Chemical & Statistical Thermodynamics Handwritten Notes PDF
Master the most scoring mathematical unit of physical chemistry. High-yield handwritten classroom notes covering Maxwell relations, partition functions, residual entropy, and solved CSIR NET & GATE questions.
- 1. File Specifications & Syllabus Coverage
- 2. Classical Thermodynamics: Maxwell Relations & Equations of State
- 3. Thermodynamic Square Mnemonic (Maxborn Relations)
- 4. Statistical Thermodynamics: Partition Functions & Ensembles
- 5. Hierarchy of Energy Level Spacings & Partition Functions
- 6. Solved Benchmark CSIR NET Part-C Questions
- 7. Classroom Notes Sample Page Preview
- 8. Frequently Asked Questions (FAQs)
- 9. Direct High-Speed Download Mirror
📚 1. File Specifications & Exam Weightage
Thermodynamics (Classical + Statistical) represents 25 to 35 marks in CSIR NET Chemical Science and 8 to 12 marks in GATE (CY). Because the questions are direct application of fundamental formulas, this unit yields nearly 100% accuracy with systematic revision.
| Module Name | Chemical and Statistical Thermodynamics (Career Notes) |
|---|---|
| Target Exams | CSIR UGC NET (JRF/LS), GATE Chemistry (CY), BARC, TIFR, SET, M.Sc./B.Sc. |
| File Size & Format | 7.4 MB • High-Resolution PDF (High-contrast, clean printer scan) |
| Authors / Source | Curated by Top Rankers of CSIR NET & GATE Chemical Sciences |
| Access Cost | 100% Free Direct Download via Google Drive |
⚖️ 2. Classical Thermodynamics: Fundamental Equations
Enthalpy: dH = T dS + V dP
Helmholtz Energy: dA = −S dT − P dV
Gibbs Free Energy: dG = −S dT + V dP
| Origin Potential | Maxwell Relation | Physical Significance |
|---|---|---|
| Internal Energy (U) | (∂T/∂V)S = −(∂P/∂S)V | Adiabatic reversible volume changes |
| Enthalpy (H) | (∂T/∂P)S = (∂V/∂S)P | Adiabatic reversible pressure changes |
| Helmholtz Energy (A) | (∂S/∂V)T = (∂P/∂T)V | Determines internal pressure (πT) |
| Gibbs Energy (G) | (∂S/∂P)T = −(∂V/∂T)P | Relates entropy change to thermal expansivity (α) |
• For an Ideal Gas: πT = 0
• For a van der Waals Gas: πT = a / Vm2
🧩 3. Maxborn Thermodynamic Square Derivations
Use the mnemonic “Vampires And Trolls Go Prowling Here” to easily write down any Maxwell relation or differential equation:
| Corner Variables | Edge Potentials | Sign Rule | Shortcut Derivation |
|---|---|---|---|
| V (Volume) & T (Temperature) | A (Helmholtz Energy) | Both incoming arrows are negative | dA = −P dV − S dT |
| T (Temperature) & P (Pressure) | G (Gibbs Energy) | T is negative, P is positive | dG = −S dT + V dP |
| P (Pressure) & S (Entropy) | H (Enthalpy) | Both incoming arrows are positive | dH = V dP + T dS |
| S (Entropy) & V (Volume) | U (Internal Energy) | S is positive, V is negative | dU = T dS − P dV |
🔬 4. Statistical Thermodynamics: Partition Functions
The molecular partition function (q) connects microscopic quantum states to macroscopic thermodynamic properties (U, H, S, G):
Canonical Ensemble (Indistinguishable): Q = qN / N! (Distinguishable: Q = qN)
| Mode | Partition Function Formula | Temperature Dependence | Symmetry Factor (σ) |
|---|---|---|---|
| Translational (3D) | qtrans = (2πm kBT / h2)3/2 × V | qtrans ∝ T3/2 · M3/2 | — |
| Rotational (Linear) | qrot = kBT / (σ h c B) = 8π2I kBT / (σ h2) | qrot ∝ T | Homonuclear (σ=2), Heteronuclear (σ=1) |
| Rotational (Non-Linear) | qrot = (π1/2 / σ) × (kBT / hc)3/2 × (1 / √(IAIBIC)) | qrot ∝ T3/2 | H2O (σ=2), NH3 (σ=3), CH4 (σ=12) |
| Vibrational | qvib = 1 / [1 − e−hν/kBT] ≈ kBT / hν (High T) | qvib ∝ T0 (Low T) → T1 (High T) | — |
Entropy: S = kB ln Q + U / T
Helmholtz Energy: A = −kBT ln Q
Residual Entropy: Sres = kB ln W
📊 5. Hierarchy of Energy Level Spacings & Partition Functions
At standard room temperature (300 K), the energy gap (Δε) relative to thermal energy (kBT) dictates the number of populated quantum states:
💡 6. Solved Benchmark CSIR NET Exam Problems
Problem 1: Calculate the molar residual entropy of crystalline Carbon Monoxide (CO) at absolute zero (0 K).
Step-by-Step Solution:
- In crystalline solid CO, each molecule has two nearly degenerate orientations in the crystal lattice (C≡O vs. O≡C) due to a very small dipole moment (0.1 Debye).
- Total number of microstates for 1 mole (NA molecules): W = 2NA.
- Applying Boltzmann’s entropy formula:
Sres = kB ln W = kB ln(2NA) = NA kB ln 2 = R ln 2. - Numerically: Sres = 8.314 × 0.693 = 5.76 J K−1 mol−1.
Problem 2: What is the ratio of the rotational partition functions of HD and D2 at the same temperature T? (Assume bond lengths are identical: rHD = rD2).
Step-by-Step Solution:
- Rotational partition function: qrot = 8π2I kBT / (σh2) ∝ μ / σ (since I = μr2).
- Reduced masses:
μHD = (1 × 2) / (1 + 2) = 2/3 amu
μD2 = (2 × 2) / (2 + 2) = 1.0 amu - Symmetry numbers (σ):
HD is heteronuclear → σHD = 1
D2 is homonuclear → σD2 = 2 - Taking the ratio:
qrot(HD) / qrot(D2) = (μHD / σHD) / (μD2 / σD2) = (2/3 / 1) / (1 / 2) = (2/3) × 2 = 4/3 = 1.33.
🖼️ 7. Classroom Notes Sample Page Preview
Below is a sample preview from the high-resolution scanned PDF notes:

❓ 8. Frequently Asked Questions (FAQs)
Yes. These classroom notes cover both classical thermodynamics (laws, Maxwell relations, chemical potential, non-ideal solutions) and statistical mechanics (ensembles, partition functions, residual entropy). Paired with previous year questions, it provides complete preparation.
In homonuclear diatomics like N2 or O2, a 180° rotation around the perpendicular axis leaves the molecule in an indistinguishable orientation. To avoid double-counting quantum microstates in phase space, the rotational partition function is divided by σ = 2.
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