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III. Long Answers Questions · Q5

Q.Discuss the simple pendulum in detail.

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Step 1. Setup. A simple pendulum is a bob of mass mm on a light, inextensible string of length ll. At any displaced angle θ\theta from the vertical, two forces act: weight mgmg (down) and tension TT (along the string). Resolving weight gives a normal component mgcos⁡θmg\cos\theta (along the string, balanced by tension) and a tangential component mgsin⁡θmg\sin\theta, which always points back towards equilibrium -- the restoring force.

Step 2. Equation of motion. Applying Newton's second law tangentially, with arc-length s=lθs=l\theta so s¨=lθ¨\ddot s=l\ddot\theta: mlθ¨=−mgsin⁡θml\ddot\theta=-mg\sin\theta, i.e. θ¨=−(g/l)sin⁡θ\ddot\theta=-(g/l)\sin\theta -- a non-linear equation because of sin⁡θ\sin\theta.

Step 3. Small-angle approximation. For angular amplitudes up to about 10°10°, sin⁡θ≈θ\sin\theta\approx\theta (in radians), which linearises the equation to θ¨=−(g/l)θ\ddot\theta=-(g/l)\theta, the standard SHM form.

Step 4. Time period. Comparing gives ω2=g/l\omega^2=g/l, so ω=g/l\omega=\sqrt{g/l}, and T=2π/ω=2πl/gT=2\pi/\omega=2\pi\sqrt{l/g}. …

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