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The Sigma Insight: Self and Mutual Inductance
The Essence of Mutual Inductance
When we place two coils close to each other, a fascinating electromagnetic interaction occurs. If we pass a time-varying current through the first coil (the primary), it generates a changing magnetic field. This magnetic field permeates the surrounding space, and a portion of its magnetic field lines inevitably passes through the second coil (the secondary).
This linkage of magnetic flux forms the basis of mutual inductance. Mathematically, the magnetic flux linked with the secondary coil is directly proportional to the current flowing through the primary coil. The constant of proportionality is what we call the mutual inductance, denoted by .
Decoding the Formula
To truly understand what mutual inductance depends on, we need to look beyond the basic definition and examine a concrete physical setup. Let's consider the classic example of two long coaxial solenoids. The mutual inductance for this system is given by the formula:
Let's break down the terms in this elegant equation:
is the permeability of free space, representing the medium inside the coils.
and are the number of turns per unit length of the inner and outer coils, respectively.
is the cross-sectional area of the inner coil.
is the length of the overlapping region of the coils.
The Geometric Truth
Notice what is conspicuously absent from this formula. Do you see any term for the current ? Do you see any term for the rate of change of current ? Do you see any mention of the electrical resistance or the material of the wire?
Absolutely not.
Just like the capacitance of a capacitor depends only on the plate area and separation, and the resistance of a wire depends on its length and cross-section, inductance is a purely geometric property. It is determined entirely by the physical dimensions of the coils (area and length), the number of turns, and crucially, their relative position and orientation.
If you were to take the secondary coil and rotate it by 90 degrees so that it is perpendicular to the primary coil, the magnetic field lines would graze past it without passing through its area. The flux linkage would drop to zero, and consequently, the mutual inductance would become zero.
Therefore, the mutual inductance of a pair of coils is fundamentally dictated by their relative position and orientation in space.
Similar Questions
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(D)
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Consider a circuit consisting of a capacitor of capacitance and a coil with turns per unit length, cross sectional area and length , where . There is another coil of length , cross sectional area and turns per unit length completely inside the larger coil, as shown in the figure. The ends of this smaller coil are connected with each other by an insulated conducting wire. The self-inductance of the larger coil is . Neglecting edge effects and all the Ohmic resistances, the resonant frequency of the circuit is:
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A circular wire loop of radius is placed in the - plane centred at the origin . A square loop of side () having two turns is placed with its centre at along the axis of the circular wire loop, as shown in figure. The plane of the square loop makes an angle of with respect to the Z-axis. If the mutual inductance between the loops is given by , then the value of is
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The self-induced emf of a coil is 25 V. When the current in it is changed at uniform rate from 10 A to 25 A in 1s, the change in the energy of the inductance is
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When the current changes from to in , an emf of is induced in a coil. The coefficient of self-induction of the coil is
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