How Do Two Masses and Three Springs Interact with a Dashpot?

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The discussion focuses on the dynamics of two masses connected by springs and a dashpot, leading to the formulation of equations of motion. Participants derive the equations for each mass using the spring force and damping effects, ultimately expressing the system in terms of new variables y1 and y2. Clarifications are made regarding the relative velocity of the masses and how it influences the forces acting on them. There is some confusion about the signs in the equations, which is addressed by emphasizing the need to clearly define the forces in terms of the displacements x1 and x2. The conversation highlights the importance of accurately representing the system's dynamics to solve the problem effectively.
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Homework Statement



Two particles, each of mass M, are hung between three identical springs. Each spring is massless and has spring constant k. Neglect gravity. The masses are connected as shown to a dashpot of negligible mass.

The dashpot exerts a force of bv, where v is the relative velocity of its two ends. The force opposes the motion. Let x1 and x2 be the displacement of the two masses from equilibrium.


a. Find the equation of motion for each mass.

b. Show that the equation of motion can be solved in terms of the new dependent variables y1 = x1 + x2 and y1 = x1 - x2.

c. Show that if the masses are initially at rest and mass 1 is given initial velocity v0, the motion of the masses after a sufficiently long time is
x1=x2
= (v0/2ω)* sin(ωt)

Evaluate ω.

Homework Equations



x.. + γx.+ ω2x = 0

x = Ae-γt/2cos(ωt + ∅)

The Attempt at a Solution



I think I managed to get the first two by just using different F = -kx formulae and adding -bv to it.

The second part I just added and subtracted the equations to get:
y..1 + ω2y1 + \frac{2bv}{m} = 0

and

y..2 + 3ω2y2 = 0

I think these are right, as far as I know. The thing is, I'm not sure how to proceed from here. I tried using:

x = Ae-γt/2cos(ωt + ∅)

I can get it very close to the answer, but I don't think that's how you're supposed to do this... using what I got in part 2 would be more relevant, I think.
 
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Seeing the diagram or at least its description would be helpful.
 
Sorry, this is the image:

35cf45ff-190f-4bc2-acc7-636af40a0b06.png
 
Could you show your equations for a) and the derivation for b)?
 
ma1=-kx1-k(x1-x2) - bv

ma2=-kx2-k(x2-x1) - bv

These were my first two equations of motion.

I just added and subtracted them, using k = ω2m to get the equations for 2.

Quick question: can I take relative velocity v as equal to the derivative of y2 with respect to time?
 
But what is v in your equations? And how come it is the same in both equations?
 
"... where v is the relative velocity of its two ends. The force opposes the motion."

So yeah, it should be the same for both cases – both magnitude and direction.
 
"Relative velocity" is relative to the velocity of the opposite end. It is the same (= zero) only of the ends have the same velocity. Express it in terms of x1 and x2 for both ends.
 
voko said:
"Relative velocity" is relative to the velocity of the opposite end. It is the same (= zero) only of the ends have the same velocity. Express it in terms of x1 and x2 for both ends.

Yeah, it's the relative velocity of one end of the dashpot to the other (thus the relative velocity of one mass to another).

So for the first mass it'll be derivate of x2 minus that of x1 with respect to time... and for the second mass it'll be negative of that? But the force opposes the motion. Therefore, for the first mass that is displaced by x1, the force will be negative (to the left). Similarly, if the second mass is displaced by x2, the force will be negative as well. Are my signs wrong?

If relative velocity is in terms of x2 - x1, then I could express it in terms of y2, right?

On another note, in the third part, if x1 = x2 then relative velocity should be 0.
 
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a.man said:
Yeah, it's the relative velocity of one end of the dashpot to the other (thus the relative velocity of one mass to another).

So for the first mass it'll be derivate of x2 minus that of x1 with respect to time... and for the second mass it'll be negative of that? But the force opposes the motion.

I am with you till this point.

Therefore, for the first mass that is displaced by x1, the force will be negative (to the left). Similarly, if the second mass is displaced by x2, the force will be negative as well. Are my signs wrong?

This is less clear. The net force acting on either mass is the sum of three forces, two due to springs and one due to damping. I think should write down the equations in terms of x1 and x2 just for clarity.

If relative velocity is in terms of x2 - x1, then I could express it in terms of y2, right?

Yes, but, again, you should write down the equations in terms of x1 and x2 first.
 
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