Linear Momentum — Question 3

Section 9-3 · Physics pages 1196–1197

Question 3 Constant momentum magnitude still permits force A 0.20 kg bead moves at constant speed 5.0 m/s around a circle of radius 2.0 m. At the rightmost point it moves upward.⃗ v⃗ F O Schematic; labels, not drawing lengths, specify the data. (a) Find its momentum and net force vectors at that point using rightward +x and upward +y. (b) Find its momentum change over the next half revolution and explain why d|⃗p|/dt = 0 does not imply zero force.
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Question 3 - Solution Constant momentum magnitude still permits force⃗ v⃗ F O (a) Derivation and calculation At the rightmost point, velocity is upward and acceleration is inward:⃗ p = mvˆy = (0, 1.0) kg m/s .⃗ F = −mv2 R ˆx = −0.20(25) 2 ˆx = (−2.5, 0) N . (b) Result and interpretation After half a revolution the tangent reverses:⃗ pf = (0, −1), ∆⃗p =⃗pf −⃗pi = (0, −2) kg m/s . Although d|⃗p|/dt = 0, the vector derivative d⃗p/dt is nonzero. Force changes the direction of momentum. Physical check The inward force is perpendicular to velocity and therefore does no work.

Question 3

Constant momentum magnitude still permits force

A 0.20kg0.20\,\mathrm{kg} bead moves at constant speed 5.0m/s5.0\,\mathrm{m/s} around a circle of radius 2.0m2.0\,\mathrm m. At the rightmost point it moves upward.

Diagram shown in the original SVG worksheet.

  1. Find its momentum and net force vectors at that point using rightward +x+x and upward +y+y.

  2. Find its momentum change over the next half revolution and explain why d|p→|/dt=0d|\vec p|/dt=0 does not imply zero force.

Question 3 - Solution

Constant momentum magnitude still permits force

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

At the rightmost point, velocity is upward and acceleration is inward: p→=mvŷ=(0,1.0)kgm/s.\boxed{\vec p=mv\hat y=(0,1.0)\ \mathrm{kg\,m/s}}. F→=−mv2Rx̂=−0.20(25)2x̂=(−2.5,0)N.\boxed{\vec F=-\frac{mv^2}{R}\hat x=-\frac{0.20(25)}{2}\hat x=(-2.5,0)\ \mathrm N}.

(b) Result and interpretation

After half a revolution the tangent reverses: p→f=(0,−1),Δp→=p→f−p→i=(0,−2)kgm/s.\vec p_f=(0,-1),\qquad\boxed{\Delta\vec p=\vec p_f-\vec p_i=(0,-2)\ \mathrm{kg\,m/s}}. Although d|p→|/dt=0d|\vec p|/dt=0, the vector derivative dp→/dtd\vec p/dt is nonzero. Force changes the direction of momentum.

Physical check

The inward force is perpendicular to velocity and therefore does no work.