The quadrupole interaction of polarized $^{92}\mathrm{Mo}$(${8}^{+}$,\ensuremath{\tau}=0.29 \ensuremath{\mu}s) and $^{93}\mathrm{Ru}$(21/${2}^{+}$,\ensuremath{\tau}=3.5 \ensuremath{\mu}s) isomers in a single crystal of Zr has been measured. The experiment utilizes the nuclear polarization induced by the tilted-multifoil interaction with separated isomer beams from a mass spectrometer. The magnitudes and signs of the quadrupole moments were deduced to be -0.33 and +0.04 b for $^{92}\mathrm{Mo}$(${8}^{+}$) and $^{93}\mathrm{Ru}$ (21/${2}^{+}$), respectively. Together with previous work on the $^{88,90}\mathrm{Zr}$(${8}^{+}$) isomers, this experiment sheds light on the particle-hole shell-model structure in the A=90 region. It also serves as a calibration of a recent experiment on parity mixing in the 17/${2}^{\mathrm{\ensuremath{-}}}$-17/${2}^{+}$ doublet in $^{93}\mathrm{Tc}$. The induced nuclear polarization under the conditions of a separated reaction-product beam is found to be substantially higher than in previous in-beam experiments.