What is the Angular Acceleration for a Rotating Computer Disk Drive?

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Homework Help Overview

The problem involves a computer disk drive that starts from rest and has a constant angular acceleration. The original poster seeks to determine the time taken for the first complete revolution and the angular acceleration, given that the second complete revolution takes 0.690 seconds.

Discussion Character

  • Exploratory, Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • Participants discuss methods to find angular acceleration and the time for the first revolution, with some proposing quadratic equations to relate the times of the two revolutions. Questions arise regarding the setup of equations and the interpretation of variables.

Discussion Status

Multiple approaches have been presented, with some participants confirming the validity of certain equations while others express confusion about specific terms and their units. There is no explicit consensus on a single method, but productive dialogue is ongoing.

Contextual Notes

Participants are working under the constraints of the problem statement and are exploring the implications of the given time for the second revolution without additional information about initial conditions or values.

PirateFan308
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Homework Statement


A computer disk drive is turned on starting from rest and has constant angular acceleration.
If it took 0.690s for the drive to make its second complete revolution, how long did it take to make the first complete revolution?
What is the angular acceleration?

Homework Equations


w2 = w02+2\alpha∅

∅=w0t+(0.5)\alphat2

The Attempt at a Solution


I'm trying to first find the angular acceleration, and from there I can find out how long it took to make the first complete revolution.

First revolution:
w0=0 t=? \alpha=\alpha w=w ∅=2∏

Second revolution:
w0=w t=0.690s \alpha=\alpha ∅=2∏

Second revolution:

∅=w0t+(0.5)\alphat2
2∏ = w0(0.690)+(0.5)\alpha(0.690)2
\alpha=\frac{2∏-w0(0.69)}{(0.5)(0.69)^2}

First equation:
w2=w02+2\alpha(2∏)
(\frac{2∏-w0(0.69)}{(0.5)(0.69)^2})(\frac{2∏-w0(0.69)}{(0.5)(0.69)^2})=2\alpha(2∏)
I rearranged to get:
4∏2=\alpha((4∏(0.69)2)+(π(0.69)2)-((0.5)(0.69)2))
\alpha=5.45
 
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PirateFan308 said:
First revolution:
w0=0 t=? \alpha=\alpha w=w ∅=2∏

Second revolution:
w0=w t=0.690s \alpha=\alpha ∅=2∏

Second revolution:

∅=w0t+(0.5)\alphat2
2∏ = w0(0.690)+(0.5)\alpha(0.690)2
\alpha=\frac{2∏-w0(0.69)}{(0.5)(0.69)^2}

I agree up to this point.

First equation:
w2=w02+2\alpha(2∏)
(\frac{2∏-w0(0.69)}{(0.5)(0.69)^2})(\frac{2∏-w0(0.69)}{(0.5)(0.69)^2})=2\alpha(2∏)
I rearranged to get:
4∏2=\alpha((4∏(0.69)2)+(π(0.69)2)-((0.5)(0.69)2))
\alpha=5.45

Your "velocity-squared" equation is all right, and \omega_{0} = 0 . But doesn't that then lead to

\omega^{2} = 0^{2} + 4 \alpha \pi \Rightarrow \omega^{2} = 4 \pi \cdot \frac{2 \pi - \omega (0.69)}{(0.5)(0.69)^2} ,

with \omega being the angular speed at the start of the second revolution? (In fact, your expression in parentheses has units of rad/(sec2), so you can't mean to insert it into the first equation for \omega .)

(And I don't see a much tidier way of doing this, in view of the information given and the fact that there are two unknowns.)

BTW, don't forget to answer the first question about how long the first revolution took.
 
Last edited:
I figured out a couple of different ways to solve this. They both lead me to the same quadratic equation for t2/t1, where t1 is the time required for the first revolution, and t2 is the time required for the second revolution (which we know to be 0.69 s).

Method 1:

Angular displacement between t = 0 and t = t1:

\Delta \theta = \frac{1}{2}\alpha (\Delta t)^2 \Rightarrow 2 \pi = \frac{1}{2}\alpha t_1^2

\Rightarrow \alpha = \frac{4\pi}{t_1^2}

Angular displacement between t = 0 and t = t2:

4 \pi = \frac{1}{2}\alpha (t_1+t_2)^2

8 \pi = \frac{4\pi}{t_1^2} (t_1+t_2)^2

2 = \frac{t_1^2 + 2t_1t_2 + t_2^2}{t_1^2}

2 = 1 + 2\frac{t_2}{t_1} + \left(\frac{t_2}{t_1}\right)^2

Letting x = t2/t1, this becomes the quadratic equation:

x^2 + 2x - 1 = 0

which you can solve.

Method 2:

Angular displacement between t = 0 and t = t1:

\Delta \theta = \frac{1}{2}\alpha (\Delta t)^2 \Rightarrow 2 \pi = \frac{1}{2}\alpha t_1^2

\Rightarrow \alpha = \frac{4\pi}{t_1^2}

Angular displacement between t = t1 and t = t2:

2\pi = \omega_1 t_2 + \frac{1}{2}\alpha t_2^2

But \omega_1 (the speed at the end of the first revolution) is just \alpha t_1. Also, if you substitute in the expression for alpha, you get:

2\pi = 4\pi \frac{t_2}{t_1} + 2\pi \frac{t_2^2}{t_1^2}

1 = 2x + x^2

Same quadratic as before. Since you know t2 (it's given), once you solve for x, you have solved for t1. Discard the solution to the quadratic in which the ratio is negative.
 
Wow, thanks guys! That helped a lot!
 
One question, how did you format your equations so that they looked so much neater and easier to read?
 

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