11. (x points) A square copper plate 1.0 cm thick, 2.0 meters on a side, has a total excess charge of Qtotal = 48 nC. You decide to use Gauss's law to find the electric field a distance of 2.0 mm from the center of the plate. 2.0 m 2.0 m Side View at center 0.01 m Add '+' signs to the Side View sketch to show the location of the electric charge, and add vectors to show the electric field. Point P is 2.0 mm above the surface, and is located in the top of a Gaussian cylinder of radius r that has its lower end inside the copper plate. Give the flux through each of these parts of the cylindrical Gaussian surface, in terms of E, r, and any other variables needed: Circular top Curved sides Circular bottom

Physics for Scientists and Engineers
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Chapter24: Electric Potential
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11. (x points) A square copper plate 1.0 cm thick, 2.0 meters on a side, has a total excess charge of
Qtotal = 48 nC. You decide to use Gauss's law to find the electric field a distance of 2.0 mm from
the center of the plate.
2.0 m
2.0 m
Side View at center
0.01 m
Add '+' signs to the Side View sketch to show the location of the electric charge, and add vectors to
show the electric field.
Point P is 2.0 mm above the surface, and is located in the top of a Gaussian cylinder of radius r that has
its lower end inside the copper plate. Give the flux through each of these parts of the cylindrical
Gaussian surface, in terms of E, r, and any other variables needed:
Circular top
Curved sides
Circular bottom
Transcribed Image Text:11. (x points) A square copper plate 1.0 cm thick, 2.0 meters on a side, has a total excess charge of Qtotal = 48 nC. You decide to use Gauss's law to find the electric field a distance of 2.0 mm from the center of the plate. 2.0 m 2.0 m Side View at center 0.01 m Add '+' signs to the Side View sketch to show the location of the electric charge, and add vectors to show the electric field. Point P is 2.0 mm above the surface, and is located in the top of a Gaussian cylinder of radius r that has its lower end inside the copper plate. Give the flux through each of these parts of the cylindrical Gaussian surface, in terms of E, r, and any other variables needed: Circular top Curved sides Circular bottom
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