We study the dependence of quark condensate Sigma on an external magne
tic field. For weak fields, it rises linearly: Sigma(H) = Sigma(0)[1 eH ln 2/(16 pi(2)F(pi)(2)) + ...]. M-pi and F-pi are also shifted so
that the Gell-Mann-Oakes-Renner relation is satisfied. In the strong f
ield region, Sigma(H) proportional to (eH)(3/2). (C) 1997 Published by
Elsevier Science B.V.