Answer
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Hint: Using Gauss law this problem can be solved easily by considering the annular region (the region bounded by the two concentric circles) as the Gaussian surface. In the case of a cylindrical capacitor, the inner and outer radius of the capacitor is considered to be the annular region.
Formula used:
\[\begin{align}
& E\times A=\dfrac{Q}{\varepsilon } \\
& A=2\pi r\times L \\
\end{align}\]
Complete step by step answer:
From given, we have the data,
The magnitude of the electric field = E
The diagram representing the Gaussian surface of the cylindrical capacitor.
Considering the annular region of the cylindrical capacitor as the Gaussian surface, we have,
\[E\times A=\dfrac{Q}{\varepsilon }\] …… (1)
Where E is the electric field, A is the surface area, Q is the charge enclosed and \[\varepsilon \]is the permittivity of the medium.
The surface area is given by,
\[A=2\pi r\times L\] …… (2)
Where r is the radius of the cylindrical capacitor and L is its length.
Substitute the equation (2) in (1), so, we get,
\[E\times (2\pi r\times L)=\dfrac{Q}{\varepsilon }\]
Considering Q’ as the charge per unit length, we get,
\[Q'=\dfrac{Q}{L}\]
Substitute the above value in the equation of electric field,
Thus, the electric field inside the cylindrical capacitor at a distance r from the centre is,
\[E=\dfrac{Q'}{2\pi \varepsilon r}\]
\[\Rightarrow E\propto \dfrac{1}{r}\]
Where \[Q'\]is the charge per unit length of the capacitor and r is the radius of the cylindrical capacitor.
As the magnitude of electric field E in the annular region of a charged cylindrical capacitor varies as \[\dfrac{1}{r}\], where r is the distance from the axis, thus option (C) is correct.
Note:
The things to be on your finger-tips for further information on solving these types of problems are: The electric field inside the annular region is due to the inner cylinder. Thus, the electric field should be calculated from the centre of the cylinder to the radius of the inner cylinder.
Formula used:
\[\begin{align}
& E\times A=\dfrac{Q}{\varepsilon } \\
& A=2\pi r\times L \\
\end{align}\]
Complete step by step answer:
From given, we have the data,
The magnitude of the electric field = E
The diagram representing the Gaussian surface of the cylindrical capacitor.
Considering the annular region of the cylindrical capacitor as the Gaussian surface, we have,
\[E\times A=\dfrac{Q}{\varepsilon }\] …… (1)
Where E is the electric field, A is the surface area, Q is the charge enclosed and \[\varepsilon \]is the permittivity of the medium.
The surface area is given by,
\[A=2\pi r\times L\] …… (2)
Where r is the radius of the cylindrical capacitor and L is its length.
Substitute the equation (2) in (1), so, we get,
\[E\times (2\pi r\times L)=\dfrac{Q}{\varepsilon }\]
Considering Q’ as the charge per unit length, we get,
\[Q'=\dfrac{Q}{L}\]
Substitute the above value in the equation of electric field,
Thus, the electric field inside the cylindrical capacitor at a distance r from the centre is,
\[E=\dfrac{Q'}{2\pi \varepsilon r}\]
\[\Rightarrow E\propto \dfrac{1}{r}\]
Where \[Q'\]is the charge per unit length of the capacitor and r is the radius of the cylindrical capacitor.
As the magnitude of electric field E in the annular region of a charged cylindrical capacitor varies as \[\dfrac{1}{r}\], where r is the distance from the axis, thus option (C) is correct.
Note:
The things to be on your finger-tips for further information on solving these types of problems are: The electric field inside the annular region is due to the inner cylinder. Thus, the electric field should be calculated from the centre of the cylinder to the radius of the inner cylinder.
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