Note: $\hat{a}$, $\hat{b}$, and $\hat{c}$ are unit vectors along the $x$, $y$, and $z$ directions, respectively.
The problem asks us to find the electric flux density, denoted by $\vec{D}$, at a specific point $P(0, 0, 5)$ caused by an infinite sheet of uniform charge lying on the $z=0$ plane.
For an infinite sheet of charge with uniform surface charge density $\rho_s$, the electric flux density $\vec{D}$ is constant everywhere (except on the sheet itself) and is directed perpendicularly away from the sheet if $\rho_s$ is positive.
The formula for the electric flux density due to an infinite sheet of charge is:
$ \vec{D} = \frac{\rho_s}{2} \hat{n} $Where:
In this specific problem:
Substituting the values into the formula:
$ \vec{D} = \frac{10 \text{ C/m}^2}{2} \hat{c} $ $ \vec{D} = 5 \hat{c} \text{ C/m}^2 $The relative permittivity ($\epsilon_r = 10$) affects the electric field intensity ($\vec{E} = \frac{\vec{D}}{\epsilon_r \epsilon_0}$), but it does not change the formula for the electric flux density $\vec{D}$ itself, which depends directly on the surface charge density and geometry.
The calculated electric flux density $\vec{D}$ at point $P(0, 0, 5)$ is $5 \hat{c} \text{ C/m}^2$. This matches one of the given options.
A uniform ring charge of radius $R$ carries a total charge $Q$. Which one of the following options correctly quantifies the magnitude of the force on a point charge of strength $q$ kept at the center of the ring?
($\epsilon$ is the permittivity of the medium)
For a uniform line charge of 8 nc/m lying along the z axis, the electric field at a radius of 3 m from the uniform line is given by :
The current in a coil of inductance 5 H changes linearly from 10 A to 2 A in t seconds. If the induced emf is 40 V, what is the time t?
What are the materials which exhibit electric polarization even in the absence of an applied electrical field?
What is the relative permittivity of slate dielectric?