Transfer-matrix-based calculations of the defect energy in two-dimensi
onal S = 1 Ising spin glasses yield a T = 0 exponent y which depends o
n the state of the spins at the boundary walls. If the boundary spins
are not allowed to be in the zero state, the exponent y agrees with th
e value obtained for S = 1/2. Otherwise the exponent is different and
S-dependent. We argue that the lower critical dimensionality should no
t depend on S. Our results point out the importance of selecting bound
ary conditions that capture the physics of the problem.