Solving for Acceleration and String Forces on Incline with Two Masses

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Homework Help Overview

The discussion revolves around a physics problem involving two masses connected by strings and pulleys on an incline. The original poster describes a scenario where one mass is heavier than the other, and they are trying to determine the acceleration of the lighter mass and the forces in the strings. The setup includes a frictionless ramp and massless strings and pulleys, which complicates the analysis.

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  • Mixed

Approaches and Questions Raised

  • Participants explore the forces acting on each mass and the role of the pulley system. There is a focus on the relationship between the tensions in the ropes and the accelerations of the masses. Questions arise about the assumptions made regarding the equality of tensions and the influence of the pulley on the motion of the masses.

Discussion Status

Participants are actively discussing the relationships between the tensions and accelerations of the masses. Some have suggested re-evaluating the assumptions about the tensions in the ropes, while others are attempting to derive the correct relationships between the accelerations of the two masses. There is an ongoing exploration of how the pulley affects the system dynamics.

Contextual Notes

There are indications of confusion regarding the influence of the pulley on the system, particularly in terms of how the tensions differ and how the accelerations relate to each other. The original poster has expressed difficulty in arriving at a solution, and there are references to textbook answers that differ from their calculations.

stunner5000pt
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Tension Problem Please help!

Ok so i got this question

Look at the attached diagram
Althoughin the diagram i drew it doesn't look like it , Mass 1 on the incline is heavier than Mass 2 and the acceleration is to the left.

The ramp is frictionless and the strings and pulleys are assumed to be massless
Find the acceleration on m2 and the string forces.

Now normally i wouldn't have trouble iwht something like this but that extra pulley throws me off

normally i'd think for the sum of the forces on mass 1

[tex]M_{1}a = M_{1} g Sin \theta - T[/tex]
and
[tex]M_{2}a = T - M_{2} g[/tex]

this however does not yield the answer after i plugged in Mass 1 = 0.4kg, Mass 2 = 0.2kg, and Theta = 30 degrees.

COuld you perhaps point out where my mistake lies and point me in the right direction. How does that left pulley influence that motion.

For the left pulley considering the mass and pulley and the wall alone

[tex]M_{1} g - T = M_{1} a[/tex] and
T = reaction force of the wall??

Am i going off on a tangent, is this totally necessary for finding the acceleration on M2??
 

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There are two distinct ropes in this scenario. Each rope has its own tension call it T1 and T2. Realize that the tension of the ropes is the same through the entire length of the rope (since this is an ideal situation).

Your mistake comes from assuming that the tension on M2 is the same as the tension on M1.. but they are two distinct ropes.

Set up FBD's for M1 and M2 keeping in mind that T1 does not necessarily equal T2.

hint: the acceleration of that pulley equals the acceleration of M2

edit: oops forgot the pulleys were massless so the FBD for the pulley doesn't help, but the rest still stands
 
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acceleration constraint

stunner5000pt said:
normally i'd think for the sum of the forces on mass 1

[tex]M_{1}a = M_{1} g Sin \theta - T[/tex]
and
[tex]M_{2}a = T - M_{2} g[/tex]
Since the masses are connected by ropes and a pulley, their accelerations are related. You assume that they are equal. Rethink that assumption.

Hint: If [itex]M_1[/itex] slides a distance x down the ramp, how far does the pulley (and thus [itex]M_2[/itex]) slide down?

Edit: That's not your only mistake, as MathStudent points out: The ropes have different tensions.
 
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hmm.. ok

so according to what mathstudent says then it would look something like this for the mass 1

[tex]M_{1} a_{1} = M_{1}g Sin \theta - T_{1}[/tex]
but what is T1?

So since the pulley is massless then the two tensions are equal, should they be because if the pulley had a mass

[tex]M_{p} = M_{p} g Sin \theta + 2T_{1} - T_{2}[/tex]
Something is wrong here isn't it ??
 
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stunner5000pt said:
so according to what mathstudent says then it would look something like this for the mass 1

[tex]M_{1} a_{1} = M_{1}g Sin \theta - T_{1}[/tex]
but what is T1?
It's an unknown which you will solve for, just like T2 and acceleration.

So since the pulley is massless then the two tensions are equal, should they be because if the pulley had a mass

[tex]M_{p} = M_{p} g Sin \theta + T_{1} - T_{2}[/tex]
Something is wrong here isn't it ??
Yes, something is wrong: (1) the mass of the pulley is zero; (2) there are three rope segments exerting force on the pulley. (The tensions are not equal; but the net force on the pulley is zero.)
 
Doc Al said:
It's an unknown which you will solve for, just like T2 and acceleration.


Yes, something is wrong: (1) the mass of the pulley is zero; (2) there are three rope segments exerting force on the pulley. (The tensions are not equal; but the net force on the pulley is zero.)
I put a 2 in front of the T1 term for the rope does that make the difference??
 
stunner5000pt said:
I put a 2 in front of the T1 term for the rope does that make the difference??
Of course.
 
Doc Al said:
Of course.

So the 2 is correct?? because the pulley feels 2 tensions in the same direction due to the mass looping around it ?/

So then taht gives me

[tex]M_{1} a_{1} = M_{1} g Sin \theta - T_{1}[/tex]
[tex]M_{2} a_{2} = T_{2} - M_{2} g[/tex]
[tex]2T_{1} = T_{2}[/tex]

But the solution for a1 and a2 is still impossible
 
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stunner5000pt said:
So the 2 is correct?? because the pulley feels 2 tensions in the same direction due to the mass looping around it ?/
Yes, the 2 is correct. Picture an imaginary box enclosing the massless pulley: You'll see three ropes sticking out. Each rope exerts its tension on whatever is in the box. Since one rope loops around the pulley, it pulls twice. [itex]\Sigma F = 2T_1 - T_2 = m_{pulley}a = 0[/itex]. So: [itex]T_2 = 2T_1[/itex].
 
  • #10
stunner5000pt said:
So then taht gives me

[tex]M_{1} a_{1} = M_{1} g Sin \theta - T_{1}[/tex]
[tex]M_{2} a_{2} = T_{2} - M_{2} g[/tex]
[tex]2T_{1} = T_{2}[/tex]

But the solution for a1 and a2 is still impossible
You give up too easily! :smile:

Follow my advice in post #3 and figure out the relationship between a1 and a2. (And be sure to use a consistent sign convention.)
 
  • #11
i'm still here aren't i! :-p

anyway i was just thinking of what you posted last : if mass 1 moxed x metres down the ramp how far down will the pulley move and I'm ... baffled

i can certainly find the relationship between a1 and a2 as follows
[tex]a_{1} = g Sin\theta - \frac{2M_{2}g}{M_{1}} - \frac{2M_{2}a_{2}}{M_{1}}[/tex]

but if the mass 1 moved x down the ramp then ... the pulley would move half as much (just a guess there, I am not sure) please help

thank you
 
  • #12
stunner5000pt said:
but if the mass 1 moved x down the ramp then ... the pulley would move half as much (just a guess there, I am not sure) please help
Exactly! So what does that tell you about how the two accelerations relate to each other?

Note: Guessing is OK to start. But don't stop there. Convince yourself that it's true by drawing the picture at two different points. (Or just play with a piece of string until you can visualize it.)
 
  • #13
I see how that happens because the pulley will feel twice a tension force from the left and half as much on the right so it will accelerate 1/2 as much as the mass 1 does because of the tension forces. SO then as a result of this happening

[tex]d = v t , v = at , d = at^2[/tex]
for mass 1

[tex]x = a_{1} t^2[/tex]
for the puller
[tex]\frac{x}{2} = a_{2} t^2[/tex]

equating these two gets [tex]2a_{2} = a_{1}[/tex]

so then i sub this into the earlier expression
[tex]a_{1} = g Sin\theta - \frac{2M_{2}g}{M_{1}} - \frac{2M_{2}a_{2}}{M_{1}}[/tex]

and i get [tex]2a_{2} = \frac{g}{2} - g - a_{2}[/tex]
which yields a2 = -g/6 and the answer is the back of the book is g/9??
is there something else with the acceleration tht i have not accounted for ??
 
  • #14
stunner5000pt said:
but if the mass 1 moved x down the ramp then ... the pulley would move half as much (just a guess there, I am not sure) please help

thank you

You're right on the money there. This might make it clearer :

[tex]x_1 = 2x_2[/tex] where the subscripts refer to mass 1 and 2 respectively.

Differentiating twice with respect to time,

[tex]\ddot{x_1} = 2\ddot{x_2}[/tex]

Does that tell you enough about the relationship of the accelerations ?
 
  • #15
stunner5000pt said:
I see how that happens because the pulley will feel twice a tension force from the left and half as much on the right so it will accelerate 1/2 as much as the mass 1 does because of the tension forces. SO then as a result of this happening

[tex]d = v t , v = at , d = at^2[/tex]
for mass 1

[tex]x = a_{1} t^2[/tex]
for the puller
[tex]\frac{x}{2} = a_{2} t^2[/tex]

equating these two gets [tex]2a_{2} = a_{1}[/tex]

so then i sub this into the earlier expression
[tex]a_{1} = g Sin\theta - \frac{2M_{2}g}{M_{1}} - \frac{2M_{2}a_{2}}{M_{1}}[/tex]

and i get [tex]2a_{2} = \frac{g}{2} - g - a_{2}[/tex]
which yields a2 = -g/6 and the answer is the back of the book is g/9??
is there something else with the acceleration tht i have not accounted for ??

I managed to get the book answer. Let us see your force equations. There should be two equations with two unknowns, the tension in the string attached to mass 2 and the acceleration of mass 2.
 
  • #16
here are the force equations
for mass 1 on the left on the ramp
[tex]M_{1} a_{1} = M_{1} g Sin \theta - T_{1}[/tex]

for the mass 2 on on the right
[tex]M_{2} a_{2} = T_{2} - M_{2} g[/tex]

and the relationships between tension and accelerations
[tex]2T_{1} = T_{2}[/tex]
[tex]a_{1} = 2a_{2}[/tex]
 
  • #17
finally got a2

i thank you for all the help you have given me really appreciate it :smile:
 

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