5.1. Models for The Energy Flow
The simplest mode of relativistic energy flow is in the form of
kinetic energy of relativistic particles. A variant that have been
suggested is based on the possibility that a fraction of the energy is
carried by Poynting flux
[224,
225,
226,
69,
227]
although in all models the power must be converted to kinetic energy
somewhere. The energy flow of ~ 1050 ergs/sec from a compact
object whose size is
107cm
requires a magnetic field of
1015Gauss or higher at the source. This large value might be
reached in stellar collapses of highly magnetized stars or amplified
from smaller fields magnethohydrodynamically
[69]. Overall
the different models can be characterized by two parameters: the ratio
of the kinetic energy flux to the Poynting flux and the location of
the energy conversion stage
(
1012 cm
for internal conversion or
1016 cm
for external conversion). This is
summarized in Table 5.1. In the following
section we will focus on the simplest possibility, that is of a
kinetic energy flux.
Kinetic Energy | Kinetic Energy and | Poynting Flux | |
Dominated | Poynting Flux | Dominated | |
Internal | [28, 29, 18] | [224] | [225, 69, 227] |
conversion | |||
External | [27, 219] | - | [226, 69] |
conversion | |||