Different tensions in a pulley system and acceleration

Click For Summary

Homework Help Overview

The discussion revolves around a pulley system involving two crates and a pulley with mass. The original poster is tasked with finding the tensions in the system, specifically Tension 1 and Tension 2, while also considering the mass of the pulley.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • The original poster presents simultaneous equations related to the system's dynamics, including forces and torques. Some participants question the correctness of the angular acceleration derived by the original poster. Others suggest alternative approaches to solve for the acceleration of the crates and the tensions, while also addressing potential sign inconsistencies in the equations.

Discussion Status

Participants are actively engaging with the original poster's attempts, providing feedback on the equations and suggesting ways to clarify the coordinate system and signs used in the calculations. There is a recognition of the complexity of the problem, with various interpretations being explored without a clear consensus on the correctness of the expressions derived for T1 and T2.

Contextual Notes

Participants note the importance of maintaining consistent signs in the equations and the implications of the mass of the pulley on the tensions. The original poster is also instructed to show that T1 equals T2 when the mass of the pulley is zero, adding another layer of complexity to the discussion.

fredrogers3
Messages
40
Reaction score
0

Homework Statement


Here is the picture: http://www.webassign.net/giocp1/8-p-058.gif
I am to find Tension 1 ( that between crate one and the pulley) and tension 2 (that between crate two and the pulley). The mass of the pulley is MP.

Homework Equations


See below




The Attempt at a Solution


I have found 4 simultaneous equations:
T1=M1ax1
Fn1-fg1=0
T2-fg2=-m2ay2
Torque:
R(T1-T2)= I*angular acceleration
I also found that with respect to the acceleration of m2, the angular acceleration of the pulley is (-ay2/R)
Are these correct so far? It seems that after I do my algebra my answer for T1 does not make sense. For instance, it comes out non-dependent on mass 2.

Thanks
 
Physics news on Phys.org
I don't think you have the angular acceleration of the pulley correct.
How did you get it?
 
Simon Bridge said:
I don't think you have the angular acceleration of the pulley correct.
How did you get it?

linear acceleration= angular acceleration * R
 
Simon Bridge said:
I don't think you have the angular acceleration of the pulley correct.
How did you get it?

Instead, I first solved for the acceleration of the crates:
I get, m2g/(m1+m2+.5mp)

Then, I subbed it in for a in the equations for T1 and T2.

I get,
T1=m1*m2g/(m1+m2+.5mp)
T2= (-m2*m2*g/(m1+m2+.5mp))+m2g
Additionally, the expression for T2 looks "too negative."
However, the next part of the question tells me to show that T1=T2 when mp =0. I can't seem to get this to work, though, with the expressions I derived.
 
Last edited:
Oh I see what's happened -have you been careful about keeping the signs consistent?

i.e. you appear to be making the +y and +x directions positive so m2 is going to pick up speed downwards, so it's acceleration is negative, while m1 is going to pick up speed to the right, so it's acceleration is positive. Thus ##a=a_1=-a_2##? But I cannot see any such reasoning in what you've told me.

Why not pick your coordinate system to make the math easy?
(It also makes it easier to mark ;) )

i.e.
for m1, pick +ve to the right so ##T_1=m_1a## ... see how we don't need the subscripts?
for the pulley, pick +ve to be clockwise, to be consistent with m1.
(You should express the entire thing in linear terms too - don't leave it as ##R(T_2-T_1)=I\alpha##)
for m2, pick +ve downwards so that ##m_2g-T_2=m_2a##
... notice how I don't mess about with this ##F_g## stuff - just write out ##mg## right away?
I label fbds like that too: having to keep track of notation just gives more opportunity to make mistakes.

3 equations, 3 unknowns.
 
Simon Bridge said:
Oh I see what's happened -have you been careful about keeping the signs consistent?

i.e. you appear to be making the +y and +x directions positive so m2 is going to pick up speed downwards, so it's acceleration is negative, while m1 is going to pick up speed to the right, so it's acceleration is positive. Thus ##a=a_1=-a_2##? But I cannot see any such reasoning in what you've told me.

Why not pick your coordinate system to make the math easy?
(It also makes it easier to mark ;) )

i.e.
for m1, pick +ve to the right so ##T_1=m_1a## ... see how we don't need the subscripts?
for the pulley, pick +ve to be clockwise, to be consistent with m1.
(You should express the entire thing in linear terms too - don't leave it as ##R(T_2-T_1)=I\alpha##)
for m2, pick +ve downwards so that ##m_2g-T_2=m_2a##
... notice how I don't mess about with this ##F_g## stuff - just write out ##mg## right away?
I label fbds like that too: having to keep track of notation just gives more opportunity to make mistakes.

3 equations, 3 unknowns.


So are my expressions for T1 and T2 correct, minus the sign problems?
 
Can't tell without doing it for you - it is up to you to check.
I was expecting to see an "R" in there from the moment of inertia of the pulley though.
 
Simon Bridge said:
Can't tell without doing it for you - it is up to you to check.
I was expecting to see an "R" in there from the moment of inertia of the pulley though.

I did it the way you told me and I got the same answer for T2.
 
You are getting:
T2= (-m2*m2*g/(m1+m2+.5mp))+m2g
... which is: $$T_2= -\frac{m_2^2g}{m_1+m_2+\frac{1}{2}m_p}+m_2g$$ ... well, looking closer, that should be a positive number. Perhaps the minus sign here is a red herring?

I'm getting $$T_2 = \frac{m_2(m_p+2m_1)g}{m_p+2m_1 + 2m_2 }$$ ... which is the same.
Looks like it you did track the minus signs correctly after all! (Though I could have made an algebra error myself ;) ).

You can check my working:

FBD for mass #1: ##T_1=m_1a## ...(1)
FBD for mass #2: ##m_2g-T_2=m_2a## ...(2)
FBD for pulley: ##R(T_2-T_1)=(\frac{1}{2}m_pR^2)(a/R) = \frac{1}{2}Rm_pa## ...(3)
... ahah: the R cancels out!

... from (3)
##\Rightarrow a = 2(T_2-T_1)/m_p## ...(4)

... sub into (1) and (2)
##T_1 = 2m_1(T_2-T_1)/m_p##
## \Rightarrow (1+2m_1/m_p)T_1 = (2m_1/m_p)T_2## ...(5)

##m_2g-T_2=2m_2 (T_2-T_1)/m_p ##
##\Rightarrow (1+2m_2/m_p)T_2 = m_2g+(2m_2/m_p)T_1## ...(6)

To find ##T_2##:
... solve for ##T_1## in (5) and sub into (6) gives:

$$\left ( 1+\frac{2m_2}{m_p}\right )T_2 = m_2g+\frac{2m_2}{m_p}\frac{2m_1/m_p}{1+2m_1/m_p}T_2\\
\Rightarrow \left ( m_p+2m_2\right )(m_p+2m_1)T_2 = m_2m_p(m_p+2m_1)g+4m_1m_2T_2\\
\Rightarrow T_2 = \frac{m_2(m_p+2m_1)g}{m_p+2m_1 + 2m_2 }$$
 

Similar threads

  • · Replies 27 ·
Replies
27
Views
3K
  • · Replies 10 ·
Replies
10
Views
3K
  • · Replies 26 ·
Replies
26
Views
3K
  • · Replies 4 ·
Replies
4
Views
2K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 22 ·
Replies
22
Views
2K
  • · Replies 34 ·
2
Replies
34
Views
4K
  • · Replies 10 ·
Replies
10
Views
5K
  • · Replies 5 ·
Replies
5
Views
3K
  • · Replies 18 ·
Replies
18
Views
1K