How does distance affect potential in an electric field?

Click For Summary

Discussion Overview

The discussion centers on the relationship between distance and electric potential in an electric field, specifically exploring how potential is defined and calculated in electrostatics. Participants engage with concepts such as electrostatic potential, electric field, and the mathematical relationships between them.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant suggests that potential is simply distance times the electric field, seeking clarification on this basic concept.
  • Another participant counters that potential is not merely distance times the electric field, emphasizing the distinction between electric potential and electrostatic potential.
  • It is noted that for constant electric fields, the potential difference can be calculated as ΔV = -Ed, where E is the electric field and d is the distance.
  • A participant explains that the electric field is the negative gradient of the electrostatic potential, indicating how the potential changes in space.
  • The mathematical relationship involving integrals is introduced, illustrating how to calculate potential differences between two points in an electric field.
  • Another participant acknowledges a previous oversight regarding the negative sign in the equations presented.

Areas of Agreement / Disagreement

Participants express differing views on the relationship between distance and electric potential, with some asserting a direct multiplication relationship and others emphasizing the need for a more nuanced understanding involving gradients and integrals. The discussion remains unresolved regarding the initial claim about potential being distance times the electric field.

Contextual Notes

There are limitations in the discussion regarding the assumptions made about the constancy of the electric field and the definitions of electric potential versus electrostatic potential. The mathematical steps involving integrals and gradients are presented but not fully resolved.

anmolnanda
Messages
20
Reaction score
0
in which case potential is distance times the electric field..please explain so that i am cleared the the basics of this.
 
Physics news on Phys.org
The potential is not the distance times the electric field. You probably think that based on the fact that distance times the electric field will give you the same dimensions as a potential. Also, you must be careful to say that this is an electrostatic potential, because the electric potential differs from the electrostatic potential. I'm going to assume you want to know how the electrostatic potential is related to the electric field. That is very simple,

<br /> \vec{E} = - \vec{\nabla}V<br />
 
Last edited:
anmolnanda said:
in which case potential is distance times the electric field..please explain so that i am cleared the the basics of this.
For simple cases, where the field is constant, you can find the potential difference by multiplying the field times the distance:

ΔV = -Ed

Read this: http://hyperphysics.phy-astr.gsu.edu/hbase/electric/elewor.html#c2"
 
Last edited by a moderator:
silmaril89 said:
<br /> \vec{E} = \vec{\nabla}V<br />

Correction: \vec{E} = -\vec{\nabla}V. Anyways, I'm sure you knew that.

anmolnanda it's important to understand the physical significance and the mathematical description of the electrostatic field vs the electrostatic potential field.

The Equation above says that the Electric Field is just the negative gradient of the electrostatic potential field. This means that the E field provides a description of how the Potential field changes in space. In particular, since the E Field is a gradient of the Potential then it points in the direction of maximum change (up hill or down hill) of the potential. Since the E field is actually the negative gradient then the E field points in the direction of maximum change down hill (towards the minimum of the potential).

(I'm just going to say E field and potential for now on knowing that I am referring to the electrostatic electric and potential fields).

You might ask why does the E field point down hill? Well the Potential field of a charge q is given by

V = kq/r where k is a constant, q is the charge and r is the radial distance from the charge. So V = V(r), that is, the potential is a function of position and there for defines a scalar field in space. So since it defines a scalar field in space and since it depends on the polarity of the charge (positive or negative) then there will be regions in space that have very negative potentials and regions with very positive potentials. So, if we draw lines pointing from the positive potential regions to the lower potential regions in such a way that the path of the lines are along the maximum change in potential, then you would have drawn the electric field lines from the positive charges to the negative charges (since the electric field is the change in the potential and so points along these lines).

So if you wanted to know what the so called "Voltage", or difference in Potential was between two different regions in space then you might need to know what the Potential field looked like. Say the potential field is given by V(r) and say that the points that we are interested in are V(A) and V(B) where A is a point of positive potential and B is a point of negative potential.

Then we could find out the difference in the potential between these two regions by writing down

V(A) - V(B) = Sum of the change in the potential in a tiny interval along the line of maximum change multiplied by the length of the tiny interval.

Now mathematically since we're talking about tiny intervals that brings us to differential calculus and since we're talking about summing up an enormous number of tiny intervals then that reminds us of integrals.

So

V(A) - V(B) = \int (Change in Potential)*(small-change-in-distance)

Ok but we said that the negative change in the Potential was the Electric field, let's call it E(r), and let's call the small change in distance dr. Then what we have is this:

V(A) - V(B) = \int -E(r)*dr

So \DeltaV = \int -E(r)*dr, where \DeltaV = V(A) - V(B).

Now consider that the Potential field changes in space in such a way that the Electric field is constant along lines of maxmimum change between two regions. In that case we can move the Electric Field outside the integral in the equation above and replace it with this,

\DeltaV = -E(r)\int dr = -Ed, where d = \int dr = distance between points A and B.

Therefore the difference in potential is just the product of the magnitude of the electric field multiplied by the distance between the two points multiplied by negative 1 to be consistent with signs.

Hope that helps.
 
Last edited:
Quite descriptive Nirgal, my bad on missing the minus sign.
 

Similar threads

  • · Replies 21 ·
Replies
21
Views
4K
  • · Replies 20 ·
Replies
20
Views
3K
  • · Replies 3 ·
Replies
3
Views
1K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 10 ·
Replies
10
Views
3K
  • · Replies 2 ·
Replies
2
Views
1K
  • · Replies 6 ·
Replies
6
Views
1K
  • · Replies 12 ·
Replies
12
Views
2K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 16 ·
Replies
16
Views
2K