Newton's Second Law in Angular Form — Question 3

Section 11-7 · Physics pages 1676–1677

Question 3 Signed torque area can reverse angular momentum before the pulse ends Initially Lz = −1 kg m2/s. About a fixed origin, τz = 2t N m for 0 ≤t < 2 s and τz = −1 N m for 2 ≤t ≤4 s. t τz 4 −1 2 4 Torque in N m; time in seconds. The jump has zero area. (a) Find final Lz and every zero of Lz during the pulse. (b) Explain why negative torque after 2 s does not immediately imply negative angular momentum.
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Question 3 - Solution Signed torque area can reverse angular momentum before the pulse ends t τz 4 −1 2 4 (a) Derivation and calculation Angular impulse determines the accumulated change. For 0 ≤t ≤2, Lz(t) = −1 + ∫t 0 2u du = −1 + t2. Therefore t = 1.00 s is a zero, and Lz(2) = 3. For 2 ≤t ≤4, Lz(t) = 3 + ∫t 2 (−1) du = 5 −t, Lz(4) = 1.00 kg m2/s . (b) Result and interpretation The second-interval formula would vanish at t = 5 s, outside the stated pulse. Thus the only zero is at 1 s. After 2 s, τz = −1 < 0, Lz = 5 −t > 0 (2 ≤t ≤4). Negative torque gives a negative slope of angular momentum, not necessarily a negative angular momentum. Physical check The positive angular impulse is 4 and the negative impulse is −2, giving net change +2 from the initial −1.

Question 3

Signed torque area can reverse angular momentum before the pulse ends

Initially Lz=−1kgm2/sL_z=-1\,\mathrm{kg\,m^2/s}. About a fixed origin, τz=2tNm\tau_z=2t\,\mathrm{N\,m} for 0≤t<2s0\le t<2\,\mathrm s and τz=−1Nm\tau_z=-1\,\mathrm{N\,m} for 2≤t≤4s2\le t\le4\,\mathrm s.

Diagram shown in the original SVG worksheet.

  1. Find final LzL_z and every zero of LzL_z during the pulse.

  2. Explain why negative torque after 2 s does not immediately imply negative angular momentum.

Question 3 - Solution

Signed torque area can reverse angular momentum before the pulse ends

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Angular impulse determines the accumulated change. For 0≤t≤20\le t\le2, Lz(t)=−1+∫0t2udu=−1+t2.L_z(t)=-1+\int_0^t2u\,du=-1+t^2. Therefore t=1.00s\boxed{t=1.00\ \mathrm s} is a zero, and Lz(2)=3L_z(2)=3. For 2≤t≤42\le t\le4, Lz(t)=3+∫2t(−1)du=5−t,L_z(t)=3+\int_2^t(-1)\,du=5-t, Lz(4)=1.00kgm2/s.\boxed{L_z(4)=1.00\ \mathrm{kg\,m^2/s}}.

(b) Result and interpretation

The second-interval formula would vanish at t=5t=5 s, outside the stated pulse. Thus the only zero is at 1 s. After 2 s, τz=−1<0,Lz=5−t>0(2≤t≤4).\tau_z=-1<0,\qquad L_z=5-t>0\quad(2\le t\le4). Negative torque gives a negative slope of angular momentum, not necessarily a negative angular momentum.

Physical check

The positive angular impulse is 4 and the negative impulse is −2-2, giving net change +2+2 from the initial −1-1.