આ MCQ મોડ્યુલ આના પર આધારિત છે: Spontaneity Second Law
Spontaneity Second Law
આ મૂલ્યાંકન આના પર આધારિત હશે: Spontaneity Second Law
મૂલ્યાંકન બનાવવામાં તેમની સામગ્રી સામેલ કરવા ચિત્રો, PDF અથવા Word દસ્તાવેજ અપલોડ કરો.
Spontaneity, Entropy and Gibbs Free Energy
5.15 Spontaneity — What Drives a Process?
A spontaneous process is one that has a natural tendency to occur without any external aid. Examples: water flowing downhill, iron rusting, ice melting at 25 °C, two gases mixing.
Some spontaneous processes are exothermic (combustion of methane, ΔH = −890 kJ/mol) and some are endothermic (NH₄Cl dissolving in water, ΔH = +14 kJ/mol). So enthalpy alone cannot predict spontaneity. We need another driving force.
5.16 Entropy (S)
The missing ingredient is entropy (S) — a measure of the disorder or randomness of a system. The higher the disorder, the higher the entropy.
5.16.1 Predicting the Sign of ΔS
| Process | ΔS | Reason |
|---|---|---|
| Solid → Liquid (melting) | + | More positions available |
| Liquid → Gas (vaporisation) | ++ (very large) | Huge increase in volume/disorder |
| Gas → Liquid (condensation) | − | Order increases |
| Reaction increases moles of gas | + | e.g., 2KClO₃ → 2KCl + 3O₂ |
| Reaction decreases moles of gas | − | e.g., N₂ + 3H₂ → 2NH₃ |
| Mixing of two gases | + | More ways to arrange |
| Increase in temperature | + | More kinetic states accessible |
5.17 The Second Law of Thermodynamics
Even an exothermic reaction with ΔS_system < 0 can be spontaneous if the surroundings gain enough entropy: ΔS_surr = −ΔH/T > 0, and the total can be positive.
5.17.1 Third Law of Thermodynamics
5.18 Gibbs Free Energy (G)
For chemists working at constant T and P (typical lab/industrial conditions), it is inconvenient to compute ΔS_universe (need data on the surroundings). The American physicist J. W. Gibbs defined a new state function:
Why is this useful? Multiplying ΔS_universe by −T gives: \[-T\Delta S_\text{universe} = \Delta H_\text{system} - T\Delta S_\text{system} = \Delta G_\text{system}\] So ΔG measures the increase of disorder of the universe, but using only system properties!
5.18.1 Criteria for Spontaneity
| ΔG | Process |
|---|---|
| < 0 (negative) | Spontaneous in forward direction |
| = 0 | Equilibrium |
| > 0 (positive) | Non-spontaneous forward (reverse is spontaneous) |
5.18.2 Sign Combinations of ΔH and ΔS
| ΔH | ΔS | ΔG = ΔH − TΔS | Spontaneity |
|---|---|---|---|
| − (exo) | + (disorder ↑) | Always − | Spontaneous at all T (e.g., 2H₂O₂ → 2H₂O + O₂) |
| + (endo) | − (disorder ↓) | Always + | Never spontaneous (e.g., 3O₂ → 2O₃) |
| − (exo) | − (disorder ↓) | − at low T | Spontaneous only at LOW T (e.g., water freezing) |
| + (endo) | + (disorder ↑) | − at high T | Spontaneous only at HIGH T (e.g., NH₄Cl dissolving, decomposition reactions) |
5.19 Standard Free Energy & Equilibrium Constant
The standard Gibbs free energy change Δ_rG° is related to the equilibrium constant K by:
\[\Delta_r G^\circ = -RT \ln K = -2.303\,RT\,\log K\]| Δ_rG° | K | Direction at standard state |
|---|---|---|
| < 0 | K > 1 | Products favoured |
| = 0 | K = 1 | Equal amounts |
| > 0 | K < 1 | Reactants favoured |
🎯 Interactive: ΔG Spontaneity Predictor
Set ΔH and ΔS for a reaction. Slide T to see when the reaction becomes spontaneous (ΔG < 0).
ΔG = ΔH − TΔS = −10.20 kJ
SPONTANEOUS (forward) ✓
Switch-over T (T_eq = ΔH/ΔS) = 400 K
Setup: For ice → liquid water at 1 atm: ΔH_fus = +6.01 kJ/mol, ΔS_fus = +22.0 J K⁻¹ mol⁻¹.
(a) T = 263 K: ΔG = 6010 − 263×22 = 6010 − 5786 = +224 J. Non-spontaneous — ice stays frozen.
(b) T = 273 K: ΔG = 6010 − 273×22 = 6010 − 6006 ≈ 0. Equilibrium — ice and water coexist (this is the melting point!).
(c) T = 283 K: ΔG = 6010 − 283×22 = 6010 − 6226 = −216 J. Spontaneous — ice melts.
Key insight: The melting point is precisely the temperature where ΔG = 0, i.e., T_m = ΔH/ΔS. Below it, freezing wins; above it, melting wins. ΔG = 0 is the natural definition of phase equilibrium.
Worked Example 5.7: Spontaneity at 298 K
For the reaction N₂(g) + 3H₂(g) → 2NH₃(g), ΔH° = −92.4 kJ and ΔS° = −198.3 J K⁻¹. Is the reaction spontaneous at 298 K? Above what temperature does it become non-spontaneous?
Switch-over temperature (ΔG° = 0): T = ΔH°/ΔS° = (−92400)/(−198.3) = 466 K (≈ 193 °C).
Above 466 K, ΔG° becomes positive — reaction becomes non-spontaneous. This is why industrial NH₃ synthesis uses high pressure to compensate for moderate temperatures (~700 K).
Worked Example 5.8: K from ΔG°
For a reaction at 298 K, Δ_rG° = −13.6 kJ/mol. Calculate the equilibrium constant K. (R = 8.314 J K⁻¹ mol⁻¹)
−13600 = −2.303 × 8.314 × 298 × log K
−13600 = −5705 × log K
log K = 2.383 → K = 10²·³⁸³ ≈ 242
A modest negative ΔG° (~13 kJ) gives K ~ 240, which is product-favoured but not overwhelmingly so.
🎯 Competency-Based Questions
Q1. The criterion of spontaneity at constant T and P is: L1 Remember
Q2. Predict the sign of ΔS for: I₂(s) → I₂(g). L2 Understand
Q3. NH₄Cl dissolves in water with ΔH = +14 kJ/mol but the process is spontaneous at room temperature. Explain. L4 Analyse
Q4. The standard ΔG° for a reaction at 300 K is +5.706 kJ. Calculate K. L3 Apply
Q5. HOT (Evaluate): Life involves building highly ordered structures (proteins, DNA) — apparently violating the second law! How is this reconciled? L5 Evaluate
🧠 Assertion–Reason Questions
Choose: (A) Both true, R explains A. (B) Both true, R doesn't explain A. (C) A true, R false. (D) A false, R true.
A: Spontaneous processes have negative ΔG.
R: Spontaneous processes always release heat.
A: The entropy of a perfectly crystalline solid is zero at 0 K.
R: At 0 K, only one microstate is accessible (all atoms locked in place).
A: A reaction with ΔH > 0 and ΔS > 0 becomes spontaneous at high temperature.
R: The TΔS term grows in magnitude with T, eventually overcoming ΔH.
Frequently Asked Questions — Spontaneity, Entropy and Gibbs Free Energy
What is a spontaneous process?
What is entropy and how does it change?
What is the second law of thermodynamics?
What is Gibbs free energy?
How are ΔH, ΔS and ΔG related to spontaneity?
What is the third law of thermodynamics?
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