A rubber sheet of infinite size has an area charge density of σ = -48.5 nC/m^2 spread uniformly on its surface. A really really (I mean really!) long glass fiber with a line density of 533 nC/m runs parallel to the sheet 57 cm away. What is the electric potential difference halfway between the rubber sheet and the glass fiber?

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A rubber sheet of infinite size has an area charge density of σ = -48.5 nC/m^2 spread uniformly on its surface. A really really (I mean really!) long glass fiber with a line density of 533 nC/m runs parallel to the sheet 57 cm away. What is the electric potential difference halfway between the rubber sheet and the glass fiber?

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