Articles
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10/16/2003--
10/16/2003
The thermal and kinematic Sunyaev-Zel'dovich effects revisited
This paper shows that a simple convolution integral expression based on the
mean value of the isotropic frequency distribution corresponding to photon
scattering off electrons leads to useful analytical expressions describing the
thermal Sunyaev-Zel'dovich effect. The approach, to first order in the Compton
parameter is able to reproduce the Kompaneets equation describing the effect.
Second order effects in the parameter $z=\frac{kT_{e}}{mc^{2}}$ induce a slight
increase in the crossover frequency.
A. Sandoval-Villalbazo
L. S. Garcia-Colin
08/03/2004--
03/10/2004
Jeans instability in the linearized Burnett regime
Jeans instability is derived for the case of a low density self-gravitating
gas beyond the Navier-Stokes equations. The Jeans instability criterium is
shown to depend on a Burnett coefficient if the formalism is taken up to fourth
order in the wave number. It is also shown that previously known viscosity
corrections to the Jeans wave-number are enhanced if the full fourth order
formalism is applied to the stability analysis.
L. S. Garcia-Colin
A. Sandoval-Villalbazo
07/15/2004--
07/15/2004
On a parity property in the thermal Sunyaev-Zel'dovich effect
The main issue in this paper is to discuss a parity property that appears in
the expressions for the distorted spectrum of the thermal Sunyaev-Zel'dovich
effect. When using the convolution integrals method involving scattering laws
we argue that the distorted spectrum contains a new term, which is an odd power
of the frequency. Such a term, absent in the conventional approaches, implies a
crossover frequency which differs in value form the ones reported in the
literature by a significant, in principle observable, amount. Also, such term
casts doubt on the demanding need of computing complicated relativistic
calculations. The relationship of our approach with the existing calculations
is discussed.
A. Sandoval-Villalbazo
L. S. Garcia-Colin
09/20/2004--
09/06/2004
The statistical nature of the second order corrections to the thermal SZE
This paper shows that the accepted expressions for the second order
corrections in the parameter $z$ to the thermal Sunyaev-Zel'dovich effect can
be accurately reproduced by a simple convolution integral approach. This
representation allows to separate the second order SZE corrections into two
type of components. One associated to a single line broadening, directly
related to the even derivative terms present in the distortion intensity curve,
while the other is related to a frequency shift, which is in turn related to
the first derivative term.
A. Sandoval-Villalbazo
L. S. Garcia-Colin
12/13/2006--
12/13/2006
Thermoelectric and Thermomagnetic Effects in Dilute Plasmas
When an electrically charged system is subjected to the action of an
electromagnetic field, it responds by generating an electrical current. In the
case of a multicomponent plasma other effects, the so called cross effects,
influence the flow of charge as well as the heat flow. In this paper we discuss
these effects and their corresponding transport coefficients in a fully ionized
plasma using Boltzmann's equation. Applications to non-confined plasmas,
specially to those prevailing in astrophysical systems are highlighted. Also, a
detailed comparison is given with other available results.
L. S. Garcia-Colin
A. L. Garcia-Perciante
A. Sandoval-Villalbazo
10/25/2002--
10/25/2002
Cosmological bulk viscosity, the Burnett regime, and the BGK equation
Einstein's field equations in FRW space-times are coupled to the BGK equation
in order to derive the stress energy tensor including dissipative effects up to
second order in the thermodynamical forces. The space-time is assumed to be
matter-dominated, but in a low density regime for which a second order
(Burnett) coefficient becomes relevant. Cosmological implications of the
solutions, as well as the physical meaning of transport coefficients in an
isotropic homogeneous universe are discussed.
A. Sandoval-Villalbazo
L. S. Garcia-Colin
03/16/2005--
03/11/2005
Relativistic non-equilibrium thermodynamics revisited
Relativistic irreversible thermodynamics is reformulated following the
conventional approach proposed by Meixner in the non-relativistic case. Clear
separation between mechanical and non-mechanical energy fluxes is made. The
resulting equations for the entropy production and the local internal energy
have the same structure as the non-relativistic ones. Assuming linear
constitutive laws, it is shown that consistency is obtained both with the laws
of thermodynamics and causality.
L. S. Garcia-Colin
A. Sandoval-Villalbazo
11/11/2005--
11/11/2005
Light scattering test regarding the relativistic nature of heat
The dynamic structure factor of a simple relativistic fluid is calculated.
The coupling of acceleration with the heat flux present in Eckart's version of
irreversible relativistic thermodynamics is examined using the
Rayleigh-Brillouin spectrum of the fluid. A modification of the width of the
Rayleigh peak associated to Eckart's picture of the relativistic nature of heat
is predicted and estimated.
A. Sandoval-Villalbazo
L. S. Garcia-Colin
01/11/2006--
01/11/2006
Hyperbolic heat equation in Kaluza's magnetohydrodynamics
This paper shows that a hyperbolic equation for heat conduction can be
obtained directly using the tenets of linear irreversible thermodynamics in the
context of the five dimensional space-time metric originally proposed by T.
Kaluza back in 1922. The associated speed of propagation is slightly lower than
the speed of light by a factor inversely proportional to the specific charge of
the fluid element. Moreover, consistency with the second law of thermodynamics
is achieved. Possible implications in the context of physics of clusters of
galaxies of this result are briefly discussed.
A. Sandoval-Villalbazo
A. L. Garcia-Perciante
L. S. Garcia-Colin
02/08/2008--
08/23/2007
Generalized Relativistic Chapman-Enskog Solution of the Boltzmann Equation
The Chapman-Enskog method of solution of the relativistic Boltzmann equation
is generalized in order to admit a time-derivative term associated to a
thermodynamic force in its first order solution. Both existence and uniqueness
of such a solution are proved based on the standard theory of integral
equations. The mathematical implications of the generalization here introduced
are thoroughly discussed regarding the nature of heat as chaotic energy
transfer in the context of relativity theory.
A. L. Garcia-Perciante
A. Sandoval-Villalbazo
L. S. Garcia-Colin
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