Conservation of Angular Momentum — Question 1

Section 11-10 · Physics pages 1732–1733

Question 1 Pulling inward conserves angular momentum while increasing energy A skater initially has inertia 4.0 kg m2 and angular speed 2.0 rad/s. By pulling inward, the skater reduces inertia to 1.6 kg m2. External torque is negligible. inward mass redistribution Pulling mass toward the spin axis reduces inertia while external torque is negligible. (a) Find final angular speed. (b) Find the change in rotational energy and identify its source.
Show solutionHide solution
Question 1 - Solution Pulling inward conserves angular momentum while increasing energy inward mass redistribution (a) Derivation and calculation Negligible external angular impulse gives L = Iiωi = 4.0(2.0) = 8.00 kg m2/s = Ifωf. Thus ωf = Iiωi If = 8 1.6 = 5.00 rad/s . (b) Result and interpretation The rotational energies are Ki = 1 2(4)(2)2 = 8.00 J, Kf = 1 2(1.6)(5)2 = 20.0 J. Therefore ∆K = 20 −8 = 12.0 J . Internal muscular work supplies this increase. Fixed angular momentum implies K = L2/(2I), so reducing inertia raises rotational energy. Physical check The final momentum 1.6(5) = 8 is unchanged even though the rotational energy increases.

Question 1

Pulling inward conserves angular momentum while increasing energy

A skater initially has inertia 4.0kgm24.0\,\mathrm{kg\,m^2} and angular speed 2.0rad/s2.0\,\mathrm{rad/s}. By pulling inward, the skater reduces inertia to 1.6kgm21.6\,\mathrm{kg\,m^2}. External torque is negligible.

Diagram shown in the original SVG worksheet.

  1. Find final angular speed.

  2. Find the change in rotational energy and identify its source.

Question 1 - Solution

Pulling inward conserves angular momentum while increasing energy

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Negligible external angular impulse gives L=Iiωi=4.0(2.0)=8.00kgm2/s=Ifωf.L=I_i\omega_i=4.0(2.0)=8.00\ \mathrm{kg\,m^2/s}=I_f\omega_f. Thus ωf=IiωiIf=81.6=5.00rad/s.\boxed{\omega_f=\frac{I_i\omega_i}{I_f}=\frac8{1.6}=5.00\ \mathrm{rad/s}}.

(b) Result and interpretation

The rotational energies are Ki=12(4)(2)2=8.00J,Kf=12(1.6)(5)2=20.0J.K_i=\tfrac12(4)(2)^2=8.00\ \mathrm J,\qquad K_f=\tfrac12(1.6)(5)^2=20.0\ \mathrm J. Therefore ΔK=20−8=12.0J.\boxed{\Delta K=20-8=12.0\ \mathrm J}. Internal muscular work supplies this increase. Fixed angular momentum implies K=L2/(2I)K=L^2/(2I), so reducing inertia raises rotational energy.

Physical check

The final momentum 1.6(5)=81.6(5)=8 is unchanged even though the rotational energy increases.