The transport properties of an A-B random copolymer melt near the orde
r-disorder phase transition are examined by using a mode coupling appr
oach. The key parameters of the model are the volume fraction of type
A monomers, f, the Flory chi parameter, and a parameter lambda that ch
aracterizes the monomer sequence distribution. The equilibrium phase d
iagram for this model of random copolymers contains a Lifshitz point a
t lambda = lambda(L). For lambda < lambda(L), CoMposition fluctuations
first become unstable at finite wavelength and the homogeneous phase
separates into microphases, while for lambda > lambda(L) the fluctuati
ons first become unstable at infinite wavelength giving a binary fluid
type transition. Our analysis shows that for lambda < lambda(L) the O
nsager coefficient remains finite as the phase transition is approache
d, while the viscosity diverges proportional to epsilon-3/2, where eps
ilon = (T - T(c))/T(c), is the dimensionless difference between the te
mperature and the critical temperature. For lambda > lambda(L), there
is a very weak divergence in the viscosity, but the Onsager coefficien
t diverges proportional to epsilon-1/2 for epsilon-1(lambda - lambda(L
)) much greater than 1, and proportional to epsilon-3/4 for epsilon-1(
lambda - lambda(L)) much less than 1. The dependence of the Onsager co
efficient and viscosity on chi, f and lambda are explicitly determined
.