The sign of F (dot) dl when finding electric potential

In summary: So since r is decreasing as you come in from infinity, |dr| = -dr.Yes. dr represents the infinitesimal change in r. So dr is negative when coming in.
  • #1
EquationOfMotion
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The electric potential can be defined as

V = - ∫C E⋅dl

where we are taking the line integral along C from some convenient reference point O, where we have set V = 0, to the point r we are trying to find the potential at. Of course, C can be any curve, but it's usually the most convenient to take it as a straight line from O to r.

Doesn't this mean dl will point in the direction from O to r? If that is the case, then say we're trying to find the potential at some distance from point charge +q and we've set our reference point infinitely far away. We have E = (kq/r^2) r(hat), where r(hat) is the spherical unit vector. Then, E⋅dl = E r(hat)⋅dl. But dl points from infinity to the point we're trying to find, and say that we've picked O so that dl points in the -r(hat) direction. Then, E⋅dl = -Edr, so evaluating the integral, we get V = -kq/r, which is evidently wrong.

I am aware that we can fix this by taking O to be somewhere else, but do you always take the line integral to be positive? If so, why? Or is there something else I'm missing?

EDIT: This seems like it'd fit better in General Physics. Woops.
 
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  • #2
Hello. Welcome to PF.
Your question is a good one. Most of us have gotten confused by this at one time or another.
EquationOfMotion said:
Doesn't this mean dl will point in the direction from O to r?
Yes
If that is the case, then say we're trying to find the potential at some distance from point charge +q and we've set our reference point infinitely far away. We have E = (kq/r^2) r(hat), where r(hat) is the spherical unit vector.
Yes. r(hat) points radially outward from q.
Then, E⋅dl = E r(hat)⋅dl. But dl points from infinity to the point we're trying to find, and say that we've picked O so that dl points in the -r(hat) direction.
OK
Then, E⋅dl = -Edr,
This is the mistake. The dot product of two vectors A and B is A⋅B = |A| |B| cosθ. So, in your case (coming in from infinity),
E⋅dl = |E| |dl| cos(180o) = -|E| |dl| = -E |dr|. When integrating from ∞ to r, how should you write |dr| in terms of dr? In particular, is dr a positive quantity or a negative quantity in this case? Hint: is r increasing or decreasing?

Or you can think about it more directly. When coming in from infinity, is E⋅dl a positive quantity or a negative quantity (assuming q is positive)? Now consider the expression E dr when coming in from infinity. Is this a positive quantity or a negative quantity?

Or, you can approach it by convincing yourself that dl = dr r(hat) whether you are coming in from infinity along a radial line or going out to infinity along a radial line. So, you can write E⋅dl = E⋅r(hat) dr for either incoming or outgoing.
 
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  • #3
TSny said:
When integrating from ∞ to r, how should you write |dr| in terms of dr? In particular, is dr a positive quantity or a negative quantity in this case? Hint: is r increasing or decreasing?

So since r is decreasing as you come in from infinity, |dr| = -dr.

TSny said:
Or you can think about it more directly. When coming in from infinity, is E⋅dl a positive quantity or a negative quantity (assuming q is positive)? Now consider the expression E dr when coming in from infinity. Is this a positive quantity or a negative quantity?

E⋅dl is negative, while E dr is positive so you need a negative sign. Nice!

TSny said:
Or, you can approach it by convincing yourself that dl = dr r(hat) whether you are coming in from infinity along a radial line or going out to infinity along a radial line. So, you can write E⋅dl = E⋅r(hat) dr for either incoming or outgoing.

Is this because going out it's obviously r(hat) dr, and coming in it's (-r(hat))(-dr)?

Thank you very much for your help!
 
  • #4
EquationOfMotion said:
So since r is decreasing as you come in from infinity, |dr| = -dr.
Yes. dr represents the infinitesimal change in r. So dr is negative when coming in.

E⋅dl is negative, while Edr is positive so you need a negative sign.
E⋅dl is negative when coming in. But Edr is also negative when coming in. Remember, dr is a negative quantity since r is decreasing. So, E⋅dl has the same sign as Edr. You can check that these two expressions also have the same sign when going out. So, E⋅dl = Edr for both coming in and going out. (These statements assume that q is positive.)

going out it's obviously r(hat) dr, and coming in it's (-r(hat))(-dr)?
You are saying that dl = r(hat) dr when going out and that dl = -r(hat) (-dr) = r(hat) dr when coming in. Yes, that's true.

When coming in, dl = -r(hat) |dr| = -r(hat) (-dr) = r(hat) dr.
 

What is the significance of the sign of F (dot) dl when finding electric potential?

The sign of F (dot) dl is important because it indicates the direction of the electric potential. A positive sign means that the electric potential is increasing, while a negative sign means that the potential is decreasing.

How is the sign of F (dot) dl determined?

The sign of F (dot) dl is determined by the direction of the electric field and the direction of the displacement vector. If these two vectors are in the same direction, the sign is positive. If they are in opposite directions, the sign is negative.

What happens when the sign of F (dot) dl is negative?

When the sign of F (dot) dl is negative, it means that the work being done on the charge is negative. This can happen when the electric field and displacement vectors are in opposite directions, and the charge is moving against the direction of the electric field.

Can the sign of F (dot) dl ever be zero?

Yes, the sign of F (dot) dl can be zero. This occurs when the electric field and displacement vectors are perpendicular to each other, resulting in no work being done on the charge.

How does the sign of F (dot) dl affect the calculation of electric potential?

The sign of F (dot) dl is an important factor in the calculation of electric potential because it determines whether the electric potential is positive or negative. This, in turn, affects the overall value of the electric potential at a given point in space.

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