Concept:
For small oscillations perpendicular to plane, motion is SHM. Effective length is vertical height of triangle.
Step 1: Geometry of system.
Triangle \(PQR\) is isosceles:
\[
PR = QR = L, \quad PQ = 2d
\]
Drop perpendicular from \(R\) to midpoint of \(PQ\):
\[
\text{Height } h = \sqrt{L^2 - d^2}
\]
Step 2: Physical interpretation.
When displaced slightly out of plane, restoring force acts like simple pendulum of length \(h\).
Step 3: Time period formula.
\[
T = 2\pi \sqrt{\frac{h}{g}}
\]
Step 4: Substitute value.
\[
T = 2\pi \sqrt{\frac{\sqrt{L^2 - d^2}}{g}}
\]
Step 5: Conclusion.
\[
T = 2\pi \sqrt{\frac{\sqrt{L^2 - d^2}}{g}}
\]