A rolling ball accelerates uniformly at .3 radians/second ^ 2. At a certain instant its angular velocity is 2 radians/second.
There is no simple way to reason this problem out. So we use the analog to the equation of uniformly accelerating linear motion which relates vf, v0, a and ds: vf ^ 2 = v0 ^ 2 + 2a (ds).
- `omegaf = `sqrt(`omega0^2 + 2 `alpha `dTheta) = +- `sqrt [( 2 rad/sec) ^ 2 + 2( .3 rad/sec ^ 2)( 11 rad)] = +- 3.255764 rad/sec.
From the initial and final angular velocities, we obtain
from which we can calculate the time required to rotate through 11 radians.
The result is `dt = ( 11 rad)/( 2.627882 rad/sec) = 4.185881 sec.
If we know
`ds, v0 and a we can use vf^2 = v0^2 + 2 a `ds to determine vf. We can then average vf and v0 to obtain vAve, which we use with `ds to determine `dt:
In the present example we know `d`theta, `omega0 and `alpha. So we can determine `omegaf, then `omegaAve. We then divide `d`theta by `omegaAve to find `dt:
Note that the reasoning is identical in the two situations.
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