Difference between revisions of "Entropy"

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(Removed everything written by people with no understanding of physics. Not much left. Even AiG has rejected the nonsense!)
(Added some definitions)
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The second law of thermodynamics states that entropy will always increase over time within a closed system, defining a closed system as one in which neither matter nor energy may enter or leave.
 
The second law of thermodynamics states that entropy will always increase over time within a closed system, defining a closed system as one in which neither matter nor energy may enter or leave.
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==Definitions==
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===Thermodynamic definition===
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In classical [[thermodynamics]], if a small amount of energy dQ is supplied to a system from a reservoir held at temperature T, the change in entropy is given by
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<math>
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dS=\frac{dQ}{T}
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</math>
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===Statistical mechanics definition 1===
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If a system can be arranged in W different ways, the entropy is
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<math> S= k_B \log W </math>
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where <math>k_B</math> is Boltzmann's constant.
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===Statistical mechanics definition 2===
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Label the different states a thermodynamic system can be in by <math>i=1,2,3\ldots N</math>. If the probability of finding the system in state i is <math>p_i</math>, the entropy is
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<math>
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S=-k_B \sum_i^N p_i \log p_i
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</math>
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This definition is closely related to ideas in [[information theory]], where the definition of information content is very similar to the definition of entropy.
  
 
==See also==
 
==See also==

Revision as of 22:05, May 12, 2008

Entropy is a measure of disorder or information content in a system, first postulated by Lazare Carnot in 1803.

The second law of thermodynamics states that entropy will always increase over time within a closed system, defining a closed system as one in which neither matter nor energy may enter or leave.

Definitions

Thermodynamic definition

In classical thermodynamics, if a small amount of energy dQ is supplied to a system from a reservoir held at temperature T, the change in entropy is given by

<math> dS=\frac{dQ}{T} </math>

Statistical mechanics definition 1

If a system can be arranged in W different ways, the entropy is

<math> S= k_B \log W </math>

where <math>k_B</math> is Boltzmann's constant.

Statistical mechanics definition 2

Label the different states a thermodynamic system can be in by <math>i=1,2,3\ldots N</math>. If the probability of finding the system in state i is <math>p_i</math>, the entropy is

<math> S=-k_B \sum_i^N p_i \log p_i </math>

This definition is closely related to ideas in information theory, where the definition of information content is very similar to the definition of entropy.

See also

References