Carnot Cycle: Difference between revisions

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<math> pV = nRT</math>
<math> pV = nRT</math>
# Isothermal compression: T is constant, thus we have <math>p = </math>cons /T.


== Air ==
== Air ==


Adiabatic index <math>\gamma = c_p/c_v</math> is for the air 7/5.
Adiabatic index <math>\gamma = c_p/c_v</math> is for the air 7/5.

Revision as of 16:56, 15 August 2024

Introduction

  1. Isothermal expansion: Heat is transferred from the hot reservoir to the gas.
  2. Isentropic (reversible adiabatic) expansion
  3. Isothermal compression
  4. Isentropic compression

Ideal Gas

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle pV = nRT}

  1. Isothermal compression: T is constant, thus we have Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle p = } cons /T.

Air

Adiabatic index Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \gamma = c_p/c_v} is for the air 7/5.