Two-Degree-Of-Freedom Linear System: Eigenvalue problem

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Homework Help Overview

The discussion revolves around a two-degree-of-freedom linear system characterized by a fourth-degree characteristic equation involving two masses and a stiffness constant. Participants are exploring the process of finding eigenfrequencies and corresponding eigenvectors, with specific challenges arising due to the complexity of the roots.

Discussion Character

  • Exploratory, Conceptual clarification, Problem interpretation

Approaches and Questions Raised

  • Participants discuss the characteristic equation and its implications for finding eigenfrequencies and eigenvectors. There are suggestions to substitute variables to simplify the equation, and questions about the coupling of the masses and springs in the system. Some participants express uncertainty about how to handle complex roots and the subsequent steps to find eigenvectors.

Discussion Status

The discussion is active, with participants providing guidance on substitution methods and questioning the original poster's approach. There is recognition that the complexity of the roots does not invalidate the solution process, and some participants suggest numerical solutions to visualize the modes.

Contextual Notes

Participants note that the system involves two masses and a single stiffness constant, raising questions about the coupling mechanism. There is an acknowledgment of the original poster's frustration with the lack of straightforward cancellations typically seen in simpler examples.

Valeron21
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I've found the characteristic equation of the system I'm trying to solve:
$$ω^{4}m_{1}m_{2}-k(m_{1}+2m_{2})ω^{2}+k^{2}=0$$

I now need to find the eigenfrequencies, i.e. the two positive roots of this equation, and then find the corresponding eigenvectors. I've been OK with other examples, but because of the different masses here, I don't see any obvious substitution or cancellation that will leave the eigenfrequencies in a manageable form.

I've been at this a while and I'm a bit lost.


Thanks in advance.
 
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Valeron21 said:
I've found the characteristic equation of the system I'm trying to solve:
$$ω^{4}m_{1}m_{2}-k(m_{1}+2m_{2})ω^{2}+k^{2}=0$$

I now need to find the eigenfrequencies, i.e. the two positive roots of this equation, and then find the corresponding eigenvectors. I've been OK with other examples, but because of the different masses here, I don't see any obvious substitution or cancellation that will leave the eigenfrequencies in a manageable form.

I've been at this a while and I'm a bit lost.


Thanks in advance.

If you substitute u=ω^2 then it's quadratic in u. Once you know u, you can find ω, right?
 
Dick said:
If you substitute u=ω^2 then it's quadratic in u. Once you know u, you can find ω, right?
Sorry. The characteristic equation isn't really the problem - I should have worded that better - it's how I use what will be pretty horrible roots to find the corresponding eigenvectors that I'm having trouble with.

EDIT: $$(k-ω_{i}^{2}m)u_{i}=0$$
is what I would usually sub the values of ω into to find the eigenvectors, where k is the stiffness matrix, m is the mass matrix and u the eigenvector.
 
Last edited:
From your characteristic equation it seems that you have only one k and two masses. Is that correct?
 
nasu said:
From your characteristic equation it seems that you have only one k and two masses. Is that correct?
Yes, that is correct. Both springs in the system have the same stiffness constant, k.
 
So how does it look like? You have two masses and two springs but how do you couple them?
I am just curios.
For the solution, it does not have to simplify to a simple expression. The fact that it does not do not implies that the solution is wrong.
Once you find a solution for frequency, you plug it in one of the equations and find the ratio of the amplitudes for that mode. You may want a numerical solution, in order to "see" how does the mode look like.
 
nasu said:
So how does it look like? You have two masses and two springs but how do you couple them?
I am just curios.
For the solution, it does not have to simplify to a simple expression. The fact that it does not do not implies that the solution is wrong.
Once you find a solution for frequency, you plug it in one of the equations and find the ratio of the amplitudes for that mode. You may want a numerical solution, in order to "see" how does the mode look like.
DRkawiX.png


Hmm, maybe there's something wrong in how I'm approaching this?

I've always previously, when working with 2.D.O.F. systems, assumed a solution of the form:

$$ \underline{X}={U}[A_{}cos(ω_{}t)+B_{}sin(ω_{}t)]$$

then through a process of differentiation and substitution obtained this equation:
$$( \underline{k}-ω^{2} \underline{m}) \underline{X}=0$$

then, for a non-trivial solution, the det =/=0, etc. And here I am now with the roots of the characteristic equation.

Previously, I've always been able to sub the values of ω into this:
$$(\underline{k}-ω_{i}^{2}\underline{m})\underline{u}_{i}=0$$

there's always been a nice cancellation and I've been able to use an arbitrary value to find the ratio, as you say, between the two elements in the eigenvector. But here, with horrible roots, I'm not sure what to do. And I'm not sure which equations you're referring to.

Sorry if I'm being stupid.
 
The method is OK.
It's just that you don't have to obtain a nice solution. In the textbook examples they pick-up parameters to get a simple result, as an example.

I mean the equations which you wrote in matrix format.
Maybe you are too formal about it. You don't really need the matrix form for two equations.
What stops you from substituting the values for omega back into the equations?
 

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