90 mH
120 mH
45 mH
30 mH
60 mH
Given:
Step 1: Find the Current (\( I \))
The power dissipated in the resistor is given by:
\[ P = I^2 R \]
Solving for \( I \):
\[ I = \sqrt{\frac{P}{R}} = \sqrt{\frac{200}{50}} = \sqrt{4} = 2 \, \text{A} \]
Step 2: Relate Energy to Inductance (\( L \))
The energy stored in the inductor's magnetic field is:
\[ E = \frac{1}{2} L I^2 \]
Solving for \( L \):
\[ L = \frac{2E}{I^2} = \frac{2 \times 0.180}{2^2} = \frac{0.360}{4} = 0.090 \, \text{H} = 90 \, \text{mH} \]
Step 1: Recall the formulas for magnetic field energy and power dissipation.
The magnetic field energy stored in an inductor is given by:
\[ U = \frac{1}{2} L I^2, \]
where \( U \) is the energy stored, \( L \) is the inductance, and \( I \) is the current through the inductor.
The power dissipated as heat in the resistor is given by:
\[ P = I^2 R, \]
where \( P \) is the power dissipated, \( R \) is the resistance, and \( I \) is the current.
Step 2: Solve for the current \( I \).
We are given that the power dissipated as heat is \( P = 200 \, \text{W} \) and the resistance is \( R = 50 \, \Omega \). Substituting into the formula for power:
\[ 200 = I^2 \cdot 50. \]
Solve for \( I^2 \):
\[ I^2 = \frac{200}{50} = 4. \]
Taking the square root:
\[ I = \sqrt{4} = 2 \, \text{A}. \]
Step 3: Solve for the inductance \( L \).
We are given that the magnetic field energy stored is \( U = 180 \, \text{mJ} = 0.180 \, \text{J} \). Using the formula for magnetic field energy:
\[ U = \frac{1}{2} L I^2. \]
Substitute \( U = 0.180 \, \text{J} \) and \( I^2 = 4 \):
\[ 0.180 = \frac{1}{2} L \cdot 4. \]
Simplify:
\[ 0.180 = 2L. \]
Solve for \( L \):
\[ L = \frac{0.180}{2} = 0.090 \, \text{H} = 90 \, \text{mH}. \]
Final Answer: The inductance of the coil is \( \mathbf{90 \, \text{mH}} \), which corresponds to option \( \mathbf{(A)} \).
A circular coil of diameter 15 mm having 300 turns is placed in a magnetic field of 30 mT such that the plane of the coil is perpendicular to the direction of the magnetic field. The magnetic field is reduced uniformly to zero in 20 ms and again increased uniformly to 30 mT in 40 ms. If the EMFs induced in the two time intervals are \( e_1 \) and \( e_2 \) respectively, then the value of \( e_1 / e_2 \) is:
Conductor wire ABCDE with each arm 10 cm in length is placed in magnetic field of $\frac{1}{\sqrt{2}}$ Tesla, perpendicular to its plane. When conductor is pulled towards right with constant velocity of $10 \mathrm{~cm} / \mathrm{s}$, induced emf between points A and E is _______ mV.} 
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: