\(\frac{R_2^2}{R_1}\)
\(\frac{R_1}{R_2}\)
\(\frac{R_2}{R_1}\)
\(\frac{R_1^2}{R_2}\)
Magnetic field at the center of primary coil
\(B=\frac{\mu_0i_1}{2R_1}\)
Now, considering it to be uniform, magnetic flux passing through secondary coil is
\(\phi_2=BA=\frac{\mu_0i_1}{2R_1}(\pi R_{2}^2)\)
Now, \(M=\frac{\phi_2}{i_1}\)
\(=\frac{\mu_0\pi R_{2}^2}{2R_1}\)
\(\therefore\ \ M \propto \frac{R_2^{2}}{R_1}\)
Therefore, the correct option is (A) : \(\frac{R_2^2}{R_1}\).
AB is a part of an electrical circuit (see figure). The potential difference \(V_A - V_B\), at the instant when current \(i = 2\) A and is increasing at a rate of 1 amp/second is:
Inductance is a key parameter in electrical and electronic circuit designs. Like resistance and capacitance, it is a basic electrical measurement that affects all circuits to some degree.
Inductance is used in many areas of electrical and electronic systems and circuits. The electronic components can be in a variety of forms and may be called by a variety of names: coils, inductors, chokes, transformers, . . . Each of these may also have a variety of different variants: with and without cores and the core materials may be of different types.
There are two ways in which inductance is used: