Solving Sphere Image Problem: Find Potential & 2nd Image Charge

In summary, the problem discussed is about finding the potential outside a grounded conducting sphere with a point charge located outside. The solution involves using the principle of superposition by adding an image charge inside the sphere to cancel out the potential from the external charge. The follow-up question asks where to place a second image charge to handle a sphere at any potential, and the answer is at the center with a charge of q=4*Pi*epsilon*R*V_0. Other possible choices for the placement of the second image charge are discussed, but the center is the most appropriate choice.
  • #1
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Homework Statement


A point charge is located outside of a grounded conducting sphere. Find the potential outside the sphere.

This problem was a solved example. It was solved by placing an image charge inside the sphere so that the potential from the charge outside the sphere would cancel the potential from the charge inside the sphere at the surface of the sphere.

The follow up question is:
By adding a second image charge the same method used above will handle the case of a sphere at any potential V_0. What charge should you use, and where should you put it?


Homework Equations





The Attempt at a Solution



It seems that by exploiting the principle of superposition, an easy solution is to add another image charge at the center. Then that charge would have to be q= 4*Pi*epsilon*R*V_0. Where "R" is the radius of the sphere.

But is that the only possible choice? Since the conductor is an equipotential, doesn't that mean that I could place the added charge anywhere inside the sphere? If so, then it seems the only problem that remains is determining what that charge would be.
 
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  • #2
Since the conductor is an equipotential, doesn't that mean that I could place the added charge anywhere inside the sphere? If so, then it seems the only problem that remains is determining what that charge would be.

I think you are mixing the model and the real object. The real object is the conducting sphere, and more exactly, the surface charge layer on the sphere. The model is the image charges. You REPLACE the real object with your model, under the constraint that E-field at the places outside "the sphere" remains the same. I put the word "the sphere" inside the inverted commas as when you replace the real sphere with the image charges, the sphere is no longer there!

That is the reason why you have to put the second image charge at the center, not anywhere else inside "the sphere". Notice that when you replace the sphere with the image charges, E-field does exist inside "the sphere", but this doesn't violate with the constraint.
 

FAQ: Solving Sphere Image Problem: Find Potential & 2nd Image Charge

What is the "Solving Sphere Image Problem"?

The Solving Sphere Image Problem is a mathematical problem in electrostatics that involves finding the electric potential and location of a second image charge outside of a conducting sphere. This problem is commonly used to demonstrate the concept of image charges and their application in solving complex electrostatic problems.

Why is solving the Sphere Image Problem important?

Solving the Sphere Image Problem is important because it helps us understand the behavior of electric charges and their interactions. It also allows us to simplify and solve complex electrostatic problems by using the concept of image charges, which can be applied to other situations as well.

What are the steps involved in solving the Sphere Image Problem?

The steps involved in solving the Sphere Image Problem include:
1. Identifying the known values, such as the radius of the conducting sphere and the position and magnitude of the original charge.
2. Applying the boundary conditions, which state that the electric potential and electric field must be continuous at the surface of the sphere.
3. Using the method of images to determine the location and magnitude of the second image charge.
4. Calculating the electric potential at any point outside of the conducting sphere using the superposition principle.
5. Verifying the solution by checking if the electric potential satisfies the boundary conditions and the Laplace equation.

What are the limitations of the Sphere Image Problem?

The Sphere Image Problem has a few limitations, such as:
1. It only applies to conducting spheres and cannot be used for other shapes or materials.
2. It assumes that the original charge is located at a distance much larger than the radius of the sphere.
3. It does not take into account the effects of other charges or the presence of dielectric materials.
4. It is only applicable in electrostatics and cannot be used to solve dynamic or time-varying problems.

How can the Sphere Image Problem be extended to more complex systems?

The Sphere Image Problem can be extended to more complex systems by combining the method of images with other mathematical techniques, such as conformal mapping or multipole expansion. These methods can be used to solve problems involving multiple charges, different geometries, and non-conducting materials. Additionally, computer simulations and numerical methods can also be used to solve complex electrostatic problems.

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