Variable Eddington Factor in a Relativistic Plane-Parallel Flow

Details Variable Eddington Factor in a Relativistic Plane-Parallel Flow Variable Eddington Factor in a Relativistic Plane-Parallel Flow

2009-04-18

arxiv.org/abs/0904.2804v1

PASJ, 60, 1209 (2008)

Astronomy and Astrophysics

Astrophysics

High Energy Astrophysical Phenomena

8 pages, 7 figures

Scientific paper

We examine the Eddington factor in an optically thick, relativistic flow accelerating in the vertical direction. % When the gaseous flow is radiatively accelerated and there is a velocity gradient, there also exists a density gradient. The comoving observer sees radiation coming from a closed surface where the optical depth measured from the observer is unity. Such a surface, called a {\it one-tau photo-oval}, is elongated in the flow direction. In general, the radiation intensity emitted by the photo-oval is non-uniform, and the photo-oval surface has a relative velocity with respect to the position of the comoving observer. Both effects introduce some degree of anisotropy in the radiation field observed in the comoving frame. As a result, the radiation field observed by the comoving observer becomes {\it anisotropic}, and the Eddington factor must deviate from the usual value of 1/3. Thus, the relativistic Eddington factor generally depends on the optical depth $\tau$ and the velocity gradient $du/d\tau$, $u$ being the four velocity. % In the case of a plane-parallel vertical flow, we obtain the shape of the photo-oval and calculate the Eddington factor in the optically thick regime. We found that the Eddington factor $f$ is well approximated by $f(\tau, \frac{du}{d\tau}) = {1/3} \exp (\frac{1}{u} \frac{du}{d\tau}) $. % This relativistic variable Eddington factor can be used in various relativistic radiatively-driven flows.

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