How Do You Determine Normal Mode Frequencies in a Coupled Oscillator System?

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Homework Help Overview

The discussion revolves around determining the normal mode frequencies in a coupled oscillator system described by a Lagrangian involving two degrees of freedom, x and y. The problem involves applying the Euler-Lagrange equation to derive equations of motion for both coordinates.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the application of the Euler-Lagrange equation to derive motion equations for x and y. There are questions about the clarity of the approach and whether the derived equations lead to the correct form for finding frequencies.

Discussion Status

Some participants have provided guidance on formatting equations for clarity and suggested checking the correctness of the derived equations. There is an ongoing exploration of the implications of the equations and whether the approach will yield separate frequencies for x and y.

Contextual Notes

Participants note potential issues with the original equations and the need for proper formatting in LaTeX. There is also a mention of a possible factor of 2 in the Lagrangian that may need to be addressed.

Yosty22
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Homework Statement



We have a particle of mass m moving in a plane described by the following Lagrangian:
\frac{1}{2}m((\dot{x}^2)+(\dot{y}^2)+2(\alpha)(\dot{x})(\dot{y}))-\frac{1}{2}k(x^2+y^2+(\beta)xy) for k>0 is a spring constant and \alpha and \beta are time-independent.

Find the normal mode frequencies, \omega_1,2

Homework Equations



Euler-Lagrange Equation

The Attempt at a Solution



I think I'm just missing here. There was a lot of math, so I won't explicitly write out all of it, but I will have my final answers. I used the Euler-Lagrange Equation twice: once for x, once for y. This yielded:

m*ddot{x}+m\alpha(\ddot{y}=-kx+\beta(y)
and
m*\ddot{y}+m\alpha(\ddot{x}=-ky+\beta(x)

I solved each for \ddot{x} and equated them, giving me:

\ddot{y} = \frac{\beta+k/(\alpha)}{m(\alpha-1/(\alpha))}*y + \frac{-k-\beta/(\alpha)}{m(\alpha-1/(\alpha))}*x

Am I approaching this the right way to find the frequencies? I know usually in 1D for example, you solve the Euler-Lagrange equation to yield something of the form: \ddot{x}=\omega^2*x, but it is a little more unclear to me as to what to do here. Would I find two separate frequencies, once in x and once in y and they are two separate answers?
 
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Update: I should probably transform to coordinates like (r,theta) and find theta dot, right?
 
Yosty22 said:

Homework Statement



We have a particle of mass m moving in a plane described by the following Lagrangian:
\frac{1}{2}m((\dot{x}^2)+(\dot{y}^2)+2(\alpha)(\dot{x})(\dot{y}))-\frac{1}{2}k(x^2+y^2+(\beta)xy) for k>0 is a spring constant and \alpha and \beta are time-independent.

Find the normal mode frequencies, \omega_1,2

Homework Equations



Euler-Lagrange Equation

The Attempt at a Solution



I think I'm just missing here. There was a lot of math, so I won't explicitly write out all of it, but I will have my final answers. I used the Euler-Lagrange Equation twice: once for x, once for y. This yielded:

m*ddot{x}+m\alpha(\ddot{y}=-kx+\beta(y)
and
m*\ddot{y}+m\alpha(\ddot{x}=-ky+\beta(x)

I solved each for \ddot{x} and equated them, giving me:

\ddot{y} = \frac{\beta+k/(\alpha)}{m(\alpha-1/(\alpha))}*y + \frac{-k-\beta/(\alpha)}{m(\alpha-1/(\alpha))}*x

Am I approaching this the right way to find the frequencies? I know usually in 1D for example, you solve the Euler-Lagrange equation to yield something of the form: \ddot{x}=\omega^2*x, but it is a little more unclear to me as to what to do here. Would I find two separate frequencies, once in x and once in y and they are two separate answers?

Perhaps if you presented the TeX/LaTeX expressions properly you would receive more responses. I edited the first of your equations above. The first one below is exactly what you wrote, but inserting the appropriate controls to make the PF processor understand you want to use LaTeX. As you can see, it looks ugly, and defeats the whole purpose of using LaTeX in the first place. The second one is the properly-edited version, in which all needed control characters are used. Right-click on it to see the TeX commands.

m*ddot{x}+m\alpha(\ddot{y}=-kx+\beta(y)

m \ddot{x}+m\alpha \ddot{y}=-kx+\beta y
 
Yosty22 said:

Homework Statement



We have a particle of mass m moving in a plane described by the following Lagrangian:
##\frac{1}{2}m((\dot{x}^2)+(\dot{y}^2)+2(\alpha)(\dot{x})(\dot{y}))-\frac{1}{2}k(x^2+y^2+(\beta)xy)##
for k>0 is a spring constant and \alpha and \beta are time-independent.

Find the normal mode frequencies, \omega_1,2

Homework Equations



Euler-Lagrange Equation

The Attempt at a Solution


I think I'm just missing here. There was a lot of math, so I won't explicitly write out all of it, but I will have my final answers. I used the Euler-Lagrange Equation twice: once for x, once for y. This yielded:

##m\ddot{x}+m\alpha\ddot{y}=-k(x+\beta y)##
and
##m\ddot{y}+m\alpha \ddot{y}=-k(y +\beta x) ##

I solved each for \ddot{x} and equated them, giving me:

##\ddot{y} = \frac{\beta+k/(\alpha)}{m(\alpha-1/(\alpha))}*y + \frac{-k-\beta/(\alpha)}{m(\alpha-1/(\alpha))}*x##

Am I approaching this the right way to find the frequencies? I know usually in 1D for example, you solve the Euler-Lagrange equation to yield something of the form: \ddot{x}=\omega^2*x, but it is a little more unclear to me as to what to do here. Would I find two separate frequencies, once in x and once in y and they are two separate answers?
Check your equations. I corrected your TeX codes. Is not a factor of 2 in front of beta in the Lagrangian?
Find the solution in form ##x=x_0 e^{i\omega t}##, ##y=y_0 e^{i\omega t} ##. You get a system of linear homogeneous equations for xo and yo that has nonzero solution for certain ω-as only.
 
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