A simple pendulum of length l has been set up inside a railway wagon sliding down a frictionless inclined plane having an angle of inclination θ=30∘ with the horizontal. The period of oscillation as recorded by an observer inside the wagon is
On the inclined plane, the effective acceleration due to gravity,
g′=g cos30=g×√32
∴T=2π√lg′=2π√2l√3g