Gauss' Law - difficulty understanding this example

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SUMMARY

This discussion focuses on the application of Gauss' Law to a long straight wire and a surrounding cylindrical conductor. The charge per unit length (λ) is distributed on the surface of the wire, resulting in an electric field of zero within the conductor for regions where no enclosed charge exists. The inner surface of the cylinder has a charge of -λ, which neutralizes the electric field from the inner wire, ensuring that the electric field does not penetrate the metal cylinder. This understanding clarifies the behavior of electric fields in conductive materials.

PREREQUISITES
  • Understanding of Gauss' Law
  • Familiarity with electric fields and charge distributions
  • Knowledge of cylindrical symmetry in electrostatics
  • Basic concepts of conductors and insulators
NEXT STEPS
  • Study the derivation of Gauss' Law in various geometries
  • Explore the concept of electric field lines and their behavior in conductors
  • Learn about charge distribution on conductors in electrostatic equilibrium
  • Investigate the implications of Gauss' Law in real-world applications, such as capacitors
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Students of physics, particularly those studying electromagnetism, educators explaining Gauss' Law, and anyone seeking to deepen their understanding of electric fields in conductive materials.

NewtonianAlch
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Homework Statement



[PLAIN]http://img851.imageshack.us/img851/5741/86853377.jpg


The Attempt at a Solution



For the long straight wire, the charge per unit length λ is already given, this is distributed on the surface of the wire. The electric field is zero for anything less than r1, because there is no enclosed charge inside the metal.

In the solutions booklet it says that the charge per unit length for the inner surface of the cylinder is -λ so that the internal charge adds to zero for r2 < r < r3.

What do they mean by that, and how did they get -λ ?

I understand that for r greater than r2, but less than r3, the same principle applies as it did earlier, the charge is on the surface, and no enclosed charge inside the metal, so therefore the electric field is zero inside. But why is -λ the charge per unit length for the inner surface of the cylinder?
 
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The charge on the inner wire attracts an opposite charge to the inner surface of the cylinder. This charge is what neutralizes the electric field over the transition into the metal cylinder. Otherwise the electric field due to the charge on the inner wire would extend through the metal cylinder, and we know that this doesn't happen!
 
Ah yes, that makes sense now that you put it that way! Of course...
 

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