Generalization of the bohr rule for harmonic oscillators

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Homework Help Overview

The discussion revolves around the generalization of the Bohr rule applied to harmonic oscillators, specifically focusing on expressing energy in terms of integrals. The original poster seeks to understand how to derive the energy spectrum for a one-dimensional harmonic oscillator using the provided integral condition.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the need to express energy as an integral and how to relate momentum to energy. Questions arise about isolating momentum and integrating it with respect to position. There is also confusion regarding the treatment of energy as a constant during integration.

Discussion Status

The discussion has seen participants providing guidance on how to express momentum as a function of position and energy. There is acknowledgment of the complexity involved in the integration process, and one participant indicates they have resolved their confusion.

Contextual Notes

Participants are navigating the constraints of expressing energy in terms of momentum and position while adhering to the conditions of the problem. There is mention of needing to integrate a potentially complicated expression, which adds to the challenge of the task.

uppiemurphy
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Homework Statement



The generalization of the bohr rule to periodic motion more general than circular orbit states that:
p.dr = nh = 2∏nh(bar).

the integral is a closed line integral and the bolded letters represent vectors.

Using the generalized, show that the spectrum for the one-dimensional harmonic oscillator, for which E = p2/2m + mw2x2/2 is E = nh(bar)w.

Homework Equations



2∏x = nλ, px = nh(bar)

The Attempt at a Solution



Basically I know how to get E = nh(bar)w for a harmonic oscillator without using integrals, but I'm confused as to how to express E as an integral which is what I assume they're asking for.

I know that the total energy of the system when the spring is fully stretched is Etot = mw2x2/2. Do I somehow have to write this in terms of momentum and then integrate? I'm probably missing something fairly obvious here, but how would I write that in terms of P?
 
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Hello, uppiemurphy.

It's not that you need to express E as an integral. Rather, you need to express the result of the integration ∫pdx in terms of E. The quantization of E will then come from the condition ∫pdx = nh.

To perform the integration ∫pdx you'll need to express p as a function of x for a specific energy E. Note E = KE + PE. See if you can express KE in terms of p and PE in terms of x. [Edit: I see that the expression for E in terms of p and x is already given in the problem. Use it to get p as a function of x so you can do the integration.]
 
Last edited:
I'm just confused as to what to do with E mainly... when I isolate my expression for p I'm left with p = sqrt(2mE-m^2w^2x^2) how do I integrate this when I have E in my expression for p?
 
E is just a constant of the motion. So, you have ## p = \sqrt{a-bx^2}## where a and b are constants.
 
I don't see how that integral would yield the correct answer at all though... You end up with a pretty complicated expression that is difficult to simplify
 
nevermind I got it! thank you for your help!
 

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