Calculating Work Against Attractive Force Along Semi-Circle Path

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The problem involves calculating the work done against an attractive force as a particle moves along a semi-circular path defined by a specific function. The force varies with the angle and is expressed in terms of a parameter related to the semi-circle's radius.

Discussion Character

  • Exploratory, Assumption checking, Problem interpretation

Approaches and Questions Raised

  • The original poster attempts to derive the work done using an integral approach, but questions arise regarding the interpretation of the differential distance element dr and the relationship between the force and the path taken.

Discussion Status

Participants are actively discussing the clarity of the problem statement and the interpretation of the variables involved. Some guidance has been offered regarding the definition of dr and its relevance to the path of the particle.

Contextual Notes

The original problem lacks a diagram, which some participants note may hinder understanding. There is also uncertainty about the source of the problem, as it is not from a textbook.

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A semi-circle is given by the function [tex]y=R cos(\frac{x\pi}{2R})[/tex]. An attractive force F at [tex]x = R[/tex] and [tex]y = 0[/tex] such that [tex]F(x, y) = F(R, 0) = 0[/tex] and [tex]F(x, y) = F(-R, 0) = F_{0}[/tex]. This force along the semi-circle, relative to its source, is given by [tex]F(\theta) = F_{0} sin(\theta/2)[/tex]. What amount of work is done against the force when a particle moves along the circle from [tex]\theta = 0[/tex] to [tex]\theta = \pi[/tex].
To find the work I have the equation
[tex]W = - \int^{\pi}_{0} F dr[/tex]
For the force I have the equation
[tex]F= F_{0} sin(\theta/2)[/tex]
For the distance from the particle to the orgin of the force I have
[tex]2 R sin(\theta/2)[/tex]
so for dr I have
[tex]2 R sin(\theta/2) d\theta[/tex]
Putting this all tegether I get
[tex]W = - \int^{\pi}_{0} F_{0} sin(\theta/2) 2 R sin(\theta/2) d\theta[/tex]
This rearanges to
[tex]W = -F_{0} R \int^{\pi}_{0} \left[1-cos(\theta) \right] d\theta[/tex]
Integrating I get
[tex]W = -F_{0} R \left[ \theta-sin(\theta) \right]^{\pi}_{0}[/tex]
This works out to
[tex]W = -F_{0} R \pi[/tex]
The answer I am suppose to get is
[tex]W = -F_{0} R[/tex]
What did I do wrong?
 
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The question doesn't make very much sense. Could you please reproduce the question exactly as it appears in the text, and also provide the name of the text ?
 
I rewrote the problem a little bit. I'm afraid it's still a little unclear without the diagram though. This question is not from a textbook.
 
I think the mistake you are making is in interpreting what dr refers to. This is an elemental distance traveled by the particle (along the semicircular path) - it is not an element of the distance of the particle from the origin. Also keep in mind that the angle between F and dr changes with the motion of the particle.
 

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