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Infinite Square Well |
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| Feb2-06, 03:38 AM | #1 |
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Mentor
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Infinite Square Well
I need a little help with the strategy on this question. My work is below the problem description.
A particle of mass m is in an infinite square well of width a (it goes from x = 0 to x = a). The eigenfunctions of the Hamiltonian are known to be: [tex] \psi_{n}(x) = \sqrt{\frac{2}{a}} \sin\left(\frac{n \pi}{a}x}\right) [/tex] The corresponding eigenvalues are: [tex] E_n = \frac{\hbar^2 n^2 \pi^2}{2ma^2} [/tex] At time t = 0, the particle has wave function [itex] \Psi(x,0) = Ax(a-x) [/itex] where [itex] A = (30/a^5)^{1/2} [/itex]. a) [itex] \Psi(x,0) [/itex] can be written as a linear combination of the eigenfunctions of the Hamiltonian. Let us use the symbol cn to denote the expansion coefficients. Obtain a general expression for the cn in terms of [itex] \pi [/itex]. Here is my work so far. Based on what we know of Fourier series, [tex] c_n = \int{\psi_n^*(x) \Psi(x,0)\, dx} = \sqrt\frac{2}{a}}\sqrt\frac{30}{a^5}} \int_0^a{\sin\left(\frac{n \pi}{a}x}\right)(ax - x^2)\, dx} [/tex] [tex] = \sqrt\frac{60}{a^4}} \int_0^a{x\sin\left(\frac{n \pi}{a}x}\right)\, dx}\, - \, \sqrt\frac{60}{a^6}} \int_0^a{x^2\sin\left(\frac{n \pi}{a}x}\right)\, dx} [/tex] ...and now I have to integrate by parts. Is this the correct method? The reason I hesitate is that it looks like the final answer will not be only in terms of pi. There will still be some a's left, surely! Yet, the next part asks me to calculate c1, c2, and c3 to seven significant figures! This isn't looking good...I must be missing something. |
| Feb2-06, 07:28 AM | #2 |
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Recognitions:
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Change the integration variable to z=ax. Then the constant a will drop out.
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| Feb3-06, 09:21 PM | #3 |
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Hope this helps Pat |
| Feb4-06, 06:16 AM | #4 |
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Infinite Square Well
You're right. I should have said z=x/a.
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| Feb5-06, 04:01 AM | #5 |
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Mentor
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I integrated without changing any variables and found that the a's did indeed drop out. Thanks for your help. I just needed to keep going on this question.
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