Newton's Second Law in Angular Form — Question 10

Section 11-7 · Physics pages 1690–1691

Question 10 Trajectory curvature reconstructs torque without a force diagram A 2 kg particle follows x = t, y = t2, z = 0 in numerical SI units relative to a fixed origin. x y Parabolic path y = x2 in numerical SI coordinates. (a) Find Lz(t) and infer torque by differentiation. (b) Independently calculate force from acceleration and verify the torque.
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Question 10 - Solution Trajectory curvature reconstructs torque without a force diagram x y (a) Derivation and calculation Differentiate the trajectory to find⃗v = (1, 2t, 0). Then Lz = m(xvy −yvx) = 2[t(2t) −t2(1)] = 2t2 kg m2/s , τz = dLz/dt = 4t N m . (b) Result and interpretation Independently, the acceleration and force are⃗ a = (0, 2, 0),⃗ F = m⃗a = (0, 4, 0) N. Their moment about the same fixed origin is (⃗r ×⃗F)z = t(4) −t2(0) = 4t N m . The force calculation agrees with the angular-momentum derivative. Physical check Both methods use the same position origin and inertial momentum, as the torque law requires.

Question 10

Trajectory curvature reconstructs torque without a force diagram

A 2kg2\,\mathrm{kg} particle follows x=tx=t, y=t2y=t^2, z=0z=0 in numerical SI units relative to a fixed origin.

Diagram shown in the original SVG worksheet.

  1. Find Lz(t)L_z(t) and infer torque by differentiation.

  2. Independently calculate force from acceleration and verify the torque.

Question 10 - Solution

Trajectory curvature reconstructs torque without a force diagram

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Differentiate the trajectory to find v→=(1,2t,0)\vec v=(1,2t,0). Then Lz=m(xvy−yvx)=2[t(2t)−t2(1)]=2t2kgm2/s,L_z=m(xv_y-yv_x)=2[t(2t)-t^2(1)] =\boxed{2t^2\ \mathrm{kg\,m^2/s}}, τz=dLz/dt=4tNm.\boxed{\tau_z=dL_z/dt=4t\ \mathrm{N\,m}}.

(b) Result and interpretation

Independently, the acceleration and force are a→=(0,2,0),F→=ma→=(0,4,0)N.\vec a=(0,2,0),\qquad\vec F=m\vec a=(0,4,0)\ \mathrm N. Their moment about the same fixed origin is (r→×F→)z=t(4)−t2(0)=4tNm.\boxed{(\vec r\times\vec F)_z=t(4)-t^2(0)=4t\ \mathrm{N\,m}}. The force calculation agrees with the angular-momentum derivative.

Physical check

Both methods use the same position origin and inertial momentum, as the torque law requires.