The equations for the flow of a viscoelastic fluid of the Maxwell type are
analyzed in a linear approximation. First, we establish that the solution d
epends continuously on changes in the relaxation time. Next, we investigate
how the solution to the linearized Maxwell system converges to the solutio
n to Stokes flow as the relaxation time tends to zero. Convergence in diffe
rent measures is examined and specific a priori bounds are derived.