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JEE Mains Chemistry · Chemical Thermodynamics

Entropy, Gibbs Energy and Spontaneity

Whether a change goes on its own: ΔG = ΔH − TΔS, the four sign cases, the entropy change of a reaction or a phase change, and the temperature at which ΔG crosses zero.

Why this matters

Twenty PYQs, twelve of them numerical, and two from 2026. Five read the signs of ΔH and ΔS, five compute an entropy or Gibbs energy change, and ten find the temperature at which ΔG changes sign — the largest single cluster in the chapter.

Concept 1 of 3: Spontaneity from the signs of ΔH and ΔS

ΔG = ΔH − TΔS. The enthalpy term hardly changes with temperature, but the entropy term grows with T. So the sign of ΔS decides which way a rise in temperature pushes ΔG, and the two signs together decide whether a change is always, never or only sometimes spontaneous.

Definition

  • At constant TT and pp: ΔG<0\Delta G < 0 spontaneous; ΔG=0\Delta G = 0 equilibrium (a reversible change); ΔG>0\Delta G > 0 non-spontaneous, and the reverse change is spontaneous.
  • When ΔH\Delta H and ΔS\Delta S share a sign, ΔG\Delta G changes sign at T=ΔHΔST = \frac{\Delta H}{\Delta S}.
  • Second law: ΔSsys+ΔSsurr>0\Delta S_{\mathrm{sys}} + \Delta S_{\mathrm{surr}} > 0 for a spontaneous change, and ΔGsysΔStotal=−T\frac{\Delta G_{\mathrm{sys}}}{\Delta S_{\mathrm{total}}} = -T at constant pressure.
  • Partial derivatives: (∂G∂T)p=−S\left(\frac{\partial G}{\partial T}\right)_p = -S, (∂G∂p)T=V\left(\frac{\partial G}{\partial p}\right)_T = V, (∂H∂T)p=Cp\left(\frac{\partial H}{\partial T}\right)_p = C_p, (∂U∂T)V=CV\left(\frac{\partial U}{\partial T}\right)_V = C_V.
ΔHΔSSign of ΔGSpontaneous
NegativePositiveNegative at every temperatureAt all temperatures
PositiveNegativePositive at every temperatureAt no temperature
PositivePositiveNegative above ΔH/ΔSAt high temperature
An endothermic change that goes at 373 K but not at 273 K belongs in this row.
NegativeNegativeNegative below ΔH/ΔSAt low temperature
The sign of ΔS decides which way a rise in temperature pushes ΔG.
Practice this conceptself-check · 4 quick reps

The same idea in a real exam question:

JEE Mains · 2025 · 24 Jan 2025 · Q33Moderate

Example 1 · Chemical Thermodynamics · Entropy, Gibbs Energy and Spontaneity

Let us consider an endothermic reaction which is non-spontaneous at the freezing point of water. However, the reaction is spontaneous at boiling point of water. Choose the correct option.

Exothermic is not enough

An exothermic change with ΔS<0\Delta S < 0 stops being spontaneous above ΔH/ΔS\Delta H/\Delta S. Only ΔH<0\Delta H < 0 with ΔS>0\Delta S > 0 is spontaneous at every temperature.

Swapping the two derivatives of G

G falls as temperature rises, at the rate S, and rises with pressure, at the rate V: (∂G/∂T)p=−S\left(\partial G/\partial T\right)_p = -S and (∂G/∂p)T=V\left(\partial G/\partial p\right)_T = V. Matching lists swap them.

Concept 2 of 3: Entropy change and Gibbs energy of a reaction

Entropy measures how spread out the energy and the particles are. Making gas raises it; freezing, losing gas molecules or sticking molecules to a surface lowers it. For a reaction, use tabulated entropies just like formation enthalpies — except that no element has zero entropy.

Definition

  • ΔrS∘=∑νS∘(products)−∑νS∘(reactants)\Delta_r S^\circ = \sum\nu S^\circ(\text{products}) - \sum\nu S^\circ(\text{reactants}). Elements have non-zero S∘S^\circ.
  • ΔrG∘=ΔrH∘−TΔrS∘\Delta_r G^\circ = \Delta_r H^\circ - T\Delta_r S^\circ. Put ΔS\Delta S in kJ K⁻¹ (divide by 1000) first.
  • Phase change at its transition temperature: ΔS=ΔHtransTtrans\Delta S = \frac{\Delta H_{\mathrm{trans}}}{T_{\mathrm{trans}}}.
  • Heating with no phase change: ΔS=∫CpT dT=Cpln⁡T2T1\Delta S = \int \frac{C_p}{T}\,dT = C_p\ln\frac{T_2}{T_1} for constant CpC_p. A path through phase changes adds one term per step.
  • Surroundings: ΔSsurr=−qsysT\Delta S_{\mathrm{surr}} = -\frac{q_{\mathrm{sys}}}{T}.
  • ΔS<0\Delta S < 0: freezing (at any temperature), N2+3H2→2NH3\mathrm{N_2 + 3H_2 \to 2NH_3}, adsorption. ΔS>0\Delta S > 0: melting, vaporising, dissolving NaCl.

Entropy and Gibbs energy of reaction

ΔrS∘=∑νSproducts∘−∑νSreactants∘,ΔrG∘=ΔrH∘−TΔrS∘\Delta_r S^\circ = \sum \nu S^\circ_{\mathrm{products}} - \sum \nu S^\circ_{\mathrm{reactants}},\qquad \Delta_r G^\circ = \Delta_r H^\circ - T\Delta_r S^\circ

Worked example

For CaCO3(s)→CaO(s)+CO2(g)\mathrm{CaCO_3(s) \to CaO(s) + CO_2(g)}, ΔrH∘=+178\Delta_r H^\circ = +178 kJ mol⁻¹. S∘S^\circ (J K⁻¹ mol⁻¹): CaCO3\mathrm{CaCO_3} 92.9, CaO 39.8, CO2\mathrm{CO_2} 213.7. Find ΔrS∘\Delta_r S^\circ and ΔrG∘\Delta_r G^\circ at 298 K.
Practice this conceptself-check · 4 quick reps

The same idea in a real exam question:

JEE Mains · 2026 · 5 Apr 2026 Shift 2 · Q29Moderate

Example 2 · Chemical Thermodynamics · Entropy, Gibbs Energy and Spontaneity

Consider the following data for the reaction X2( g)+Y2( g)⇌2XY(g)X_{2}(\text{ }g) +Y_{2}(\text{ }g) \rightleftharpoons 2XY(g) at 600 K. The ΔrG⊖\Delta_{r}G^{\ominus} (in kJ mol−1kJ\,mol^{-1}) for the reaction is:
Compound
ΔfH600 KΘ\Delta_{f}H_{600\text{ }K}^{\Theta}
(kJmol−1)\left( kJmol^{- 1} \right)
S600 KΘS_{600\text{ }K}^{\Theta}
(Jmol−1 K−1)\left( Jmol^{- 1}{\text{ }K}^{- 1} \right)
XY(g)XY(g)
42200
X2( g)X_{2}(\text{ }g)
8140
Y2( g)Y_{2}(\text{ }g)
80250

ΔS in joules, ΔH in kilojoules

This is the most common slip in the chapter. With ΔH=50\Delta H = 50 kJ, ΔS=100\Delta S = 100 J K⁻¹ and T = 400 K, 50−400×10050 - 400 \times 100 is nonsense; 50−400×0.100=1050 - 400 \times 0.100 = 10 kJ is right.

Heating entropy needs the 1/T

The entropy of warming is ∫Cp dT/T\int C_p\,dT/T, not ∫Cp dT\int C_p\,dT (that is the enthalpy). Each phase change on the way adds its own ΔH/T\Delta H/T, at its own temperature.

Concept 3 of 3: Temperature at which ΔG changes sign

When ΔH and ΔS have the same sign, the two terms of ΔG pull against each other, and at one temperature they balance. There ΔG = 0. That temperature is a boiling point, a melting point, a transition point, or the lowest temperature at which a reduction starts to work.

Definition

  • T=ΔHΔST = \frac{\Delta H}{\Delta S}, with ΔH\Delta H in J (or ΔS\Delta S in kJ K⁻¹).
  • ΔH>0\Delta H > 0, ΔS>0\Delta S > 0: spontaneous ABOVE this temperature. ΔH<0\Delta H < 0, ΔS<0\Delta S < 0: spontaneous BELOW it.
  • Boiling and melting points: Tb=ΔvapHΔvapST_b = \frac{\Delta_{\mathrm{vap}}H}{\Delta_{\mathrm{vap}}S}, Tf=ΔfusHΔfusST_f = \frac{\Delta_{\mathrm{fus}}H}{\Delta_{\mathrm{fus}}S}.
  • If ΔG∘\Delta G^\circ is given as a function of T, set it to zero and solve. If ΔS\Delta S itself depends on T, solve ΔH=T ΔS(T)\Delta H = T\,\Delta S(T).
  • From a table: find ΔrH∘\Delta_r H^\circ and ΔrS∘\Delta_r S^\circ first, then divide.

Temperature at which ΔG changes sign

ΔG=0 ⇒ T=ΔHΔS\Delta G = 0\ \Rightarrow\ T = \frac{\Delta H}{\Delta S}

Worked example

For Br2(l)→Br2(g)\mathrm{Br_2(l) \to Br_2(g)}, ΔH=30.9\Delta H = 30.9 kJ mol⁻¹ and ΔS=93.0\Delta S = 93.0 J K⁻¹ mol⁻¹. Find the boiling point of bromine.
Practice this conceptself-check · 4 quick reps

The same idea in a real exam question:

JEE Mains · 2021 · Paper 21 · Q60Moderate

Example 3 · Chemical Thermodynamics · Entropy, Gibbs Energy and Spontaneity

Data given for the following reaction is as follows:
FeO(s)+C(graphite)⟶Fe(s)+CO(g)FeO_{(s)} + C_{\text{(graphite)}} \longrightarrow Fe_{(s)} + CO_{(g)}
SubstanceΔH∘ (kJ mol−1)\Delta H^{\circ}\ \left( kJ\ mol^{- 1} \right)ΔS∘ (J mol−1 K−1)\Delta S^{\circ}\ \left( J\ mol^{- 1}\ K^{- 1} \right)
FeO(s)FeO_{(s)}-266.357.49
C(graphite)C_{\text{(graphite)}}05.74
Fe(s)Fe_{(s)}027.28
CO(g)CO_{(g)}-110.5197.6
The minimum temperature in KK at which the reaction becomes spontaneous is (Integer answer)

A factor of a thousand

With ΔH=60\Delta H = 60 kJ and ΔS=150\Delta S = 150 J K⁻¹, T=60 000/150=400T = 60\,000/150 = 400 K, not 0.4 K. Convert before dividing.

Below, not above

For an exothermic change with falling entropy, ΔH/ΔS\Delta H/\Delta S is the temperature to stay BELOW. Quoting it as a minimum temperature reverses the answer.

Summary — formulas & gotchas at a glance

A revision cheat-sheet for the formulas and gotchas above. Click any concept name to jump back to its full explanation.

Formulas (2)

  • Entropy change and Gibbs energy of a reaction

    Entropy and Gibbs energy of reaction

    ΔrS∘=∑νSproducts∘−∑νSreactants∘,ΔrG∘=ΔrH∘−TΔrS∘\Delta_r S^\circ = \sum \nu S^\circ_{\mathrm{products}} - \sum \nu S^\circ_{\mathrm{reactants}},\qquad \Delta_r G^\circ = \Delta_r H^\circ - T\Delta_r S^\circ
  • Temperature at which ΔG changes sign

    Temperature at which ΔG changes sign

    ΔG=0 ⇒ T=ΔHΔS\Delta G = 0\ \Rightarrow\ T = \frac{\Delta H}{\Delta S}

Reference tables (1)

Spontaneity from the signs of ΔH and ΔS4 rows
ΔHΔSSign of ΔGSpontaneous
NegativePositiveNegative at every temperatureAt all temperatures
PositiveNegativePositive at every temperatureAt no temperature
PositivePositiveNegative above ΔH/ΔSAt high temperature
An endothermic change that goes at 373 K but not at 273 K belongs in this row.
NegativeNegativeNegative below ΔH/ΔSAt low temperature
The sign of ΔS decides which way a rise in temperature pushes ΔG.

Watch out for (6)

Test yourself on Chemical Thermodynamics

20 past JEE Mains questions from this chapter, timed at 48 minutes and marked the way the exam marks it. You see your score and every answer the moment you finish. Free to start.