Chapter 21: Problem 7
In Gauss's law, \(\oint \vec{E} \cdot d \vec{A}=q / \epsilon_{0},\) does the field \(\vec{E}\) necessarily arise only from charges within the closed surface?
Chapter 21: Problem 7
In Gauss's law, \(\oint \vec{E} \cdot d \vec{A}=q / \epsilon_{0},\) does the field \(\vec{E}\) necessarily arise only from charges within the closed surface?
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Get started for freeA spherical shell \(30 \mathrm{cm}\) in diameter carries \(85 \mu \mathrm{C}\) distributed uniformly over its surface. A \(1.0-\mu \mathrm{C}\) point charge is located at the shell's center. Find the electric field strength (a) \(5.0 \mathrm{cm}\) from the center and (b) \(45 \mathrm{cm}\) from the center. (c) How would your answers change if the charge on the shell were doubled?
A \(6.8-\mu \mathrm{C}\) charge and a \(-4.7-\mu \mathrm{C}\) charge are inside an uncharged sphere. What's the electric flux through the sphere?
What's the electric field strength in a region where the flux through a \(1.0 \mathrm{cm} \times 1.0 \mathrm{cm}\) flat surface is \(65 \mathrm{N} \cdot \mathrm{m}^{2} / \mathrm{C},\) if the field is uniform and the surface is at right angles to the field?
An infinitely long rod of radius \(R\) carries a uniform volume charge density \(\rho .\) Show that the electric field strengths outside and inside the rod are given, respectively, by \(E=\rho R^{2} / 2 \epsilon_{0} r\) and \(E=\rho r / 2 \epsilon_{0},\) where \(r\) is the distance from the rod axis. (Although an infinite rod is an impossibility, your answer is a good approximation for the field of a finite rod whose length is much greater than its diameter.)
Eight field lines emerge from a closed surface surrounding an isolated point charge. Would the number of field lines change if a second identical charge were brought to a point just outside the surface? If not, would anything change? Explain.
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