The magnetic relaxation measurements on a heavily Pb-doped Bi 2 Sr 2 CaCu 2 O 8ϩ␦ single crystal were carried out in the vicinity of both the anomalous magnetization peak H 2 p and its onset field H on at different temperatures. The results show that both the normalized magnetic relaxation rate S(ϭϪd ln M/d ln t) and the pinning potential U 0 exhibit remarkable changes near H on and H 2 p in the temperature region where H on (T) follows the relation of the disorder induced vortex lattice transition, H on (T)ϭH on (0)͓1Ϫ(T/T c ) 4 ͔ 3/2 . For both HϽH on and HϾH 2 p , S increases and U 0 decreases, respectively, with increasing magnetic fields. A negative power law of U 0 (H)ϰH Ϫ␣ was observed for both HϽH on and for HϾH 2 p . There exists a minimum in the magnetic-field dependence of S(H) and a maximum in the pinning potential U 0 (H) in the field range between H on and H 2 p . At lower temperature region where H on (T) deviates from the above relation, U 0 (H) behaves differently. The results are discussed in terms of both collective flux creep model and plastic flux creep model.