We discuss the Hall effect and resistivity above T(c), using a variant
of the bipolaron theory which takes into account Anderson localizatio
n of the bosons by disorder. The model supposes that R(H) = 1/2en(b)C,
where n(b) is the number of delocalized carriers. Temperature and dop
ing dependences of rho, R(H), cot THETA(H), and the ''spin'' gap in YB
a2Cu3O7-delta are explained.