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The Period of Simple Pendulum Motion is Independent of the Pendulum's Mass 📂Physics

The Period of Simple Pendulum Motion is Independent of the Pendulum's Mass

Theorem

The period TT of a simple pendulum motion is independent of the mass of the pendulum mm.

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Description

Therefore, the period TT of a simple pendulum motion is independent of the pendulum’s mass, the amplitude’s size, etc., and depends solely on the pendulum’s length and the acceleration due to gravity.

Proof

The restoring force of the pendulum is as follows:

F=mgsinθ F=-mg\sin\theta

Since x=lθx=l\theta, when θ\theta is sufficiently small, the following approximation holds:

sinθθ \sin\theta \simeq \theta

At this time, the restoring force is:

F= mgsinθ= mgθ= mgxl= mglx \begin{align*} F =&\ -mg \sin\theta \\ =&\ -mg\theta \\ =&\ -mg\frac{x}{l} \\ =&\ -\frac{mg}{l} x \end{align*}

The restoring force of the pendulum can also be expressed as F=kxF=-kx. Therefore,

k=mgl    mk=lg k=\dfrac{mg}{l} \quad \implies \quad \dfrac{m}{k}=\dfrac{l}{g}

The period is T=2πw=2πmkT=\frac{2\pi}{w}=2\pi \sqrt{\frac{m}{k}} , so

T=2πlg T=2\pi\sqrt{\frac{l}{g}}