\(\frac{R_2^2}{R_1}\)
\(\frac{R_1}{R_2}\)
\(\frac{R_2}{R_1}\)
\(\frac{R_1^2}{R_2}\)
To determine the mutual inductance between two concentric conducting loops of radii \(R_1\) and \(R_2\), where \(R_1\) (radius of the larger loop) is much greater than \(R_2\) (radius of the smaller loop), we must understand the concept of mutual inductance:
Mutual inductance (\(M\)) between two loops is a measure of the magnetic linkage between them. When one loop carries a current, it generates a magnetic field that induces an EMF in the other loop.
Given the configuration:
The mutual inductance can be expressed using the following approximation due to the large ratio:
The magnetic flux \(\Phi\) through the smaller loop is then given by: \(\Phi = B \times \pi R_2^2 = \frac{\mu_0 I \pi R_2^2}{2R_1}\)
By definition, mutual inductance \(M\) is: \(M = \frac{\Phi}{I} = \frac{\mu_0 \pi R_2^2}{2R_1}\)
Therefore, the mutual inductance is directly proportional to: \(\frac{R_2^2}{R_1}\)
Thus, the correct answer is: \(\frac{R_2^2}{R_1}\)
This approach assumes the radius \(R_1\) of the larger loop is much larger than that of the smaller loop \(R_2\), thus justifying the approximation used for the uniform magnetic field over the smaller loop area.