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Q.Find the time period of a simple pendulum of length 'l'. Also show that it does not depend upon mass.

Rajasthan RbseRajasthan Board Senior Secondary Part-I Examination 2024Subjective· 3mImportance★★★★★
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The time period of a simple pendulum is T=2πl/gT = 2\pi\sqrt{l/g}; the mass cancels out of the derivation, so TT is independent of the bob's mass.

Setup: a simple pendulum consists of a point mass (bob) of mass mm suspended from a fixed point by a light, inextensible string of length ll. When displaced by a small angle θ\theta from the vertical and released, gravity provides a restoring torque about the point of suspension.

Deriving the time period: the restoring force along the arc of swing (tangential component of gravity) is

F=−mgsin⁡θF = -mg\sin\theta

For small angles, sin⁡θ≈θ\sin\theta \approx \theta (in radians), so

F≈−mgθF \approx -mg\theta

The displacement along the arc is x=lθx = l\theta, so θ=x/l\theta = x/l, giving

F=−mgxl=−(mgl)xF = -mg\dfrac{x}{l} = -\left(\dfrac{mg}{l}\right)x

This is the SHM force equation F=−kxF = -kx, with an effective "spring constant" k=mg/lk = mg/l. Comparing with Newton's second law F=ma=md2xdt2F = ma = m\dfrac{d^2x}{dt^2}:

md2xdt2=−mglx⇒d2xdt2=−glxm\dfrac{d^2x}{dt^2} = -\dfrac{mg}{l}x \quad\Rightarrow\quad \dfrac{d^2x}{dt^2} = -\dfrac{g}{l}x

Comparing with the standard SHM equation d2xdt2=−ω2x\dfrac{d^2x}{dt^2} = -\omega^2 x, we identify

ω2=gl⇒ω=gl\omega^2 = \dfrac{g}{l} \quad\Rightarrow\quad \omega = \sqrt{\dfrac{g}{l}}

Since T=2π/ωT = 2\pi/\omega:

T=2πlgT = 2\pi\sqrt{\dfrac{l}{g}}

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