Conservation of Mechanical Energy — Question 3

Section 8-4 · Physics pages 1076–1077

Question 3 Pendulum amplitude inferred from a bottom speed Neglect friction and air resistance, take g = 10 m/s2, and treat all stated guides as fixed. A 0.40 kg bob on a massless 1.5 m cord passes the bottom with speed √ 15 m/s. The pivot is fixed. L The bottom velocity is tangent; the second position illustrates a later part of the swing. (a) Find the maximum angle from downward vertical. (b) Find speed at an angle of 30◦. (c) Check that cord tension is positive at the turning point.
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Question 3 - Solution Pendulum amplitude inferred from a bottom speed L (a) Compare bottom kinetic energy with the height gain. The turning-point speed vanishes: 1 2mv2 0 = mgL(1 −cos θmax), 1 −cos θmax = 15 2(10)(1.5) = 1 2. θmax = 60◦. (b) Subtract the partial gravitational rise. At 30◦, v2 = 15 −30(1 −cos 30◦) = 15( √ 3 −1), v = √ 15( √ 3 −1) = 3.314 m/s . (c) Use the radial equation at zero speed. The radial equation toward the pivot is T −mg cos θ = mv2 L . At the turn, T = .40(10) cos 60◦= 2 N > 0 . Throughout |θ| ≤60◦, both terms in T = mv2/L + mg cos θ are nonnegative and the second is positive.

Question 3

Pendulum amplitude inferred from a bottom speed

Neglect friction and air resistance, take g=10g=10 m/s2^2, and treat all stated guides as fixed. A 0.40 kg bob on a massless 1.5 m cord passes the bottom with speed 15\sqrt{15} m/s. The pivot is fixed.

Diagram shown in the original SVG worksheet.

  1. Find the maximum angle from downward vertical.

  2. Find speed at an angle of 30∘30^\circ.

  3. Check that cord tension is positive at the turning point.

Question 3 - Solution

Pendulum amplitude inferred from a bottom speed

Diagram shown in the original SVG worksheet.

(a) Compare bottom kinetic energy with the height gain.

The turning-point speed vanishes: 12mv02=mgL(1−cos⁡θmax),1−cos⁡θmax=152(10)(1.5)=12.\tfrac12mv_0^2=mgL(1-\cos\theta_{\max}),\quad1-\cos\theta_{\max}=\frac{15}{2(10)(1.5)}=\frac12. θmax=60∘.\boxed{\theta_{\max}=60^\circ}.

(b) Subtract the partial gravitational rise.

At 30∘30^\circ, v2=15−30(1−cos⁡30∘)=15(3−1),v^2=15-30(1-\cos30^\circ)=15(\sqrt3-1), v=15(3−1)=3.314m/s.\boxed{v=\sqrt{15(\sqrt3-1)}=3.314\ \mathrm{m/s}}.

(c) Use the radial equation at zero speed.

The radial equation toward the pivot is T−mgcos⁡θ=mv2L.T-mg\cos\theta=\frac{mv^2}{L}. At the turn, T=.40(10)cos⁡60∘=2N>0\boxed{T=.40(10)\cos60^\circ=2\ \mathrm N>0}. Throughout |θ|≤60∘|\theta|\leq60^\circ, both terms in T=mv2/L+mgcos⁡θT=mv^2/L+mg\cos\theta are nonnegative and the second is positive.