Why Does the Mirror Charge Method Double the Potential Energy?

In summary, the conversation discusses a situation involving a point charge above a grounded conductor and the potential energy of the system. The argument to replace the point charge with a negative charge is mentioned, and the use of Gauss law is suggested to explain the absence of electric field in the region below the conductor. The concept of mirror charges is also mentioned as a way to analyze the electric field in the region where the real charge is located.
  • #1
Aroldo
14
0
Hi everybody,
The situation is the classic one: a point charge q+ in a distance d above a conductor plane grounded:
The conductor is grounded so V = 0, for z = 0.
Also, far away from the system (x2 + y2 + z2 >> d) V --> 0

The argument to replace it for a q- charge seems perfect to me.
What I can't understand why W (potential energy) of the two point charges is twice as much as the conductor plane + q+ charge system.
I mean, why E = 0 for z < 0 in the conductor plane + q+.
Thank you a lot!
 
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  • #2
Try Gauss law on the "underside" of the conductor: no charge, no field.
 
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Likes Aroldo
  • #3
What do you mean by 'underside', the region immediately bellow the conductor, or a phill box that starts inside the conductor and ends in z < 0?
 
  • #4
Both give E = 0.

The mirror charge method only says something about the region where the real charge is (because a solution to the field equation is unique, anything is allowed, but the solution is only for that region).
 

What is the method of image charges?

The method of image charges is a mathematical technique used to solve electrostatic problems in which charged particles are located near a conductive surface. It involves creating imaginary point charges (or images) that are strategically placed to mimic the behavior of the actual charges, simplifying the problem and allowing for easier calculation of electric fields and potentials.

How does the method of image charges work?

The method of image charges works by utilizing the principle of superposition, which states that the total electric field at any point is the sum of the individual electric fields from each charge. By placing images at specific locations, the total electric field can be simplified and calculated using basic principles of electrostatics.

When is the method of image charges useful?

The method of image charges is useful in a variety of situations, including problems involving point charges near conductive surfaces, point charges near dielectric interfaces, and conducting spheres in an external electric field. It is also commonly used in problems involving capacitors and other electrical components.

What are the limitations of the method of image charges?

While the method of image charges is a powerful tool for solving electrostatic problems, it does have some limitations. It can only be applied to problems with simple geometries, and it assumes that the conductive surface or interface is perfectly smooth and flat. Additionally, it does not take into account the effect of induced charges.

Are there any real-life applications of the method of image charges?

Yes, the method of image charges has been used in various real-life applications, including in the design of capacitors, transmission lines, and other electrical components. It has also been applied in the study of electrostatic phenomena in biological systems and in the modeling of lightning strikes.

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