- #1
gdumont
- 16
- 0
Hi,
I have the following problem to solve:
Consider a planet of radius [itex]R[/itex] and mass [itex]M[/itex]. The plante's atmosphere is an ideal gas of [itex]N[/itex] particles of mass [itex]m[/itex] at temperature [itex]T[/itex]. Find the equilibrium distribution function of the gas accounting for the gas itself and the gravitationnal potential of the planet.
Here are my thoughts
The equilibrium function of the gas alone is simply the Maxwell-Boltzmann distribution function [itex]f_0(\mathbf{v})[/itex], so the full distribution is just
[tex]
f(\vec{v})=f_0(\vec{v})e^{-U/kT}
[/tex]
where
[tex]
U=-\frac{GMm}{r}
[/tex]
is the gravitational potential and [itex]r[/itex] is the distance from the center of the planet to the molecule of velocity [itex]\vec{v}[/itex]. I'm not sure if I should replace [itex]r[/itex] by [itex]r-R[/itex] in [itex]U[/itex].
Can anyone confirm if I'm right or not?
Thanks
I have the following problem to solve:
Consider a planet of radius [itex]R[/itex] and mass [itex]M[/itex]. The plante's atmosphere is an ideal gas of [itex]N[/itex] particles of mass [itex]m[/itex] at temperature [itex]T[/itex]. Find the equilibrium distribution function of the gas accounting for the gas itself and the gravitationnal potential of the planet.
Here are my thoughts
The equilibrium function of the gas alone is simply the Maxwell-Boltzmann distribution function [itex]f_0(\mathbf{v})[/itex], so the full distribution is just
[tex]
f(\vec{v})=f_0(\vec{v})e^{-U/kT}
[/tex]
where
[tex]
U=-\frac{GMm}{r}
[/tex]
is the gravitational potential and [itex]r[/itex] is the distance from the center of the planet to the molecule of velocity [itex]\vec{v}[/itex]. I'm not sure if I should replace [itex]r[/itex] by [itex]r-R[/itex] in [itex]U[/itex].
Can anyone confirm if I'm right or not?
Thanks