A mass $\mathrm{m}$ on an inclined smooth surface is attached to two springs as shown in figure. The other ends of both springs are attached to rigid surface. If the force constant of both spring is $k$, then the periodic time of oscillation for the system is $\ldots \ldots \ldots$
(A) $2 \pi(\mathrm{M} / 2 \mathrm{k})^{1 / 2}$
(B) $2 \pi(2 \mathrm{M} / \mathrm{k})^{1 / 2}$
(C) $2 \pi\{(\mathrm{Mg} \operatorname{Sin} \theta) /(2 \mathrm{k})\}^{1 / 2}$
(C) $2 \pi\{(2 \mathrm{Mg}) / \mathrm{k}\}^{1 / 2}$