Previous comparisons of optical and X-ray observations of clusters of
galaxies have led to the so-called beta-discrepancy that has persisted
for the last decade. The standard hydrostatic-isothermal model for cl
usters predicts that the parameter beta(spec) = sigma(r)2/(kT/mum(p)),
which describes the ratio of energy per unit mass in galaxies to that
in the gas, should equal the parameter beta(fit) (where rho(gas)(r) i
s-proportional-to rho(gal)(r)(beta(fit)) determined from the X-ray sur
face brightness distribution. The observations suggest an apparent dis
crepancy: beta(spec) approximately 1.2 (i.e., the galaxies are ''hotte
r'' than the gas), while beta(fit) approximately 0.65 (i.e., the gas i
s ''hotter'' and more extended than the galaxies). Here we show that t
he discrepancy is resolved when the actual observed galaxy distributio
n in clusters is used, rho(gal)(r) is-proportional-to r -2.4+/-0.2, in
stead of the previously assumed steeper King approximation, rho(gal)(r
) is-proportional-to r-3. Using the correct galaxy profile in clusters
, we show that the standard hydrostatic-isothermal model predicts beta
(spec) = beta(fit)c congruent-to (1.25 +/- 0.1)beta(fit), rather than
beta(spec) congruent-to beta(fit), (where beta(fit) is the standard pa
rameter using the King approximation, and beta(fit)c is the corrected
parameter using the proper galaxy distribution). Using a large sample
of clusters, we find best-fit mean values of beta(spec) = 0.94 +/- 0.0
8 and beta(fit)c = 1.25beta(fit) = 0.84 +/- 0.1. These results resolve
the beta-discrepancy and provide additional support for the hydrostat
ic cluster model.