PHYSICS: Poschel-Teller Potential and Natural Frequency Derivation

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Homework Help Overview

The discussion revolves around deriving the natural frequency of small oscillations for a particle in a one-dimensional Poschel-Teller potential, described by the equation V(x) = -V_{0}sech^{2}(x/\lambda). Participants are exploring the implications of this potential on oscillatory motion.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • The original poster attempts to derive the angular frequency from the potential but expresses uncertainty about how to proceed. Some participants suggest using a Taylor series expansion around the minimum of the potential to identify the leading quadratic term, which relates to harmonic motion. There is also a question regarding the necessity of including higher-order terms in the expansion.

Discussion Status

The discussion is active, with participants providing guidance on how to approach the problem through graphical analysis and series expansion. There is acknowledgment of the need to verify the potential's characteristics before proceeding with the expansion. One participant indicates they have made progress but seeks clarification on the expansion's order.

Contextual Notes

Participants are navigating assumptions about the nature of the potential and its implications for oscillatory behavior. There is mention of the potential not being harmonic, which raises questions about the appropriate methods for analysis.

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Homework Statement



A particle of mass m moves in the one dimensional Poschel-Teller potential [tex]V(x)[/tex]. Find an expression for the natural frequency of small oscillations.

Homework Equations



[tex]V(x) = -V_{0}sech^{2}(x/\lambda)[/tex]

The Attempt at a Solution



I am making the uncertain assumption that this would be the angular frequency. But, I do not know how to derive it based on just the potential alone. I have tried to determine the period as well, graphically, but this function doesn't seem to be the type associated with normal periodic motion.
 
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The potential that you have is not a harmonic potential, however any potential that is an even function can be expanded in Taylor series about its minimum and will have a leading term that is quadratic in x. The words "small oscillations" is a hint that you need to make this expansion. First plot your potential to make sure that it has a minimum, then expand about x = 0. Ignore the constant, that's the "zero of energy". The leading term will be

[tex]\frac{1}{2}\;\frac{d^{2}V}{dx^{2}}\big|_{x=0}\;x^{2}[/tex]

That's a term that can be related to a harmonic potential of the form

[tex]\frac{1}{2}\;kx^{2}[/tex]

whose frequency you can easily extract from the effective spring constant k.
 
kuruman said:
The potential that you have is not a harmonic potential, however any potential that is an even function can be expanded in Taylor series about its minimum and will have a leading term that is quadratic in x. The words "small oscillations" is a hint that you need to make this expansion. First plot your potential to make sure that it has a minimum, then expand about x = 0. Ignore the constant, that's the "zero of energy". The leading term will be

[tex]\frac{1}{2}\;\frac{d^{2}V}{dx^{2}}\big|_{x=0}\;x^{2}[/tex]

That's a term that can be related to a harmonic potential of the form

[tex]\frac{1}{2}\;kx^{2}[/tex]

whose frequency you can easily extract from the effective spring constant k.

I figured it out. Thanks!

But just one tiny question, if the leading term is going to be a quadratic, then the original expansion has to be out to the fourth power?
 
Last edited:
I must not be doing something right, the whole thing went to zero.
 

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