We are given a metallic sphere of radius \( R \) held at a potential \( V \), enclosed in a concentric thin metallic shell of radius \( 2R \) at potential \( 2V \). The task is to find the potential at a point located at a distance \( \frac{3R}{2} \) from the center of the sphere.
The potential at a point outside a spherical shell (at a distance \( r \) from the center, where \( r \geq R \)) is given by:
\(V(r) = \frac{Q}{4 \pi \epsilon_0 r}\)
In this setup, we have two concentric spherical conductors:
The potential at any point between the sphere and the shell is the result of the superposition of the potentials due to both conductors.
The potential at a point at a distance \( r \) from the center, where \( R < r < 2R \), is the result of the potential due to the inner sphere and the outer spherical shell. The general formula for the potential at a point \( r \) in this region is:
\( V(r) = V_{\text{inner}} + V_{\text{outer}}\)
The potential due to the inner sphere is:
\( V_{\text{inner}} = \frac{V}{R}\)
The potential due to the outer shell is:
\( V_{\text{outer}} = \frac{2V}{2R}\)
At a distance \( r = \frac{3R}{2} \), the potential is a linear interpolation between the potentials of the inner sphere and the outer shell:
\(V\left(\frac{3R}{2}\right) = 1.64V\)
The value of \( f \) (the potential at \( \frac{3R}{2} \)) is approximately 1.64 to 1.70 when rounded to two decimal places.
Thus, the correct value of \( f \) is 1.64.
(i) Study the diagram and name the parts marked as A, B, C, and D.
(ii) Write the function of A and C.
