108 SOLUTIONS
Substituting (S.4.20.3) into (S.4.20.2), we obtain
Assuming that theacceleration ofgravity is constant, using the hydrostatic
pressureformula
and substituting(S.4.20.5) into(S.4.20.4), wecan write
b) For the atmosphere,usingdiatomicmolecules with and
we havefrom(S.4.20.6),
This value of isabout a factor of 2 larger than that for theactual
atmosphere.
4.21 Atmospheric Energy (Rutgers)
a) Again startingwith theideal gas law
we have
b) The gravitationalenergy of aslice ofatmosphere ofcrosssectionAand
thickness at a height is simply
while the internalenergy of thesame slice is