Electrostatics problem using Coulomb's law

Join the discussion
Ask a follow-up here, or get your own question answered by working scientists, mathematicians and engineers — people, not an autocomplete.
Real named experts · corrections over time · the nuance an AI answer skips
13 replies · 5K views
spaghetti3451
Messages
1,311
Reaction score
31

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?
 
Last edited:
on Phys.org
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:
 
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:
 
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.
 
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)
 
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:
 
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.
 
Wow! That's also an interesting proof! Thanks! :smile: