Problem 1:
A bicycle wheel starts off at rest. It is acted on by a constant
torque for a time of 15 seconds. During this time, the wheel makes
80 revolutions.
-
a) What is magnitude of the angular acceleration of the wheel?
-
b) Assume that the torque was created by a force
F = (6N i + 5N j) acting at a displacement
of r = (2m i - 3m j) from the axle of the wheel.
Calculate the torque vector.
-
c) Given the results from a) and b), what is the moment of inertia of
the bicycle wheel (about its axle)?
Solution:
- a) Constant torque implies constant angular acceleration. Therefore we can
use our =constant relations, and
thus we know that
the total angle turned through is given by
- = (1/2)t2
- since the initial angular velocity 0 = 0 .
- Thus we have
- = 2/t2
- We convert the number of revolutions into an angle:
- = (80 rev)(2 rad/rev)
= 160 rad
- thus
- = 2 (160
rad)/(15 s)2 = 4.47 rad/s2
- b) Apply the cross product:
- =
r x F = (2m i - 3m j) x (6N i + 5N j)
- = 10 N·m k + (-18 N·m) (-k)
- = 28 N·m k
- where we have used i x i = 0, i x j = +k,
j x i = -k, and j x j = 0.
- c) Now use = I
to get the moment of inertia:
- I =/
- = (28 N·m)/(4.47 rad/s2) = 6.27 Kg·m2
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