Calculating tensions and acceleration

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Homework Help Overview

The problem involves two masses, M1 and M2, connected by a string over a pulley, with M1 sliding on a table and M2 falling under gravity. The pulley is a solid cylinder, and the scenario considers both frictionless and frictional cases, requiring calculations of tensions and accelerations in both situations.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants discuss the net forces acting on the masses and the tensions in the string, with some attempting to derive equations for acceleration and tension based on free body diagrams.
  • Questions arise regarding the treatment of tensions as internal forces and the implications for the overall force balance.
  • Some participants suggest substituting acceleration into tension equations and simplifying, while others question the validity of this approach.
  • There is exploration of the moment balance on the pulley and the need for separate equations for each mass and the pulley.

Discussion Status

The discussion is ongoing, with participants providing guidance on the need for a moment balance and separate equations. There are differing interpretations of the relationships between tensions, and some participants are clarifying their understanding of the equations involved.

Contextual Notes

Participants note that part (a) of the problem is not fully resolved, and there are concerns about the assumptions made regarding the pulley and the forces acting on it. The complexity of the problem is acknowledged, particularly in the transition from part (a) to part (b).

shepherd882
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Homework Statement


A mass M1 is sliding across a table with coefficient of kinetic friction μk. A string is tied to this mass and runs over a pulley, drops vertically and is tied to another mass M2 which is falling. The pulley is connected to the table by a support. The pulley is a solid cylinder of mass M3, radius R. See figure. As the figure indicates, you may assume that the string is tied to the midpoint of both masses, that it runs horizontally from M1 to the pulley and vertically from the pulley to M2. You may also assume that the mass M1 is not tipping over as it slides.
pulley.jpg

a) Assume the string slips over the pulley with zero friction, and that the pulley is not rotating. Calculate the magnitude of the acceleration of M1 and M2. (This is the same for both masses.) Also find the tensions T1 in the string attached to M1 and T2 in the string attached to M2. Express your answers in terms of g and the various parameters given in the question.
b) Now assume that the string runs over the pulley without slipping, making the pulley rotate with increasing angular speed. Assume the pulley is attached to the table by a support which allows it to rotate on an axle with no friction between the pulley and axle. Calculate the magnitude of the acceleration of the masses M1 and M2 in this case. Also calculate the tensions T1 and T2 in this case.

Thanks for you help!

Homework Equations


Fnet = ma
Torque net = I*a
I = (MR^2)/2
Ff = uFn

The Attempt at a Solution


a) [/B]Fnet = ma
Fg2-T2+T1-Ff1 = (M1+M2)a
Fg2 - Ff1 = (M1+M2)a
M2g-uM1g = (M1+M2)a
(M2g-uM1g)/(M1+M2) = a

Fnet1 = T1-Ff1 = M1a
T1 = M1a + Ff1
T1 = M1a + uM1g
Fnet2 = Fg2 - T2 = M2a
T2 = Fg2 - M2a
T2 = M2g - M2a

b) Torque = I*a
T2R-T1R = Ia
a = [R^2/(M3R^2)]*(T2-T1)
a = (T2-T1)(2/M3)

T1 and T2 same as part a)?
 

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T1 and T2 same as part a)?
Simple answer: no. Some difference is needed for ... (fill it in)

[edit] by the way, part a) isn't finished yet !
 
In the first part of your analysis for part (a), the tensions should not be included in the overall tangential force balance because they are internal to the system.
 
BvU said:
Simple answer: no. Some difference is needed for ... (fill it in)

[edit] by the way, part a) isn't finished yet !

for part a), would i just substitute acceleration into each of the tension equations then simplify?
also for part b), the difference would be that mass 3 has the normal force at an angle which would add to the fnetx component. am i on the right track?
 
shepherd882 said:
for part a), would i just substitute acceleration into each of the tension equations then simplify?
Yes. You should get the same answer for both tensions. Do you?
also for part b), the difference would be that mass 3 has the normal force at an angle which would add to the fnetx component. am i on the right track?
No. This is not the right approach. You should start by doing a moment balance on the pulley. In part (b), you should have 3 separate balance equations: one for each mass, and one for the pulley.
 
Chestermiller said:
Yes. You should get the same answer for both tensions. Do you?
No. This is not the right approach. You should start by doing a moment balance on the pulley. In part (b), you should have 3 separate balance equations: one for each mass, and one for the pulley.

46008188_1032680056921313_5955096860279439360_n.jpg?_nc_cat=109&_nc_ht=scontent.fyvr3-1.jpg

That's what I got for T1 and T2 for part a) ...
 

Attachments

  • 46008188_1032680056921313_5955096860279439360_n.jpg?_nc_cat=109&_nc_ht=scontent.fyvr3-1.jpg
    46008188_1032680056921313_5955096860279439360_n.jpg?_nc_cat=109&_nc_ht=scontent.fyvr3-1.jpg
    12.4 KB · Views: 740
Chestermiller said:
Yes. You should get the same answer for both tensions. Do you?
No. This is not the right approach. You should start by doing a moment balance on the pulley. In part (b), you should have 3 separate balance equations: one for each mass, and one for the pulley.

46043809_183818689223175_8685283553165967360_n.jpg?_nc_cat=108&_nc_ht=scontent.fyvr3-1.jpg

Is this correct?
 

Attachments

  • 46043809_183818689223175_8685283553165967360_n.jpg?_nc_cat=108&_nc_ht=scontent.fyvr3-1.jpg
    46043809_183818689223175_8685283553165967360_n.jpg?_nc_cat=108&_nc_ht=scontent.fyvr3-1.jpg
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shepherd882 said:
View attachment 233904
That's what I got for T1 and T2 for part a) ...
That's not what I get. For part (a), I get ##T_1=T_2=T## with $$T=\frac{m_1m_2(1+\mu_k)}{(m_1+m_2)}g$$
This is equivalent to your result for ##T_2## but not for ##T_1##
 
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shepherd882 said:
View attachment 233905
Is this correct?
I can't read your handwriting, but the equations should read:
$$T_1-m_1g\mu_k=m_1a$$
$$m_2g-T_2=m_2a$$and, for the moment balance on the pulley:
$$T_2R-T_1R=I\frac{a}{R}$$
This gives you 3 equations in the three unknowns ##T_1##, ##T_2##, and a
 
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  • #10
Chestermiller said:
I can't read your handwriting, but the equations should read:
$$T_1-m_1g\mu_k=m_1a$$
$$m_2g-T_2=m_2a$$and, for the moment balance on the pulley:
$$T_2R-T_1R=I\frac{a}{R}$$
This gives you 3 equations in the three unknowns ##T_1##, ##T_2##, and a
I got those equations
45885830_521481118367409_8579983341753729024_n.jpg?_nc_cat=108&_nc_ht=scontent.fyvr3-1.jpg

How do you simplify this...?
 

Attachments

  • 45885830_521481118367409_8579983341753729024_n.jpg?_nc_cat=108&_nc_ht=scontent.fyvr3-1.jpg
    45885830_521481118367409_8579983341753729024_n.jpg?_nc_cat=108&_nc_ht=scontent.fyvr3-1.jpg
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  • #11
shepherd882 said:
I got those equations
View attachment 233909
How do you simplify this...?
You have one linear algebraic equation in one unknown ("a"); are you really saying that you don't know how to solve this equation for the unknown?
 

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