Understanding Electric Potential Energy Calculations: Addressing Sign Confusion

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Discussion Overview

The discussion revolves around the calculation of electric potential energy changes when moving a point charge in the electric field of another point charge. Participants explore the implications of sign conventions in the context of electrostatic forces and potential energy, addressing confusion over the integration process and the interpretation of work done by external agents versus the electric field.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant expresses confusion about the signs in calculating potential energy change when moving charge +q2 closer to +q1, questioning where the sign error occurs.
  • Another participant suggests checking the integration part and the substitution of values, hinting at a potential oversight.
  • A different participant confirms the integration process but questions whether the integral should have been calculated from c to b instead of b to c.
  • One participant mentions that switching the limits of integration would yield a positive potential energy, prompting a discussion about the meaning of positive versus negative potential energy.
  • Another participant states that if an external agent does positive work, the potential energy change should also be positive, yet they remain puzzled by their negative calculation result.
  • Several participants discuss the relationship between the direction of displacement (ds) and the electric force, debating the correctness of the assumption that F⋅ds is negative due to opposing directions.
  • One participant clarifies that calculating the negative of the work done by the field accounts for the sign, suggesting that the dot product provides magnitude rather than sign.
  • Another participant concludes that setting limits from a larger to smaller distance inherently establishes the direction of the electric force relative to displacement.
  • One participant emphasizes that the force should be viewed as the negative gradient of potential, suggesting that the change in potential should be positive when moving from infinity to a point closer to the charge.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the correct approach to the integration or the interpretation of signs in potential energy calculations. Multiple competing views remain regarding the directionality of forces and displacements, as well as the implications of work done by external agents versus the electric field.

Contextual Notes

Participants express uncertainty regarding the assumptions made in the integration process, the definitions of displacement and force directions, and the implications of sign conventions in potential energy calculations. There are unresolved mathematical steps and differing interpretations of the physical concepts involved.

Jzhang27143
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I am confused about the signs in calculating the potential energy change from the electrostatic force.

Suppose there was a point charge +q1 and I moved a second point charge +q2 from a distance of b from q1 to a distance of c from q1. c is smaller than b.

So the potential energy change is - ∫ F ⋅ ds where F is the electric force due to q1. F is radially outward and ds is dr radially inward (from b to c)$, so F⋅ds = - F dr. So - ∫ F⋅ds = ∫ F dr = ∫ Kq1q2 / r^2 dr from b to c so the integral is Kq1q2 (-1/c + 1/b) which is negative. But the potential energy should be positive when q2 is brought closer to q1. Where is the sign error?
 
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Jzhang27143 said:
So the potential energy change is - ∫ F ⋅ ds where F is the electric force due to q1. F is radially outward and ds is dr radially inward (from b to c)$, so F⋅ds = - F dr. So - ∫ F⋅ds = ∫ F dr = ∫ Kq1q2 / r^2 dr from b to c so the integral is Kq1q2 (-1/c + 1/b) which is negative.
just check the integration part and substitution of values -i think there is a catch there!
 
i'm not sure what the problem is with the integration. ∫ Kq1q2/r^2 dr from b to c is kq1 q2 ∫ dr/r^2 from b to c = kq1q2 (-1/r) from b to c = kq1q2(-1/c - (-1/b)) = kq1q2(-1/c + 1/b). Should i have done the integral from c to b? if so, why?
 
You forget the negative sign outside the integral.
Also, calculating from point b to c, or vice versa, would depend on the question you'll be solving.

Hope this helps,
Qwertywerty.
 
Jzhang27143 said:
Should i have done the integral from c to b? if so, why?

well such a switch will correctly give you sign of P.E. to be + ve. but what does it mean?
i.e. how the P.E. is termed +ve or negative -
what is the concept of sign of P.E. related with work done by the field
or by an external agent carrying the task of doing work?
 
well, I know that if an external agent is doing positive work, then the potential energy change is positive, and the potential energy change is negative if the external agent is doing negative work. In my example of moving q2 closer to q1, the work from the external agent should be positive and so should the potential energy change. However, I still don't understand why my calculations gave a negative change in potential energy.
 
Jzhang27143 said:
well, I know that if an external agent is doing positive work, then the potential energy change is positive, and the potential energy change is negative if the external agent is doing negative work. In my example of moving q2 closer to q1, the work from the external agent should be positive and so should the potential energy change. However, I still don't understand why my calculations gave a negative change in potential energy.
Maybe you'd care to read my reply?
 
Last edited:
Edited.
 
Qwertywerty said:
Edited.
Oh, I thought I took care of the negative outside the integral though.

Jzhang27143 said:
So the potential energy change is - ∫ F ⋅ ds where F is the electric force due to q1. F is radially outward and ds is dr radially inward (from b to c)$, so F⋅ds = - F dr. So - ∫ F⋅ds = ∫ F dr = ∫ Kq1q2 / r^2 dr from b to c
 
  • #10
Jzhang27143 said:
Oh, I thought I took care of the negative outside the integral though.
'ds' represents displacement. So does 'dr'. Your assumption that F.ds = -F.dr, is wrong.
 
  • #11
Qwertywerty said:
'ds' represents displacement. So does 'dr'. Your assumption that F.ds = -F.dr, is wrong.
Wait i thought the direction of ds was the direction of the path taken. Thats why I thought ds and the electric field pointed in opposite direction so the dot product was negative. If that's not the case, what determines the direction of ds?
 
  • #12
What you basically want to do is, calculate the negative of the work done by the field existing between the two charges.

When you calculate ∫F.dr, you are automatically taking into consideration the dot product while assigning the limits. It can be seen that, for example, WEF=F.Δr - Δr takes care of the sign, and the dot product simply serves to help provide a magnitude, and not a sign.
 
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  • #13
Jzhang27143 said:
Wait i thought the direction of ds was the direction of the path taken. Thats why I thought ds and the electric field pointed in opposite direction so the dot product was negative. If that's not the case, what determines the direction of ds?
'ds' does what you think it does. As in, ds represents the displacement in the direction you move. I have tried to clarify the dot product part in my previous reply.
 
  • #14
Oh, that makes sense now. So setting the limits from a larger to smaller distance by itself establishes that the electric force is in the opposite direction of the displacement, meaning that the negative from the dot product is redundant.
 
  • #15
Yes.
 
  • #16
Jzhang27143 said:
Wait i thought the direction of ds was the direction of the path taken. Thats why I thought ds and the electric field pointed in opposite direction so the dot product was negative. If that's not the case, what determines the direction of ds?
Your force should be negative gradient of potential so change in potential = (-) F. dr dr is not an increment but opposite to r a decrement in r suppose you are coming from infinity to b you should get a positive potential at b similarly at c and the difference of the two should be positive!
try to guess/find the error!
 

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