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**Adiabatic** refers to a process in which no heat is transferred into or out of a system, and the change in internal energy is only done by work. Often this is accomplished in an insulated container, where the process happens too quickly for heat to be transferred. Since heat moves because of a difference in temperature between a system and its surroundings, an adiabatic process can also happen when the system is in thermal equilibrium.^{[1]} By the first law of thermodynamics, this then looks like

where:

- [math]\Delta U[/math] is the change in the system's internal energy and
- [math]W[/math] is the work done
*on*the system (if the system*does*work to its surroundings, the work is negative and the systems internal energy thereby decreases).

For an adiabatic *compression* (decreasing the volume of the system, like a piston), the temperature must increase. Likewise, for an *expansion* (increasing volume), the temperature must decrease. This is because there is no heat able to flow in or out in order to balance the temperature, which is what occurs in an isothermal process.

Isotherms and adiabats may look similar at first glance, but in Figure 1, it's clear that adiabats exhibit much steeper curves. Therefore, the ideal gas law slightly differs too, as seen in the equation below:

^{[2]}

where:

- [math]p[/math] is pressure

- [math]V[/math] is volume

- [math]γ[/math] is gamma, which represents the specific heat ratio defined as:

- 1.67 for a
*monatomic*gas

- 1.67 for a

- 1.40 for a
*diatomic*gas

- 1.40 for a

The gas law above equals a constant, and it does so because the changes in temperature can be encompassed in this formula by measuring the changes in pressure and volume. Mathematically, an integration was done to solve for this formula—and a constant is always added to the equation being integrated—resulting in the constant seen in the equation.

To get a detailed derivation of the modified ideal gas law click here

Adiabatic processes are used in the Otto cycle (when the piston does work on the gasoline) and Brayton cycles within gas turbines. Diesel engines also make use of a (somewhat) adiabatic compression in order to ignite its fuel. Adiabats are also important for the derivation of the Carnot efficiency (the maximum thermal efficiency of any thermodynamic system) which relies on two adiabatic processes.^{[3]}

The video below (from Educational Innovations, Inc.) demonstrates an adiabatic compression: the temperature inside the chamber is increased enough to ignite cotton.

Changing the design of a house can drastically alter its energy efficiency. See energy efficient building design to learn more or explore one of the pages below:

- Isothermal
- Isobar (pressure)
- Isochore
- Ideal gas law
- First law of thermodynamics
- Or explore a random page

- ↑ H. Gould and J. Tobochnik, "Quasistatic Adiabatic Processes," in
*Statistical and Thermal Physics*, 1st ed., Princeton, NJ: Princeton University Press, 2010, ch.2, sec.11, pp. 51-55 - ↑ [2]R. Knight, Physics for scientists and engineers, 2nd ed. San Francisco: Pearson Addison Wesley, 2008, p. 527.
- ↑ R. D. Knight, "The Limits of Efficiency" in
*Physics for Scientists and Engineers: A Strategic Approach,*3nd ed. San Francisco, U.S.A.: Pearson Addison-Wesley, 2008, ch.19, sec.5, pp. 540-542

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Bethel Afework, Allison Campbell, Jordan Hanania, Amanda Musgrove, Kailyn Stenhouse, Jason Donev

Last updated: July 21, 2018

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