Newton's Second Law in Angular Form — Question 2

Section 11-7 · Physics pages 1674–1675

Question 2 A measured vector history identifies torque and its effect on magnitude Angular momentum about a fixed origin is⃗L(t) = (2t, 3t2, 4) in numerical SI units.⃗ L⃗ τ = ˙⃗L τ∥ˆL Only the instantaneous torque component along angular momentum changes its magnitude. (a) Find torque at t = 1 s. (b) Find the instantaneous rate of change of |⃗L| at that time.
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Question 2 - Solution A measured vector history identifies torque and its effect on magnitude⃗ L⃗ τ = ˙⃗L τ∥ˆL (a) Derivation and calculation Differentiate each component:⃗ L(t) = (2t, 3t2, 4) ⇒⃗τ(t) = (2, 6t, 0). Thus⃗ τ(1) = (2, 6, 0) N m ,⃗ L(1) = (2, 3, 4). (b) Result and interpretation Differentiate L2 =⃗L ·⃗L: 2L ˙L = 2⃗L ·⃗τ ⇒˙L =⃗L ·⃗τ L . At t = 1 s, ˙L = 2(2) + 3(6) + 4(0) √ 22 + 32 + 42 = 22 √ 29 = 4.085 N m . The perpendicular torque component changes direction rather than magnitude instantaneously. Physical check The magnitude-change rate is smaller than |⃗τ| = √ 40 N m because the torque is not parallel to⃗L.

Question 2

A measured vector history identifies torque and its effect on magnitude

Angular momentum about a fixed origin is L→(t)=(2t,3t2,4)\vec L(t)=(2t,3t^2,4) in numerical SI units.

Diagram shown in the original SVG worksheet.

  1. Find torque at t=1st=1\,\mathrm s.

  2. Find the instantaneous rate of change of |L→||\vec L| at that time.

Question 2 - Solution

A measured vector history identifies torque and its effect on magnitude

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Differentiate each component: L→(t)=(2t,3t2,4)⇒τ→(t)=(2,6t,0).\vec L(t)=(2t,3t^2,4)\Rightarrow\vec\tau(t)=(2,6t,0). Thus τ→(1)=(2,6,0)Nm,L→(1)=(2,3,4).\boxed{\vec\tau(1)=(2,6,0)\ \mathrm{N\,m}},\qquad\vec L(1)=(2,3,4).

(b) Result and interpretation

Differentiate L2=L→⋅L→L^2=\vec L\cdot\vec L: 2LL̇=2L→⋅τ→⇒L̇=L→⋅τ→L.2L\dot L=2\vec L\cdot\vec\tau\Rightarrow\dot L=\frac{\vec L\cdot\vec\tau}{L}. At t=1t=1 s, L̇=2(2)+3(6)+4(0)22+32+42=2229=4.085Nm.\boxed{\dot L=\frac{2(2)+3(6)+4(0)}{\sqrt{2^2+3^2+4^2}} =\frac{22}{\sqrt{29}}=4.085\ \mathrm{N\,m}}. The perpendicular torque component changes direction rather than magnitude instantaneously.

Physical check

The magnitude-change rate is smaller than |τ→|=40|\vec\tau|=\sqrt{40} N m because the torque is not parallel to L→\vec L.