21joanna12
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[Note from mentor: this thread originated in a non-homework forum, therefore it doesn't use the standard homework template]
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This exercise pops up in the Cavendish Quantum Mechanics Primer (M. Warner and A. Cheung) but I can't seem to figure it out. So far, when looking at the infinite square well of width a (and at this point in the book complex wavefunctions are not yet considered), the general form of the wave function is A_nsin(k_nx) where k_n=\frac{\sqrt{2mE}}{\hbar}=\frac{n\pi}{a}=\frac{2\pi}{\lambda}.
I am really at a loss here. I was thinking about \langle x^2 \rangle - \langle x\rangle but I don't know how to apply it here.
The answer should be a^2\left(\frac{1}{12}-\frac{1}{2\pi ^2n^2}\right)...
Thanks in advance!
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This exercise pops up in the Cavendish Quantum Mechanics Primer (M. Warner and A. Cheung) but I can't seem to figure it out. So far, when looking at the infinite square well of width a (and at this point in the book complex wavefunctions are not yet considered), the general form of the wave function is A_nsin(k_nx) where k_n=\frac{\sqrt{2mE}}{\hbar}=\frac{n\pi}{a}=\frac{2\pi}{\lambda}.
I am really at a loss here. I was thinking about \langle x^2 \rangle - \langle x\rangle but I don't know how to apply it here.
The answer should be a^2\left(\frac{1}{12}-\frac{1}{2\pi ^2n^2}\right)...
Thanks in advance!
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