Thermodynamic relations - Revision history

Carl McBride: Placed notation in a box

2011-10-05T14:10:14Z

Placed notation in a box

@@ Line 1: / Line 1: @@
-These thermodynamic relations are also known as ''coefficient relations''.
+<div style="border:1px solid #f3f3ff; padding-left: 0.5em !important; background-color: #f3f3ff; border-width: 0 0 0 1.4em; clear:right; float:right;">
 <math>T=\left(\frac{\partial U}{\partial S}\right)_V </math>
@@ Line 18: / Line 29: @@
 <math> V=\left(\frac{\partial G}{\partial p}\right)_T </math>
 ==See also==
 *[[Maxwell's relations]]
 *[[Bridgman thermodynamic formulas]]
 [[Category: Classical thermodynamics]]

2011-10-05T14:08:31Z

Added an internal link

← Older revision		Revision as of 16:08, 5 October 2011
Line 30:		Line 30:
	==See also==		==See also==
	*[[Maxwell's relations]]		*[[Maxwell's relations]]
			*[[Bridgman thermodynamic formulas]]
	[[Category: Classical thermodynamics]]		[[Category: Classical thermodynamics]]

2008-01-29T15:32:18Z

Added internal link

← Older revision		Revision as of 17:32, 29 January 2008
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	where		where
	*<math>H</math> is the [[enthalpy]]		*<math>H</math> is the [[enthalpy]]
	*<math>T</math> is the temperature		*<math>T</math> is the [[temperature]]
	*<math>G</math> is the [[Gibbs energy function]]		*<math>G</math> is the [[Gibbs energy function]]
	*<math>U</math> is the [[internal energy]],		*<math>U</math> is the [[internal energy]],

2007-06-28T12:16:48Z

← Older revision		Revision as of 14:16, 28 June 2007
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	<math>T=\left(\frac{\partial U}{\partial S}\right)_V </math>		<math>T=\left(\frac{\partial U}{\partial S}\right)_V </math>

	<math> P=-\left(\frac{\partial U}{\partial V}\right)_S </math>		<math> p=-\left(\frac{\partial U}{\partial V}\right)_S </math>

	<math>T=\left(\frac{\partial H}{\partial S}\right)_p </math>		<math>T=\left(\frac{\partial H}{\partial S}\right)_p </math>

2007-06-08T15:37:25Z

← Older revision		Revision as of 17:37, 8 June 2007
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	*<math>V</math> is the volume		*<math>V</math> is the volume
	*<math>A</math> is the [[Helmholtz energy function]]		*<math>A</math> is the [[Helmholtz energy function]]
	*<math>p</math> is the pressure		*<math>p</math> is the [[pressure]]
	*<math>S</math> is the [[entropy]]		*<math>S</math> is the [[entropy]]
	==See also==		==See also==
	*[[Maxwell's relations]]		*[[Maxwell's relations]]
	[[Category: Classical thermodynamics]]		[[Category: Classical thermodynamics]]

2007-06-07T16:28:22Z

← Older revision		Revision as of 18:28, 7 June 2007
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	*<math>T</math> is the temperature		*<math>T</math> is the temperature
	*<math>G</math> is the [[Gibbs energy function]]		*<math>G</math> is the [[Gibbs energy function]]
	*<math>U</math> is the [[~~First law of thermodynamics \|~~ internal energy]],		*<math>U</math> is the [[internal energy]],
	*<math>V</math> is the volume		*<math>V</math> is the volume
	*<math>A</math> is the [[Helmholtz energy function]]		*<math>A</math> is the [[Helmholtz energy function]]

2007-05-28T17:29:29Z

← Older revision		Revision as of 19:29, 28 May 2007
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	<math> V=\left(\frac{\partial H}{\partial p}\right)_S </math>		<math> V=\left(\frac{\partial H}{\partial p}\right)_S </math>

	<math>S=-\left(\frac{\partial F}{\partial T}\right)_V </math>		<math>S=-\left(\frac{\partial A}{\partial T}\right)_V </math>

	<math> p=-\left(\frac{\partial A}{\partial V}\right)_T </math>		<math> p=-\left(\frac{\partial A}{\partial V}\right)_T </math>
Line 18:		Line 18:
	<math> V=\left(\frac{\partial G}{\partial p}\right)_T </math>		<math> V=\left(\frac{\partial G}{\partial p}\right)_T </math>


			where
			*<math>H</math> is the [[enthalpy]]
			*<math>T</math> is the temperature
			*<math>G</math> is the [[Gibbs energy function]]
			*<math>U</math> is the [[First law of thermodynamics \| internal energy]],
			*<math>V</math> is the volume
			*<math>A</math> is the [[Helmholtz energy function]]
			*<math>p</math> is the pressure
			*<math>S</math> is the [[entropy]]
	==See also==		==See also==
	*[[Maxwell's relations]]		*[[Maxwell's relations]]
	[[Category: Classical thermodynamics]]		[[Category: Classical thermodynamics]]

2007-05-28T16:46:11Z

← Older revision		Revision as of 18:46, 28 May 2007
Line 1:		Line 1:
	These thermodynamic relations are also known as ''coefficient ~~relations'' or ''Maxwell's~~ relations''.		These thermodynamic relations are also known as ''coefficient relations''.

	<math>T=\left(\frac{\partial U}{\partial S}\right)_V </math>		<math>T=\left(\frac{\partial U}{\partial S}\right)_V </math>
Line 17:		Line 17:

	<math> V=\left(\frac{\partial G}{\partial p}\right)_T </math>		<math> V=\left(\frac{\partial G}{\partial p}\right)_T </math>

			==See also==
			*[[Maxwell's relations]]
	[[Category: Classical thermodynamics]]		[[Category: Classical thermodynamics]]

2007-05-28T10:28:26Z

← Older revision		Revision as of 12:28, 28 May 2007
Line 1:		Line 1:
	These thermodynamic relations are also known as ''coefficient relations''.		These thermodynamic relations are also known as ''coefficient relations'' or ''Maxwell's relations''.

	<math>T=\left(\frac{\partial U}{\partial S}\right)_V </math>		<math>T=\left(\frac{\partial U}{\partial S}\right)_V </math>

2007-05-25T16:04:10Z

← Older revision		Revision as of 18:04, 25 May 2007
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	~~Also~~ known as coefficient relations.		These thermodynamic relations are also known as ''coefficient relations''.

	<math>T=\left(\frac{\partial U}{\partial S}\right)_V </math>		<math>T=\left(\frac{\partial U}{\partial S}\right)_V </math>