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Question: The intensity of an electric field depends only on the coordinate x, y and z as follows \(\overright...

The intensity of an electric field depends only on the coordinate x, y and z as follows E=a(xi+yj+zk)(x2+y2+z2)32\overrightarrow{E}=\dfrac{a({{x}_{i}}+{{y}_{j}}+{{z}_{k}})}{{{({{x}^{2}}+{{y}^{2}}+{{z}^{2}})}^{\dfrac{3}{2}}}} Unit. The electrostatic energy stored between two imaginary concentric spherical shells of radii R and 2R with center at origin is
A)4πε0a2R\dfrac{4\pi {{\varepsilon }_{0}}{{a}^{2}}}{R}
B) 2πε0a2R\dfrac{2\pi {{\varepsilon }_{0}}{{a}^{2}}}{R}
C) πε0a2R\dfrac{\pi {{\varepsilon }_{0}}{{a}^{2}}}{R}
D) aRk\dfrac{aR}{k}

Explanation

Solution

The solution to this problem is obtained by gauss’s diversion theorem. Field is a region where each point has a corresponding value of some physical function. For example, an electric field in a region has some specific direction of E\overrightarrow{E} component at different points. Electric field(E) is a vector quantity.

Complete answer:
In scalar units if the value of physical functions at each point of a field is a scalar quantity then it is a scalar field like temperature of atmosphere, depth of sea water from surfaces etc.
In a vector field if the value of function at each point of a field is vector quantity then it is called vector field like wind velocity of atmosphere ,the force of gravity on a mass in space ,forces on a charged body placed in an electric field etc. Electric field which has both magnitude and direction.
On the sphere the points P(X, Y, Z)
x2+y2+z2=R2{{x}^{2}}+{{y}^{2}}+{{z}^{2}}={{R}^{2}}
A unit vector which is perpendicular to the sphere radially outwards is given by:
N^=xx2+y2+z2i^+yx2+y2+z2j^+Zx2+y2+z2k^ N^=xRi^+yRj^+zRk^ \begin{aligned} & \widehat{N}=\dfrac{x}{\sqrt{{{x}^{2}}+{{y}^{2}}+{{z}^{2}}}}\widehat{i}+\dfrac{y}{\sqrt{{{x}^{2}}+{{y}^{2}}+{{z}^{2}}}}\widehat{j}+\dfrac{Z}{\sqrt{{{x}^{2}}+{{y}^{2}}+{{z}^{2}}}}\widehat{k} \\\ & \widehat{N}=\dfrac{x}{R}\widehat{i}+\dfrac{y}{R}\widehat{j}+\dfrac{z}{R}\widehat{k} \\\ \end{aligned}
On the sphere at point P the electric flux through small area dS is given by:
dϕe=E.dSN^ dϕe=(ax2R(x2+y2)+ay2R(x2+y2))dS dϕe=adSR ϕe=dϕe=adSR ϕe=4πaR \begin{aligned} & d{{\phi }_{e}}=\overrightarrow{E}.dS\widehat{N} \\\ & d{{\phi }_{e}}=(\dfrac{a{{x}^{2}}}{R({{x}^{2}}+{{y}^{2}})}+\dfrac{a{{y}^{2}}}{R({{x}^{2}}+{{y}^{2}})})dS \\\ & d{{\phi }_{e}}=\dfrac{adS}{R} \\\ & {{\phi }_{e}}={{\oint{d\phi }}_{e}}=\oint{\dfrac{adS}{R}} \\\ & {{\phi }_{e}}=4\pi aR \\\ \end{aligned}
By applying gauss law
ϕe=qincε0 qinc=4πε0aR K=14πε0 qinc=aRK \begin{aligned} & {{\phi }_{e}}=\dfrac{{{q}_{inc}}}{{{\varepsilon }_{0}}} \\\ & {{q}_{inc}}=4\pi {{\varepsilon }_{0}}aR \\\ & K=\dfrac{1}{4\pi {{\varepsilon }_{0}}} \\\ & {{q}_{inc}}=\dfrac{aR}{K} \\\ \end{aligned}
The electrostatic energy stored is equal to aRK\dfrac{aR}{K}

So option D is correct

Note:
Students unit vector is the ratio of vector itself by its magnitude and Gauss’s diversion theorem which states that volume integral of the divergence of vector field A\overrightarrow{A}.taken over any volume V is equal to surface integral of A\overrightarrow{A} taken over the closed surface that bonds the volume V V(A).dV=SAdS\int_{V}{(\nabla }\cdot \overrightarrow{A}).dV=\oint\limits_{S}{\overrightarrow{A}\cdot \overrightarrow{dS}}.