  This paper is divided into two parts. In the first part we analyze the
consequences, for the LHC, of gauge and third family Yukawa coupling
unification with a particular set of boundary conditions defined at the GUT
scale. We perform a global chi^2 analysis including the observables M_W, M_Z,
G_F, 1/alpha_em, alpha_s(M_Z), M_t,m_b(m_b), M_tau, BR(B -> X_s gamma), BR(B_s
-> mu^+ mu^-) and M_h. The fit is performed in the MSSM in terms of 9 GUT scale
parameters, while tan beta and mu are fixed at the weak scale. Good fits
suggest an upper bound on the gluino mass, M_gluino \lesssim 2 TeV. This
constraint comes predominantly from fitting the bottom quark and Higgs masses
(assuming a 125 GeV Higgs). Gluinos should be visible at the LHC in the 14 TeV
run but they cannot be described by the typical simplified models. This is
because the branching ratios for gluino -> t tbar neutralino, b bbar
neutralino, t bbar chargino^-, b tbar chargino^+, g neutralino are comparable.
Stops and sbottoms may also be visible. Charginos and neutralinos can be light
with the LSP predominantly bino-like. In the second part of the paper we
analyze a complete three family model and discuss the quality of the global
chi^2 fits and the differences between the third family analysis and the full
three family analysis for overlapping observables. We note that the light Higgs
in our model couples to matter like the Standard Model Higgs. Any deviation
from this would rule out this model.
