Entropy (astrophysics) explained

In astrophysics, what is referred to as "entropy" is actually the adiabatic constant derived as follows.[1]

Using the first law of thermodynamics for a quasi-static, infinitesimal process for a hydrostatic system

dQ=dU-dW.

[2]

For an ideal gas in this special case, the internal energy, U, is a function of only the temperature T; therefore the partial derivative of heat capacity with respect to T is identically the same as the full derivative, yielding through some manipulation

dQ=CvdT+PdV.

Further manipulation using the differential version of the ideal gas law, the previous equation, and assuming constant pressure, one finds

dQ=CpdT-VdP.

dQ=0

and recalling

\gamma={Cp

}/\,, [3] one finds
VdP=CpdT
PdV=-CvdT
dP
P

=-

dV
V

\gamma.

One can solve this simple differential equation to find

PV\gamma=constant=K

This equation is known as an expression for the adiabatic constant, K, also called the adiabat. From the ideal gas equation one also knows

P=\rhokBT
\mumH

,

where

kB

is the Boltzmann constant.Substituting this into the above equation along with

V=[g]/\rho

and

\gamma=5/3

for an ideal monatomic gas one finds

K=

kBT
(\rho/\mu
2/3
m
H)

,

where

\mu

is the mean molecular weight of the gas or plasma; [4] and

mH

is the mass of the hydrogen atom, which is extremely close to the mass of the proton,

mp

, the quantity more often used in astrophysical theory of galaxy clusters.This is what astrophysicists refer to as "entropy" and has units of [keV⋅cm<sup>2</sup>]. This quantity relates to the thermodynamic entropy as

\DeltaS=3/2lnK.

Notes and References

  1. Web site: Adiabatic Condition Development . 2024-11-03 . hyperphysics.phy-astr.gsu.edu.
  2. Web site: m300l5 . 2024-11-03 . personal.ems.psu.edu.
  3. Web site: THERMAL PROPERTIES OF MATTER . 2024-11-03 . www.sciencedirect.com.
  4. Web site: Mean molecular weight .