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โ™จ๏ธThermodynamics of Fluids Unit 5 Review

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5.2 Carnot cycle and thermodynamic temperature scale

โ™จ๏ธThermodynamics of Fluids
Unit 5 Review

5.2 Carnot cycle and thermodynamic temperature scale

Written by the Fiveable Content Team โ€ข Last updated September 2025
Written by the Fiveable Content Team โ€ข Last updated September 2025
โ™จ๏ธThermodynamics of Fluids
Unit & Topic Study Guides

The Carnot cycle is a key concept in thermodynamics, showing how heat engines work at their best. It's all about turning heat into work efficiently, using a series of steps that move heat between hot and cold places.

The thermodynamic temperature scale builds on the Carnot cycle idea. It gives us a way to measure temperature that doesn't depend on any specific material, starting from absolute zero where there's no heat at all.

Carnot Cycle and Efficiency

Carnot Cycle Concepts

  • Carnot cycle represents the most efficient heat engine cycle operating between two thermal energy reservoirs at constant temperatures
  • Consists of four reversible processes: isothermal expansion, adiabatic expansion, isothermal compression, and adiabatic compression
  • Carnot cycle is an ideal thermodynamic cycle that provides an upper limit on the efficiency of any classical thermodynamic engine
  • Operates in a closed system, meaning the working fluid is returned to its initial state at the end of each cycle (piston-cylinder device)

Carnot Engine Characteristics

  • Carnot engine is a theoretical heat engine that operates on the Carnot cycle
  • Consists of a heat source at a high temperature (TH), a heat sink at a low temperature (TL), and a working fluid (ideal gas)
  • Work is done by the working fluid during the isothermal expansion process, while work is done on the working fluid during the isothermal compression process
  • Carnot engines are the most efficient heat engines that operate between two specific temperatures

Ideal Gas Carnot Cycle Processes

  • Isothermal expansion: gas expands at constant temperature TH while in contact with the hot reservoir, absorbing heat and doing work (pV = nRT)
  • Adiabatic expansion: gas continues to expand without exchanging heat with the surroundings, causing its temperature to decrease from TH to TL
  • Isothermal compression: gas is compressed at constant temperature TL while in contact with the cold reservoir, releasing heat and having work done on it
  • Adiabatic compression: gas is further compressed without exchanging heat, causing its temperature to increase from TL back to TH

Carnot Efficiency Calculation

  • Carnot efficiency ($\eta_{Carnot}$) represents the maximum efficiency attainable by a heat engine operating between two temperatures
  • Defined as the ratio of the net work output (W) to the heat input from the hot reservoir (QH): $\eta_{Carnot} = \frac{W}{Q_H} = 1 - \frac{Q_L}{Q_H}$
  • For an ideal gas Carnot cycle, the efficiency can be expressed in terms of the reservoir temperatures: $\eta_{Carnot} = 1 - \frac{T_L}{T_H}$
  • Carnot efficiency increases as the temperature difference between the hot and cold reservoirs increases (steam power plants, internal combustion engines)

Thermodynamic Temperature Scale

Absolute Temperature and Absolute Zero

  • Thermodynamic temperature scale is based on the concept of absolute zero, the lowest possible temperature
  • Absolute zero is the temperature at which a system has no thermal energy and cannot transfer heat to any other system
  • Kelvin (K) is the SI unit of thermodynamic temperature, with 0 K representing absolute zero (โˆ’273.15ยฐC or โˆ’459.67ยฐF)
  • Temperatures on the Kelvin scale are always positive, as they represent the absolute magnitude of thermal energy

Relation to Reversible Heat Engines

  • The thermodynamic temperature scale is defined by the efficiency of reversible heat engines, such as the Carnot engine
  • For reversible heat engines, the ratio of heat transferred ($\frac{Q_H}{Q_L}$) is equal to the ratio of the absolute temperatures of the reservoirs ($\frac{T_H}{T_L}$)
  • This relationship allows for the establishment of an absolute temperature scale that is independent of the properties of any particular substance (ideal gas law)

Practical Implications and Applications

  • Thermodynamic temperature is essential for understanding and analyzing heat engine efficiency and performance
  • Absolute zero is a fundamental limit in thermodynamics and cannot be reached in practice, as it would require an infinite number of steps in a Carnot cycle (third law of thermodynamics)
  • Cryogenics and ultra-low temperature research aim to achieve temperatures as close to absolute zero as possible (superconductivity, quantum computing)
  • The thermodynamic temperature scale is used in various fields, including physics, chemistry, and engineering, to describe the thermal behavior of systems (heat transfer, chemical reactions, materials science)