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Hooke's law and angular freq. |
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| Aug19-05, 10:30 PM | #1 |
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Hooke's law and angular freq.
hmm ok, i was watching the MIT opencourseware video on oscillations and there was a part where it was mentioned that,
the diff. eq. [tex] x''+ \frac {k}{m} x = 0 [/tex] has solution [tex] x= x_0 cos (\omega t + \phi) [/tex] if and only if [tex]\omega= \sqrt{\frac {k}{m}} [/tex] how do i show that omega is the sqaureoot of k over m? thanks alot. |
| Aug19-05, 10:36 PM | #2 |
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Recognitions:
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Differentiate the solution twice with respect to time and substitute it back into the differential equation - then tell us what you discovered! :)
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| Aug19-05, 10:47 PM | #3 |
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ohhh, i see, it can be gotten by verifying the solution. I thought we needed to do something to hooke's law, but verifying the solution works great too.
: ) edit: a tinge of doubt crosses my mind though. When we solve the original differential equation, we get the solution in terms of k, m and x and no omega. While verifying the solution works when the solution is given, and we see that [tex]\omega= \sqrt{\frac {k}{m}} [/tex]. How do we know that [tex]\omega= \sqrt{\frac {k}{m}} [/tex] when we are solving it? |
| Aug19-05, 11:10 PM | #4 |
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Recognitions:
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Hooke's law and angular freq.
If you just substitute [itex]x = x_0 \cos(\omega t - \phi)[/itex] into the differential equation the required value of [itex]\omega[/itex] will jump out at you!
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| Aug19-05, 11:10 PM | #5 |
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| Aug21-05, 10:28 AM | #6 |
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try the following:
in your original ODE, consider [itex] \omega ^2[\itex] just as a mathematically sound way to express the positiveness of the factor [itex] \frac{k}{m} [\itex]. After all the calculations you will realize that this choice has proven itself useful and physically meaningful. |
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