Find work given two conservative forces and a nonconservative force

  • #1
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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  • #2
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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  • #3
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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  • #4
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.
 
  • #5
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.
 
  • #6
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?
 
  • #7
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.
 
  • #8
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!
 
  • #9
(Is there any way I can mark a thread as solved? Still new to this forum :smile:)
 
  • #10
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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FAQ: Find work given two conservative forces and a nonconservative force

What is a conservative force?

A conservative force is a force that does work on an object in such a way that the work done is independent of the path taken by the object. The work done by a conservative force depends only on the initial and final positions of the object. Examples include gravitational force and spring force.

What is a nonconservative force?

A nonconservative force is a force for which the work done depends on the path taken. This means that if an object is moved along different paths between the same two points, the work done by the nonconservative force can vary. Examples include friction and air resistance.

How do you calculate the work done by multiple forces?

To calculate the total work done by multiple forces, you can sum the work done by each individual force. For conservative forces, the work can be determined using potential energy differences, while for nonconservative forces, you can calculate the work directly from the force and displacement. The total work is given by the equation: W_total = W_conservative1 + W_conservative2 + W_nonconservative.

What is the work-energy theorem?

The work-energy theorem states that the total work done by all forces acting on an object is equal to the change in its kinetic energy. This can be expressed mathematically as W_total = ΔKE, where ΔKE is the change in kinetic energy. This theorem can be applied to analyze systems involving both conservative and nonconservative forces.

How do you determine the potential energy associated with conservative forces?

The potential energy associated with conservative forces can be determined by integrating the force with respect to displacement. For gravitational force, the potential energy can be calculated using the formula U = mgh, where m is mass, g is the acceleration due to gravity, and h is the height above a reference point. For other conservative forces, the specific potential energy function must be derived based on the force's characteristics.

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