Period of an Oscillating Particle

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Homework Help Overview

The discussion revolves around determining the period of an oscillating particle of mass m in one dimension, using conservation of energy principles. The potential energy is defined with terms involving both quadratic and quartic components, and the original poster is seeking guidance on how to approach the problem, particularly regarding the integration needed to find the period.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • The original poster expresses uncertainty about how to start the problem and seeks direction. Some participants suggest examining the relationship between kinetic and potential energy, while others question whether a driving force is present in the system. There is also discussion about the interchangeability of the Hamiltonian with total energy.

Discussion Status

The discussion is ongoing, with participants exploring different interpretations of the problem and clarifying concepts related to energy in oscillations. Some guidance has been offered regarding the relationships between forces and energy, but no consensus has been reached on the specifics of the approach.

Contextual Notes

The original poster indicates this is their first post, and there may be uncertainties regarding the problem setup, particularly concerning the presence of a driving force in the oscillation.

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Homework Statement



A particle of mass m is oscillating with amplitude A in 1D (without damping). Using conservation of energy, I'm asked to determine the period T with the correct proportionality factor and period of integration.

Homework Equations



Potential energy: U(x) = a x^2 + b x^4 where a > 0 and b ≥ 0
Period: T(A) \propto∫\frac{dx}{\sqrt{E(A) + U(X)}} (from conservation of energy)

The Attempt at a Solution



I scribbled down a few attempts but none of them went anywhere. I don't have the slightest idea where to start so I'm hoping someone can point me in the right direction.

I think that's all the information provided, but feel free to ask if you have any questions. It's my first time posting here, my apologies if I haven't follow proper rules or etiquette.

Thanks
 
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Welcome to PF;
I take it the oscillations are harmonic and though undamped, there may be a driving force?
If it were SHM, then the potential energy terms would be quadratic right?

It looks like you are expected to exploit the relationship you already know about between kinetic and potential energy. i.e. you need to examine what else you know about energy in oscillations - which should net you an appropriate proportionality and a region of integration.

Compare with http://www.cscamm.umd.edu/people/faculty/tiglio/reviewch14-15.pdf.
 
That appears to be the case. I found some relevant relations while looking through the notes again.

F = -\frac{dU}{dx}

So that would give a driving force of

F = -2ax -4b x^3 = m\ddot{x}

The Hamiltonian is also given as

H = \frac{p^2}{2m} + U(x)

Would that be interchangeable with the total energy E(A)? In that case I would be able to integrate using just the kinetic energy.
 
Is the Hamiltonian interchangeable with the total energy?
Do you know the relationship between kinetic and potential energy for your oscillator?

Wouldn't F=-dU/dx be the restoring force rather than the "driving force"?
The problem statement only says that the oscillation is un-damped, does not say there is no driving force - I don't know, there may be: is there?
 

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