Finding the acceleration of two masses on a pulley system

In summary: Can I assume the net acceleration for m2 is the one given in the problem?Yes, assuming the conditions are met.Yes.
  • #36
Jpyhsics said:
That is exactly where I am too!
But i think that the positive x direction has been switched in your x direction equations.
 
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  • #37
Jpyhsics said:
So since it is in equilibrium can we assume forces in the x and y direction equal zero? So is the tension force equal to m2g?
It is in equilibrium just before the surface starts to accelerate, so yes, at that time the tension equals the weight of m2. But not once the acceleration starts.
 
  • #38
FriedChicken885 said:
based off of the fact that the system began in equilibrium
Not just that it was in equilibrium, but that it was on the point of not being so.
FriedChicken885 said:
I don’t know how to use the acceleration of the surface and the pulley...
I refer you to posts #2, #6 and #27, which @Jpyhsics is studiously ignoring.
 
  • #39
haruspex said:
Not just that it was in equilibrium, but that it was on the point of not being so.

I refer you to posts #2, #6 and #27, which @Jpyhsics is studiously ignoring.
I am not ignoring it, I just don't know. As I was taught that the accelerations of both the objects would be the same just in opposite directions, but you have said that is not the case, so I don't know what to assume.
 
  • #40
haruspex said:
I refer you to posts #2, #6 and #27

Is it something along the line that the difference in the accelerations of m1 and the surface would be the maximum possible acceleration of m2?

Since the string is fixed length, the mass 2 can't fall any faster than the length of the vertical part of the string is growing? Am I on the right track here?
 
  • #41
Jpyhsics said:
I was taught that the accelerations of both the objects would be the same just in opposite directions,
That must have been for some specific context that does not occur here. What context was that in?
Jpyhsics said:
I am not ignoring it,
You are in that you have not responded to it. If you don't understand a hint say so.
Think about the two lengths of string, the vertical part and the horizontal part. Each of those has has an "acceleration", i.e. a second derivative of length wrt time.
What is the relationship between them?
How does the "acceleration" of the horizontal part relate to the acceleration of the platform and the acceleration of m1?
 
  • #42
FriedChicken885 said:
Is it something along the line that the difference in the accelerations of m1 and the surface would be the maximum possible acceleration of m2?

Since the string is fixed length, the mass 2 can't fall any faster than the length of the vertical part of the string is growing? Am I on the right track here?
Yes, but you can assume the string remains taut.
 
  • #43
haruspex said:
Yes, but you can assume the string remains taut.

Okay, from this point I get to a(2) = a(surface) + a(1) if a(1) is towards the left and a(2) = a(surface) - a(1) is a(1) is towards the right

How would I find the direction of a(1) and go about solving it from here? Also is the previously found equation a1 = (1/2)(a2) valid?
 
  • #44
Jpyhsics said:

Homework Statement


Two blocks of the masses m1=7.40 kg and m2=m1/2 are connected via a massless pulley and massless string. The system is currently in equilibrium but is about to start sliding, if m2 would increase even by a bit. For the friction between the surface and m1 assume that µs=µk. The block m2 is suspended from the pulley and is free to swing. What will be the acceleration of m1 if the surface starts to move in a horizontal direction to the right with an acceleration a=5.43 m/s2? Take +x direction to be toward the left. Give your answer in m/s2.

Homework Equations


F=ma

The Attempt at a Solution


For m1
ΣFx=FT
m1a1=FT

For m2
ΣFy=FT-mg
m2a2=FT-mg

I am not sure how to use the given acceleration in the problem. Also, does µs=µk mean there is no friction?If anyone could help me with this, I would be grateful.
Were you given a diagram for this question?
 
  • #45
bluejay27 said:
Were you given a diagram for this question?
See post #3 for a diagram.
 
  • #46
FriedChicken885 said:
How would I find the direction of a(1)
You do not need to guess the direction. Just define a particular direction as positive and write the equation accordingly. If you get a negative answer then the acceleration is in the other direction.
 
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  • #47
FriedChicken885 said:
Also is the previously found equation a1 = (1/2)(a2) valid?
Looks right.
 
  • #48
haruspex said:
Looks right.
So does that mean that the acceleration of 1 is half the acceleration of 2? Why would that be so?
 
  • #49
FriedChicken885 said:
Okay, from this point I get to a(2) = a(surface) + a(1) if a(1) is towards the left and a(2) = a(surface) - a(1) is a(1) is towards the right

How would I find the direction of a(1) and go about solving it from here? Also is the previously found equation a1 = (1/2)(a2) valid?
haruspex said:
You do not need to guess the direction. Just define a particular direction as positive and write the equation accordingly. If you get a negative answer then the acceleration is in the other direction.

So if you were to define the right as a negative direction, as indicated in the question would the formulae become:

a2= -asurface + a1 ? Does that seem valid?
 
  • #50
Jpyhsics said:
So if you were to define the right as a negative direction, as indicated in the question would the formulae become (defining left as a positive direction):

a2= -asurface + a1 ? Does that seem valid?

So based on the previous post #43 would that mean that
a2= -2a1

If that is the case then it seems as though the acceleration of the surface is not needed as
T2 = m2(a2 +g)
T1 = m1(a1+μg)

Which I would equate the two equations and just for a1

Based on intuition, I don't think we would have been given the acceleration of the surface if we were not required to use it...
So where am I going wrong?

Woul
 
  • #51
So I guess my question is which of these two equations do we use in the tension force equations (if either is correct...and if my tension force equations are correct...):
a2= -asurface + a1
a2= -2a1
 
  • #52
Jpyhsics said:
a2= -asurface + a1 ?
Which way are you defining as positive for asurface?
 
  • #53
Jpyhsics said:
it seems as though the acceleration of the surface is not needed
You are to find the accelerations of the masses in terms of the acceleration of the surface.
 
  • #54
So I went through the entire question with +x as left and +y as up, I got to the two equations a(2) = 2a(1) and -a(2) = a - a(1) and solved for a(1) = -a. Yet I got the incorrect answer, what did I do wrong?
 
  • #55
FriedChicken885 said:
-a(2) = a - a(1)
If you are taking a2 as positive up and a1 positive left then you have a sign error there.
 
  • #56
haruspex said:
If you are taking a2 as positive up and a1 positive left then you have a sign error there.
I also tried it for:
a2 = 2a1 and a2 = a - a1 and solved for a1 = ⅓a, but that's still the incorrect answer. Also I wonder if I'm missing something since I don't use the given value of m1.
 
  • #57
FriedChicken885 said:
a2 = a - a1
still the wrong combination of signs.
The easiest way to get this right is to imagine holding one acceleration at zero and thinking how the other two interact.
Since a1 and a2 are both positive towards the pulley, if a were zero their sum would be constant. So we have a1+a2= f(a).
If we imagine a2 held at zero but the string remaining taut then m1 must be at constant distance from the pulley. Since a is positive right but (bizarrely) a1 is positive left then, again, their sum must be constant. This leads to a1+a2= -a.
 
  • #58
So does this solution make sense to you?
 

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  • #59
haruspex said:
a1+a2= -a.
Jpyhsics said:
So does this solution make sense to you?

I again tried solving that solution with the system of equations:

a1+a2= -a and a2 = 2a1

and I got a1 = (-1/3)a which is still incorrect despite every step seeming to be correct.

Also do we need to use the numerical value for m1 at all?
 
  • #60
FriedChicken885 said:
and I got a1 = (-1/3)a which is still incorrect despite every step seeming to be correct.
hmm.. that is the answer I get.
FriedChicken885 said:
Also do we need to use the numerical value for m1 at all?
No. Only the ratio of the masses can be relevant.
 
  • #61
Jpyhsics said:
So does this solution make sense to you?
That is the same as the general equation I obtained.
 
  • #62
haruspex said:
That is the same as the general equation I obtained.
So I plugged in my values and it was wrong, so I don't really know what else to do.
 

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  • #63
haruspex said:
hmm.. that is the answer I get

Okay, thank you very very very much for all of your help!
 
  • #64
Should one not consider that the tension supporting the hanging mass is no longer parallel to the vertical side of the table but at an angle?
Also, I think that ##g=9.81 ~m/s^2## in the expression posted by OP in #62 should be replaced by an effective acceleration. This problem can be solved quite simply in the accelerated frame with additional fictitious horizontal forces ##-m_i\vec a_0## acting on masses ##m_i##. Here, ##\vec a_0## is the given horizontal acceleration of the table.
 
  • #65
kuruman said:
Should one not consider that the tension supporting the hanging mass is no longer parallel to the vertical side of the table but at an angle?
we are asked for the accelerations immediately after the surface has started to accelerate. The string is still vertical.
kuruman said:
Also, I think that ##g=9.81 ~m/s^2## in the expression posted by OP in #62 should be replaced by an effective acceleration.
I don't see why. Do you get a different answer? If so, please post your solution.
 
  • #66
I don't get a different answer, but I am bothered by the fact that one writes the same equation for the hanging mass whether the pulley supporting it accelerates or not. When the pulley accelerates, the hanging mass must have a horizontal acceleration at t = 0 because its horizontal position changes a moment later. Should this not affect the tension? I need to think about this some more.

On Edit: OK, I got it. At t = 0 the horizontal acceleration is instantaneously zero and then changes as it reaches a constant value in the steady state.
 
Last edited:
  • #67
kuruman said:
At t = 0 the horizontal acceleration is instantaneously zero
Right.
kuruman said:
then changes as it reaches a constant value in the steady state.
Or maybe oscillates.
 

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