Electric potential energy due to a point charge

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Discussion Overview

The discussion revolves around the derivation of electric potential energy due to a point charge, specifically focusing on the work done by an external agent in moving a test charge from infinity to a point in the electric field of another charge. The scope includes theoretical derivation, conceptual understanding, and clarification of definitions related to potential energy in electrostatics.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant expresses confusion over a minus sign in the derivation of electric potential energy, questioning the work done by an external agent.
  • Another participant states that potential energy is the negative of the work done by the force of a field, suggesting this might be the source of confusion.
  • Some participants argue that when considering the work done by an external agent, it must be positive in cases of repulsive forces, as the potential energy increases.
  • There is a discussion about the definition of electrostatic potential energy and how it relates to the work done by external forces, with one participant noting a contradiction in their textbook's definition.
  • Several participants provide alternative derivations and clarify the relationship between work done and potential energy, emphasizing the need to consider the direction of forces and displacements.
  • One participant questions the integration process and the resulting signs in the expressions for work done, expressing uncertainty about how positive infinitesimal work can lead to a negative total work.
  • Another participant clarifies that the work done by an external force should equal the change in potential energy, leading to further discussion on the correct interpretation of the work-energy relationship.

Areas of Agreement / Disagreement

Participants exhibit disagreement regarding the interpretation of work done by external forces and the resulting signs in the equations. There is no consensus on the correct derivation or the implications of the definitions provided in textbooks.

Contextual Notes

Limitations include potential misunderstandings of the definitions of work and energy, as well as the dependence on the direction of forces and displacements in the derivation process. Some mathematical steps remain unresolved, particularly regarding the integration and the signs of the resulting expressions.

Ashu2912
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Hey friends, I am stuck up in the derivation of the electric potential energy due to a charge 'Q' at the origin on test charge 'q' at a point p (position vector 'rp'). The derivation is shown below, am just struggling with a minus sign...

Electric Potential Energy at P
= Work done to move 'q' from infinity to P quasi-statically by external agent

=\int kQq/r2 -r\wedge.-dr

(Since External Force = - Coulumbic Force and displacement vector = -dr)

=kQq [-1/r]\inftyrp

=-kQq/r

I know that when Qq is +ve, work done should be positive, but the sign is changing due to the integral.

NOTE : all vectors shown in bold faces, r^ is unit vector along r and dr is infinitesimal displacement in direction of r...
 
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Potential energy is the negative of the work done by the force of a field. Could the be the issue you're having?
 
Ya, that's true but here I am considering the work done by an external agent, which provides force just enough to counter-balance the force of the electric field. Therefore, this external agent must do positive work in case of repulsive forces (Qq is positive) as the potential energy of the charge 'q' is increased on it's action...
 
Since Qq is positive, the external force must be doing negative work (and the field doing positive work) when allowing the charges to move apart.
 
Ya, I got your point. However, my textbook defines electrostatic potential energy as
"Potential energy of a charge q at a point in the presence of field due to any charge configuration is the work done by the external force (equal and opposite to the electric force) in bringing a charge q from infinity to that point".
Now, if we go to see
Work done by external force in moving charge from \infty to the point
= W\inftyP
= Uinitial - Ufinal
= -Ufinal

or Electrostatic potential Ufinal = -W\inftyP (by external force), which is a contradiction to the definition.

My guess if that the work done by the external force should be positive, in case of let's say Q,q > 0, but it is coming to be negative, equal to -kQq/r. Even though the infinitesimal work is coming to be positive, the net work is coming negative. Don't know why. Please help!
 
Looks to me like your original derivation is off a bit. Note that 'dr' points in the direction of increasing r, so the work done against the field is:
dW = -qEdr (dot product, of course)

For a point charge Q, the potential energy at r is the work done against the field from infinity to point r:
U(r) \equiv -\int_{\infty}^r q\vec{E} \cdot d\vec{r}

U(r) \equiv -\int_{\infty}^r \frac{kQq}{r^2} dr = \frac{kQq}{r}
 
However, the infinitesimal work done should be
dw = Fext.ds (ds is in the direction of \infty to rp)
Since ds = -dr and Fext is -Felectric
dw = Felectric.dr, which is positive, assuming Q,q>0
 
I'm once again showing my complete derivation, with the diagram attached. The diagram is made in MS Paint, so...my apologies. All vectors are shown in bold face.
Consider a charge Q>0 at origin. We bring another charge q>0 from infinity to P, with position vector p. At each instant we apply an external force, equal and opposite to the Coulumbic force, so that the charge q comes from infinity to P quasi-statically, with constant velocity. Now,
Work done in moving the charge q from infinity to P
= w\inftyP

=\intFexternal.ds from \infty to p

=\int-Felectric.-dr (as ds = -dr. Since r is the general position vector at a point directed from the origin, dr too, points away from the origin and is parallel to r, and joins r to r + dr. ds is used in the main equation as we have to integrate along the path followed).

=\intkQq/r2 dr (Felectric and dr are in the same direction, so their dot product is Fdrcos0 = Fdr)

=-kQq/p

I have one more confusion. We know that \DeltaU = Ufinal - Uinitial = -Work done by a force. Using this, we get Ufinal = kQq/p, since Uinitial is taken as 0.

However my textbook says that work done by external force to move charge from A to B =
UB - UA.

Please solve my big confusion. My exam's on Monday. Pls. help as fast as you can...
 

Attachments

Ashu2912 said:
I'm once again showing my complete derivation, with the diagram attached. The diagram is made in MS Paint, so...my apologies. All vectors are shown in bold face.
Consider a charge Q>0 at origin. We bring another charge q>0 from infinity to P, with position vector p. At each instant we apply an external force, equal and opposite to the Coulumbic force, so that the charge q comes from infinity to P quasi-statically, with constant velocity. Now,
Work done in moving the charge q from infinity to P
= w\inftyP

=\intFexternal.ds from \infty to p

=\int-Felectric.-dr (as ds = -dr. Since r is the general position vector at a point directed from the origin, dr too, points away from the origin and is parallel to r, and joins r to r + dr. ds is used in the main equation as we have to integrate along the path followed).

=\intkQq/r2 dr (Felectric and dr are in the same direction, so their dot product is Fdrcos0 = Fdr)

=-kQq/p
Too many minus signs.

The work done would be:
\int_\infty^r \vec{F_{ext}}\cdot d\vec{s}

Since s points toward the charge, the force Fext is positive, not negative.

\int_\infty^r \frac{kQq}{r^2} ds = -\int_\infty^r \frac{kQq}{r^2} dr

I have one more confusion. We know that \DeltaU = Ufinal - Uinitial = -Work done by a force. Using this, we get Ufinal = kQq/p, since Uinitial is taken as 0.

However my textbook says that work done by external force to move charge from A to B =
UB - UA.
I guess I don't understand the question. The work required to move a charge quasi-statically from A to B will equal ΔU = UB - UA.
 
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  • #10
Doc Al said:
Work done =
\int_\infty^r \frac{kQq}{r^2} ds = -\int_\infty^r \frac{kQq}{r^2} dr
In the above equation, Fext and ds are in the same direction. The above integral shouldn't therefore contain |Fext||ds|cos0
=kQq/r2 X dr, as ds = -dr => |ds| = |dr|. Therefore, shouldn't the final expression contain a minus sign? I understand that since Fext and ds are in the same direction, thus the work done by the external force should be positive. However, the infinitesimal work is coming to be positive, but the total work is coming to be negative, just because of integration...

In my second question, I meant that \DeltaU = -W, right? So, Ui - Uf = Wi to f, as per the work - PE relation. But in my book, it is given that Uf - Ui = W. So, which of them is correct?
 
  • #11
Doc Al said:
Work done =
\int_\infty^r \frac{kQq}{r^2} ds = -\int_\infty^r \frac{kQq}{r^2} dr
Ashu2912 said:
In the above equation, Fext and ds are in the same direction. The above integral shouldn't therefore contain |Fext||ds|cos0
=kQq/r2 X dr, as ds = -dr => |ds| = |dr|. Therefore, shouldn't the final expression contain a minus sign?
I'm not sure what you mean by 'final expression', but the last expression in the quoted segment does have a minus sign.
I understand that since Fext and ds are in the same direction, thus the work done by the external force should be positive.
Right.
However, the infinitesimal work is coming to be positive, but the total work is coming to be negative, just because of integration...
No. How can the sum of positives end up negative?

In my second question, I meant that \DeltaU = -W, right?
That depends on what force is doing the work. In the definition of potential energy that we are discussing above, it's an external force doing the work. Thus ΔU = W, not -W.
 
  • #12
The last expression i meant was:
dW = kQq/r2ds
In this, kQq/r2ds is a scalar expression, a dot product. Since ds=-dr (please check my diagram again) so |ds| = |dr|. Thus, dW is coming to be +ve.
How can the sum of positives end up negative?
Thats what I am thinking.
Thanks, I got the second part. Thanks a lot!
 
  • #13
Ashu2912 said:
The last expression i meant was:
dW = kQq/r2ds
OK.
In this, kQq/r2ds is a scalar expression, a dot product.
Right. And F and ds point in the same direction, so Fds is positive.
Since ds=-dr (please check my diagram again) so |ds| = |dr|. Thus, dW is coming to be +ve.
This is confusing. Fds is positive. Now you want to change your variable of integration from s to r, so use ds = -dr (not ds = dr).
 
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  • #14
Ya, but in terms of magnitude, ds = dr, since ds = -dr, right? Thanks so much for your time...
 
  • #15
Ashu2912 said:
Ya, but in terms of magnitude, ds = dr, since ds = -dr, right?
Well, sure. The magnitude of ds and dr are equal. But you cannot ignore the sign!
 
  • #16
I have finished with my exam, but still have one doubt in my mind...
When we have a limit of integration like [-1/r] from \infty to let's say any positive number, we get a negative number, even though the infinitesimal quantity is positive, since the direction of integration also matters. So do you mean that we will have to change the sign of the integration variable so that the work done comes to be positive??
However, if this is the case, then why do we get a negative sign even when we integrate from -\infty to a positive number?
I'm oinfused totally in this matter. Please help!
 
  • #17
Ashu2912 said:
I have finished with my exam, but still have one doubt in my mind...
When we have a limit of integration like [-1/r] from \infty to let's say any positive number, we get a negative number, even though the infinitesimal quantity is positive, since the direction of integration also matters.
I assume you mean to integrate -1/r^2, not -1/r. In any case, why do you think the integral from ∞ to some positive number would be negative?
 
  • #18
Bumping this because I have exactly the same doubt, and reading through this thread didn't help me clear it :/

We know that F(ext) = -qE, where E is the field due to a positive charge along 'r' vector. Also, our displacement in moving the test charge near the original charge is along 'r' vector, but in the opposite direction, hence '-dr'.

Now dW = F(ext).ds = (-qE) * (-dr), integration of which gives me a negative quantity. Where have I made a mistake of a minus sign?
 
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  • #19
Hey dreamlord, I think I have understood this now!
Fext(vector) =- qE(vector) like you said. However, while integrating you have to consider dr(vector) only, the integration limits being from 0 to infinity!
 
  • #20
dreamLord said:
We know that F(ext) = -qE, where E is the field due to a positive charge along 'r' vector. Also, our displacement in moving the test charge near the original charge is along 'r' vector, but in the opposite direction, hence '-dr'.

Now dW = F(ext).ds = (-qE) * (-dr), integration of which gives me a negative quantity. Where have I made a mistake of a minus sign?
The sign of dr is taken care of by your limits of integration. You move in the '-dr' direction by integrating from ∞ to r.
 
  • #21
Ashu2912 said:
Hey dreamlord, I think I have understood this now!
Fext(vector) =- qE(vector) like you said. However, while integrating you have to consider dr(vector) only, the integration limits being from 0 to infinity!
Sorry I mean infinity to zero! And what doc al said is absolutely correct!
 

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