- #1
Trying2Learn
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- TL;DR Summary
- Justify common frequency, yet different amplitudes
Hello!
Suppose you have two masses, that are connected by a spring.
Each mass is, in turn, connected by a spring to a wall
So there is a straight line: left wall to first mass, first mass to second mass, second mass to right wall
This problem can be analyzed as an eigenvalue problem.
We assume a solution for the displacement of each mass as:
x1(t) = X1 exp(i*omega*time)
x2(t) = X2 exp(i*omega*time)
Do you see that?
We assume a solution with:
So my question is: can someone justify this assumption?
I know the process works and we must solve for an eigenvalue problem.
But could someone provide (in words), a justification for this assumption?
Suppose you have two masses, that are connected by a spring.
Each mass is, in turn, connected by a spring to a wall
So there is a straight line: left wall to first mass, first mass to second mass, second mass to right wall
This problem can be analyzed as an eigenvalue problem.
We assume a solution for the displacement of each mass as:
x1(t) = X1 exp(i*omega*time)
x2(t) = X2 exp(i*omega*time)
Do you see that?
We assume a solution with:
- an unspecified common frequency
- two different amplitudes
So my question is: can someone justify this assumption?
I know the process works and we must solve for an eigenvalue problem.
But could someone provide (in words), a justification for this assumption?