(N/A) Let the mass be displaced by a small distance $x$ to the right side of the equilibrium position,as shown in the figure. Under this situation,the spring on the left side gets elongated by a length equal to $x$ and that on the right side gets compressed by the same length.
The forces acting on the mass are then:
$F_{1} = -k x$ (force exerted by the spring on the left side,trying to pull the mass towards the mean position)
$F_{2} = -k x$ (force exerted by the spring on the right side,trying to push the mass towards the mean position)
The net force,$F$,acting on the mass is then given by:
$F = F_{1} + F_{2} = -k x - k x = -2 k x$
Since the net force $F$ is proportional to the displacement $x$ and is directed towards the mean position $(F \propto -x)$,the motion executed by the mass is simple harmonic.
Comparing this with the standard equation of simple harmonic motion $F = -K_{eff} x$,we get the effective spring constant $K_{eff} = 2 k$.
The time period of oscillations is given by:
$T = 2 \pi \sqrt{\frac{m}{K_{eff}}} = 2 \pi \sqrt{\frac{m}{2 k}}$