The induced electromotive force (EMF) in a coil due to a changing current is given by Faraday's Law of Induction and is related to the self-inductance (L) by the following formula:
\( EMF = -L \frac{\Delta I}{\Delta t} \)
Where:
We are given:
We need to find the self-inductance \( L \). Rearranging the formula to solve for \( L \):
\( L = -\frac{EMF}{\frac{\Delta I}{\Delta t}} = -\frac{EMF \cdot \Delta t}{\Delta I} \)
Substituting the given values:
\( L = -\frac{100 \, \text{V} \cdot 0.1 \, \text{s}}{5 \, \text{A}} = -\frac{10}{5} \, \text{H} = -2 \, \text{H} \)
Since self-inductance \( L \) is always a positive quantity, we take the absolute value:
\( L = |-2 \, \text{H}| = 2 \, \text{H} \)
Therefore, the self-inductance of the coil is 2 H.
\(\text{ The induced emf } \varepsilon \text{ in a coil is related to the self-inductance } L \text{ by the formula:}\\\)
\[\varepsilon = L \frac{dI}{dt}\]\(\text{where } \frac{dI}{dt} \text{ is the rate of change of current. In this case, } \frac{dI}{dt} = \frac{10 - 5}{0.1} = 50 \, \text{A/s}.\\\)
\(\text{Substituting the values:}\\\)
\(100 = L \times 50 \quad \Rightarrow \quad L = \frac{100}{50} = 2 \, H\)
\(\text{Thus, the self-inductance is } 2 \, H.\)
The Wheatstone bridge is an arrangement of four resistances, say \(R_1, R_2, R_3\), and \(R_4\). The null point condition is given by: