Module 1 gave you tools for drawing a molecule as a single fixed structure. This module is about what happens when a single structure is not good enough — when the electrons in a molecule are genuinely spread over more atoms than any one Lewis drawing can show. That spreading out is delocalization, and it is the most important stabilizing effect in organic chemistry. Resonance is how we draw it.
What resonance is
Some molecules and ions cannot be captured by a single Lewis structure. When you can draw two or more valid structures that differ only in where the electrons are — never in where the atoms are — those are resonance structures, conventionally linked by a double-headed arrow (↔).
The real molecule is a single resonance hybrid: a blend of every valid structure, existing at all times. It is not flipping back and forth between them. This is the point people most often get wrong, so it is worth stating in the strongest terms.
The requirement: conjugation
Resonance is not available everywhere. It requires that the electrons in question have somewhere adjacent to go — specifically, an available p orbital next door that theirs can overlap with.
In practice this means one of three arrangements: a lone pair next to a pi bond; a pi bond next to another pi bond; or a lone pair or pi bond next to an empty p orbital, such as a carbocation. A system connected this way is conjugated, and delocalization runs the length of the conjugated system and stops where the conjugation stops.
The word "adjacent" is doing real work. An sp³ carbon between two pi bonds breaks the conjugation entirely, because it has no available p orbital to pass the electrons through. A lone pair with no neighboring pi bond or empty orbital has nowhere to delocalize into, and there is simply no resonance structure to draw.
The carboxylate carbon is double-bonded to one oxygen and single-bonded to another that carries the negative charge and three lone pairs. Push one of that oxygen's lone pairs into a new C–O pi bond, and simultaneously push the existing C=O pi bond up onto the other oxygen as a lone pair.
You now have a second structure, identical to the first except that the double bond and the charge have swapped oxygens. Because the two oxygens are equivalent by symmetry, both structures contribute equally — there is no major contributor here.
The experimental payoff: both C–O bonds in acetate are measured at 126 pm, exactly between a C–O single bond (143 pm) and a C=O double bond (123 pm), and both oxygens carry exactly −½ charge. Neither drawn structure says that. The hybrid does.
Ranking contributors
When resonance structures are not equivalent, they do not contribute equally, and the more stable structure dominates the hybrid. Rank them with these criteria, in roughly this order of importance:
- Complete octets win. A structure where every second-row atom that can have a full octet has one beats a structure that leaves an atom electron-deficient. This criterion outranks the charge rules below.
- Fewer and smaller formal charges win. No charges beats +1/−1, which beats +2/−2.
- Negative charge belongs on the more electronegative atom, and positive charge on the less electronegative one.
- Like charges should not sit on adjacent atoms. Two adjacent negatives, or two adjacent positives, is electrostatically expensive.
- More bonds and less charge separation generally wins when everything else is close.
None of the valid structures is "wrong" to draw — each contributes something. These rules only say which contributes more.
How much stabilization are we talking about?
Resonance stabilization is not a small correction. The allyl cation is roughly 15 kcal/mol more stable than a comparable non-delocalized cation, which is why a carbocation next to a double bond forms as readily as one carrying three carbon neighbours, despite carrying only two — Module 6 explains why the neighbour count matters in the first place. Benzene is about 36 kcal/mol more stable than the hypothetical non-delocalized "cyclohexatriene," which is the entire reason aromatic compounds behave as a separate class. An amide's C–N bond has roughly 18 kcal/mol of rotational barrier from resonance, enough to lock it flat — which is why peptide bonds are planar and why protein secondary structure exists at all.
The three moves
Nearly every resonance structure you will ever draw comes from one of three electron pushes, and recognizing them turns resonance from guesswork into pattern matching.
Lone pair into an adjacent pi bond. The lone pair becomes a new pi bond, and the old pi bond's electrons move onto the far atom as a lone pair. This is acetate, and it is every amide, ester and enolate.
Pi bond into an adjacent empty orbital. The pi electrons slide over to form a new bond with a carbocation next door, moving the positive charge to the far end. This is the allyl cation, and it is the mechanism behind allylic rearrangement in Module 6.
Pi bond broken onto one atom. The pi electrons collapse onto the more electronegative atom, generating a charge-separated structure. This is the minor but crucial contributor that makes a carbonyl carbon electrophilic — the resonance form with C⁺ and O⁻ is a poor contributor by the ranking rules, but it is exactly the one that predicts the reactivity.
What carries forward
Resonance is the single most reusable idea in the rest of the course. It sets the acidity of carboxylic acids, phenols and alpha hydrogens in Modules 3 and 11; it stabilizes the carbocations of Modules 6 and 7; it is what makes an amide unreactive and an acid chloride ferocious in Module 10; it defines aromaticity in Module 13; and the directing effects of Module 13 are resonance arguments almost in their entirety. The next section teaches the notation for getting from one structure to another without breaking any rules.