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		<id>https://en.formulasearchengine.com/index.php?title=Hyperfinite_type_II_factor&amp;diff=7129</id>
		<title>Hyperfinite type II factor</title>
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		<updated>2013-07-02T21:14:43Z</updated>

		<summary type="html">&lt;p&gt;92.23.156.146: +1&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{Unreferenced stub|auto=yes|date=December 2009}}&lt;br /&gt;
In [[fluid mechanics]] and [[astrophysics]], the &#039;&#039;&#039;relativistic Euler equations&#039;&#039;&#039; are a generalization of the [[Euler equations (fluid dynamics)|Euler equations]] that account for the effects of [[special relativity]].&lt;br /&gt;
&lt;br /&gt;
The [[equations of motion]] are contained in the [[continuity equation]] of the [[stress-energy tensor]] &amp;lt;math&amp;gt;T^{\mu\nu}&amp;lt;/math&amp;gt;:&lt;br /&gt;
:&amp;lt;math&amp;gt;\nabla_\mu T^{\mu\nu}=0.&amp;lt;/math&amp;gt;&lt;br /&gt;
For a [[perfect fluid]], &lt;br /&gt;
:&amp;lt;math&amp;gt;T^{\mu\nu}  \, =  (e+p)u^\mu u^\nu+p \eta^{\mu\nu}.&amp;lt;/math&amp;gt;&lt;br /&gt;
Here &amp;lt;math&amp;gt;e&amp;lt;/math&amp;gt; is the relativistic rest energy  density of the fluid, &amp;lt;math&amp;gt;p&amp;lt;/math&amp;gt; is the [[fluid pressure]], &amp;lt;math&amp;gt;u^\mu&amp;lt;/math&amp;gt; is the [[four-velocity]] of the fluid, and &amp;lt;math&amp;gt;\eta^{\mu\nu}&amp;lt;/math&amp;gt; is the [[Minkowski metric|Minkowski metric tensor]] with [[metric signature|signature]] {{math|(-,+,+,+)}}.  &lt;br /&gt;
&lt;br /&gt;
To the above equations, a  [[Conservation law|statement of conservation]] is usually added, usually conservation of [[baryon number]].  If &amp;lt;math&amp;gt;n&amp;lt;/math&amp;gt; is the [[number density]] of [[baryon]]s this may be stated&lt;br /&gt;
:&amp;lt;math&amp;gt;&lt;br /&gt;
\nabla_\mu&lt;br /&gt;
(nu^\mu)=0.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
These equations reduce to the classical Euler equations if the fluid three-velocity is [[classical mechanics#The Newtonian approximation to special relativity|much less]] than the speed of light, the pressure is much less than the [[energy density]], and the latter is dominated by the rest mass density.&lt;br /&gt;
&lt;br /&gt;
The relativistic Euler equations may be applied to calculate the [[speed of sound]] in a fluid with a relativistic [[equation of state]] (that is, one in which the pressure is comparable with the [[internal energy]] density &amp;lt;math&amp;gt;e&amp;lt;/math&amp;gt;, including the [[rest energy]]; &amp;lt;math&amp;gt;e=\rho c^2+\rho e^C&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;e^C&amp;lt;/math&amp;gt; is the classical internal energy per unit mass).  &lt;br /&gt;
&lt;br /&gt;
Under these circumstances, the speed of sound &amp;lt;math&amp;gt;S&amp;lt;/math&amp;gt; is given by&lt;br /&gt;
:&amp;lt;math&amp;gt;&lt;br /&gt;
S^2=c^2&lt;br /&gt;
\left.&lt;br /&gt;
\frac{\partial p}{\partial e}&lt;br /&gt;
\right|_{\rm adiabatic}.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
(note that &lt;br /&gt;
:&amp;lt;math&amp;gt;e=\rho (c^2+e^C)&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
is the relativistic internal energy density).  This formula differs from the classical case in that &amp;lt;math&amp;gt;\rho&amp;lt;/math&amp;gt; has been replaced by &amp;lt;math&amp;gt;e/c^2&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==See also==&lt;br /&gt;
* [[Relativistic heat conduction]]&lt;br /&gt;
* [[Equation of  state (cosmology)]]&lt;br /&gt;
&lt;br /&gt;
{{DEFAULTSORT:Relativistic Euler Equations}}&lt;br /&gt;
[[Category:Special relativity]]&lt;br /&gt;
[[Category:Equations of fluid dynamics]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{Relativity-stub}}&lt;/div&gt;</summary>
		<author><name>92.23.156.146</name></author>
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