Period of an Oscillating Particle

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SUMMARY

The discussion centers on determining the period T of an oscillating particle of mass m with amplitude A, utilizing conservation of energy principles. The potential energy is defined as U(x) = a x^2 + b x^4, where a > 0 and b ≥ 0. The period is expressed as T(A) ∝ ∫(dx/√(E(A) + U(X))). Participants emphasize the importance of understanding the relationship between kinetic and potential energy in oscillations, and the Hamiltonian H = p²/(2m) + U(x) is discussed as potentially interchangeable with total energy E(A).

PREREQUISITES
  • Understanding of classical mechanics, specifically oscillatory motion.
  • Familiarity with potential energy functions, particularly U(x) = a x^2 + b x^4.
  • Knowledge of conservation of energy principles in physics.
  • Basic understanding of Hamiltonian mechanics and its applications.
NEXT STEPS
  • Study the derivation of the period of simple harmonic motion (SHM) and its implications.
  • Explore the relationship between kinetic and potential energy in oscillatory systems.
  • Investigate the role of the Hamiltonian in classical mechanics and its application to energy conservation.
  • Review advanced topics in potential energy functions and their effects on oscillation periods.
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Students of physics, particularly those studying classical mechanics, as well as educators and anyone interested in understanding oscillatory motion and energy conservation principles.

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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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