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energy-momentum density of point particle |
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| Jul29-07, 04:08 PM | #1 |
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energy-momentum density of point particle
I'm using a following notation. [itex](v^1,v^2,v^3)[/itex] is the usual velocity vector, and
[tex] (u^0,u^1,u^2,u^3) = \frac{1}{\sqrt{1-|v|^2/c^2}}(c,v^1,v^2,v^3) [/tex] is the four velocity. So a energy-momentum tensor of dust is [tex] T^{\mu\nu} = \rho_0 u^{\mu} u^{\nu} = \frac{\rho_0}{1-|v|^2/c^2}\left[\begin{array}{cccc} c^2 & cv^1 & cv^2 & cv^3 \\ cv^1 & v^1 v^1 & v^1 v^2 & v^1 v^3 \\ cv^2 & v^2 v^1 & v^2 v^2 & v^2 v^3 \\ cv^3 & v^3 v^1 & v^2 v^3 & v^3 v^3 \\ \end{array}\right] [/tex] My first though was, that a energy-momentum tensor of a point particle would be this multiplied with a delta function, but after some struggling with the transformations of the delta function, I concluded that the result is, nontrivially [tex] T^{\mu\nu} = m_0 \delta^3(x-x(t)) \sqrt{1-|v|^2/c^2} u^{\mu} u^{\nu} = \frac{m_0\delta^3(x-x(t))}{\sqrt{1-|v|^2/c^2}}\left[\begin{array}{cccc} c^2 & cv^1 & cv^2 & cv^3 \\ cv^1 & v^1 v^1 & v^1 v^2 & v^1 v^3 \\ cv^2 & v^2 v^1 & v^2 v^2 & v^2 v^3 \\ cv^3 & v^3 v^1 & v^2 v^3 & v^3 v^3 \\ \end{array}\right] [/tex] Is this correct? |
| Jul29-07, 06:34 PM | #2 |
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Recognitions:
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I'm not sure whether or not there is a totally mathematically consistent formulation of the stress-energy tensor of a point particle or not. See for instance Stingray's comments (and more importantly his references) in the old thread
http://www.physicsforums.com/showthread.php?t=111148 If stingray is around, maybe he could comment in more detail. |
| Jul29-07, 07:14 PM | #3 |
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Mentor
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This looks the same as what I got.
In that post, I initially used inertial motion along the x-axix, Y means [itex]\gamma[/itex] and (x) means [itex]\otimes[/itex]. |
| Jul30-07, 04:10 PM | #4 |
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energy-momentum density of point particle
It seems there are some problems with point masses and metrics in general relativity, if I understood stingray's comments correctly. In special relativity that can probably be ignored.
My derivation went through the fact that [tex] \delta^3(x-x(t))(c,v)^{\mu} [/tex] is a four vector, like a four current of a point charge, and for example [tex] \delta^3(x-x(t)) u^{\mu} [/tex] is not. Good to see that George Jones got the same factors in a different way. |
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