Perturbation Techniques and Theory for Nonlinear Systems

In summary, vela suggests using a simplified ODE to approximate the solution to the original equation. Ali Hasan Nayfeh's Introduction to Perturbation Techniques has information on how to do this.
  • #1
sharrington3
7
0

Homework Statement


Given the equation
[tex] \ddot{\theta}=\Omega^2\sin{\theta}\cos{\theta}-\frac{g}{R}\sin{\theta} [/tex]
Determine a first-order uniform expansion for small but finite theta.

Homework Equations


Other than the equation above, none so far as I am aware.


The Attempt at a Solution


The only thing I could think to do was try to solve this differential equation via the method of undetermined coefficients, which I do not think is right at all. I then planned to expand my solution in a Taylor series about 0. This is from Ali Hasan Nayfeh's Introduction to Perturbation Techniques. My professor gave us a packet of the fourth chapter of the aforementioned text as a basis to solve this and other problems. Nowhere in the text does it give a clear example of what exactly a "first order uniform expansion" is, nor do I even know where to begin. My professor's research interests lie in nonlinear dynamics and chaos, and I fear he is going a little too in depth for my second year physics course. Thank you for any input.
 
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  • #2
I'm only making an educated guess here, but I think what you want to do is expand the trig functions using the Taylor series and retain only the lowest-order non-vanishing term. This will leave you with a linear second-order differential equation. Then you want to convert this second-order equation into a system of two first-order equations.
 
  • #3
I think that finding the solution to the original ODE and then expand it using Taylor series is equivalent to solve the "simplified" ODE that vela suggests. Vela's way is much easier for sure.
 
  • #4
That's something along the lines of what I thought of doing. I read up on the subject, and "uniform expansion" only means "without secular terms", so the approximation of my system won't blow up as t→∞. I'm just going to do the Taylor series DE thing. Thanks for your input, guys. It's greatly appreciated.
 
  • #5


I would like to provide a response to the above content by explaining the concept of perturbation techniques and theory for nonlinear systems and how it applies to the given homework statement.

Perturbation techniques and theory are methods used to approximate solutions for nonlinear systems, where the equations cannot be solved analytically. These methods involve expanding the solution in a series of small parameter, typically denoted as ε, and then solving the equations order by order. This allows us to obtain an approximate solution that is valid for small values of the parameter ε.

In the given homework statement, we have a nonlinear system described by the equation \ddot{\theta}=\Omega^2\sin{\theta}\cos{\theta}-\frac{g}{R}\sin{\theta}. To apply perturbation techniques, we can introduce a small parameter ε and write the equation as \ddot{\theta}=\epsilon f(\theta), where f(\theta)=\Omega^2\sin{\theta}\cos{\theta}-\frac{g}{R}\sin{\theta}. Now, we can solve this equation order by order in ε to obtain an approximate solution for small values of ε.

A first-order uniform expansion refers to expanding the solution in a Taylor series about the point \theta=0, where ε is also assumed to be small. This means that we can write the solution as \theta(\epsilon)=a_0+a_1\epsilon+a_2\epsilon^2+..., where a_0, a_1, a_2, etc. are constants that can be determined by substituting this series into the original equation and equating coefficients of ε to zero.

In summary, the approach to solving this problem using perturbation techniques would involve introducing a small parameter ε, rewriting the equation in terms of this parameter, and then expanding the solution in a Taylor series about \theta=0. The resulting series can then be used to obtain an approximate solution for small values of ε. I would recommend consulting your professor or a textbook on perturbation techniques for further guidance and examples.
 

Related to Perturbation Techniques and Theory for Nonlinear Systems

1. What are perturbation techniques and theory for nonlinear systems?

Perturbation techniques and theory for nonlinear systems are mathematical tools used to approximate the solution of a nonlinear system by breaking it down into simpler, linear components. This approach is often used when the nonlinear system is too complex to be solved analytically.

2. What are the advantages of using perturbation techniques and theory?

The main advantage of using perturbation techniques and theory is that they can provide an approximate solution to a nonlinear system that would otherwise be too difficult or impossible to solve. These techniques can also help to better understand the behavior of a nonlinear system and identify critical parameters that affect its stability.

3. What types of nonlinear systems can be analyzed using perturbation techniques and theory?

Perturbation techniques and theory can be applied to a wide range of nonlinear systems, including differential equations, difference equations, and integral equations. These techniques are also used in various fields such as physics, engineering, and biology.

4. What are some common perturbation techniques used in nonlinear systems?

Some common perturbation techniques used in nonlinear systems include the method of multiple scales, Lindstedt-Poincaré method, and the method of averaging. These techniques involve expanding the solution of a nonlinear system in terms of a small parameter and then solving the resulting series of equations.

5. How accurate are the results obtained from perturbation techniques and theory?

The accuracy of the results obtained from perturbation techniques and theory depends on the complexity of the nonlinear system and the chosen perturbation method. In general, these techniques provide a good approximation of the solution for small perturbations, but their accuracy decreases as the perturbation parameter becomes larger.

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