Finding ##x_c(t=0)## for a system of coupled Masses & Springs

AI Thread Summary
The discussion revolves around finding the initial position, ##x_c(t=0)##, for a system of coupled masses and springs, particularly focusing on the motion of block A. Participants explore the relationship between eigenvalues, eigenvectors, and the equations of motion, noting that the amplitude modulation complicates the understanding of the system's behavior. The importance of the dot product between the position vector and eigenvectors is highlighted, revealing that it determines whether certain modes of oscillation occur at t=0. Clarifications about the physical significance of eigenvectors and the conditions for oscillation modes to be active are also discussed. Ultimately, the conversation leads to a better understanding of how these mathematical concepts apply to the dynamics of the coupled mass-spring system.
Redwaves
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Homework Statement
Find ##x_c(t=0)## for which the frequency on the block a is ##\frac{(3+\sqrt{4})}{2}## and the amplitude is ##\frac{(cos(3-\sqrt{7}t))}{2}##
The block B oscillate in pure sine.
All the blocks are at rest, thus ##v_a = v_b = v_c = 0##
Relevant Equations
##x_a(t=0) = 6, x_b(t=0) =-6, x_c(t=0) = ?##
Hi,

First of all, I'm not sure at all how to start this question. I found the eigenvectors in a previous question, but I'm not sure if I need it to solve this one.

I think I need to use the expression for the position and velocity.
##a_n = C_n cos (\omega_n t + \alpha_n)##
##v_n = -\omega_n C_n sin (\omega_n t + \alpha_n)##

However, I don't how this can help me to find ##x_c(t=0)## for which the movement of the block A matches a frequency of ##\frac{(3+\sqrt{4})}{2}## and an amplitude ##\frac{(cos(3-\sqrt{7}t))}{2}##

FlBWwrP.png
 
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What are you talking about ? What block ?

##\ ##
 
BvU said:
What are you talking about ? What block ?

##\ ##

I drew the system. Sorry If it wasn't clear.
 
I don't understand the expression for the amplitude. It should be a constant, not a function of time.
 
It is probably just me having hard time to understand the question. It says the amplitude is modulated by that function. However, I don't really know what that means. Once again I'm sorry.
 
Redwaves said:
It says the amplitude is modulated by that function.
That suggests to me that A is supposed to move like ##\sin(\frac{(3+\sqrt{7})}{2}t)\frac{(cos(3-\sqrt{7}t))}{2}##, but I would not have thought that consistent with B moving as pure sine. Though maybe C also having that sort of modulation makes that possible.
 
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I think I found something with what you said.
In general if I have the eigenvectors and the eigenvalues and the system doesn't have any damping force, can I use ##x_a(t) = C_1 X_{1a}cos(\omega_1 t + \alpha_1) + C_2 X_{2a}cos(\omega_2 t + \alpha_2) + C_3 X_{3a}cos(\omega_3 t + \alpha_3)##

What ##X_{na}## means. I mean is it some kind of displacement? I realized that I'm not even sure what ##x_a(t) = C_1 X_{1a}cos(\omega_1 t + \alpha_1) + C_2 X_{2a}cos(\omega_2 t + \alpha_2) + C_3 X_{3a}cos(\omega_3 t + \alpha_3)## really is.

I just realized that I have a graph for ##x_a(t)## which is a beats frequency graph.

I have my eigenvalues and eigenvectors which are ##\omega_1^2 = 2k/m, \omega_2^2 = 7k/m, \omega_3^2 = 9k/m, <1| = (1,5,3), <2| = (3,0,-1), <3| = (1,-2,3)##

I know ##x_c(t=0) = 8##

So I'm trying a lot of different thing just to find the correct answer. I really don't know what I'm doing.
 
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Redwaves said:
a beats frequency graph
Which is what you get from the expression in post #6.
 
I'm not sure to understand the ##\sin## If the amplitude of the beats frequencies is ##2A \cos(\omega_1 - \omega_2)t/2##. Does it means that ##x_a(t) = \cos(3+\sqrt{7})t / 2 (\cos (3-\sqrt{7})t/2)##.
Thus, ##\omega_1 = 3## and ##\omega_? = \sqrt{7}## ?

Using trig identity, I get ##(\cos(a) + \cos(b))/2##

##x_a(t) = \frac{cos(3)}{2} + \frac{cos(\sqrt{7})}{2}##, so based of my eigenvalues. I can see that ##x_a(t)## oscillate in 2 modes only, the second and the third.

I have my vector for ##x_n(t=0) = (6,-6,c)## if I do a dot product with my eigenvector for the first mode I get ##x_c(0) = 8## which is the right answer! However, I don't know how it works. I mean why the dot product between my vector ##x_n(0)## and the first eigenvector gives me the correct answer.
 
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  • #10
Redwaves said:
I'm not sure to understand the sin
I wrote "something like". The choice of sin rather than cos was arbitrary.
 
  • #11
All right, I see.
Can you confirm that what I said is not totally wrong?
 
  • #12
Redwaves said:
why the dot product between my vector ##x_n(0)## and the first eigenvector gives me the correct answer.
I'd say it's because it does not oscillate in that mode.
For an eigenvector ##e##, ##\ddot x.e=\lambda x.e##. Setting ##x(0).e=0## gives ##\ddot x.e=0##. Since ##\dot x(0)=0##, that combo is constant.
 
  • #13
I understand that at t=0, all the blocks doesn't moves, but does it means that the block A shouldn't oscillate in that mode? so, this is the only mode that A is at rest. Furthermore, I don't know why a dot product between an eigenvector and the position vector give me the position for C. What's the meaning of this eigenvector.

For me it's like if I did a dot product between my position vector and something for I whatever reason.
 
  • #14
Redwaves said:
I understand that at t=0, all the blocks doesn't moves, but does it means that the block A shouldn't oscillate in that mode? so, this is the only mode that A is at rest. Furthermore, I don't know why a dot product between an eigenvector and the position vector give me the position for C. What's the meaning of this eigenvector.

For me it's like if I did a dot product between my position vector and something for I whatever reason.
The eigenvector represents a linear combination of the displacements. Specifically, it is a combination which satisfies the equation I wrote in post #13:
##\ddot x.e=\lambda x.e##
where ##\lambda## is the corresponding eigenvalue.
You can check that works here.
As you can see, this means the scalar ##x.e## obeys 1D SHM.

You (somehow) determined that only modes 2 and 3 occur. We know that ##\dot x.e## is zero at t=0. If ##x.e## is also zero at t=0, the equation tells us that ##\ddot x.e## is zero at t=0. It follows that ##x.e## is always zero. This is precisely what we need for the mode not to occur (i.e. it is if and only if), so we can conclude ##x.e## is indeed zero at t=0 for mode 1.
 
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  • #15
I think I understand. That begin to make sense. I had no idea about the equation you wrote and if ##\ddot{x}## = 0 then the mode don't occur. Thanks !
 
  • #16
Redwaves said:
I think I understand. That begin to make sense. I had no idea about the equation you wrote and if ##\ddot{x}## = 0 then the mode don't occur. Thanks !
Well, it also requires ##\dot x=0##.

Btw, this is not an area I ever studied, though I did encounter eigenvalues and eigenvectors in a couple of other contexts. I didn't know that equation either, but when you asked me about the physical significance of the eigenvector it made me give it some thought.
 
  • #17
I think what you said make plenty of sense. It is exactly what I was looking for.
 
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