  Conventional and hybrid light quark baryons are constructed in the
non-relativistic flux-tube model of Isgur and Paton, which is motivated by
lattice QCD. The motion of the flux tube with the three quark positions fixed,
except for center of mass corrections, is discussed. It is shown that the
problem can be reduced to the independent motion of the junction and the
strings connecting the junction to the quarks. The important role played by
quark-exchange symmetry in constraining the flavor structure of (hybrid)
baryons is emphasized. The flavor, quark spin S, total spin J, and parity P of
the seven low-lying hybrid baryons are found to be N2(1/2)+, N2(3/2)+,
Delta4(1/2)+, Delta4(3/2)+, and Delta4(5/2)+, where the notation is
flavor[2S+1](J)P, and the N2(1/2)+ and N2(3/2)+ states are doublets. The motion
of the three quarks in an adiabatic potential derived from the flux-tube
dynamics is considered. A mass of 1870 +/- 100 MeV for the lightest nucleon
hybrids is found by employing a variational method.
