Rho (greek letter, not sure on spelling)

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SUMMARY

The discussion centers on the concept of volume charge density, denoted as rho (ρ), and its application in electrostatics. Participants clarify that while surface charges are common in conductors, volume charge density is relevant for insulating materials where charge remains distributed throughout the volume. The conversation emphasizes the importance of understanding Gauss's Law and the behavior of electric fields in relation to volume charge distributions, particularly in spherical geometries.

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  • Understanding of Gauss's Law
  • Familiarity with electric fields and charge distributions
  • Knowledge of conductors vs. insulators
  • Basic principles of electrostatics
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  • Study the application of Gauss's Law to spherical charge distributions
  • Explore the concept of electric fields generated by volume charge densities
  • Investigate the differences between conductors and insulators in electrostatics
  • Learn about the mathematical treatment of charge distributions in electrostatics
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Students of physics, electrical engineers, and anyone interested in understanding electrostatics and charge distribution principles.

Bad-Wolf
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I don't quite understand how to use rho charge per volume. I understand the applications of lamda and sigma as sigma is useful Gauss's Law and lambda is easy when dealing with wires and such. However, how the hell do you use charge per volume? I mean charges only occupy the surfaces of conductors... What law or physical concept can I use to determine how a sphere with volume charge density rho would effect well anything.

Basically, what laws or tricks do I use when working with rho? How could a sphere have a volume charge density when all the charges are on the surface to begin with?
 
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I believe charge per unit volume applies when you are dealing with an insulating object that has had a charge applied to it. As my prof would say, when you apply a charge to an insulating object, the charge stays where you put it. so if you have an insulating object with the charge evenly distributed throughout, it stays there, rather than moving to the surfaces, thus charge is equally distributed through the volume of the object.

please anyone correct me if I'm wrong.
 

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