Calculating Net Force on a Charge Near an Infinite Grounded Conductor

AI Thread Summary
The discussion centers on calculating the net force on a charge near an infinite grounded conductor, specifically with two positive charges, q and 2q, positioned on the x-axis. Participants highlight the concept of using a mirror image of the charges to simplify the analysis, as the grounded conductor induces negative charges that affect the force on q. The net force is calculated by considering the repulsive force from the positive charge and the attractive force from the induced negative charges, leading to a formula involving k, q, and distances. There is also a mention of the complexities involved when dealing with nonplanar conducting surfaces, which require an infinite series of image charges. The conversation emphasizes the importance of understanding electric fields and potentials in such scenarios.
quantumworld
Messages
36
Reaction score
0
Dear reader,
here is a question that I stumbled upon, and I would like some insight on it :bugeye:

two positive charges q and 2q coulombs are located on the x-axis
at x = .5a and 1.5a, respectively. There is an infinite, grounded conduction plane at x =0. What is the magnitude of the net force on the charge q?

my problem is that I am unable to account for that infinite grounded conductor, I am unable to imagine which kind of force is it going to
exert on q.

Many thanks :shy:
 
Physics news on Phys.org
quantumworld said:
two positive charges q and 2q coulombs are located on the x-axis
at x = .5a and 1.5a, respectively. There is an infinite, grounded conduction plane at x =0. What is the magnitude of the net force on the charge q?

my problem is that I am unable to account for that infinite grounded conductor, I am unable to imagine which kind of force is it going to
exert on q.

There are some negative charges on the grounded conductor plane accumulated by induction. The effect of this charge distribution is the same as if we had the mirror images of the charges in front of the plane behind the plane, and with opposite sign.

ehild
 
Last edited:
So is it (1/2)*k*q^2 ? I have to take the GRE's in a month, and the Physics Subject one in November. I am dreading the physics one...

I got this answer by mirroring both across the plane with opposite charges, then added the 3 forces together.
 
THank you Healey, and ehild ! :smile:

I do remember something about this mirror image, and now I got it right, but it is kindof a magical solution, instead of dealing with the mess of charges on the conducting plate, we could treated as a mirror image, I wonder how did they come up with that theory, but I am glad they did :biggrin:
 
Last edited:
Healey01 said:
So is it (1/2)*k*q^2 ? I have to take the GRE's in a month, and the Physics Subject one in November. I am dreading the physics one...

I got this answer by mirroring both across the plane with opposite charges, then added the 3 forces together.


Draw arrows pointing into the direction of the forces the individual charges exert on the charge "+q". The "+2q" charge repels it, the negative charges on the opposite side attract it. And do not forget to include the distance between the charges in the formula for the force.

ehild
 
ehild said:
Draw arrows pointing into the direction of the forces the individual charges exert on the charge "+q". The "+2q" charge repels it, the negative charges on the opposite side attract it. And do not forget to include the distance between the charges in the formula for the force.

ehild

Ahh, forgot about which way theyre pushing. Gotta get more complicated and use vectors.

k*([(-2q)(q)/2^2](-i) + [(-q)(q)/1^2](-i) + [(2q)(q)/1^2](i)) = (7/2)kq^2
 
quantumworld said:
THank you Healey, and ehild ! :smile:

I do remember something about this mirror image, and now I got it right, but it is kindof a magical solution, instead of dealing with the mess of charges on the conducting plate, we could treated as a mirror image, I wonder how did they come up with that theory, but I am glad they did :biggrin:

It's not magic. A (perfectly) conducting surface must be an equipotential. You probably know from your introduction to fields that if you have two charges of opposite sign that there is a plane between them that is at a single potential.

The problem really becomes interesting when you try the image charge approach to a nonplanar conducting surface such as a sphere. It turns out that it requires an infinite series of image charges to get the equipotential!
 
Healey01 said:
Ahh, forgot about which way theyre pushing. Gotta get more complicated and use vectors.

k*([(-2q)(q)/2^2](-i) + [(-q)(q)/1^2](-i) + [(2q)(q)/1^2](i)) = (7/2)kq^2

This is almost all right but a^2 is missing from the denominator.

ehild
 
ehild said:
This is almost all right but a^2 is missing from the denominator.

ehild

I don't see it, please show me.
 
  • #10
Healey01 said:
I don't see it, please show me.

There were "a*s in your first post.

Healey01 said:
Dear reader,
here is a question that I stumbled upon, and I would like some insight on it

two positive charges q and 2q coulombs are located on the x-axis
at x = .5a and 1.5a, respectively. There is an infinite, grounded conduction plane at x =0. What is the magnitude of the net force on the charge q?

ehild
 
  • #11
ehild said:
There were "a*s in your first post.



ehild


uhhh, i didnt post this problem. And i assumed those were angstroms. I like how you quoted someone elses post then put my name on it :-p
 
  • #12
Healey01 said:
uhhh, i didnt post this problem. And i assumed those were angstroms. I like how you quoted someone elses post then put my name on it :-p


Sorry... I just did not look at your name, I did not recognize that it was not quamtumworld any more but you... Or it was not you who originally posted the problem. Can you forgive a scatterbrained old lady? :blushing:
By the way I do not think they are angstroms. Charge "q" and 2q, position "0.5a" and 1.5a. "q" and "a" can be anything.

ehild
 
Back
Top