Second law of Thermodynamics free study material

Equivalence of Statements

  • Violation of one statement implies violation of the other.
  • Hence, both statements are equivalent forms of the second law.

Heat Engine

  • Absorbs heat Q1Q_1Q1โ€‹ from a high-temperature source
  • Produces work WWW
  • Rejects heat Q2Q_2Q2โ€‹ to a low-temperature sink

Efficiency:ฮท=WQ1\eta = \frac{W}{Q_1}

Refrigerator

  • Removes heat from a low-temperature region
  • Requires work input

Coefficient of Performance (COP):COPR=Q2WCOP_R = \frac{Q_2}{W}

Heat Pump

  • Supplies heat to a high-temperature region

COPHP=Q1WCOP_{HP} = \frac{Q_1}{W}

The Carnot cycle is an ideal reversible cycle consisting of:

  1. Isothermal Expansion
  2. Adiabatic Expansion
  3. Isothermal Compression
  4. Adiabatic Compression

Carnot Efficiency:

ฮทCarnot=1โˆ’T2T1\eta_{Carnot} = 1 – \frac{T_2}{T_1}

Where:

  • T1T_1T1โ€‹ = Temperature of source (K)
  • T2T_2T2โ€‹ = Temperature of sink (K)

Key Points:

  • It is the maximum possible efficiency.
  • Depends only on temperature limits.

Definition

Entropy is a measure of disorder or randomness in a system.

For a reversible process:dS=ฮดQTdS = \frac{\delta Q}{T}

Important Principles

  1. Entropy increases for irreversible processes.
  2. For isolated systems: ฮ”Sโ‰ฅ0\Delta S \geq 0
  3. Reversible process: ฮ”S=0\Delta S = 0ฮ”S=0
  4. Irreversible process: ฮ”S>0\Delta S > 0ฮ”S>0

Real processes are irreversible due to:

  • Friction
  • Heat loss
  • Unrestrained expansion
  • Mixing of fluids

Hence, real efficiency is always less than Carnot efficiency.

  • Thermal power plants
  • Refrigeration & air conditioning
  • Internal combustion engines
  • Turbines and compressors

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