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 \( \mathbf{(A)} \).
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: