Springs with Dashpot: Understanding Motion Equations

In summary, Wololo attempted to solve an equation of motion for a system of two masses using a dashpot, but was unsuccessful due to the force opposing the motion being canceled out. The final equation of motion obtained is solely expressed in terms of x1+x2.
  • #1
wololo
27
0

Homework Statement


Capture.PNG


Homework Equations


∑F=ma
F=-kx
x = Ae-γt/2cos(ωt + ∅)

The Attempt at a Solution


I have looked up this old thread but don't understand how to get the equation of motion from :
ma1=-kx1-k(x1-x2) - bv
ma2=-kx2-k(x2-x1) - bv

https://www.physicsforums.com/threads/system-of-2-masses-3-springs.648400/
 
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  • #2
Is your problem what to do with v? How do you think that relates to x1 and x2?
But there is something wrong with the signs. The forces the dashpot exerts on the two masses must be in opposite directions, so they can't both be -bv.
 
  • #3
What i got so far:
ma1=-kx1-k(x1-x2)-bv <==> bv=-kx1-k(x1-x2)-ma1
ma2=-kx2+k(x1-x2)-bv <==> bv=-kx2+k(x1-x2)-ma2
Substitute bv
-kx1-k(x1-x2)-ma1=-kx2+k(x1-x2)-ma2
m(a2-a1)=-kx2+kx1+k(x1-x2)+k(x1-x2)
m(a2-a1)=3k(x1-k2)

This relation is only in terms of x1-x2 not x1+x2 and also the equation of motion should be ma1+ma2=m(a1+a2) but i can't get that since ma has the same sign on both sides of the equation. Does anyone have advice on how to get to b) ? thanks
 
  • #4
wololo said:
What i got so far:
ma1=-kx1-k(x1-x2)-bv <==> bv=-kx1-k(x1-x2)-ma1
ma2=-kx2+k(x1-x2)-bv <==> bv=-kx2+k(x1-x2)-ma2
Substitute bv
-kx1-k(x1-x2)-ma1=-kx2+k(x1-x2)-ma2
m(a2-a1)=-kx2+kx1+k(x1-x2)+k(x1-x2)
m(a2-a1)=3k(x1-k2)

This relation is only in terms of x1-x2 not x1+x2 and also the equation of motion should be ma1+ma2=m(a1+a2) but i can't get that since ma has the same sign on both sides of the equation. Does anyone have advice on how to get to b) ? thanks
You don't seem to have addressed either of my comments in post #2. Do I need to explain them more?
 
  • #5
haruspex said:
The forces the dashpot exerts on the two masses must be in opposite directions, so they can't both be -bv.
The problem states that " .. v is the relative velocity of its two ends." By itself, this statement is of course ambiguous. But the additional statement that the dashpot force "opposes the motion", when considered for each mass separately, implies that F for the left mass (mass 1) has to be -b (d/dt)(x1 - x2) and for the #2 mass, -b (d/dt)(x2 - x1), thus resolving the ambiguity.
 
  • #6
rude man said:
The problem states that " .. v is the relative velocity of its two ends." By itself, this statement is of course ambiguous. But the additional statement that the dashpot force "opposes the motion", when considered for each mass separately, implies that F for the left mass (mass 1) has to be -b (d/dt)(x1 - x2) and for the #2 mass, -b (d/dt)(x2 - x1), thus resolving the ambiguity.
Ok, you are saying that the two v's are equal and opposite. But it does not look as though wololo understood that. (And it strikes me as a misleading way to have written the equations.)
 
  • #7
haruspex said:
Ok, you are saying that the two v's are equal and opposite. But it does not look as though wololo understood that. (And it strikes me as a misleading way to have written the equations.)
Agreed.
 
  • #8
I considered the force by the dashpot bv as being opposite for m1 and m2 but when I put them together to get the total force they cancel themselves. Also the force caused by the middle spring cancels itself (since it points on opposite direction at m1 and m2). The equation of motion I get is then solely expressed in terms of x1+x2 . I know that if if I considered the middle spring force as being equal for both m1 and m2, I would get an equation that depends on x1-x2, but I don't see how this could be true since a spring exerts a force in different direction at it's ends. Am I correct in assuming that in order to solve my two equations I need to put them together and find the total force exerted on the system? Perhaps the way I attempt to solve these equations is wrong and stops me from obtaining an equation that depends on both y1 and y2. Thanks for helping me clarify the way the dashpot works but I am still at a lost on how to successfully answer part b. Any ideas? Here is how I proceeded:

ma1=-kx1-k(x1-x2)-b(d/dt)(x1-x2)
ma2=-kx2+k(x1-x2)-b(d/dt)(x2-x1) <==> (rearrange) ma2=-kx2+k(x1-x2)+b(d/dt)(x1-x2)

m(a1+a2)=-kx1-kx2-k(x1-x2)+k(x1-x2)-b(d/dt)(x1-x2)+b(d/dt)(x1-x2)
Ftot=-k(x1+x2) (all the other terms cancel)
 
  • #9
wololo said:
I considered the force by the dashpot bv as being opposite for m1 and m2 but when I put them together to get the total force they cancel themselves.
They only cancel because of the way you are combining the two equations.
Assuming you corrected the sign (so that they are now opposite) if you add them the bv terms cancel. What else could you do?
Please also answer my other question: what equation directly relates v to x1, x2 and time?
Oh, and before all that, you need to define clearly what v means.
 
  • #10
wololo said:
ma1=-kx1-k(x1-x2)-b(d/dt)(x1-x2)
ma2=-kx2+k(x1-x2)-b(d/dt)(x2-x1) <==> (rearrange) ma2=-kx2+k(x1-x2)+b(d/dt)(x1-x2)
These equations are correct, except why "rearrange" them? Solve for x1 and x2 for part (a).
Ftot=-k(x1+x2) (all the other terms cancel)
why are you adding the forces on m1 and m2?
Do part (a); then part (b) and (c) follow without too much trouble.
 
  • #11
haruspex said:
They only cancel because of the way you are combining the two equations.
Assuming you corrected the sign (so that they are now opposite) if you add them the bv terms cancel. What else could you do?
Please also answer my other question: what equation directly relates v to x1, x2 and time?
Oh, and before all that, you need to define clearly what v means.

v is the relative speed betwen both ends of the dashpot, so v2-v1. Speed is equal to the derivate of position in regards to time, dx/dt, in this case dx will be the relative variation of x between both ends of the dashpot so bv=bd(x2-x1)/dt

rude man said:
These equations are correct, except why "rearrange" them? Solve for x1 and x2 for part (a).
why are you adding the forces on m1 and m2?
Do part (a); then part (b) and (c) follow without too much trouble.

If I develop develop F1 and F2 seperately, assuming y1=x1+x2 and y2=x1-x2, I get:

F1=-kx1-ky2-b(d/dt)(y2)
F2=-kx2+ky2+b(d/dt)(y2)

I don't see how I can express them in terms of y1

Could it be that the dashpot only exerts a force on the system as a whole, such that

Ftot=F1+F2-bv

Which would give
Ftot=(-kx1-ky2)+(-kx2+ky2)-b(d/dt)(y2)
Ftot=-ky1-b(d/dt)(y2)
?
 
  • #12
wololo said:
v is the relative speed betwen both ends of the dashpot, so v2-v1. Speed is equal to the derivate of position in regards to time, dx/dt, in this case dx will be the relative variation of x between both ends of the dashpot so bv=bd(x2-x1)/dt
No, as I pointed out before, the two v's are different for the two equations, and haruspex has also pointed out that they can't be the same for both equations.
I don't see how I can express them in terms of y1
First, what are F1 and F2 in terms of x1 and x2?
Then, try adding the two equations (in post 10) together.
Then, try subtracting the second equation from the first.
 
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  • #13
rude man said:
First, what are F1 and F2 in terms of x1 and x2?

Post 8 (ma1=F1 and ma2=F2):
wololo said:
ma1=-kx1-k(x1-x2)-b(d/dt)(x1-x2)
ma2=-kx2+k(x1-x2)-b(d/dt)(x2-x1)

rude man said:
Then, try adding the two equations (in post 10) together.

I already added the two equations together in post 8:
wololo said:
m(a1+a2)=-kx1-kx2-k(x1-x2)+k(x1-x2)-b(d/dt)(x1-x2)+b(d/dt)(x1-x2)
=-k(x1+x2) (all the other terms cancel)

rude man said:
Then, try subtracting the first equation from the second
-kx1-k(x1-x2)-b(d/dt)(x1-x2)-(-kx2+k(x1-x2)-b(d/dt)(x2-x1))
=-k(x1-x2)-2k(x1-x2)-2b(d/dt)(x1-x2)
=-3k(x1-x2)-2b(d/dt)(x1-x2)

I must be forgetting some relation since both you and Haruspex seem to be trying to point me towards something, though I evidently cant't tell what . Would one of you please be willing to point out what I am missing? I added and substracted the equations and still can't express them in terms of x1-x2 and x1+x2. I really am at a loss. Thanks!
 
  • #14
wololo said:
Post 8 (ma1=F1 and ma2=F2):
Again: what are F1 and F2 in terms of x1 and x2? Saying F1 = ma1 does not answer that question. This is the first thing you need to get right.
I already added the two equations together in post 8:.
Right, and you got F1 + F2 = -k(x1 + x2). So - one mo' time - what are F1 and F2 in terms of x1 and x2?
EDIT: I just noticed, part (a) does not ask you to solve for x1 and x2. Good thing, because that's a real mess. But in part (b) you substitute y1 = x1 + x2 and y2 = x1 - x2, that makes solving for y1 very easy and then y2 is similarly easily obtained. Finally, solve for x1(t→∞) and x2(t→∞) from y1(t→∞) and y2(t→∞).
 
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  • #15
wololo said:
Post 8 (ma1=F1 and ma2=F2):
I already added the two equations together in post 8:
Yes, that was good. Sorry i asked you why you did it. I was concentrating on solving for x1 and x2 separately which would be a big mess - see my previous post. You got F1 + F2 = -k(x1+x2) (all the other terms cancel) which is right. So can you replace x1+x2 with one of the two y's?
-kx1-k(x1-x2)-b(d/dt)(x1-x2)-(-kx2+k(x1-x2)-b(d/dt)(x2-x1))
=-k(x1-x2)-2k(x1-x2)-2b(d/dt)(x1-x2)
=-3k(x1-x2)-2b(d/dt)(x1-x2)
equals what? Can you replace x1-x2 with the other y?
I must be forgetting some relation since both you and Haruspex seem to be trying to point me towards something, though I evidently cant't tell what . Would one of you please be willing to point out what I am missing? I added and substracted the equations and still can't express them in terms of x1-x2 and x1+x2. I really am at a loss. Thanks!
see my previous post.
 
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Related to Springs with Dashpot: Understanding Motion Equations

1. What is a spring with dashpot?

A spring with dashpot is a mechanical system that combines a spring and a dashpot (also known as a shock absorber) to create a damping effect on motion. It is often used in engineering and physics to model the behavior of objects in motion.

2. How does a spring with dashpot work?

The spring component of a spring with dashpot provides the restoring force that opposes the motion of the system, while the dashpot component absorbs energy and dissipates it as heat. Together, they work to dampen the oscillations of the system and bring it to rest.

3. What are the equations used to describe motion in a spring with dashpot system?

The equations used to describe motion in a spring with dashpot system are the spring force equation (F = -kx), the damping force equation (F = -bv), and the equation of motion (ma + bv + kx = 0). These equations can be used to determine the displacement, velocity, and acceleration of the system at any given time.

4. How is the behavior of a spring with dashpot affected by the values of k and b?

The values of k (spring constant) and b (damping coefficient) affect the behavior of a spring with dashpot system in the following ways:

  • A higher value of k results in a stiffer spring, which leads to faster oscillations and a shorter time to reach equilibrium.
  • A higher value of b results in a stronger damping effect, causing the system to reach equilibrium more quickly.
  • If the value of b is too high, it can cause the system to become overdamped, meaning it takes longer to reach equilibrium.

5. What are some practical applications of springs with dashpots?

Springs with dashpots have various practical applications, including shock absorbers in vehicles, vibration dampers in buildings and bridges, and suspension systems in mechanical devices. They are also used in seismometers to detect and measure earthquakes.

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