INaine 3. Pind the relation between the electric potentials below and above b at end may shrink path to zero length an infinite surface with a charge density o. Use the line integral of Б he electric field from below (ā) to above (b) the surface, de. E(f) - - V(6) + Va)
INaine 3. Pind the relation between the electric potentials below and above b at end may shrink path to zero length an infinite surface with a charge density o. Use the line integral of Б he electric field from below (ā) to above (b) the surface, de. E(f) - - V(6) + Va)
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Transcribed Image Text:INaine
3. Pind the relation between the electric potentials below and above
b at end may
shrink path
to zero length
an infinite surface with a charge density o. Use the line integral of
Б
he electric field from below (ā) to above (b) the surface, de. E(f)
- - V(6) + Va)
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