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Unit 2: Compound Structure and Properties

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Electrons are the currency of chemical bonding. Whether electrons are fully transferred, shared, or pooled determines the type of bond and, in broad terms, how strong and how directional that interaction is.

An ionic bond arises between a metal and a nonmetal when electrons are transferred so that both partners approach stable electron counts. The metal loses electrons to become a cation and the nonmetal gains electrons to become an anion. The resulting ions attract one another by Coulomb’s law (see Unit 1). For two point charges Q1Q_1 and Q2Q_2 separated by distance rr, the electrostatic potential energy has the familiar form as seen in Unit 1 (with kk a constant):

U=kQ1Q2rU = k \frac{Q_1 Q_2}{r}

Oppositely charged ions (Q1Q2<0Q_1 Q_2 < 0) lower their energy as rr decreases, which is why a crystal lattice of alternating cations and anions is stable. Lattice energy trends (larger charges, smaller ions) follow from this same inverse dependence on rr and linear dependence on the product of charges.

A standard example is sodium chloride: chlorine accepts an electron to form Clβˆ’\text{Cl}^-, and sodium becomes Na+\text{Na}^+. The compound is held together by attraction between those ions, not by shared pairs in the sense of a covalent bond. There is no universal ranking in which ionic bonds are always strongest; compare the specified substances and the energy required for the same kind of process.

Example. Compare idealized ion-pair attractions for Na+Clβˆ’\mathrm{Na^+Cl^-} and Mg2+O2βˆ’\mathrm{Mg^{2+}O^{2-}} at the same separation. Would doubling the separation of the magnesium-oxide pair make their potential energies equal?

The charge products are βˆ’e2-e^2 and βˆ’4e2-4e^2, so the magnesium-oxide pair has four times the magnitude of attractive potential energy at equal separation. Doubling its separation leaves twice the sodium-chloride magnitude because U∝Q1Q2/rU\propto Q_1Q_2/r. Equal magnitudes would require four times the separation. This compares pair energies, not complete crystal lattice energies.

A covalent bond forms between atoms that are both relatively electronegative, typically two nonmetals, when they share one or more pairs of valence electrons. Neither atom fully owns the electrons; instead, both nuclei are attracted to the same shared density. Bond polarity appears when the two atoms differ in electronegativity: the shared pair is pulled toward the more electronegative atom, giving partial charges (Ξ΄+\delta^+ and Ξ΄βˆ’\delta^-) even though the bond is still covalent. Usually, the cutoff for a bond being polar is a absolute difference of electronegativity above 0.5, and for an ionic bond it is usually 2.0.

Compared with ionic lattices, individual covalent bonds are often discussed in terms of bond energy (the energy required to break one mole of that bond in the gas phase, for a defined process). Triple bonds are generally stronger and shorter than double bonds, which are stronger and shorter than single bonds between the same elements.

Example. Both CO2\mathrm{CO_2} and H2O\mathrm{H_2O} contain polar covalent bonds. Why is only one molecule polar overall?

Bond polarity concerns unequal electron sharing along one bond; molecular polarity concerns the vector sum of all bond dipoles. The equal C-O dipoles cancel in linear CO2\mathrm{CO_2}. The O-H dipoles do not cancel in bent water, leaving a net dipole. Knowing the electronegativity difference without the geometry is insufficient.

In a metal, valence electrons are not localized between two nuclei. Instead, they occupy a sea of delocalized electrons that extends through the crystal, while the metal cations sit in orderly positions. That delocalization explains electrical conductivity and malleability: applying stress shifts ion layers without necessarily breaking localized bonds, because the electron sea can still bind the structure.

Example. A solid does not conduct electricity, but its melt does. Another conducts in both states. Identify the likely bonding models and explain why melting matters.

The first is consistent with an ionic solid: ions are fixed in the lattice but mobile in the melt. The second is consistent with a metal, whose delocalized electrons carry charge in either state. Conductivity depends on mobile charge carriers, so the mere presence of charged particles is insufficient.


Systematic names tell a chemist which elements are present, in what ratio, and (for ions) what the charges are. The rules differ for ionic compounds and molecular (covalent) compounds.

If a substance contains only covalent bonds between nonmetals, it is a molecular compound. For a binary molecular compound (exactly two different elements), use numerical prefixes (mono-, di-, tri-, …) to indicate how many atoms of each element are present. The less electronegative element is usually named first; the second element takes an -ide ending. For example, N2O\text{N}_2\text{O} is dinitrogen monoxide, the prefixes di- and mono- describe a two-to-one ratio of nitrogen to oxygen.

If the second species is a polyatomic ion, name it as such rather than forcing an -ide ending on a single atom. Acids containing hydrogen often have special names; those conventions are developed in Unit 8.

Example. A student reduces N2O4\mathrm{N_2O_4} to NO2\mathrm{NO_2} before naming it. Explain why this changes the answer rather than simplifying the same molecular formula.

Molecular formulas preserve the actual atom counts in one molecule. N2O4\mathrm{N_2O_4} is dinitrogen tetroxide, whereas NO2\mathrm{NO_2} is nitrogen dioxide. They share an empirical ratio but describe different molecules. Reducing a molecular formula discards the information that numerical prefixes are meant to communicate.

An ionic compound is named beginning with the cation. For metals that can take more than one charge in compounds (many transition metals) include the charge as a Roman numeral in parentheses after the metal name: Fe3+\text{Fe}^{3+} in a compound is iron(III). Then name the anion: monatomic anions use the -ide ending (Fβˆ’\text{F}^- is fluoride). Ammonium, NH4+\text{NH}_4^+, behaves like a polyatomic cation in naming even though it contains no metal. Hydrogen ion, H+\text{H}^+, does not behave like a typical metal cation in nomenclature. Prefixes are not used to show stoichiometry in simple ionic names because the charges determine the ratio.

Example. Determine the formula of iron(III) sulfide and explain why Fe3S2\mathrm{Fe_3S_2} is not consistent with the name.

Iron(III) is Fe3+\mathrm{Fe^{3+}} and sulfide is S2βˆ’\mathrm{S^{2-}}. The smallest neutral combination contains two iron ions and three sulfide ions, giving Fe2S3\mathrm{Fe_2S_3}. The proposed Fe3S2\mathrm{Fe_3S_2} would have net charge 3(+3)+2(βˆ’2)=+53(+3)+2(-2)=+5 with those ions. The Roman numeral gives a charge, not a subscript to copy directly.

Organic chemistry is the study of compounds built around carbon frameworks. Many of the same ideas (Lewis structures, hybridization, geometry) carry over, but carbon compounds also use a parallel naming system (IUPAC names, functional groups, and common names). Those details are not necessary for AP Chemistry, and usually organic molecules will be given to you, or will show up on the list of polyatomic ions.

Example. Ethanol and dimethyl ether both have formula C2H6O\mathrm{C_2H_6O}. Draw their atom connectivity and explain why a molecular formula is insufficient to choose an organic name.

Their connectivities are CH3βˆ’CH2βˆ’OH\mathrm{CH_3-CH_2-OH} and CH3βˆ’Oβˆ’CH3\mathrm{CH_3-O-CH_3}. In the first, oxygen is bonded to carbon and hydrogen; in the second, it joins two carbons. These are constitutional isomers with different functional groups and different names. A molecular formula fixes the atom counts, but the bonds between those atoms must also be specified.


Lewis structures are schematic: they show valence electrons and bonds in two dimensions even though real molecules are three-dimensional. They are still very useful for drawing bonds, assigning formal charge, and spotting resonance.

The octet rule says that in many compounds, atoms are most stable when they are surrounded by eight valence electrons (four pairs), matching the noble gas configuration of the noble gas in the same period. Hydrogen and helium are exceptions in the strict sense: hydrogen/helium aim for two electrons (a duet), not eight.

Beryllium and boron in period 2 can form electron-deficient compounds such as BeCl2\text{BeCl}_2 and BF3\text{BF}_3, with fewer than eight electrons around the central atom. Aluminum, in period 3, can also form electron-deficient compounds. There is no general rule that an atom must end with twice its original valence-electron count.

Heavier main-group elements (the square from phosphorus through astatine in the pp block, in the usual textbook treatment) can exhibit expanded octets, using dd orbitals in the hybridization picture to accommodate more than eight valence electrons when they are the central atom in certain compounds.

When drawing, always ask whether the central atom is allowed to expand or must remain octet-complete for the story you are telling.

Example. Why can BF3\mathrm{BF_3} accept an electron pair from NH3\mathrm{NH_3} without breaking a B-F bond? Describe the electron counts before and after bonding.

Boron has three bonds and only six surrounding electrons in BF3\mathrm{BF_3}. Nitrogen’s lone pair supplies the new B-N bond, bringing boron to eight surrounding electrons while nitrogen still has an octet. A valid electron-deficient Lewis structure can therefore explain reactivity; forcing an initial octet onto boron would hide the available acceptor site.

Formal charge is a bookkeeping tool for a single Lewis structure. It assigns each valence electron in the structure either to an atom or to a bond. For an atom,

FC=(valenceΒ eβˆ’Β forΒ theΒ freeΒ atom)βˆ’(nonbondingΒ eβˆ’)βˆ’12(bondingΒ eβˆ’)\text{FC} = (\text{valence } e^- \text{ for the free atom}) - (\text{nonbonding } e^-) - \frac{1}{2}(\text{bonding } e^-)

Structures that minimize formal charge (and place negative formal charge on more electronegative atoms when a choice exists) are generally preferred as major contributors in a resonance hybrid.

Example. In NH4+\mathrm{NH_4^+}, all N-H bonds are covalent. Why does nitrogen nevertheless have formal charge +1+1? Does this mean one identifiable electron was removed from nitrogen after bonding?

Nitrogen is assigned half of the eight bonding electrons and no lone-pair electrons, so its formal charge is 5βˆ’4=+15-4=+1. Formal charge is an equal-sharing bookkeeping convention, not a record of how the species formed or a measurement of the atom’s actual partial charge. Ammonium can form when ammonia’s lone pair binds a proton; no electron has to be removed in that process.

Resonance occurs when two or more Lewis structures differ only in the placement of Ο€\pi bonds and lone pairs, not in the arrangement of nuclei. The classic example is nitrate, NO3βˆ’\text{NO}_3^-: the double bond can be drawn to any of the three oxygen atoms with equal validity. The real ion is a resonance hybrid: a single averaged distribution in which N–O bonds are equivalent by symmetry, with fractional bond order between single and double.

For resonance to be meaningful, the alternative structures must involve the same connectivity; swapping which atoms are bonded (for example, interchanging roles of carbon and nitrogen) is not resonance.

Example. A student draws two ozone contributors and claims that one O-O bond repeatedly switches from single to double. What observation would contradict a literal switching model?

The two O-O bonds are equivalent in the isolated ozone molecule, with lengths intermediate between typical single and double bonds. The contributors describe one delocalized electron distribution, not distinct structures that the molecule alternates between. Moving electrons on paper changes the representation; it does not imply a time-dependent rearrangement of the real bonds.

A practical algorithm:

Example. For CO2\mathrm{CO_2}, compare O-C-O with two single bonds against O=C=O. Both use 16 valence electrons if lone pairs are included. Decide which is the better structure.

In the single-bond drawing, carbon has only four electrons around it and formal charge +2+2, while each oxygen is βˆ’1-1. Converting one lone pair on each oxygen into a bond gives octets on every atom and zero formal charges. Counting total electrons is necessary, but checking local octets and charges is also necessary.


Valence-shell electron-pair repulsion (VSEPR) theory explains electron-domain geometry and molecular shape by assuming that both bonding pairs and lone pairs around a central atom repel one another. The arrangement that maximizes separation minimizes repulsion (thus minimizes the amount of energy needed to hold the molecules) and thus corresponds to observed geometry. A double bond or triple bond counts as one electron domain toward the steric number, just like a single bond or a lone pair.

Typical pairings of steric number and lone pairs give names such as linear, trigonal planar, tetrahedral, trigonal bipyramidal, and octahedral for the electron-domain geometry; lone pairs then influence the molecular geometry (for example, bent instead of trigonal planar when one lone pair sits on a central atom with three domains).

Electron domainsElectron geometryCommon molecular shapeExample
2linearlinearCO2\mathrm{CO_2}
3trigonal planartrigonal planar / bentBF3\mathrm{BF_3} / SO2\mathrm{SO_2}
4tetrahedraltetrahedral / trigonal pyramidal / bentCH4\mathrm{CH_4} / NH3\mathrm{NH_3} / H2O\mathrm{H_2O}
5trigonal bipyramidalseesaw / T-shaped / linearSF4\mathrm{SF_4}
6octahedralsquare pyramidal / square planarBrF5\mathrm{BrF_5} / XeF4\mathrm{XeF_4}

Example. Both CO2\mathrm{CO_2} and SO2\mathrm{SO_2} have two atoms attached to a central atom. Explain why one is linear and the other bent.

Carbon in CO2\mathrm{CO_2} has two electron domains and no lone pair; its bonds point in opposite directions. Sulfur in SO2\mathrm{SO_2} has two bonding domains and one lone-pair domain. Three domains give a trigonal planar electron arrangement, but only the atoms define the bent molecular shape.


Atomic orbitals on a bonded atom can mix to form hybrid orbitals that are consistent with VESPR. For carbon in many organic molecules, four sigma frameworks point toward the corners of a tetrahedron, described by sp3\text{sp}^3 hybridization. sp2\text{sp}^2 hybrids lie in a plane at 120∘120^\circ (trigonal planar arrangement); sp\text{sp} hybrids are linear at 180∘180^\circ. In addition, sp3d\text{sp}^3 d hybridization occurs in trigonal bipyramidal configurations, while sp3d2\text{sp}^3 d^2 hybridization occurs in an octahedral configuration.

Steric numberHybridizationIdeal geometryApprox. angle
2spsplinear180∘180^\circ
3sp2sp^2trigonal planar120∘120^\circ
4sp3sp^3tetrahedral109.5∘109.5^\circ
5sp3dsp^3dtrigonal bipyramidal90∘,120∘90^\circ,120^\circ
6sp3d2sp^3d^2octahedral90∘90^\circ

Example. In CH3CHO\mathrm{CH_3CHO}, must both carbon atoms have the same hybridization because they are in the same molecule? Determine each in the localized bonding model.

The methyl carbon has four sigma-bond directions, giving sp3sp^3. The carbonyl carbon has three sigma-bond directions, giving sp2sp^2; its remaining unhybridized p orbital contributes to the C=O pi bond. Hybridization is assigned locally, not once for the entire molecule.


A sigma bond (Οƒ\sigma) has electron density concentrated along the internuclear axis; it arises from head-on overlap of hybrid or atomic orbitals. A pi bond (Ο€\pi) forms from side-by-side overlap of unhybridized pp orbitals above and below the sigma framework. A single bond is one Οƒ\sigma; a double bond is one Οƒ\sigma plus one Ο€\pi; a triple bond is one Οƒ\sigma plus two Ο€\pi.

Bond order is half the difference between bonding and antibonding electrons in molecular orbital theory, but in Lewis terms it is simply the average number of bonding electron pairs between two atoms across resonance structures. Bond length decreases and bond strength increases as bond order increases between the same two elements.

Example. Count sigma and pi bonds in HC≑Cβˆ’CH=CH2\mathrm{HC\equiv C-CH=CH_2} and explain why counting bond lines alone can mislead.

There are four C-H sigma bonds and three C-C sigma bonds, for seven sigma bonds. The triple bond supplies two pi bonds and the double bond supplies one, for three pi bonds. Every connected pair of atoms has one sigma bond; the additional lines in multiple bonds represent pi bonding.


When two atoms approach, the potential energy of the system typically drops as attractive interactions dominate, passes through a minimum at an equilibrium bond length, and then rises steeply as nuclear repulsion dominates at short distance.

bondlengthstablebondrepulsioninternucleardistancepotentialenergy

Bond energy is related to the depth of that well. Comparing curves for the same bond order (single vs double vs triple) illustrates why higher bond order correlates with shorter, stronger bonds.

These same curves also motivate reaction coordinates later: along a reaction path, the system moves on a potential energy surface connecting reactants, transition states, and products.

Example. Bond X has a deeper potential-energy minimum than bond Y, but its minimum occurs at a larger separation. Which bond is stronger, and which is shorter?

X requires more energy to dissociate from its minimum to separated atoms, so it is stronger. Y has the smaller equilibrium separation, so it is shorter. Well depth measures dissociation energy and the horizontal position measures bond length; neither can be inferred solely from the other for different atom pairs.


The Born–Haber cycle is a Hess’s law (See more in Unit 6) construction for an ionic solid. It expresses the standard enthalpy of formation Ξ”Hf∘\Delta H_f^\circ of the compound from its elements in standard states as a sum of steps that convert those elements into gas-phase ions and then let those ions crystallize. Any one unknown step (most often lattice energy) can be found if the others are known.

Take a 1:1 alkali halide MX\text{MX}, formed from M(s)\text{M}(s) and 12X2(g)\tfrac{1}{2}\text{X}_2(g). Imagine the path:

  1. Atomize the metal (sublimation): M(s)β†’M(g)\text{M}(s) \rightarrow \text{M}(g) with Ξ”H=Ξ”Hsub\Delta H = \Delta H_{\text{sub}} (usually endothermic).

  2. Ionize the metal: M(g)β†’M+(g)+eβˆ’\text{M}(g) \rightarrow \text{M}^+(g) + e^- with Ξ”H=IE\Delta H = \text{IE} (endothermic; use the correct successive ionization energies if more than one electron is lost).

  3. Atomize the halogen: 12X2(g)β†’X(g)\tfrac{1}{2}\text{X}_2(g) \rightarrow \text{X}(g) with Ξ”H=12DX–X\Delta H = \tfrac{1}{2}D_{\text{X–X}} (endothermic; half the X–X\text{X–X} bond enthalpy).

  4. Attach an electron to the halogen: X(g)+eβˆ’β†’Xβˆ’(g)\text{X}(g) + e^- \rightarrow \text{X}^-(g) with Ξ”H=Ξ”Hea\Delta H = \Delta H_{\text{ea}}. For halogens this step is exothermic, so Ξ”Hea\Delta H_{\text{ea}} is negative when reported as an enthalpy change. (If a table lists electron affinity with a different sign convention, convert it to Ξ”H\Delta H for this step before you add.)

  5. Form the crystal from gas ions: M+(g)+Xβˆ’(g)β†’MX(s)\text{M}^+(g) + \text{X}^-(g) \rightarrow \text{MX}(s). This step is strongly exothermic. Textbooks often define lattice energy UlatticeU_{\text{lattice}} as a positive number equal to the endothermic enthalpy of the reverse process: one mole of solid separated into isolated gaseous ions:

MX(s)β†’M+(g)+Xβˆ’(g)Ξ”H=+Ulattice\text{MX}(s) \rightarrow \text{M}^+(g) + \text{X}^-(g) \qquad \Delta H = +U_{\text{lattice}}

Then step 5 (lattice formation from ions) has Ξ”H=βˆ’Ulattice\Delta H = -U_{\text{lattice}}.

Because the overall enthalpy change from M(s)+12X2(g)\text{M}(s) + \tfrac{1}{2}\text{X}_2(g) to MX(s)\text{MX}(s) is Ξ”Hf∘\Delta H_f^\circ,

Ξ”Hf∘(MX, s)=Ξ”Hsub+IE+12DX–X+Ξ”Heaβˆ’Ulattice.\Delta H_f^\circ(\text{MX},\,s) = \Delta H_{\text{sub}} + \text{IE} + \frac{1}{2}D_{\text{X–X}} + \Delta H_{\text{ea}} - U_{\text{lattice}}.

Rearranging isolates the lattice term:

Ulattice=Ξ”Hsub+IE+12DX–X+Ξ”Heaβˆ’Ξ”Hf∘.U_{\text{lattice}} = \Delta H_{\text{sub}} + \text{IE} + \frac{1}{2}D_{\text{X–X}} + \Delta H_{\text{ea}} - \Delta H_f^\circ.

For salts with other stoichiometries (e.g. MgCl2\text{MgCl}_2, Na2O\text{Na}_2\text{O}), use the correct multiple of atomization, all required ionization steps, the appropriate nonmetal atomization (e.g. 12O2\tfrac{1}{2}\text{O}_2), and electron-gain steps that match the anion charge (second-electron addition to oxygen is very endothermic; the huge lattice energy of oxides is what makes the overall formation from elements favorable). The cycle is still closed: the sum of steps along one route equals the sum along any other route between the same two thermodynamic states.

Qualitatively, larger ion charges and smaller ions (shorter internuclear distances in the lattice) increase UlatticeU_{\text{lattice}}, consistent with Coulomb attraction in the lattice and with the trends introduced earlier in this unit. The diagram below shows the energy changes in the cycle.

enthalpyionicsolidseparatedgaseousionsatomsionsformingsublimation/bondionizationelectronaΒ±nitylatticeenergy

Example. For a hypothetical MX salt, sublimation, ionization, half the bond dissociation, and electron gain contribute 100100, 500500, 120120, and βˆ’350Β kJ/mol-350\ \mathrm{kJ/mol}. If formation is βˆ’400Β kJ/mol-400\ \mathrm{kJ/mol}, find the lattice separation energy and explain its sign.

The cycle is βˆ’400=100+500+120βˆ’350βˆ’U-400=100+500+120-350-U, so U=770Β kJ/molU=770\ \mathrm{kJ/mol}. This is positive for separating the crystal into gas ions. The lattice-formation step is instead βˆ’770Β kJ/mol-770\ \mathrm{kJ/mol}; using the positive separation value as a formation term would reverse the physical process.


  1. Which pair has the same electron-domain geometry but different molecular geometries?

    (A) CO2\mathrm{CO_2} and BF3\mathrm{BF_3}
    (B) CH4\mathrm{CH_4} and NH3\mathrm{NH_3}
    (C) BF3\mathrm{BF_3} and NH3\mathrm{NH_3}
    (D) CO2\mathrm{CO_2} and H2O\mathrm{H_2O}

  1. In a simple ionic model, salt X contains +1,βˆ’1+1,-1 ions at separation r, while salt Y contains +2,βˆ’2+2,-2 ions at separation 2r2r. Compare pair-attraction energy magnitudes.

    (A) Y is half of X
    (B) They are equal
    (C) Y is twice X
    (D) Y is four times X

  1. An octet-obeying Lewis structure of NO2βˆ’\mathrm{NO_2^-} contains one N=O bond and one N-O bond. Which formal-charge assignment is correct?

    (A) N is 0, double-bond O is 0, single-bond O is -1
    (B) N is +1 and each O is -1
    (C) N is -1 and both O are 0
    (D) Every atom has zero formal charge

  1. Which observation supports resonance in carbonate rather than one fixed C=O bond?

    (A) Carbonate has a net charge
    (B) Oxygen is more electronegative than carbon
    (C) Carbon has no lone pair
    (D) All three C-O bond lengths are equal and intermediate between typical single and double bonds

  1. In ethene, H2C=CH2\mathrm{H_2C=CH_2}, rotation around the C-C axis is restricted primarily because rotation would disrupt which interaction?

    (A) Overlap of the carbon 1s orbitals
    (B) Side-by-side overlap of the unhybridized p orbitals
    (C) Every C-H sigma bond
    (D) The attraction between separate ethene molecules

  1. For a hypothetical salt, gas-ion formation from the elements costs +450Β kJ/mol+450\ \mathrm{kJ/mol} overall and crystal formation from those ions releases 800Β kJ/mol800\ \mathrm{kJ/mol}. What is the standard formation enthalpy of the solid?

    (A) +1250Β kJ/mol+1250\ \mathrm{kJ/mol}
    (B) +350Β kJ/mol+350\ \mathrm{kJ/mol}
    (C) βˆ’350Β kJ/mol-350\ \mathrm{kJ/mol}
    (D) βˆ’800Β kJ/mol-800\ \mathrm{kJ/mol}

  1. Consider the molecules CH2O\text{CH}_2\text{O} and CH3OH\text{CH}_3\text{OH}.

    (A)(A) Draw a reasonable Lewis structure for each molecule.

    (B)(B) Identify the hybridization of the carbon atom in each molecule.

    (C)(C) Explain which molecule can form stronger intermolecular attractions with water.

    (D)(D) Original extension. Count the sigma and pi bonds in each molecule. Explain why rotation around the carbon-oxygen bond is more restricted in formaldehyde than in methanol.

  1. The 2026 AP Chemistry exam asked students about chromate resonance and VSEPR geometry. (Adapted from College Board, 2026 AP Chemistry FRQ 2.)

    (A)(A) Predict the molecular geometry around chromium in CrO42βˆ’\text{CrO}_4^{2-}.

    (B)(B) Explain why multiple resonance structures can be drawn for CrO42βˆ’\text{CrO}_4^{2-}.

    (C)(C) Explain why the four Cr-O bonds are expected to be equivalent in the resonance hybrid.

    (D)(D) Original extension. Compare formal charges in a chromate structure with four single Cr-O bonds and one with two double and two single Cr-O bonds. Explain why choosing one resonance contributor does not establish two permanently different types of Cr-O bond.