Why is the surface of a conductor equipotential?

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SUMMARY

The discussion centers on the concept of equipotential surfaces in conductors, specifically in the context of a positive point charge near a neutral conducting sphere. When a test charge is introduced, the presence of the conducting sphere causes the free charges within it to redistribute, resulting in equal potential at points A and B on the sphere's surface. This redistribution occurs because the electric field from the point charge induces a separation of charge within the conductor, ensuring that the potential remains constant across its surface. Thus, the conducting sphere effectively neutralizes the potential difference that would exist without it.

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  • Basic concepts of point charges and their effects on surrounding space
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I am having trouble understanding this. For example, say I have this:


[positive point charge] [A][neutral conducting sphere] [...infinity]


I know the point charge will create a field radially outward. But now I'm thinking of a test charge being brought in from infinity. If the sphere was not there, point A would obviously have a higher potential than point B. But somehow the conducting sphere being there would allow A to have the same potential as B. I do not understand this.
 
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The free charge on the conducting sphere will re-distribute in the presence of the field from the point charge. The electron density will increase near the positive charge (side A) and decrease on the opposite side. The field of the charge distribution will add up to the field of the point charge.
 

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