Chapter 21: Problem 10
The field of an infinite charged line decreases as \(1 / r .\) Why isn't this a violation of the inverse-square law?
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Chapter 21: Problem 10
The field of an infinite charged line decreases as \(1 / r .\) Why isn't this a violation of the inverse-square law?
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What's the approximate field strength \(1 \mathrm{cm}\) above a sheet of paper carrying uniform surface charge density \(\sigma=45 \mathrm{nC} / \mathrm{m}^{2} ?\)
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.)
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.
If a charged particle were released from rest on a curved field line, would its subsequent motion follow the field line? Explain.
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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