Newton's Second Law in Angular Form — Question 9

Section 11-7 · Physics pages 1688–1689

Question 9 A small unmeasured torque gives a rigorous conservation tolerance Angular momentum initially has magnitude 10 kg m2/s. The net torque about a fixed origin has magnitude at most 0.030 N m for 20 s, with unknown time-dependent direction.⃗ Li⃗ Lf |∆⃗L| ≤.60 Allowed final-vector tips lie within a radius-.60 ball about the initial tip; a planar slice is shown. (a) Bound the change in the angular momentum vector. (b) Give a guaranteed interval for the final magnitude and explain whether the bound must be attained.
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Question 9 - Solution A small unmeasured torque gives a rigorous conservation tolerance⃗ Li⃗ Lf |∆⃗L| ≤.60 (a) Derivation and calculation The angular impulse and integral triangle inequality give ∆⃗L = ∫20 0⃗ τ(t) dt, |∆⃗L| ≤ ∫20 0 |⃗τ(t)| dt ≤(.030)(20). Thus |∆⃗L| ≤.600 kg m2/s . (b) Result and interpretation By the reverse and ordinary triangle inequalities, |Li| −|∆⃗L| ≤|Lf| ≤|Li| + |∆⃗L|. Therefore 9.40 ≤|Lf| ≤10.60 kg m2/s . This is a guaranteed bound, not a statistical uncertainty. Direction changes can cancel angular impulse; equality requires appropriately aligned torque throughout. Physical check Constant maximum torque parallel or antiparallel to the initial vector attains the two limiting magnitudes.

Question 9

A small unmeasured torque gives a rigorous conservation tolerance

Angular momentum initially has magnitude 10kgm2/s10\,\mathrm{kg\,m^2/s}. The net torque about a fixed origin has magnitude at most 0.030Nm0.030\,\mathrm{N\,m} for 20s20\,\mathrm s, with unknown time-dependent direction.

Diagram shown in the original SVG worksheet.

  1. Bound the change in the angular momentum vector.

  2. Give a guaranteed interval for the final magnitude and explain whether the bound must be attained.

Question 9 - Solution

A small unmeasured torque gives a rigorous conservation tolerance

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

The angular impulse and integral triangle inequality give ΔL→=∫020τ→(t)dt,\Delta\vec L=\int_0^{20}\vec\tau(t)\,dt, |ΔL→|≤∫020|τ→(t)|dt≤(.030)(20).|\Delta\vec L|\le\int_0^{20}|\vec\tau(t)|\,dt \le(.030)(20). Thus |ΔL→|≤.600kgm2/s.\boxed{|\Delta\vec L|\le.600\ \mathrm{kg\,m^2/s}}.

(b) Result and interpretation

By the reverse and ordinary triangle inequalities, |Li|−|ΔL→|≤|Lf|≤|Li|+|ΔL→|.|L_i|-|\Delta\vec L|\le|L_f|\le|L_i|+|\Delta\vec L|. Therefore 9.40≤|Lf|≤10.60kgm2/s.\boxed{9.40\le|L_f|\le10.60\ \mathrm{kg\,m^2/s}}. This is a guaranteed bound, not a statistical uncertainty. Direction changes can cancel angular impulse; equality requires appropriately aligned torque throughout.

Physical check

Constant maximum torque parallel or antiparallel to the initial vector attains the two limiting magnitudes.