  In a general supersymmetric standard model there is an upper bound $m_h$ on
the tree level mass of the $CP=+1$ lightest Higgs boson which depends on the
electroweak scale, $\tan \beta$ and the gauge and Yukawa couplings of the
theory. When radiative corrections are included, the allowed region in the
$(m_h,m_t)$ plane depends on the scale $\Lambda$, below which the theory
remains perturbative, and the supersymmetry breaking scale $\Lambda_s$, that we
fix to $1\ TeV$. In the minimal model with $\Lambda=10^{16}\ GeV$: $m_h<130\
GeV$ and $m_t<185\ GeV$. In non-minimal models with an arbitrary number of
gauge singlets and $\Lambda=10^{16}\ GeV$: $m_h<145\ GeV$ and $m_t<185\ GeV$.
We also consider supersymmetric standard models with arbitrary Higgs sectors.
For models whose couplings saturate the scale $\Lambda=10^{16}\ GeV$ we find
$m_h<155\ GeV$ and $m_t<190\ GeV$. As one pushes the saturation scale $\Lambda$
down to $\Lambda_s$, the bounds on $m_h$ and $m_t$ increase. For instance, in
models with $\Lambda=10\ TeV$, the upper bounds for $m_h$ and $m_t$ go to $415\
GeV$ and $385\ GeV$, respectively.
