Work and Rotational Kinetic Energy — Question 10

Section 10-9 · Physics pages 1550–1551

Question 10 Storage capacity limits how far regenerative braking can proceed A flywheel has inertia 2.0 kg m2 and initial angular speed 30 rad/s. A regenerative brake stores 75% of the removed kinetic energy; its storage device has 500 J of free capacity. Assume this is the only braking mechanism. flywheel brake −∆K storage: 75% heat: 25% The storage limit applies only to the recovered fraction of the energy removed from the flywheel. (a) Can it slow the flywheel to 10 rad/s without filling the device? (b) Find the angular speed when capacity is first reached and the energy dissipated by then.
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Question 10 - Solution Storage capacity limits how far regenerative braking can proceed flywheel brake −∆K storage: 75% heat: 25% (a) Derivation and calculation The desired kinetic-energy reduction and stored share are ∆Kremoved = 1 2(2)(302 −102) = 800 J. Estored = 0.75(800) = 600 J > 500 J. The target speed cannot be reached with uninterrupted regeneration into this storage device alone. (b) Result and interpretation At capacity, the removed and remaining energies are ∆Kcap = 500 0.75 = 2000 3 J, Kf = 900 −2000 3 = 700 3 J. ωcap = √ 2Kf I = √ 700/3 = 15.275 rad/s . Q = (1 −0.75)2000 3 = 500 3 = 166.67 J . Physical check The final kinetic energy, stored energy, and heat sum to 233.33 + 500 + 166.67 = 900 J.

Question 10

Storage capacity limits how far regenerative braking can proceed

A flywheel has inertia 2.0kgm22.0\,\mathrm{kg\,m^2} and initial angular speed 30rad/s30\,\mathrm{rad/s}. A regenerative brake stores 75%75\% of the removed kinetic energy; its storage device has 500J500\,\mathrm J of free capacity. Assume this is the only braking mechanism.

Diagram shown in the original SVG worksheet.

  1. Can it slow the flywheel to 10rad/s10\,\mathrm{rad/s} without filling the device?

  2. Find the angular speed when capacity is first reached and the energy dissipated by then.

Question 10 - Solution

Storage capacity limits how far regenerative braking can proceed

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

The desired kinetic-energy reduction and stored share are ΔKremoved=12(2)(302−102)=800J.\Delta K_{\mathrm{removed}}=\tfrac12(2)(30^2-10^2)=800\ \mathrm J. Estored=0.75(800)=600J>500J.\boxed{E_{\mathrm{stored}}=0.75(800)=600\ \mathrm J}>500\ \mathrm J. The target speed cannot be reached with uninterrupted regeneration into this storage device alone.

(b) Result and interpretation

At capacity, the removed and remaining energies are ΔKcap=5000.75=20003J,Kf=900−20003=7003J.\Delta K_{\mathrm{cap}}=\frac{500}{0.75}=\frac{2000}{3}\ \mathrm J,\qquad K_f=900-\frac{2000}{3}=\frac{700}{3}\ \mathrm J. ωcap=2KfI=700/3=15.275rad/s.\boxed{\omega_{\mathrm{cap}}=\sqrt{\frac{2K_f}{I}}=\sqrt{700/3}=15.275\ \mathrm{rad/s}}. Q=(1−0.75)20003=5003=166.67J.\boxed{Q=(1-0.75)\frac{2000}{3}=\frac{500}{3}=166.67\ \mathrm J}.

Physical check

The final kinetic energy, stored energy, and heat sum to 233.33+500+166.67=900233.33+500+166.67=900 J.