Question:

An inductor coil with an internal resistance of 50 Ω stores magnetic field energy 180 mJ and dissipates energy as heat at the rate of 200 W when a constant current 9 passed through it. The inductance of the coil will be:

Updated On: Apr 7, 2025
  • 90 mH

  • 120 mH

  • 45 mH

  • 30 mH

  • 60 mH

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The Correct Option is A

Approach Solution - 1

Given:

  • Internal resistance, \( R = 50 \, \Omega \)
  • Magnetic field energy stored, \( E = 180 \, \text{mJ} = 0.180 \, \text{J} \)
  • Power dissipated as heat, \( P = 200 \, \text{W} \)

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 \( L \):

\[ L = \frac{2E}{I^2} = \frac{2 \times 0.180}{2^2} = \frac{0.360}{4} = 0.090 \, \text{H} = 90 \, \text{mH} \]

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Approach Solution -2

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

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Top Questions on Electromagnetic induction

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Concepts Used:

Inductance

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:

  • Self-inductance: Self-inductance is the property of a circuit, often a coil, whereby a change in current causes a change in voltage in that circuit due to the magnetic effect of caused by the current flow. It can be seen that self-inductance applies to a single circuit - in other words it is an inductance, typically within a single coil. This effect is used in single coils or chokes.
  • Mutual-inductance: Mutual inductance is an inductive effect where a change in current in one circuit causes a change in voltage across a second circuit as a result of a magnetic field that links both circuits. This effect is used in transformers.