183_notes:examples:rotational_kinetic_energy_and_work

This is an old revision of the document!


In the figure which is in the representations section you observe that a wheel is mounted on a stationary axel, which is nearly frictionless so that the wheel turns freely. The wheel has an inner ring with mass 5 kg and radius 10 cm and an outer ring with mass 2 kg and radius 25 cm; the spokes have negligible mass. A string with negligible mass is wrapped around the outer ring and you pull on it, increasing the rotational speed of the wheel. During the time that the wheel's rotation changes from 4 revolutions per second to 7 revolutions per second, how much work do you do?

Facts

Assumptions and Approximations

Lacking

Representations

System: Wheel and string

Surroundings: Your hand, axle, Earth

Solution

From the Energy Principle:

$E_{f} = E{i} + W$

$\frac{1}{2}I\omega^{2}_{f} = \frac{1}{2}I\omega^{2}_{i} + W$

$W = \frac{1}{2}I(\omega^{2}_{f} - \omega^{2}_{i})$

What is the moment of inertia $I = m_{1}r^{2}_{\perp1}$ + $m_{2}r^{2}_{\perp2}$ + $m_{3}r^{3}_{\perp3}$ + $m_{4}r^{4}_{\perp4} + \cdot \cdot \cdot$ ? Group this sum into a part that includes just the atoms of the inner ring and another part that includes just the atoms of the outer ring:

$I = (m_{1}r^{2}_{\perp1}$ + $m_{2}r^{2}_{\perp2}$ + $\cdot \cdot \cdot)_{inner}$ + $(m_{1}r^{2}_{\perp1}$ + $m_{2}r^{2}_{\perp2})_{outer}$ + $\cdot \cdot \cdot$

$I = I_{inner} + I_{outer}$

This is a general result: The moment of inertia of a composite object is the sum of the moments of inertia of the individual pieces, because we have to add up all the contributions of all the atoms. We already determined that the moment of inertia of a ring is $MR^{2}$ (all the atoms are at the same perpendicular distance R from the center), so the moment of inertia of this wheel is:

$I = M_{inner}R^{2}_{inner} + M_{outer}R^{2}_{outer}$

$I = (5kg)(.1m)^2$ + $(2 kg)(.25 m)^2$ = $(0.050 + 0.125) kg \cdot m^2 = 0.175 kg \cdot m^2$

We need to convert revolutions per second into radians per second:

$\omega_{i} = (4\frac{rev}{s})(\frac{2\pi\;radians}{rev}) = 25.1 \;radian\;s/s$

$\omega_{f} = (7\frac{rev}{s})(\frac{2\pi\;radians}{rev}) = 44.0 \;radian\;s/s$

You, the Earth, and the axle will exert forces on the system. How much work does the Earth do? Zero, because the center of mass of the wheel doesn't move. How much work does the axle do? If there is negligible friction between the axle and the wheel, the axle does no work, because there is no-displacement of the axle's force. Therefore only you do work, and the work that you do is

$W = \frac{1}{2}(0.175 kg \cdot m^{2})(44.0^2 = 25.1^2)\frac{radians^2}{s^2} = 114J$

  • 183_notes/examples/rotational_kinetic_energy_and_work.1414790504.txt.gz
  • Last modified: 2014/10/31 21:21
  • by pwirving