GR8677 #60
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Comments |
ernest21 2019-08-23 02:03:37 | I enjoyed reading your Solutions together with the answers of others. This is truly a great read for me. brick breaker 2 |  | a62 2016-09-20 02:36:59 | Easy, but even easier if you look at it this way: a is absolutely meaningless because the zero of potential is arbitrary. So it\'s exactly like the mass-on-a-spring model. |  | Almno10 2010-11-11 23:02:29 | Force is the negative gradient of potential energy. The a drops out.
psychonautQQ 2013-09-26 08:41:23 |
but this is asking for the frequency, how does force and frequency relate?
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|  | sirius 2008-11-05 22:26:45 | A similar solution if you remember . The given V(x) has a vertical shift, a, which can be ignored by shifting your zero-point energy. So, , solving for makes it depend on b and m.
This is enough, but the problem asks for frequency . So . making f depend on b and m. The answer then is (C).
alemsalem 2010-09-21 06:25:37 |
i totally agree, to be sure that it doesn't depend on a, just remember that shifting the potential energy by a constant cannot change the motion (classically) so it doesn't affect the frequency.
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$\int_0^\infty$ |
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$\partial$ |
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$\Rightarrow$ |
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$\ddot{x},\dot{x}$ |
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$\sqrt{z}$ |
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$\langle my \rangle$ |
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$\left( abacadabra \right)_{me}$ |
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$\vec{E}$ |
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$\frac{a}{b}$ |
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