Two masses m₁ and m₂ are suspended from a spring of spring constant ‘k’. When the masses are in equilibrium, m₁ is gently removed. The
angular frequency and amplitude of oscillation of m₂ will be respectively

• A

  $\sqrt{\frac{\mathrm{K}}{{\mathrm{m}}_2}},\frac{{\mathrm{m}}_1\mathrm{g}}{\mathrm{K}}$

• B

  $\sqrt{\frac{\mathrm{K}}{{\mathrm{m}}_1}},\frac{{\mathrm{m}}_2\mathrm{g}}{\mathrm{K}}$

• C

  $\sqrt{\frac{\mathrm{K}}{{\mathrm{m}}_2}},\frac{{\mathrm{m}}_2\mathrm{g}}{\mathrm{K}}$

• D

  $\sqrt{\frac{\mathrm{K}}{{\mathrm{m}}_1}},\frac{{\mathrm{m}}_1\mathrm{g}}{\mathrm{K}}$