Given Information:
Initial current, \( I_i = 2\,A \)
Final current, \( I_f = 5\,A \)
Change in time, \( \Delta t = 0.3\,s \)
Induced emf, \( E = 1.0\,V \)
Step-by-Step Explanation:
Step 1: Using formula for induced emf due to self-induction:
Self-induced emf (\( E \)) in a coil is given by the formula:
\[ E = L \frac{\Delta I}{\Delta t} \]
Where \( L \) is the self-inductance, \( \Delta I \) is the change in current, and \( \Delta t \) is the time interval.
Step 2: Solve for self-inductance \( L \):
\[ L = \frac{E \times \Delta t}{\Delta I} \]
Calculate change in current, \( \Delta I \):
\[ \Delta I = I_f - I_i = 5\,A - 2\,A = 3\,A \]
Substitute values:
\[ L = \frac{1.0\,V \times 0.3\,s}{3\,A} = \frac{0.3}{3} = 0.1\,H \]
Step 3: Convert inductance into millihenry (mH):
\[ 0.1\,H = 0.1 \times 1000\,mH = 100\,mH \]
Final Conclusion:
The self-inductance of the coil is 100 mH.
The induced emf in a coil is given by the formula: \[ \text{emf} = L \cdot \frac{\Delta I}{\Delta t} \] where:
\( L \) is the self-inductance of the coil,
\( \Delta I \) is the change in current, and
\( \Delta t \) is the time interval. We are given:
\( \Delta I = 5 \, \text{A} - 2 \, \text{A} = 3 \, \text{A} \),
\( \Delta t = 0.3 \, \text{s} \),
emf = 1.0 V.
Using the formula, we solve for \( L \): \[ 1.0 = L \cdot \frac{3}{0.3} \] \[ 1.0 = L \cdot 10 \] \[ L = \frac{1.0}{10} = 0.1 \, \text{H} = 100 \, \text{mH} \] Thus, the self-inductance of the coil is 100 mH.
Show that the energy required to build up the current \( I \) in a coil of inductance \( L \) is \( \frac{1}{2} L I^2 \).
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
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: