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Q.Show that the motion of a simple pendulum is simple harmonic and hence derive an equation for its time period. Calculate the change in the length of a simple pendulum of length 1 m, when its period of oscillation changes from 2 sec to 1.5 sec.

Telangana TsbieTelangana Board of Intermediate Education (Intermediate 1st Year) 2018Subjective· 8mImportance★★★★★
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A simple pendulum's restoring torque is proportional to its (small) angular displacement, making its motion SHM with T = 2π√(L/g); reducing T from 2 s to 1.5 s requires shortening the 1 m pendulum by about 0.44 m.

Showing the motion is SHM:

Consider a simple pendulum of length L and bob of mass m, displaced through a small angle θ from the vertical. The forces on the bob are gravity (mg, downward) and the tension in the string. Resolving gravity along and perpendicular to the string, the component of gravity that provides the restoring force (tangential to the arc) is mgsin⁡θmg\sin\theta, directed back toward the equilibrium (mean) position.

Restoring force: F=−mgsin⁡θF = -mg\sin\theta

For small angular displacements (θ in radians, small), sin⁡θ≈θ\sin\theta \approx \theta, so:

F≈−mgθF \approx -mg\theta

Since the arc length displacement is x=Lθx = L\theta, i.e., θ=x/L\theta = x/L:

F=−mgxL=−(mgL)xF = -mg\dfrac{x}{L} = -\left(\dfrac{mg}{L}\right)x

This is of the form F=−kxF = -kx with k=mg/Lk = mg/L, i.e., the restoring force is directly proportional to the displacement x and directed opposite to it — the defining condition of simple harmonic motion.

Deriving the time period:

For SHM, F=−mω2xF = -m\omega^2 x. Comparing with F=−(mg/L)xF = -(mg/L)x:

mω2=mgL⇒ω2=gL⇒ω=gLm\omega^2 = \dfrac{mg}{L} \Rightarrow \omega^2 = \dfrac{g}{L} \Rightarrow \omega = \sqrt{\dfrac{g}{L}}

Since T=2πωT = \dfrac{2\pi}{\omega}:

T=2πLgT = 2\pi\sqrt{\dfrac{L}{g}}

Numerical part:

Given: L1=1L_1 = 1 m, T1=2T_1 = 2 s. Using T1=2πL1/gT_1 = 2\pi\sqrt{L_1/g}: …

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