The hfs of the $(4{d}^{9}5{s}^{2})^{2}D_{\frac{5}{2}}$ and $(4{d}^{9}5s5p)^{4}F_{\frac{9}{2}}$ metastable electronic states in ${\mathrm{Ag}}^{107}$ and ${\mathrm{Ag}}^{109}$ have been measured by the atomic-beam magnetic-resonance method. The results, including the hfs dipole interaction constants which have been corrected for second-order interactions with neighboring fine-structure levels, are as follows: $\ensuremath{\Delta}\ensuremath{\nu}({\mathrm{Ag}}^{109}; ^{2}D_{\frac{5}{2}}; F=3\ensuremath{\leftrightarrow}F=2)=435.4750(15) \mathrm{Mc}/sec,$ $\ensuremath{\Delta}\ensuremath{\nu}({\mathrm{Ag}}^{107}; ^{2}D_{\frac{5}{2}}; F=3\ensuremath{\leftrightarrow}F=2)=378.8453(3) \mathrm{Mc}/sec,$ $\ensuremath{\Delta}\ensuremath{\nu}({\mathrm{Ag}}^{109}; ^{4}F_{\frac{9}{2}}; F=5\ensuremath{\leftrightarrow}F=4)=1841.1564(9) \mathrm{Mc}/sec,$ $\ensuremath{\Delta}\ensuremath{\nu}({\mathrm{Ag}}^{107}; ^{4}F_{\frac{9}{2}}; F=5\ensuremath{\leftrightarrow}F=4)=1596.7506(6) \mathrm{Mc}/sec,$ $A{(^{2}D_{\frac{5}{2}})}^{109}=\ensuremath{-}145.1584(5)\mathrm{Mc}/sec, A{(^{2}D_{\frac{5}{2}})}^{107}=\ensuremath{-}126.2818(1) \mathrm{Mc}/sec,$ $A{(^{4}F_{\frac{9}{2}})}^{109}=\ensuremath{-}368.214(9) \mathrm{Mc}/sec, A{(^{4}F_{\frac{9}{2}})}^{107}=\ensuremath{-}319.339(5) \mathrm{Mc}/sec.$ The hfs anomaly for each of the two states is $^{107}\ensuremath{\Delta}^{109}(^{2}D_{\frac{5}{2}})=0.00012(1) \mathrm{and} ^{107}\ensuremath{\Delta}^{109}(^{4}F_{\frac{9}{2}})=\ensuremath{-}0.00298(3).$ By comparing the anomaly in the $^{2}D_{\frac{5}{2}}$ state with that in the ground $^{2}S_{\frac{1}{2}}$ state, we have obtained the amount of $s$-state mixing into the $^{2}D_{\frac{5}{2}}$ state. The contribution to the hfs of the $^{4}F_{\frac{9}{2}}$ level from each of the individual valence electrons has been estimated. The observed anomaly in the $^{4}F_{\frac{9}{2}}$ state is in good agreement with the estimated $s$-electron contribution to the state.