Classical Perturbation Theory-Time Dep. vs. Time Indep (Goldstein).

In summary, Classical Perturbation Theory is a mathematical framework used to study systems that can be approximated as a small deviation from a simpler system. It is commonly used in physics and engineering for complex systems. There are two types: Time Dependent and Time Independent, with Time Dependent being used for varying systems and Time Independent for constant systems. Goldstein's perturbation parameter is a small quantity used to quantify the deviation of the system from the unperturbed system, allowing for a systematic approach to solving the perturbed system. It is a classical approximation to quantum mechanics and has limitations such as only being applicable to small perturbations and not considering quantum effects.
  • #1
Bosh
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Classical Perturbation Theory--Time Dep. vs. Time Indep (Goldstein).

Hi,

I'm going through Goldstein, and I'm a little confused on the distinction between time dependent and time independent perturbation theory. In section 12.2, they do the case of a simple harmonic perturbation on force free motion. I would have thought that the perturbation [itex]\Delta H = \frac{m\omega^2 x^2}{2}[/itex] would not be considered time-dependent. Is the key that when you plug in the unperturbed solution for x, i.e., [itex]\frac{\alpha t}{m} + \beta[/itex], the perturbation hamiltonian is now time-dependent?

If so, it would seem that the example they treat in the section on time-independent perturbation theory, the anharmonic oscillator with [itex]\Delta H = \frac{\epsilon m^2 \omega_0^2 q^3}{q_0}[/itex], could also have been treated as a time-dependent problem.

Any insight would be appreciated! Thanks!

Dan
 
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  • #2


Dear Dan,

Thank you for your question regarding the distinction between time dependent and time independent perturbation theory. I can understand your confusion, as the two cases may seem similar at first glance.

The key difference between the two is in the nature of the perturbation itself. In time dependent perturbation theory, the perturbation term is explicitly time dependent, as in your example of \frac{m\omega^2 x^2}{2}. This means that the perturbation is changing with time and cannot be separated from the time variable. As you correctly noted, when the unperturbed solution is plugged in for x, the perturbation Hamiltonian becomes time dependent.

On the other hand, in time independent perturbation theory, the perturbation term is not explicitly time dependent. This means that the perturbation can be separated from the time variable, as in the case of the anharmonic oscillator with \frac{\epsilon m^2 \omega_0^2 q^3}{q_0}. This allows for the use of the time-independent perturbation theory approach, which is often simpler and more straightforward than time-dependent perturbation theory.

In summary, the key distinction between time dependent and time independent perturbation theory lies in the nature of the perturbation term itself. I hope this helps clarify the difference between the two cases. Please let me know if you have any further questions.


 

1. What is Classical Perturbation Theory?

Classical Perturbation Theory is a mathematical framework used to study systems in which the behavior of the system can be approximated as a small deviation from a simpler, more easily solvable system. It is commonly used in physics and engineering to analyze systems that are too complex to solve directly.

2. What is the difference between Time Dependent and Time Independent Classical Perturbation Theory?

Time Dependent Classical Perturbation Theory is used to study systems that vary with time, while Time Independent Classical Perturbation Theory is used to study systems that do not vary with time. In Time Dependent Classical Perturbation Theory, the perturbation is a function of time, while in Time Independent Classical Perturbation Theory, the perturbation is a constant.

3. What is the role of Goldstein's perturbation parameter in Classical Perturbation Theory?

Goldstein's perturbation parameter is a small quantity that is used to quantify the deviation of the system from the unperturbed system. It is typically denoted by epsilon (ε) and is used to expand the equations of motion and other relevant quantities in a series of powers of ε. This allows for a systematic approach to solving the perturbed system.

4. How does Classical Perturbation Theory relate to quantum mechanics?

Classical Perturbation Theory is a classical approximation to quantum mechanics. It is used to study systems that are too complex to solve using traditional quantum mechanical methods. By applying perturbation theory to the classical equations of motion, we can obtain approximate solutions that are in good agreement with quantum mechanical results.

5. What are the limitations of Classical Perturbation Theory?

Classical Perturbation Theory is only applicable to systems that can be approximated as a small deviation from a simpler system. It also assumes that the perturbation is small, and the system is near equilibrium. In addition, it does not take into account quantum effects, so it is not suitable for systems that exhibit quantum behavior. Finally, it is a perturbative method, so it may not provide accurate results for large perturbations.

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