Find work given two conservative forces and a nonconservative force

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Homework Help Overview

The discussion revolves around a problem involving work done by conservative and non-conservative forces on a particle moving along different paths. The original poster attempts to understand the relationship between potential energy and work done in the context of the work-energy theorem.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants explore the implications of the work-energy theorem, questioning how work done by conservative and non-conservative forces affects the total energy of the system. Some participants raise concerns about the interpretation of potential energy changes and the relevance of non-conservative forces in the calculations.

Discussion Status

Participants are actively engaging with the problem, clarifying misunderstandings about the conditions of the particle's motion and the application of the work-energy theorem. There is a recognition of the need to differentiate between paths and the work done by various forces.

Contextual Notes

There are mentions of potential confusion regarding the initial and final states of the particle across different paths, as well as the specific work done by each force. The original problem statement is noted to be in a different language, which may have contributed to misunderstandings.

bremenfallturm
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Homework Statement
A particle starts from rest in the point ##A## to the point ##B## along four different paths according to the figure (see my post):
1. A conservative force ##F_{K1}## does work ##10J## on the particle
2. A conservative force ##F_{K2}## does work ##5## on the particle
3. A nonconservative force ##F_{IK}## does work ##-5J## on the particle.
Now assume all forces act at the same time on the particle, when it is moved along the path 4. Find the work done by ##F_{IK}## given that the particle stops at point ##B##
Relevant Equations
##U=\int_{\mathcal C} \vec F \cdot \vec dr##

##U=V(A)-V(B)## if a force is conservative and ##V## is a potential function for it

##U=\oint_{\gamma} \vec F \cdot \vec dr## for a closed curve ##\gamma##
The figure provided with the question is:
1715270384810.png

I set up the following equation for path 4
##U_{path 4}=U_{Fk1, path 4}+U_{Fk2, path 4}+U_{FIK, path 4}## where ##U_{FIK,AB}## is the unknown.
I know that the work will be the same regardless the path for conservative forces, so I have:
##U_{path 4}=10+5+U_{FIK, path 4} (J)##
The answer key says ##U_{FIK, path 4}=-15J## (no further solution given), but I do not understand why ##U_{path 4}## is ##0##, if I set up my equations correctly and interpret the answer key. I know that mechanical energy is conserved with conservative forces, and that the work done over a closed curve with conservative forces is 0.
How can I come to a reasoning that ##-15J## is correct?
Thanks!
 
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Since the particle starts from rest and stops at B, the work-energy theorem requires the total work done on the particle is zero.
 
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bremenfallturm said:
Homework Statement: A particle starts from rest in the point ##A## to the point ##B## along four different paths according to the figure (see my post):
1. A conservative force ##F_{K1}## does work ##10J## on the particle
2. A conservative force ##F_{K1}## does work ##10J## on the particle
3. A nonconservative force ##F_{IK}## does work ##-5J## on the particle.
The work done by ##F_{K1}## is mentioned twice and the work done by ##F_{K2}## is not mentioned at all. Please specify.
 
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kuruman said:
The work done by ##F_{K1}## is mentioned twice and the work done by ##F_{K2}## is not mentioned at all. Please specify.
Megasuperdupersorry, copy paste let me down. I've clarified, see #1.
 
Thank you for the clarification. You should cast the problem not in terms of potential energy changes because non-conservative forces cannot be derived from a potential energy function. Use the work-energy energy theorem approach as @Orodruin suggested in post #2. Note that
  1. The total work done by the conservative forces is independent of path.
  2. The work done by the non-conservative force along path 3 (= -5 J) is totally irrelevant to the answer.
 
kuruman said:
Thank you for the clarification. You should cast the problem not in terms of potential energy changes because non-conservative forces cannot be derived from a potential energy function. Use the work-energy energy theorem approach as @Orodruin suggested in post #2. Note that
  1. The total work done by the conservative forces is independent of path.
  2. The work done by the non-conservative force along path 3 (= -5 J) is totally irrelevant to the answer.
Alright! So for path (4), we simply know that
$$U_{1-2}=\underbrace{\frac{1}{2}mv_b^2}_{=0}-\underbrace{\frac{1}{2}mv_a^2}_{=0}$$
$$\implies 0=5+10+U_{FIk, path 4}\implies U_{FIk, path 4}=-15 J$$

I think I missed the fact that the work-energy theorem applies to all forces, I don't know why I've thought the other way around, it seems obvious now when I think about it. With the reservation of this being a dumb question, for the other three paths we also start and end at rest, but there is not zero work. That's, what I assume, from other unknown forces acting on the particle. We assume that they don't do any work on it for path (4), since the work-energy theorem is for the sum of all forces, or did I misunderstand the concept of it?
 
bremenfallturm said:
for the other three paths we also start and end at rest
No we don't. There is no such statement in the problem.
 
Orodruin said:
No we don't. There is no such statement in the problem.
Hm, okay. You're right, I re-read the statement. It says that the particle "stops" at B in situation 4 and "moves" to B in the other scenarios. It was even clearer in the original problem statement, which is not in English so I had to translate it. Thank you, I think I get it now!
 
(Is there any way I can mark a thread as solved? Still new to this forum :smile:)
 
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bremenfallturm said:
(Is there any way I can mark a thread as solved? Still new to this forum :smile:)
We are not formal in that regard. Once the OP (original poster) provides a solution as you have in post #6, that’s it. Thank you for your contribution and do come back. We are here to help.
 
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