The time-dependent Ginzburg-Landau equations of superconductivity defi
ne a dynamical process when the applied magnetic field varies with tim
e. Sufficient conditions (in terms of the time rate of change of the a
pplied field) are given that, if satisfied, guarantee that this dynami
cal process is asymptotically autonomous. As time goes to infinity, th
e dynamical process asymptotically approaches a dynamical system whose
attractor coincides with the omega-limit set of the dynamical process
.