For the hydrogenlike atom, with central potential -Z/r, partial differentia
l equations exist for the Slater sum Z(r,beta) [beta = (k(B)T)(-1)] and for
its s-wave (l = 0) component Z(0)(r,beta). It is shown that Z can be elimi
nated, to lead to a result in which Z(r,beta) is solely characterized by Z(
0)(r,beta). A similar situation is exhibited for the three-dimensional isot
ropic harmonic oscillator, for which closed forms of both Z(r,beta,omega) a
nd Z(0)(r,beta,omega) can be obtained explicitly. Finally, a third central
field problem is considered in which independent electrons are confined wit
hin a sphere of radius R, but are otherwise free. We are able to derive exp
licitly for this model the s-wave component Z(0)(r,beta,R). The full Slater
sum Z(r,beta,R) then is also analyzed in some detail. (C) 1999 American In
stitute of Physics. [S0022-2488(99)01706-5].