Nucleophilic Substitution at Saturated Carbon
This is the most examined mechanism in organic chemistry and the one students think they already understand. The two-mechanism picture taught at undergraduate level is a simplification, and the exam knows it. This part builds the real picture: the continuous spectrum between the two extremes, the ion pairs that explain partial racemisation, the substrates that refuse to react by either route, and the experimental evidence — rate laws, stereochemistry, salt effects, isotope effects — that tells you which pathway you are looking at. Two layers on every section: a slow, hand-held beginner path and a research-grade advanced/reference path.
The 9 sections in Part 4
- 1The SN2 transition state, backside attack and Walden inversion Free below
- 2Substrate structure — steric control, and the carbons that never react
- 3The nucleophile — nucleophilicity is not basicity
- 4The SN1 mechanism, the rate law, and the price of a carbocation
- 5Ion pairs — the mechanism between the two mechanisms
- 6Solvolysis, the Winstein–Grunwald treatment, and the borderline region
- 7Leaving-group ability and its correlation with conjugate-acid pKa
- 8Solvent effects on both mechanisms — the Hughes–Ingold analysis
- 9Ambident nucleophiles, allylic systems, and the decision procedure
The SN2 transition state, backside attack and Walden inversion
Free extractSection D.1 of Part 4, reproduced in full from the book — figures and all. No sign-in, no paywall on this section.
One step, one transition state, no intermediate — and a geometry that is forced on the reaction by the shape of an orbital.
Start from the observation, not the picture. When methyl bromide is treated with hydroxide in aqueous ethanol, doubling the concentration of methyl bromide doubles the rate; doubling the concentration of hydroxide also doubles the rate. The rate law is second order overall, first order in each partner.
A rate law counts the species present in and before the rate-determining transition state. Both partners appear, so both are present in the transition state — hence bimolecular, the ‘2’ in SN2. The mechanism has exactly one step: bond making and bond breaking are concerted, and there is no intermediate of any lifetime.
Mechanism — SN2 — concerted bimolecular substitution
- The nucleophile approaches the carbon along the line of the C–X bond, from the face opposite the leaving group.
- In a single continuous motion the Nu–C bond forms while the C–X bond breaks; the transition state has partial bonds to both, and negative charge shared between Nu and X.
- The three spectator groups flatten into a plane containing the carbon and then continue through to the other side.
- Product and leaving group separate. Configuration at carbon is inverted.
Why 180°? Not by decree. The nucleophile has to put electrons somewhere, and the only orbital available on the substrate that can take them and simultaneously weaken the C–X bond is the antibonding σ*(C–X). That orbital is built out of a carbon lobe and a halogen lobe of opposite phase, with a node between them, and the carbon lobe — the big one, because carbon is the less electronegative partner — points away from X. Overlap with it is best along the extension of the X–C axis. Approach from anywhere else means poorer overlap, and approach from the front means overlapping the small out-of-phase halogen lobe as well, which cancels part of the interaction.
The stereochemical consequence — Walden inversion
If the nucleophile always arrives on the face opposite the leaving group, then at a stereogenic carbon the product configuration is fixed by the mechanism, not by chance. The three spectator groups are pushed through the plane like an umbrella in a gale.
The name is historical, and the history is worth thirty seconds because it is examinable. In the 1890s Paul Walden found that malic acid could be converted into chlorosuccinic acid and back again, and that the sign of rotation you ended with depended on which reagents you used and in which order. Starting from a single enantiomer of malic acid, one two-step sequence returned that same enantiomer while a different two-step sequence returned its mirror image. Since the starting material was the same in both cases, at least one of the steps must have turned the molecule inside out. That was the first evidence that a substitution can change configuration at carbon, decades before anyone could draw a transition state.
The trap inside the definition: R/S is a name, not a geometry
Configuration inverts every time. The CIP descriptor may or may not change with it, because the descriptor depends on the priority ranking of four groups and you have just swapped one of them. Work through the mechanical rule once and you will never guess again:
(R)-2-Bromooctane is treated with sodium hydroxide in aqueous acetone. Give the product with its configuration. Easy
Methyl (R)-2-bromopropanoate is treated (a) with NaCN and (b) with NaN3, both in DMF. Both reactions are clean SN2. Give both products with configurations. Medium
The experimental case for the concerted mechanism, the isotope-effect evidence, and what the transition state looks like when it is not symmetrical.
Proving inversion without knowing any absolute configuration
The neatest experiment in the field, and a standing favourite in Part C, uses radioactive iodide and optically active 2-iodooctane. Treat the enantiopure iodide with 128I− (or any labelled iodide) in acetone and monitor two things independently: the rate at which label enters the organic compound, and the rate at which optical rotation decays.
If every substitution event inverts, then each act of exchange converts one molecule of the (R) form into one molecule of the (S) form. That destroys two units of optical activity per event — the molecule that inverted no longer contributes its rotation, and it now cancels a partner. Hence:
krac = kexch (complete retention or attack on a symmetric intermediate)
The measured ratio is 2. Notice how much the experiment gets for free: it needs no knowledge of absolute configuration, no reference compound, and no assumption about which way round the molecule is. It is a relative measurement, and it is decisive.
Kinetic isotope effects: measuring the crowding at the transition state
Replace the hydrogens on the reacting carbon by deuterium and the rate barely changes — but the direction and size of the small change is diagnostic. An α-deuterium secondary kinetic isotope effect reports on how the out-of-plane bending vibration of the C–H bond changes between the ground state and the transition state.
| Mechanism | Coordination at the reacting carbon in the TS | Typical kH/kD per α-D |
|---|---|---|
| SN2 | Five — more crowded than the ground state; the C–H bending mode stiffens | ≈ 0.95–1.06 (unity or slightly inverse) |
| SN1 (ionisation) | Three — less crowded; the bending mode loosens as carbon flattens | ≈ 1.15–1.25 (clearly normal) |
The transition state is not a fixed object
Textbook drawings show a symmetrical transition state with Nu–C and C–X equally formed. Real ones are almost never symmetrical, and where they sit is governed by the same Hammond-type reasoning developed in Part 2. Two independent coordinates matter: how far the C–X bond has broken and how far the Nu–C bond has formed. A transition state in which both are advanced is called tight (or associative); one in which C–X breaking runs ahead of Nu–C making, leaving substantial positive charge on carbon, is loose (or dissociative, or ‘exploded’).
Better nucleophiles and poorer leaving groups tighten the transition state; poorer nucleophiles, better leaving groups and cation-stabilising substituents loosen it. A loose SN2 transition state has a great deal in common with an SN1 ion pair, and that overlap — not any sharp boundary — is what the borderline region of D.6 is made of. The two-dimensional bookkeeping device for this is the More O’Ferrall–Jencks diagram, drawn in D.6.
Gas phase: the barrier you see in solution is mostly desolvation
Run the same reaction with no solvent at all, in a mass spectrometer, and the energy profile changes shape completely. An anion and a neutral molecule attract each other, so they first fall into an ion–dipole complex that lies below the separated reactants. From there the system climbs to a central barrier and falls into a second ion–dipole complex on the product side. The result is a double-well profile, and for many identity reactions the central barrier lies below the energy of the separated reactants — the reaction has a negative apparent activation energy measured from infinite separation.
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Read the rest of Part 4
The remaining 8 sections of this part — Substrate structure — steric control, and the carbons that never react, The nucleophile — nucleophilicity is not basicity, The SN1 mechanism, the rate law, and the price of a carbocation… — and all nine parts of Reaction Mechanisms are part of ChemVidya Full Access, along with the other books, 55 Study Notes and 6,000+ practice questions.
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