solve in R\mathbb{R}: ex+eβˆ’x=136.e^x+e^{-x}=\frac{13}{6}.
  7. Rewrite the following expression as a single logarithm with coefficient 11, and state the full domain of the original expression: 12ln⁑(x2βˆ’9)βˆ’2ln⁑(xβˆ’3)+ln⁑(x+1x).\frac12\ln(x^2-9)-2\ln(x-3)+\ln\left(\frac{x+1}{x}\right).
  8. Expand completely using logarithm properties, and state all restrictions on xx and yy: log⁑3(x4yβˆ’2(x2+1)3(5βˆ’y)).\log_3\left(\frac{x^4\sqrt{y-2}}{(x^2+1)^3(5-y)}\right).
  9. Solve in R\mathbb{R}: log⁑1/3(2xβˆ’1)β‰₯log⁑1/3(7βˆ’x).\log_{1/3}(2x-1)\ge \log_{1/3}(7-x).
  10. Solve in R\mathbb{R}: ln⁑(x2βˆ’5x+6)≀ln⁑(2x+3).\ln(x^2-5x+6)\le \ln(2x+3).
  11. Let h(x)=log⁑4(16βˆ’4x)βˆ’2h(x)=\log_4(16-4x)-2. State the domain, range, vertical asymptote, intercepts, intervals of increase/decrease, and find hβˆ’1(x)h^{-1}(x). Graph both equations.
  12. A population is modeled by P(t)=12001+19eβˆ’0.4tP(t)=\dfrac{1200}{1+19e^{-0.4t}} for tβ‰₯0t\ge 0. Find the initial population, the limiting population (aka horizontal asymptote), and the exact time when P(t)=900P(t)=900.
  13. Find the unique positive integer nn such that log⁑2(log⁑16n)=log⁑4(log⁑4n)\log_2 (\log_{16} n) = \log_4 (\log_4 n) (2020 AMC 12A).
  14. Let F(x)=ln⁑(xβˆ’abβˆ’x)F(x)=\ln\left(\dfrac{x-a}{b-x}\right), where a<ba<b. Find the domain, intercepts in terms of aa and bb, the vertical asymptotes, and an explicit formula for Fβˆ’1(x)F^{-1}(x). Then determine the range of FF.
  15. Find the exact value of the product ∏k=463log⁑k(5k2βˆ’1)log⁑k+1(5k2βˆ’4)\prod_{k=4}^{63}\frac{\log_k\left(5^{k^2-1}\right)}{\log_{k+1}\left(5^{k^2-4}\right)}. (Hint: Use change of base and cancel out things to simplify the expression) (2025 AIME II)
  16. (Bonus, The EML function)

Define a binary operation called EML⁑\operatorname{EML} by

EML⁑(x,y)=exβˆ’ln⁑y,\operatorname{EML}(x,y)=e^x-\ln y,

where y>0y>0.

(A)(A) First, show that EML contains the exponential function directly: ex=EML⁑(x,1).e^x=\operatorname{EML}(x,1).

(B)(B) Now show that EML also contains logarithms: EML⁑(0,x)=1βˆ’ln⁑x.\operatorname{EML}(0,x)=1-\ln x. Use this equation to solve for ln⁑x\ln x in terms of EML⁑(0,x)\operatorname{EML}(0,x).

(C)(C) Using part (B)(B), write log⁑bx\log_b x in terms of EML expressions, where b>0b>0, bβ‰ 1b\ne1, and x>0x>0.

(D)(D) Since EML can produce both exponentials and logarithms, it can also build simpler operations. Use the identities x+y=ln⁑(exey)x+y=\ln(e^x e^y) and xβˆ’y=ln⁑(exey)x-y=\ln\left(\frac{e^x}{e^y}\right) to write formulas for x+yx+y and xβˆ’yx-y using EML expressions.

(E)(E) An EML tree is an expression built by repeatedly feeding outputs of EML into new EML operations. For example, EML⁑(EML⁑(x,1),EML⁑(0,y))\operatorname{EML}\left(\operatorname{EML}(x,1),\operatorname{EML}(0,y)\right) is an EML tree. Draw its tree diagram, then simplify the expression as much as possible using exponent and logarithm rules.

(F)(F) It is claimed that EML trees can represent all standard elementary functions. In a short paragraph, compare this idea to the way a single NAND gate can generate all Boolean logic. A NAND gate outputs 00 only when both inputs are 11, and outputs 11 otherwise.

This problem is inspired by the paper All elementary functions from a single operator by Andrzej OdrzywoΕ‚ek. Learn more here: https://arxiv.org/html/2603.21852v2.


The domain is all real numbers:

(βˆ’βˆž,∞).\boxed{(-\infty,\infty)}.

Since 5x+1>05^{x+1}>0, we have βˆ’2β‹…5x+1<0-2\cdot 5^{x+1}<0, so

f(x)<3.f(x)<3.

Thus the range is

(βˆ’βˆž,3).\boxed{(-\infty,3)}.

The horizontal asymptote is

y=3.\boxed{y=3}.

The yy-intercept is

f(0)=3βˆ’2β‹…5=βˆ’7,f(0)=3-2\cdot 5=-7,

so the yy-intercept is

(0,βˆ’7).\boxed{(0,-7)}.

For the xx-intercept,

0=3βˆ’2β‹…5x+10=3-2\cdot 5^{x+1}

so

5x+1=32.5^{x+1}=\frac32.

Therefore

x+1=log⁑5(32),x+1=\log_5\left(\frac32\right),

so the xx-intercept is

(log⁑5(32)βˆ’1,0).\boxed{\left(\log_5\left(\frac32\right)-1,0\right)}.

Since 5x+15^{x+1} is increasing and the coefficient is negative, ff is decreasing on

(βˆ’βˆž,∞).\boxed{(-\infty,\infty)}.

It is never increasing.

To find the inverse, let

y=3βˆ’2β‹…5x+1.y=3-2\cdot 5^{x+1}.

Then

2β‹…5x+1=3βˆ’y,2\cdot 5^{x+1}=3-y,

so

5x+1=3βˆ’y2.5^{x+1}=\frac{3-y}{2}.

Take log⁑5\log_5 of both sides:

x+1=log⁑5(3βˆ’y2).x+1=\log_5\left(\frac{3-y}{2}\right).

Thus

x=log⁑5(3βˆ’y2)βˆ’1.x=\log_5\left(\frac{3-y}{2}\right)-1.

Switch xx and yy:

fβˆ’1(x)=log⁑5(3βˆ’x2)βˆ’1.\boxed{f^{-1}(x)=\log_5\left(\frac{3-x}{2}\right)-1}.

The domain of fβˆ’1f^{-1} is the range of ff:

(βˆ’βˆž,3).\boxed{(-\infty,3)}.

The range of fβˆ’1f^{-1} is the domain of ff:

(βˆ’βˆž,∞).\boxed{(-\infty,\infty)}.

Since the horizontal asymptote is y=βˆ’1y=-1 and h=1h=1, the function has the form

g(x)=aβ‹…bxβˆ’1βˆ’1.g(x)=a\cdot b^{x-1}-1.

Use the point (βˆ’1,17)(-1,17):

17=aβ‹…bβˆ’2βˆ’1.17=a\cdot b^{-2}-1.

So

ab2=18.\frac{a}{b^2}=18.

Use the point (2,1)(2,1):

1=aβ‹…b1βˆ’1.1=a\cdot b^{1}-1.

Thus

ab=2.ab=2.

From ab=2ab=2,

a=2b.a=\frac2b.

Substitute into ab2=18\frac{a}{b^2}=18:

2/bb2=18.\frac{2/b}{b^2}=18.

Then

2b3=18,\frac{2}{b^3}=18,

so

b3=19.b^3=\frac19.

Therefore

b=193=9βˆ’1/3.\boxed{b=\sqrt[3]{\frac19}=9^{-1/3}}.

Then

a=2b=293.a=\frac2b=2\sqrt[3]{9}.

So

a=293.\boxed{a=2\sqrt[3]{9}}.

Since 0<b<10<b<1 and a>0a>0, this represents

exponentialΒ decay.\boxed{\text{exponential decay}}.

Rewrite everything in terms of 2x2^x:

4x+1=4β‹…4x=4β‹…22x.4^{x+1}=4\cdot 4^x=4\cdot 2^{2x}.

So the equation becomes

4β‹…22xβˆ’10β‹…2x+1=0.4\cdot 2^{2x}-10\cdot 2^x+1=0.

Let

u=2x.u=2^x.

Then

4u2βˆ’10u+1=0.4u^2-10u+1=0.

Use the quadratic formula:

u=10Β±100βˆ’168=10Β±848=5Β±214.u=\frac{10\pm\sqrt{100-16}}{8} =\frac{10\pm\sqrt{84}}{8} =\frac{5\pm\sqrt{21}}{4}.

Both values are positive, so both are valid values of 2x2^x. Therefore

2x=5+214or2x=5βˆ’214.2^x=\frac{5+\sqrt{21}}{4} \qquad\text{or}\qquad 2^x=\frac{5-\sqrt{21}}{4}.

Thus

x=log⁑2(5+214)orx=log⁑2(5βˆ’214).\boxed{x=\log_2\left(\frac{5+\sqrt{21}}4\right) \quad\text{or}\quad x=\log_2\left(\frac{5-\sqrt{21}}4\right)}.

Let

u=3x.u=3^x.

Since 3x>03^x>0, we need u>0u>0. The inequality becomes

u2βˆ’28u+27≀0.u^2-28u+27\le 0.

Factor:

(uβˆ’1)(uβˆ’27)≀0.(u-1)(u-27)\le 0.

Thus

1≀u≀27.1\le u\le 27.

Substitute back:

1≀3x≀27.1\le 3^x\le 27.

Since 1=301=3^0 and 27=3327=3^3,

30≀3x≀33.3^0\le 3^x\le 3^3.

Because 3x3^x is increasing,

[0,3].\boxed{[0,3]}.

Take natural logs of both sides:

ln⁑(2x+1)=ln⁑(52xβˆ’3).\ln(2^{x+1})=\ln(5^{2x-3}).

Use the power rule:

(x+1)ln⁑2=(2xβˆ’3)ln⁑5.(x+1)\ln 2=(2x-3)\ln 5.

Expand:

xln⁑2+ln⁑2=2xln⁑5βˆ’3ln⁑5.x\ln 2+\ln 2=2x\ln 5-3\ln 5.

Move the xx terms to one side:

xln⁑2βˆ’2xln⁑5=βˆ’3ln⁑5βˆ’ln⁑2.x\ln 2-2x\ln 5=-3\ln 5-\ln 2.

Factor:

x(ln⁑2βˆ’2ln⁑5)=βˆ’(3ln⁑5+ln⁑2).x(\ln 2-2\ln 5)=-(3\ln 5+\ln 2).

Therefore

x=3ln⁑5+ln⁑22ln⁑5βˆ’ln⁑2.\boxed{x=\frac{3\ln 5+\ln 2}{2\ln 5-\ln 2}}.

Let

u=ex.u=e^x.

Then

eβˆ’x=1u.e^{-x}=\frac1u.

The equation becomes

u+1u=136.u+\frac1u=\frac{13}{6}.

Multiply by 6u6u:

6u2+6=13u.6u^2+6=13u.

So

6u2βˆ’13u+6=0.6u^2-13u+6=0.

Factor:

(3uβˆ’2)(2uβˆ’3)=0.(3u-2)(2u-3)=0.

Thus

u=23oru=32.u=\frac23 \qquad\text{or}\qquad u=\frac32.

Since u=exu=e^x,

ex=23orex=32.e^x=\frac23 \qquad\text{or}\qquad e^x=\frac32.

Therefore

x=ln⁑(23)orx=ln⁑(32).\boxed{x=\ln\left(\frac23\right) \quad\text{or}\quad x=\ln\left(\frac32\right)}.

Start with

12ln⁑(x2βˆ’9)βˆ’2ln⁑(xβˆ’3)+ln⁑(x+1x).\frac12\ln(x^2-9)-2\ln(x-3)+\ln\left(\frac{x+1}{x}\right).

Use the power rule:

ln⁑x2βˆ’9βˆ’ln⁑((xβˆ’3)2)+ln⁑(x+1x).\ln\sqrt{x^2-9}-\ln((x-3)^2)+\ln\left(\frac{x+1}{x}\right).

Combine the logarithms:

ln⁑(x2βˆ’9(x+1x)(xβˆ’3)2).\ln\left( \frac{\sqrt{x^2-9}\left(\frac{x+1}{x}\right)}{(x-3)^2} \right).

So the expression becomes

ln⁑((x+1)x2βˆ’9x(xβˆ’3)2).\boxed{\ln\left(\frac{(x+1)\sqrt{x^2-9}}{x(x-3)^2}\right)}.

Now find the domain of the original expression.

The first logarithm requires

x2βˆ’9>0,x^2-9>0,

so

x<βˆ’3orx>3.x<-3 \qquad\text{or}\qquad x>3.

The second logarithm requires

xβˆ’3>0,x-3>0,

so

x>3.x>3.

The third logarithm requires

x+1x>0,\frac{x+1}{x}>0,

so

x<βˆ’1orx>0.x<-1 \qquad\text{or}\qquad x>0.

The intersection is

x>3.\boxed{x>3}.

The expression is

log⁑3(x4yβˆ’2(x2+1)3(5βˆ’y)).\log_3\left(\frac{x^4\sqrt{y-2}}{(x^2+1)^3(5-y)}\right).

Use the quotient rule:

log⁑3(x4yβˆ’2)βˆ’log⁑3((x2+1)3(5βˆ’y)).\log_3(x^4\sqrt{y-2})-\log_3((x^2+1)^3(5-y)).

Use the product rule:

log⁑3(x4)+log⁑3(yβˆ’2)βˆ’log⁑3((x2+1)3)βˆ’log⁑3(5βˆ’y).\log_3(x^4)+\log_3(\sqrt{y-2})-\log_3((x^2+1)^3)-\log_3(5-y).

Use the power rule:

4log⁑3∣x∣+12log⁑3(yβˆ’2)βˆ’3log⁑3(x2+1)βˆ’log⁑3(5βˆ’y).\boxed{4\log_3\lvert x\rvert+\frac12\log_3(y-2)-3\log_3(x^2+1)-\log_3(5-y)}.

For restrictions, the square root requires

yβˆ’2β‰₯0.y-2\ge 0.

But the full logarithm cannot have input 00, so we need

y>2.y>2.

Also, the denominator must not be zero and the argument must be positive. Since x2+1>0x^2+1>0 always, we need

5βˆ’y>0,5-y>0,

so

y<5.y<5.

Finally, x4x^4 cannot be 00, so

x≠0.x\ne 0.

Thus the restrictions are

x≠0,2<y<5.\boxed{x\ne 0,\qquad 2<y<5}.

The domain requires

2xβˆ’1>0and7βˆ’x>0.2x-1>0 \qquad\text{and}\qquad 7-x>0.

So

12<x<7.\frac12<x<7.

The inequality is

log⁑1/3(2xβˆ’1)β‰₯log⁑1/3(7βˆ’x).\log_{1/3}(2x-1)\ge \log_{1/3}(7-x).

Since the base 13\frac13 is between 00 and 11, the logarithm is decreasing. Therefore the inequality reverses when we compare inputs:

2xβˆ’1≀7βˆ’x.2x-1\le 7-x.

Solve:

3x≀8,3x\le 8,

so

x≀83.x\le \frac83.

Intersect this with the domain 12<x<7\frac12<x<7:

(12,83].\boxed{\left(\frac12,\frac83\right]}.

First find the logarithm domain:

x2βˆ’5x+6>0x^2-5x+6>0

and

2x+3>0.2x+3>0.

Factor:

(xβˆ’2)(xβˆ’3)>0.(x-2)(x-3)>0.

Thus

x<2orx>3.x<2 \qquad\text{or}\qquad x>3.

Also,

x>βˆ’32.x>-\frac32.

So the domain is

(βˆ’32,2)βˆͺ(3,∞).\left(-\frac32,2\right)\cup(3,\infty).

Since ln⁑x\ln x is increasing,

ln⁑(x2βˆ’5x+6)≀ln⁑(2x+3)\ln(x^2-5x+6)\le \ln(2x+3)

is equivalent to

x2βˆ’5x+6≀2x+3x^2-5x+6\le 2x+3

inside the logarithm domain.

Simplify:

x2βˆ’7x+3≀0.x^2-7x+3\le 0.

The roots are

x=7Β±49βˆ’122=7Β±372.x=\frac{7\pm\sqrt{49-12}}{2} =\frac{7\pm\sqrt{37}}{2}.

Since the parabola opens upward,

7βˆ’372≀x≀7+372.\frac{7-\sqrt{37}}{2}\le x\le \frac{7+\sqrt{37}}{2}.

Intersect with the logarithm domain:

[7βˆ’372,2)βˆͺ(3,7+372].\boxed{\left[\frac{7-\sqrt{37}}2,2\right)\cup\left(3,\frac{7+\sqrt{37}}2\right]}.

The function is

h(x)=log⁑4(16βˆ’4x)βˆ’2.h(x)=\log_4(16-4x)-2.

The logarithm requires

16βˆ’4x>0.16-4x>0.

Thus

x<4,x<4,

so the domain is

(βˆ’βˆž,4).\boxed{(-\infty,4)}.

A logarithmic function can output every real number, so the range is

(βˆ’βˆž,∞).\boxed{(-\infty,\infty)}.

The vertical asymptote occurs where the logarithm input approaches 00:

16βˆ’4x=0.16-4x=0.

So the vertical asymptote is

x=4.\boxed{x=4}.

For the xx-intercept, set h(x)=0h(x)=0:

log⁑4(16βˆ’4x)βˆ’2=0.\log_4(16-4x)-2=0.

Then

log⁑4(16βˆ’4x)=2.\log_4(16-4x)=2.

So

16βˆ’4x=42=16.16-4x=4^2=16.

Thus

x=0.x=0.

The xx-intercept is

(0,0).\boxed{(0,0)}.

The yy-intercept is also

h(0)=log⁑4(16)βˆ’2=2βˆ’2=0,h(0)=\log_4(16)-2=2-2=0,

so the yy-intercept is

(0,0).\boxed{(0,0)}.

Since 16βˆ’4x16-4x decreases as xx increases and log⁑4x\log_4 x is increasing, hh is decreasing on

(βˆ’βˆž,4).\boxed{(-\infty,4)}.

It is never increasing.

Now find the inverse. Let

y=log⁑4(16βˆ’4x)βˆ’2.y=\log_4(16-4x)-2.

Then

y+2=log⁑4(16βˆ’4x).y+2=\log_4(16-4x).

Rewrite exponentially:

4y+2=16βˆ’4x.4^{y+2}=16-4x.

Then

4x=16βˆ’4y+2.4x=16-4^{y+2}.

So

x=4βˆ’4y+1.x=4-4^{y+1}.

Switch xx and yy:

hβˆ’1(x)=4βˆ’4x+1.\boxed{h^{-1}(x)=4-4^{x+1}}.

The inverse has domain (βˆ’βˆž,∞)(-\infty,\infty) and range (βˆ’βˆž,4)(-\infty,4). The graphs of hh and hβˆ’1h^{-1} are reflections across the line y=xy=x.

The graph of both functions are shown below (green = inverse function):

parent functions

The model is

P(t)=12001+19eβˆ’0.4t.P(t)=\frac{1200}{1+19e^{-0.4t}}.

The initial population is

P(0)=12001+19e0=120020=60.P(0)=\frac{1200}{1+19e^0} =\frac{1200}{20} =60.

So

P(0)=60.\boxed{P(0)=60}.

As tβ†’βˆžt\to\infty,

eβˆ’0.4tβ†’0.e^{-0.4t}\to 0.

Thus

P(t)β†’12001=1200.P(t)\to \frac{1200}{1}=1200.

So the limiting population is

1200.\boxed{1200}.

Now solve P(t)=900P(t)=900:

900=12001+19eβˆ’0.4t.900=\frac{1200}{1+19e^{-0.4t}}.

Then

900(1+19eβˆ’0.4t)=1200.900(1+19e^{-0.4t})=1200.

Divide by 300300:

3(1+19eβˆ’0.4t)=4.3(1+19e^{-0.4t})=4.

So

1+19eβˆ’0.4t=43.1+19e^{-0.4t}=\frac43.

Then

19eβˆ’0.4t=13.19e^{-0.4t}=\frac13.

Thus

eβˆ’0.4t=157.e^{-0.4t}=\frac1{57}.

Take natural logs:

βˆ’0.4t=ln⁑(157)=βˆ’ln⁑57.-0.4t=\ln\left(\frac1{57}\right)=-\ln 57.

Therefore

t=ln⁑570.4=52ln⁑57.t=\frac{\ln 57}{0.4} =\frac52\ln 57.

So

t=52ln⁑57.\boxed{t=\frac52\ln 57}.

Let

t=log⁑4n.t=\log_4 n.

Then

log⁑16n=log⁑4nlog⁑416=t2.\log_{16} n=\frac{\log_4 n}{\log_4 16} =\frac{t}{2}.

The equation becomes

log⁑2(t2)=log⁑4(t).\log_2\left(\frac{t}{2}\right)=\log_4(t).

Rewrite both sides in base 22:

log⁑2tβˆ’log⁑22=log⁑2tlog⁑24.\log_2 t-\log_2 2=\frac{\log_2 t}{\log_2 4}.

So

log⁑2tβˆ’1=12log⁑2t.\log_2 t-1=\frac12\log_2 t.

Then

12log⁑2t=1.\frac12\log_2 t=1.

Thus

log⁑2t=2,\log_2 t=2,

so

t=4.t=4.

Since t=log⁑4nt=\log_4 n,

log⁑4n=4.\log_4 n=4.

Therefore

n=44=256.\boxed{n=4^4=256}.

The function is

F(x)=ln⁑(xβˆ’abβˆ’x),F(x)=\ln\left(\frac{x-a}{b-x}\right),

where a<ba<b.

For the logarithm to be defined,

xβˆ’abβˆ’x>0.\frac{x-a}{b-x}>0.

Since a<ba<b, this happens exactly when

a<x<b.a<x<b.

So the domain is

(a,b).\boxed{(a,b)}.

For the xx-intercept, set F(x)=0F(x)=0:

ln⁑(xβˆ’abβˆ’x)=0.\ln\left(\frac{x-a}{b-x}\right)=0.

Then

xβˆ’abβˆ’x=1.\frac{x-a}{b-x}=1.

So

xβˆ’a=bβˆ’x.x-a=b-x.

Thus

2x=a+b,2x=a+b,

and

x=a+b2.x=\frac{a+b}{2}.

The xx-intercept is

(a+b2,0).\boxed{\left(\frac{a+b}{2},0\right)}.

The yy-intercept exists only if 00 is in the domain, meaning

a<0<b.a<0<b.

If this is true, then

F(0)=ln⁑(βˆ’ab).F(0)=\ln\left(\frac{-a}{b}\right).

So the yy-intercept is

(0,ln⁑(βˆ’ab))\boxed{\left(0,\ln\left(\frac{-a}{b}\right)\right)}

if a<0<ba<0<b. Otherwise, there is no yy-intercept.

The vertical asymptotes occur at the endpoints of the domain:

x=aandx=b.\boxed{x=a\quad\text{and}\quad x=b}.

Now find the inverse. Let

y=ln⁑(xβˆ’abβˆ’x).y=\ln\left(\frac{x-a}{b-x}\right).

Rewrite exponentially:

ey=xβˆ’abβˆ’x.e^y=\frac{x-a}{b-x}.

Multiply:

ey(bβˆ’x)=xβˆ’a.e^y(b-x)=x-a.

Expand:

beyβˆ’xey=xβˆ’a.be^y-xe^y=x-a.

Move the xx terms together:

bey+a=x+xey.be^y+a=x+xe^y.

Factor:

bey+a=x(1+ey).be^y+a=x(1+e^y).

Thus

x=a+bey1+ey.x=\frac{a+be^y}{1+e^y}.

Switch xx and yy:

Fβˆ’1(x)=a+bex1+ex.\boxed{F^{-1}(x)=\frac{a+be^x}{1+e^x}}.

As xx moves through (a,b)(a,b), the ratio xβˆ’abβˆ’x\frac{x-a}{b-x} moves through (0,∞)(0,\infty), so the logarithm moves through all real numbers. Therefore the range is

(βˆ’βˆž,∞).\boxed{(-\infty,\infty)}.

The product is

∏k=463log⁑k(5k2βˆ’1)log⁑k+1(5k2βˆ’4).\prod_{k=4}^{63}\frac{\log_k\left(5^{k^2-1}\right)}{\log_{k+1}\left(5^{k^2-4}\right)}.

Use change of base:

log⁑k(5k2βˆ’1)=(k2βˆ’1)ln⁑5ln⁑k,\log_k\left(5^{k^2-1}\right) =\frac{(k^2-1)\ln 5}{\ln k},

and

log⁑k+1(5k2βˆ’4)=(k2βˆ’4)ln⁑5ln⁑(k+1).\log_{k+1}\left(5^{k^2-4}\right) =\frac{(k^2-4)\ln 5}{\ln(k+1)}.

So each factor becomes

(k2βˆ’1)ln⁑5ln⁑k(k2βˆ’4)ln⁑5ln⁑(k+1)=k2βˆ’1k2βˆ’4β‹…ln⁑(k+1)ln⁑k.\frac{\frac{(k^2-1)\ln 5}{\ln k}}{\frac{(k^2-4)\ln 5}{\ln(k+1)}} =\frac{k^2-1}{k^2-4}\cdot\frac{\ln(k+1)}{\ln k}.

Factor the polynomials:

k2βˆ’1k2βˆ’4=(kβˆ’1)(k+1)(kβˆ’2)(k+2).\frac{k^2-1}{k^2-4} =\frac{(k-1)(k+1)}{(k-2)(k+2)}.

Thus the product is

∏k=463(kβˆ’1)(k+1)(kβˆ’2)(k+2)β‹…βˆk=463ln⁑(k+1)ln⁑k.\prod_{k=4}^{63} \frac{(k-1)(k+1)}{(k-2)(k+2)} \cdot \prod_{k=4}^{63}\frac{\ln(k+1)}{\ln k}.

First,

∏k=463kβˆ’1kβˆ’2=32β‹…43β‹…54β‹―6261=31.\prod_{k=4}^{63}\frac{k-1}{k-2} =\frac32\cdot\frac43\cdot\frac54\cdots\frac{62}{61} =31.

Also,

∏k=463k+1k+2=56β‹…67β‹…78β‹―6465=565=113.\prod_{k=4}^{63}\frac{k+1}{k+2} =\frac56\cdot\frac67\cdot\frac78\cdots\frac{64}{65} =\frac5{65} =\frac1{13}.

So the rational part is

31β‹…113=3113.31\cdot\frac1{13}=\frac{31}{13}.

The logarithm part telescopes:

∏k=463ln⁑(k+1)ln⁑k=ln⁑5ln⁑4β‹…ln⁑6ln⁑5β‹―ln⁑64ln⁑63=ln⁑64ln⁑4.\prod_{k=4}^{63}\frac{\ln(k+1)}{\ln k} =\frac{\ln 5}{\ln 4}\cdot\frac{\ln 6}{\ln 5}\cdots\frac{\ln 64}{\ln 63} =\frac{\ln 64}{\ln 4}.

Since 64=4364=4^3,

ln⁑64ln⁑4=3.\frac{\ln 64}{\ln 4}=3.

Therefore the product is

3113β‹…3=9313.\frac{31}{13}\cdot 3=\boxed{\frac{93}{13}}.

For part (A)(A),

EML⁑(x,1)=exβˆ’ln⁑1.\operatorname{EML}(x,1)=e^x-\ln 1.

Since ln⁑1=0\ln 1=0,

EML⁑(x,1)=ex.\operatorname{EML}(x,1)=e^x.

Thus

ex=EML⁑(x,1).\boxed{e^x=\operatorname{EML}(x,1)}.

For part (B)(B),

EML⁑(0,x)=e0βˆ’ln⁑x.\operatorname{EML}(0,x)=e^0-\ln x.

Since e0=1e^0=1,

EML⁑(0,x)=1βˆ’ln⁑x.\operatorname{EML}(0,x)=1-\ln x.

Solving for ln⁑x\ln x gives

ln⁑x=1βˆ’EML⁑(0,x).\boxed{\ln x=1-\operatorname{EML}(0,x)}.

For part (C)(C), use change of base:

log⁑bx=ln⁑xln⁑b.\log_b x=\frac{\ln x}{\ln b}.

Using part (B)(B),

ln⁑x=1βˆ’EML⁑(0,x)\ln x=1-\operatorname{EML}(0,x)

and

ln⁑b=1βˆ’EML⁑(0,b).\ln b=1-\operatorname{EML}(0,b).

Therefore

log⁑bx=1βˆ’EML⁑(0,x)1βˆ’EML⁑(0,b).\boxed{\log_b x=\frac{1-\operatorname{EML}(0,x)}{1-\operatorname{EML}(0,b)}}.

For part (D)(D), use

ex=EML⁑(x,1)e^x=\operatorname{EML}(x,1)

and

ln⁑z=1βˆ’EML⁑(0,z).\ln z=1-\operatorname{EML}(0,z).

Since

x+y=ln⁑(exey),x+y=\ln(e^xe^y),

we get

x+y=1βˆ’EML⁑(0,EML⁑(x,1)EML⁑(y,1)).\boxed{x+y=1-\operatorname{EML}\left(0,\operatorname{EML}(x,1)\operatorname{EML}(y,1)\right)}.

Similarly,

xβˆ’y=ln⁑(exey),x-y=\ln\left(\frac{e^x}{e^y}\right),

so

xβˆ’y=1βˆ’EML⁑(0,EML⁑(x,1)EML⁑(y,1)).\boxed{x-y=1-\operatorname{EML}\left(0,\frac{\operatorname{EML}(x,1)}{\operatorname{EML}(y,1)}\right)}.

For part (E)(E), the tree for

EML⁑(EML⁑(x,1),EML⁑(0,y))\operatorname{EML}\left(\operatorname{EML}(x,1),\operatorname{EML}(0,y)\right)

has a top EML node. Its left input is another EML node with inputs xx and 11. Its right input is another EML node with inputs 00 and yy.

In text form:

EML⁑(EML⁑(x,1),EML⁑(0,y)).\operatorname{EML} \left( \begin{array}{c} \operatorname{EML}(x,1),\\ \operatorname{EML}(0,y) \end{array} \right).

Now simplify:

EML⁑(x,1)=ex\operatorname{EML}(x,1)=e^x

and

EML⁑(0,y)=1βˆ’ln⁑y.\operatorname{EML}(0,y)=1-\ln y.

Therefore

EML⁑(EML⁑(x,1),EML⁑(0,y))=EML⁑(ex,1βˆ’ln⁑y).\operatorname{EML}\left(\operatorname{EML}(x,1),\operatorname{EML}(0,y)\right) =\operatorname{EML}(e^x,1-\ln y).

Using the definition of EML,

EML⁑(ex,1βˆ’ln⁑y)=eexβˆ’ln⁑(1βˆ’ln⁑y).\operatorname{EML}(e^x,1-\ln y) =e^{e^x}-\ln(1-\ln y).

So the expression simplifies to

eexβˆ’ln⁑(1βˆ’ln⁑y).\boxed{e^{e^x}-\ln(1-\ln y)}.

This requires

1βˆ’ln⁑y>0,1-\ln y>0,

so

0<y<e.0<y<e.

For part (F)(F), the comparison is that both EML and NAND are examples of a very small set of building blocks being powerful enough to generate a much larger system. A NAND gate alone can build NOT, AND, OR, and therefore all Boolean logic circuits. Similarly, the paper claims that EML, together with the constant 11, can be composed into trees that represent the standard elementary functions. In both cases, complicated expressions can be built from repeated uses of one simple operation.

Full notes β†’

  1. Let ΞΈ=βˆ’29Ο€6\theta=-\frac{29\pi}{6}.

    (A)(A) Find the least positive coterminal angle with ΞΈ\theta.

    (B)(B) Convert both angles to degrees.

    (C)(C) Find the reference angle and quadrant of ΞΈ\theta.

    (D)(D) Evaluate all six trigonometric functions of ΞΈ\theta exactly.

  2. A sector of a circle has perimeter 4040 cm and central angle 5Ο€6\frac{5\pi}{6}. Find the radius, arc length, and area of the sector exactly.

  3. A wheel of radius 1818 cm rotates counterclockwise at 4545 revolutions per minute. A bug starts at the point on the wheel closest to the ground. After 77 seconds, find the bug’s angle in standard position, its coordinates relative to the center of the wheel, and its linear speed in cm/sec.

  4. A pulley system has two wheels connected by a belt without slipping. Wheel A has radius 44 inches and rotates at 150150 revolutions per minute. Wheel B rotates at 6060 revolutions per minute. Find the radius of Wheel B. Then find the linear belt speed in inches per second.

  5. Let ΞΈ\theta be in Quadrant II and suppose tan⁑θ=βˆ’815\tan\theta=-\frac{8}{15}. Find exact values of sin⁑θ\sin\theta, cos⁑θ\cos\theta, sec⁑θ\sec\theta, csc⁑θ\csc\theta, and cot⁑θ\cot\theta. Then evaluate sin⁑(Ο€βˆ’ΞΈ)\sin(\pi-\theta) and cos⁑(ΞΈ+Ο€)\cos(\theta+\pi).

  6. Let P=(x,y)P=(x,y) be a point on the unit circle in Quadrant III. If xβˆ’y=22x-y=\frac{\sqrt2}{2}, find PP and the angle θ∈[0,2Ο€)\theta\in[0,2\pi) whose terminal side passes through PP.

  7. Evaluate exactly: 6sin⁑(βˆ’7Ο€6)βˆ’4cos⁑(11Ο€3)+3tan⁑(βˆ’13Ο€4)βˆ’2sec⁑(17Ο€6).6\sin\left(-\frac{7\pi}{6}\right)-4\cos\left(\frac{11\pi}{3}\right)+3\tan\left(-\frac{13\pi}{4}\right)-2\sec\left(\frac{17\pi}{6}\right).

  8. Solve exactly on [0,4Ο€)[0,4\pi): 2sin⁑2xβˆ’sin⁑xβˆ’1=0.2\sin^2x-\sin x-1=0.

  9. Solve exactly on [0,2Ο€)[0,2\pi):2cos⁑2x+3cos⁑xβˆ’1=0.2\cos^2x+\sqrt3\cos x-1=0.

  10. Solve exactly on [0,3Ο€)[0,3\pi):tan⁑2xβˆ’3=0.\tan^2x-3=0.

  11. The radius of the circle in the figure is 2 units. Express the length of DCDC in terms of Ξ±\alpha.

parent functions
  1. Prove the identity: 1βˆ’cos⁑θsin⁑θ+sin⁑θ1βˆ’cos⁑θ=2csc⁑θ.\frac{1-\cos\theta}{\sin\theta}+\frac{\sin\theta}{1-\cos\theta}=2\csc\theta. Then state all values of ΞΈ\theta in [0,2Ο€)[0,2\pi) for which the original identity is undefined.
  2. Prove the identity: 1βˆ’sin⁑2ΞΈ1+cotβ‘ΞΈβˆ’cos⁑2ΞΈ1+tan⁑θ=sin⁑θcos⁑θ.1-\frac{\sin^2\theta}{1+\cot\theta}-\frac{\cos^2\theta}{1+\tan\theta}=\sin\theta\cos\theta.
  3. For each of the following trigonometric expressions, find a segment in the diagram that has length equal to the trigonometric expression: sin⁑θ,cos⁑θ,sec⁑θ,csc⁑θ,tan⁑θ,cot⁑θ\sin\theta, \cos\theta, \sec\theta, \csc\theta, \tan\theta, \cot\theta. Note that you are not asked to express each trigonometric function in terms of multiple segments in the diagram. You must find a segment whose whole length equals the corresponding trig function. The graph is given below:
parent functions
  1. On [0,2Ο€)[0,2\pi), solve the equation numerically to three decimal places: 3sin⁑xβˆ’2cos⁑x=1.3\sin x-2\cos x=1. (Hint: Try the substitution t=tan⁑(x/2)t=\tan(x/2), and solve for xx using the tanβ‘βˆ’1\tan^{-1} button on the calculator.)
  2. (Bonus, rational points on the unit circle)

The unit circle is

x2+y2=1.x^2+y^2=1.

One obvious rational point on the unit circle is (βˆ’1,0)(-1,0). Now draw a line with rational slope mm through (βˆ’1,0)(-1,0):

y=m(x+1).y=m(x+1).

(A)(A) Substitute y=m(x+1)y=m(x+1) into x2+y2=1x^2+y^2=1 and show that the line intersects the unit circle at (βˆ’1,0)(-1,0) and one other point.

(B)(B) Find the coordinates of the second intersection point in terms of mm.

(C)(C) Explain why every rational value of mm gives a rational point on the unit circle.

(D)(D) Use your formula to find a rational point on the unit circle when m=23m=\frac23, then interpret that point as (cos⁑θ,sin⁑θ)(\cos\theta,\sin\theta) for some angle θ\theta.

(E)(E) Why does this method not produce the point (βˆ’1,0)(-1,0) as the second intersection point? What slope would be needed to reach the point (1,0)(1,0)?


Add multiples of 2Ο€2\pi to find a positive coterminal angle:

βˆ’29Ο€6+3(2Ο€)=βˆ’29Ο€6+36Ο€6=7Ο€6.-\frac{29\pi}{6}+3(2\pi) =-\frac{29\pi}{6}+\frac{36\pi}{6} =\frac{7\pi}{6}.

This is positive, but not least positive, since

7Ο€6βˆ’2Ο€=βˆ’5Ο€6<0.\frac{7\pi}{6}-2\pi=-\frac{5\pi}{6}<0.

So the least positive coterminal angle is

7Ο€6.\boxed{\frac{7\pi}{6}}.

Convert the original angle to degrees:

βˆ’29Ο€6β‹…180Ο€=βˆ’870∘.-\frac{29\pi}{6}\cdot\frac{180}{\pi} =-870^\circ.

Also,

7Ο€6β‹…180Ο€=210∘.\frac{7\pi}{6}\cdot\frac{180}{\pi} =210^\circ.

Thus

βˆ’29Ο€6=βˆ’870∘,7Ο€6=210∘.\boxed{-\frac{29\pi}{6}=-870^\circ,\qquad \frac{7\pi}{6}=210^\circ}.

The angle 7Ο€6\frac{7\pi}{6} is in Quadrant III, and its reference angle is

7Ο€6βˆ’Ο€=Ο€6.\frac{7\pi}{6}-\pi=\frac{\pi}{6}.

So

referenceΒ angleΒ =Ο€6,QuadrantΒ III.\boxed{\text{reference angle }=\frac{\pi}{6},\quad \text{Quadrant III}}.

Since ΞΈ\theta is coterminal with 7Ο€6\frac{7\pi}{6},

sin⁑θ=βˆ’12,cos⁑θ=βˆ’32,tan⁑θ=33.\sin\theta=-\frac12, \qquad \cos\theta=-\frac{\sqrt3}{2}, \qquad \tan\theta=\frac{\sqrt3}{3}.

The reciprocal functions are

csc⁑θ=βˆ’2,sec⁑θ=βˆ’233,cot⁑θ=3.\csc\theta=-2, \qquad \sec\theta=-\frac{2\sqrt3}{3}, \qquad \cot\theta=\sqrt3.

For a sector,

P=2r+s.P=2r+s.

Since s=rΞΈs=r\theta,

P=2r+rΞΈ=r(2+ΞΈ).P=2r+r\theta=r(2+\theta).

We are given P=40P=40 and ΞΈ=5Ο€6\theta=\frac{5\pi}{6}, so

40=r(2+5Ο€6).40=r\left(2+\frac{5\pi}{6}\right).

Thus

r=402+5Ο€6=24012+5Ο€.r=\frac{40}{2+\frac{5\pi}{6}} =\frac{240}{12+5\pi}.

So

r=24012+5π cm.\boxed{r=\frac{240}{12+5\pi}\text{ cm}}.

The arc length is

s=rΞΈ=24012+5Ο€β‹…5Ο€6=200Ο€12+5Ο€.s=r\theta =\frac{240}{12+5\pi}\cdot\frac{5\pi}{6} =\frac{200\pi}{12+5\pi}.

Thus

s=200Ο€12+5π cm.\boxed{s=\frac{200\pi}{12+5\pi}\text{ cm}}.

The sector area is

A=12r2ΞΈ.A=\frac12r^2\theta.

So

A=12(24012+5Ο€)2(5Ο€6)=24000Ο€(12+5Ο€)2.A=\frac12\left(\frac{240}{12+5\pi}\right)^2\left(\frac{5\pi}{6}\right) =\frac{24000\pi}{(12+5\pi)^2}.

Therefore

A=24000Ο€(12+5Ο€)2Β cm2.\boxed{A=\frac{24000\pi}{(12+5\pi)^2}\text{ cm}^2}.

The wheel rotates at

45Β rev/min=45(2Ο€)=90π rad/min.45\text{ rev/min}=45(2\pi)=90\pi\text{ rad/min}.

Convert to radians per second:

Ο‰=90Ο€60=3Ο€2Β rad/sec.\omega=\frac{90\pi}{60}=\frac{3\pi}{2}\text{ rad/sec}.

The bug starts at the point closest to the ground, so its starting angle is

3Ο€2.\frac{3\pi}{2}.

After 77 seconds, the angle swept out is

Ο‰t=3Ο€2(7)=21Ο€2.\omega t=\frac{3\pi}{2}(7)=\frac{21\pi}{2}.

The total angle is

3Ο€2+21Ο€2=24Ο€2=12Ο€.\frac{3\pi}{2}+\frac{21\pi}{2} =\frac{24\pi}{2} =12\pi.

This is coterminal with 00, so the bug is at

(18,0).\boxed{(18,0)}.

The angle in standard position is

0Β radians\boxed{0\text{ radians}}

after reducing coterminally.

The linear speed is

v=rω=18⋅3π2=27π.v=r\omega=18\cdot\frac{3\pi}{2}=27\pi.

Thus

v=27π cm/sec.\boxed{v=27\pi\text{ cm/sec}}.

Wheel A rotates at

150Β rev/min=300π rad/min.150\text{ rev/min}=300\pi\text{ rad/min}.

Its linear speed is

v=rΟ‰=4(300Ο€)=1200π in/min.v=r\omega=4(300\pi)=1200\pi\text{ in/min}.

The belt does not slip, so Wheel B has the same linear speed.

Wheel B rotates at

60Β rev/min=120π rad/min.60\text{ rev/min}=120\pi\text{ rad/min}.

So

1200Ο€=rB(120Ο€).1200\pi=r_B(120\pi).

Therefore

rB=10Β inches.\boxed{r_B=10\text{ inches}}.

Convert the belt speed to inches per second:

1200π in/min=1200Ο€60Β in/sec=20π in/sec.1200\pi\text{ in/min} =\frac{1200\pi}{60}\text{ in/sec} =20\pi\text{ in/sec}.

Thus

20π in/sec.\boxed{20\pi\text{ in/sec}}.

Since ΞΈ\theta is in Quadrant II and

tan⁑θ=βˆ’815,\tan\theta=-\frac{8}{15},

we can use a reference triangle with opposite side 88, adjacent side βˆ’15-15, and hypotenuse

82+152=17.\sqrt{8^2+15^2}=17.

Thus

sin⁑θ=817,cos⁑θ=βˆ’1517,tan⁑θ=βˆ’815.\boxed{\sin\theta=\frac8{17}}, \qquad \boxed{\cos\theta=-\frac{15}{17}}, \qquad \boxed{\tan\theta=-\frac8{15}}.

The reciprocal functions are

sec⁑θ=βˆ’1715,csc⁑θ=178,cot⁑θ=βˆ’158.\boxed{\sec\theta=-\frac{17}{15}}, \qquad \boxed{\csc\theta=\frac{17}{8}}, \qquad \boxed{\cot\theta=-\frac{15}{8}}.

Now,

sin⁑(Ο€βˆ’ΞΈ)=sin⁑θ=817.\sin(\pi-\theta)=\sin\theta=\frac8{17}.

Also,

cos⁑(ΞΈ+Ο€)=βˆ’cos⁑θ=1517.\cos(\theta+\pi)=-\cos\theta=\frac{15}{17}.

So

sin⁑(Ο€βˆ’ΞΈ)=817,cos⁑(ΞΈ+Ο€)=1517.\boxed{\sin(\pi-\theta)=\frac8{17}}, \qquad \boxed{\cos(\theta+\pi)=\frac{15}{17}}.

Since P=(x,y)P=(x,y) is on the unit circle,

x2+y2=1.x^2+y^2=1.

We are also given

xβˆ’y=22.x-y=\frac{\sqrt2}{2}.

So

y=xβˆ’22.y=x-\frac{\sqrt2}{2}.

Substitute:

x2+(xβˆ’22)2=1.x^2+\left(x-\frac{\sqrt2}{2}\right)^2=1.

Expand:

x2+x2βˆ’2x+12=1.x^2+x^2-\sqrt2x+\frac12=1.

Thus

2x2βˆ’2xβˆ’12=0.2x^2-\sqrt2x-\frac12=0.

Multiply by 22:

4x2βˆ’22xβˆ’1=0.4x^2-2\sqrt2x-1=0.

Use the quadratic formula:

x=22Β±8+168=22Β±268=2Β±64.x=\frac{2\sqrt2\pm\sqrt{8+16}}{8} =\frac{2\sqrt2\pm2\sqrt6}{8} =\frac{\sqrt2\pm\sqrt6}{4}.

Since the point is in Quadrant III, x<0x<0. Therefore

x=2βˆ’64.x=\frac{\sqrt2-\sqrt6}{4}.

Then

y=xβˆ’22=2βˆ’64βˆ’224=βˆ’2+64.y=x-\frac{\sqrt2}{2} =\frac{\sqrt2-\sqrt6}{4}-\frac{2\sqrt2}{4} =-\frac{\sqrt2+\sqrt6}{4}.

So

P=(2βˆ’64,βˆ’2+64).\boxed{P=\left(\frac{\sqrt2-\sqrt6}{4},-\frac{\sqrt2+\sqrt6}{4}\right)}.

This is the unit-circle point for

ΞΈ=17Ο€12.\boxed{\theta=\frac{17\pi}{12}}.

Equivalently, ΞΈβ‰ˆ4.451\theta\approx4.451 radians.

Use coterminal angles:

sin⁑(βˆ’7Ο€6)=sin⁑(5Ο€6)=12.\sin\left(-\frac{7\pi}{6}\right)=\sin\left(\frac{5\pi}{6}\right)=\frac12.

Also,

cos⁑(11Ο€3)=cos⁑(5Ο€3)=12.\cos\left(\frac{11\pi}{3}\right)=\cos\left(\frac{5\pi}{3}\right)=\frac12.

Next,

tan⁑(βˆ’13Ο€4)=tan⁑(3Ο€4)=βˆ’1.\tan\left(-\frac{13\pi}{4}\right)=\tan\left(\frac{3\pi}{4}\right)=-1.

Finally,

sec⁑(17Ο€6)=sec⁑(5Ο€6)=1βˆ’32=βˆ’233.\sec\left(\frac{17\pi}{6}\right)=\sec\left(\frac{5\pi}{6}\right) =\frac1{-\frac{\sqrt3}{2}} =-\frac{2\sqrt3}{3}.

Substitute:

6(12)βˆ’4(12)+3(βˆ’1)βˆ’2(βˆ’233).6\left(\frac12\right) -4\left(\frac12\right) +3(-1) -2\left(-\frac{2\sqrt3}{3}\right).

This becomes

3βˆ’2βˆ’3+433.3-2-3+\frac{4\sqrt3}{3}.

Therefore

βˆ’2+433.\boxed{-2+\frac{4\sqrt3}{3}}.

Let

u=sin⁑x.u=\sin x.

Then

2u2βˆ’uβˆ’1=0.2u^2-u-1=0.

Factor:

(2u+1)(uβˆ’1)=0.(2u+1)(u-1)=0.

Thus

sin⁑x=1orsin⁑x=βˆ’12.\sin x=1 \qquad\text{or}\qquad \sin x=-\frac12.

On [0,4Ο€)[0,4\pi), sin⁑x=1\sin x=1 at

x=Ο€2,5Ο€2.x=\frac{\pi}{2},\frac{5\pi}{2}.

Also, sin⁑x=βˆ’12\sin x=-\frac12 at

x=7Ο€6,11Ο€6,19Ο€6,23Ο€6.x=\frac{7\pi}{6},\frac{11\pi}{6},\frac{19\pi}{6},\frac{23\pi}{6}.

Therefore

x=Ο€2,7Ο€6,11Ο€6,5Ο€2,19Ο€6,23Ο€6.\boxed{x=\frac{\pi}{2},\frac{7\pi}{6},\frac{11\pi}{6},\frac{5\pi}{2},\frac{19\pi}{6},\frac{23\pi}{6}}.

Let

u=cos⁑x.u=\cos x.

Then

2u2+3uβˆ’1=0.2u^2+\sqrt3u-1=0.

Use the quadratic formula:

u=βˆ’3Β±3+84=βˆ’3Β±114.u=\frac{-\sqrt3\pm\sqrt{3+8}}{4} =\frac{-\sqrt3\pm\sqrt{11}}{4}.

The value

βˆ’3βˆ’114\frac{-\sqrt3-\sqrt{11}}{4}

is less than βˆ’1-1, so it is impossible for cos⁑x\cos x. Thus

cos⁑x=11βˆ’34.\cos x=\frac{\sqrt{11}-\sqrt3}{4}.

On [0,2Ο€)[0,2\pi), cosine is positive in Quadrants I and IV, so

x=cosβ‘βˆ’1(11βˆ’34)orx=2Ο€βˆ’cosβ‘βˆ’1(11βˆ’34).\boxed{x=\cos^{-1}\left(\frac{\sqrt{11}-\sqrt3}{4}\right) \quad\text{or}\quad x=2\pi-\cos^{-1}\left(\frac{\sqrt{11}-\sqrt3}{4}\right)}.

We have

tan⁑2xβˆ’3=0.\tan^2x-3=0.

So

tan⁑2x=3,\tan^2x=3,

which gives

tan⁑x=±3.\tan x=\pm\sqrt3.

The tangent function has period Ο€\pi. On [0,3Ο€)[0,3\pi), the solutions are

x=Ο€3,2Ο€3,4Ο€3,5Ο€3,7Ο€3,8Ο€3.\boxed{x=\frac{\pi}{3},\frac{2\pi}{3},\frac{4\pi}{3},\frac{5\pi}{3},\frac{7\pi}{3},\frac{8\pi}{3}}.

The radius of the circle is 22, and CC is the point on the positive xx-axis at the right edge of the circle. Thus

OC=2.OC=2.

The ray from OO through BB and DD makes angle Ξ±\alpha with the positive xx-axis. In right triangle ODCODC,

tan⁑α=DCOC.\tan\alpha=\frac{DC}{OC}.

Substitute OC=2OC=2:

tan⁑α=DC2.\tan\alpha=\frac{DC}{2}.

Therefore

DC=2tan⁑α.\boxed{DC=2\tan\alpha}.

Start with the left-hand side:

1βˆ’cos⁑θsin⁑θ+sin⁑θ1βˆ’cos⁑θ.\frac{1-\cos\theta}{\sin\theta}+\frac{\sin\theta}{1-\cos\theta}.

Use the common denominator sin⁑θ(1βˆ’cos⁑θ)\sin\theta(1-\cos\theta):

(1βˆ’cos⁑θ)2+sin⁑2ΞΈsin⁑θ(1βˆ’cos⁑θ).\frac{(1-\cos\theta)^2+\sin^2\theta}{\sin\theta(1-\cos\theta)}.

Expand the numerator:

1βˆ’2cos⁑θ+cos⁑2ΞΈ+sin⁑2ΞΈ.1-2\cos\theta+\cos^2\theta+\sin^2\theta.

Use sin⁑2θ+cos⁑2θ=1\sin^2\theta+\cos^2\theta=1:

1βˆ’2cos⁑θ+cos⁑2ΞΈ+sin⁑2ΞΈ=2βˆ’2cos⁑θ.1-2\cos\theta+\cos^2\theta+\sin^2\theta =2-2\cos\theta.

So the expression becomes

2βˆ’2cos⁑θsin⁑θ(1βˆ’cos⁑θ).\frac{2-2\cos\theta}{\sin\theta(1-\cos\theta)}.

Factor:

2(1βˆ’cos⁑θ)sin⁑θ(1βˆ’cos⁑θ).\frac{2(1-\cos\theta)}{\sin\theta(1-\cos\theta)}.

Cancel:

2sin⁑θ=2csc⁑θ.\frac2{\sin\theta}=2\csc\theta.

Therefore

1βˆ’cos⁑θsin⁑θ+sin⁑θ1βˆ’cos⁑θ=2csc⁑θ.\boxed{\frac{1-\cos\theta}{\sin\theta}+\frac{\sin\theta}{1-\cos\theta}=2\csc\theta}.

The original expression is undefined when

sin⁑θ=0\sin\theta=0

or

1βˆ’cos⁑θ=0.1-\cos\theta=0.

On [0,2Ο€)[0,2\pi), this happens at

ΞΈ=0,Ο€.\boxed{\theta=0,\pi}.

Start with the left-hand side:

1βˆ’sin⁑2ΞΈ1+cotβ‘ΞΈβˆ’cos⁑2ΞΈ1+tan⁑θ.1-\frac{\sin^2\theta}{1+\cot\theta}-\frac{\cos^2\theta}{1+\tan\theta}.

Rewrite cotangent and tangent using sine and cosine:

1βˆ’sin⁑2ΞΈ1+cos⁑θsinβ‘ΞΈβˆ’cos⁑2ΞΈ1+sin⁑θcos⁑θ.1-\frac{\sin^2\theta}{1+\frac{\cos\theta}{\sin\theta}}-\frac{\cos^2\theta}{1+\frac{\sin\theta}{\cos\theta}}.

Simplify the denominators:

1+cos⁑θsin⁑θ=sin⁑θ+cos⁑θsin⁑θ1+\frac{\cos\theta}{\sin\theta}=\frac{\sin\theta+\cos\theta}{\sin\theta}

and

1+sin⁑θcos⁑θ=sin⁑θ+cos⁑θcos⁑θ.1+\frac{\sin\theta}{\cos\theta}=\frac{\sin\theta+\cos\theta}{\cos\theta}.

So the expression becomes

1βˆ’sin⁑3ΞΈsin⁑θ+cosβ‘ΞΈβˆ’cos⁑3ΞΈsin⁑θ+cos⁑θ.1-\frac{\sin^3\theta}{\sin\theta+\cos\theta}-\frac{\cos^3\theta}{\sin\theta+\cos\theta}.

Combine the fractions:

1βˆ’sin⁑3ΞΈ+cos⁑3ΞΈsin⁑θ+cos⁑θ.1-\frac{\sin^3\theta+\cos^3\theta}{\sin\theta+\cos\theta}.

Use the sum of cubes formula:

a3+b3=(a+b)(a2βˆ’ab+b2).a^3+b^3=(a+b)(a^2-ab+b^2).

Then

sin⁑3ΞΈ+cos⁑3ΞΈ=(sin⁑θ+cos⁑θ)(sin⁑2ΞΈβˆ’sin⁑θcos⁑θ+cos⁑2ΞΈ).\sin^3\theta+\cos^3\theta=(\sin\theta+\cos\theta)(\sin^2\theta-\sin\theta\cos\theta+\cos^2\theta).

Cancel the common factor:

1βˆ’(sin⁑2ΞΈβˆ’sin⁑θcos⁑θ+cos⁑2ΞΈ).1-(\sin^2\theta-\sin\theta\cos\theta+\cos^2\theta).

Since

sin⁑2θ+cos⁑2θ=1,\sin^2\theta+\cos^2\theta=1,

this becomes

1βˆ’(1βˆ’sin⁑θcos⁑θ)=sin⁑θcos⁑θ.1-(1-\sin\theta\cos\theta)=\sin\theta\cos\theta.

Therefore,

1βˆ’sin⁑2ΞΈ1+cotβ‘ΞΈβˆ’cos⁑2ΞΈ1+tan⁑θ=sin⁑θcos⁑θ.\boxed{1-\frac{\sin^2\theta}{1+\cot\theta}-\frac{\cos^2\theta}{1+\tan\theta}=\sin\theta\cos\theta}.

In the diagram, the circle is the unit circle and A=(cos⁑θ,sin⁑θ)A=(\cos\theta,\sin\theta).

The horizontal segment from the origin to the foot under AA is

OC=cos⁑θ.\boxed{OC=\cos\theta}.

The vertical segment from the xx-axis up to AA is

AC=sin⁑θ.\boxed{AC=\sin\theta}.

The line through AA is tangent to the unit circle. Its equation is

xcos⁑θ+ysin⁑θ=1.x\cos\theta+y\sin\theta=1.

At the xx-intercept, y=0y=0, so

xcos⁑θ=1x\cos\theta=1

and

x=sec⁑θ.x=\sec\theta.

Thus

OD=sec⁑θ.\boxed{OD=\sec\theta}.

At the yy-intercept, x=0x=0, so

ysin⁑θ=1y\sin\theta=1

and

y=csc⁑θ.y=\csc\theta.

Thus

OB=csc⁑θ.\boxed{OB=\csc\theta}.

The tangent segment from AA to DD has length

AD=(secβ‘ΞΈβˆ’cos⁑θ)2+(0βˆ’sin⁑θ)2.AD=\sqrt{(\sec\theta-\cos\theta)^2+(0-\sin\theta)^2}.

Since

secβ‘ΞΈβˆ’cos⁑θ=1cosβ‘ΞΈβˆ’cos⁑θ=1βˆ’cos⁑2ΞΈcos⁑θ=sin⁑2ΞΈcos⁑θ,\sec\theta-\cos\theta =\frac1{\cos\theta}-\cos\theta =\frac{1-\cos^2\theta}{\cos\theta} =\frac{\sin^2\theta}{\cos\theta},

this length simplifies to tan⁑θ\tan\theta in the first-quadrant diagram. Therefore

AD=tan⁑θ.\boxed{AD=\tan\theta}.

The tangent segment from AA to BB has length

AB=(0βˆ’cos⁑θ)2+(cscβ‘ΞΈβˆ’sin⁑θ)2.AB=\sqrt{(0-\cos\theta)^2+(\csc\theta-\sin\theta)^2}.

Similarly,

cscβ‘ΞΈβˆ’sin⁑θ=1sinβ‘ΞΈβˆ’sin⁑θ=cos⁑2ΞΈsin⁑θ,\csc\theta-\sin\theta =\frac1{\sin\theta}-\sin\theta =\frac{\cos^2\theta}{\sin\theta},

so this length simplifies to cot⁑θ\cot\theta in the first-quadrant diagram. Therefore

AB=cot⁑θ.\boxed{AB=\cot\theta}.

So the six matching segments are

sin⁑θ=AC,cos⁑θ=OC,sec⁑θ=OD,csc⁑θ=OB,tan⁑θ=AD,cot⁑θ=AB.\boxed{\sin\theta=AC,\quad \cos\theta=OC,\quad \sec\theta=OD,\quad \csc\theta=OB,\quad \tan\theta=AD,\quad \cot\theta=AB}.

Use the substitution

t=tan⁑x2.t=\tan\frac{x}{2}.

Then

sin⁑x=2t1+t2\sin x=\frac{2t}{1+t^2}

and

cos⁑x=1βˆ’t21+t2.\cos x=\frac{1-t^2}{1+t^2}.

Substitute into

3sin⁑xβˆ’2cos⁑x=1.3\sin x-2\cos x=1.

This gives

3(2t1+t2)βˆ’2(1βˆ’t21+t2)=1.3\left(\frac{2t}{1+t^2}\right)-2\left(\frac{1-t^2}{1+t^2}\right)=1.

Multiply by 1+t21+t^2:

6tβˆ’2(1βˆ’t2)=1+t2.6t-2(1-t^2)=1+t^2.

Expand:

6tβˆ’2+2t2=1+t2.6t-2+2t^2=1+t^2.

Rearrange:

t2+6tβˆ’3=0.t^2+6t-3=0.

Use the quadratic formula:

t=βˆ’6Β±36+122=βˆ’3Β±23.t=\frac{-6\pm\sqrt{36+12}}{2} =-3\pm2\sqrt3.

So

tan⁑x2=βˆ’3+23\tan\frac{x}{2}=-3+2\sqrt3

or

tan⁑x2=βˆ’3βˆ’23.\tan\frac{x}{2}=-3-2\sqrt3.

Using a calculator and choosing values of xx in [0,2Ο€)[0,2\pi) gives

xβ‰ˆ0.869orxβ‰ˆ3.450.\boxed{x\approx0.869\quad\text{or}\quad x\approx3.450}.

For part (A)(A), substitute

y=m(x+1)y=m(x+1)

into

x2+y2=1.x^2+y^2=1.

This gives

x2+m2(x+1)2=1.x^2+m^2(x+1)^2=1.

Expand:

x2+m2(x2+2x+1)=1.x^2+m^2(x^2+2x+1)=1.

So

(1+m2)x2+2m2x+m2βˆ’1=0.(1+m^2)x^2+2m^2x+m^2-1=0.

Since x=βˆ’1x=-1 is one solution, factor:

(x+1)((1+m2)x+(m2βˆ’1))=0.(x+1)\left((1+m^2)x+(m^2-1)\right)=0.

Therefore the line intersects the circle at (βˆ’1,0)(-1,0) and one other point.

For part (B)(B), the second point comes from

(1+m2)x+(m2βˆ’1)=0.(1+m^2)x+(m^2-1)=0.

Thus

x=1βˆ’m21+m2.x=\frac{1-m^2}{1+m^2}.

Now plug into y=m(x+1)y=m(x+1):

y=m(1βˆ’m21+m2+1).y=m\left(\frac{1-m^2}{1+m^2}+1\right).

Simplify:

y=m(1βˆ’m2+1+m21+m2)=m(21+m2)=2m1+m2.y=m\left(\frac{1-m^2+1+m^2}{1+m^2}\right) =m\left(\frac{2}{1+m^2}\right) =\frac{2m}{1+m^2}.

So the second intersection point is

(1βˆ’m21+m2,2m1+m2).\boxed{\left(\frac{1-m^2}{1+m^2},\frac{2m}{1+m^2}\right)}.

For part (C)(C), if mm is rational, then m2m^2 is rational. The expressions

1βˆ’m21+m2and2m1+m2\frac{1-m^2}{1+m^2} \qquad\text{and}\qquad \frac{2m}{1+m^2}

are made from rational numbers using addition, subtraction, multiplication, and division. Therefore both coordinates are rational.

For part (D)(D), use m=23m=\frac23:

x=1βˆ’(23)21+(23)2=1βˆ’491+49=59139=513.x=\frac{1-\left(\frac23\right)^2}{1+\left(\frac23\right)^2} =\frac{1-\frac49}{1+\frac49} =\frac{\frac59}{\frac{13}{9}} =\frac5{13}.

Also,

y=2(23)1+(23)2=43139=1213.y=\frac{2\left(\frac23\right)}{1+\left(\frac23\right)^2} =\frac{\frac43}{\frac{13}{9}} =\frac{12}{13}.

So the rational point is

(513,1213).\boxed{\left(\frac5{13},\frac{12}{13}\right)}.

This means there is an angle ΞΈ\theta such that

cos⁑θ=513,sin⁑θ=1213.\boxed{\cos\theta=\frac5{13},\qquad \sin\theta=\frac{12}{13}}.

For part (E)(E), this method does not produce (βˆ’1,0)(-1,0) as the second intersection point because (βˆ’1,0)(-1,0) is the fixed point used to build every line. A finite nonvertical slope through (βˆ’1,0)(-1,0) intersects the circle at exactly one other point.

To reach (1,0)(1,0), the line must be the xx-axis, which has slope

m=0.\boxed{m=0}.

Full notes β†’

  1. For f(x)=βˆ’3sin⁑(2(xβˆ’Ο€6))+1f(x)=-3\sin\left(2\left(x-\frac{\pi}{6}\right)\right)+1, find the amplitude, period, phase shift, midline, range, and five key points for one full period. Then sketch one full period.
  2. A sinusoidal function has maximum value 77 at x=Ο€3x=\frac{\pi}{3} and minimum value βˆ’1-1 at x=7Ο€6x=\frac{7\pi}{6}. Write a cosine model for the function, assuming the given maximum and minimum are consecutive. Then find five key points and sketch one full period.
  3. For g(x)=2tan⁑(3(x+Ο€12))βˆ’1g(x)=2\tan\left(3\left(x+\frac{\pi}{12}\right)\right)-1, find the period, center point of one branch, vertical asymptotes surrounding that branch, and the xx-intercept in that branch. Then sketch the branch.
  4. For h(x)=βˆ’2sec⁑(12(xβˆ’Ο€))+3h(x)=-2\sec\left(\frac12(x-\pi)\right)+3, find the period, midline, vertical asymptotes in one period starting at x=Ο€x=\pi, and range. Then sketch one full period, including the guiding cosine curve.
  5. Solve exactly on [0,4Ο€)[0,4\pi). Then sketch y=2sin⁑2xβˆ’sin⁑xβˆ’1y=2\sin^2x-\sin x-1 on [0,4Ο€)[0,4\pi) and label all xx-intercepts: 2sin⁑2xβˆ’sin⁑xβˆ’1=0.2\sin^2x-\sin x-1=0.
  6. Solve on [0,4Ο€)[0, 4\pi): 4sin⁑(4x)cos⁑(6x)=2sin⁑(10x)+14\sin(4x)\cos(6x)= 2\sin(10x)+1.
  7. Solve exactly on [0,2Ο€)[0,2\pi): tan⁑x+cot⁑x=4.\tan x+\cot x=4.
  8. Evaluate each of these exactly: sin⁑75∘,cos⁑15∘,tan⁑105∘.\sin 75^\circ, \cos 15^\circ,\tan 105^\circ. The sine and cosine values for 15∘15^\circ and 75∘75^\circ are also useful to memorize as well.
  9. Prove the identity: sin⁑(x+y)+sin⁑(xβˆ’y)cos⁑(x+y)+cos⁑(xβˆ’y)=tan⁑x.\frac{\sin(x+y)+\sin(x-y)}{\cos(x+y)+\cos(x-y)}=\tan x.
  10. Solve exactly on [0,2Ο€)[0,2\pi). Then use the product-to-sum form to sketch enough of the graph to explain why your number of solutions makes sense: cos⁑(5x)+cos⁑(3x)=0.\cos(5x)+\cos(3x)=0.
  11. Evaluate exactly: sin⁑(cosβ‘βˆ’135)+cos⁑(sinβ‘βˆ’1(βˆ’513))+tan⁑(cosβ‘βˆ’1(βˆ’45)).\sin\left(\cos^{-1}\frac35\right)+\cos\left(\sin^{-1}\left(-\frac5{13}\right)\right)+\tan\left(\cos^{-1}\left(-\frac45\right)\right).
  12. How many solutions does the equation tan⁑(2x)=cos⁑(x2)\tan(2x)=\cos(\tfrac{x}{2}) have on the interval [0,2Ο€][0,2\pi]?
  13. Suppose Ο€2<ΞΈ<Ο€\frac{\pi}{2}<\theta<\pi and cos⁑θ=βˆ’35\cos\theta=-\frac35. Find exact values of sin⁑(ΞΈ2),cos⁑(ΞΈ2),\sin\left(\frac{\theta}{2}\right), \cos\left(\frac{\theta}{2}\right), and tan⁑(ΞΈ2).\tan\left(\frac{\theta}{2}\right).
  14. Let xx and yy be real numbers such that sin⁑xsin⁑y=3\frac{\sin x}{\sin y} = 3 and cos⁑xcos⁑y=12\frac{\cos x}{\cos y} = \frac{1}{2}. The value of sin⁑2xsin⁑2y+cos⁑2xcos⁑2y\frac{\sin 2x}{\sin 2y} + \frac{\cos 2x}{\cos 2y} can be expressed in the form pq\frac{p}{q}, where pp and qq are relatively prime positive integers. Find p+qp+q. (2014 AIME II)
  15. A tide height is modeled by a sinusoidal function of time. At t=2t=2 hours, the tide is at a high of 1111 feet. At t=8t=8 hours, the tide is at the next low of 33 feet.

(A)(A) Write a cosine model H(t)H(t) for the tide height.

(B)(B) Find the period and midline.

(C)(C) Find the first time after t=2t=2 when the tide height is 99 feet.

(D)(D) Sketch one full period of the tide model and label the high tide, low tide, midline, and the point where H(t)=9H(t)=9 first occurs after t=2t=2.

  1. (Bonus, ViΓ¨te’s formula for Ο€\pi)

Let

a1=2a_1=\sqrt2

and define

an+1=2+an.a_{n+1}=\sqrt{2+a_n}.

The nested radicals

2,2+2,2+2+2,…\sqrt2,\quad \sqrt{2+\sqrt2},\quad \sqrt{2+\sqrt{2+\sqrt2}},\quad \ldots

are connected to repeated half-angle identities.

(A)(A) Use the half-angle identity for cosine to show that

an=2cos⁑(Ο€2n+1).a_n=2\cos\left(\frac{\pi}{2^{n+1}}\right).

(B)(B) Use part (A)(A) and the identity sin⁑(2x)=2sin⁑xcos⁑x\sin(2x)=2\sin x\cos x to show how products of the terms an2\frac{a_n}{2} are related to 2Ο€\frac{2}{\pi}.

(C)(C) Explain why this leads to ViΓ¨te’s infinite product:

2Ο€=22β‹…2+22β‹…2+2+22⋯ .\frac{2}{\pi} =\frac{\sqrt2}{2}\cdot \frac{\sqrt{2+\sqrt2}}{2}\cdot \frac{\sqrt{2+\sqrt{2+\sqrt2}}}{2}\cdots.

The function is

f(x)=βˆ’3sin⁑(2(xβˆ’Ο€6))+1.f(x)=-3\sin\left(2\left(x-\frac{\pi}{6}\right)\right)+1.

The amplitude is

3.\boxed{3}.

The period is

2Ο€βˆ£2∣=Ο€.\frac{2\pi}{\lvert 2 \rvert}=\pi.

So

period=Ο€.\boxed{\text{period}=\pi}.

The phase shift is

Ο€6Β right.\boxed{\frac{\pi}{6}\text{ right}}.

The midline is

y=1.\boxed{y=1}.

The range is

1βˆ’3≀y≀1+3,1-3\le y\le 1+3,

so

[βˆ’2,4].\boxed{[-2,4]}.

The key-point increment is one fourth of the period:

Ο€4.\frac{\pi}{4}.

Starting at x=Ο€6x=\frac{\pi}{6}, the five key xx-values are

Ο€6,5Ο€12,2Ο€3,11Ο€12,7Ο€6.\frac{\pi}{6},\quad \frac{5\pi}{12},\quad \frac{2\pi}{3},\quad \frac{11\pi}{12},\quad \frac{7\pi}{6}.

Because the sine graph is reflected over the xx-axis, the corresponding yy-values are

1,βˆ’2,1,4,1.1,\quad -2,\quad 1,\quad 4,\quad 1.

Thus the five key points are

(Ο€6,1),(5Ο€12,βˆ’2),(2Ο€3,1),(11Ο€12,4),(7Ο€6,1).\boxed{\left(\frac{\pi}{6},1\right), \left(\frac{5\pi}{12},-2\right), \left(\frac{2\pi}{3},1\right), \left(\frac{11\pi}{12},4\right), \left(\frac{7\pi}{6},1\right)}.

A graph with many key points is shown below:

parent functions

The maximum is 77 and the minimum is βˆ’1-1. The midline is the average:

D=7+(βˆ’1)2=3.D=\frac{7+(-1)}{2}=3.

The amplitude is half the distance between max and min:

A=7βˆ’(βˆ’1)2=4.A=\frac{7-(-1)}{2}=4.

The distance from a maximum to the next minimum is half a period:

7Ο€6βˆ’Ο€3=7Ο€6βˆ’2Ο€6=5Ο€6.\frac{7\pi}{6}-\frac{\pi}{3} =\frac{7\pi}{6}-\frac{2\pi}{6} =\frac{5\pi}{6}.

So the period is

2β‹…5Ο€6=5Ο€3.2\cdot\frac{5\pi}{6}=\frac{5\pi}{3}.

Thus

B=2Ο€5Ο€3=65.B=\frac{2\pi}{\frac{5\pi}{3}}=\frac65.

Since the function has a maximum at x=Ο€3x=\frac{\pi}{3}, use a positive cosine model:

f(x)=4cos⁑(65(xβˆ’Ο€3))+3.\boxed{f(x)=4\cos\left(\frac65\left(x-\frac{\pi}{3}\right)\right)+3}.

The key-point increment is

14β‹…5Ο€3=5Ο€12.\frac14\cdot\frac{5\pi}{3}=\frac{5\pi}{12}.

Starting at the maximum x=Ο€3x=\frac{\pi}{3}, the five key points are

(Ο€3,7),(3Ο€4,3),(7Ο€6,βˆ’1),(19Ο€12,3),(2Ο€,7).\boxed{\left(\frac{\pi}{3},7\right), \left(\frac{3\pi}{4},3\right), \left(\frac{7\pi}{6},-1\right), \left(\frac{19\pi}{12},3\right), \left(2\pi,7\right)}.

A graph with many key points is shown below:

parent functions

The function is

g(x)=2tan⁑(3(x+Ο€12))βˆ’1.g(x)=2\tan\left(3\left(x+\frac{\pi}{12}\right)\right)-1.

The period of tangent is

Ο€βˆ£3∣=Ο€3.\frac{\pi}{\lvert 3 \rvert}=\frac{\pi}{3}.

So

period=Ο€3.\boxed{\text{period}=\frac{\pi}{3}}.

The center point occurs where the tangent input is 00:

3(x+Ο€12)=0.3\left(x+\frac{\pi}{12}\right)=0.

Thus

x=βˆ’Ο€12.x=-\frac{\pi}{12}.

At the center,

g(βˆ’Ο€12)=2tan⁑(0)βˆ’1=βˆ’1.g\left(-\frac{\pi}{12}\right)=2\tan(0)-1=-1.

So the center point is

(βˆ’Ο€12,βˆ’1).\boxed{\left(-\frac{\pi}{12},-1\right)}.

The distance from the center to each vertical asymptote is half the period:

12β‹…Ο€3=Ο€6.\frac12\cdot\frac{\pi}{3}=\frac{\pi}{6}.

So the surrounding vertical asymptotes are

βˆ’Ο€12βˆ’Ο€6=βˆ’Ο€4-\frac{\pi}{12}-\frac{\pi}{6}=-\frac{\pi}{4}

and

βˆ’Ο€12+Ο€6=Ο€12.-\frac{\pi}{12}+\frac{\pi}{6}=\frac{\pi}{12}.

Thus

x=βˆ’Ο€4andx=Ο€12.\boxed{x=-\frac{\pi}{4}\quad\text{and}\quad x=\frac{\pi}{12}}.

For the xx-intercept, set g(x)=0g(x)=0:

2tan⁑(3(x+Ο€12))βˆ’1=0.2\tan\left(3\left(x+\frac{\pi}{12}\right)\right)-1=0.

Then

tan⁑(3(x+Ο€12))=12.\tan\left(3\left(x+\frac{\pi}{12}\right)\right)=\frac12.

On the center branch,

3(x+Ο€12)=tanβ‘βˆ’1(12).3\left(x+\frac{\pi}{12}\right)=\tan^{-1}\left(\frac12\right).

Therefore

x=13tanβ‘βˆ’1(12)βˆ’Ο€12.\boxed{x=\frac13\tan^{-1}\left(\frac12\right)-\frac{\pi}{12}}.

The branch should increase from the vertical asymptote x=βˆ’Ο€4x=-\frac{\pi}{4} to the vertical asymptote x=Ο€12x=\frac{\pi}{12}, passing through the center point (βˆ’Ο€12,βˆ’1)\left(-\frac{\pi}{12},-1\right) and the xx-intercept above.

A graph with many key points is shown below:

parent functions

The function is

h(x)=βˆ’2sec⁑(12(xβˆ’Ο€))+3.h(x)=-2\sec\left(\frac12(x-\pi)\right)+3.

The period of secant is

2Ο€βˆ£12∣=4Ο€.\frac{2\pi}{\left\lvert \frac12\right\rvert}=4\pi.

So

period=4Ο€.\boxed{\text{period}=4\pi}.

The midline is

y=3.\boxed{y=3}.

One period starting at x=Ο€x=\pi runs from

x=Ο€x=\pi

to

x=Ο€+4Ο€=5Ο€.x=\pi+4\pi=5\pi.

Secant has vertical asymptotes when the cosine inside is 00:

12(xβˆ’Ο€)=Ο€2+kΟ€.\frac12(x-\pi)=\frac{\pi}{2}+k\pi.

Multiply by 22:

xβˆ’Ο€=Ο€+2kΟ€.x-\pi=\pi+2k\pi.

Thus

x=2Ο€+2kΟ€.x=2\pi+2k\pi.

In the period [Ο€,5Ο€][\pi,5\pi], the vertical asymptotes are

x=2Ο€andx=4Ο€.\boxed{x=2\pi\quad\text{and}\quad x=4\pi}.

The parent secant has range (βˆ’βˆž,βˆ’1]βˆͺ[1,∞)(-\infty,-1]\cup[1,\infty). Multiplying by βˆ’2-2 gives (βˆ’βˆž,βˆ’2]βˆͺ[2,∞)(-\infty,-2]\cup[2,\infty) with the branches swapped, and adding 33 gives

(βˆ’βˆž,1]βˆͺ[5,∞).\boxed{(-\infty,1]\cup[5,\infty)}.

The guiding cosine curve is

y=βˆ’2cos⁑(12(xβˆ’Ο€))+3.y=-2\cos\left(\frac12(x-\pi)\right)+3.

On [Ο€,5Ο€][\pi,5\pi], its key values are

(Ο€,1),(2Ο€,3),(3Ο€,5),(4Ο€,3),(5Ο€,1).(\pi,1),\quad (2\pi,3),\quad (3\pi,5),\quad (4\pi,3),\quad (5\pi,1).

The secant graph has vertices at (Ο€,1)(\pi,1), (3Ο€,5)(3\pi,5), and (5Ο€,1)(5\pi,1), with vertical asymptotes at x=2Ο€x=2\pi and x=4Ο€x=4\pi.

A graph with many key points is shown below:

parent functions

Let

u=sin⁑x.u=\sin x.

Then

2u2βˆ’uβˆ’1=0.2u^2-u-1=0.

Factor:

(2u+1)(uβˆ’1)=0.(2u+1)(u-1)=0.

Thus

sin⁑x=βˆ’12orsin⁑x=1.\sin x=-\frac12 \qquad\text{or}\qquad \sin x=1.

On [0,4Ο€)[0,4\pi),

sin⁑x=1\sin x=1

at

x=Ο€2,5Ο€2.x=\frac{\pi}{2},\frac{5\pi}{2}.

Also,

sin⁑x=βˆ’12\sin x=-\frac12

at

x=7Ο€6,11Ο€6,19Ο€6,23Ο€6.x=\frac{7\pi}{6},\frac{11\pi}{6},\frac{19\pi}{6},\frac{23\pi}{6}.

Therefore

x=Ο€2,7Ο€6,11Ο€6,5Ο€2,19Ο€6,23Ο€6.\boxed{x=\frac{\pi}{2},\frac{7\pi}{6},\frac{11\pi}{6},\frac{5\pi}{2},\frac{19\pi}{6},\frac{23\pi}{6}}.

The graph of y=2sin⁑2xβˆ’sin⁑xβˆ’1y=2\sin^2x-\sin x-1 crosses the xx-axis exactly at those values on [0,4Ο€)[0,4\pi).

A graph with many key points is shown below:

parent functions

Start with

4sin⁑(4x)cos⁑(6x)=2sin⁑(10x)+1.4\sin(4x)\cos(6x)=2\sin(10x)+1.

Use the product-to-sum identity

sin⁑Acos⁑B=12[sin⁑(A+B)+sin⁑(Aβˆ’B)].\sin A\cos B=\frac12[\sin(A+B)+\sin(A-B)].

Then

4sin⁑(4x)cos⁑(6x)=2[sin⁑(10x)+sin⁑(βˆ’2x)].4\sin(4x)\cos(6x) =2[\sin(10x)+\sin(-2x)].

Since sin⁑(βˆ’2x)=βˆ’sin⁑(2x)\sin(-2x)=-\sin(2x),

4sin⁑(4x)cos⁑(6x)=2sin⁑(10x)βˆ’2sin⁑(2x).4\sin(4x)\cos(6x)=2\sin(10x)-2\sin(2x).

So the equation becomes

2sin⁑(10x)βˆ’2sin⁑(2x)=2sin⁑(10x)+1.2\sin(10x)-2\sin(2x)=2\sin(10x)+1.

Subtract 2sin⁑(10x)2\sin(10x) from both sides:

βˆ’2sin⁑(2x)=1.-2\sin(2x)=1.

Thus

sin⁑(2x)=βˆ’12.\sin(2x)=-\frac12.

Let u=2xu=2x. Since x∈[0,4Ο€)x\in[0,4\pi),

u∈[0,8Ο€).u\in[0,8\pi).

On [0,8Ο€)[0,8\pi), sin⁑u=βˆ’12\sin u=-\frac12 at

u=7Ο€6,11Ο€6,19Ο€6,23Ο€6,31Ο€6,35Ο€6,43Ο€6,47Ο€6.u=\frac{7\pi}{6},\frac{11\pi}{6},\frac{19\pi}{6},\frac{23\pi}{6}, \frac{31\pi}{6},\frac{35\pi}{6},\frac{43\pi}{6},\frac{47\pi}{6}.

Divide by 22:

x=7Ο€12,11Ο€12,19Ο€12,23Ο€12,31Ο€12,35Ο€12,43Ο€12,47Ο€12.\boxed{x=\frac{7\pi}{12},\frac{11\pi}{12},\frac{19\pi}{12},\frac{23\pi}{12}, \frac{31\pi}{12},\frac{35\pi}{12},\frac{43\pi}{12},\frac{47\pi}{12}}.

The equation is

tan⁑x+cot⁑x=4.\tan x+\cot x=4.

Let

t=tan⁑x.t=\tan x.

Then cot⁑x=1t\cot x=\frac1t, so

t+1t=4.t+\frac1t=4.

Multiply by tt:

t2+1=4t.t^2+1=4t.

So

t2βˆ’4t+1=0.t^2-4t+1=0.

Use the quadratic formula:

t=4Β±16βˆ’42=2Β±3.t=\frac{4\pm\sqrt{16-4}}{2} =2\pm\sqrt3.

Since

tan⁑(Ο€12)=2βˆ’3\tan\left(\frac{\pi}{12}\right)=2-\sqrt3

and

tan⁑(5Ο€12)=2+3,\tan\left(\frac{5\pi}{12}\right)=2+\sqrt3,

the solutions on [0,2Ο€)[0,2\pi) are

x=Ο€12,5Ο€12,13Ο€12,17Ο€12.\boxed{x=\frac{\pi}{12},\frac{5\pi}{12},\frac{13\pi}{12},\frac{17\pi}{12}}.

Use angle addition and subtraction formulas.

First,

sin⁑75∘=sin⁑(45∘+30∘).\sin75^\circ=\sin(45^\circ+30^\circ).

So

sin⁑75∘=sin⁑45∘cos⁑30∘+cos⁑45∘sin⁑30∘.\sin75^\circ =\sin45^\circ\cos30^\circ+\cos45^\circ\sin30^\circ.

Thus

sin⁑75∘=22β‹…32+22β‹…12=6+24.\sin75^\circ =\frac{\sqrt2}{2}\cdot\frac{\sqrt3}{2} +\frac{\sqrt2}{2}\cdot\frac12 =\frac{\sqrt6+\sqrt2}{4}.

Next,

cos⁑15∘=cos⁑(45βˆ˜βˆ’30∘).\cos15^\circ=\cos(45^\circ-30^\circ).

So

cos⁑15∘=cos⁑45∘cos⁑30∘+sin⁑45∘sin⁑30∘=6+24.\cos15^\circ =\cos45^\circ\cos30^\circ+\sin45^\circ\sin30^\circ =\frac{\sqrt6+\sqrt2}{4}.

Finally,

tan⁑105∘=tan⁑(60∘+45∘).\tan105^\circ=\tan(60^\circ+45^\circ).

Then

tan⁑105∘=3+11βˆ’3.\tan105^\circ =\frac{\sqrt3+1}{1-\sqrt3}.

Rationalize:

3+11βˆ’3β‹…1+31+3=4+23βˆ’2=βˆ’2βˆ’3.\frac{\sqrt3+1}{1-\sqrt3}\cdot\frac{1+\sqrt3}{1+\sqrt3} =\frac{4+2\sqrt3}{-2} =-2-\sqrt3.

Therefore

sin⁑75∘=6+24,\boxed{\sin75^\circ=\frac{\sqrt6+\sqrt2}{4}}, cos⁑15∘=6+24,\boxed{\cos15^\circ=\frac{\sqrt6+\sqrt2}{4}},

and

tan⁑105∘=βˆ’2βˆ’3.\boxed{\tan105^\circ=-2-\sqrt3}.

Start with the left-hand side:

sin⁑(x+y)+sin⁑(xβˆ’y)cos⁑(x+y)+cos⁑(xβˆ’y).\frac{\sin(x+y)+\sin(x-y)}{\cos(x+y)+\cos(x-y)}.

Use sum-to-product formulas:

sin⁑(x+y)+sin⁑(xβˆ’y)=2sin⁑xcos⁑y.\sin(x+y)+\sin(x-y) =2\sin x\cos y.

Also,

cos⁑(x+y)+cos⁑(xβˆ’y)=2cos⁑xcos⁑y.\cos(x+y)+\cos(x-y) =2\cos x\cos y.

Therefore

sin⁑(x+y)+sin⁑(xβˆ’y)cos⁑(x+y)+cos⁑(xβˆ’y)=2sin⁑xcos⁑y2cos⁑xcos⁑y.\frac{\sin(x+y)+\sin(x-y)}{\cos(x+y)+\cos(x-y)} =\frac{2\sin x\cos y}{2\cos x\cos y}.

Cancel:

2sin⁑xcos⁑y2cos⁑xcos⁑y=sin⁑xcos⁑x=tan⁑x.\frac{2\sin x\cos y}{2\cos x\cos y} =\frac{\sin x}{\cos x} =\tan x.

Thus

sin⁑(x+y)+sin⁑(xβˆ’y)cos⁑(x+y)+cos⁑(xβˆ’y)=tan⁑x.\boxed{\frac{\sin(x+y)+\sin(x-y)}{\cos(x+y)+\cos(x-y)}=\tan x}.

Use the sum-to-product formula:

cos⁑A+cos⁑B=2cos⁑(A+B2)cos⁑(Aβˆ’B2).\cos A+\cos B =2\cos\left(\frac{A+B}{2}\right)\cos\left(\frac{A-B}{2}\right).

With A=5xA=5x and B=3xB=3x,

cos⁑(5x)+cos⁑(3x)=2cos⁑(4x)cos⁑x.\cos(5x)+\cos(3x) =2\cos(4x)\cos x.

So the equation becomes

2cos⁑(4x)cos⁑x=0.2\cos(4x)\cos x=0.

Thus

cos⁑(4x)=0\cos(4x)=0

or

cos⁑x=0.\cos x=0.

For cos⁑x=0\cos x=0 on [0,2Ο€)[0,2\pi),

x=Ο€2,3Ο€2.x=\frac{\pi}{2},\frac{3\pi}{2}.

For cos⁑(4x)=0\cos(4x)=0,

4x=Ο€2+kΟ€.4x=\frac{\pi}{2}+k\pi.

So

x=Ο€8+kΟ€4.x=\frac{\pi}{8}+\frac{k\pi}{4}.

On [0,2Ο€)[0,2\pi), this gives

x=Ο€8,3Ο€8,5Ο€8,7Ο€8,9Ο€8,11Ο€8,13Ο€8,15Ο€8.x=\frac{\pi}{8},\frac{3\pi}{8},\frac{5\pi}{8},\frac{7\pi}{8}, \frac{9\pi}{8},\frac{11\pi}{8},\frac{13\pi}{8},\frac{15\pi}{8}.

Therefore

x=Ο€8,3Ο€8,Ο€2,5Ο€8,7Ο€8,9Ο€8,11Ο€8,3Ο€2,13Ο€8,15Ο€8.\boxed{x=\frac{\pi}{8},\frac{3\pi}{8},\frac{\pi}{2},\frac{5\pi}{8},\frac{7\pi}{8},\frac{9\pi}{8},\frac{11\pi}{8},\frac{3\pi}{2},\frac{13\pi}{8},\frac{15\pi}{8}}.

The product-to-sum form

cos⁑(5x)+cos⁑(3x)=2cos⁑(4x)cos⁑x\cos(5x)+\cos(3x)=2\cos(4x)\cos x

shows that zeros occur whenever either factor is zero. A sketch should mark the eight zeros from cos⁑(4x)=0\cos(4x)=0 and the two zeros from cos⁑x=0\cos x=0.

ADD IMAGE OF GRAPH

Let

Ξ±=cosβ‘βˆ’135.\alpha=\cos^{-1}\frac35.

Then cos⁑α=35\cos\alpha=\frac35, and since α∈[0,Ο€]\alpha\in[0,\pi], Ξ±\alpha is in Quadrant I. Therefore

sin⁑α=45.\sin\alpha=\frac45.

So

sin⁑(cosβ‘βˆ’135)=45.\sin\left(\cos^{-1}\frac35\right)=\frac45.

Next, let

Ξ²=sinβ‘βˆ’1(βˆ’513).\beta=\sin^{-1}\left(-\frac5{13}\right).

Since β∈[βˆ’Ο€2,Ο€2]\beta\in\left[-\frac{\pi}{2},\frac{\pi}{2}\right] and sine is negative, Ξ²\beta is in Quadrant IV. Thus

cos⁑β=1213.\cos\beta=\frac{12}{13}.

So

cos⁑(sinβ‘βˆ’1(βˆ’513))=1213.\cos\left(\sin^{-1}\left(-\frac5{13}\right)\right)=\frac{12}{13}.

Finally, let

Ξ³=cosβ‘βˆ’1(βˆ’45).\gamma=\cos^{-1}\left(-\frac45\right).

Then γ∈[0,Ο€]\gamma\in[0,\pi] and cosine is negative, so Ξ³\gamma is in Quadrant II. Hence

sin⁑γ=35,\sin\gamma=\frac35,

and

tan⁑γ=35βˆ’45=βˆ’34.\tan\gamma=\frac{\frac35}{-\frac45}=-\frac34.

Now add:

45+1213βˆ’34.\frac45+\frac{12}{13}-\frac34.

Using common denominator 260260:

208260+240260βˆ’195260=253260.\frac{208}{260}+\frac{240}{260}-\frac{195}{260} =\frac{253}{260}.

Therefore

253260.\boxed{\frac{253}{260}}.

We need count solutions to

tan⁑(2x)=cos⁑(x2)\tan(2x)=\cos\left(\frac{x}{2}\right)

on [0,2Ο€][0,2\pi].

The tangent side is undefined when

2x=Ο€2+kΟ€.2x=\frac{\pi}{2}+k\pi.

Thus

x=Ο€4+kΟ€2.x=\frac{\pi}{4}+\frac{k\pi}{2}.

On [0,2Ο€][0,2\pi], these asymptotes occur at

Ο€4,3Ο€4,5Ο€4,7Ο€4.\frac{\pi}{4},\frac{3\pi}{4},\frac{5\pi}{4},\frac{7\pi}{4}.

These split the interval into five pieces:

[0,Ο€4),(Ο€4,3Ο€4),(3Ο€4,5Ο€4),(5Ο€4,7Ο€4),(7Ο€4,2Ο€].\left[0,\frac{\pi}{4}\right),\quad \left(\frac{\pi}{4},\frac{3\pi}{4}\right),\quad \left(\frac{3\pi}{4},\frac{5\pi}{4}\right),\quad \left(\frac{5\pi}{4},\frac{7\pi}{4}\right),\quad \left(\frac{7\pi}{4},2\pi\right].

Let

F(x)=tan⁑(2x)βˆ’cos⁑(x2).F(x)=\tan(2x)-\cos\left(\frac{x}{2}\right).

On each of the five pieces, tan⁑(2x)\tan(2x) increases from βˆ’βˆž-\infty to ∞\infty, except on the first and last pieces where one endpoint is finite. Also, cos⁑(x2)\cos\left(\frac{x}{2}\right) decreases from 11 to βˆ’1-1 on [0,2Ο€][0,2\pi].

More formally,

Fβ€²(x)=2sec⁑2(2x)+12sin⁑(x2)>0F'(x)=2\sec^2(2x)+\frac12\sin\left(\frac{x}{2}\right)>0

wherever FF is defined on [0,2Ο€][0,2\pi]. So FF is strictly increasing on each piece.

On each piece, the function changes from negative to positive:

  • On the first interval, F(0)=βˆ’1F(0)=-1 and F(x)β†’βˆžF(x)\to\infty as xβ†’Ο€4βˆ’x\to\frac{\pi}{4}^{-}.
  • On each middle interval, F(x)β†’βˆ’βˆžF(x)\to-\infty from the left asymptote and F(x)β†’βˆžF(x)\to\infty at the right asymptote.
  • On the last interval, F(x)β†’βˆ’βˆžF(x)\to-\infty as xβ†’7Ο€4+x\to\frac{7\pi}{4}^{+} and F(2Ο€)=1F(2\pi)=1.

Therefore there is exactly one solution in each of the five pieces.

5\boxed{5}

We are given

Ο€2<ΞΈ<Ο€,\frac{\pi}{2}<\theta<\pi,

so ΞΈ\theta is in Quadrant II. Therefore

ΞΈ2\frac{\theta}{2}

is in Quadrant I.

Since

cos⁑θ=βˆ’35,\cos\theta=-\frac35,

the half-angle formulas give

sin⁑(ΞΈ2)=1βˆ’cos⁑θ2.\sin\left(\frac{\theta}{2}\right) =\sqrt{\frac{1-\cos\theta}{2}}.

Substitute:

sin⁑(ΞΈ2)=1βˆ’(βˆ’35)2=852=45=255.\sin\left(\frac{\theta}{2}\right) =\sqrt{\frac{1-\left(-\frac35\right)}{2}} =\sqrt{\frac{\frac85}{2}} =\sqrt{\frac45} =\frac{2\sqrt5}{5}.

Also,

cos⁑(ΞΈ2)=1+cos⁑θ2=1βˆ’352=252=15=55.\cos\left(\frac{\theta}{2}\right) =\sqrt{\frac{1+\cos\theta}{2}} =\sqrt{\frac{1-\frac35}{2}} =\sqrt{\frac{\frac25}{2}} =\sqrt{\frac15} =\frac{\sqrt5}{5}.

Thus

tan⁑(θ2)=sin⁑(θ2)cos⁑(θ2)=2.\tan\left(\frac{\theta}{2}\right) =\frac{\sin\left(\frac{\theta}{2}\right)}{\cos\left(\frac{\theta}{2}\right)} =2.

Therefore

sin⁑(θ2)=255,cos⁑(θ2)=55,tan⁑(θ2)=2.\boxed{\sin\left(\frac{\theta}{2}\right)=\frac{2\sqrt5}{5}}, \qquad \boxed{\cos\left(\frac{\theta}{2}\right)=\frac{\sqrt5}{5}}, \qquad \boxed{\tan\left(\frac{\theta}{2}\right)=2}.

We are given

sin⁑xsin⁑y=3\frac{\sin x}{\sin y}=3

and

cos⁑xcos⁑y=12.\frac{\cos x}{\cos y}=\frac12.

So

sin⁑x=3sin⁑y\sin x=3\sin y

and

cos⁑x=12cos⁑y.\cos x=\frac12\cos y.

Let

S=sin⁑2yandC=cos⁑2y.S=\sin^2 y \qquad\text{and}\qquad C=\cos^2 y.

Since S+C=1S+C=1, we also know

sin⁑2x+cos⁑2x=1.\sin^2x+\cos^2x=1.

Substitute the given ratios:

(3sin⁑y)2+(12cos⁑y)2=1.(3\sin y)^2+\left(\frac12\cos y\right)^2=1.

Thus

9S+14C=1.9S+\frac14C=1.

Since C=1βˆ’SC=1-S,

9S+14(1βˆ’S)=1.9S+\frac14(1-S)=1.

Multiply by 44:

36S+1βˆ’S=4.36S+1-S=4.

So

35S=3,35S=3,

and

S=335.S=\frac3{35}.

Then

C=1βˆ’335=3235.C=1-\frac3{35}=\frac{32}{35}.

Now,

sin⁑2xsin⁑2y=2sin⁑xcos⁑x2sin⁑ycos⁑y=sin⁑xsin⁑yβ‹…cos⁑xcos⁑y=3β‹…12=32.\frac{\sin 2x}{\sin 2y} =\frac{2\sin x\cos x}{2\sin y\cos y} =\frac{\sin x}{\sin y}\cdot\frac{\cos x}{\cos y} =3\cdot\frac12 =\frac32.

Also,

cos⁑2xcos⁑2y=cos⁑2xβˆ’sin⁑2xcos⁑2yβˆ’sin⁑2y.\frac{\cos 2x}{\cos 2y} =\frac{\cos^2x-\sin^2x}{\cos^2y-\sin^2y}.

Compute the numerator:

cos⁑2xβˆ’sin⁑2x=14Cβˆ’9S.\cos^2x-\sin^2x =\frac14C-9S.

Using C=3235C=\frac{32}{35} and S=335S=\frac3{35}:

14Cβˆ’9S=14β‹…3235βˆ’9β‹…335=835βˆ’2735=βˆ’1935.\frac14C-9S =\frac14\cdot\frac{32}{35}-9\cdot\frac3{35} =\frac8{35}-\frac{27}{35} =-\frac{19}{35}.

The denominator is

Cβˆ’S=3235βˆ’335=2935.C-S=\frac{32}{35}-\frac3{35} =\frac{29}{35}.

Therefore

cos⁑2xcos⁑2y=βˆ’19352935=βˆ’1929.\frac{\cos 2x}{\cos 2y} =\frac{-\frac{19}{35}}{\frac{29}{35}} =-\frac{19}{29}.

Now add:

sin⁑2xsin⁑2y+cos⁑2xcos⁑2y=32βˆ’1929.\frac{\sin 2x}{\sin 2y}+\frac{\cos 2x}{\cos 2y} =\frac32-\frac{19}{29}.

Use denominator 5858:

32βˆ’1929=8758βˆ’3858=4958.\frac32-\frac{19}{29} =\frac{87}{58}-\frac{38}{58} =\frac{49}{58}.

Thus

p=49andq=58.p=49 \qquad\text{and}\qquad q=58.

So

p+q=107.\boxed{p+q=107}.

The high tide is 1111 feet and the low tide is 33 feet. The midline is

D=11+32=7.D=\frac{11+3}{2}=7.

The amplitude is

A=11βˆ’32=4.A=\frac{11-3}{2}=4.

The time from high to the next low is half a period:

8βˆ’2=6.8-2=6.

So the period is

12.12.

Thus

B=2Ο€12=Ο€6.B=\frac{2\pi}{12}=\frac{\pi}{6}.

Since the tide is at a high when t=2t=2, use a positive cosine model:

H(t)=4cos⁑(Ο€6(tβˆ’2))+7.\boxed{H(t)=4\cos\left(\frac{\pi}{6}(t-2)\right)+7}.

The period is

12Β hours,\boxed{12\text{ hours}},

and the midline is

H=7.\boxed{H=7}.

Now solve for when H(t)=9H(t)=9:

9=4cos⁑(Ο€6(tβˆ’2))+7.9=4\cos\left(\frac{\pi}{6}(t-2)\right)+7.

Then

2=4cos⁑(Ο€6(tβˆ’2)),2=4\cos\left(\frac{\pi}{6}(t-2)\right),

so

cos⁑(Ο€6(tβˆ’2))=12.\cos\left(\frac{\pi}{6}(t-2)\right)=\frac12.

The first time after the high occurs when the angle is Ο€3\frac{\pi}{3}:

Ο€6(tβˆ’2)=Ο€3.\frac{\pi}{6}(t-2)=\frac{\pi}{3}.

Multiply by 6Ο€\frac6\pi:

tβˆ’2=2.t-2=2.

So

t=4Β hours.\boxed{t=4\text{ hours}}.

One full period runs from t=2t=2 to t=14t=14. The main key points are

(2,11),(5,7),(8,3),(11,7),(14,11).(2,11),\quad (5,7),\quad (8,3),\quad (11,7),\quad (14,11).

The point where H(t)=9H(t)=9 first occurs after t=2t=2 is

(4,9).\boxed{(4,9)}.

ADD IMAGE OF GRAPH

For part (A)(A), first note that

a1=2=2β‹…22=2cos⁑(Ο€4).a_1=\sqrt2=2\cdot\frac{\sqrt2}{2}=2\cos\left(\frac{\pi}{4}\right).

Since

Ο€4=Ο€22,\frac{\pi}{4}=\frac{\pi}{2^{2}},

this matches

a1=2cos⁑(Ο€21+1).a_1=2\cos\left(\frac{\pi}{2^{1+1}}\right).

Now assume

an=2cos⁑(Ο€2n+1).a_n=2\cos\left(\frac{\pi}{2^{n+1}}\right).

Then

an+1=2+an=2+2cos⁑(Ο€2n+1).a_{n+1} =\sqrt{2+a_n} =\sqrt{2+2\cos\left(\frac{\pi}{2^{n+1}}\right)}.

Use the half-angle identity

cos⁑(u2)=1+cos⁑u2\cos\left(\frac{u}{2}\right)=\sqrt{\frac{1+\cos u}{2}}

for angles in Quadrant I. Rearranging gives

2cos⁑(u2)=2+2cos⁑u.2\cos\left(\frac{u}{2}\right)=\sqrt{2+2\cos u}.

With

u=Ο€2n+1,u=\frac{\pi}{2^{n+1}},

we get

an+1=2cos⁑(Ο€2n+2).a_{n+1} =2\cos\left(\frac{\pi}{2^{n+2}}\right).

Thus

an=2cos⁑(Ο€2n+1).\boxed{a_n=2\cos\left(\frac{\pi}{2^{n+1}}\right)}.

For part (B)(B), part (A)(A) gives

an2=cos⁑(Ο€2n+1).\frac{a_n}{2}=\cos\left(\frac{\pi}{2^{n+1}}\right).

Consider the finite product

PN=∏n=1Nan2=∏n=1Ncos⁑(Ο€2n+1).P_N=\prod_{n=1}^{N}\frac{a_n}{2} =\prod_{n=1}^{N}\cos\left(\frac{\pi}{2^{n+1}}\right).

Use the repeated double-angle identity

sin⁑(2x)=2sin⁑xcos⁑x.\sin(2x)=2\sin x\cos x.

Starting with x=Ο€2N+1x=\frac{\pi}{2^{N+1}},

sin⁑(Ο€2)=2Nsin⁑(Ο€2N+1)∏n=1Ncos⁑(Ο€2n+1).\sin\left(\frac{\pi}{2}\right) =2^N\sin\left(\frac{\pi}{2^{N+1}}\right) \prod_{n=1}^{N}\cos\left(\frac{\pi}{2^{n+1}}\right).

Since sin⁑(Ο€2)=1\sin\left(\frac{\pi}{2}\right)=1,

1=2Nsin⁑(Ο€2N+1)PN.1=2^N\sin\left(\frac{\pi}{2^{N+1}}\right)P_N.

Therefore

PN=12Nsin⁑(Ο€2N+1).P_N=\frac{1}{2^N\sin\left(\frac{\pi}{2^{N+1}}\right)}.

For part (C)(C), let

uN=Ο€2N+1.u_N=\frac{\pi}{2^{N+1}}.

Then

2N=Ο€2uN.2^N=\frac{\pi}{2u_N}.

So

PN=12Nsin⁑uN=1Ο€2uNsin⁑uN=2Ο€β‹…uNsin⁑uN.P_N=\frac{1}{2^N\sin u_N} =\frac{1}{\frac{\pi}{2u_N}\sin u_N} =\frac{2}{\pi}\cdot\frac{u_N}{\sin u_N}.

As Nβ†’βˆžN\to\infty, uNβ†’0u_N\to0, and

uNsin⁑uNβ†’1.\frac{u_N}{\sin u_N}\to1.

Thus

lim⁑Nβ†’βˆžPN=2Ο€.\lim_{N\to\infty}P_N=\frac2\pi.

Since

a12=22,\frac{a_1}{2}=\frac{\sqrt2}{2}, a22=2+22,\frac{a_2}{2}=\frac{\sqrt{2+\sqrt2}}{2},

and so on, we get ViΓ¨te’s product:

2Ο€=22β‹…2+22β‹…2+2+22β‹―.\boxed{ \frac{2}{\pi} =\frac{\sqrt2}{2}\cdot \frac{\sqrt{2+\sqrt2}}{2}\cdot \frac{\sqrt{2+\sqrt{2+\sqrt2}}}{2}\cdots }.

Unit 10: Additional Topics in Trigonometry (Triangle Laws, Parametric, Polar, and Vectors)

Section titled β€œUnit 10: Additional Topics in Trigonometry (Triangle Laws, Parametric, Polar, and Vectors)”

Full notes β†’

  1. Solve the triangle with A=60∘A=60^\circ, a=9a=9 cm, and b=10b=10 cm. Determine whether there are zero, one, or two possible triangles. For each valid triangle, find the remaining side and angles.

  2. A plane is flying above the ocean. The angle of depression to a submarine is 24∘24^\circ, and the angle of depression to a ship is 17∘17^\circ. The distance from the plane to the ship is 51205120 feet. Assuming the submarine and ship are in the same vertical plane as the airplane, find the distance between the submarine and the ship.

  3. Two towns AA and BB are 1.41.4 miles apart, with BB due east of AA. A signal is detected on a bearing of S22∘ES22^\circ E from AA and S43∘WS43^\circ W from BB. Draw a labeled diagram and find the distance from each town to the signal.

  4. Prove that for any triangle with side lengths a,b,ca,b,c and semiperimeter s=12(a+b+c)s=\frac12(a+b+c), sin⁑2(C2)=(sβˆ’a)(sβˆ’b)ab.\sin^2\left(\frac C2\right)=\frac{(s-a)(s-b)}{ab}.

  5. Let u=βŸ¨βˆ’2,1⟩\mathbf u=\langle -2,1\rangle and v=βŸ¨βˆ’5,3⟩\mathbf v=\langle -5,3\rangle.

    (A)(A) Find 2uβˆ’3v2\mathbf u-3\mathbf v.

    (B)(B) Find the angle between u\mathbf u and v\mathbf v to the nearest degree.

    (C)(C) Find a unit vector in the direction of u+v\mathbf u+\mathbf v.

  6. A plane is heading 40∘40^\circ east of north at 120120 mph. A wind blows directly from the east at 1010 mph. Find the ground-speed vector, the ground speed, and the drift angle from the plane’s intended heading.

  7. A force of 1818 Newtons acts in the direction 235∘235^\circ from the positive xx-axis. Resolve the force into horizontal and vertical components. Then find the magnitude and direction of the vector obtained by adding this force to ⟨12,βˆ’5⟩\langle 12,-5\rangle.

  8. A particle moves according to x(t)=2cos⁑tβˆ’sin⁑(2t),y(t)=6sin⁑t,x(t)=2\cos t-\sin(2t),\qquad y(t)=6\sin t, for 0≀t≀2Ο€0\le t\le 2\pi.

    (A)(A) Find all exact xx-intercepts.

    (B)(B) Find the particle’s position when t=Ο€2t=\frac{\pi}{2} and when t=7Ο€6t=\frac{7\pi}{6}.

    (C)(C) Write a formula for the particle’s distance from the origin as a function of tt.

  9. Eliminate the parameter and describe the curve, including any domain restrictions and orientation: x=etx=e^t, y=e2tβˆ’3y=e^{2t}-3, βˆ’ln⁑2≀t≀ln⁑3.-\ln2\le t\le \ln3.

  10. The curve x=4cos⁑tx=4\cos t, y=βˆ’2sin⁑ty=-2\sin t is traced for 0≀t≀2Ο€0\le t\le 2\pi. Eliminate the parameter, state where the curve starts, and determine the direction (clockwise or counterclockwise) the curve is traced in.

  11. Classify each polar curve as a cardioid, limacon, rose curve, lemniscate, circle, line, or spiral. For rose curves, state the number of petals. Graph each of the curves.

    (A)(A) Graph r=3βˆ’3sin⁑θr=3-3\sin\theta

    (B)(B) Graph r=2+5cos⁑θr=2+5\cos\theta

    (C)(C) Graph r=4sin⁑(3θ)r=4\sin(3\theta)

    (D)(D) Graph r2=25sin⁑(2θ)r^2=25\sin(2\theta)

  12. Graph both r=2+2cos⁑θr=2+2\cos\theta and r=2βˆ’2cos⁑θr=2-2\cos\theta. Then, find the number of intersection points.

  13. Suppose you have an octagon centered at the origin with one vertex at P1=22P_1=2\sqrt2. (A)(A) Find a vertex in the third quadrant and a vertex in the fourth quadrant. (B)(B) Without finding all of the vertices calculate P1+P2+β‹―+P8P_1+P_2+\cdots+P_8 (C)(C) Without finding all of the vertices calculate P1P2β‹―P8P_1P_2\cdots P_8.

  14. Let z1=βˆ’2+23i,z2=1βˆ’i.z_1=-2+2\sqrt3i,\qquad z_2=1-i.

    (A)(A) Write both numbers in polar form.

    (B)(B) Write both numbers in exponential form.

    (C)(C) Compute z1z2z_1z_2 in polar form and rectangular form.

  15. Use De Moivre’s Theorem to find all fourth roots of 16(cos⁑2Ο€3+isin⁑2Ο€3).16\left(\cos\frac{2\pi}{3}+i\sin\frac{2\pi}{3}\right).

  16. (Bonus, Brahmagupta’s and Bretschneider’s formulas)

Let ABCDABCD be a cyclic quadrilateral, meaning all four vertices lie on one circle. Let its side lengths be a,b,c,da,b,c,d, and let its semiperimeter be

s=12(a+b+c+d).s=\frac12(a+b+c+d).

The goal is to prove the area of a cyclic quadrilateral is:

K=(sβˆ’a)(sβˆ’b)(sβˆ’c)(sβˆ’d),K=\sqrt{(s-a)(s-b)(s-c)(s-d)},

where KK is the area of the cyclic quadrilateral. We will also extend the area formula to all cases, not just cyclic ones.

(A)(A) Draw diagonal ACAC. Let ∠ABC=B\angle ABC=B and ∠ADC=D\angle ADC=D. Use triangle area formulas and D=180βˆ˜βˆ’BD=180^\circ-B (A property of cyclic quadrilaterals) to rewrite the area as K=12(ab+cd)sin⁑B.K=\frac12(ab+cd)\sin B.

(B)(B) Apply the Law of Cosines to triangles ABCABC and ADCADC to show that 2abcos⁑B=a2+b2βˆ’c2βˆ’d2+2cdcos⁑D.2ab\cos B=a^2+b^2-c^2-d^2+2cd\cos D.

(C)(C) Use cos⁑D=βˆ’cos⁑B\cos D=-\cos B to solve for cos⁑B\cos B, then combine this with K=12(ab+cd)sin⁑BK=\frac12(ab+cd)\sin B and sin⁑2B=1βˆ’cos⁑2B\sin^2B=1-\cos^2B to prove K2=(sβˆ’a)(sβˆ’b)(sβˆ’c)(sβˆ’d).K^2=(s-a)(s-b)(s-c)(s-d). This is Brahmagupta’s formula.

(D)(D) Now suppose ABCDABCD is not necessarily cyclic. Keep the same notation, with opposite angles BB and DD. Show that (4K)2+(a2+b2βˆ’c2βˆ’d2)2=4(a2b2+c2d2βˆ’2abcdcos⁑(B+D)).(4K)^2+(a^2+b^2-c^2-d^2)^2=4(a^2b^2+c^2d^2-2abcd\cos(B+D)).

(E)(E) Now prove Bretschneider’s formula: K2=(sβˆ’a)(sβˆ’b)(sβˆ’c)(sβˆ’d)βˆ’abcdcos⁑2(B+D2).K^2=(s-a)(s-b)(s-c)(s-d)-abcd\cos^2\left(\frac{B+D}{2}\right).

(F)(F) Explain why Bretschneider’s formula turns into Brahmagupta’s formula when ABCDABCD is cyclic.


By the Law of Sines,

sin⁑B10=sin⁑60∘9,\frac{\sin B}{10}=\frac{\sin 60^\circ}{9},

so

sin⁑B=10sin⁑60∘9=539.\sin B=\frac{10\sin 60^\circ}{9}=\frac{5\sqrt3}{9}.

This gives two possible angles:

Bβ‰ˆ74.2∘orBβ‰ˆ105.8∘.B\approx 74.2^\circ\quad \text{or}\quad B\approx 105.8^\circ.

If Bβ‰ˆ74.2∘B\approx 74.2^\circ, then

Cβ‰ˆ45.8∘,cβ‰ˆ7.45Β cm.C\approx 45.8^\circ,\qquad c\approx 7.45\text{ cm}.

If Bβ‰ˆ105.8∘B\approx 105.8^\circ, then

Cβ‰ˆ14.2∘,cβ‰ˆ2.55Β cm.C\approx 14.2^\circ,\qquad c\approx 2.55\text{ cm}.

Therefore, there are two possible triangles.

The plane-to-ship distance is 51205120 ft, and the angle of depression to the ship is 17∘17^\circ. So the plane’s height is

h=5120sin⁑17βˆ˜β‰ˆ1496.94Β ft.h=5120\sin 17^\circ\approx 1496.94\text{ ft}.

The horizontal distance from the plane to the ship is

5120cos⁑17βˆ˜β‰ˆ4896.28Β ft.5120\cos 17^\circ\approx 4896.28\text{ ft}.

The horizontal distance from the plane to the submarine is

htan⁑24βˆ˜β‰ˆ3362.19Β ft.\frac{h}{\tan 24^\circ}\approx 3362.19\text{ ft}.

Assuming the ship and submarine are on the same side of the plane, their distance apart is

4896.28βˆ’3362.19β‰ˆ1534.09Β ft.4896.28-3362.19\approx 1534.09\text{ ft}.

Place town AA at (0,0)(0,0) and town BB at (1.4,0)(1.4,0). The bearing S22∘ES22^\circ E from AA points down and right, while S43∘WS43^\circ W from BB points down and left.

Solving the two bearing lines gives the signal at approximately

(0.423,βˆ’1.047).(0.423,-1.047).

Therefore,

ASβ‰ˆ1.13Β miles,BSβ‰ˆ1.43Β miles.AS\approx 1.13\text{ miles},\qquad BS\approx 1.43\text{ miles}.

Use the half-angle identity:

sin⁑2(C2)=1βˆ’cos⁑C2.\sin^2\left(\frac C2\right)=\frac{1-\cos C}{2}.

By the Law of Cosines,

cos⁑C=a2+b2βˆ’c22ab.\cos C=\frac{a^2+b^2-c^2}{2ab}.

Substitute:

sin⁑2(C2)=12(1βˆ’a2+b2βˆ’c22ab)=c2βˆ’(aβˆ’b)24ab.\sin^2\left(\frac C2\right) =\frac{1}{2}\left(1-\frac{a^2+b^2-c^2}{2ab}\right) =\frac{c^2-(a-b)^2}{4ab}.

Factor the numerator:

c2βˆ’(aβˆ’b)2=(cβˆ’a+b)(c+aβˆ’b).c^2-(a-b)^2=(c-a+b)(c+a-b).

Since s=12(a+b+c)s=\frac12(a+b+c),

cβˆ’a+b=2(sβˆ’a),c+aβˆ’b=2(sβˆ’b).c-a+b=2(s-a),\qquad c+a-b=2(s-b).

Thus,

sin⁑2(C2)=(sβˆ’a)(sβˆ’b)ab.\sin^2\left(\frac C2\right)=\frac{(s-a)(s-b)}{ab}.

We have

u=βŸ¨βˆ’2,1⟩,v=βŸ¨βˆ’5,3⟩.\mathbf u=\langle -2,1\rangle,\qquad \mathbf v=\langle -5,3\rangle.

For part (A),

2uβˆ’3v=βŸ¨βˆ’4,2βŸ©βˆ’βŸ¨βˆ’15,9⟩=⟨11,βˆ’7⟩.2\mathbf u-3\mathbf v =\langle -4,2\rangle-\langle -15,9\rangle =\langle 11,-7\rangle.

For part (B),

uβ‹…v=(βˆ’2)(βˆ’5)+(1)(3)=13.\mathbf u\cdot \mathbf v=(-2)(-5)+(1)(3)=13.

Also,

∣u∣=5,∣v∣=34.\lvert \mathbf u \rvert=\sqrt5,\qquad \lvert \mathbf v \rvert=\sqrt{34}.

So

cos⁑θ=13534=13170.\cos\theta=\frac{13}{\sqrt5\sqrt{34}}=\frac{13}{\sqrt{170}}.

Therefore,

ΞΈβ‰ˆ4∘.\theta\approx 4^\circ.

For part (C), since

u+v=βŸ¨βˆ’7,4⟩,\mathbf u+\mathbf v=\langle -7,4\rangle,

a unit vector in that direction is

βŸ¨βˆ’7,4⟩65=βŸ¨βˆ’765,465⟩.\frac{\langle -7,4\rangle}{\sqrt{65}} =\left\langle \frac{-7}{\sqrt{65}},\frac{4}{\sqrt{65}}\right\rangle.

Let east be positive xx and north be positive yy. A heading of 40∘40^\circ east of north at 120120 mph has velocity

⟨120sin⁑40∘,120cos⁑40∘⟩.\langle 120\sin40^\circ,120\cos40^\circ\rangle.

A wind directly from the east blows west, so its vector is

βŸ¨βˆ’10,0⟩.\langle -10,0\rangle.

The ground-speed vector is

⟨120sin⁑40βˆ˜βˆ’10,120cos⁑40βˆ˜βŸ©β‰ˆβŸ¨67.13,91.93⟩.\langle 120\sin40^\circ-10,120\cos40^\circ\rangle \approx \langle 67.13,91.93\rangle.

The ground speed is

67.132+91.932β‰ˆ113.83Β mph.\sqrt{67.13^2+91.93^2}\approx 113.83\text{ mph}.

The actual direction is about

tanβ‘βˆ’1(67.1391.93)β‰ˆ36.1∘\tan^{-1}\left(\frac{67.13}{91.93}\right)\approx 36.1^\circ

east of north. Since the intended heading was 40∘40^\circ east of north, the drift angle is about

40βˆ˜βˆ’36.1∘=3.9∘40^\circ-36.1^\circ=3.9^\circ

west of the intended heading.

The force components are

⟨18cos⁑235∘,18sin⁑235βˆ˜βŸ©β‰ˆβŸ¨βˆ’10.32,βˆ’14.74⟩.\langle 18\cos235^\circ,18\sin235^\circ\rangle \approx \langle -10.32,-14.74\rangle.

Add ⟨12,βˆ’5⟩\langle 12,-5\rangle:

βŸ¨βˆ’10.32,βˆ’14.74⟩+⟨12,βˆ’5βŸ©β‰ˆβŸ¨1.68,βˆ’19.74⟩.\langle -10.32,-14.74\rangle+\langle 12,-5\rangle \approx \langle 1.68,-19.74\rangle.

The magnitude is

1.682+(βˆ’19.74)2β‰ˆ19.82.\sqrt{1.68^2+(-19.74)^2}\approx 19.82.

The direction angle is approximately

274.9∘.274.9^\circ.

The particle has

x(t)=2cos⁑tβˆ’sin⁑(2t),y(t)=6sin⁑t.x(t)=2\cos t-\sin(2t),\qquad y(t)=6\sin t.

For part (A), use sin⁑(2t)=2sin⁑tcos⁑t\sin(2t)=2\sin t\cos t:

x(t)=2cos⁑tβˆ’2sin⁑tcos⁑t=2cos⁑t(1βˆ’sin⁑t).x(t)=2\cos t-2\sin t\cos t=2\cos t(1-\sin t).

So x(t)=0x(t)=0 when

cos⁑t=0orsin⁑t=1.\cos t=0\quad \text{or}\quad \sin t=1.

On 0≀t≀2Ο€0\le t\le 2\pi, this gives

t=Ο€2,3Ο€2.t=\frac{\pi}{2},\frac{3\pi}{2}.

The exact xx-intercepts are

(0,6)and(0,βˆ’6).(0,6)\quad \text{and}\quad (0,-6).

For part (B), when t=Ο€2t=\frac{\pi}{2},

(x,y)=(0,6).(x,y)=(0,6).

When t=7Ο€6t=\frac{7\pi}{6},

x=2cos⁑7Ο€6βˆ’sin⁑7Ο€3=βˆ’3βˆ’32=βˆ’332,x=2\cos\frac{7\pi}{6}-\sin\frac{7\pi}{3} =-\sqrt3-\frac{\sqrt3}{2} =-\frac{3\sqrt3}{2},

and

y=6sin⁑7Ο€6=βˆ’3.y=6\sin\frac{7\pi}{6}=-3.

So the position is

(βˆ’332,βˆ’3).\left(-\frac{3\sqrt3}{2},-3\right).

For part (C), the distance from the origin is

d(t)=x(t)2+y(t)2.d(t)=\sqrt{x(t)^2+y(t)^2}.

Therefore,

d(t)=(2cos⁑tβˆ’sin⁑(2t))2+36sin⁑2t.d(t)=\sqrt{(2\cos t-\sin(2t))^2+36\sin^2t}.

Since

x=et,x=e^t,

we have

t=ln⁑x.t=\ln x.

Then

y=e2tβˆ’3=(et)2βˆ’3=x2βˆ’3.y=e^{2t}-3=(e^t)^2-3=x^2-3.

Because

βˆ’ln⁑2≀t≀ln⁑3,-\ln2\le t\le \ln3,

the domain is

12≀x≀3.\frac12\le x\le 3.

The curve is the parabola

y=x2βˆ’3y=x^2-3

restricted to 12≀x≀3\frac12\le x\le 3. As tt increases, x=etx=e^t increases, so the curve moves from

(12,βˆ’114)\left(\frac12,-\frac{11}{4}\right)

to

(3,6).(3,6).

From

x=4cos⁑t,x=4\cos t,

we get

cos⁑t=x4.\cos t=\frac{x}{4}.

From

y=βˆ’2sin⁑t,y=-2\sin t,

we get

sin⁑t=βˆ’y2.\sin t=-\frac{y}{2}.

Using cos⁑2t+sin⁑2t=1\cos^2t+\sin^2t=1,

x216+y24=1.\frac{x^2}{16}+\frac{y^2}{4}=1.

This is an ellipse. At t=0t=0, the curve starts at

(4,0).(4,0).

For small positive tt, y=βˆ’2sin⁑ty=-2\sin t is negative, so the curve moves downward from (4,0)(4,0). Therefore, the ellipse is traced clockwise.

This is an Archimedean spiral:

r=2ΞΈΟ€.r=\frac{2\theta}{\pi}.

As ΞΈ\theta increases from βˆ’4Ο€-4\pi to 4Ο€4\pi, rr increases from βˆ’8-8 to 88. Negative rr values are plotted in the opposite direction from the angle ΞΈ\theta.

ADD IMAGE HERE

The curves are

r=2+2cos⁑θr=2+2\cos\theta

and

r=2βˆ’2cos⁑θ.r=2-2\cos\theta.

Both are cardioids. The first opens to the right, and the second opens to the left.

ADD IMAGE HERE

To find intersections with the same angle, set the equations equal:

2+2cos⁑θ=2βˆ’2cos⁑θ.2+2\cos\theta=2-2\cos\theta.

Then

4cos⁑θ=0,4\cos\theta=0,

so

cos⁑θ=0.\cos\theta=0.

Thus,

ΞΈ=Ο€2,3Ο€2.\theta=\frac{\pi}{2},\frac{3\pi}{2}.

These give the points

(0,2)and(0,βˆ’2).(0,2)\quad \text{and}\quad (0,-2).

Both cardioids also pass through the pole: r=0r=0 for the first curve when ΞΈ=Ο€\theta=\pi, and r=0r=0 for the second curve when ΞΈ=0\theta=0. Therefore, the curves have

3\boxed{3}

intersection points.

For part (A), the resulting octagon is regular, so consecutive vertices differ by an angle of

2Ο€8=Ο€4.\frac{2\pi}{8}=\frac{\pi}{4}.

Since

P1=22,P_1=2\sqrt2,

the first vertex lies on the positive real axis with magnitude 222\sqrt2. The vertices in the third and fourth quadrants can be found by rotating by multiples of 45∘45^\circ.

A third-quadrant vertex occurs at angle 225∘225^\circ:

22(cos⁑225∘+isin⁑225∘)=βˆ’2βˆ’2i.2\sqrt2(\cos225^\circ+i\sin225^\circ)=-2-2i.

A fourth-quadrant vertex occurs at angle 315∘315^\circ:

22(cos⁑315∘+isin⁑315∘)=2βˆ’2i.2\sqrt2(\cos315^\circ+i\sin315^\circ)=2-2i.

For part (B), for a regular polygon centered at the origin, the vertices balance evenly around the circle, so

P1+P2+β‹―+P8=0.P_1+P_2+\cdots+P_8=0.

For part (C), for the product P1P2β‹―P8P_1P_2\cdots P_8, multiply magnitudes and add angles. The magnitude is

(22)8=4096.(2\sqrt2)^8=4096.

The eight angles are

0∘,45∘,90∘,135∘,180∘,225∘,270∘,315∘,0^\circ,45^\circ,90^\circ,135^\circ,180^\circ,225^\circ,270^\circ,315^\circ,

whose sum is

1260∘.1260^\circ.

Since 1260∘1260^\circ is coterminal with 180∘180^\circ,

P1P2β‹―P8=4096(cos⁑180∘+isin⁑180∘).P_1P_2\cdots P_8=4096(\cos180^\circ+i\sin180^\circ).

Therefore,

P1P2β‹―P8=βˆ’4096.P_1P_2\cdots P_8=-4096.

For part (A), for

z1=βˆ’2+23i,z_1=-2+2\sqrt3i,

the magnitude is

∣z1∣=(βˆ’2)2+(23)2=4.\lvert z_1 \rvert=\sqrt{(-2)^2+(2\sqrt3)^2}=4.

Since z1z_1 is in Quadrant II,

ΞΈ1=120∘=2Ο€3.\theta_1=120^\circ=\frac{2\pi}{3}.

So

z1=4(cos⁑2Ο€3+isin⁑2Ο€3).z_1=4\left(\cos\frac{2\pi}{3}+i\sin\frac{2\pi}{3}\right).

For

z2=1βˆ’i,z_2=1-i,

the magnitude is 2\sqrt2 and the angle is βˆ’45∘=βˆ’Ο€4-45^\circ=-\frac{\pi}{4}. So

z2=2(cos⁑(βˆ’Ο€4)+isin⁑(βˆ’Ο€4)).z_2=\sqrt2\left(\cos\left(-\frac{\pi}{4}\right)+i\sin\left(-\frac{\pi}{4}\right)\right).

For part (B), in exponential form,

z1=4e2Ο€i/3,z2=2eβˆ’Ο€i/4.z_1=4e^{2\pi i/3},\qquad z_2=\sqrt2e^{-\pi i/4}.

For part (C), multiply magnitudes and add angles:

z1z2=42ei(2Ο€/3βˆ’Ο€/4)=42e5Ο€i/12.z_1z_2=4\sqrt2e^{i(2\pi/3-\pi/4)}=4\sqrt2e^{5\pi i/12}.

In polar form,

z1z2=42(cos⁑5Ο€12+isin⁑5Ο€12).z_1z_2=4\sqrt2\left(\cos\frac{5\pi}{12}+i\sin\frac{5\pi}{12}\right).

In rectangular form,

z1z2=(23βˆ’2)+(23+2)i.z_1z_2=(2\sqrt3-2)+(2\sqrt3+2)i.

Write the complex number as

16(cos⁑2Ο€3+isin⁑2Ο€3).16\left(\cos\frac{2\pi}{3}+i\sin\frac{2\pi}{3}\right).

The fourth roots have magnitude

164=2.\sqrt[4]{16}=2.

Their angles are

2Ο€3+2Ο€k4=Ο€6+kΟ€2,\frac{\frac{2\pi}{3}+2\pi k}{4} =\frac{\pi}{6}+\frac{k\pi}{2},

where k=0,1,2,3k=0,1,2,3. Therefore the roots are

2cis⁑π6,2cis⁑2Ο€3,2cis⁑7Ο€6,2cis⁑5Ο€3.2\operatorname{cis}\frac{\pi}{6},\quad 2\operatorname{cis}\frac{2\pi}{3},\quad 2\operatorname{cis}\frac{7\pi}{6},\quad 2\operatorname{cis}\frac{5\pi}{3}.

In rectangular form, these are

3+i,βˆ’1+3i,βˆ’3βˆ’i,1βˆ’3i.\sqrt3+i,\quad -1+\sqrt3i,\quad -\sqrt3-i,\quad 1-\sqrt3i.

For part (A), draw diagonal ACAC. The diagonal splits the quadrilateral into triangles ABCABC and ADCADC. Using K=12absin⁑CK=\frac12ab\sin C for triangle area,

[ABC]=12absin⁑B[ABC]=\frac12ab\sin B

and

[ADC]=12cdsin⁑D.[ADC]=\frac12cd\sin D.

Therefore,

K=12absin⁑B+12cdsin⁑D.K=\frac12ab\sin B+\frac12cd\sin D.

Since ABCDABCD is cyclic, opposite angles are supplementary:

B+D=180∘.B+D=180^\circ.

So

D=180βˆ˜βˆ’BD=180^\circ-B

and

sin⁑D=sin⁑(180βˆ˜βˆ’B)=sin⁑B.\sin D=\sin(180^\circ-B)=\sin B.

Therefore,

K=12absin⁑B+12cdsin⁑B=12(ab+cd)sin⁑B.K=\frac12ab\sin B+\frac12cd\sin B =\frac12(ab+cd)\sin B.

For part (B), apply the Law of Cosines to triangle ABCABC:

AC2=a2+b2βˆ’2abcos⁑B.AC^2=a^2+b^2-2ab\cos B.

Apply the Law of Cosines to triangle ADCADC:

AC2=c2+d2βˆ’2cdcos⁑D.AC^2=c^2+d^2-2cd\cos D.

Set these equal:

a2+b2βˆ’2abcos⁑B=c2+d2βˆ’2cdcos⁑D.a^2+b^2-2ab\cos B=c^2+d^2-2cd\cos D.

Rearranging gives

2abcos⁑B=a2+b2βˆ’c2βˆ’d2+2cdcos⁑D.2ab\cos B=a^2+b^2-c^2-d^2+2cd\cos D.

For part (C), since D=180βˆ˜βˆ’BD=180^\circ-B,

cos⁑D=βˆ’cos⁑B.\cos D=-\cos B.

Substitute into the result from part (C)(C):

2abcos⁑B=a2+b2βˆ’c2βˆ’d2βˆ’2cdcos⁑B.2ab\cos B=a^2+b^2-c^2-d^2-2cd\cos B.

So

2(ab+cd)cos⁑B=a2+b2βˆ’c2βˆ’d2,2(ab+cd)\cos B=a^2+b^2-c^2-d^2,

and

cos⁑B=a2+b2βˆ’c2βˆ’d22(ab+cd).\cos B=\frac{a^2+b^2-c^2-d^2}{2(ab+cd)}.

From part (B)(B),

K=12(ab+cd)sin⁑B.K=\frac12(ab+cd)\sin B.

Square both sides:

K2=14(ab+cd)2sin⁑2B.K^2=\frac14(ab+cd)^2\sin^2B.

Use sin⁑2B=1βˆ’cos⁑2B\sin^2B=1-\cos^2B:

K2=14(ab+cd)2(1βˆ’(a2+b2βˆ’c2βˆ’d22(ab+cd))2).K^2=\frac14(ab+cd)^2\left(1-\left(\frac{a^2+b^2-c^2-d^2}{2(ab+cd)}\right)^2\right).

Simplifying gives

K2=4(ab+cd)2βˆ’(a2+b2βˆ’c2βˆ’d2)216.K^2=\frac{4(ab+cd)^2-(a^2+b^2-c^2-d^2)^2}{16}.

This factors as

K2=(a+b+cβˆ’d)(a+bβˆ’c+d)(aβˆ’b+c+d)(βˆ’a+b+c+d)16.K^2=\frac{(a+b+c-d)(a+b-c+d)(a-b+c+d)(-a+b+c+d)}{16}.

Since

s=12(a+b+c+d),s=\frac12(a+b+c+d),

the four factors are

2(sβˆ’d),2(sβˆ’c),2(sβˆ’b),2(sβˆ’a).2(s-d),\quad 2(s-c),\quad 2(s-b),\quad 2(s-a).

Therefore,

K2=(sβˆ’a)(sβˆ’b)(sβˆ’c)(sβˆ’d),K^2=(s-a)(s-b)(s-c)(s-d),

so

K=(sβˆ’a)(sβˆ’b)(sβˆ’c)(sβˆ’d).K=\sqrt{(s-a)(s-b)(s-c)(s-d)}.

For part (D), for a general quadrilateral, the area is still

K=12absin⁑B+12cdsin⁑D,K=\frac12ab\sin B+\frac12cd\sin D,

so

4K=2absin⁑B+2cdsin⁑D.4K=2ab\sin B+2cd\sin D.

Also, using the shared diagonal ACAC again,

a2+b2βˆ’2abcos⁑B=c2+d2βˆ’2cdcos⁑D.a^2+b^2-2ab\cos B=c^2+d^2-2cd\cos D.

Thus,

a2+b2βˆ’c2βˆ’d2=2abcos⁑Bβˆ’2cdcos⁑D.a^2+b^2-c^2-d^2=2ab\cos B-2cd\cos D.

Now compute

(4K)2+(a2+b2βˆ’c2βˆ’d2)2.(4K)^2+(a^2+b^2-c^2-d^2)^2.

Substitute the two expressions above:

(2absin⁑B+2cdsin⁑D)2+(2abcos⁑Bβˆ’2cdcos⁑D)2.(2ab\sin B+2cd\sin D)^2+(2ab\cos B-2cd\cos D)^2.

Expand:

4a2b2sin⁑2B+8abcdsin⁑Bsin⁑D+4c2d2sin⁑2D4a^2b^2\sin^2B+8abcd\sin B\sin D+4c^2d^2\sin^2D +4a2b2cos⁑2Bβˆ’8abcdcos⁑Bcos⁑D+4c2d2cos⁑2D.+4a^2b^2\cos^2B-8abcd\cos B\cos D+4c^2d^2\cos^2D.

Group terms:

4a2b2(sin⁑2B+cos⁑2B)+4c2d2(sin⁑2D+cos⁑2D)4a^2b^2(\sin^2B+\cos^2B)+4c^2d^2(\sin^2D+\cos^2D) +8abcd(sin⁑Bsin⁑Dβˆ’cos⁑Bcos⁑D).+8abcd(\sin B\sin D-\cos B\cos D).

Since

sin⁑2x+cos⁑2x=1\sin^2x+\cos^2x=1

and

cos⁑(B+D)=cos⁑Bcos⁑Dβˆ’sin⁑Bsin⁑D,\cos(B+D)=\cos B\cos D-\sin B\sin D,

this becomes

4a2b2+4c2d2βˆ’8abcdcos⁑(B+D).4a^2b^2+4c^2d^2-8abcd\cos(B+D).

Therefore,

(4K)2+(a2+b2βˆ’c2βˆ’d2)2=4(a2b2+c2d2βˆ’2abcdcos⁑(B+D)).(4K)^2+(a^2+b^2-c^2-d^2)^2=4(a^2b^2+c^2d^2-2abcd\cos(B+D)).

For part (E), rearrange the result from part (D):

16K2=4(a2b2+c2d2βˆ’2abcdcos⁑(B+D))βˆ’(a2+b2βˆ’c2βˆ’d2)2.16K^2=4(a^2b^2+c^2d^2-2abcd\cos(B+D))-(a^2+b^2-c^2-d^2)^2.

Use

cos⁑(B+D)=2cos⁑2(B+D2)βˆ’1.\cos(B+D)=2\cos^2\left(\frac{B+D}{2}\right)-1.

Then

βˆ’2abcdcos⁑(B+D)=βˆ’4abcdcos⁑2(B+D2)+2abcd.-2abcd\cos(B+D) =-4abcd\cos^2\left(\frac{B+D}{2}\right)+2abcd.

So

16K2=4(a2b2+c2d2+2abcd)βˆ’(a2+b2βˆ’c2βˆ’d2)216K^2=4(a^2b^2+c^2d^2+2abcd)-(a^2+b^2-c^2-d^2)^2 βˆ’16abcdcos⁑2(B+D2).-16abcd\cos^2\left(\frac{B+D}{2}\right).

Since

4(a2b2+c2d2+2abcd)=4(ab+cd)2,4(a^2b^2+c^2d^2+2abcd)=4(ab+cd)^2,

we get

16K2=4(ab+cd)2βˆ’(a2+b2βˆ’c2βˆ’d2)2βˆ’16abcdcos⁑2(B+D2).16K^2=4(ab+cd)^2-(a^2+b^2-c^2-d^2)^2 -16abcd\cos^2\left(\frac{B+D}{2}\right).

From part (D)(D), the first two terms factor as

16(sβˆ’a)(sβˆ’b)(sβˆ’c)(sβˆ’d).16(s-a)(s-b)(s-c)(s-d).

Therefore,

16K2=16(sβˆ’a)(sβˆ’b)(sβˆ’c)(sβˆ’d)βˆ’16abcdcos⁑2(B+D2).16K^2=16(s-a)(s-b)(s-c)(s-d) -16abcd\cos^2\left(\frac{B+D}{2}\right).

Divide by 1616:

K2=(sβˆ’a)(sβˆ’b)(sβˆ’c)(sβˆ’d)βˆ’abcdcos⁑2(B+D2).K^2=(s-a)(s-b)(s-c)(s-d)-abcd\cos^2\left(\frac{B+D}{2}\right).

This is Bretschneider’s formula.

For part (F), if ABCDABCD is cyclic, then opposite angles are supplementary:

B+D=180∘.B+D=180^\circ.

Thus,

B+D2=90∘,\frac{B+D}{2}=90^\circ,

so

cos⁑2(B+D2)=cos⁑2(90∘)=0.\cos^2\left(\frac{B+D}{2}\right)=\cos^2(90^\circ)=0.

Bretschneider’s formula becomes

K2=(sβˆ’a)(sβˆ’b)(sβˆ’c)(sβˆ’d),K^2=(s-a)(s-b)(s-c)(s-d),

which is Brahmagupta’s formula.

Full notes β†’

  1. Solve the system using Gaussian elimination:

    {2xβˆ’y+3z=9x+2yβˆ’z=23x+y+z=8\begin{cases} 2x-y+3z=9\\ x+2y-z=2\\ 3x+y+z=8 \end{cases}
  2. Solve the system and classify it as having one solution, no solution, or infinitely many solutions:

    {x+2yβˆ’z=42x+4yβˆ’2z=83xβˆ’y+z=1\begin{cases} x+2y-z=4\\ 2x+4y-2z=8\\ 3x-y+z=1 \end{cases}
  3. Find all values of kk for which the system has no unique solution:

    {kx+2y=68x+ky=12\begin{cases} kx+2y=6\\ 8x+ky=12 \end{cases}

    For each such value of kk, determine whether the system has no solution or infinitely many solutions.

  4. Let

    A=[2βˆ’134],B=[05βˆ’21].A=\begin{bmatrix}2&-1\\3&4\end{bmatrix}, \qquad B=\begin{bmatrix}0&5\\-2&1\end{bmatrix}.

    Compute 2Aβˆ’3B2A-3B, ABAB, and BABA.

  5. Let

    A=[1203],B=[abcd].A=\begin{bmatrix}1&2\\0&3\end{bmatrix}, \qquad B=\begin{bmatrix}a&b\\c&d\end{bmatrix}.

    Find all matrices BB such that AB=BAAB=BA.

  6. Find Aβˆ’1A^{-1}, if it exists, and use it to solve AX=BAX=B:

    A=[4725],B=[1βˆ’3].A=\begin{bmatrix}4&7\\2&5\end{bmatrix}, \qquad B=\begin{bmatrix}1\\-3\end{bmatrix}.
  7. Find the inverse of

    A=[120013002].A=\begin{bmatrix} 1&2&0\\ 0&1&3\\ 0&0&2 \end{bmatrix}.
  8. Find all values of tt for which the matrix is singular:

    A=[t102t103t].A=\begin{bmatrix} t&1&0\\ 2&t&1\\ 0&3&t \end{bmatrix}.
  9. Use Cramer’s Rule to solve:

    {3xβˆ’2y=115x+4y=7\begin{cases} 3x-2y=11\\ 5x+4y=7 \end{cases}
  10. A quadratic function f(x)=ax2+bx+cf(x)=ax^2+bx+c passes through (βˆ’1,6)(-1,6), (2,3)(2,3), and (4,15)(4,15). Use a system of equations to find a,b,ca,b,c.

  11. Solve the nonlinear system:

    {x2+y2=25xβˆ’y=1\begin{cases} x^2+y^2=25\\ x-y=1 \end{cases}
  12. Solve the nonlinear system:

    {xy=12x+y=8\begin{cases} xy=12\\ x+y=8 \end{cases}
  13. Find the vertices and area of the region satisfying

    {xβ‰₯0yβ‰₯0x+2y≀83x+y≀9\begin{cases} x\ge 0\\ y\ge 0\\ x+2y\le 8\\ 3x+y\le 9 \end{cases}
  14. A matrix transformation sends the point (x,y)(x,y) to

    [xβ€²yβ€²]=[2βˆ’111][xy].\begin{bmatrix} x'\\ y' \end{bmatrix} = \begin{bmatrix} 2&-1\\ 1&1 \end{bmatrix} \begin{bmatrix} x\\ y \end{bmatrix}.

    Find the original point (x,y)(x,y) that maps to (7,5)(7,5). Then find the image of the line y=2x+1y=2x+1 under this transformation.

  15. A small economy has two sectors: food and tools. Producing one unit of food requires 0.200.20 units of food and 0.100.10 units of tools. Producing one unit of tools requires 0.300.30 units of food and 0.200.20 units of tools. External demand is 110110 units of food and 8080 units of tools. Let FF and TT be the total production levels. Set up and solve the matrix equation for FF and TT.

  16. Extension (Cayley-Hamilton and Matrix Powers). Let

    A=[abcd],tr⁑(A)=a+d,det⁑(A)=adβˆ’bc.A=\begin{bmatrix}a&b\\c&d\end{bmatrix}, \qquad \operatorname{tr}(A)=a+d, \qquad \det(A)=ad-bc.

    (A)(A) Prove the Cayley-Hamilton identity

    A2βˆ’tr⁑(A)A+det⁑(A)I=0.A^2-\operatorname{tr}(A)A+\det(A)I=0.

    (B)(B) Use part (A)(A) to derive the inverse formula for AA when det⁑(A)β‰ 0\det(A)\ne 0.

    (C)(C) Explain why every power AnA^n for nβ‰₯2n\ge 2 can be rewritten in the form

    An=Ξ±nA+Ξ²nIA^n=\alpha_n A+\beta_n I

    for some constants Ξ±n\alpha_n and Ξ²n\beta_n.

    (D)(D) Let

    M=[2111].M=\begin{bmatrix}2&1\\1&1\end{bmatrix}.

    Use part (C)(C) to compute M6M^6 without multiplying six matrices directly.


Start with the augmented matrix:

[2βˆ’13912βˆ’123118].\left[ \begin{array}{ccc|c} 2&-1&3&9\\ 1&2&-1&2\\ 3&1&1&8 \end{array} \right].

Swap rows 11 and 22:

[12βˆ’122βˆ’1393118].\left[ \begin{array}{ccc|c} 1&2&-1&2\\ 2&-1&3&9\\ 3&1&1&8 \end{array} \right].

Eliminate below the first pivot:

R2←R2βˆ’2R1,R3←R3βˆ’3R1.R_2\leftarrow R_2-2R_1,\qquad R_3\leftarrow R_3-3R_1.

Then

[12βˆ’120βˆ’5550βˆ’542].\left[ \begin{array}{ccc|c} 1&2&-1&2\\ 0&-5&5&5\\ 0&-5&4&2 \end{array} \right].

Subtract row 22 from row 33:

[12βˆ’120βˆ’55500βˆ’1βˆ’3].\left[ \begin{array}{ccc|c} 1&2&-1&2\\ 0&-5&5&5\\ 0&0&-1&-3 \end{array} \right].

The last row gives

βˆ’z=βˆ’3,-z=-3,

so

z=3.z=3.

From row 22,

βˆ’5y+5z=5.-5y+5z=5.

Thus

βˆ’5y+15=5,-5y+15=5,

so

y=2.y=2.

From row 11,

x+2yβˆ’z=2.x+2y-z=2.

Therefore

x+4βˆ’3=2,x+4-3=2,

so x=1x=1. The solution is

(1,2,3).\boxed{(1,2,3)}.

The second equation is exactly 22 times the first equation, so it does not add new information. Use the first and third equations:

{x+2yβˆ’z=43xβˆ’y+z=1\begin{cases} x+2y-z=4\\ 3x-y+z=1 \end{cases}

Let z=tz=t. Then

x+2y=4+tx+2y=4+t

and

3xβˆ’y=1βˆ’t.3x-y=1-t.

From the first equation,

x=4+tβˆ’2y.x=4+t-2y.

Substitute:

3(4+tβˆ’2y)βˆ’y=1βˆ’t.3(4+t-2y)-y=1-t.

Then

12+3tβˆ’7y=1βˆ’t,12+3t-7y=1-t,

so

7y=11+4t,y=11+4t7.7y=11+4t, \qquad y=\frac{11+4t}{7}.

Now

x=4+tβˆ’2(11+4t7)=6βˆ’t7.x=4+t-2\left(\frac{11+4t}{7}\right)=\frac{6-t}{7}.

Thus the system has infinitely many solutions:

(x,y,z)=(6βˆ’t7,11+4t7,t),t∈R.\boxed{(x,y,z)=\left(\frac{6-t}{7},\frac{11+4t}{7},t\right),\quad t\in\mathbb R}.

The coefficient matrix is

[k28k].\begin{bmatrix} k&2\\ 8&k \end{bmatrix}.

The system has no unique solution when the determinant is zero:

k2βˆ’16=0.k^2-16=0.

Thus

k=Β±4.k=\pm4.

If k=4k=4, the system is

{4x+2y=68x+4y=12\begin{cases} 4x+2y=6\\ 8x+4y=12 \end{cases}

and the second equation is 22 times the first. So there are infinitely many solutions.

If k=βˆ’4k=-4, the system is

{βˆ’4x+2y=68xβˆ’4y=12\begin{cases} -4x+2y=6\\ 8x-4y=12 \end{cases}

Multiplying the first equation by βˆ’2-2 gives

8xβˆ’4y=βˆ’12,8x-4y=-12,

which contradicts 8xβˆ’4y=128x-4y=12. So there is no solution.

Therefore:

k=4Β givesΒ infinitelyΒ manyΒ solutions,Β andΒ k=βˆ’4Β givesΒ noΒ solution.\boxed{k=4\text{ gives infinitely many solutions, and }k=-4\text{ gives no solution}.}

First,

2A=[4βˆ’268],3B=[015βˆ’63].2A= \begin{bmatrix} 4&-2\\ 6&8 \end{bmatrix}, \qquad 3B= \begin{bmatrix} 0&15\\ -6&3 \end{bmatrix}.

So

2Aβˆ’3B=[4βˆ’17125].2A-3B= \begin{bmatrix} 4&-17\\ 12&5 \end{bmatrix}.

Next,

AB=[2βˆ’134][05βˆ’21]=[29βˆ’819].AB= \begin{bmatrix} 2&-1\\ 3&4 \end{bmatrix} \begin{bmatrix} 0&5\\ -2&1 \end{bmatrix} = \begin{bmatrix} 2&9\\ -8&19 \end{bmatrix}.

Also,

BA=[05βˆ’21][2βˆ’134]=[1520βˆ’16].BA= \begin{bmatrix} 0&5\\ -2&1 \end{bmatrix} \begin{bmatrix} 2&-1\\ 3&4 \end{bmatrix} = \begin{bmatrix} 15&20\\ -1&6 \end{bmatrix}.

Thus

2Aβˆ’3B=[4βˆ’17125],AB=[29βˆ’819],BA=[1520βˆ’16].\boxed{ 2A-3B= \begin{bmatrix} 4&-17\\ 12&5 \end{bmatrix}, \quad AB= \begin{bmatrix} 2&9\\ -8&19 \end{bmatrix}, \quad BA= \begin{bmatrix} 15&20\\ -1&6 \end{bmatrix} }.

Compute ABAB:

AB=[1203][abcd]=[a+2cb+2d3c3d].AB= \begin{bmatrix} 1&2\\ 0&3 \end{bmatrix} \begin{bmatrix} a&b\\ c&d \end{bmatrix} = \begin{bmatrix} a+2c&b+2d\\ 3c&3d \end{bmatrix}.

Compute BABA:

BA=[abcd][1203]=[a2a+3bc2c+3d].BA= \begin{bmatrix} a&b\\ c&d \end{bmatrix} \begin{bmatrix} 1&2\\ 0&3 \end{bmatrix} = \begin{bmatrix} a&2a+3b\\ c&2c+3d \end{bmatrix}.

Set corresponding entries equal:

a+2c=a,b+2d=2a+3b,3c=c,3d=2c+3d.a+2c=a,\qquad b+2d=2a+3b,\qquad 3c=c,\qquad 3d=2c+3d.

The first and third equations give c=0c=0. Then the fourth is automatically true. The second equation gives

2d=2a+2b,2d=2a+2b,

so

d=a+b.d=a+b.

Therefore

B=[ab0a+b]Β forΒ anyΒ realΒ numbersΒ a,b.\boxed{ B= \begin{bmatrix} a&b\\ 0&a+b \end{bmatrix} \text{ for any real numbers }a,b. }

The determinant is

4(5)βˆ’7(2)=6.4(5)-7(2)=6.

Since the determinant is nonzero, the inverse exists:

Aβˆ’1=16[5βˆ’7βˆ’24].A^{-1} = \frac16 \begin{bmatrix} 5&-7\\ -2&4 \end{bmatrix}.

Then

X=Aβˆ’1B=16[5βˆ’7βˆ’24][1βˆ’3].X=A^{-1}B = \frac16 \begin{bmatrix} 5&-7\\ -2&4 \end{bmatrix} \begin{bmatrix} 1\\ -3 \end{bmatrix}.

Compute:

X=16[5+21βˆ’2βˆ’12]=16[26βˆ’14]=[13/3βˆ’7/3].X= \frac16 \begin{bmatrix} 5+21\\ -2-12 \end{bmatrix} = \frac16 \begin{bmatrix} 26\\ -14 \end{bmatrix} = \begin{bmatrix} 13/3\\ -7/3 \end{bmatrix}.

So

Aβˆ’1=16[5βˆ’7βˆ’24]andX=[13/3βˆ’7/3].\boxed{A^{-1}=\frac16 \begin{bmatrix} 5&-7\\ -2&4 \end{bmatrix} \quad\text{and}\quad X= \begin{bmatrix} 13/3\\ -7/3 \end{bmatrix}.}

Let

Aβˆ’1=[pqrstuvwn].A^{-1}= \begin{bmatrix} p&q&r\\ s&t&u\\ v&w&n \end{bmatrix}.

Since AA is upper triangular, solve by row-reducing [A∣I][A\mid I]:

[120100013010002001].\left[ \begin{array}{ccc|ccc} 1&2&0&1&0&0\\ 0&1&3&0&1&0\\ 0&0&2&0&0&1 \end{array} \right].

Make the third pivot 11:

R3←12R3R_3\leftarrow \frac12R_3

so

[120100013010001001/2].\left[ \begin{array}{ccc|ccc} 1&2&0&1&0&0\\ 0&1&3&0&1&0\\ 0&0&1&0&0&1/2 \end{array} \right].

Eliminate above the third pivot:

R2←R2βˆ’3R3.R_2\leftarrow R_2-3R_3.

Then

[12010001001βˆ’3/2001001/2].\left[ \begin{array}{ccc|ccc} 1&2&0&1&0&0\\ 0&1&0&0&1&-3/2\\ 0&0&1&0&0&1/2 \end{array} \right].

Eliminate above the second pivot:

R1←R1βˆ’2R2.R_1\leftarrow R_1-2R_2.

Then

[1001βˆ’2301001βˆ’3/2001001/2].\left[ \begin{array}{ccc|ccc} 1&0&0&1&-2&3\\ 0&1&0&0&1&-3/2\\ 0&0&1&0&0&1/2 \end{array} \right].

Thus

Aβˆ’1=[1βˆ’2301βˆ’3/2001/2].\boxed{ A^{-1}= \begin{bmatrix} 1&-2&3\\ 0&1&-3/2\\ 0&0&1/2 \end{bmatrix} }.

Compute the determinant:

det⁑(A)=∣t102t103t∣.\det(A) = \begin{vmatrix} t&1&0\\ 2&t&1\\ 0&3&t \end{vmatrix}.

Expand along the first row:

det⁑(A)=t∣t13tβˆ£βˆ’1∣210t∣.\det(A) = t \begin{vmatrix} t&1\\ 3&t \end{vmatrix} - 1 \begin{vmatrix} 2&1\\ 0&t \end{vmatrix}.

So

det⁑(A)=t(t2βˆ’3)βˆ’2t=t3βˆ’5t=t(t2βˆ’5).\det(A)=t(t^2-3)-2t=t^3-5t=t(t^2-5).

The matrix is singular when det⁑(A)=0\det(A)=0:

t(t2βˆ’5)=0.t(t^2-5)=0.

Therefore

t=0,Β 5,Β βˆ’5.\boxed{t=0,\ \sqrt5,\ -\sqrt5}.

Compute

D=∣3βˆ’254∣=3(4)βˆ’(βˆ’2)(5)=22.D= \begin{vmatrix} 3&-2\\ 5&4 \end{vmatrix} =3(4)-(-2)(5)=22.

Then

Dx=∣11βˆ’274∣=11(4)βˆ’(βˆ’2)(7)=58,D_x= \begin{vmatrix} 11&-2\\ 7&4 \end{vmatrix} =11(4)-(-2)(7)=58,

and

Dy=∣31157∣=3(7)βˆ’11(5)=βˆ’34.D_y= \begin{vmatrix} 3&11\\ 5&7 \end{vmatrix} =3(7)-11(5)=-34.

Thus

x=DxD=5822=2911,y=DyD=βˆ’3422=βˆ’1711.x=\frac{D_x}{D}=\frac{58}{22}=\frac{29}{11}, \qquad y=\frac{D_y}{D}=\frac{-34}{22}=-\frac{17}{11}.

So

(2911,βˆ’1711).\boxed{\left(\frac{29}{11},-\frac{17}{11}\right)}.

Use the three points in f(x)=ax2+bx+cf(x)=ax^2+bx+c.

For (βˆ’1,6)(-1,6):

aβˆ’b+c=6.a-b+c=6.

For (2,3)(2,3):

4a+2b+c=3.4a+2b+c=3.

For (4,15)(4,15):

16a+4b+c=15.16a+4b+c=15.

Subtract the first equation from the second:

3a+3b=βˆ’3,3a+3b=-3,

so

a+b=βˆ’1.a+b=-1.

Subtract the second equation from the third:

12a+2b=12,12a+2b=12,

so

6a+b=6.6a+b=6.

Subtract a+b=βˆ’1a+b=-1 from 6a+b=66a+b=6:

5a=7,5a=7,

so

a=75.a=\frac75.

Then

b=βˆ’1βˆ’75=βˆ’125.b=-1-\frac75=-\frac{12}{5}.

Use aβˆ’b+c=6a-b+c=6:

75βˆ’(βˆ’125)+c=6,\frac75-\left(-\frac{12}{5}\right)+c=6,

so

195+c=6,c=115.\frac{19}{5}+c=6, \qquad c=\frac{11}{5}.

Therefore

f(x)=75x2βˆ’125x+115.\boxed{f(x)=\frac75x^2-\frac{12}{5}x+\frac{11}{5}}.

From xβˆ’y=1x-y=1,

x=y+1.x=y+1.

Substitute into x2+y2=25x^2+y^2=25:

(y+1)2+y2=25.(y+1)^2+y^2=25.

Then

2y2+2y+1=25,2y^2+2y+1=25,

so

2y2+2yβˆ’24=0.2y^2+2y-24=0.

Divide by 22:

y2+yβˆ’12=0.y^2+y-12=0.

Factor:

(y+4)(yβˆ’3)=0.(y+4)(y-3)=0.

Thus y=βˆ’4y=-4 or y=3y=3. Since x=y+1x=y+1, the solutions are

(βˆ’3,βˆ’4)Β andΒ (4,3).\boxed{(-3,-4)\text{ and }(4,3)}.

Since

x+y=8x+y=8

and

xy=12,xy=12,

the numbers xx and yy are roots of the quadratic

t2βˆ’8t+12=0.t^2-8t+12=0.

Factor:

(tβˆ’2)(tβˆ’6)=0.(t-2)(t-6)=0.

So the two numbers are 22 and 66. Therefore

(x,y)=(2,6)Β orΒ (6,2).\boxed{(x,y)=(2,6)\text{ or }(6,2)}.

The region is in the first quadrant and below both lines:

x+2y=8x+2y=8

and

3x+y=9.3x+y=9.

The intercepts on the axes are:

  • On the xx-axis: 3x+y≀93x+y\le 9 gives x≀3x\le 3, so the vertex is (3,0)(3,0).
  • On the yy-axis: x+2y≀8x+2y\le 8 gives y≀4y\le 4, so the vertex is (0,4)(0,4).

Find the intersection of the two boundary lines:

{x+2y=83x+y=9\begin{cases} x+2y=8\\ 3x+y=9 \end{cases}

From the first equation, x=8βˆ’2yx=8-2y. Substitute:

3(8βˆ’2y)+y=9.3(8-2y)+y=9.

Then

24βˆ’5y=9,24-5y=9,

so

y=3.y=3.

Then

x=8βˆ’2(3)=2.x=8-2(3)=2.

The vertices are

(0,0),(3,0),(2,3),(0,4).(0,0),\quad (3,0),\quad (2,3),\quad (0,4).

Use the shoelace formula:

Area=12∣(0β‹…0+3β‹…3+2β‹…4+0β‹…0)βˆ’(0β‹…3+0β‹…2+3β‹…0+4β‹…0)∣.\text{Area} =\frac12\left|(0\cdot0+3\cdot3+2\cdot4+0\cdot0)-(0\cdot3+0\cdot2+3\cdot0+4\cdot0)\right|.

Thus

Area=12(9+8)=172.\text{Area}=\frac12(9+8)=\frac{17}{2}.

So

verticesΒ (0,0),(3,0),(2,3),(0,4)Β andΒ areaΒ 172.\boxed{\text{vertices }(0,0),(3,0),(2,3),(0,4)\text{ and area }\frac{17}{2}}.

We need

[2βˆ’111][xy]=[75].\begin{bmatrix} 2&-1\\ 1&1 \end{bmatrix} \begin{bmatrix} x\\ y \end{bmatrix} = \begin{bmatrix} 7\\ 5 \end{bmatrix}.

This gives

{2xβˆ’y=7x+y=5\begin{cases} 2x-y=7\\ x+y=5 \end{cases}

Add the equations:

3x=12,3x=12,

so x=4x=4. Then y=1y=1. The original point is

(4,1).\boxed{(4,1)}.

Now let points on the original line be written as

(x,y)=(x,2x+1).(x,y)=(x,2x+1).

The transformed coordinates satisfy

xβ€²=2xβˆ’y=2xβˆ’(2x+1)=βˆ’1,x'=2x-y=2x-(2x+1)=-1,

and

yβ€²=x+y=x+(2x+1)=3x+1.y'=x+y=x+(2x+1)=3x+1.

As xx varies, yβ€²y' varies freely, but xβ€²x' is always βˆ’1-1. Therefore the image of the line is

xβ€²=βˆ’1.\boxed{x'=-1}.

The total production must satisfy internal demand plus external demand.

Food production:

F=0.20F+0.30T+110.F=0.20F+0.30T+110.

Tools production:

T=0.10F+0.20T+80.T=0.10F+0.20T+80.

Move internal demand terms to the left:

0.80Fβˆ’0.30T=110,0.80F-0.30T=110,

and

βˆ’0.10F+0.80T=80.-0.10F+0.80T=80.

In matrix form:

[0.80βˆ’0.30βˆ’0.100.80][FT]=[11080].\begin{bmatrix} 0.80&-0.30\\ -0.10&0.80 \end{bmatrix} \begin{bmatrix} F\\ T \end{bmatrix} = \begin{bmatrix} 110\\ 80 \end{bmatrix}.

Clear decimals by multiplying both equations by 1010:

{8Fβˆ’3T=1100βˆ’F+8T=800\begin{cases} 8F-3T=1100\\ -F+8T=800 \end{cases}

From the second equation,

F=8Tβˆ’800.F=8T-800.

Substitute into the first:

8(8Tβˆ’800)βˆ’3T=1100.8(8T-800)-3T=1100.

Then

64Tβˆ’6400βˆ’3T=1100,64T-6400-3T=1100,

so

61T=7500.61T=7500.

Thus

T=750061.T=\frac{7500}{61}.

Then

F=8(750061)βˆ’800=6000061βˆ’4880061=1120061.F=8\left(\frac{7500}{61}\right)-800 =\frac{60000}{61}-\frac{48800}{61} =\frac{11200}{61}.

So the required production levels are

F=1120061β‰ˆ183.61,T=750061β‰ˆ122.95.\boxed{F=\frac{11200}{61}\approx 183.61,\qquad T=\frac{7500}{61}\approx 122.95}.

Part (A)(A). Compute A2A^2:

A2=[abcd][abcd]=[a2+bcab+bdac+cdbc+d2].A^2= \begin{bmatrix} a&b\\ c&d \end{bmatrix} \begin{bmatrix} a&b\\ c&d \end{bmatrix} = \begin{bmatrix} a^2+bc&ab+bd\\ ac+cd&bc+d^2 \end{bmatrix}.

Also,

tr⁑(A)A=(a+d)[abcd]=[a2+adab+bdac+cdad+d2].\operatorname{tr}(A)A =(a+d) \begin{bmatrix} a&b\\ c&d \end{bmatrix} = \begin{bmatrix} a^2+ad&ab+bd\\ ac+cd&ad+d^2 \end{bmatrix}.

Finally,

det⁑(A)I=(adβˆ’bc)[1001]=[adβˆ’bc00adβˆ’bc].\det(A)I =(ad-bc) \begin{bmatrix} 1&0\\ 0&1 \end{bmatrix} = \begin{bmatrix} ad-bc&0\\ 0&ad-bc \end{bmatrix}.

Now compute

A2βˆ’tr⁑(A)A+det⁑(A)I.A^2-\operatorname{tr}(A)A+\det(A)I.

The top-left entry is

(a2+bc)βˆ’(a2+ad)+(adβˆ’bc)=0.(a^2+bc)-(a^2+ad)+(ad-bc)=0.

The top-right entry is

(ab+bd)βˆ’(ab+bd)+0=0.(ab+bd)-(ab+bd)+0=0.

The bottom-left entry is

(ac+cd)βˆ’(ac+cd)+0=0.(ac+cd)-(ac+cd)+0=0.

The bottom-right entry is

(bc+d2)βˆ’(ad+d2)+(adβˆ’bc)=0.(bc+d^2)-(ad+d^2)+(ad-bc)=0.

Thus

A2βˆ’tr⁑(A)A+det⁑(A)I=0.\boxed{A^2-\operatorname{tr}(A)A+\det(A)I=0}.

Part (B)(B). Now suppose det⁑(A)β‰ 0\det(A)\ne 0. Rearrange the identity:

A2βˆ’tr⁑(A)A=βˆ’det⁑(A)I.A^2-\operatorname{tr}(A)A=-\det(A)I.

Factor out AA on the left:

A(Aβˆ’tr⁑(A)I)=βˆ’det⁑(A)I.A(A-\operatorname{tr}(A)I)=-\det(A)I.

Multiply both sides by βˆ’1det⁑(A)-\frac{1}{\det(A)}:

A(tr⁑(A)Iβˆ’Adet⁑(A))=I.A\left(\frac{\operatorname{tr}(A)I-A}{\det(A)}\right)=I.

So

Aβˆ’1=tr⁑(A)Iβˆ’Adet⁑(A).A^{-1}=\frac{\operatorname{tr}(A)I-A}{\det(A)}.

Since

tr⁑(A)Iβˆ’A=[a+d00a+d]βˆ’[abcd]=[dβˆ’bβˆ’ca],\operatorname{tr}(A)I-A = \begin{bmatrix} a+d&0\\ 0&a+d \end{bmatrix} - \begin{bmatrix} a&b\\ c&d \end{bmatrix} = \begin{bmatrix} d&-b\\ -c&a \end{bmatrix},

we get the usual inverse formula:

Aβˆ’1=1adβˆ’bc[dβˆ’bβˆ’ca].\boxed{ A^{-1} = \frac{1}{ad-bc} \begin{bmatrix} d&-b\\ -c&a \end{bmatrix} }.

Part (C)(C). From part (A)(A),

A2=tr⁑(A)Aβˆ’det⁑(A)I.A^2=\operatorname{tr}(A)A-\det(A)I.

This already writes A2A^2 as a linear combination of AA and II.

Now multiply both sides by AA:

A3=tr⁑(A)A2βˆ’det⁑(A)A.A^3=\operatorname{tr}(A)A^2-\det(A)A.

Since A2A^2 is already a combination of AA and II, this means A3A^3 is also a combination of AA and II.

More generally, multiply the Cayley-Hamilton identity by Anβˆ’2A^{n-2}:

Anβˆ’tr⁑(A)Anβˆ’1+det⁑(A)Anβˆ’2=0.A^n-\operatorname{tr}(A)A^{n-1}+\det(A)A^{n-2}=0.

So

An=tr⁑(A)Anβˆ’1βˆ’det⁑(A)Anβˆ’2.A^n=\operatorname{tr}(A)A^{n-1}-\det(A)A^{n-2}.

If Anβˆ’1A^{n-1} and Anβˆ’2A^{n-2} are both combinations of AA and II, then AnA^n is too. Therefore every power AnA^n with nβ‰₯2n\ge 2 can be written as

An=Ξ±nA+Ξ²nI.\boxed{A^n=\alpha_n A+\beta_n I}.

Part (D)(D). For

M=[2111],M=\begin{bmatrix}2&1\\1&1\end{bmatrix},

the trace is

tr⁑(M)=3,\operatorname{tr}(M)=3,

and the determinant is

det⁑(M)=2(1)βˆ’1(1)=1.\det(M)=2(1)-1(1)=1.

So Cayley-Hamilton gives

M2βˆ’3M+I=0,M^2-3M+I=0,

or

M2=3Mβˆ’I.M^2=3M-I.

Use the recurrence

Mn=3Mnβˆ’1βˆ’Mnβˆ’2.M^n=3M^{n-1}-M^{n-2}.

Start:

M0=I,M1=M.M^0=I,\qquad M^1=M.

Then

M2=3Mβˆ’I.M^2=3M-I.

Next,

M3=3M2βˆ’M=3(3Mβˆ’I)βˆ’M=8Mβˆ’3I.M^3=3M^2-M=3(3M-I)-M=8M-3I.

Then

M4=3M3βˆ’M2=3(8Mβˆ’3I)βˆ’(3Mβˆ’I)=21Mβˆ’8I.M^4=3M^3-M^2=3(8M-3I)-(3M-I)=21M-8I.

Next,

M5=3M4βˆ’M3=3(21Mβˆ’8I)βˆ’(8Mβˆ’3I)=55Mβˆ’21I.M^5=3M^4-M^3=3(21M-8I)-(8M-3I)=55M-21I.

Finally,

M6=3M5βˆ’M4=3(55Mβˆ’21I)βˆ’(21Mβˆ’8I)=144Mβˆ’55I.M^6=3M^5-M^4=3(55M-21I)-(21M-8I)=144M-55I.

Now substitute the matrix MM:

M6=144[2111]βˆ’55[1001].M^6= 144 \begin{bmatrix} 2&1\\ 1&1 \end{bmatrix} -55 \begin{bmatrix} 1&0\\ 0&1 \end{bmatrix}.

Thus

M6=[288144144144]βˆ’[550055]=[23314414489].M^6= \begin{bmatrix} 288&144\\ 144&144 \end{bmatrix} - \begin{bmatrix} 55&0\\ 0&55 \end{bmatrix} = \boxed{ \begin{bmatrix} 233&144\\ 144&89 \end{bmatrix} }.

Full notes β†’

  1. Complete the square for 4x2+9y2βˆ’24x+36y+36=04x^{2}+9y^{2}-24x+36y+36=0. Write the equation in standard form and give the center, vertices, co-vertices, foci, eccentricity, and major/minor axis lengths. Graph the conic.
  2. Find the equation of the parabola whose focus is (5,βˆ’2)(5,-2) and whose directrix is x=βˆ’1x=-1. Give the vertex, value of pp, axis of symmetry, and latus rectum endpoints.
  3. Find all lines with slope βˆ’2-2 that are tangent to the parabola (xβˆ’1)2=8(y+3)(x-1)^{2}=8(y+3).
  4. An ellipse has foci (1,4)(1,4) and (1,βˆ’2)(1,-2) and passes through (5,1)(5,1). Find its standard-form equation and its eccentricity.
  5. The ellipse (x+2)236+(yβˆ’1)220=1\dfrac{(x+2)^{2}}{36}+\dfrac{(y-1)^{2}}{20}=1 has foci F1F_1 and F2F_2. If PP is the point on the ellipse with x=1x=1 and y>1y>1, find PF1PF_1 and PF2PF_2 separately.
  6. Find all real numbers mm such that the line y=mx+3y=mx+3 is tangent to the ellipse x29+y24=1\dfrac{x^{2}}{9}+\dfrac{y^{2}}{4}=1.
  7. Complete the square for 9y2βˆ’4x2βˆ’54yβˆ’16x+29=09y^{2}-4x^{2}-54y-16x+29=0. Write the equation in standard form and give the center, vertices, foci, eccentricity, and asymptotes. Graph the conic.
  8. A hyperbola has center (2,βˆ’1)(2,-1), asymptotes y+1=Β±32(xβˆ’2)y+1=\pm\dfrac{3}{2}(x-2), and one focus at (2+52,βˆ’1)(2+\sqrt{52},-1). Assuming it opens left/right, find its standard-form equation.
  9. Find all intersection points in R2\mathbb{R}^{2} of the ellipse x216+y29=1\dfrac{x^{2}}{16}+\dfrac{y^{2}}{9}=1 and the hyperbola x24βˆ’y29=1\dfrac{x^{2}}{4}-\dfrac{y^{2}}{9}=1.
  10. With focus at (0,0)(0,0), directrix x=βˆ’6x=-6, and eccentricity e=23e=\dfrac{2}{3}, derive the Cartesian equation of the conic. Write it in standard form and identify the conic type.
  11. Convert r=102βˆ’cos⁑θr=\dfrac{10}{2-\cos\theta} to a Cartesian equation. Identify the conic type, eccentricity, center, vertices, and foci.
  12. For r=123+4cos⁑θr=\dfrac{12}{3+4\cos\theta}, identify the conic type and eccentricity, then find the values of θ\theta where the denominator vanishes. Explain what those angles represent geometrically.
  13. A circle is tangent to both axes in Quadrant I and its center lies on the ellipse x225+y29=1\dfrac{x^{2}}{25}+\dfrac{y^{2}}{9}=1. Find the circle’s radius.
  14. Show that the conic Ax2+Cy2+Dx+Ey+F=0Ax^{2}+Cy^{2}+Dx+Ey+F=0 has center (h,k)(h,k) when Aβ‰ 0A\ne 0 and Cβ‰ 0C\ne 0. Derive formulas for hh and kk in terms of A,C,D,EA,C,D,E, then find the center of 5x2βˆ’3y2+20x+18yβˆ’11=05x^{2}-3y^{2}+20x+18y-11=0.
  15. For the parabola y2=4pxy^{2}=4px with p>0p>0, let a line through the focus (p,0)(p,0) have slope mβ‰ 0m\ne 0 and meet the parabola at two distinct points AA and BB. Prove that the product of the yy-coordinates of AA and BB equals βˆ’4p2-4p^{2}.
  16. (Bonus, 2026 USAPhO)

You are studying the motion of charged particles constrained to the xyxy-plane. Particle Ξ±\alpha, with charge +1Β C+1\ \mathrm{C}, is fixed at the origin.

For motion under an inverse-square central force, trajectories are conic sections with the fixed particle at a focus. In polar coordinates:

  • For an attractive interaction (ellipse),
r=r01+ecos⁑ϕ,e<1.r=\frac{r_0}{1+e\cos\phi},\qquad e<1.
  • For a repulsive interaction (hyperbola),
r=r0ecosβ‘Ο•βˆ’1,e>1.r=\frac{r_0}{e\cos\phi-1},\qquad e>1.

You have a camera that takes three snapshots of a moving particle at equal time intervals.

(A)(A) A particle Ξ²\beta, with charge βˆ’1Β C-1\ \mathrm{C}, moves under the electrostatic force of particle Ξ±\alpha. In three consecutive snapshots, its positions are

(0,βˆ’5Β m),(3Β m,0),(0,5Β m).(0,-5\ \mathrm{m}),\qquad (3\ \mathrm{m},0),\qquad (0,5\ \mathrm{m}).

Assuming the motion is governed only by the Coulomb interaction with Ξ±\alpha, determine the maximum distance that particle Ξ²\beta reaches from the origin.

(B)(B) Now particle Ξ²\beta is replaced by particle Ξ³\gamma, which has charge +2Β C+2\ \mathrm{C} and is free to move in the plane. In three consecutive snapshots, its positions are

(3Β m,βˆ’4Β m),(2Β m,0),(3Β m,4Β m).(3\ \mathrm{m},-4\ \mathrm{m}),\qquad (2\ \mathrm{m},0),\qquad (3\ \mathrm{m},4\ \mathrm{m}).

Assuming the motion is governed only by the Coulomb interaction with Ξ±\alpha, determine the angle ΞΈ\theta, measured from the positive xx-axis, of the velocity of particle Ξ³\gamma at a large time.

(C)(C) A family of particles, each identical to particle γ\gamma (that is, each has charge +2 C+2\ \mathrm{C}), approaches from infinity in the xyxy-plane. All particles have the same speed v∞v_{\infty} far from the origin and move along lines parallel to the initial asymptotic direction of particle γ\gamma from part (B)(B). The particles are injected one at a time, so they do not interact with one another.

For each trajectory, define the impact parameter BB to be the perpendicular distance between the initial straight-line path of the particle and the origin.

As a particle passes near the scattering center, its direction changes due to Coulomb repulsion. Let Ξ±\alpha denote the total deflection angle of the trajectory, i.e. the angle between the incoming and outgoing asymptotic directions.

(i)(i) Using the conic form of the trajectory, derive a formula for B(Ξ±)B(\alpha).

(ii)(ii) Using the result of part (B)(B), express B(Ξ±)B(\alpha) in terms of r0r_0.

Complete the square:

4x2+9y2βˆ’24x+36y+36=04x^{2}+9y^{2}-24x+36y+36=0 4(x2βˆ’6x)+9(y2+4y)+36=0.4(x^{2}-6x)+9(y^{2}+4y)+36=0.

Then

4((xβˆ’3)2βˆ’9)+9((y+2)2βˆ’4)+36=0.4\bigl((x-3)^{2}-9\bigr)+9\bigl((y+2)^{2}-4\bigr)+36=0.

Simplify:

4(xβˆ’3)2+9(y+2)2=36.4(x-3)^{2}+9(y+2)^{2}=36.

Divide by 3636:

(xβˆ’3)29+(y+2)24=1.\frac{(x-3)^{2}}{9}+\frac{(y+2)^{2}}{4}=1.

This is an ellipse centered at (3,βˆ’2)(3,-2) with horizontal major axis. Here a2=9a^{2}=9, b2=4b^{2}=4, so a=3a=3 and b=2b=2. Also

c2=a2βˆ’b2=9βˆ’4=5,c^{2}=a^{2}-b^{2}=9-4=5,

so c=5c=\sqrt{5} and e=ca=53e=\dfrac{c}{a}=\dfrac{\sqrt{5}}{3}.

Thus

(xβˆ’3)29+(y+2)24=1\boxed{\frac{(x-3)^{2}}{9}+\frac{(y+2)^{2}}{4}=1}

with center (3,βˆ’2)\boxed{(3,-2)}, vertices (0,βˆ’2),(6,βˆ’2)\boxed{(0,-2),(6,-2)}, co-vertices (3,βˆ’4),(3,0)\boxed{(3,-4),(3,0)}, foci (3βˆ’5,βˆ’2),(3+5,βˆ’2)\boxed{(3-\sqrt{5},-2),(3+\sqrt{5},-2)}, eccentricity 53\boxed{\frac{\sqrt{5}}{3}}, major axis length 6\boxed{6}, and minor axis length 4\boxed{4}.

The graph of the conic is displayed below:

Ellipse

The focus is (5,βˆ’2)(5,-2) and the directrix is x=βˆ’1x=-1, so the parabola opens horizontally. The vertex is halfway between the focus and directrix along the horizontal axis:

(5+(βˆ’1)2,βˆ’2)=(2,βˆ’2).\left(\frac{5+(-1)}{2},-2\right)=(2,-2).

Thus h=2h=2 and k=βˆ’2k=-2. Since the focus is (h+p,k)=(5,βˆ’2)(h+p,k)=(5,-2),

p=3.p=3.

Use the horizontal parabola form

(yβˆ’k)2=4p(xβˆ’h).(y-k)^{2}=4p(x-h).

So

(y+2)2=12(xβˆ’2).\boxed{(y+2)^{2}=12(x-2)}.

The axis of symmetry is y=βˆ’2\boxed{y=-2}. The latus rectum is vertical through the focus. Its length is ∣4p∣=12\lvert 4p \rvert=12, so its endpoints are 66 units above and below the focus:

(5,4)Β andΒ (5,βˆ’8).\boxed{(5,4)\text{ and }(5,-8)}.

A line with slope βˆ’2-2 has equation

y=βˆ’2x+b.y=-2x+b.

Substitute into the parabola

(xβˆ’1)2=8(y+3).(x-1)^{2}=8(y+3).

Then

(xβˆ’1)2=8(βˆ’2x+b+3).(x-1)^{2}=8(-2x+b+3).

Expand:

x2βˆ’2x+1=βˆ’16x+8b+24.x^{2}-2x+1=-16x+8b+24.

Move everything to one side:

x2+14xβˆ’(8b+23)=0.x^{2}+14x-(8b+23)=0.

For the line to be tangent, this quadratic must have exactly one solution, so its discriminant is 00:

142βˆ’4(1)(βˆ’(8b+23))=0.14^{2}-4(1)(-(8b+23))=0.

Thus

196+32b+92=0⟹32b=βˆ’288⟹b=βˆ’9.196+32b+92=0 \quad\Longrightarrow\quad 32b=-288 \quad\Longrightarrow\quad b=-9.

Therefore the tangent line is

y=βˆ’2xβˆ’9.\boxed{y=-2x-9}.

The foci (1,4)(1,4) and (1,βˆ’2)(1,-2) have midpoint

(h,k)=(1,4+(βˆ’2)2)=(1,1).(h,k)=\left(1,\frac{4+(-2)}{2}\right)=(1,1).

The foci are vertical, so the major axis is vertical. The distance from the center to either focus is

c=3.c=3.

The point (5,1)(5,1) lies on the ellipse. Its distances to the foci are

(5βˆ’1)2+(1βˆ’4)2=5\sqrt{(5-1)^{2}+(1-4)^{2}}=5

and

(5βˆ’1)2+(1βˆ’(βˆ’2))2=5.\sqrt{(5-1)^{2}+(1-(-2))^{2}}=5.

The sum of distances is 1010, so 2a=102a=10 and a=5a=5. Then

b2=a2βˆ’c2=25βˆ’9=16.b^{2}=a^{2}-c^{2}=25-9=16.

Since the major axis is vertical,

(xβˆ’1)216+(yβˆ’1)225=1.\boxed{\frac{(x-1)^{2}}{16}+\frac{(y-1)^{2}}{25}=1}.

The eccentricity is

e=ca=35.\boxed{e=\frac{c}{a}=\frac{3}{5}}.

The ellipse

(x+2)236+(yβˆ’1)220=1\frac{(x+2)^{2}}{36}+\frac{(y-1)^{2}}{20}=1

has center (βˆ’2,1)(-2,1), a2=36a^{2}=36, and b2=20b^{2}=20. Therefore

c2=a2βˆ’b2=36βˆ’20=16,c^{2}=a^{2}-b^{2}=36-20=16,

so c=4c=4. The foci are

(βˆ’2βˆ’4,1)=(βˆ’6,1)and(βˆ’2+4,1)=(2,1).(-2-4,1)=(-6,1) \quad\text{and}\quad (-2+4,1)=(2,1).

Now use x=1x=1:

(1+2)236+(yβˆ’1)220=1.\frac{(1+2)^{2}}{36}+\frac{(y-1)^{2}}{20}=1.

So

936+(yβˆ’1)220=1⟹(yβˆ’1)220=34.\frac{9}{36}+\frac{(y-1)^{2}}{20}=1 \quad\Longrightarrow\quad \frac{(y-1)^{2}}{20}=\frac{3}{4}.

Thus

(yβˆ’1)2=15.(y-1)^{2}=15.

Since y>1y>1,

y=1+15.y=1+\sqrt{15}.

So P=(1,1+15)P=(1,1+\sqrt{15}). Its distance to the right focus (2,1)(2,1) is

(1βˆ’2)2+(15)2=16=4.\sqrt{(1-2)^{2}+(\sqrt{15})^{2}}=\sqrt{16}=4.

Its distance to the left focus (βˆ’6,1)(-6,1) is

(1+6)2+(15)2=64=8.\sqrt{(1+6)^{2}+(\sqrt{15})^{2}}=\sqrt{64}=8.

Therefore

PFright=4andPFleft=8.\boxed{PF_{\text{right}}=4\quad\text{and}\quad PF_{\text{left}}=8}.

Substitute y=mx+3y=mx+3 into

x29+y24=1.\frac{x^{2}}{9}+\frac{y^{2}}{4}=1.

Then

x29+(mx+3)24=1.\frac{x^{2}}{9}+\frac{(mx+3)^{2}}{4}=1.

Multiply by 3636:

4x2+9(mx+3)2=36.4x^{2}+9(mx+3)^{2}=36.

Expand:

4x2+9(m2x2+6mx+9)=36.4x^{2}+9(m^{2}x^{2}+6mx+9)=36.

So

(4+9m2)x2+54mx+45=0.(4+9m^{2})x^{2}+54mx+45=0.

For tangency, the discriminant must be 00:

(54m)2βˆ’4(4+9m2)(45)=0.(54m)^{2}-4(4+9m^{2})(45)=0.

Simplify:

2916m2βˆ’180(4+9m2)=02916m^{2}-180(4+9m^{2})=0 1296m2βˆ’720=0⟹m2=59.1296m^{2}-720=0 \quad\Longrightarrow\quad m^{2}=\frac{5}{9}.

Thus

m=Β±53.\boxed{m=\pm\frac{\sqrt{5}}{3}}.

Start with

9y2βˆ’4x2βˆ’54yβˆ’16x+29=0.9y^{2}-4x^{2}-54y-16x+29=0.

Group and complete the square:

9(y2βˆ’6y)βˆ’4(x2+4x)+29=0.9(y^{2}-6y)-4(x^{2}+4x)+29=0.

Then

9((yβˆ’3)2βˆ’9)βˆ’4((x+2)2βˆ’4)+29=0.9\bigl((y-3)^{2}-9\bigr)-4\bigl((x+2)^{2}-4\bigr)+29=0.

Simplify:

9(yβˆ’3)2βˆ’4(x+2)2βˆ’36=0.9(y-3)^{2}-4(x+2)^{2}-36=0.

So

9(yβˆ’3)2βˆ’4(x+2)2=36.9(y-3)^{2}-4(x+2)^{2}=36.

Divide by 3636:

(yβˆ’3)24βˆ’(x+2)29=1.\boxed{\frac{(y-3)^{2}}{4}-\frac{(x+2)^{2}}{9}=1}.

This is a vertical hyperbola. The center is (βˆ’2,3)(-2,3). Here a2=4a^{2}=4, b2=9b^{2}=9, so a=2a=2 and b=3b=3. Also

c2=a2+b2=4+9=13,c^{2}=a^{2}+b^{2}=4+9=13,

so c=13c=\sqrt{13} and e=132e=\dfrac{\sqrt{13}}{2}.

The vertices are

(βˆ’2,1)Β andΒ (βˆ’2,5).\boxed{(-2,1)\text{ and }(-2,5)}.

The foci are

(βˆ’2,3βˆ’13)Β andΒ (βˆ’2,3+13).\boxed{(-2,3-\sqrt{13})\text{ and }(-2,3+\sqrt{13})}.

The asymptotes are

yβˆ’3=Β±23(x+2).\boxed{y-3=\pm\frac{2}{3}(x+2)}.

An image of the hyperbola is shown below:

Ellipse

A horizontal hyperbola centered at (2,βˆ’1)(2,-1) has form

(xβˆ’2)2a2βˆ’(y+1)2b2=1.\frac{(x-2)^{2}}{a^{2}}-\frac{(y+1)^{2}}{b^{2}}=1.

Its asymptotes are

y+1=Β±ba(xβˆ’2).y+1=\pm\frac{b}{a}(x-2).

We are given slope 32\frac{3}{2}, so

ba=32.\frac{b}{a}=\frac{3}{2}.

Let a=2ta=2t and b=3tb=3t. The focus distance satisfies

c2=a2+b2.c^{2}=a^{2}+b^{2}.

Since one focus is (2+52,βˆ’1)(2+\sqrt{52},-1), we have c=52c=\sqrt{52}. Thus

52=(2t)2+(3t)2=13t2.52=(2t)^{2}+(3t)^{2}=13t^{2}.

So t2=4t^{2}=4, and therefore

a2=(2t)2=16,b2=(3t)2=36.a^{2}=(2t)^{2}=16, \qquad b^{2}=(3t)^{2}=36.

Thus the equation is

(xβˆ’2)216βˆ’(y+1)236=1.\boxed{\frac{(x-2)^{2}}{16}-\frac{(y+1)^{2}}{36}=1}.

Solve the system

x216+y29=1\frac{x^{2}}{16}+\frac{y^{2}}{9}=1

and

x24βˆ’y29=1.\frac{x^{2}}{4}-\frac{y^{2}}{9}=1.

Let X=x2X=x^{2} and Y=y2Y=y^{2}. Then

X16+Y9=1\frac{X}{16}+\frac{Y}{9}=1

and

X4βˆ’Y9=1.\frac{X}{4}-\frac{Y}{9}=1.

From the second equation,

X=4+4Y9.X=4+\frac{4Y}{9}.

Substitute into the first:

4+4Y916+Y9=1.\frac{4+\frac{4Y}{9}}{16}+\frac{Y}{9}=1.

This gives

14+Y36+Y9=1⟹14+5Y36=1.\frac{1}{4}+\frac{Y}{36}+\frac{Y}{9}=1 \quad\Longrightarrow\quad \frac{1}{4}+\frac{5Y}{36}=1.

So

5Y36=34⟹Y=275.\frac{5Y}{36}=\frac{3}{4} \quad\Longrightarrow\quad Y=\frac{27}{5}.

Then

X=4+49β‹…275=4+125=325.X=4+\frac{4}{9}\cdot\frac{27}{5} =4+\frac{12}{5} =\frac{32}{5}.

Therefore

x=Β±325=Β±4105,y=Β±275=Β±3155.x=\pm\sqrt{\frac{32}{5}}=\pm\frac{4\sqrt{10}}{5}, \qquad y=\pm\sqrt{\frac{27}{5}}=\pm\frac{3\sqrt{15}}{5}.

All sign combinations work, so the intersection points are

(Β±4105, ±3155).\boxed{\left(\pm\frac{4\sqrt{10}}{5},\,\pm\frac{3\sqrt{15}}{5}\right)}.

The focus is (0,0)(0,0) and the directrix is x=βˆ’6x=-6. For a point (x,y)(x,y) on the conic,

PF=x2+y2PF=\sqrt{x^{2}+y^{2}}

and

d(P,β„“)=x+6d(P,\ell)=x+6

on the appropriate side of the directrix. Since e=23e=\dfrac{2}{3},

x2+y2=23(x+6).\sqrt{x^{2}+y^{2}}=\frac{2}{3}(x+6).

Square both sides:

x2+y2=49(x+6)2.x^{2}+y^{2}=\frac{4}{9}(x+6)^{2}.

Multiply by 99:

9x2+9y2=4x2+48x+144.9x^{2}+9y^{2}=4x^{2}+48x+144.

So

5x2+9y2βˆ’48xβˆ’144=0.5x^{2}+9y^{2}-48x-144=0.

Complete the square in xx:

5(x2βˆ’485x)+9y2=144.5\left(x^{2}-\frac{48}{5}x\right)+9y^{2}=144.

Since

x2βˆ’485x=(xβˆ’245)2βˆ’57625,x^{2}-\frac{48}{5}x=\left(x-\frac{24}{5}\right)^{2}-\frac{576}{25},

we get

5(xβˆ’245)2+9y2=12965.5\left(x-\frac{24}{5}\right)^{2}+9y^{2}=\frac{1296}{5}.

Divide by 12965\dfrac{1296}{5}:

(xβˆ’245)2129625+y21445=1.\boxed{\frac{\left(x-\frac{24}{5}\right)^{2}}{\frac{1296}{25}}+\frac{y^{2}}{\frac{144}{5}}=1}.

Since 0<e<10<e<1, this conic is an ellipse.

Start with

r=102βˆ’cos⁑θ.r=\frac{10}{2-\cos\theta}.

Rewrite:

2rβˆ’rcos⁑θ=10.2r-r\cos\theta=10.

Use r=x2+y2r=\sqrt{x^{2}+y^{2}} and rcos⁑θ=xr\cos\theta=x:

2x2+y2βˆ’x=10.2\sqrt{x^{2}+y^{2}}-x=10.

So

2x2+y2=x+10.2\sqrt{x^{2}+y^{2}}=x+10.

Square both sides:

4(x2+y2)=(x+10)2.4(x^{2}+y^{2})=(x+10)^{2}.

Expand:

4x2+4y2=x2+20x+100.4x^{2}+4y^{2}=x^{2}+20x+100.

So

3x2+4y2βˆ’20xβˆ’100=0.3x^{2}+4y^{2}-20x-100=0.

Complete the square:

3(x2βˆ’203x)+4y2=100.3\left(x^{2}-\frac{20}{3}x\right)+4y^{2}=100.

Since

x2βˆ’203x=(xβˆ’103)2βˆ’1009,x^{2}-\frac{20}{3}x=\left(x-\frac{10}{3}\right)^{2}-\frac{100}{9},

we get

3(xβˆ’103)2+4y2=4003.3\left(x-\frac{10}{3}\right)^{2}+4y^{2}=\frac{400}{3}.

Divide by 4003\dfrac{400}{3}:

(xβˆ’103)24009+y21003=1.\boxed{\frac{\left(x-\frac{10}{3}\right)^{2}}{\frac{400}{9}}+\frac{y^{2}}{\frac{100}{3}}=1}.

The conic is an ellipse. From

r=102βˆ’cos⁑θ=51βˆ’12cos⁑θ,r=\frac{10}{2-\cos\theta}=\frac{5}{1-\frac{1}{2}\cos\theta},

the eccentricity is e=12\boxed{e=\frac{1}{2}}. The center is (103,0)\boxed{\left(\frac{10}{3},0\right)}. Since a2=4009a^{2}=\frac{400}{9}, a=203a=\frac{20}{3}. The vertices are

(βˆ’103,0)Β andΒ (10,0).\boxed{\left(-\frac{10}{3},0\right)\text{ and }(10,0)}.

Also c=ea=103c=ea=\frac{10}{3}, so the foci are

(0,0)Β andΒ (203,0).\boxed{(0,0)\text{ and }\left(\frac{20}{3},0\right)}.

Rewrite

r=123+4cos⁑θr=\frac{12}{3+4\cos\theta}

by factoring 33 from the denominator:

r=41+43cos⁑θ.r=\frac{4}{1+\frac{4}{3}\cos\theta}.

This matches polar conic form with eccentricity

e=43.e=\frac{4}{3}.

Since e>1e>1, the conic is a hyperbola.

The denominator vanishes when

3+4cos⁑θ=0.3+4\cos\theta=0.

Thus

cos⁑θ=βˆ’34.\cos\theta=-\frac{3}{4}.

So the angles are

ΞΈ=arccos⁑(βˆ’34)andΞΈ=2Ο€βˆ’arccos⁑(βˆ’34).\boxed{\theta=\arccos\left(-\frac{3}{4}\right)\quad\text{and}\quad \theta=2\pi-\arccos\left(-\frac{3}{4}\right)}.

At those angles, rr is not finite. Geometrically, they give the asymptotic directions of the hyperbola.

A circle tangent to both axes in Quadrant I has center (r,r)(r,r) and radius rr. Since the center lies on

x225+y29=1,\frac{x^{2}}{25}+\frac{y^{2}}{9}=1,

substitute (r,r)(r,r):

r225+r29=1.\frac{r^{2}}{25}+\frac{r^{2}}{9}=1.

Then

r2(125+19)=1.r^{2}\left(\frac{1}{25}+\frac{1}{9}\right)=1.

Compute:

125+19=9+25225=34225.\frac{1}{25}+\frac{1}{9}=\frac{9+25}{225}=\frac{34}{225}.

So

r2β‹…34225=1⟹r2=22534.r^{2}\cdot\frac{34}{225}=1 \quad\Longrightarrow\quad r^{2}=\frac{225}{34}.

Since r>0r>0,

r=1534=153434.\boxed{r=\frac{15}{\sqrt{34}}=\frac{15\sqrt{34}}{34}}.

Start with

Ax2+Cy2+Dx+Ey+F=0,Ax^{2}+Cy^{2}+Dx+Ey+F=0,

where A≠0A\ne 0 and C≠0C\ne 0. Complete the square separately in xx and yy:

A(x2+DAx)+C(y2+ECy)+F=0.A\left(x^{2}+\frac{D}{A}x\right)+C\left(y^{2}+\frac{E}{C}y\right)+F=0.

The centers of the completed squares occur at

x=βˆ’D2Aandy=βˆ’E2C.x=-\frac{D}{2A} \qquad\text{and}\qquad y=-\frac{E}{2C}.

Therefore the center is

(βˆ’D2A,βˆ’E2C).\boxed{\left(-\frac{D}{2A},-\frac{E}{2C}\right)}.

For

5x2βˆ’3y2+20x+18yβˆ’11=0,5x^{2}-3y^{2}+20x+18y-11=0,

we have A=5A=5, C=βˆ’3C=-3, D=20D=20, and E=18E=18. Thus

h=βˆ’202(5)=βˆ’2h=-\frac{20}{2(5)}=-2

and

k=βˆ’182(βˆ’3)=3.k=-\frac{18}{2(-3)}=3.

So the center is

(βˆ’2,3).\boxed{(-2,3)}.

The parabola is

y2=4px,y^{2}=4px,

and its focus is (p,0)(p,0). A line through the focus with slope m≠0m\ne 0 has equation

y=m(xβˆ’p).y=m(x-p).

Solve this for xx:

x=p+ym.x=p+\frac{y}{m}.

Substitute into the parabola:

y2=4p(p+ym).y^{2}=4p\left(p+\frac{y}{m}\right).

Expand:

y2=4p2+4pmy.y^{2}=4p^{2}+\frac{4p}{m}y.

Move everything to one side:

y2βˆ’4pmyβˆ’4p2=0.y^{2}-\frac{4p}{m}y-4p^{2}=0.

This quadratic has roots equal to the yy-coordinates of the two intersection points AA and BB. By Vieta’s formula, the product of the roots is the constant term divided by the leading coefficient:

yAyB=βˆ’4p21.y_Ay_B=\frac{-4p^{2}}{1}.

Therefore

yAyB=βˆ’4p2.\boxed{y_Ay_B=-4p^{2}}.

For part (A), use the attractive model

r=r01+ecos⁑ϕ.r=\frac{r_0}{1+e\cos\phi}.

Since the first and third snapshots are at (0,βˆ’5)(0,-5) and (0,5)(0,5), while the middle snapshot is at (3,0)(3,0), and the time intervals are equal, the path is symmetric about the xx-axis. Therefore, (3,0)(3,0) is the closest point to the origin, called the pericenter.

At pericenter, Ο•=0\phi=0, so

rmin⁑=r01+e=3.r_{\min}=\frac{r_0}{1+e}=3.

The other two photographed points are on the yy-axis. There,

Ο•=Β±Ο€2,r=5.\phi=\pm\frac{\pi}{2},\qquad r=5.

Since cos⁑(Β±Ο€2)=0\cos\left(\pm\frac{\pi}{2}\right)=0,

5=r01+e(0)=r0.5=\frac{r_0}{1+e(0)}=r_0.

So

r0=5.r_0=5.

Now use the pericenter equation:

3=51+e.3=\frac{5}{1+e}.

Thus,

1+e=53,1+e=\frac53,

so

e=23.e=\frac23.

The farthest point on the ellipse is the apocenter, where Ο•=Ο€\phi=\pi and cos⁑ϕ=βˆ’1\cos\phi=-1. Therefore,

rmax⁑=r01βˆ’e=51βˆ’23=15.r_{\max}=\frac{r_0}{1-e} =\frac{5}{1-\frac23} =15.

So

rmax⁑=15 m.\boxed{r_{\max}=15\ \mathrm{m}}.

For part (B), use the repulsive model

r=r0ecosβ‘Ο•βˆ’1.r=\frac{r_0}{e\cos\phi-1}.

Again, the first and third snapshots are symmetric about the xx-axis, and the middle snapshot is at (2,0)(2,0). Since the snapshots are equally spaced in time, (2,0)(2,0) is the point of closest approach.

At closest approach,

rmin⁑=r0eβˆ’1=2.r_{\min}=\frac{r_0}{e-1}=2.

Thus,

r0=2(eβˆ’1).r_0=2(e-1).

Now use the point (3,4)(3,4). Its distance from the origin is

r=32+42=5,r=\sqrt{3^2+4^2}=5,

and

cos⁑ϕ=xr=35.\cos\phi=\frac{x}{r}=\frac35.

Substitute into the polar equation:

5=r0eβ‹…35βˆ’1.5=\frac{r_0}{e\cdot\frac35-1}.

Using r0=2(eβˆ’1)r_0=2(e-1),

5=2(eβˆ’1)35eβˆ’1.5=\frac{2(e-1)}{\frac35e-1}.

Multiply through:

5(35eβˆ’1)=2(eβˆ’1).5\left(\frac35e-1\right)=2(e-1).

So

3eβˆ’5=2eβˆ’2,3e-5=2e-2,

which gives

e=3.e=3.

Then

r0=2(eβˆ’1)=4.r_0=2(e-1)=4.

At large times, the particle approaches an asymptote of the hyperbola. The asymptote occurs when the denominator goes to zero:

ecosβ‘Ο•βˆ’1=0.e\cos\phi-1=0.

Therefore,

cos⁑ϕ=1e=13.\cos\phi=\frac1e=\frac13.

Thus the outgoing velocity direction at large positive time is

θ=arccos⁑(13)\boxed{\theta=\arccos\left(\frac13\right)}

measured from the positive xx-axis. Numerically,

ΞΈβ‰ˆ70.5∘.\theta\approx70.5^\circ.

For part (C), for a repulsive inverse-square force, the trajectory is

r=r0ecosβ‘Ο•βˆ’1,e>1.r=\frac{r_0}{e\cos\phi-1},\qquad e>1.

The asymptotes occur when the denominator vanishes:

ecosβ‘Ο•βˆ’1=0.e\cos\phi-1=0.

Thus,

cos⁑ϕ=1e.\cos\phi=\frac1e.

The two asymptotes are symmetric about the xx-axis, so the total deflection angle is

Ξ±=2Ο•=2arccos⁑(1e).\alpha=2\phi=2\arccos\left(\frac1e\right).

Hence,

cos⁑(α2)=1e,\cos\left(\frac{\alpha}{2}\right)=\frac1e,

so

e=1cos⁑(α/2).e=\frac{1}{\cos(\alpha/2)}.

Now relate the impact parameter BB to the conic parameters. Starting from

r=r0ecosβ‘Ο•βˆ’1,r=\frac{r_0}{e\cos\phi-1},

multiply through:

r(ecosβ‘Ο•βˆ’1)=r0.r(e\cos\phi-1)=r_0.

Since rcos⁑ϕ=xr\cos\phi=x,

exβˆ’r=r0.ex-r=r_0.

So

r=exβˆ’r0.r=ex-r_0.

Square both sides and use r2=x2+y2r^2=x^2+y^2:

x2+y2=(exβˆ’r0)2.x^2+y^2=(ex-r_0)^2.

Rearrange:

(e2βˆ’1)x2βˆ’2er0x+r02βˆ’y2=0.(e^2-1)x^2-2er_0x+r_0^2-y^2=0.

Complete the square:

(e2βˆ’1)(xβˆ’er0e2βˆ’1)2βˆ’y2=r02e2βˆ’1.(e^2-1)\left(x-\frac{er_0}{e^2-1}\right)^2-y^2 =\frac{r_0^2}{e^2-1}.

Thus the hyperbola has asymptotes

y=Β±e2βˆ’1(xβˆ’er0e2βˆ’1).y=\pm\sqrt{e^2-1}\left(x-\frac{er_0}{e^2-1}\right).

The impact parameter BB is the perpendicular distance from the origin to the incoming asymptote. For a line

y=m(xβˆ’h),y=m(x-h),

the distance from the origin is

∣mh∣m2+1.\frac{\lvert mh \rvert}{\sqrt{m^2+1}}.

Here

m=e2βˆ’1m=\sqrt{e^2-1}

and

h=er0e2βˆ’1.h=\frac{er_0}{e^2-1}.

Therefore,

B=e2βˆ’1β‹…er0e2βˆ’1(e2βˆ’1)+1.B= \frac{\sqrt{e^2-1}\cdot \frac{er_0}{e^2-1}} {\sqrt{(e^2-1)+1}}.

Since (e2βˆ’1)+1=e\sqrt{(e^2-1)+1}=e,

B=r0e2βˆ’1.B=\frac{r_0}{\sqrt{e^2-1}}.

Now substitute

e=1cos⁑(α/2).e=\frac{1}{\cos(\alpha/2)}.

Then

e2βˆ’1=1cos⁑2(Ξ±/2)βˆ’1=tan⁑2(Ξ±2).e^2-1 =\frac{1}{\cos^2(\alpha/2)}-1 =\tan^2\left(\frac{\alpha}{2}\right).

So

e2βˆ’1=tan⁑(Ξ±2).\sqrt{e^2-1}=\tan\left(\frac{\alpha}{2}\right).

Therefore,

B(α)=r0cot⁑(α2).\boxed{B(\alpha)=r_0\cot\left(\frac{\alpha}{2}\right)}.

For the particular trajectory in part (B)(B), the asymptote angle satisfies

cos⁑(α2)=13,\cos\left(\frac{\alpha}{2}\right)=\frac13,

so

tan⁑(α2)=22.\tan\left(\frac{\alpha}{2}\right)=2\sqrt2.

Therefore, for any trajectory whose asymptote angle matches the one from part (B)(B),

B=r0cot⁑(α2)=r022.B=r_0\cot\left(\frac{\alpha}{2}\right) =\frac{r_0}{2\sqrt2}.

For the specific particle in part (B)(B), r0=4r_0=4, so

B=422=2Β m.B=\frac{4}{2\sqrt2}=\sqrt2\ \mathrm{m}.

Note that the answer may be different depending on how you define the asymptote angle, so always match your work instead of necessarily matching solutions.

Full notes β†’

  1. Evaluate lim⁑xβ†’βˆž5x3βˆ’2x+1x3+4x2βˆ’7\displaystyle \lim_{x\to\infty}\frac{5x^3-2x+1}{x^3+4x^2-7}.
  2. Find the horizontal asymptote, if it exists, of f(x)=3x2+8xβˆ’1x2βˆ’5\displaystyle f(x)=\frac{3x^2+8x-1}{x^2-5}.
  3. Find the oblique asymptote of g(x)=x2+4xβˆ’1x+2\displaystyle g(x)=\frac{x^2+4x-1}{x+2}.
  4. Prove by induction that βˆ‘k=1nk3=n2(n+1)24\sum_{k=1}^{n} k^3 = \frac{n^2 (n+1)^2}{4} for all integers nβ‰₯1n \ge 1. Extension: This looks like the square of 1+2+...+n=n(n+1)21 + 2 + ... + n = \frac{n(n+1)}{2}! Prove that this is true (you should not use induction here).
  5. Prove by induction that 82nβˆ’32n8^{2n} - 3^{2n} is divisible by 5555 for all integers nβ‰₯1n \ge 1.
  6. Prove by induction that 2nβ‰₯n32^{n}\ge n^{3} for all integers nβ‰₯10n\ge 10.
  7. Expand (3x+2y)5(3x+2y)^{5} using the binomial theorem.
  8. What is the coefficient of the term containing x22x^{22} in (x3βˆ’4x)12\left(x^{3} - \dfrac{4}{\sqrt{x}}\right)^{12}?
  9. Use the binomial theorem to prove that 9nβˆ’19^{n}-1 is divisible by 88 for every integer nβ‰₯1n\ge 1.
  10. A nonconstant arithmetic sequence has first term 55 and common difference dd. Its first, third, and seventh terms form a geometric sequence in that order. Find dd and the three geometric terms.
  11. The sequence 1,x,y,z1,x,y,z is arithmetic. The sequence 1,p,q,z1,p,q,z is geometric. Both sequences are strictly increasing and contain only integers, and zz is as small as possible. What is the value of x+y+z+p+qx+y+z+p+q? (2025 AMC 10A)
  12. Find βˆ‘i=5100(3iβˆ’2)\sum_{i=5}^{100}(3i-2).
  13. Evaluate βˆ‘i=6123β‹…2i\sum_{i=6}^{12} 3\cdot 2^i.
  14. The first three terms of a geometric series are the integers aa, 720720, and bb, where a<720<ba < 720 < b. What is the sum of the digits of the least possible value of bb? (2024 AMC 10A).
  15. Evaluate the finite sum βˆ‘k=0n(nk)3k2nβˆ’k(k+1)\sum_{k=0}^{n}\binom{n}{k}3^{k}2^{n-k}(k+1) in closed form. Hint: k(nk)=n(nβˆ’1kβˆ’1)k\binom{n}{k} = n\binom{n-1}{k-1}
  16. (Bonus, Binet’s Formula)

Binet’s Formula is a famous explicit formula for the Fibonnaci series. Let F0=0F_0=0, F1=1F_1=1, and Fn+2=Fn+1+FnF_{n+2}=F_{n+1}+F_n for nβ‰₯0n\ge 0.

(A)(A) Define a function G(x)=βˆ‘n=0∞FnxnG(x)=\sum_{n=0}^{\infty}F_nx^n. Use the recurrence to show that G(x)=x1βˆ’xβˆ’x2G(x)=\frac{x}{1-x-x^2}. G(x)G(x) is called the generating function of FnF_n. Hint: How can you telescope to cancel out the correct terms?

(B)(B) Decompose G(x)G(x) into partial fractions (Hint: All terms should be linear!).

(C)(C) Set the linear factors found in part (B) to Ξ±\alpha and Ξ²\beta (so your partial fraction looks like A1βˆ’Ξ±x\frac{A}{1 - \alpha x} and B1βˆ’Ξ²x\frac{B}{1 - \beta x}). Use the geometric series formula to prove Binet’s formula:

Fn=Ξ±nβˆ’Ξ²n5.F_n=\frac{\alpha^n-\beta^n}{\sqrt5}.

Divide numerator and denominator by x3x^3:

lim⁑xβ†’βˆž5x3βˆ’2x+1x3+4x2βˆ’7=lim⁑xβ†’βˆž5βˆ’2x2+1x31+4xβˆ’7x3.\lim_{x\to\infty}\frac{5x^3-2x+1}{x^3+4x^2-7} = \lim_{x\to\infty} \frac{5-\frac{2}{x^2}+\frac{1}{x^3}}{1+\frac{4}{x}-\frac{7}{x^3}}.

As xβ†’βˆžx\to\infty, every term with xx in the denominator approaches 00. Therefore

lim⁑xβ†’βˆž5x3βˆ’2x+1x3+4x2βˆ’7=5.\boxed{\lim_{x\to\infty}\frac{5x^3-2x+1}{x^3+4x^2-7}=5}.

Since the numerator and denominator have the same degree, this is also the ratio of leading coefficients.

Evaluate the end behavior:

lim⁑xβ†’βˆž3x2+8xβˆ’1x2βˆ’5=lim⁑xβ†’βˆž3+8xβˆ’1x21βˆ’5x2=3.\lim_{x\to\infty}\frac{3x^2+8x-1}{x^2-5} = \lim_{x\to\infty} \frac{3+\frac{8}{x}-\frac{1}{x^2}}{1-\frac{5}{x^2}} =3.

Likewise,

lim⁑xβ†’βˆ’βˆž3x2+8xβˆ’1x2βˆ’5=3.\lim_{x\to-\infty}\frac{3x^2+8x-1}{x^2-5}=3.

Therefore the horizontal asymptote is

y=3.\boxed{y=3}.

Use polynomial division:

x2+4xβˆ’1x+2=x+2βˆ’5x+2.\frac{x^2+4x-1}{x+2} =x+2-\frac{5}{x+2}.

Since

lim⁑xβ†’βˆž(βˆ’5x+2)=0\lim_{x\to\infty}\left(-\frac{5}{x+2}\right)=0

and

lim⁑xβ†’βˆ’βˆž(βˆ’5x+2)=0,\lim_{x\to-\infty}\left(-\frac{5}{x+2}\right)=0,

the graph approaches the line

y=x+2.\boxed{y=x+2}.

Base case: n=1n=1:

βˆ‘i=11i3=13=1\sum_{i=1}^{1} i^{3}=1^{3}=1

and

12(1+1)24=12β‹…224=1.\frac{1^{2}(1+1)^{2}}{4}=\frac{1^{2}\cdot 2^{2}}{4}=1.

Since both sides are equal, the statement is true for n=1n=1.

Induction hypothesis: Assume that for some integer kβ‰₯1k \ge 1,

βˆ‘i=1ki3=k2(k+1)24.\sum_{i=1}^{k} i^{3} = \frac{k^{2}(k+1)^{2}}{4}.

Inductive step: We need to show that

βˆ‘i=1k+1i3=(k+1)2(k+2)24.\sum_{i=1}^{k+1} i^{3} = \frac{(k+1)^{2}(k+2)^{2}}{4}.

Start with the expression for k+1k+1:

βˆ‘i=1k+1i3=βˆ‘i=1ki3+(k+1)3.\sum_{i=1}^{k+1} i^{3} = \sum_{i=1}^{k} i^{3} + (k+1)^{3}.

Use the induction hypothesis:

βˆ‘i=1k+1i3=k2(k+1)24+(k+1)3.\sum_{i=1}^{k+1} i^{3} = \frac{k^{2}(k+1)^{2}}{4} + (k+1)^{3}.

Factor (k+1)2(k+1)^{2}:

k2(k+1)24+(k+1)3=(k+1)2(k24+(k+1)).\frac{k^{2}(k+1)^{2}}{4} + (k+1)^{3} = (k+1)^{2}\left(\frac{k^{2}}{4} + (k+1)\right).

Simplify inside the parentheses:

(k+1)2(k24+(k+1))=(k+1)2(k2+4k+44)=(k+1)2((k+2)24)=(k+1)2(k+2)24.(k+1)^{2}\left(\frac{k^{2}}{4} + (k+1)\right) = (k+1)^{2}\left(\frac{k^{2}+4k+4}{4}\right) = (k+1)^{2}\left(\frac{(k+2)^{2}}{4}\right) = \frac{(k+1)^{2}(k+2)^{2}}{4}.

Thus the formula is true for k+1k+1. By induction,

βˆ‘i=1ni3=n2(n+1)24\boxed{\sum_{i=1}^{n} i^{3} = \frac{n^{2}(n+1)^{2}}{4}}

for all integers nβ‰₯1n \ge 1.

Extension (no induction): Let Sn=βˆ‘k=1nk=n(n+1)2S_{n}=\sum_{k=1}^{n}k=\dfrac{n(n+1)}{2}. Then

Sn2βˆ’Snβˆ’12=(n(n+1)2)2βˆ’((nβˆ’1)n2)2=n24((n+1)2βˆ’(nβˆ’1)2)=n24β‹…4n=n3.S_{n}^{2}-S_{n-1}^{2} = \left(\frac{n(n+1)}{2}\right)^{2}-\left(\frac{(n-1)n}{2}\right)^{2} = \frac{n^{2}}{4}\bigl((n+1)^{2}-(n-1)^{2}\bigr) = \frac{n^{2}}{4}\cdot 4n = n^{3}.

Telescoping gives

βˆ‘k=1nk3=Sn2βˆ’S02=Sn2=n2(n+1)24\boxed{\sum_{k=1}^{n}k^{3}=S_{n}^{2}-S_{0}^{2}=S_{n}^{2}=\frac{n^{2}(n+1)^{2}}{4}}

with S0=0S_{0}=0.

Base case: n=1n=1: 82βˆ’32=64βˆ’9=558^{2}-3^{2}=64-9=55, divisible by 5555.

Induction hypothesis: Assume 55∣82kβˆ’32k55 \mid 8^{2k}-3^{2k} for some integer kβ‰₯1k \ge 1.

Inductive step: We need to show that

55∣82(k+1)βˆ’32(k+1).55 \mid 8^{2(k+1)} - 3^{2(k+1)}.

Start with the expression for k+1k+1:

82(k+1)βˆ’32(k+1)=82k+2βˆ’32k+2.8^{2(k+1)} - 3^{2(k+1)} = 8^{2k+2} - 3^{2k+2}.

Rewrite using 82=648^{2}=64 and 32=93^{2}=9:

82k+2βˆ’32k+2=64β‹…82kβˆ’9β‹…32k.8^{2k+2} - 3^{2k+2} = 64\cdot 8^{2k} - 9\cdot 3^{2k}.

Now add and subtract 64β‹…32k64\cdot 3^{2k} so that the induction hypothesis appears:

64β‹…82kβˆ’9β‹…32k=64(82kβˆ’32k)+64β‹…32kβˆ’9β‹…32k.64\cdot 8^{2k} - 9\cdot 3^{2k} = 64(8^{2k}-3^{2k}) + 64\cdot 3^{2k} - 9\cdot 3^{2k}.

Simplify:

64(82kβˆ’32k)+(64βˆ’9)32k=64(82kβˆ’32k)+55β‹…32k.64(8^{2k}-3^{2k}) + (64-9)3^{2k} = 64(8^{2k}-3^{2k}) + 55\cdot 3^{2k}.

By the induction hypothesis, 82kβˆ’32k8^{2k}-3^{2k} is divisible by 5555, so 64(82kβˆ’32k)64(8^{2k}-3^{2k}) is also divisible by 5555. The term 55β‹…32k55\cdot 3^{2k} is clearly divisible by 5555. Therefore, their sum is divisible by 5555.

Thus 55∣82(k+1)βˆ’32(k+1)55 \mid 8^{2(k+1)} - 3^{2(k+1)}. By induction,

55∣82nβˆ’32nΒ forΒ allΒ integersΒ nβ‰₯1.\boxed{55 \mid 8^{2n} - 3^{2n} \text{ for all integers } n \ge 1}.

Base case: n=10n=10:

210=10242^{10}=1024

and

103=1000.10^{3}=1000.

Since 1024β‰₯10001024\ge 1000, the inequality is true for n=10n=10.

Induction hypothesis: Assume that for some integer kβ‰₯10k\ge 10,

2kβ‰₯k3.2^{k}\ge k^{3}.

Inductive step: We need to show that

2k+1β‰₯(k+1)3.2^{k+1}\ge (k+1)^{3}.

Start with the left-hand side:

2k+1=2β‹…2k.2^{k+1}=2\cdot 2^{k}.

Use the induction hypothesis:

2β‹…2kβ‰₯2k3.2\cdot 2^{k}\ge 2k^{3}.

Now we need to show that 2k32k^{3} is at least (k+1)3(k+1)^{3}. Compare them:

2k3βˆ’(k+1)3=2k3βˆ’(k3+3k2+3k+1)=k3βˆ’3k2βˆ’3kβˆ’1.2k^{3}-(k+1)^{3} =2k^{3}-(k^{3}+3k^{2}+3k+1) =k^{3}-3k^{2}-3k-1.

For kβ‰₯10k\ge 10,

k3βˆ’3k2βˆ’3kβˆ’1=k2(kβˆ’6)+3k(kβˆ’1)βˆ’1.k^{3}-3k^{2}-3k-1 = k^{2}(k-6)+3k(k-1)-1.

Since kβ‰₯10k\ge 10, both k2(kβˆ’6)k^{2}(k-6) and 3k(kβˆ’1)3k(k-1) are positive, and more specifically,

k2(kβˆ’6)+3k(kβˆ’1)βˆ’1β‰₯102(4)+0βˆ’1=399>0.k^{2}(k-6)+3k(k-1)-1\ge 10^{2}(4)+0-1=399>0.

Therefore

2k3β‰₯(k+1)3.2k^{3}\ge (k+1)^{3}.

Combining the inequalities,

2k+1β‰₯2k3β‰₯(k+1)3.2^{k+1}\ge 2k^{3}\ge (k+1)^{3}.

Thus the inequality is true for k+1k+1. By induction,

2nβ‰₯n3Β forΒ allΒ integersΒ nβ‰₯10.\boxed{2^{n}\ge n^{3} \text{ for all integers } n\ge 10}.

Use the binomial theorem with a=3xa=3x, b=2yb=2y, and n=5n=5:

(3x+2y)5=βˆ‘k=05(5k)(3x)5βˆ’k(2y)k.(3x+2y)^{5} = \sum_{k=0}^{5} \binom{5}{k} (3x)^{5-k}(2y)^{k}.

The coefficients from row 55 of Pascal’s Triangle are 1,5,10,10,5,11,5,10,10,5,1, so

(3x+2y)5=(3x)5+5(3x)4(2y)+10(3x)3(2y)2+10(3x)2(2y)3+5(3x)(2y)4+(2y)5=243x5+810x4y+1080x3y2+720x2y3+240xy4+32y5.\begin{aligned} (3x+2y)^{5} &= (3x)^5+5(3x)^4(2y)+10(3x)^3(2y)^2+10(3x)^2(2y)^3+5(3x)(2y)^4+(2y)^5\\ &= 243x^5+810x^4y+1080x^3y^2+720x^2y^3+240xy^4+32y^5. \end{aligned}

Thus

(3x+2y)5=243x5+810x4y+1080x3y2+720x2y3+240xy4+32y5.\boxed{(3x+2y)^5=243x^5+810x^4y+1080x^3y^2+720x^2y^3+240xy^4+32y^5}.

Write (x3βˆ’4x)12=(x3βˆ’4xβˆ’1/2)12\left(x^{3} - \dfrac{4}{\sqrt{x}}\right)^{12} = \left(x^{3} - 4x^{-1/2}\right)^{12}. A general term in the binomial expansion is

(12k)(x3)12βˆ’k(βˆ’4xβˆ’1/2)k=(12k)(βˆ’4)k x36βˆ’7k/2.\binom{12}{k} (x^{3})^{12-k}\left(-4x^{-1/2}\right)^{k} = \binom{12}{k}(-4)^{k}\, x^{36 - 7k/2}.

We need the exponent of xx to equal 2222:

36βˆ’7k2=22.36 - \frac{7k}{2}=22.

Then

7k2=14⟹7k=28⟹k=4.\frac{7k}{2}=14 \quad\Longrightarrow\quad 7k=28 \quad\Longrightarrow\quad k=4.

Since k=4k=4 is an integer between 00 and 1212, the desired term exists. Its coefficient is

(124)(βˆ’4)4=495β‹…256=126720.\binom{12}{4}(-4)^4=495\cdot 256=126720.

Therefore, the coefficient of x22x^{22} is

126720.\boxed{126720}.
9nβˆ’1=(8+1)nβˆ’1.9^{n}-1=(8+1)^{n}-1.

By the binomial theorem,

(8+1)n=βˆ‘k=0n(nk)8k1nβˆ’k.(8+1)^{n}=\sum_{k=0}^{n}\binom{n}{k}8^{k}1^{n-k}.

So

(8+1)n=(n0)80+βˆ‘k=1n(nk)8k.(8+1)^n=\binom{n}{0}8^{0}+\sum_{k=1}^{n}\binom{n}{k}8^{k}.

Since (n0)80=1\binom{n}{0}8^{0}=1,

(8+1)nβˆ’1=βˆ‘k=1n(nk)8k.(8+1)^n-1=\sum_{k=1}^{n}\binom{n}{k}8^{k}.

Every term in the sum has a factor of 88 because kβ‰₯1k\ge 1. Therefore the entire sum is divisible by 88. Thus

8∣9nβˆ’1Β forΒ everyΒ integerΒ nβ‰₯1.\boxed{8\mid 9^{n}-1 \text{ for every integer } n\ge 1}.

The arithmetic sequence has terms

a1=5,a3=5+2d,a7=5+6d.a_1=5,\qquad a_3=5+2d,\qquad a_7=5+6d.

These three terms form a geometric sequence in order, so the middle term squared equals the product of the first and third terms:

(5+2d)2=5(5+6d).(5+2d)^2=5(5+6d).

Expand:

25+20d+4d2=25+30d.25+20d+4d^{2}=25+30d.

Simplify:

4d2βˆ’10d=0.4d^{2}-10d=0.

Factor:

2d(2dβˆ’5)=0.2d(2d-5)=0.

So d=0d=0 or d=52d=\frac{5}{2}. The sequence is nonconstant, so d≠0d\ne 0. Therefore

d=52.d=\frac{5}{2}.

The three geometric terms are

5,5+2(52)=10,5+6(52)=20.5,\qquad 5+2\left(\frac{5}{2}\right)=10,\qquad 5+6\left(\frac{5}{2}\right)=20.

Thus

d=52andΒ theΒ geometricΒ termsΒ areΒ 5,10,20.\boxed{d=\frac{5}{2}\quad\text{and the geometric terms are }5,10,20}.

Arithmetic: Since 1,x,y,z1,x,y,z is arithmetic, let the common difference be dd. Then

x=1+d,y=1+2d,z=1+3d.x=1+d,\qquad y=1+2d,\qquad z=1+3d.

Geometric: Since 1,p,q,z1,p,q,z is geometric and all terms are strictly increasing integers, the common ratio must be an integer rβ‰₯2r\ge 2. Thus

p=r,q=r2,z=r3.p=r,\qquad q=r^{2},\qquad z=r^{3}.

The same value zz must work for both sequences, so

r3=1+3d.r^{3}=1+3d.

This means r3βˆ’1r^{3}-1 must be divisible by 33. Try the smallest possible integer values of rr:

r=2:z=8,3d=7notΒ possible,r=2:\quad z=8,\quad 3d=7 \quad \text{not possible}, r=3:z=27,3d=26notΒ possible,r=3:\quad z=27,\quad 3d=26 \quad \text{not possible}, r=4:z=64,3d=63,d=21.r=4:\quad z=64,\quad 3d=63,\quad d=21.

So the arithmetic sequence is 1,22,43,641,22,43,64 and the geometric sequence is 1,4,16,641,4,16,64. Therefore

x+y+z+p+q=22+43+64+4+16=149.\boxed{x+y+z+p+q=22+43+64+4+16=149}.

The terms of the sum form an arithmetic series. The first term occurs when i=5i=5:

a1=3(5)βˆ’2=13.a_{1}=3(5)-2=13.

The last term occurs when i=100i=100:

a96=3(100)βˆ’2=298.a_{96}=3(100)-2=298.

There are

100βˆ’5+1=96100-5+1=96

terms. Using the finite arithmetic series formula,

βˆ‘i=5100(3iβˆ’2)=962(13+298)=48(311)=14928.\sum_{i=5}^{100}(3i-2)=\frac{96}{2}(13+298)=48(311)=14928.

So the answer is

14928.\boxed{14928}.

This is a finite geometric series with first term 192192, common ratio 22, and 77 terms:

βˆ‘i=6123β‹…2i=3βˆ‘i=6122i=3β‹…26βˆ‘i=062i=192β‹…1βˆ’271βˆ’2=192(27βˆ’1).\sum_{i=6}^{12} 3\cdot 2^{i} = 3\sum_{i=6}^{12}2^{i} = 3\cdot2^6\sum_{i=0}^{6}2^i = 192\cdot\frac{1-2^{7}}{1-2} = 192(2^{7}-1).

Since 27=1282^{7}=128, the answer is 192β‹…127192\cdot127 which is

24384.\boxed{24384}.

For a geometric sequence a,720,ba,720,b, the middle term squared equals the product of the neighboring terms:

7202=ab.720^{2}=ab.

Since 720<b720<b, the value of bb is positive, so aa is also positive. We want the least possible integer b>720b>720 such that bb divides 7202720^{2}. Factor:

7202=(24β‹…32β‹…5)2=28β‹…34β‹…52.720^{2}=(2^{4}\cdot 3^{2}\cdot 5)^{2}=2^{8}\cdot 3^{4}\cdot 5^{2}.

So bb must have the form 2Ξ±3Ξ²5Ξ³2^{\alpha}3^{\beta}5^{\gamma}, where 0≀α≀80\le \alpha\le 8, 0≀β≀40\le \beta\le 4, and 0≀γ≀20\le \gamma\le 2. Checking the smallest divisor above 720720:

  • If Ξ³=0\gamma=0, the smallest possible divisor above 720720 is 28β‹…3=7682^{8}\cdot 3=768.
  • If Ξ³=1\gamma=1, we need 2Ξ±3Ξ²>1442^{\alpha}3^{\beta}>144, and the smallest option is 2β‹…34=1622\cdot 3^{4}=162, giving 5β‹…162=8105\cdot 162=810.
  • If Ξ³=2\gamma=2, we need 2Ξ±3Ξ²>28.82^{\alpha}3^{\beta}>28.8, and the smallest option above that is 3232, giving 25β‹…32=80025\cdot 32=800.

Thus the smallest possible value of bb is 768768. Then

a=7202768=675,a=\frac{720^{2}}{768}=675,

which is an integer and satisfies 675<720<768675<720<768. The sum of the digits of 768768 is

7+6+8=21.\boxed{7+6+8=21}.

Let

S=βˆ‘k=0n(nk)3k2nβˆ’k(k+1).S=\sum_{k=0}^{n}\binom{n}{k}3^{k}2^{n-k}(k+1).

Split k+1k+1 into kk and 11:

S=βˆ‘k=0n(nk)3k2nβˆ’kk+βˆ‘k=0n(nk)3k2nβˆ’k.S= \sum_{k=0}^{n}\binom{n}{k}3^{k}2^{n-k}k + \sum_{k=0}^{n}\binom{n}{k}3^{k}2^{n-k}.

The second sum is a direct binomial expansion:

βˆ‘k=0n(nk)3k2nβˆ’k=(3+2)n=5n.\sum_{k=0}^{n}\binom{n}{k}3^{k}2^{n-k}=(3+2)^n=5^n.

For the first sum, use

k(nk)=n(nβˆ’1kβˆ’1).k\binom{n}{k}=n\binom{n-1}{k-1}.

Then

βˆ‘k=0n(nk)3k2nβˆ’kk=βˆ‘k=1nn(nβˆ’1kβˆ’1)3k2nβˆ’k.\sum_{k=0}^{n}\binom{n}{k}3^{k}2^{n-k}k = \sum_{k=1}^{n}n\binom{n-1}{k-1}3^k2^{n-k}.

Factor out 3n3n:

=3nβˆ‘k=1n(nβˆ’1kβˆ’1)3kβˆ’12nβˆ’k.=3n\sum_{k=1}^{n}\binom{n-1}{k-1}3^{k-1}2^{n-k}.

Let j=kβˆ’1j=k-1. Then

3nβˆ‘j=0nβˆ’1(nβˆ’1j)3j2nβˆ’1βˆ’j=3n(3+2)nβˆ’1=3n5nβˆ’1.3n\sum_{j=0}^{n-1}\binom{n-1}{j}3^j2^{n-1-j} =3n(3+2)^{n-1} =3n5^{n-1}.

Therefore

S=3n5nβˆ’1+5n=5nβˆ’1(3n+5).S=3n5^{n-1}+5^n =5^{n-1}(3n+5).

So

βˆ‘k=0n(nk)3k2nβˆ’k(k+1)=5nβˆ’1(3n+5).\boxed{\sum_{k=0}^{n}\binom{n}{k}3^{k}2^{n-k}(k+1)=5^{n-1}(3n+5)}.

For part (A), start with

G(x)=F0+F1x+F2x2+F3x3+⋯ .G(x)=F_0+F_1x+F_2x^2+F_3x^3+\cdots.

Compute

xG(x)=F0x+F1x2+F2x3+β‹―xG(x)=F_0x+F_1x^2+F_2x^3+\cdots

and

x2G(x)=F0x2+F1x3+F2x4+⋯ .x^2G(x)=F_0x^2+F_1x^3+F_2x^4+\cdots.

Then

G(x)βˆ’xG(x)βˆ’x2G(x)G(x)-xG(x)-x^2G(x)

has constant term F0=0F_0=0, coefficient of xx equal to F1=1F_1=1, and for every nβ‰₯2n\ge 2 the coefficient of xnx^n is

Fnβˆ’Fnβˆ’1βˆ’Fnβˆ’2=0.F_n-F_{n-1}-F_{n-2}=0.

Thus

G(x)βˆ’xG(x)βˆ’x2G(x)=x.G(x)-xG(x)-x^2G(x)=x.

Factor:

G(x)(1βˆ’xβˆ’x2)=x.G(x)(1-x-x^2)=x.

Therefore

G(x)=x1βˆ’xβˆ’x2.\boxed{G(x)=\frac{x}{1-x-x^2}}.

For part (B), use

Ξ±+Ξ²=1andΞ±Ξ²=βˆ’1.\alpha+\beta=1 \qquad\text{and}\qquad \alpha\beta=-1.

Then

(1βˆ’Ξ±x)(1βˆ’Ξ²x)=1βˆ’(Ξ±+Ξ²)x+Ξ±Ξ²x2=1βˆ’xβˆ’x2.(1-\alpha x)(1-\beta x) =1-(\alpha+\beta)x+\alpha\beta x^2 =1-x-x^2.

So

G(x)=x(1βˆ’Ξ±x)(1βˆ’Ξ²x).G(x)=\frac{x}{(1-\alpha x)(1-\beta x)}.

Now, just solve out for the constants. We claim that

G(x)=15(11βˆ’Ξ±xβˆ’11βˆ’Ξ²x).G(x)=\frac{1}{\sqrt5} \left( \frac{1}{1-\alpha x} - \frac{1}{1-\beta x} \right).

Check this by combining the fractions (or derive it algebraically which is a bit tedious):

15(11βˆ’Ξ±xβˆ’11βˆ’Ξ²x)=15β‹…(1βˆ’Ξ²x)βˆ’(1βˆ’Ξ±x)(1βˆ’Ξ±x)(1βˆ’Ξ²x).\frac{1}{\sqrt5} \left( \frac{1}{1-\alpha x} - \frac{1}{1-\beta x} \right) = \frac{1}{\sqrt5}\cdot \frac{(1-\beta x)-(1-\alpha x)} {(1-\alpha x)(1-\beta x)}.

The numerator simplifies:

(1βˆ’Ξ²x)βˆ’(1βˆ’Ξ±x)=(Ξ±βˆ’Ξ²)x.(1-\beta x)-(1-\alpha x) =(\alpha-\beta)x.

Since

Ξ±βˆ’Ξ²=5,\alpha-\beta=\sqrt5,

we get

15β‹…(Ξ±βˆ’Ξ²)x(1βˆ’Ξ±x)(1βˆ’Ξ²x)=x(1βˆ’Ξ±x)(1βˆ’Ξ²x).\frac{1}{\sqrt5}\cdot \frac{(\alpha-\beta)x} (1-\alpha x)(1-\beta x) = \frac{x}{(1-\alpha x)(1-\beta x)}.

Thus

G(x)=15(11βˆ’Ξ±xβˆ’11βˆ’Ξ²x).\boxed{ G(x)=\frac{1}{\sqrt5} \left( \frac{1}{1-\alpha x} - \frac{1}{1-\beta x} \right) }.

For part (C), use the geometric series formula:

11βˆ’Ξ±x=βˆ‘n=0∞αnxn\frac{1}{1-\alpha x}=\sum_{n=0}^{\infty}\alpha^nx^n

and

11βˆ’Ξ²x=βˆ‘n=0∞βnxn.\frac{1}{1-\beta x}=\sum_{n=0}^{\infty}\beta^nx^n.

Therefore

G(x)=15(βˆ‘n=0∞αnxnβˆ’βˆ‘n=0∞βnxn).G(x) = \frac{1}{\sqrt5} \left( \sum_{n=0}^{\infty}\alpha^nx^n - \sum_{n=0}^{\infty}\beta^nx^n \right).

Combine the sums:

G(x)=βˆ‘n=0∞αnβˆ’Ξ²n5xn.G(x)= \sum_{n=0}^{\infty} \frac{\alpha^n-\beta^n}{\sqrt5}x^n.

But by definition,

G(x)=βˆ‘n=0∞Fnxn.G(x)=\sum_{n=0}^{\infty}F_nx^n.

Matching coefficients of xnx^n gives

Fn=Ξ±nβˆ’Ξ²n5.\boxed{F_n=\frac{\alpha^n-\beta^n}{\sqrt5}}.

Last updated: