Chapter 21: Problem 22
A flat surface with area \(0.14 \mathrm{m}^{2}\) lies in the \(x-y\) plane, in a uniform electric field \(\vec{E}=5.1 \hat{\imath}+2.1 \hat{\jmath}+3.5 \hat{k} \mathrm{kN} / \mathrm{C} .\) Find the flux through the surface.
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Chapter 21: Problem 22
A flat surface with area \(0.14 \mathrm{m}^{2}\) lies in the \(x-y\) plane, in a uniform electric field \(\vec{E}=5.1 \hat{\imath}+2.1 \hat{\jmath}+3.5 \hat{k} \mathrm{kN} / \mathrm{C} .\) Find the flux through the surface.
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Why can't you use Gauss's law to determine the field of a uniformly charged cube? Why couldn't you use a cubical Gaussian surface?
Find the field produced by a uniformly charged sheet carrying \(87 \mathrm{pC} / \mathrm{m}^{2}.\)
A 15 -nC point charge is at the center of a thin spherical shell of radius \(10 \mathrm{cm},\) carrying -22 nC of charge distributed uniformly over its surface. Find the magnitude and direction of the electric field (a) \(2.2 \mathrm{cm},\) (b) \(5.6 \mathrm{cm},\) and (c) \(14 \mathrm{cm}\) from the point charge.
An irregular conductor containing an irregular, empty cavity carries a net charge \(Q\). (a) Show that the electric field inside the cavity must be zero. (b) If you put a point charge inside the cavity, what value must it have in order to make the charge density on the outer surface of the conductor everywhere zero?
The electric field in a certain region is given by \(\vec{E}=a x \hat{\imath},\) where \(a=40 \mathrm{N} / \mathrm{C} \cdot \mathrm{m}\) and \(x\) is in meters. Find the volume charge density in the region. (Hint: Apply Gauss's law to a cube 1 m on a side.)
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