Centripetal Force and Work: Understanding the Relationship

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Homework Help Overview

The discussion revolves around the relationship between centripetal force and work in the context of a ball being swung in a circular motion. The original poster presents a problem involving a 5kg ball moving in a circle with a specified radius and speed, asking about the work done by the centripetal force and the differences when considering a straight-line motion.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants explore the definition of work, questioning how it applies to circular motion versus linear motion. There are attempts to derive equations related to centripetal force and its implications for work done.

Discussion Status

Participants are actively engaging with the problem, offering guidance on reviewing definitions and clarifying concepts. There is an exploration of the reasons why work done in circular motion is considered zero, with some participants providing insights into the relationship between force and displacement.

Contextual Notes

There is a noted emphasis on understanding the definition of work and the conditions under which it is calculated, particularly regarding the direction of force and displacement. The original poster expresses uncertainty about the problem's wording and its implications.

EthanVandals
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Homework Statement


A 5kg ball is swung in a circle of radius .5 meters at a constant speed of 2 meters per second, how much work does the centripetal force do as the ball does once in a circle?If the ball were pushed the same distance as the circumference of the circle with a force equivalent to the centripetal force but in a straight line on a friction-less surface, what is the work this force would do? Explain why the answers are different. (Hint: They are, review the definition of work)

Homework Equations


Unknown

The Attempt at a Solution


I looked through all of the slides and notes that the professor posted, as well as my own notes, but I couldn't find anything relating to this style of problem. There were many equations talking about Omega and all sorts of different ways to solve similar problems, but I could not figure out how to translate it. Could anybody give me a hand with this problem? Thanks in advance!

PS: Sorry about the way the problem is worded. I just typed it in, word for word as my professor has it on our homework.
 
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Answer the straight line case first. You should be able to do that and it will help with the circular case.
 
You should also review the definition of work. Its not just "force times distance", there is a bit more to it and that's important for this problem.
 
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CWatters said:
You should also review the definition of work. Its not just "force times distance", there is a bit more to it and that's important for this problem.
Ah, I see. I found the equation for Centripetal Force (mv^2)/r, and I found that the Centripetal Force (and therefore the force that would be pushing the ball in a straight line in) is equivalent to about 40 Newtons. Applying that to the frictionless surface, using the same formula would give me the same answer. The work done by both would be 40pi Joules. Looking at the definition of work, it appears that Displacement would need to occur for there to be ANY work done at all. Therefore, since the ball on the string returned to its starting point, it could be said that no work was done at all. Is this correct? Thanks!
 
It's not because it returns to the starting position. The work would still be zero if it only moved say quarter of a revolution. There is another reason.
 
CWatters said:
It's not because it returns to the starting position. The work would still be zero if it only moved say quarter of a revolution. There is another reason.
Oh, is it because the force itself isn't causing the displacement? Since the force is the tension pulling towards the center, but the movement is in another direction? Other than that, I can't really think of what it could be...My apologies, I'm not very good at physics.
 
EthanVandals said:
is it because the force itself isn't causing the displacement?
Yes. Vectorially, ##W=\int \vec F.\vec{ds}##, where the . denotes dot product. So it is only the displacement in the direction of the force that matters. (Or, equivalently, use the whole displacement but only the component of the force in that direction.)
 
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EthanVandals said:
Since the force is the tension pulling towards the center, but the movement is in another direction?

Specifically the force and displacement are orthogonal (at right angles to each other). So the component of force in the direction of the displacement is zero.
 
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CWatters said:
Specifically the force and displacement are orthogonal (at right angles to each other). So the component of force in the direction of the displacement is zero.
Awesome, I was hoping that was what it was. Thank you so much for the help!
 

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