knapklara said:
The difference between what and what ?
Google gets you
plenty places with angular motion formulas, but
some (this one on unform circular motion) are clearer than others. (
basics,
Wikipedia,
Hyperphysics, )
We can't attempt to write better textbooks here on PF, so you 'll have to search for something you like.
Once around a circle is ##2\pi## radians. If the motion is uniform (constant speed ##\vec v = \vec \omega \times \vec r\ ##), one revolution/second, you have ##\omega = 2\pi ## rad/s
It is confusing to write 'ω = 2π/t
0' (but correct if t
0 is the time for one revolution in uniform circular motion), and it is wrong to write 'ω = 2πv' --- check the dimensions (but ##\omega = 2\pi\nu## is again right for uniform circular motion; a subtle difference beteween ##v## (meter/s) and ##\nu## (1/s) ).
And 'ω = αt + v
0' is also wrong: v
0 has the wrong dimension. (again: ##\omega = \omega_0+\alpha t## is OK).In your exercise you have constant angular acceleration, so the angular analog for the SUVAT equation for linear motion with constant acceleration (
here ##s = v_it +{1\over 2} at^2 \ ##, and -- more complete --
here : ##x = x_0 + v_0 t + (1/2) a t^2## ) applies:
$$\theta = \theta_0 + \omega_0 t + {1\over 2} \alpha t^2 \tag 1$$and now we have to link that to the situation in your exercise.
'At one point' we can state that the angle at that point is ##\theta_0##.
'spins at circular frequency of 0.5 s-1' is supposed to give us ##\omega_0##
I have a problem there: The angular velocity can be 0.5 rad/s, or the frequency can be 0.5 Hz, i.e. half a revolution per second.
A little googling helps me out with my personal problem: the term
circular frequency a.k.a. angular frequency that I find confusing refers to omega.
So we can state ##\omega_0 = 0.5## rad/s.
Then: 'What angular velocity ω will he have after another 1.5 twist?' sets our ##\theta-\theta_0## in ##(1)## to ##3 \pi## radians.
That means we now have $$3\pi = \omega_0 t + {1\over 2} \alpha t^2 $$ which we can solve for ##t##.
Once we have ##t## the analog of ##v = v_0 + at\ ## helps us find the ##\omega(t)## the exercise wants.
And the ##v = \omega r ## gets the tangential velocity.
[edit] It took me some time to collect all this and type it up.
@kuruman was much faster, but perhaps the combination of the two replies is even better than each of them on its own
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