Difference between revisions of "Entropy"
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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== | ||
| + | ===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== | ==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.