We derive the long-wavelength elastic theory for the quantum Hall smectic s
tate starting from the Hartree-Fock approximation. Dislocations in this sta
te lead to an effective nematic model for T>0, which undergoes a disclinati
on unbinding transition from a phase with algebraic orientational order int
o an isotropic phase. We obtain transition temperatures that are in qualita
tive agreement with recent experiments that have observed large anisotropie
s of the longitudinal resistivities in half-filled Landau levels, lending c
redence to the liquid crystal interpretation of experiments.