X 5) In Fig. 22.8, a cube of insulating material has one corner at the origin. Each side of the cube has length 0.080 m, so the top face of the cube is parallel to the xz-plane and is at y = 0.08 m. It is observed that there is an electric field E = (3280 N/C my j, that is in the ty direction and whose magnitude depends only on y. Use Gauss's law to calculate the net charge enclosed by the cube. (Note: &o=8.854 x 10-12 C2/N • m2)

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Figure 22.8
X
6) In Fig. 22.8, a cube of insulating material has one corner at the origin. Each side of the
cube has length 0.080 m, so the top face of the cube is parallel to the xz-plane and is at
y = 0.08 m. It is observed that there is an electric field E = (3280 N/C • myj, that is in
the ty direction and whose magnitude depends only on y. Use Gauss's law to calculate
the net charge enclosed by the cube.
(Note: &o=8.854 x 10-12 C2/N m2)
Transcribed Image Text:Figure 22.8 X 6) In Fig. 22.8, a cube of insulating material has one corner at the origin. Each side of the cube has length 0.080 m, so the top face of the cube is parallel to the xz-plane and is at y = 0.08 m. It is observed that there is an electric field E = (3280 N/C • myj, that is in the ty direction and whose magnitude depends only on y. Use Gauss's law to calculate the net charge enclosed by the cube. (Note: &o=8.854 x 10-12 C2/N m2)
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