To find the ratio of the radii of the spheres, we need to determine the change in the capacitance of the isolated conducting sphere when it is enclosed by a concentric conducting sphere connected to the earth.
The capacitance \( C \) of an isolated conducting sphere of radius \( R_1 \) is given by:
\(C = 4 \pi \epsilon_0 R_1\)
When the sphere is enclosed by a larger concentric conducting sphere of radius \( R_2 \) connected to earth, the capacitance becomes:
\(C' = 4 \pi \epsilon_0 \frac{R_1 R_2}{R_2 - R_1}\)
According to the problem, the capacitance increases by a factor of \( n \). Therefore:
\(C' = nC\)
Substituting the expression for \( C \) and equating, we have:
\(4 \pi \epsilon_0 \frac{R_1 R_2}{R_2 - R_1} = n \times 4 \pi \epsilon_0 R_1\)
Simplifying this equation gives:
\(\frac{R_1 R_2}{R_2 - R_1} = n R_1\)
Canceling \( R_1 \) from both sides:
\(\frac{R_2}{R_2 - R_1} = n\)
Rearranging for \( R_2/R_1 \), we get:
\(\frac{R_2}{R_1} = n + n \frac{R_1}{R_2} \Rightarrow 1 + \frac{R_1}{R_2} = \frac{n}{n-1}\)
Thus, the ratio of their radii is:
\(\frac{R_2}{R_1} = \frac{n}{n-1}\)
Therefore, the correct answer is:
\(\frac{n}{n-1}\)
A beam of unpolarised light of intensity \( I_0 \) is passed through a polaroid A and then through another polaroid B which is oriented so that its principal plane makes an angle of 45° relative to that of A. The intensity of emergent light is:
Two polaroide $A$ and $B$ are placed in such a way that the pass-axis of polaroids are perpendicular to each other Now, another polaroid $C$ is placed between $A$ and $B$ bisecting angle between them If intensity of unpolarized light is $I _0$ then intensity of transmitted light after passing through polaroid $B$ will be: