Electric potential for a sphere of charge

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SUMMARY

The electric potential at the origin of a sphere with a radius of 65 cm and equal charges of 2 µC placed at 72-degree intervals along the equator is calculated to be 138 kV. The capacitance of the sphere is determined using the formula C = 4πε0R, resulting in a value of 7.23×10^-11 F. The potential is uniform across the surface and inside the sphere, as it behaves like a conducting sphere. However, the potential at the north pole requires consideration of the individual charges rather than treating the sphere as conducting, leading to confusion in the solution process.

PREREQUISITES
  • Understanding of electric potential and capacitance
  • Familiarity with Coulomb's law and the Coulomb constant
  • Knowledge of the formula for electric potential due to point charges
  • Basic concepts of spherical charge distributions
NEXT STEPS
  • Study the derivation and applications of the electric potential formula V = 1/(4πε0)∑(qi/ri)
  • Learn about the properties of conducting spheres and their electric fields
  • Explore the concept of electric potential due to discrete charge distributions
  • Investigate the implications of charge placement on electric potential in spherical geometries
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Students and educators in physics, electrical engineers, and anyone studying electrostatics and electric potential in spherical charge configurations.

peaceandlove
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Homework Statement


A sphere with radius 65 cm has its center at the origin. Equal charges of 2 µC are placed at 72 degree intervals along the equator of the sphere. The Coulomb constant is 8.99×10 N·m^2 / C^2. (a) What is the electric potential at the origin? Answer in units of kV. (b) What is the electric potential at the north pole? Answer in units of kV.


Homework Equations


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The Attempt at a Solution


The capacitance of an isolated sphere is C = 4*π*ε0*R = (1/K)*R where K = electric constant = 8.99*10^9 N-m²/C². C = 7.23*10^-11 F. The total charge on the sphere is 2*10^-6*(360/72) = 10*10^-6 C. It doesn't matter where the charges are, the conducting sphere will have the same potential at all points on the surface and inside the sphere. V = Q/C = 10*10^-6 / 7.23*10^-11 = 1.38*10^5 V = 138 kV.

The "north pole" would be at the "top" of the sphere, the equator being defined by the location of the charges. Of course, there is no distinction between "top" and "bottom", but it doesn't matter, since the potential is the same everywhere on the sphere. However, my answer got marked wrong for part (b), and I'm not sure why.
 
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I don't think that the sphere is conducting. In fact, I think that you whould basically ignore the sphere, and simply consider the ring of charges. The problem is worded strangely.
 
Could you please explain how you would solve for (b)? Since there are 2 µC at 72 degree intervals along the equation, I tried dividing 2 µC by C, but that is wrong as well.
 
Are you familiar with this equation?
V = \frac{1}{4\pi\epsilon_0}\sum_i\frac{q_i}{r_i}
If not... you have some catching up to do :wink:
 

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