1. Chapter at a Glance
Chemical thermodynamics deals with energy changes in chemical reactions and tells us whether a reaction can happen on its own (spontaneity). It uses a few big ideas: the system and surroundings, internal energy and enthalpy, the first law, Hess's law, entropy and Gibbs energy. NEET asks one or two questions every year — usually on ΔH–ΔU relation, Hess's law, bond enthalpies, work done in expansion, or the sign of ΔG.
- State vs path functions; intensive vs extensive properties.
- First law ΔU = q + w; work in isothermal expansion.
- ΔH = ΔU + ΔngRT.
- Hess's law, enthalpies of formation, combustion and bond enthalpies.
- Entropy, ΔG = ΔH − TΔS and ΔG° = −RT ln K.
2. Basic Terms
- System: the part of the universe we study; surroundings: everything else.
- Open system exchanges energy and matter; closed exchanges only energy; isolated exchanges neither (an ideal thermos flask).
- State functions depend only on the initial and final states: U, H, S, G, p, V, T. Path functions depend on the route taken: heat q and work w.
- Extensive properties depend on the amount of matter (mass, volume, U, H, heat capacity). Intensive properties do not (T, p, density, molar heat capacity).
- Processes: isothermal (T constant), adiabatic (q = 0), isobaric (p constant), isochoric (V constant), reversible (infinitely slow, always near equilibrium).
3. First Law of Thermodynamics
- Work of expansion against constant external pressure: w = −pextΔV.
- Free expansion (into vacuum, pext = 0): w = 0.
- Isothermal reversible expansion of an ideal gas: w = −2.303 nRT log(V₂/V₁). Since ΔU = 0 at constant T, q = −w.
- At constant volume, ΔU = qV; at constant pressure, ΔH = qp.
4. Enthalpy and Heat Capacity
- Δng = moles of gaseous products − moles of gaseous reactants. If Δng = 0 (e.g. H₂ + Cl₂ → 2HCl), ΔH = ΔU.
- Heat capacity: q = C ΔT; for n moles, q = nCmΔT; for mass m, q = mcΔT.
- ΔU is measured in a bomb calorimeter (constant volume); ΔH in a coffee-cup calorimeter (constant pressure).
- Exothermic reactions have ΔH < 0; endothermic have ΔH > 0.
5. Enthalpies of Reaction and Hess's Law
| Enthalpy change | Definition | NEET Note |
|---|---|---|
| Standard enthalpy of formation (ΔfH°) | 1 mol of compound from its elements in their standard states | Zero for elements in standard states (O₂(g), C(graphite)) |
| Enthalpy of combustion (ΔcH) | Complete burning of 1 mol in oxygen | Always negative |
| Enthalpy of neutralisation | 1 mol of water from acid and base | −57.1 kJ mol⁻¹ for strong acid + strong base |
| Bond dissociation enthalpy | Breaking 1 mol of a bond in the gas phase | Always positive |
| Enthalpy of atomisation | 1 mol of gaseous atoms from the substance | — |
| Lattice enthalpy | 1 mol of ionic solid into gaseous ions | Born–Haber cycle |
| Enthalpy of fusion / vaporisation / sublimation | Phase changes | ΔsubH = ΔfusH + ΔvapH |
- Hess's law: the total enthalpy change is the same whether a reaction takes place in one step or many. So equations can be added and subtracted like algebra, along with their ΔH values.
- ΔrH° = ΣΔfH°(products) − ΣΔfH°(reactants).
- From bond enthalpies (gas phase): ΔrH = Σ(bonds broken) − Σ(bonds formed).
6. Entropy and the Second Law
- Entropy (S) measures disorder or randomness. ΔS = qrev/T.
- Entropy increases: solid → liquid → gas; dissolving a solid; increasing temperature; reactions that increase the number of gas molecules.
- Second law: the total entropy of the universe increases in every spontaneous process: ΔStotal = ΔSsystem + ΔSsurroundings > 0.
- At a phase transition, ΔS = ΔHtransition/T.
- Third law: the entropy of a perfect crystal at 0 K is zero.
7. Gibbs Energy and Spontaneity
| ΔH | ΔS | ΔG | Spontaneity |
|---|---|---|---|
| − | + | Always − | Spontaneous at all temperatures |
| + | − | Always + | Never spontaneous |
| − | − | − at low T | Spontaneous below T = ΔH/ΔS |
| + | + | − at high T | Spontaneous above T = ΔH/ΔS |
- ΔG < 0 spontaneous; ΔG > 0 non-spontaneous; ΔG = 0 at equilibrium.
- ΔG° < 0 ⇒ K > 1 (products favoured).
- Spontaneous does not mean fast: diamond turning into graphite has ΔG < 0 but is extremely slow.
8. Formula Master Table
| Quantity | Formula |
|---|---|
| First law | ΔU = q + w |
| Work (constant pext) | w = −pextΔV |
| Isothermal reversible work | w = −2.303nRT log(V₂/V₁) |
| Enthalpy | ΔH = ΔU + ΔngRT |
| Heat capacities | Cp − CV = R |
| Heat | q = nCmΔT = mcΔT |
| From formation enthalpies | ΔrH° = ΣΔfH°(P) − ΣΔfH°(R) |
| From bond enthalpies | ΔrH = ΣBE(broken) − ΣBE(formed) |
| Entropy change | ΔS = qrev/T |
| Gibbs energy | ΔG = ΔH − TΔS |
| Standard Gibbs energy and K | ΔG° = −2.303RT log K |
| Crossover temperature | T = ΔH/ΔS |
9. Master Summary Table
| Concept | Key idea | NEET Note |
|---|---|---|
| State function | Path-independent | q and w are not state functions |
| First law | Energy conserved | ΔU = 0 for isothermal ideal gas |
| ΔH vs ΔU | Differ by ΔngRT | Equal when Δng = 0 |
| Hess's law | Add equations | Consequence of H being a state function |
| Entropy | Disorder | Gas > liquid > solid |
| Gibbs energy | ΔG < 0 spontaneous | Four sign cases |
| ΔG° and K | −RT ln K | K > 1 when ΔG° < 0 |
10. Mind Map
- System types
- State functions
- Processes
- ΔU = q + w
- Work
- ΔH = ΔU + ΔngRT
- ΔfH, ΔcH
- Hess's law
- Bond enthalpy
- Entropy
- ΔG = ΔH − TΔS
- ΔG° = −RT ln K
11. Tips and Tricks
- Use R = 8.314 J K⁻¹ mol⁻¹ with ΔH in joules; convert kJ carefully (divide by 1000).
- 2.303RT at 298 K ≈ 5.71 kJ mol⁻¹, so ΔG° = −5.71 log K kJ mol⁻¹.
- Only gases count in Δng; ignore liquids and solids.
- To decide the sign of ΔS for a reaction, compare the moles of gas on both sides.
- Using the old sign convention (w positive for work done by the system).
- Including water as a gas in Δng when it is formed as a liquid.
- Saying exothermic reactions are always spontaneous.
- Forgetting that ΔfH° of an element in its standard state is zero.
12. Important One-liners
- Heat and work are path functions; internal energy and enthalpy are state functions.
- In an isolated system, energy remains constant.
- In an adiabatic process, q = 0, so ΔU = w.
- The enthalpy of neutralisation of a strong acid by a strong base is about −57.1 kJ mol⁻¹.
- Graphite, not diamond, is the standard state of carbon.
- A reaction is spontaneous when ΔG is negative.
- The entropy of a perfectly crystalline substance at 0 K is zero.
13. Solved Numericals: Average to Advanced
Five average and five advanced numericals. Take R = 8.314 J K⁻¹ mol⁻¹. Click to reveal each answer and working.
Average level
2 mol of an ideal gas expands isothermally and reversibly at 300 K from 10 L to 20 L. Find the work done and the heat absorbed.
Show answer & solution
Concept: w = −2.303nRT log(V₂/V₁); ΔU = 0 for an isothermal ideal gas.
- w = −2.303 × 2 × 8.314 × 300 × log 2.
- = −2.303 × 4988.4 × 0.301 ≈ −3458 J.
- q = −w = +3458 J (heat absorbed).
Answer: w ≈ −3.46 kJ; q ≈ +3.46 kJ
For N₂(g) + 3H₂(g) → 2NH₃(g), ΔU = −87.4 kJ at 298 K. Find ΔH.
Show answer & solution
Concept: ΔH = ΔU + ΔngRT.
- Δng = 2 − 4 = −2.
- ΔngRT = −2 × 8.314 × 298 = −4955 J ≈ −4.96 kJ.
- ΔH = −87.4 − 4.96 ≈ −92.4 kJ.
Answer: about −92.4 kJ
How much heat is needed to raise the temperature of 36 g of water from 25 °C to 75 °C? (Molar heat capacity of water = 75.3 J K⁻¹ mol⁻¹)
Show answer & solution
Concept: q = nCmΔT.
- n = 36/18 = 2 mol; ΔT = 50 K.
- q = 2 × 75.3 × 50 = 7530 J ≈ 7.53 kJ.
Answer: 7.53 kJ
For a reaction, ΔH = +30 kJ mol⁻¹ and ΔS = +100 J K⁻¹ mol⁻¹. At what temperature is it at equilibrium? Above or below this temperature will it be spontaneous?
Show answer & solution
Concept: at equilibrium ΔG = 0 ⇒ T = ΔH/ΔS.
- T = 30000/100 = 300 K.
- Both ΔH and ΔS are positive, so TΔS wins at higher T: spontaneous above 300 K.
Answer: 300 K; spontaneous above 300 K
A system absorbs 500 J of heat and does 200 J of work on the surroundings. Find the change in its internal energy.
Show answer & solution
Concept: ΔU = q + w with IUPAC signs.
- q = +500 J (absorbed); w = −200 J (done by the system).
- ΔU = 500 − 200 = +300 J.
Answer: +300 J
Advanced level
The enthalpies of combustion of C(graphite), H₂(g) and CH₄(g) are −393.5, −285.8 and −890.3 kJ mol⁻¹. Find the standard enthalpy of formation of methane.
Show answer & solution
Concept: Hess's law: C + 2H₂ → CH₄ = (burn C) + 2(burn H₂) − (burn CH₄).
- ΔfH = ΔcH(C) + 2ΔcH(H₂) − ΔcH(CH₄).
- = −393.5 + 2(−285.8) − (−890.3).
- = −393.5 − 571.6 + 890.3 = −74.8 kJ mol⁻¹.
Answer: −74.8 kJ mol⁻¹
Using bond enthalpies H–H = 436, Cl–Cl = 242 and H–Cl = 431 kJ mol⁻¹, find ΔH for H₂(g) + Cl₂(g) → 2HCl(g). Is ΔU different from ΔH here?
Show answer & solution
Concept: ΔH = Σ bonds broken − Σ bonds formed.
- Broken: 436 + 242 = 678 kJ.
- Formed: 2 × 431 = 862 kJ.
- ΔH = 678 − 862 = −184 kJ. Δng = 2 − 2 = 0, so ΔU = ΔH.
Answer: −184 kJ; ΔU = ΔH
The equilibrium constant of a reaction at 300 K is 10. Find ΔG°. Is the forward reaction favoured under standard conditions?
Show answer & solution
Concept: ΔG° = −2.303RT log K.
- ΔG° = −2.303 × 8.314 × 300 × log 10.
- = −5744 J ≈ −5.74 kJ mol⁻¹.
- ΔG° < 0 and K > 1, so products are favoured.
Answer: about −5.74 kJ mol⁻¹; yes
The enthalpy of vaporisation of water is 40.79 kJ mol⁻¹ at its boiling point, 373 K. Find the entropy change of vaporisation.
Show answer & solution
Concept: at a phase transition, ΔS = ΔH/T.
- ΔS = 40790/373.
- ΔS ≈ 109.4 J K⁻¹ mol⁻¹ (positive: liquid → gas increases disorder).
Answer: about 109.4 J K⁻¹ mol⁻¹
For the synthesis of ammonia, ΔH° = −92.4 kJ mol⁻¹ and ΔS° = −198.3 J K⁻¹ mol⁻¹. Find ΔG° at 298 K, and the temperature above which the reaction stops being spontaneous.
Show answer & solution
Concept: ΔG = ΔH − TΔS (use the same units).
- ΔG° = −92.4 − 298 × (−0.1983) = −92.4 + 59.1 = −33.3 kJ mol⁻¹ (spontaneous).
- Both ΔH and ΔS are negative, so it is spontaneous only at low T.
- T = ΔH/ΔS = 92400/198.3 ≈ 466 K; above this, ΔG becomes positive.
Answer: about −33.3 kJ mol⁻¹; above about 466 K
14. NEET-pattern Questions with Detailed Answers
These questions are original and based on concepts that NEET UG asks again and again.
Which of the following is NOT a state function?
- Internal energy
- Enthalpy
- Work
- Entropy
Show solution
Work depends on the path taken between two states, so it is a path function. Internal energy, enthalpy and entropy depend only on the initial and final states.
Answer: (C)
For which reaction is ΔH equal to ΔU?
- N₂(g) + 3H₂(g) → 2NH₃(g)
- H₂(g) + I₂(g) → 2HI(g)
- PCl₅(g) → PCl₃(g) + Cl₂(g)
- 2SO₂(g) + O₂(g) → 2SO₃(g)
Show solution
ΔH = ΔU when Δng = 0. In reaction (B), Δng = 2 − 2 = 0. For the others, Δng is −2, +1 and −1.
Answer: (B)
A reaction has ΔH < 0 and ΔS < 0. It will be spontaneous:
- At all temperatures
- At low temperatures only
- At high temperatures only
- At no temperature
Show solution
ΔG = ΔH − TΔS. Here −TΔS is positive, and it grows with T. So ΔG is negative only when T is small enough (below ΔH/ΔS).
Answer: (B)
The enthalpy of formation is zero for:
- O₃(g)
- C(diamond)
- Br₂(l)
- H₂O(l)
Show solution
Only elements in their standard states have ΔfH° = 0. Liquid bromine is the standard state of bromine. O₃ is not the standard form of oxygen, diamond is not the standard form of carbon, and water is a compound.
Answer: (C)
In an adiabatic process:
- ΔU = 0
- q = 0
- w = 0
- ΔT = 0
Show solution
An adiabatic process allows no heat exchange, so q = 0 and ΔU = w. ΔU = 0 and ΔT = 0 describe an isothermal process for an ideal gas.
Answer: (B)
Entropy increases in which change?
- Freezing of water
- Condensation of steam
- Sublimation of iodine
- 2NO₂(g) → N₂O₄(g)
Show solution
Sublimation turns a solid into a gas, which increases disorder a great deal. Freezing and condensation make the system more ordered. In (D), the moles of gas fall from 2 to 1, so entropy decreases.
Answer: (C)
If ΔG° for a reaction at 298 K is −11.4 kJ mol⁻¹, its equilibrium constant is about (2.303RT = 5.7 kJ mol⁻¹):
- 10
- 100
- 0.01
- 2
Show solution
log K = −ΔG°/(2.303RT) = 11.4/5.7 = 2, so K = 100. (C) comes from a sign error, and (D) confuses log K with K.
Answer: (B)
An ideal gas expands freely into a vacuum under adiabatic conditions. Which set is correct?
- q = 0, w = 0, ΔU = 0
- q = 0, w < 0, ΔU < 0
- q > 0, w = 0, ΔU > 0
- q = 0, w > 0, ΔU > 0
Show solution
The process is adiabatic, so q = 0. Against zero external pressure w = 0, so ΔU = 0 and the temperature of an ideal gas stays the same. (B) would be true for an adiabatic expansion against a pressure.
Answer: (A)
15. Quick Revision Summary
- ΔU = q + w; w = −pextΔV; isothermal reversible w = −2.303nRT log(V₂/V₁).
- ΔH = ΔU + ΔngRT; Cp − CV = R.
- Hess's law; ΔrH = ΣΔfH(P) − ΣΔfH(R); bonds broken − bonds formed.
- ΔS = qrev/T; ΔStotal > 0 for spontaneous change.
- ΔG = ΔH − TΔS; ΔG° = −2.303RT log K; four sign cases.