In a pair of adjacent coils, for a change of current in one of the coils from 0 A to 10 A in 0.25 s, the magnetic flux in the adjacent coil changes by 15 Wb. The mutual inductance of the coils is:
1.5 H
Mutual inductance is a property of two adjacent coils where a change in current in one coil induces an electromotive force (EMF) in the other coil. It quantifies how effectively a change in current in one coil can induce a voltage in a nearby coil through the magnetic flux linkage.
The relationship between the change in magnetic flux ($\Delta \Phi_2$) in the second coil and the change in current ($\Delta I_1$) in the first coil is given by the formula:
\(\Delta \Phi_2 = M \Delta I_1\)
where \(M\) is the mutual inductance between the two coils.
We are given the following information:
Using the formula \(\Delta \Phi_2 = M \Delta I_1\), we can solve for \(M\):
\(15 \text{ Wb} = M \times 10 \text{ A}\)
To find \(M\), we rearrange the equation:
\(M = \frac{\Delta \Phi_2}{\Delta I_1}\)
\(M = \frac{15 \text{ Wb}}{10 \text{ A}}\)
\(M = 1.5 \text{ H}\)
The mutual inductance of the coils is 1.5 H.
Based on the provided values, the mutual inductance between the adjacent coils is calculated to be 1.5 H.
| Concept | Definition/Formula | Units |
|---|---|---|
| Mutual Inductance (\(M\)) | Relates change in flux in one coil to change in current in another: \(\Delta \Phi_2 = M \Delta I_1\) | Henry (H) |
| Magnetic Flux (\(\Phi\)) | Measure of the total magnetic field lines passing through a given area | Weber (Wb) |
| Current (\(I\)) | Flow of electric charge | Ampere (A) |
| Induced EMF (\(\mathcal{E}\)) | Voltage induced in a coil due to changing magnetic flux or current: \(\mathcal{E}_2 = -M \frac{dI_1}{dt}\) | Volt (V) |
Mutual inductance depends on the geometry of the two coils (their size, shape, distance apart, and relative orientation) and the properties of the core material between them (if any). It is a reciprocal property; the mutual inductance from coil 1 to coil 2 is the same as the mutual inductance from coil 2 to coil 1 (\(M_{12} = M_{21} = M\)).
Mutual inductance is important in many electrical components and circuits, including transformers, induction motors, and some types of sensors. In transformers, the principle of mutual inductance is used to transfer energy between coils with different numbers of turns to step up or step down voltage.
The unit of mutual inductance, the Henry (H), is defined as the mutual inductance between two circuits when a current change of one ampere per second in one circuit induces an electromotive force of one volt in the other circuit. Alternatively, as used in this problem, it can be defined based on flux linkage: one Henry is the mutual inductance when a change of 1 Ampere in one coil causes a change of 1 Weber of magnetic flux in the other coil.
1.5 H
Using the formula: \( M = \frac{\Delta \Phi}{\Delta I} \)
\( \Delta \Phi = 15 \, \text{Wb}, \quad \Delta I = 10 \, \text{A} \)
\( M = \frac{15}{10} = 1.5 \, \text{H} \)
1.5 H
1.5 H
Given:
Step 1: Formula for Mutual Inductance (M)
\[ M = \frac{\Delta \Phi}{\Delta I} \]
Step 2: Plug in the values
\[ M = \frac{15\ \text{Wb}}{10\ \text{A}} = 1.5\ \text{H} \]
Note: The time interval (0.25 s) is not needed for this calculation as we're given the total flux change, not the rate of change of flux.
The mutual inductance of the coils is \[ \boxed{1.5\ \text{H}} \].
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