Man connected to harness standing on plank

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SUMMARY

The discussion revolves around a physics problem involving a professor seated in a harness connected to a rope and pulley system, analyzing forces on a plank supported by a hinge. Key variables include the professor's mass (75 kg), the plank's mass (15 kg), and the length of the plank (2 m). Participants emphasize the importance of drawing accurate Free Body Diagrams (FBDs) for both the professor and the plank, noting that the tension (T) in the rope is not equal to the professor's weight due to the harness's support. The conversation highlights the need for clarity in understanding the forces acting on the system.

PREREQUISITES
  • Understanding of Free Body Diagrams (FBDs)
  • Knowledge of torque and equilibrium equations (ΣMhing = 0)
  • Familiarity with tension in ropes and pulley systems
  • Basic principles of mechanics and forces
NEXT STEPS
  • Study the principles of torque and how to calculate it in static systems
  • Learn about Free Body Diagram techniques for complex systems
  • Explore the effects of tension in ropes connected to multiple masses
  • Review mechanics of materials, focusing on forces and moments
USEFUL FOR

Students in physics or engineering courses, educators teaching mechanics, and anyone interested in understanding static equilibrium and forces in systems involving pulleys and harnesses.

Jtwa
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Homework Statement


A professor (m= 75 kg )is seated on a light harness connected to a rope and pulley system. The professor's feet touch a uniform plank (mplank = 15kg) which is supported by a hinge at the wall. A bucket (M) is suspended from the right end of the plank.

m = 75kg
mplank = 15kg
l = 2m
L = 4.9m

Find: Label all the forces on a FBD
Find: T if M=0
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Homework Equations


ΣMhing = 0

The Attempt at a Solution


I took the moment about the hinge and looked at the man by himself. I think I'm drawing my FBD diagram incorrectly.

KpST7JT.png
 
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Hello JT, :welcome:

From your drawing it's clear that the rope is attached to the end of the plank. That should be in the problem statement !

If prof is sitting in the harness, I expect one more force in his FBD. Otherwise I think you have most of it covered. Fry is the only horizontal force I see, so it may well be 0...
 
Have you tried writing the equations for the torques about the hinge end of the plank?
Also, you know that T is constant throughout the length of the rope.
This greatly would simplify the solution since you don't need to consider the forces
acting through the hinge.
 
J Hann said:
Also, you know that T is constant throughout the length of the rope.
Well, not quite. Since the rope is attached to the end of the plank, the section of rope below the plank will be at a different tension.
 
Yes, but the problem statement reads M = 0
 
BvU said:
Yes, but the problem statement reads M = 0
Which post is that in response to? It does not appear to contradict my post #4.
Also, that M=0 condition is only for the final part of the question.
 
##T## is the tension in the section of rope above the plank. The section below will have a tension equal to ##Mg## which will generally be different than ##T##, particularly if ##M=0##.
 
You are absolutely right :smile: ! (Haru and T2)
 
Since the rope is connected to the man, why isn't T=(mass of man)*g
 
  • #10
Part of his weight is taken by the harness !
 
  • #11
I'm still having trouble understanding this question. Can someone draw a FBD ? Is Normal Force suppose to be on the FBD?
 
  • #12
BvU said:
Part of his weight is taken by the harness !
No, that's why it could have been mg. The reason that T is not mg is that not all of the weight is taken by the harness.
 
  • #13
Jtwa said:
I'm still having trouble understanding this question. Can someone draw a FBD ? Is Normal Force suppose to be on the FBD?
An FBD relates to a single rigid body. There are two appropriate FBDs here, one for the man and one for the plank.
Your diagram depicted both, which is ok except that where those two bodies interact you need to show the equal and opposite forces between them.
 
  • #14
Part of his weight = not all of the weight
 
  • #15
BvU said:
Part of his weight = not all of the weight
It's a question of emphasis in English. If you write that the reason that T is not mg is that part of his weight is taken by the harness it implies that the part taken by the harness accounts for the discrepancy. If you mean that the part not taken by the harness accounts for it then you need to write "only part of his weight...".
 
  • #16
Didn't want to give too much emphasis, just get the OP to think it over.

Non-native english typist... But then again, weren't you in Australia ?
:smile:
 
  • #17
BvU said:
Didn't want to give too much emphasis, just get the OP to think it over.

Non-native english typist... But then again, weren't you in Australia ?
:smile:
I am now.
 
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  • #18
Can't beat Oxford English :cool:
 

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