Understanding the Radial Field Generated by an Infinite Line of Charge

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SUMMARY

An infinite line of charge with a linear charge density of 8.00×10-12 C/m generates an electric field that has only a radial component. This occurs because the field lines are perpendicular to the line of charge, radiating outward for positive charge. The symmetry of the infinite line ensures that any lateral components of the electric field cancel out due to equal charge distribution on either side. Consequently, the equipotential surfaces formed are concentric cylinders around the line of charge.

PREREQUISITES
  • Understanding of electric fields and charge distributions
  • Familiarity with Coulomb's Law
  • Knowledge of equipotential surfaces
  • Basic principles of electrostatics
NEXT STEPS
  • Study the concept of electric field lines and their properties
  • Learn about the mathematical derivation of electric fields from line charges
  • Explore the concept of equipotential surfaces in electrostatics
  • Investigate the effects of different charge densities on electric field strength
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Students of physics, particularly those focusing on electromagnetism, educators teaching electrostatics, and anyone interested in understanding electric fields generated by charge distributions.

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"Stopping the Proton"

Homework Statement



An infinitely long line of charge has a linear charge density of 8.00×10−12 C/m. A proton is at distance 14.0 cm from the line and is moving directly toward the line with speed 1500 m/s.

I just want a better understanding of this statement:

"An infinite line of charge will generate a field with only a radial component."

Why, again? I can post more parts of the problem if that's too confusing.
 
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Because the line charge is infinite, the field lines will all be perpendicular to the wire - radially outward for plus charge - if for no other reason than that any calculation of the field will find as much charge to one side as to the other and any component of the field that might be calculated for charge on one side is canceled out by the field component from an equal charge an equal distance to the other. The equipotential surfaces will then be concentric cylinders.
 

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