Electrical potential of charged sphere

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SUMMARY

The discussion centers on the electrical potential of two charged metal spheres connected by a wire. Sphere A, being larger than Sphere B, has a lower electrical potential due to its greater radius, as described by the formula V = q/(4*pi*e0*r). The conclusion drawn is that the electrical potential at the surface of Sphere A is less than that at the surface of Sphere B, confirming option b) as the correct answer. The concept of equipotential surfaces is emphasized, indicating that while charge may not be equally distributed, the potential must remain constant across connected conductors.

PREREQUISITES
  • Understanding of electric potential and the formula V = q/(4*pi*e0*r)
  • Knowledge of the concept of equipotential surfaces in electrostatics
  • Familiarity with the behavior of conductors in electrostatic equilibrium
  • Basic principles of charge distribution in connected conductive objects
NEXT STEPS
  • Study the principles of electrostatics and electric fields
  • Learn about equipotential surfaces and their implications in electrostatics
  • Explore the behavior of conductors when connected in circuits
  • Investigate the concept of charge distribution in different geometries
USEFUL FOR

Students studying physics, particularly those focusing on electrostatics, as well as educators and anyone looking to deepen their understanding of electric potential and charge distribution in conductive materials.

kasse
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Homework Statement



Two charged metal spheres are connected by a wire. Sphere A is larger than sphere B. The magnitude of the electrical potential of A...

a) is greater than at the surface of sphere B
b) is less than at the surface of sphere B
c) is the same as that at the surface of sphere B

The Attempt at a Solution



Electric potential: V = q/(4*pi*e0*r)

Since the spheres are connected by a wire, their charge will be equal. We regard the charges at the spheres as point charges in the centers of the spheres. Then the magnitude of the electrical potential of A is less than at the surface of B since rA > rB

Why am I wrong?
 
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I don't know how to say this without giving the whole thing away, but do you really think that if I connect a huge sphere with a lot of charge (like the earth) to a small sphere (like a steel marble) that they will they will split the charge equally? Something will be equal between the two spheres, but it won't be charge.
 
So c) is the correct answer. How can this be explained?
 
The potential on the surface must be constant, otherwise there would exist tangential field E that moves the charges until equipotential is reached.
 

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