Problem 36
Question
Two circuits have mutual inductance of \(0.09 \mathrm{H}\). Average emf induced in the secondary by a change of current from 0 to \(20 \mathrm{~A}\) in \(0.006 \mathrm{~s}\) in primary will be (a) \(120 \mathrm{~V}\) (b) \(200 \mathrm{~V}\) (c) \(180 \mathrm{~V}\) (d) \(300 \mathrm{~V}\)
Step-by-Step Solution
Verified Answer
The average induced emf is \( 300 \, \mathrm{V} \), so the answer is (d).
1Step 1: Identify Given Values
Extract the given information from the problem. The mutual inductance \( M \) is \( 0.09 \, \mathrm{H} \), the change in current \( \Delta I \) is from \( 0 \, \mathrm{A} \) to \( 20 \, \mathrm{A} \), and the change in time \( \Delta t \) is \( 0.006 \, \mathrm{s} \).
2Step 2: Recall the Formula for Induced EMF
The formula for the average electromotive force (emf) induced in the secondary coil due to a change in current through the primary coil is given by \( \mathcal{E} = M \frac{\Delta I}{\Delta t} \).
3Step 3: Calculate the Change in Current
Calculate the change in current \( \Delta I \) which is the final current minus the initial current. Since it changes from \( 0 \) to \( 20 \), \( \Delta I = 20 \, \mathrm{A} - 0 \, \mathrm{A} = 20 \, \mathrm{A} \).
4Step 4: Substitute Values into the Formula
Substitute the given values into the emf formula. We have \[ \mathcal{E} = 0.09 \, \mathrm{H} \times \frac{20 \, \mathrm{A}}{0.006 \, \mathrm{s}} \].
5Step 5: Calculate the Induced EMF
Calculate the emf using the substituted values: \[ \mathcal{E} = 0.09 \times \frac{20}{0.006} = 0.09 \times 3333.33 \approx 300 \, \mathrm{V} \].
6Step 6: Choose the Correct Answer
Match the calculated result of \( 300 \, \mathrm{V} \) with the options given. The correct option is (d) \( 300 \, \mathrm{V} \).
Key Concepts
Electromotive ForceChange in CurrentMutual Inductance Formula
Electromotive Force
Electromotive force, often abbreviated as emf, is a fundamental concept in electromagnetism. It represents the energy provided by a source to move electrical charge through a circuit.
Emf can be thought of as the electrical "pressure" that pushes charges through a conductor. It is measured in volts (V) and is similar to how water pressure pushes water through pipes.
In a scenario involving mutual inductance, the emf can be induced in a secondary coil when the current through a primary coil changes. This happens due to the magnetic field created by the current flow.
Emf can be thought of as the electrical "pressure" that pushes charges through a conductor. It is measured in volts (V) and is similar to how water pressure pushes water through pipes.
In a scenario involving mutual inductance, the emf can be induced in a secondary coil when the current through a primary coil changes. This happens due to the magnetic field created by the current flow.
- The faster the change in current, the greater the induced emf.
- The induced emf is directly proportional to the rate of current change and the mutual inductance between the coils.
Change in Current
The change in current, often denoted as \( \Delta I \), is a measure of how much the current flowing through a circuit changes over a specific period.
This concept is pivotal in understanding how and why the electromotive force is induced in circuits that are mutually inductive.
In the context of the exercise, the current changes from 0 to 20 A, making \( \Delta I = 20 \text{ A} \).
This concept is pivotal in understanding how and why the electromotive force is induced in circuits that are mutually inductive.
In the context of the exercise, the current changes from 0 to 20 A, making \( \Delta I = 20 \text{ A} \).
- \( \Delta I \) indicates the total amount of change in current, which tells us the speed and magnitude of this change.
- The change in current affects how quickly the magnetic field around the primary circuit is altered.
Mutual Inductance Formula
The mutual inductance formula expresses the relationship between the induced emf in one coil and the change in current through another coil. It is given by the equation:\[ \mathcal{E} = M \frac{\Delta I}{\Delta t}\] where:
In our exercise, using the given values of \( M = 0.09 \text{ H} \), \( \Delta I = 20 \text{ A} \), and \( \Delta t = 0.006 \text{ s} \), the induced emf turns out to be approximately 300 V.
This relationship is fundamental in designing and studying systems involving inductive components, like transformers and inductors, ensuring efficient energy transfer through varying magnetic fields.
- \( \mathcal{E} \) is the induced electromotive force (emf) in volts.
- \( M \) is the mutual inductance in henries (H).
- \( \Delta I \) is the change in current in amperes (A).
- \( \Delta t \) is the time period over which the change occurs, in seconds (s).
In our exercise, using the given values of \( M = 0.09 \text{ H} \), \( \Delta I = 20 \text{ A} \), and \( \Delta t = 0.006 \text{ s} \), the induced emf turns out to be approximately 300 V.
This relationship is fundamental in designing and studying systems involving inductive components, like transformers and inductors, ensuring efficient energy transfer through varying magnetic fields.
Other exercises in this chapter
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