Conservation of Angular Momentum — Question 7

Section 11-10 · Physics pages 1744–1745

Question 7 After a tether is cut angular speed falls while angular momentum stays fixed A particle of mass m is at (R, 0) moving at (0, V ) when its tether is cut. No external force acts afterward. V R The released particle travels along the tangent. (a) Find its angular momentum about the original tether point for t > 0. (b) Find its polar angular speed and explain why it is not constant.
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Question 7 - Solution After a tether is cut angular speed falls while angular momentum stays fixed V R (a) Derivation and calculation After the cut the motion is force-free:⃗ r(t) = Rˆx + V tˆy,⃗ p = mV ˆy. Consequently,⃗ L =⃗r ×⃗p = mRV ˆz for all t > 0. (b) Result and interpretation The polar angular rate is ˙θ = x ˙y −y ˙x x2 + y2 = RV R2 + V 2t2 . Equivalently, mr2 ˙θ = m(R2 + V 2t2) RV R2 + V 2t2 = mRV. The distance from the origin grows, so the angular rate decreases even though angular momentum remains constant. Physical check The rate starts at V/R and approaches zero along the straight outgoing trajectory.

Question 7

After a tether is cut angular speed falls while angular momentum stays fixed

A particle of mass mm is at (R,0)(R,0) moving at (0,V)(0,V) when its tether is cut. No external force acts afterward.

Diagram shown in the original SVG worksheet.

  1. Find its angular momentum about the original tether point for t>0t>0.

  2. Find its polar angular speed and explain why it is not constant.

Question 7 - Solution

After a tether is cut angular speed falls while angular momentum stays fixed

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

After the cut the motion is force-free: r→(t)=Rx̂+Vtŷ,p→=mVŷ.\vec r(t)=R\hat x+Vt\hat y,\qquad\vec p=mV\hat y. Consequently, L→=r→×p→=mRVẑfor all t>0.\boxed{\vec L=\vec r\times\vec p=mRV\hat z}\quad\text{for all }t>0.

(b) Result and interpretation

The polar angular rate is θ̇=xẏ−yẋx2+y2=RVR2+V2t2.\dot\theta=\frac{x\dot y-y\dot x}{x^2+y^2} =\boxed{\frac{RV}{R^2+V^2t^2}}. Equivalently, mr2θ̇=m(R2+V2t2)RVR2+V2t2=mRV.mr^2\dot\theta=m(R^2+V^2t^2)\frac{RV}{R^2+V^2t^2}=mRV. The distance from the origin grows, so the angular rate decreases even though angular momentum remains constant.

Physical check

The rate starts at V/RV/R and approaches zero along the straight outgoing trajectory.