Electrostatics problem using Coulomb's law

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Homework Help Overview

The problem involves electrostatics and Coulomb's law, specifically examining the net force on a test charge located at the center of regular polygons with equal charges at the vertices. The discussion includes scenarios with both 12-sided and 13-sided polygons, exploring the effects of removing one charge from each configuration.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants discuss symmetry arguments to analyze the cancellation of forces from charges positioned symmetrically around the test charge. Questions arise regarding how to account for vertical components of forces and the implications of rotating the charge configuration.

Discussion Status

The discussion is active, with participants exploring various angles of reasoning. Some have suggested that the net force could be zero based on symmetry and rotational invariance, while others are still working through the implications of these concepts.

Contextual Notes

Participants are considering the effects of removing a charge from the configurations and how that impacts the net force on the test charge. There is an ongoing examination of the assumptions regarding symmetry and force directionality.

spaghetti3451
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Homework Statement



This problem is taken from 'Introduction to Electrodynamics' by David Griffiths.

(a) Twelve equal charges, ##q##, are situated at the corners of a regular 12-sided polygon (for instance, one on each numeral of a clock face). What is the net force on a test charge Q at the center?

(b) Suppose one of the 12 ##q##'s is removed (the one on "6 o'clock"). What is the force on Q? Explain your reasoning carefully?

(c) Now 13 equal charges, ##q##, are placed at the corners of a regular 13-sided polygon. What is the force on a test charge ##Q## at the center?

(d) If one of the 13 ##q##'s is removed, what is the force on ##Q##? Explain your reasoning.

Homework Equations



3. The Attempt at a Solution [/B]

(a) Zero, because each of pair of opposite charges exert forces on ##Q## of equal magnitude in opposite directions.

(b) The force on ##Q## is given by Coulomb's law, and acts in the direction of "6 o'clock."

(c) This is where I've got stuck. I picture one charge ##q## at the 12 o'clock position, and the others spread symmetrically throughout the rim of the clock face. Then, I have a gut feeling that the net force is due only to the charge at the 12 o'clock position. Using the above picture of the position of the charges, the horizontal components of the forces cancel by symmetry. However, I'm unable to account for the cancellation of the vertical forces due to the other 12 charges.

Thoughts?
 
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Did you try applying symmetry arguments?
 
Yes. Using symmetry arguments, I was able to cancel out the horizontal components of the forces.

But, how I can cancel out the vertical components of the forces using symmetry arguments eludes me. :frown:
 
What happens if you turn the whole contraption by an angle 2pi/13?
 
The system's behaviour is invariant under a rotation of ##\frac{2 \pi n}{13}## - I get that. :smile:

But how that relates to the problem at hand is a bit perplexing. :sorry:
 
So if you assume that the resulting force points in any direction, what would happen to it during the 2pi/13 rotation?
 
The configurations of the system under a rotation of ##\frac{2 \pi n}{13}## all have a net force of the same magnitude pointing in the same direction.

How might it be possible to determine the direction of that force and its magnitude?
 
failexam said:
The configurations of the system under a rotation of ##\frac{2 \pi n}{13}## all have a net force of the same magnitude pointing in the same direction.

How might it be possible to determine the direction of that force and its magnitude?

Exactly, but what happens to any force on the charge if you rotate the charge distribution responsible for the force by any angle?
 
The direction of the net force will change in general, but its magnitude will remain the same, under an arbitrary rotation.
 
  • #10
Yes, so now you have two pieces of information. The direction of the force will change by an angle 2pi/13, but the force will remain the same because the charge configuration is the same. What is the only way of accommodating both these criteria?
 
  • #11
I see. It's by having the effects due to 12 charges being equal to zero, and the effect of only one charge contributing to the net force. :nb)
 
  • #12
Wait! Actually, the net force is zero. That's because the configuration of charges remains invariant under a rotation of ##\frac{2 \pi n}{13}##, yet the direction of the net force ought to change by an angle of ##\frac{2 \pi n}{13}##. The only way this can happen is for the net force to be zero.

I think this is the correct argument, isn't it?:smile:
 
  • #13
failexam said:
I think this is the correct argument, isn't it?:smile:
Correct.

Another way to deduce it is to take your argument that the "horizontal" component is zero. You can make the same argument with any other direction which is rotated by a multiple of 2pi/13. You will then know that the projection onto two linearly independent directions is zero, meaning that the force must be zero.
 
  • #14
Wow! That's also an interesting proof! Thanks! :smile:
 

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