The sign reversal phenomenon of the quantized Hall conductance observe
d in (TMTSF)2X is explained theoretically in terms of the mean field s
olution for the field-induced spin density wave (FISDW) characterized
by many-order parameters (MOP). The many competing OPs can make the si
gn of the Hall constant change particularly near the subphase boundary
. It is shown that the jump of the Hall constant is accompanied by the
energy gap closing of the FISDW.