  We explore further the idea that the lattice QCD data for hadron properties
in the region m_\pi^2 > 0.2 GeV^2 can be described by the constituent quark
model. This leads to a natural explanation of the fact that nucleon excited
states are generally stable for pion masses greater than their physical
excitation energies. Finally we apply these same ideas to the problem of how
pentaquarks might behave in lattice QCD, with interesting conclusions.
