Answer
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Hint: This can be solved by using the electric field due to a uniformly charged disc formula. We shall substitute the given values of radius and electric field at the center of the disc to find the electric field along the axis.
Complete step-by-step answer:
The general expression for an electric field due to a uniformly charged disc of radius R and charge density σ can be written as
${{E}_{x}}=k\sigma 2\pi \left( 1-\dfrac{x}{\sqrt{{{x}^{2}}+{{R}^{2}}}} \right)$
Where, $k=\dfrac{1}{4\pi {{\in }_{0}}}$
On substituting ‘k’ in the formula, we get
${{E}_{x}}=\dfrac{\sigma }{2{{\in }_{0}}}\left( 1-\dfrac{x}{\sqrt{{{x}^{2}}+{{R}^{2}}}} \right)$
Here, the given electric field intensity at the center of the disc shall be ‘E’ i.e., $x=0$,
$E=\dfrac{\sigma }{2{{\in }_{0}}}$
Let electric field along the axis at a distance ‘x’ from the center of the disc be ‘E1’ and written as
${{E}_{1}}=\dfrac{\sigma }{2{{\in }_{0}}}\left( 1-\dfrac{x}{\sqrt{{{x}^{2}}+{{R}^{2}}}} \right)$
As $x=R$, the equation becomes
${{E}_{1}}=\dfrac{\sigma }{2{{\in }_{0}}}\left( 1-\dfrac{R}{\sqrt{{{R}^{2}}+{{R}^{2}}}} \right)$
${{E}_{1}}=\dfrac{\sigma }{2{{\in }_{0}}}\left( 1-\dfrac{R}{\sqrt{2}R} \right)$
On taking ‘R’ common, it gets cancelled
${{E}_{1}}=\dfrac{\sigma }{2{{\in }_{0}}}\left( 1-\dfrac{1}{\sqrt{2}} \right)$
We also know, $E=\dfrac{\sigma }{2{{\in }_{0}}}$
On substituting ‘E’ in the equation, we get
${{E}_{1}}=E\left( 1-\dfrac{1}{\sqrt{2}} \right)$
The percentage of reduction in the value of electric field can be calculated as
$=\dfrac{{{E}_{1}}-E}{E}\times 100$
$=\dfrac{\left( E\left( 1-\dfrac{1}{\sqrt{2}} \right)-E \right)}{E}\times 100$
$=\left( 1-\dfrac{1}{\sqrt{2}}-1 \right)\times 100$
$=-\dfrac{100}{\sqrt{2}}=70.7%$
The negative sign indicates the reduction.
Therefore, the correct answer for the given question is option (A).
Note: The electric field due to a uniformly charged disc is based on the applications of gauss’s law. The law states that the total flux of electric field over a closed surface is equal to $\dfrac{1}{{{\in }_{0}}}$ times the total charge enclosed by the surface.
Complete step-by-step answer:
The general expression for an electric field due to a uniformly charged disc of radius R and charge density σ can be written as
${{E}_{x}}=k\sigma 2\pi \left( 1-\dfrac{x}{\sqrt{{{x}^{2}}+{{R}^{2}}}} \right)$
Where, $k=\dfrac{1}{4\pi {{\in }_{0}}}$
On substituting ‘k’ in the formula, we get
${{E}_{x}}=\dfrac{\sigma }{2{{\in }_{0}}}\left( 1-\dfrac{x}{\sqrt{{{x}^{2}}+{{R}^{2}}}} \right)$
Here, the given electric field intensity at the center of the disc shall be ‘E’ i.e., $x=0$,
$E=\dfrac{\sigma }{2{{\in }_{0}}}$
Let electric field along the axis at a distance ‘x’ from the center of the disc be ‘E1’ and written as
${{E}_{1}}=\dfrac{\sigma }{2{{\in }_{0}}}\left( 1-\dfrac{x}{\sqrt{{{x}^{2}}+{{R}^{2}}}} \right)$
As $x=R$, the equation becomes
${{E}_{1}}=\dfrac{\sigma }{2{{\in }_{0}}}\left( 1-\dfrac{R}{\sqrt{{{R}^{2}}+{{R}^{2}}}} \right)$
${{E}_{1}}=\dfrac{\sigma }{2{{\in }_{0}}}\left( 1-\dfrac{R}{\sqrt{2}R} \right)$
On taking ‘R’ common, it gets cancelled
${{E}_{1}}=\dfrac{\sigma }{2{{\in }_{0}}}\left( 1-\dfrac{1}{\sqrt{2}} \right)$
We also know, $E=\dfrac{\sigma }{2{{\in }_{0}}}$
On substituting ‘E’ in the equation, we get
${{E}_{1}}=E\left( 1-\dfrac{1}{\sqrt{2}} \right)$
The percentage of reduction in the value of electric field can be calculated as
$=\dfrac{{{E}_{1}}-E}{E}\times 100$
$=\dfrac{\left( E\left( 1-\dfrac{1}{\sqrt{2}} \right)-E \right)}{E}\times 100$
$=\left( 1-\dfrac{1}{\sqrt{2}}-1 \right)\times 100$
$=-\dfrac{100}{\sqrt{2}}=70.7%$
The negative sign indicates the reduction.
Therefore, the correct answer for the given question is option (A).
Note: The electric field due to a uniformly charged disc is based on the applications of gauss’s law. The law states that the total flux of electric field over a closed surface is equal to $\dfrac{1}{{{\in }_{0}}}$ times the total charge enclosed by the surface.
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