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 block of certain mass is placed on a rough floor. The coefficients of static and kinetic friction between the block and the floor are 0.4 and 0.25 respectively. A constant horizontal force \( F = 20 \, \text{N} \) acts on it so that the velocity of the block varies with time according to the following graph. The mass of the block is nearly (Take \( g = 10 \, \text{m/s}^2 \)):
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
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: