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Chapter 5 Capacitance and Dielectrics

Chapter 5 Capacitance and Dielectrics

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Using Gauss’s law, we have () 00 2 2 S dEAEr E r λ λ π ε πε ∫∫EA⋅== =⇒= A A JGJG w (5.2.5) where λ=Q/L is the charge per unit length. Notice that the electric field is non-vanishing only in the region ar<<b. For r<a, the enclosed charge is since any net charge in a conductor must reside on its surface. Similarly, for , the enclosed

  S law

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