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: Aug 18, 2024
  • 90 mH

  • 120 mH

  • 45 mH

  • 30 mH

  • 60 mH

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The Correct Option is A

Approach Solution - 1

The correct answer is (A): 90 mH
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Approach Solution -2

To find the inductance of the coil, let's use the information provided:

1. Internal resistance (\( R \)): 50 Ω
2. Stored magnetic field energy (\( E \)): 180 mJ = 0.18 J
3. Power dissipation (\( P \)): 200 W
4. Current (\( I \)): 9 A

First, we need to confirm the power dissipation due to the resistance. The power dissipated by a resistor is given by:

\[ P = I^2 R \]

Substituting the given values:

\[ P = 9^2 \times 50 \]
\[ P = 81 \times 50 \]
\[ P = 4050 \text{ W} \]

Since the problem states that the power dissipation is 200 W, this discrepancy suggests that either the stated current or the stated power dissipation might be incorrect. Assuming the given power dissipation is correct and constant, we need to check the current using:

\[ I = \sqrt{\frac{P}{R}} \]

So,

\[ I = \sqrt{\frac{200}{50}} \]
\[ I = \sqrt{4} \]
\[ I = 2 \text{ A} \]

Now, we assume the current 2 A is correct and use it to find the inductance of the coil.

The energy stored in the inductor is given by:

\[ E = \frac{1}{2} L I^2 \]

Rearranging for \( L \):

\[ L = \frac{2E}{I^2} \]

Substitute the given values:

\[ L = \frac{2 \times 0.18}{2^2} \]
\[ L = \frac{0.36}{4} \]
\[ L = 0.09 \text{ H} \]

Therefore, the inductance of the coil is \( 0.09 \text{ H} \) or \( 90 \text{ mH} \).
So The correct Answer is Option  (A): 90 mH

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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.