Step 1: Understanding the Concept:
In SHM the maximum velocity occurs at the mean position and equals amplitude times angular frequency. For a spring-mass system, \(\omega = \sqrt{K/m}\).
Step 2: Key Formula or Approach:
\[ v_{max} = A\omega = A\sqrt{\frac Km} \]
Step 3: Detailed Explanation:
The masses of A and B are equal, so write for each particle:
\[ A_A\sqrt{\frac{K_A}{m}} = A_B\sqrt{\frac{K_B}{m}} \]
Cancel \(m\):
\[ A_A\sqrt{K_A} = A_B\sqrt{K_B} \]
\[ \frac{A_B}{A_A} = \frac{\sqrt{K_A}}{\sqrt{K_B}} \]
So the ratio is \(\sqrt{K_A}:\sqrt{K_B}\). The stiffer spring gives the smaller amplitude. Option (D) is the inverse of this ratio, and options (A) and (C) forget the square root.
Final Answer:
The ratio of the amplitude of B to that of A is \(\sqrt{K_A}:\sqrt{K_B}\), option (B).
\[ \boxed{\sqrt{K_A}:\sqrt{K_B} \text{ (B)}} \]