108 SOLUTIONSSubstituting (S.4.20.3) into (S.4.20.2), we obtainAssuming that theacceleration ofgravity is constant, using the hydrostatic
pressureformulaand substituting(S.4.20.5) into(S.4.20.4), wecan writeb) 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 lawwe haveb) The gravitationalenergy of aslice ofatmosphere ofcrosssectionAand
thickness at a height is simply
while the internalenergy of thesame slice is