A rubber sheet of infinite size has an area charge density of σ = -66.3 nC/m^2 spread uniformly on its surface. A really really long glass fiber with a line density of 648 nC/m runs parallel to the sheet 45 cm away. What is the electric potential difference due to the sheet halfway between the rubber sheet and the glass fiber?
A rubber sheet of infinite size has an area charge density of σ = -66.3 nC/m^2 spread uniformly on its surface. A really really long glass fiber with a line density of 648 nC/m runs parallel to the sheet 45 cm away. What is the electric potential difference due to the sheet 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 = -66.3 nC/m^2 spread uniformly on its surface. A really really long glass fiber with a line density of 648 nC/m runs parallel to the sheet 45 cm away.
What is the electric potential difference due to the sheet halfway between the rubber sheet and the glass fiber?
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