The relationship between electric potential and field.

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Homework Help Overview

The discussion revolves around the relationship between electric potential and electric field, specifically in the context of a problem involving electrons distributed on a circle. The original poster presents a scenario where 12 electrons are evenly spread on the circumference of a circle and asks about the electric potential at the center in two different configurations.

Discussion Character

  • Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants explore the concept of electric potential as a scalar quantity and its implications for electric fields in different configurations. Questions arise regarding how the same electric potential can lead to different electric fields, prompting discussions about gradients and the nature of potential variation.

Discussion Status

The discussion is active, with participants providing insights into the relationship between potential and field. Some have offered analogies to clarify the concepts, while others continue to question how to differentiate between the two scenarios despite having the same potential expression.

Contextual Notes

Participants are examining the implications of the superposition principle and the nature of electric fields in relation to potential, highlighting the need for a deeper understanding of gradients and their role in determining electric field behavior.

Yumrey
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Homework Statement


There are 12 electrons spread on the circumference of a circle with radius R evenly. What's the electric potential at the centre? Then the electrons are concentrated on the upper half of the circle, spread evenly. What's the electric potential at the centre now?

Homework Equations

The Attempt at a Solution


Since electric potential is a scalar, the potential due to one electron is V=kq/R. By superposition principle, the potential due to all the electrons is simply 12kq/R=12V. Both situations have the same potentials.
What confuses me is that the electric fields in both situations are indeed different. In the first case, the field is simply zero because they all cancel at that point, while it's nonzero in the second case. But electric field is the negative gradient of the electric potential, then how come the same potentials result in different fields?
 
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The field is related to the gradient. The same numerical value at a point may not have the same gradient.

Gradient is like a two or three dimensional slope.

Two functions can have the same value at a point but have different slopes.
 
Because the field is proportional to the gradient of the potential and not the potential. Also in one dimension you can have functions which take the same value in a point but have different derivatives.
 
To expand on that, the field depends on how the potential varies in a neighbourhood of a point, not on the value in the point only.
 
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Dr. Courtney said:
The field is related to the gradient. The same numerical value at a point may not have the same gradient.

Gradient is like a two or three dimensional slope.

Two functions can have the same value at a point but have different slopes.

But then how should I differentiate the two Vs(which have the exact same expression) such that they'll yield different electric fields?
 
Think of potential like the height of the ground at a point. If the ground is flat, a ball won't roll. If the potential is flat, a charge won't move because there is no net electric force.

But if the ground is sloped, the ball will roll. If the potential is sloped, a charge will accelerate, because there is a net electric force.
 
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Yumrey said:
But then how should I differentiate the two Vs(which have the exact same expression) such that they'll yield different electric fields?
Read my last post before this one. If you only know the function value in a single point you cannot take the derivative.
 
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