The Angular Momentum of a System of Particles — Question 10

Section 11-8 · Physics pages 1710–1711

Question 10 An open catcher must account for incoming angular momentum A stationary catcher at radius R = 0.50 m receives particles tangentially at speed u = 4 m/s counterclockwise. Mass arrives at rate ˙m = 0.20 kg/s and remains at rest in the catcher. Consider moments about the central fixed axis. C u R Particles enter tangentially and stop in the supported catcher. (a) Find the angular momentum inflow rate. (b) Find the external support torque required to keep the accumulated material at rest, neglecting other moments.
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Question 10 - Solution An open catcher must account for incoming angular momentum C u R (a) Derivation and calculation Each unit of incoming mass carries specific angular momentum ℓz = Ru = .50(4) = 2.00 m2/s. Multiplying by the arrival rate, ˙Lin = ˙mℓz = .20(2.00) = +.400 N m . (b) Result and interpretation For the catcher as an open system, dLstored dt = τext + ˙Lin. The accumulated material stays at rest, so τext = −˙Lin = −.400 N m . The support must remove the incoming angular momentum; a closed-system balance without the flux term would miss this torque. Physical check The clockwise support torque exactly balances the counterclockwise angular-momentum inflow.

Question 10

An open catcher must account for incoming angular momentum

A stationary catcher at radius R=0.50mR=0.50\,\mathrm m receives particles tangentially at speed u=4m/su=4\,\mathrm{m/s} counterclockwise. Mass arrives at rate ṁ=0.20kg/s\dot m=0.20\,\mathrm{kg/s} and remains at rest in the catcher. Consider moments about the central fixed axis.

Diagram shown in the original SVG worksheet.

  1. Find the angular momentum inflow rate.

  2. Find the external support torque required to keep the accumulated material at rest, neglecting other moments.

Question 10 - Solution

An open catcher must account for incoming angular momentum

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Each unit of incoming mass carries specific angular momentum ℓz=Ru=.50(4)=2.00m2/s.\ell_z=Ru=.50(4)=2.00\ \mathrm{m^2/s}. Multiplying by the arrival rate, L̇in=ṁℓz=.20(2.00)=+.400Nm.\boxed{\dot L_{\mathrm{in}}=\dot m\ell_z=.20(2.00)=+.400\ \mathrm{N\,m}}.

(b) Result and interpretation

For the catcher as an open system, dLstoreddt=τext+L̇in.\frac{dL_{\mathrm{stored}}}{dt}=\tau_{\mathrm{ext}}+\dot L_{\mathrm{in}}. The accumulated material stays at rest, so τext=−L̇in=−.400Nm.\boxed{\tau_{\mathrm{ext}}=-\dot L_{\mathrm{in}}=-.400\ \mathrm{N\,m}}. The support must remove the incoming angular momentum; a closed-system balance without the flux term would miss this torque.

Physical check

The clockwise support torque exactly balances the counterclockwise angular-momentum inflow.