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The Hammett Equation — Substituent Effects as a Straight Line

By Aniket Bhardwaj · 15 September 2026 · Advanced Chemistry

Physical organic chemistry has one central question: what is actually happening at the transition state? You cannot photograph a transition state, so you probe it indirectly. The Hammett equation is the oldest and still the most used of those probes. You change a substituent on a benzene ring, measure how the rate or equilibrium changes, plot the results, and the slope of that straight line tells you whether positive or negative charge is building up in the rate-determining step. This is standard CSIR-NET and GATE organic material, and it is one of the few topics where a genuine least-squares fit is part of the chemistry.

The equation

log (kX / kH) = σ ρ      and for equilibria   log (KX / KH) = σ ρ

What each symbol means:

Both σ and ρ are dimensionless. Because log k is proportional to a free energy (ΔG‡ = −RT ln k + constant), a straight line in log k is a straight line in free energy — which is why this family of relationships is called a linear free energy relationship (LFER).

Where σ values come from

σ is not fitted to the reaction you are studying. It is defined once, from the ionisation of substituted benzoic acids in water at 25 °C, and that reference reaction is assigned ρ = 1 exactly:

σ = log (Ka,X / Ka,H) = pKa(benzoic acid) − pKa(substituted benzoic acid)

Worked example 1 — deriving σp for the nitro group.
Benzoic acid has pKa ≈ 4.20; 4-nitrobenzoic acid has pKa ≈ 3.42.
σp(NO2) = 4.20 − 3.42 = +0.78

The positive sign says the nitro group withdraws electron density, stabilises the carboxylate anion, and therefore makes the acid stronger. Different compilations quote pKa values that differ in the second decimal place, so tabulated σp for NO2 is usually given as 0.78 but you will also see 0.81 — use one table consistently rather than mixing sources.

Some widely tabulated values, for orientation:

SubstituentσmetaσparaElectronic character
−NO2+0.71+0.78Strongly withdrawing (−I, −M)
−CN+0.56+0.66Withdrawing (−I, −M)
−Cl+0.37+0.23Withdrawing by induction, weakly donating by resonance
−H0.000.00Reference
−CH3−0.07−0.17Weakly donating (+I, hyperconjugation)
−OCH3+0.12−0.27Withdrawing from meta, donating from para (+M)
−NH2−0.16−0.66Strongly donating by resonance

Look carefully at −Cl and −OCH3. Their meta and para values have opposite signs or very different sizes, because resonance donation reaches the para position but not the meta position, while induction reaches both. That single observation is the reason two separate scales exist at all.

Worked example 2 — predicting a rate ratio

Problem: a reaction of substituted benzene derivatives is found to have ρ = +2.30. By what factor does a para-nitro group speed it up relative to the unsubstituted compound?

log (kX/kH) = σp × ρ = 0.78 × 2.30 = 1.794
kX/kH = 101.794

Break the power up: 101.794 = 101 × 100.794. Since log 6.22 = 0.794, we get 100.794 = 6.22.
kX/kH = 10 × 6.22 = 62 times faster.

Now repeat for a para-methoxy group, σp = −0.27:
log (kX/kH) = (−0.27)(2.30) = −0.621
kX/kH = 10−0.621 = 0.239, i.e. about 4.2 times slower (1 ÷ 0.239 = 4.18).

So across just these two substituents the rate spans a factor of 62 ÷ 0.239 ≈ 260. A modest σ range produces a large rate range because the relationship is logarithmic.

Worked example 3 — fitting ρ by least squares

In practice you do the opposite: you measure rates, and the slope gives you ρ. Suppose a set of measurements gives these four points.

Substituentx = σy = log(kX/kH)
p-OCH3−0.27−0.62
H0.000.00
p-Cl0.230.53
p-NO20.781.79

Step 1 — means.
Σx = −0.27 + 0 + 0.23 + 0.78 = 0.74, so x̄ = 0.74 ÷ 4 = 0.185
Σy = −0.62 + 0 + 0.53 + 1.79 = 1.70, so ȳ = 1.70 ÷ 4 = 0.425

Step 2 — deviations and their products.
(−0.455)(−1.045) = 0.475475
(−0.185)(−0.425) = 0.078625
(0.045)(0.105) = 0.004725
(0.595)(1.365) = 0.812175
Σ(x − x̄)(y − ȳ) = 1.371000

Step 3 — sum of squared x deviations.
(−0.455)² = 0.207025; (−0.185)² = 0.034225; (0.045)² = 0.002025; (0.595)² = 0.354025
Σ(x − x̄)² = 0.597300

Step 4 — slope and intercept.
ρ = 1.371000 ÷ 0.597300 = +2.30
intercept = ȳ − ρx̄ = 0.425 − (2.2953 × 0.185) = 0.425 − 0.4246 = 0.0004 ≈ 0

The intercept coming out at essentially zero is not luck — it is the built-in check on your working. Because σ(H) = 0 and log(kH/kH) = 0, a correct Hammett plot must pass through the origin. If your fitted intercept is far from zero, you have either used the wrong reference kH or mixed up meta and para σ values.

Reading the sign and size of ρ

ρ valueWhat it means about the transition stateTypical situation
Large positive (ρ > +1)Negative charge builds up near the ring; electron-withdrawing groups helpNucleophilic attack on a carbonyl; ester saponification
Small positiveSlight negative charge build-up, or the reaction centre is far from the ringSide-chain reactions several bonds away
Near zeroLittle charge change, or opposing effects cancelRadical reactions, some concerted processes
Negative (ρ < 0)Positive charge builds up; electron-donating groups helpSN1 solvolysis of benzylic halides; electrophilic aromatic substitution

A break or curvature in the plot is itself a result, not a failure. If electron-rich substituents lie on one line and electron-poor ones on another, the usual interpretation is a change of mechanism or a change in the rate-determining step across the series. Hunting for that break is often the whole point of running the study.

The σ+ and σ scales

The ordinary σ scale is calibrated on benzoic acid ionisation, where the substituent and the reaction centre are separated by the carboxyl carbon. When the transition state puts charge in direct conjugation with the substituent, ordinary σ under-describes it and the plot goes crooked. Two extra scales exist for this:

Choosing the scale that straightens the plot is itself mechanistic evidence: if only σ+ gives a good line, direct resonance stabilisation of a cationic centre is implicated. Related treatments you may meet by name include the Yukawa–Tsuno equation, which blends σ and σ+, and the Taft equation, which separates polar from steric effects for aliphatic systems.

Common mistakes that cost marks

  • Using σpara for a meta substituent. They are genuinely different numbers, and for OCH3 they even have opposite signs. Always read the position from the structure first.
  • Applying Hammett to ortho substituents. The standard scales do not cover ortho, because steric interference and direct field effects contaminate the purely electronic term. Ortho points are simply left out.
  • Forcing the fit through a nonzero intercept. The origin is a theoretical requirement here, not a fitting choice.
  • Reading ρ as a bond order or a charge. ρ measures sensitivity, not the number of electrons moved. A ρ of +2.3 does not mean "2.3 units of negative charge".
  • Mixing σ and σ+ in the same plot. Pick one scale for the whole data set and say which you used.
  • Comparing ρ across different solvents or temperatures. ρ is defined for a specific set of conditions; changing the solvent changes ρ.
  • Using ln instead of log. The equation is defined with base-10 logarithms. Using natural logs inflates every value by a factor of 2.303.

Where this appears in exams

ExamTypical use
CSIR-NETSign and interpretation of ρ; deducing a mechanism from a Hammett plot; σ vs σ+ choice
GATE (Chemistry)Numerical: calculate kX/kH from given σ and ρ, or find ρ from two data points
IIT-JAMQualitative substituent effects on acidity and reactivity, the conceptual base of this topic
M.Sc. / research workBuilding a full plot from measured rate constants and reporting ρ with its fit quality

Check the current official syllabus for whichever paper you are sitting — the depth expected on physical organic topics is revised from time to time.

Fit your own Hammett plot. The Linear Regression tool fits y = mx + c by least squares. Enter σ as x and log(kX/kH) as y, and the slope m it returns is ρ — with the intercept c as your built-in check that the line really does pass through the origin.

Open the Linear Regression (y = mx + c) Calculator →

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