Volume enclosed by isosurfaces in electrostatics

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SUMMARY

The discussion focuses on calculating the area and perimeter enclosed by equipotential lines in electrostatics generated by multiple point charges. The potential due to a single point charge is expressed as φ = 1/r, leading to circular equipotential lines. For multiple charges, the potential is given by φ = 1/r1 + 1/r2 + ... + 1/rN, resulting in complex shapes such as deformed circles or merged circles resembling the number eight. The challenge lies in deriving analytical expressions for the perimeter and surface area of these equipotential lines as the number of point charges increases.

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  • Understanding of Coulomb's Law and electrostatic potential
  • Familiarity with geometry of circles and their properties
  • Knowledge of analytical methods for solving equations
  • Basic concepts of electrostatics in two and three dimensions
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Physicists, electrical engineers, and students studying electrostatics who are interested in the mathematical modeling of electric fields and equipotential surfaces.

woertgner
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Imagine that you have N points scattered in the plane. Each point is charged and contributes to the total potential the same Coulomb potential proportional to 1/r. Now consider some equipotential line of the total electrostatic potential. Is there an analytical expression for the surface enclosed by this line and for the length of this line?
 
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woertgner said:
Imagine that you have N points scattered in the plane. Each point is charged and contributes to the total potential the same Coulomb potential proportional to 1/r. Now consider some equipotential line of the total electrostatic potential. Is there an analytical expression for the surface enclosed by this line and for the length of this line?
If you are saying you want to find out the area enclosed by this line then by simple geometry you know the circle has maximum area.
The potential due to a sheet is diectly proportional to r.
that due to line is proportional to ln(r)
You wrote about the "volume" enclosed by isosurfaces
 
I am not sure if I understood your answer. I rephrase my question in more detail. Imagine you have one charged point in the plane. The electrostatic potential due to this point charge is up to a multiplicative factor: phi=1/r. Consider an equipotential line by setting phi=c. This equipotential line clearly is a circle and it is easy to compute its perimeter and surface. Now consider two equally charged points in the plane. The electrostatic potential due to these two charged points is up to a multiplicative factor phi=1/r1+1/r2, where r1 is the distance from the first point and r2 is the distance from the second one. Consider an equipotential line again by setting phi=c. If c is small enough you obtain two slightly deformed circles, if c is larger you obtain two merged circles forming something like number eight. How to compute the perimeter and surface now? What about a general case when we have N points in the plane and the potential is given by phi=1/r1+1/r2+1/r3+...+1/rN? By setting phi=c we obtain a set of deformed circles around points, which are sufficiently far away from other points and merged circles from others that are not sufficiently isolated. How to compute the perimeter and surface now? The generalisation of this problem to 3D is similar.
 

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