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Summary of Thermodynamics Principles

Apr 27, 2025

Thermodynamics Lecture Summary

Key Topics Covered

  • Solving thermodynamic problems
  • Processes: isothermal, isochoric, adiabatic, isobaric
  • Important equations for work, heat, and internal energy

Important Equations

General Equations

  • First Law of Thermodynamics: \Delta U = Q - W
    • (Q): Heat added to the system
    • (W): Work done by the system
    • (\Delta U): Change in internal energy

Process-Specific Equations

Isocoric (Constant Volume)

  • (\Delta V = 0) (Work (W = 0))
  • (\Delta U = Q = nC_V\Delta T)
  • (Q = V \cdot C_V \cdot \Delta P / R)

Isobaric (Constant Pressure)

  • (\Delta P = 0)
  • (W = P \cdot \Delta V) or (W = nR \Delta T)
  • (Q = nC_P \Delta T) or (Q = P \cdot C_P \cdot \Delta V / R)
  • Use Charles's Law: (V_1/T_1 = V_2/T_2)

Isothermal (Constant Temperature)

  • (\Delta T = 0)
  • (\Delta U = 0), thus (Q = W)
  • (W = nRT \ln(V_{\text{final}}/V_{\text{initial}}))
  • (P_1V_1 = P_2V_2) (Boyle's Law)

Adiabatic (No Heat Exchange)

  • (Q = 0)
  • (\Delta U = -W)
  • (\Delta U = nC_V\Delta T)
  • (P_1V_1^\gamma = P_2V_2^\gamma)
  • (T_1V_1^{\gamma-1} = T_2V_2^{\gamma-1})

Concepts

Thermodynamic Terms

  • Work (W): Positive if done by the system; negative if done on the system.
  • Heat (Q): Positive if absorbed; negative if released.
  • Internal Energy (U): Related to temperature; changes with (\Delta U).

System Types

  • Open System: Matter and energy can enter/leave.
  • Closed System: Only energy can enter/leave.
  • Isolated System: No matter or energy exchange.

Specific Heat Capacities

  • Monoatomic Gases:
    • (C_V = \frac{3}{2}R)
    • (C_P = \frac{5}{2}R)
  • Diatomic Gases:
    • (C_V = \frac{5}{2}R)
    • (C_P = \frac{7}{2}R)
  • Polyatomic Gases: (Approximate for three atoms)
    • (C_V \approx \frac{7}{2}R)
    • (C_P \approx \frac{9}{2}R)

Cyclic Processes

  • Net heat flow (Q = W) for cyclic processes
  • Work done is equal to the area enclosed in a PV diagram.

Practice Problems

  • Calculate internal energy change given heat and work.
  • Isothermal and adiabatic processes: Derive final temperature and pressure.
  • Application of thermodynamic laws in real-world scenarios like car engines.

Efficiency and Performance

  • Efficiency of Engines: Calculated as (\eta = \frac{W}{Q_H} \times 100%)
  • Heat Transfer: Understanding how heat is absorbed or released by systems during various processes.

This summary provides a comprehensive overview of thermodynamic processes and calculations essential for understanding heat, work, and energy changes in various systems.