Quote:
A flywheel with a radius of 0.454m starts from rest and accelerates with a constant angular acceleration of 0.500 rad/s2
Compute the magnitude of the tangential acceleration, the radial acceleration, and the resultant acceleration of a point on its rim after it has turned through 55.3∘
Seems easy enough.
a
z(t) = 0.500 s
-2v
z(t) = 0.500t + v
0z = 0.500t (starting from rest, so v
0z = 0)
s
z(t) = (1/2)0.500t
2 + s
0zWhere a
z(t), v
z(t), and s
z(t) are angular acceleration, angular velocity, and angular position respectively. We don't know s
0z, but it isn't relevant to the problem since we're dealing with a definite integral.
First we need to find t
n, the time when the flywheel has rotated through 55.3 degrees. So we have:
The integral from t
0 to t
n of v
z(t) = ~0.965 radians
0.250t
n2 - 0.250t
02 = 0.965
Since t
0 = 0, this reduces to:
0.250t
n2 = 0.965
t
n = 1.965s
Angular velocity at t=1.965 is thus:
v
z(1.965) = 0.500 * 1.965 = 0.982 s
-1Radial acceleration is just:
a
r = v
z2/r
Which gives us:
a
r = (0.982 s
-1)
2 / 0.454m = 2.126 ms
-2Tangential acceleration is:
a
t = a
z*r = 0.500 s
-2 * 0.454m = 0.227 ms
-2Total acceleration is:
a = a
t + a
r = 2.353 ms
-2According to MasteringPhysics, this answer is wrong.
Our textbook supplies a similarly derived equation:
v
z2=v
0z2+2a
z*Δθ
Plugging in the values from the problem gives me exactly the same value for v
r.
Also, the first part of this problem asked for a
t, a
r, and a at t
0. I answered 0.227, 0, and 0.227 respectively, which it marked as correct. Since angular acceleration is constant, tangential acceleration should also be. So I'm 99% sure that the problem is in my calculation of a{sub]r[/sub], but I can't figure out how it's wrong.
Edit: derped an equation. a
r=v
z2/r, not a
r=v
z2*r. It still doesn't like my answer, though.