 Solution

Assume that the transverse field is large enough to saturate through the thickness despite demagnetizing effects, and retain the thin-layer plane-stress and open-circuit assumptions from part(a). The two imposed in-plane strains now becomeTheir sum is $-\Lambda$, whereas it was $\Lambda /2$ for longitudinal saturation. The in-plane stress sum, and hence the induced open-circuit voltage, is multiplied by $-2$:Thus the magnitude is about $24\mathrm{mV}$ with the opposite polarity, under this model. The larger demagnetizing field for an out-of-plane direction means the same external field magnitude might not produce the same degree of saturation. Changes in thickness constraint or strain transfer would also modify the estimate.