In this section we are going to look at the case of rigid
bodies whose mass is spread over a definite area. The behaviour of rotating objects is of
considerable importance in our lives: the results of our considerations can be applied to
rotating car wheels, flywheels, the rotation of high divers and many other things.
A
rotating object has kinetic energy associated with it. Flywheels can be used to store
rotational kinetic energy; for example, current to energise the electromagnets of the proton
accelerator at the Rutherford laboratory in Oxfordshire is provided by a generator this driven
by a 5 m diameter flywheel; this allows pulses of electricity to be obtained without putting a
sudden large drain on the mains supply.
Rotational energy is also important in
stability, which is due to the angular momentum of the body (discussed below); many
washing machines have a disc of concrete fixed to the base of the drum to prevent vibrations
due to uneven loading with clothes.
If we think of a mass m on a string being swung
round in a circle of radius r (Figure 1) then its kinetic energy at any instant is given by:
Linear motion | Angular equivalent | |
Displacement (s) | Angular displacement (q) | |
Velocity (v) | Angular velocity (w) | |
Acceleration (a) | Angular acceleration (a) | |
Momentum = mu | Angular momentum = Iw | |
Kinetic energy = ½mv2 | Rotational kinetic energy = ½Iw2 | |
Force = ma | Torque = Ia | |
s = vt | q = wt | |
s = ut + ½at2 | q = qo + ½at2 | |
v2 = u2 + 2as | w12 = wo2 + 2aq | |
v = u + at | w1 = wo + at |