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.
A conducting square loop initially lies in the $ XZ $ plane with its lower edge hinged along the $ X $-axis. Only in the region $ y \geq 0 $, there is a time dependent magnetic field pointing along the $ Z $-direction, $ \vec{B}(t) = B_0 (\cos \omega t) \hat{k} $, where $ B_0 $ is a constant. The magnetic field is zero everywhere else. At time $ t = 0 $, the loop starts rotating with constant angular speed $ \omega $ about the $ X $ axis in the clockwise direction as viewed from the $ +X $ axis (as shown in the figure). Ignoring self-inductance of the loop and gravity, which of the following plots correctly represents the induced e.m.f. ($ V $) in the loop as a function of time:
A conducting square loop of side $ L $, mass $ M $, and resistance $ R $ is moving in the $ XY $ plane with its edges parallel to the $ X $ and $ Y $ axes. The region $ y \geq 0 $ has a uniform magnetic field, $ \vec{B} = B_0 \hat{k} $. The magnetic field is zero everywhere else. At time $ t = 0 $, the loop starts to enter the magnetic field with an initial velocity $ v_0 \hat{j} \, \text{m/s} $, as shown in the figure. Considering the quantity $ K = \frac{B_0^2 L^2}{RM} $ in appropriate units, ignoring self-inductance of the loop and gravity, which of the following statements is/are correct:
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
The circuit shown in the figure contains two ideal diodes \( D_1 \) and \( D_2 \). If a cell of emf 3V and negligible internal resistance is connected as shown, then the current through \( 70 \, \Omega \) resistance (in amperes) is: