How Does Integrating mgR Relate to Force and Work in a Semicircle?

AI Thread Summary
The discussion focuses on the integration of gravitational force in the context of work done on a particle moving along a semicircular path. The key point is that the work done is calculated using the integral W = ∫F·dr, where the force is mg cos(θ) and the displacement is represented in terms of the angle θ. Participants clarify that work is not the same as external force and emphasize that the integration accounts for the varying angle as the particle moves. The confusion arises around the limits of integration and the assumption of angles, particularly whether the angle is 90 degrees. Ultimately, the work done is expressed as mgR sin(θ), highlighting the importance of correctly interpreting the semicircular motion.
omarMihilmy
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Okay so the answer in b) is mgR how is this possible when we integrate ?

The work is the external force right?
Secondly the F inside the integral is the mg sin(theta) the force of gravity?
dr ---> pi R (semicircle)
 
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The force, according to the problem, is mg cos(\theta). Are you saying you do not believe that?

I don't know what you mean by "dr--> pi R". First, in this problem you are dealing with d\vec{r}, not "dr". (Since we are moving on a circle, r is constant and dr= 0!) On a circle of radius r, x= r cos(\theta) and y= r sin(\theta) so that \vec{r}= r cos(\theta)\vec{i}+ r sin(\theta)\vec{j} and d\vec{r}= -r sin(\theta)\vec{i}+ r cos(\theta)\vec{j} d\theta

No, the "work" is NOT the "external force". Work is not force. And since there is only one force here, I don't know what you mean by "external" force.
 
No I believe that no problem. Force done by pulling the small particle is mgcos(θ)

my problem is with the work done by that force to pull the particle is the W = ∫F.dr
This is the work done by the external force in puling the particle which should be the mgcos(θ) x the distance moved

We integrate here because the force done varies with the displacement moved due to the angle.

In the integral I will add the which force the gravitational force which is mg j
the dr⃗ =−rsin(θ)i⃗ +rcos(θ)j⃗ dθ

when we integrate this it will lead us to mgr be outside the integral and cosine(θ) which integrate to sin(θ)

Work done is mgRsin(θ) not mgR

or did he assume that the angle is 90 which is 1 ?

please help with that work part and correct me if I ma giving an faulty information
 
omarMihilmy said:
or did he assume that the angle is 90 which is 1 ?
It says: "... from the bottom to the top", so what is the range for theta?
 
180 sin180 is 0 so the whole thing is zero?
 
omarMihilmy said:
180 sin180 is 0 so the whole thing is zero?
No, not 180. It's a half cylinder lying on its flat side.
 
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Its a semi-circle with 180 degrees
A full circle is 360
Quarter is 90

Cant argue with that!
 
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