We show that the present LEPI lower bound on the Standard Model Higgs boson mass (\(M_H\gsim60\GeV\)) applies as well to the lightest Higgs boson (\(h\)) of the minimal \(SU(5)\) and no-scale flipped \(SU(5)\) supergravity models. This result would persist even for the ultimate LEPI lower bound (\(M_H\gsim70\GeV\)). We show that this situation is a consequence of a decoupling phenomenon in the Higgs sector driven by radiative electroweak breaking for increasingly larger sparticle masses, and thus it should be common to a large class of supergravity models. A consequence of \(m_h\gsim60\GeV\) in the minimal \(SU(5)\) supergravity model is the exclusion from the allowed parameter space of `spoiler modes' (\(\chi^0_2\to\chi^0_1 h\)) which would make the otherwise very promising trilepton signal in \(p\bar p\to\chi^\pm_1\chi^0_2X\) unobservable at Fermilab. Within this model we also obtain stronger upper bounds on the lighter neutralino and chargino masses, \ie, \(m_{\chi^0_1}\lsim50\GeV\), \(m_{\chi^0_2,\chi^\pm_1}\lsim100\GeV\). This should encourage experimental searches with existing facilities.