Spontaneity, Entropy & Second Law of Thermodynamics
The First Law of Thermodynamics tells us that energy is conserved in every physical and chemical change, but it provides no clue regarding the direction of natural processes. Why does heat flow spontaneously only from a hot body to a cold body? Why does a gas expand to fill an evacuated flask but never re-compress on its own? The answers lie in the thermodynamic concepts of Spontaneity and Entropy.
1. The Concept of Spontaneity & Driving Forces
A Spontaneous Process (or feasible process) is an irreversible process that occurs on its own under a specified set of conditions, without requiring continuous external work. Once initiated, or proceeding by itself, it moves towards a state of dynamic equilibrium.
- Examples of spontaneous processes: Water flowing down a hill, gas diffusing into vacuum, dissolving sugar in hot water, rusting of iron in moist air.
- Driving forces behind spontaneity:
- Tendency towards minimum energy: Many exothermic reactions (ΔH < 0) are spontaneous because lower potential energy states are more stable.
- Tendency towards maximum disorder/randomness: Even endothermic processes (ΔH > 0, such as melting of ice at 25 °C or evaporation of alcohol) occur spontaneously because the system gains molecular randomness.
2. Entropy (S): Definition & Physical Meaning
Entropy (S) is a thermodynamic state function that serves as a quantitative measure of molecular disorder, randomness, or the number of microstates (Ω) accessible to a macroscopic system: S = kB ln(Ω).
For an infinitesimal reversible transfer of heat dqrev at absolute temperature T:
dS = dqrev / T ⇒ ΔS = ∫ (dqrev / T)
Units of Entropy: J K−1 mol−1 (Joules per Kelvin per mole).
| Physical State / Transformation | Relative Entropy | Reasoning |
|---|---|---|
| Solid Phase | Lowest entropy (Ssolid) | Particles are locked in rigid crystal lattices with only vibrational motion. |
| Liquid Phase | Intermediate entropy (Sliquid) | Molecules possess translational and rotational freedom of movement. |
| Gaseous Phase | Highest entropy (Sgas) | Molecules move completely independently in vast empty space. |
Entropy Transformation Across Phase Transitions
Entropy (S)
^ / Vapor State
| / (High Entropy)
| +--------*
| | Δ_vap S = Δ_vap H / T_b
| Liquid State|
| +-------------*
| | Δ_fus S = Δ_fus H / T_m
| Solid State |
| /
| /
+-------------+---------------+-------------+----------> Temperature (T)
0 K T_melting T_boiling
3. Mathematical Formulae for Entropy Changes (ΔS)
A. Phase Transitions at Equilibrium (Constant T and P)
- Entropy of Fusion: ΔfusS = ΔfusH / Tf
- Entropy of Vaporization: ΔvapS = ΔvapH / Tb
- Entropy of Sublimation: ΔsubS = ΔsubH / Tsub = ΔfusS + ΔvapS
B. Entropy Change for an Ideal Gas (n moles)
From First Law (dqrev = dU + PdV = nCvdT + (nRT/V)dV):
ΔS = n Cv ln(T2 / T1) + n R ln(V2 / V1)
In terms of pressure:
ΔS = n Cp ln(T2 / T1) − n R ln(P2 / P1)
- Isothermal Process (T1 = T2): ΔS = 2.303 n R log10(V2 / V1) = 2.303 n R log10(P1 / P2)
- Isochoric Process (V1 = V2): ΔS = 2.303 n Cv log10(T2 / T1)
- Isobaric Process (P1 = P2): ΔS = 2.303 n Cp log10(T2 / T1)
- Reversible Adiabatic Process (qrev = 0): ΔS = 0 (Isentropic Process)
4. The Second Law of Thermodynamics
The Second Law of Thermodynamics establishes the universal criterion for spontaneous change:
ΔStotal = ΔSsystem + ΔSsurroundings > 0 (Spontaneous / Irreversible process)
ΔStotal = ΔSsystem + ΔSsurroundings = 0 (Reversible process at dynamic equilibrium)
ΔStotal < 0 (Non-spontaneous / Impossible process)
Entropy Change of the Surroundings
Because the surroundings act as an infinitely large thermal reservoir at constant temperature T:
ΔSsurr = qsurr / T = −qsys / T = −ΔHsys / T
Therefore:
ΔStotal = ΔSsys − (ΔHsys / T)
Multiplying both sides by −T gives: −TΔStotal = ΔHsys − TΔSsys, which directly leads to Gibbs Free Energy (ΔG)!
5. Solved High-Yield Numerical Examples & Exam MCQs
1. Identify the given values:
ΔvapH = 40.66 kJ mol−1 = 40,660 J mol−1
Tb = 373 K
2. Apply the entropy of vaporization formula at equilibrium:
ΔvapS = ΔvapH / Tb
ΔvapS = 40,660 J mol−1 / 373 K = +109.0 J K−1 mol−1.
Notice that ΔvapS is positive, reflecting the tremendous increase in randomness when molecules leave the liquid phase and expand into vapour.
Show answer
In reaction (B), a solid reactant decomposes to produce 1 mole of gas: Δng = 1 − 0 = +1. Gaseous molecules have vastly greater entropy than solids; hence ΔS° > 0. In (A) and (C), Δng is negative, causing an entropy decrease. In (D), condensation of gas to liquid also decreases entropy (ΔS < 0).
Show answer
For an isothermal process of an ideal gas:
ΔS = 2.303 n R log10(V2 / V1)
ΔS = 2.303 × 1 × 8.314 × log10(100 / 10) = 2.303 × 8.314 × 1 = +19.15 J K−1.
6. Frequently Asked Questions (FAQs)
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