The induced emf in a coil is given by the formula: \[ \text{emf} = -L \frac{\Delta I}{\Delta t} \] Where:
\( L \) is the inductance of the coil,
\( \Delta I \) is the change in current,
\( \Delta t \) is the time interval during which the change occurs. Given:
\( L = 0.2 \, \text{H} \), - \( \Delta I = 5 \, \text{A} - 2 \, \text{A} = 3 \, \text{A} \),
\( \Delta t = 0.5 \, \text{sec} \).
Substitute the values into the formula: \[ \text{emf} = -0.2 \cdot \frac{3}{0.5} = -0.2 \cdot 6 = -1.2 \, \text{V} \] The negative sign indicates the direction of the induced emf, but the magnitude is \( 1.2 \, \text{V} \).
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: