[Commits] [svn:einsteintoolkit] incoming/Outflow/ (Rev. 61)
roland.haas at physics.gatech.edu
roland.haas at physics.gatech.edu
Mon Apr 16 11:15:44 CDT 2012
User: rhaas
Date: 2012/04/16 11:15 AM
Added:
/Outflow/
README, interface.ccl, param.ccl, schedule.ccl
/Outflow/doc/
documentation.tex, openformula.mw, sphericalinfall.mw
/Outflow/src/
make.code.defn, outflow.c
/Outflow/test/
moving_tov.par
/Outflow/test/moving_tov/
outflow_det_0.asc, outflow_det_1.asc, outflow_surface_det_0_fluxdens.asc, outflow_surface_det_1_fluxdens.asc, surface_projection_0[0].xy.asc, surface_projection_0[1].xy.asc, surface_projection_1[0].xy.asc, surface_projection_1[1].xy.asc
Log:
Outflow: GT/PSU's outflow thorn
Outflow provides a means to calcuate the flow of rest mass D = rho*w_lorentz
through a spherical surface. We take the definition of the rest mass from Eq.
(11) in arXiv:0812.2245v2 to be
M = \int \rho W \sqrt\gamma d^3x
this meshes with the EOM for hydro which gives:
D_{,t} + (D [\alpha v^i - \beta^i])_{,\i} = 0
(eg. Font lrr-2008-7 Eq. (28) ff) where D=D_{whisky} = \sqrt\gamma*D_{lrr}
with this we can easyly get
M_{,t} = - \oint_{\partial V} D [\alpha v^i - \beta^i] d\Sigma_i
File Changes:
Directory: /Outflow/
====================
File [added]: README
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File [added]: interface.ccl
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File [added]: param.ccl
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File [added]: schedule.ccl
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Directory: /Outflow/doc/
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File [added]: documentation.tex
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File [added]: openformula.mw
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File [added]: sphericalinfall.mw
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Directory: /Outflow/test/moving_tov/
====================================
File [added]: outflow_det_0.asc
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File [added]: outflow_det_1.asc
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File [added]: outflow_surface_det_0_fluxdens.asc
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File [added]: outflow_surface_det_1_fluxdens.asc
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File [added]: surface_projection_0[0].xy.asc
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File [added]: surface_projection_0[1].xy.asc
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File [added]: surface_projection_1[0].xy.asc
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File [added]: surface_projection_1[1].xy.asc
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Directory: /Outflow/src/
========================
File [added]: make.code.defn
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File [added]: outflow.c
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Directory: /Outflow/test/
=========================
File [added]: moving_tov.par
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