Complex Eigen Values: Physical Insight

  • Context: Graduate 
  • Thread starter Thread starter svishal03
  • Start date Start date
  • Tags Tags
    Complex Eigen values
Click For Summary

Discussion Overview

The discussion revolves around the physical interpretation of complex eigenvalues in the context of vibration analysis, particularly for single degree of freedom (SDOF) systems and modal analysis of multi-degree of freedom systems. Participants explore the implications of real, imaginary, and complex eigenvalues in relation to oscillatory and exponential solutions in vibrating systems.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants suggest that complex eigenvalues typically indicate a combination of oscillatory and exponential solutions.
  • Others argue that real eigenvalues correspond to exponential solutions, while imaginary eigenvalues indicate oscillatory solutions.
  • A participant questions the assertion that eigenvalues are purely imaginary in undamped systems, citing a cantilever beam example.
  • Another participant clarifies that for undamped free oscillations, the eigenvalues are indeed purely imaginary, leading to perpetual oscillation.
  • There is a discussion about how damping affects eigenvalues, with complex eigenvalues arising when damping is present.
  • Some participants propose that the interpretation of eigenvalues can vary depending on the approach taken in vibration analysis, such as using different forms of the governing equations.
  • One participant seeks clarification on the physical meaning of "exponential" in the context of moving to equilibrium, asking whether it refers to rapid movement or rapid decay of oscillation.

Areas of Agreement / Disagreement

Participants express differing views on the nature of eigenvalues in undamped systems, with some asserting they are purely imaginary while others challenge this claim. The discussion remains unresolved regarding the interpretation of eigenvalues and their implications in various damping scenarios.

Contextual Notes

There are limitations in the assumptions made regarding damping and the definitions of eigenvalues, as well as unresolved mathematical steps in the derivations presented. The discussion reflects a range of interpretations and approaches to the topic.

svishal03
Messages
124
Reaction score
1
Please can anyone provide an insight into what do complex eigen values physically indicate?

Vishal
 
Physics news on Phys.org
Hi svishal,

What part of Physics do you mean?

ehild
 
complex eigenvalues usually represent some linear combination of sin and cos
 
Typically, real eigenvalues signify exponential solutions, imaginary eigenvalues signify oscillatory solutions and complex eigenvalues signify a combination of the two.
 
@ehild:I meant the part for finding the solution of SDOF (or a modal analysis of a multi degree of freedom) vibration problem.

@boneh3ad: if ω = √k/ m, where ω is the natural frequency and m the mass, suppose we get a real value for ω (say 1.1 or 3.0), what you mean by exponential here in terms of vibration?

Also, if we get an imaginary value i.e ω^2= -2 , then, what you mena by osciallting?Anyways the body is vibratiing (i.eosciallating), right?
 
In case of vibrating systems, you transform the system of differential equations into a homogeneous system of linear equations by assuming the solution in form of y=yoeλt. The eigenvalues are imaginary in case of vibration without damping, and they are complex when damping is present.

ehild
 
The eigenvalues are imaginary in case of vibration without damping

How can you say so?Take a simple cantilever beam example with a mass at the free end.Then

ω=√k/m

k = 3EI / L^3

That does not give an imaginary Eigen value?
 
Sure it does. If you have no damping, for an unforced oscillation you have the governing equation
m\ddot{x} + kx = 0
This admits solutions of the form
x = Ce^{\lambda t}
where \lambda are the eigenvalues. Here, your eigenvalues are
\lambda^2 = -\frac{k}{m}
which means that \lambda is always imaginary since both k and m are real and positive. For an undamped, free oscillation, the eigenvalues are always purely imaginary. That means without the damping force, the oscillation will continue into infinity.

Now, for damping the governing equation is
m\ddot{x} +c\dot{x}+ kx = 0
which has the same general form of the solution, only the eigenvalues are now
\lambda = \frac{-c \pm \sqrt{c^2 - 4km}}{2m}
In this case, the eigenvalues are purely imaginary if c = 0 (the undamped case), are purely real if c > 2\sqrt{km} and are complex if c < 2\sqrt{km}.

A purely imaginary eigenvalue means the system oscillates for all time. A purely real eigenvalue means that the solutions are exponential and decay directly to zero (since it is impossible to have a positive eigenvalue). A complex eigenvalue means you have an oscillation of decreasing amplitude until eventually you reach zero.
 
There are two different ways to define "the eigenvalues" here.

If you are doing vibration analysis of a system without damping, you "know" the response is going to be an oscillation, so instead of Boned3ad's ##x = Ce^{\lambda t}## you usually start from ##x = Ce^{i\omega t}##.

The first one gives you an imaginary value of ##\lambda##, the second gives a real value of ##\omega##.

If you have a general damping matrix, you would normally folllow Boned3ad's math (which leads to a quadratic eigenproblem). On the other hand if you assume a special forms of damping matrix (e.g. Rayleigh damping) it can be shown that the damped mode shapes are the same as the undamped, so you usually formulate the math in terms of the real values of ##\omega##.
 
  • #10
Thank you very much boneh3ad, it was very useful for me.

Thanks to Alephzero for pointing out what I was actually trying to ask. However the texts on Structural Dynamics (Anil K Chopra, UCB) do not start the way boneh3ad explained. I fell that is how it should be explianed which brings out the physical interpretation of real,imaginary,complex Eigen values.

Thanks to all.
 
  • #11
@Boneh3d:

You said:

A purely real eigenvalue means that the solutions are exponential and decay directly to zero (since it is impossible to have a positive eigenvalue)

Did you mean a pure real eigen value would indicate that the system is stationary?
 
  • #12
svishal03 said:
@Boneh3d:

You said:



Did you mean a pure real eigen value would indicate that the system is stationary?

No, the oscillator (be it a beam, spring, circuit or whatever else) would move exponentially to the equilibrium position. Assuming the initial conditions are \dot{x}=0 and x=0 then it would be stationary, but in that case it would be stationary regardless of the eigenvalues.
 
  • #13
@boneh3ad:Thanks a lot for the swift reply.

When you say:
move exponentially to the equilibrium position

do you mean (perhaps I'm looking for a physical meaning of the word 'exponential' here) that it moves very rapidly to the equilibrium position or the oscillation decays to zero (stops moving) very rapidly?
 
  • #14
Meaning it moves to zero at an exponential rate. Remember, the solutions were exponential and with negative, real eigenvalues, the solutions therefore approach zero exponentially.
 
  • #15
Can we put it like this:

1)c= 0- undamped case
2)c>2√kmmeans the system does NOT oscillate thus returns to equilibrium position without oscillating
3)c<2√km system oscillates with a decreasing amplitude and eventually stops oscillating.
 
Last edited:

Similar threads

  • · Replies 4 ·
Replies
4
Views
5K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 13 ·
Replies
13
Views
2K
  • · Replies 6 ·
Replies
6
Views
2K
  • · Replies 13 ·
Replies
13
Views
2K
  • · Replies 11 ·
Replies
11
Views
3K
  • · Replies 7 ·
Replies
7
Views
7K
  • · Replies 3 ·
Replies
3
Views
4K
  • · Replies 108 ·
4
Replies
108
Views
12K
  • · Replies 1 ·
Replies
1
Views
1K