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 \( 1.2 \, \text{V} \).
The induced emf in a coil is given by Faraday's law of electromagnetic induction: \[ \varepsilon = -L \frac{\Delta I}{\Delta t} \] where:
\( \varepsilon \) is the induced emf,
\( L \) is the inductance of the coil,
\( \Delta I \) is the change in current,
\( \Delta t \) is the time interval during which the current changes. Given:
\( L = 0.2 \, \text{H} \),
Initial current \( I_{\text{initial}} = 5 \, \text{A} \),
Final current \( I_{\text{final}} = 2 \, \text{A} \),
\( \Delta t = 0.5 \, \text{sec} \).
The change in current is: \[ \Delta I = I_{\text{final}} - I_{\text{initial}} = 2 \, \text{A} - 5 \, \text{A} = -3 \, \text{A} \] Now, substituting the values into the formula for induced emf: \[ \varepsilon = -0.2 \times \frac{-3}{0.5} = 0.2 \times 6 = 1.2 \, \text{V} \] Thus, the magnitude of the average induced emf is \({1.2 \, \text{V}} \).
A wooden block of mass M lies on a rough floor. Another wooden block of the same mass is hanging from the point O through strings as shown in the figure. To achieve equilibrium, the coefficient of static friction between the block on the floor and the floor itself is
In an experiment to determine the figure of merit of a galvanometer by half deflection method, a student constructed the following circuit. He applied a resistance of \( 520 \, \Omega \) in \( R \). When \( K_1 \) is closed and \( K_2 \) is open, the deflection observed in the galvanometer is 20 div. When \( K_1 \) is also closed and a resistance of \( 90 \, \Omega \) is removed in \( S \), the deflection becomes 13 div. The resistance of galvanometer is nearly:
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: