Pendulums — Question 1

Section 15-5 · Physics pages 2312–2313

Question 1 The small-angle approximation is an approximation to the torque A point mass on a massless inextensible string of length ℓswings in gravity. Angle θ is measured from downward vertical. Ignore air drag and use radians in expansions. θ ℓ Pendulum schematic; angle is measured from the downward vertical. (a) Derive the exact angular equation and its SHM approximation. Express the corresponding equation for arc displacement s = ℓθ. (b) At amplitude 30◦, find the ratio of exact restoring-torque magnitude to the linear approximation. Using sin θ/θ ≈1 −θ2/6, estimate an amplitude limit for a 1% torque error relative to the linear value.
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Question 1 - Solution The small-angle approximation is an approximation to the torque θ ℓ (a) Derivation and calculation mℓ2¨θ = −mgℓsin θ ⇒¨θ = −g ℓsin θ . |θ| ≪1 : sin θ ≃θ, ¨θ + g ℓθ = 0. s = ℓθ ⇒¨s + g ℓs = 0 , ω = √ g/ℓ. (b) Result and interpretation At 30◦= π/6, τexact τlinear = sin θ θ = 3 π = .95493 . θ −sin θ θ ≃θ2 6 ≤.01 ⇒|θ| ≲.24495 rad = 14.03◦. This is the leading-order torque error, not the period error. Physical check The linear torque slightly overestimates the restoring torque because sin θ < θ for small positive angles.

Question 1

The small-angle approximation is an approximation to the torque

A point mass on a massless inextensible string of length ℓ\ell swings in gravity. Angle θ\theta is measured from downward vertical. Ignore air drag and use radians in expansions.

Diagram shown in the original SVG worksheet.

  1. Derive the exact angular equation and its SHM approximation. Express the corresponding equation for arc displacement s=ℓθs=\ell\theta.

  2. At amplitude 30∘30^\circ, find the ratio of exact restoring-torque magnitude to the linear approximation. Using sin⁡θ/θ≈1−θ2/6\sin\theta/\theta\approx1-\theta^2/6, estimate an amplitude limit for a 1%1\% torque error relative to the linear value.

Question 1 - Solution

The small-angle approximation is an approximation to the torque

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

mℓ2θ̈=−mgℓsin⁡θ⇒θ̈=−gℓsin⁡θ.m\ell^2\ddot\theta=-mg\ell\sin\theta\Rightarrow\boxed{\ddot\theta=-\frac g\ell\sin\theta}.|θ|≪1:sin⁡θ≃θ,θ̈+gℓθ=0.|\theta|\ll1:\quad\sin\theta\simeq\theta,\quad\ddot\theta+\frac g\ell\theta=0.s=ℓθ⇒s̈+gℓs=0,ω=g/ℓ.s=\ell\theta\Rightarrow\boxed{\ddot s+\frac g\ell s=0},\quad\omega=\sqrt{g/\ell}.

(b) Result and interpretation

At 30∘=π/630^\circ=\pi/6,τexactτlinear=sin⁡θθ=3π=.95493.\frac{\tau_{\mathrm{exact}}}{\tau_{\mathrm{linear}}}=\frac{\sin\theta}{\theta}=\frac3\pi=\boxed{.95493}.θ−sin⁡θθ≃θ26≤.01⇒|θ|≲.24495rad=14.03∘.\frac{\theta-\sin\theta}{\theta}\simeq\frac{\theta^2}{6}\le.01\Rightarrow\boxed{|\theta|\lesssim.24495\,\mathrm{rad}=14.03^\circ}.This is the leading-order torque error, not the period error.

Physical check

The linear torque slightly overestimates the restoring torque because sin⁡θ<θ\sin\theta<\theta for small positive angles.