| Item | Key Features | Notes / Differences |
|---|---|---|
| Ideal Gas | pV = nRT; no interactions | Simplified model, accurate at low P, T |
| Van der Waals Gas | (p + a(n/V)^2)(V - nb) = nRT | Accounts for molecular interactions |
| Reversible Process | No entropy production; idealized | Maximum work obtainable |
| Irreversible Process | Entropy increases; real processes | Less work, more entropy production |
| Isothermal | Constant T; work = -nRT ln(Vf/Vi) | ΔU = 0 |
| Adiabatic | No heat transfer; pV^γ = constant | T ∝ V^(γ-1) |
| Isobaric | Constant pressure; work = -p(Vf - Vi) | ΔH = Qp |
| Isochoric | Constant volume; no work, heat changes U or H | ΔU = Qv |
Thermodynamic System
├─ System Types
│ ├─ Closed
│ ├─ Open
│ └─ Isolated
├─ Equilibrium Conditions
│ ├─ Mechanical (p uniform)
│ └─ Thermal (T uniform)
├─ State Variables
│ ├─ Extensive: U, V
│ └─ Intensive: p, T
├─ Processes & Transformations
│ ├─ Quasi-static
│ ├─ Reversible
│ ├─ Adiabatic
│ ├─ Isothermal
│ └─ Isobaric / Isochoric
└─ Phase Diagram & Transitions
End of Revision Sheet
Take a 10-question practice quiz on Thermodynamics of Equilibrium Systems, with every answer explained.
1. What is the primary difference between a closed and an open thermodynamic system?
2. Which of the following conditions are necessary for a system to be in thermodynamic equilibrium?
Memorize the key concepts of Thermodynamics of Equilibrium Systems with 10 flashcards.
Systems — types?
Open, closed, and isolated.
Equilibrium — conditions?
Uniform pressure and temperature.
Variables — types?
Extensive: U, V; Intensive: p, T.
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