Method of Images in Electrostatics

In summary, the potential outside the sphere may be found by placing an image charge at a distance c=a2/d from the centre of the sphere, and determine the charge stored on the spherical conductor.
  • #1
timhunderwood
12
0

Homework Statement



A point charge q is held a distance d > a below the centre of a large spherical conductor of radius a. Show that, if the spherical conductor is earthed, the potential outside the sphere may be found by placing an image charge at a distance c=a2/d from the centre of the sphere, and determine the charge stored on the spherical conductor.
(I CAN DO THIS PART OF THE QUESTION FINE)

Instead of being earthed, the net charge on the spherical conductor is now set to zero. Explain why, in order to represent the electric field outside the conductor an additional image charge must now be included inside the sphere, and determine the potential of the conductor.

Homework Equations


I found the image charge to have a charge -aq/d

The Attempt at a Solution



I can do the first part of the question fine. But I'm getting confused when we set the conductor to zero charge.

My reasoning for why we need an additional image charge is that ( I Think) the overall charge of all the image charges inside the conductor should now also be zero. Hence, we would need an image charge of +aq/d inside the sphere...

My intuition was to put it at a distance a^2/d in the opposite direction to the other image charge so it makes a dipole with it centred at the origin of the sphere... But I don't really no if this is right or if its justified.

I don't know how I can then calculate the potential easily without doing a lot of trig and maths?

Thanks very much
 
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  • #2
hmmm... I had a nice long writeup and then I realized that I was completely misunderstanding the problem :rofl:

Anyway, you had a good idea, thinking about the total of all the image charges. To justify it (I don't know if you did this), I would use Gauss's law with a very large Gaussian sphere. Since the two configurations (point charge with uncharged conductor vs. point charge with image charges) need to generate the same electric field, they had better have the same total charge, q.

To find exactly where you need to place the other image charge, I would try using the fact that the electric field at the surface of the conductor needs to be perpendicular to the conductor. (I haven't done the problem myself, so I can't guarantee this will work, but I suspect it'll get you somewhere) Once you figure out where that other charge goes, you can use the fact that the potential is constant throughout a conductor: in order to find the potential of the conductor, you only need to compute it at one point. And I'm sure you know how to compute the potential produced by a system of point charges at one point...
 
  • #3
I'm having trouble calculating the position of the second image charge. I tried putting it at an arbitrary distance from the centre on line with the other image particle.

Then I try to calculate the field due to all three particles at the radius of the conductor. But I think I'm making a mistake as I get a quartic equation which I had to get my computer to solve.

Whats the best way to do this bit? Is there a trick to simplify the mathematics of working out the field on radius at an arbitrary angle?

Thanks
 
  • #4
Don't calculate it at an arbitrary angle - calculate it at whatever angle is most convenient, and then check it at an arbitrary angle.

But here's my line of thought: if you know that there is exactly one additional image charge, there's really only one place you can put it that will make the net electric field perpendicular to the surface of the sphere at all points.
 
  • #5
ah got it now

thanks very much
 
  • #6
timhunderwood said:
ah got it now

thanks very much

2005 Paper 1 Question B7? :D
 

1. What is the Method of Images in Electrostatics?

The Method of Images is a mathematical technique used in electrostatics to solve boundary value problems for a point charge in the presence of one or more conducting or dielectric surfaces.

2. How does the Method of Images work?

The Method of Images works by introducing a fictitious charge, also known as an "image charge", to satisfy the boundary conditions of the problem. The image charge is placed symmetrically with respect to the real charge, creating a mirror-like effect, and the resulting electric field from the real and image charges satisfies the boundary conditions.

3. What are some applications of the Method of Images?

The Method of Images is commonly used in various fields such as electrostatics, electromagnetism, and fluid dynamics. Some specific applications include analyzing the electric fields near conducting or dielectric surfaces, calculating the capacitance of a system, and modeling the flow of fluids around obstacles.

4. What are the limitations of the Method of Images?

The Method of Images is limited to problems with simple geometries and boundary conditions, such as a point charge near a conducting plane or a conducting sphere. It also assumes that the conducting surfaces are perfect conductors, which may not always be the case in real-world scenarios.

5. Are there any alternative methods to the Method of Images?

Yes, there are alternative methods to the Method of Images, such as the Finite Element Method and the Boundary Element Method. These methods allow for more complex geometries and boundary conditions to be analyzed, but they may require more computational resources and expertise to implement.

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