Intuition What this page is for
The parent note showed the idea of resonance. This page drills the calculation you will actually be asked to do: given a molecule, find its bond order , its charge spread , and its resonance energy . We march through every kind of case — symmetric, asymmetric, degenerate (zero resonance), charged, and word-problem style — so no exam twist can surprise you.
Before anything, the two quantities we lean on constantly:
Definition Bond order (the number we compute)
Bond order of a link between two atoms = how many shared electron-pairs "belong" to that link. A single bond = 1 , a double = 2 , a triple = 3 . When resonance spreads a bond over several equivalent links, we average :
B.O. = number of equivalent links total bond-pairs shared among the equivalent links
Higher bond order ⇒ shorter, stronger bond. This is the bridge to Bond Order & Bond Length .
Definition Resonance energy (RE) — the stability we compute
Resonance energy is the extra stability a real (delocalized) molecule has compared to the single best Lewis structure imagined with localized , non-interacting bonds. Written with energies (a lower energy = more stable):
RE = E single structure − E actual hybrid
Because the real hybrid sits lower (more stable) than the single structure, E single > E hybrid , so RE comes out positive — it is the amount of stabilization , a positive number of kJ/mol. A big positive RE ⇒ the molecule is much more stable than any one drawing suggests (benzene, E7). RE ≈ 0 ⇒ one drawing already tells the whole truth (CO₂, E5). Nothing oscillates — it is a static comparison .
Common mistake Watch the sign when you use
Δ H data
In E7 we won't have E single and E hybrid directly — we'll have heats of hydrogenation Δ H (energy released , so negative for exothermic reactions). The safe rule: RE is always the positive stabilization , so compute it as
RE = Δ H predicted − Δ H actual > 0 ,
i.e. "how much less energy the real molecule released, because it was already stabilized." Keep RE positive and you can never mix the sign up.
Every resonance problem you can be handed falls into one of these cells . The examples below are tagged with the cell they cover, and together they hit all of them.
Cell
Case class
What makes it tricky
Example
A
Symmetric, 2 equal forms
split one π over 2 links
E1 (ozone)
B
Symmetric, 3 equal forms + net charge
split charge too
E2 (carbonate)
C
Ring delocalization (aromatic)
count π over a loop
E3 (benzene)
D
Asymmetric — forms not equal
must weight them
E4 (OCN⁻)
E
Degenerate / zero — only one valid form
resonance energy = 0
E5 (CO₂ vs "fake")
F
Charged, non-equivalent oxygens
mix of B.O. on one molecule
E6 (nitrate vs nitrite)
G
Word / real-world — heats of hydrogenation
build RE from data
E7 (benzene RE)
H
Exam twist — limiting/edge reasoning
naive averaging fails
E8 (allyl vs butadiene ends)
Worked example Find the O–O bond order and charge on each O in
O 3 .
Forecast: guess the bond order now — is it 1 , 1.5 , or 2 ? And where does the negative charge sit?
1. Draw both structures.
O = O + − O − ↔ O − − O + = O
Why this step? The extra π-bond can sit on the left or the right O. Both drawings obey the octet and have the same charges, so they are equally valid — a symmetric pair (Cell A).
2. Count bond-pairs on one O–O link across all forms.
Left link: double (2) in form 1, single (1) in form 2. That's 1 + 2 = 3 pairs over 2 forms.
Why this step? Bond order averages the pairs that occupy that link as we sweep through the forms.
3. Divide.
B.O. = 2 1 + 2 = 1.5
Why this step? Delocalization means the real bond is literally the average of the two drawings.
4. Spread the charge. The two terminal O's are equivalent, each carries − 1 in exactly one of the two forms, so each holds
2 − 1 = − 2 1 on average.
The central O keeps + 1 throughout. (See Formal Charge for how the + / − were assigned.)
Verify: predicted bond length is between single (148 pm) and double (121 pm) — real O₃ is 128 pm ✔. Total charge = ( + 1 ) + 2 ( − 2 1 ) = 0 ✔ (ozone is neutral).
Worked example Bond order and per-oxygen charge in
CO 3 2 − .
Forecast: three oxygens, one double bond. Will B.O. be more or less than ozone's 1.5 ?
1. Draw all three structures. The single C=O rotates among the three oxygens — three symmetric forms (Cell B, with a real 2 − charge to also spread).
Why this step? Each drawing is one snapshot; because all three are equally valid, the averaging formula treats every C–O link on equal footing — we need every form on the page before we can average across them.
2. Count bond-pairs on one C–O link. Across the three forms a given C–O is: double (2) once, single (1) twice ⇒ 2 + 1 + 1 = 4 pairs.
Why this step? Same averaging idea, now over three equivalent links.
3. Divide.
B.O. = 3 2 + 1 + 1 = 3 4 ≈ 1.33
Why this step? One π-bond shared over three links gives a smaller extra share than one π over two — so it's less than ozone's 1.5 , matching the forecast intuition.
4. Spread the charge. The 2 − sits equally on three oxygens:
3 − 2 ≈ − 0.67 per O.
Verify: all three C–O equal, length between single (143 ) and double (122 ) — real is ∼ 129 pm ✔. Charge check: 3 × ( − 3 2 ) = − 2 ✔.
Worked example Bond order of each C–C in benzene.
Forecast: aromatic ring — same as ozone or different?
1. The two Kekulé forms. Each C–C is single in one drawing, double in the other.
Why this step? The three π-bonds shift as a set around the loop; two forms suffice by symmetry.
2. Average one link.
B.O. = 2 1 + 2 = 1.5
Why this step? Each link is single once, double once — identical to ozone's arithmetic.
3. Consequence. All six equal ⇒ perfect hexagon.
Verify: predicted length between 154 (single) and 134 (double) — real is 139 pm ✔. This delocalization is the source of aromatic stability , built from the parallel p-orbitals of Hybridization ($sp^2$) .
This is the cell students lose marks on: the forms are not equal , so you cannot just average blindly — you must weight them, and then average with those weights .
The figure below lays the three forms side by side, colour-coded by how much each contributes — read it top (best) to bottom (worst), following the up-arrow of increasing stability.
Worked example Rank the cyanate
OCN − forms, then estimate the weighted bond orders and charge spread.
Forecast: three drawings differ in where the double bonds and the − 1 sit. Which is best — and will the C–O or the C–N bond come out stronger?
1. Draw the three forms (moving only π/lone pairs, nuclei fixed):
Form I: O − − C ≡ N — negative on oxygen ; C–O single, C–N triple.
Form II: O = C = N − — negative on nitrogen ; C–O double, C–N double.
Form III: O + ≡ C − N 2 − — charges large and separated; C–O triple, C–N single.
Why this step? Unlike the symmetric cells, here the forms are not interchangeable , so we cannot just average equally — we must lay all candidates out first, then judge each one's stability to decide how much it contributes to the hybrid.
2. Apply the weighting rules (from the parent note): least charge, more bonds, negative on the more electronegative atom.
Why this step? Unequal forms contribute unequally; the most stable drawing describes the real molecule best.
3. Score and assign approximate weights (these numbers are also written on figure s01, so you never need the colours):
Form I: − 1 on O (electronegativity 3.44 ) — very good ✔. Weight ≈ 0.60 (dominant).
Form II: − 1 on N (3.04 ) — decent, less good. Weight ≈ 0.35 .
Form III: a + 1 and a 2 − , charges separated — worst . Weight ≈ 0.05 (negligible).
Why this step? Oxygen is more electronegative than nitrogen, so it "wants" the negative charge more; the split-charge form barely counts.
4. Weighted bond orders. Multiply each form's bond order by its weight and add. With C–O bond orders ( 1 , 2 , 3 ) and C–N bond orders ( 3 , 2 , 1 ) for forms ( I , II , III ) :
B.O. C-O = 0.60 ( 1 ) + 0.35 ( 2 ) + 0.05 ( 3 ) = 1.45
B.O. C-N = 0.60 ( 3 ) + 0.35 ( 2 ) + 0.05 ( 1 ) = 2.55
Why this step? The hybrid is the weighted blend, not the equal average — this is exactly what makes Cell D different from Cells A–C.
5. Weighted charge spread. The − 1 sits on O in Form I, on N in Form II, and (as part of a − 2/ + 1 ) mostly on N in Form III:
q O ≈ − 0.60 , q N ≈ − 0.40.
Why this step? The dominant Form I puts more of the negative charge on oxygen — consistent with the ranking.
Verify: the C–N bond order (2.55 ) exceeds the C–O bond order (1.45 ), so the C–N bond is shorter/stronger — real OCN⁻ has C–N ≈ 117 pm (near triple) vs C–O ≈ 126 pm (near single–double) ✔. Charge check: q O + q N = − 0.60 + ( − 0.40 ) = − 1 ✔ (matches the anion charge). Weights sum: 0.60 + 0.35 + 0.05 = 1 ✔.
CO 2 gain resonance energy? Compare its "single structure" to reality.
Forecast: CO₂ is O = C = O . Is there delocalization energy like benzene?
1. Draw the main structure: O = C = O , symmetric, no formal charge, full octets.
Why this step? RE is measured relative to the best single structure (see the definition up top). So we must first pin down that dominant drawing — it is the E single structure baseline against which any delocalization stabilization would be measured.
2. Are there other equal forms? You can draw O − − C ≡ O + , but it has separated charges — a worse, minor form. There is no set of equivalent, equally-good structures like ozone's.
Why this step? Resonance energy needs several forms of comparable stability to blend. When one dominant form vastly outweighs the rest, delocalization is minimal.
3. Conclusion. The best single structure already describes CO₂ almost perfectly, so
RE ≈ 0.
Why this step? RE = E single − E hybrid ; if the hybrid ≈ the single structure, the difference vanishes — the zero / degenerate cell.
Verify: both C=O bonds are 116 pm — very close to a pure C=O double (122 pm elsewhere), not stretched toward single. No bond-length "smearing" ⇒ negligible resonance ✔. Contrast: ozone's 128 pm sits between single and double, betraying real delocalization.
Worked example Compare N–O bond order in
NO 3 − and NO 2 − .
Forecast: which has the shorter N–O bond?
1. Nitrate NO 3 − : three equal forms, one N=O rotating over three oxygens.
B.O. = 3 2 + 1 + 1 = 3 4 ≈ 1.33
2. Nitrite NO 2 − : two equal forms, one N=O over two oxygens.
B.O. = 2 1 + 2 = 1.5
Why this step? Same one π-bond, but shared over fewer links in nitrite ⇒ bigger share each ⇒ higher bond order.
3. Compare. 1.5 > 1.33 , so nitrite's N–O is shorter/stronger than nitrate's.
Why this step? Higher bond order ⇒ shorter bond (the Bond Order & Bond Length rule).
Verify: measured N–O is ∼ 124 pm in nitrite vs ∼ 126 pm in nitrate — nitrite indeed shorter ✔. Charge: nitrate spreads − 1 over 3 O (− 3 1 each), nitrite over 2 O (− 2 1 each) ✔.
The bar chart below turns the three data points into energies: the tall pink bar is the predicted release for three isolated double bonds, the yellow bar is what benzene actually releases, and the pink double-arrow between them is the resonance energy gap.
Δ H (what the data means)
Δ H is the enthalpy change of a reaction: the heat exchanged at constant pressure. For hydrogenation (adding H₂ across a double bond) the reaction is exothermic , so it releases heat and Δ H is negative (e.g. − 120 kJ/mol). A more negative Δ H means more heat released , which means the starting molecule was less stable to begin with. We only ever compare magnitudes of Δ H here, so the sign confusion cannot creep in.
Worked example Given: hydrogenating
cyclohexene releases 120 kJ/mol; hydrogenating benzene releases 208 kJ/mol. Find benzene's resonance energy.
Forecast: three double bonds — will "fake benzene" release about 360 ? Will real benzene release more or less ?
1. Cost of one localized C=C. Cyclohexene has exactly one double bond:
Δ H one = − 120 kJ/mol , ∣Δ H one ∣ = 120 kJ/mol .
Why this step? It calibrates the energy released per isolated double bond.
2. Predict "cyclohexatriene" (fake benzene). If benzene were three separate C=C:
Δ H predicted = 3 × ( − 120 ) = − 360 kJ/mol , ∣Δ H predicted ∣ = 360.
Why this step? Builds the E single structure baseline, assuming bonds don't interact.
3. Real benzene releases less.
Δ H actual = − 208 kJ/mol , ∣Δ H actual ∣ = 208.
Why this step? Less energy released means benzene started lower (more stable) — see figure s02, the actual (yellow) bar is shorter than the predicted (pink) one.
4. Take the difference of magnitudes (keeps RE positive).
RE = ∣Δ H predicted ∣ − ∣Δ H actual ∣ = 360 − 208 = + 152 kJ/mol .
Why this step? RE = "how much less heat the real molecule gave off" = the stability it already had from delocalization. This equals the boxed E single − E hybrid because the more stable (lower-energy) hybrid releases less on hydrogenation. RE is a positive stabilization .
Verify: magnitude 152 kJ/mol ≈ 150 (the parent's recall value) ✔. Sign: benzene is more stable, and RE = + 152 > 0 as the definition demands ✔. Units: kJ/mol throughout ✔.
The trap: "resonance means all atoms share equally." False. Some positions carry charge; others carry none . This edge reasoning separates top scorers.
Worked example In the allyl anion
[ CH 2 -CH-CH 2 ] − , on which carbons does the − 1 charge live?
Forecast: all three carbons, or only some?
1. Draw the two forms.
Form 1: C − H 2 − CH = CH 2 — negative on C1 .
Form 2: CH 2 = CH − C − H 2 — negative on C3 .
Why this step? Only the π-bond and the lone pair shift; the middle carbon is double-bonded in both forms.
2. Where does the charge appear? C1 in form 1, C3 in form 2 — the middle carbon C2 is never charged in either form.
Why this step? Averaging: C2's charge = 2 0 + 0 = 0 . The ends: each is − 1 in one of two forms ⇒ − 2 1 each.
3. Bond order of each C–C link. Each C–C is single in one form, double in the other:
B.O. = 2 1 + 2 = 1.5.
Why this step? The bonds delocalize even though the charge does not sit on the centre.
4. The twist stated plainly. Delocalization spreads the charge to the terminal carbons only, while the bonding is equal across both links.
Verify: charge check 2 × ( − 2 1 ) + 0 = − 1 ✔ (matches the anion charge). Symmetry: swapping C1↔C3 maps form 1↔form 2, confirming ends are equivalent and the middle is special ✔. Molecular Orbital Theory confirms it: the non-bonding MO has a node exactly on C2, so C2 holds no extra electron density.
Recall Cover the answers first
O₃ bond order ::: 1.5
CO₃²⁻ bond order ::: 4/3 ≈ 1.33
NO₂⁻ vs NO₃⁻ — which shorter N–O? ::: nitrite (B.O. 1.5 > 1.33)
Benzene resonance energy ::: +152 kJ/mol (positive stabilization)
CO₂ resonance energy ::: ≈ 0 (one dominant structure)
Allyl anion — charge on middle carbon? ::: zero; only the two ends carry −½
Which OCN⁻ form dominates, O⁻ or N⁻? ::: the O⁻ form (oxygen more electronegative)
Mnemonic The averaging shortcut
"Total π-pairs ÷ equal links = bond order." Then for charge: "net charge ÷ equivalent atoms." But first check the forms are actually equal (Cell D warns you — there you must weight ) and that more than one good form exists at all (Cell E warns you). And for RE: "keep it positive — bigger box, lower energy, plus sign."
Yeh Hinglish mein →
Formal Charge — the ranking tool for asymmetric cases (E4).
Bond Order & Bond Length — turns every B.O. above into a predicted length.
Molecular Orbital Theory — explains the allyl node in E8.
Aromaticity & Hückel's Rule — why benzene's RE (E7) is exceptionally large.