The maximum velocity \( v_{\text{max}} \) of a spring-mass system in simple harmonic motion is \( v_{\text{max}} = A \omega \), where \( A \) is the amplitude and \( \omega \) is the angular frequency. The angular frequency \( \omega \) is defined as \( \omega = \sqrt{\frac{k}{m}} \), with \( k \) being the spring constant and \( m \) the mass. For two bodies with identical amplitudes, the ratio of their maximum velocities is \( \frac{v_A}{v_B} = \frac{A \omega_A}{A \omega_B} = \frac{\omega_A}{\omega_B} = \sqrt{\frac{k_1}{k_2}} \). Consequently, the ratio of the maximum velocity of body A to that of body B equals \( \sqrt{\frac{k_1}{k_2}} \).