Work Done by the Gravitational Force — Question 5

Section 7-5 · Physics pages 940–941

Question 5 A fixed pendulum support does no work while gravity changes speed Take a uniform gravitational field with g = 10 m/s2, upward y positive, and neglect air resistance. A 0.50 kg bob hangs from a massless inextensible cord of length 2 m at a fixed pivot. It is released from rest with the cord 60◦from vertical. The cord remains taut. 2 m vertical Release is 60 degrees from the downward vertical; both bob positions lie on the same circle. (a) Find the vertical drop to the lowest point and gravity work. (b) Find speed at the lowest point and explain why tension does no work. (c) Find tension at the lowest point using the radial acceleration.
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Question 5 - Solution A fixed pendulum support does no work while gravity changes speed 2 m vertical (a) Use the pendulum geometry. The governing relation is h = L −L cos θ, Wg = mgh h = L(1 −cos 60◦) = 1 m, so Wg = mgh = 5 J. (b) Apply the work theorem. Tension is radial and displacement tangent to the fixed circle, so its work is zero. Thus 1 2(0.50)v2 = 5, giving v = √ 20 = 2 √ 5 m/s. (c) Include the inward acceleration. At the bottom, T −mg = mv2/L. Hence T = 5 + 0.50(20)/2 = 10 N, larger than weight even though tension did no work.

Question 5

A fixed pendulum support does no work while gravity changes speed

Take a uniform gravitational field with g=10g=10 m/s2^2, upward y positive, and neglect air resistance. A 0.50 kg bob hangs from a massless inextensible cord of length 2 m at a fixed pivot. It is released from rest with the cord 60∘60^\circ from vertical. The cord remains taut.

Diagram shown in the original SVG worksheet.

  1. Find the vertical drop to the lowest point and gravity work.

  2. Find speed at the lowest point and explain why tension does no work.

  3. Find tension at the lowest point using the radial acceleration.

Question 5 - Solution

A fixed pendulum support does no work while gravity changes speed

Diagram shown in the original SVG worksheet.

(a) Use the pendulum geometry.

The governing relation is h=L−Lcos⁡θ,Wg=mgh\boxed{h=L-L\cos\theta,\qquad W_g=mgh}

h=L(1−cos⁡60∘)=1m,h=L(1-\cos60^\circ)=1\ \mathrm m, so Wg=mgh=5J.W_g=mgh=5\ \mathrm J.

(b) Apply the work theorem.

Tension is radial and displacement tangent to the fixed circle, so its work is zero. Thus 12(0.50)v2=5,\tfrac12(0.50)v^2=5, giving v=20=25m/s.v=\sqrt{20}=2\sqrt5\ \mathrm{m/s}.

(c) Include the inward acceleration.

At the bottom, T−mg=mv2/L.T-mg=mv^2/L. Hence T=5+0.50(20)/2=10N,T=5+0.50(20)/2=10\ \mathrm N, larger than weight even though tension did no work.