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A point charge qq is brought to a position a distance dd away from an infinite...
Feb 15, 2024
A point charge qq is brought to a position a distance dd away from an infinite plane conductor held at zero potential. Using the method of images, find the surface-charge density induced on the plane, and find the force between the plane and the charge by using Coulomb’s law for the force between the charge.
A
Key Concept
Method of Images and Surface Charge Density
Explanation
The method of images involves replacing the conducting plane with a virtual charge (image charge) of equal magnitude but opposite sign, located symmetrically on the other side of the plane at a distance dd. The surface charge density σ\sigma on the plane can be found using the principle that the electric field just outside a conductor is perpendicular to the surface and has a magnitude of σϵ0\frac{\sigma}{\epsilon_0}. For a point charge qq at a distance dd from the plane, the surface charge density at a point rr from the projection of qq onto the plane is given by σ(r)=q2πϵ0(d2+r2)3/2\sigma(r) = \frac{-q}{2\pi\epsilon_0(d^2+r^2)^{3/2}}.
Key Concept
Coulomb's Law and Force Calculation
Explanation
The force between the point charge qq and its image charge q-q can be calculated using Coulomb's law as if they were two point charges in free space. The force is attractive and given by F=q24πϵ0(2d)2F = \frac{q^2}{4\pi\epsilon_0(2d)^2}. This is the magnitude of the force that the plane exerts on the point charge qq.
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