What is the last relation in this tension problem?

In summary, the conversation is about a physics problem involving finding the missing relation in order to solve for tension. The person asking for help provides links to their question and a picture. The solution involves drawing a free body diagram and using Newton's laws to solve for the unknown tension force. Some confusion arises about the role of T3 in the equations, but it is eventually clarified that T3 is simply an extension of the same reciprocal gravitational force and does not affect the distribution of tensions from the first two cords.
  • #1
Theorγ
57
0
My problem is explained from the below yahoo answers link. I know I'm suppose to follow the template, but my question is kind of long to write, and being so that I already wrote it up on Yahoo Answers, I thought it would be easier if I just list the link.

http://answers.yahoo.com/question/index;_ylt=Alqivg5bWrdr5QJRc5UwitTIDH1G;_ylv=3?qid=20110106181202AAHJqvJ

My problem is not on finding the actual tension, but is just the missing relation in order to solve the tension. I understand how to solve the tension, just that I am currently being hindered by not knowing the last relation.

Edit: Also you can skip the first paragraph that I wrote on Yahoo Answers for I have provided the picture to which the paragraph describes below:
http://www.webassign.net/serpop/p4-24alt.gif
 
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  • #2
The 3rd equation you are looking for can be derived by taking a free body diagram of the hanging mass, identify the forces acting on that mass, and use Newton 1 to solve for the unknown tnsion force T3 acting on that mass.
 
  • #3
PhanthomJay said:
The 3rd equation you are looking for can be derived by taking a free body diagram of the hanging mass, identify the forces acting on that mass, and use Newton 1 to solve for the unknown tnsion force T3 acting on that mass.

I drew a free body diagram but I see nothing new, just the gravitational force going downwards, and the tension force going upwards; is there something I'm not seeing?
 
  • #4
Solve for T3 using Newton 1. But I just realized your first equation is wrong. In your first 2 equations, you are drawing a free body diagram of the joint. In so doing, the massweight does not enter into the equation. Watch your plus and minus signs also.
 
  • #5
So, it's easier for you to post a couple of links than it is to cut & paste & figure out how to show an image!

I suppose you want help with solving your problem too.

p4-24alt.gif


See, it's not all that difficult!
 
  • #6
PhanthomJay said:
Solve for T3 using Newton 1. But I just realized your first equation is wrong. In your first 2 equations, you are drawing a free body diagram of the joint. In so doing, the massweight does not enter into the equation. Watch your plus and minus signs also.

actually, the equations I wrote did include the mass weight as I set the combined vertical tensions equal to the gravitational force of the mass weight
 
  • #7
Theorγ said:
actually, the equations I wrote did include the mass weight as I set the combined vertical tensions equal to the gravitational force of the mass weight

T3=-mg

and

T1sin40° + T2sin50° + T3 = 0
 
  • #8
SammyS said:

T3 = -mg

and

T1sin40° + T2sin50° + T3 = 0

Wait how can T3 alone be the reciprocal force of the gravitational force? Shouldn't the reciprocal force of the gravitational force be equal to the vertical combination of the tension forces opposite to the gravitational force?

T1sin40° + T2sin50° + T3 = -mg

Because T3=-mg alone means that T1sin40° + T2sin50° has to be equal to mg for the equation you wrote to equal zero.
 
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  • #9
Theorγ said:
Wait how can T3 alone be the reciprocal force of the gravitational force? Shouldn't the reciprocal force of the gravitational force be equal to the vertical combination of the tension forces opposite to the gravitational force?

T1sin40° + T2sin50° + T3 = -mg
No. If you look at the entire system, T3 is internal to the system, and does not enter into the equilbrium equation. Only the support forces and gravity force are external to the system.
Because T3=-mg alone means that T1sin40° + T2sin50° has to be equal to mg for the equation you wrote to equal zero.
Yes.

As a note, at the risk of confusing you, when you draw free body diagrams of part of the system, the internal forces become external to that portion of the system when you apply Newton's laws, Fnetexternal = ma (where a =0 in this problem).
 
  • #10
Theorγ said:
Wait how can T3 alone be the reciprocal force of the gravitational force? Shouldn't the reciprocal force of the gravitational force be equal to the vertical combination of the tension forces opposite to the gravitational force?

T1sin40° + T2sin50° + T3 = -mg

Because T3=-mg alone means that T1sin40° + T2sin50° has to be equal to mg for the equation you wrote to equal zero.

SammyS said:

T3=-mg

and

T1sin40° + T2sin50° + T3 = 0

As I look back on what I wrote, it would have been better if I had written things a bit differently. What I posted should give the correct answer, but the following will explain things better (I hope.)

A Free Body Diagram of the hanging mass, m1, has force T3 upward, and the force of gravity, m1g pointing downward.

This gives T3 - m1g = 0  →  T3 = m1g . (Yes, the sign is different than in my previous post, but indicates that as far as m1 is concerned, T3 is upward.)

As PhanthomJay points out, a Free Body Diagram of the joint where the three cables meet, does not include m1 directly. It has the three cables with tensions T1, T2, and T3, meeting at the given angles. The vertical components of the forces involved gives:

T1sin40° + T2sin50° - T3 = 0  →  T1sin40° + T2sin50° - m1g = 0  →  T1sin40° + T2sin50° = m1g

I hope that is clearer.
[ ][ ]
 
  • #11
Ohh I see now, so T3 in a way had no affect on the distribution of the tensions from the first two cords, and should have been treated as just an extension of the same reciprocal gravitational force. Thank you both for taking your time to explain this to me!
 

FAQ: What is the last relation in this tension problem?

What is the last relation in this tension problem?

The last relation in a tension problem is typically the equation that is used to solve for the unknown variable.

Why is the last relation important in a tension problem?

The last relation is important because it allows us to find the solution to the tension problem by using mathematical equations and principles.

What are some common equations used as the last relation in tension problems?

Some common equations used as the last relation in tension problems include Newton's Second Law, Hooke's Law, and the Pythagorean Theorem.

How do you determine which equation to use as the last relation in a tension problem?

The equation used as the last relation in a tension problem will depend on the given information and what you are trying to solve for. It is important to carefully read the problem and identify the unknown variable before selecting the appropriate equation.

What steps should be taken after identifying the last relation in a tension problem?

After identifying the last relation, you should plug in the known values and solve for the unknown variable. It is also important to check your answer and make sure it is reasonable.

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