All induction type transducers are based on
Faraday's law
Induction type transducers are a class of sensors that convert physical quantities like displacement, velocity, or vibration into an electrical signal. Their operation relies on the principle of electromagnetic induction, which is precisely described by Faraday's law. This law forms the core foundation for how these transducers generate an output signal in response to a change in the measured quantity.
Faraday's law of electromagnetic induction states that a change in magnetic flux passing through a coil induces an electromotive force (EMF) or voltage across the coil. This induced EMF is directly proportional to the rate of change of the magnetic flux. In simpler terms, if the amount of magnetic field lines (flux) passing through a coil changes, an electrical voltage will be produced in that coil.
Mathematically, Faraday's law can be expressed as:
$$ \text{EMF} = -N \frac{d\Phi}{dt} $$
Where:
In induction type transducers, the physical quantity being measured (e.g., displacement) is converted into a change in magnetic flux. This change in magnetic flux then induces a voltage in a coil, as per Faraday's law.
Let's briefly look at why the other options are not the fundamental basis for induction type transducers:
Therefore, the core principle governing all induction type transducers is indeed Faraday's law, which dictates how changes in magnetic fields generate electrical signals.
In the table shown, List I and List II, respectively, contain terms appearing on the left-hand side and the right-hand side of Maxwell’s equations (in their standard form). Match the left-hand side with the corresponding right-hand side.
List I | List II | ||
1. | ∇. D | P | 0 |
2. | ∇ × E | Q | \(\rho_v\) |
3. | ∇. B | R | \( - \frac{{\partial B}}{{\partial t}}\) |
4. | ∇ × H | S | \(J+ \frac{{\partial D}}{{\partial t}}\) |
“By the motion of the conductor or the coil in a magnetic field, i.e., the magnetic field is stationary and the moving conductors cut through it. The EMF generated in this way is normally called dynamically induced EMF.”
The given statement is specified by which of the following laws?
A flux of 0.25 mWb is produced by a coil of 1000 turns wound on a ring with a current of 2 A in it. Calculate the e.m.f induced in the coil when a current of 10 A is switched off, assuming the current will fall to zero in 1 millisecond.
Which of the following law states that “whenever the magnetic flux linked with a conductor or coil changes, an emf is induced in it?
The figure shows an arbitrarily shaped planar conducting loop A in the XY plane. Two nonintersecting regions with areas $a_1$ and $a_2$ within the loop are subjected to magnetic fields $\vec{B}_1 = \frac{m}{\sqrt{2}} \sin(\omega t) (1\hat{x} + 0\hat{y} + 1\hat{z})$, and
$\vec{B}_2 = -\frac{n}{\sqrt{2}} \cos(2\omega t + \pi/4) (0\hat{x} + 1\hat{y} + 1\hat{z})$, respectively.

What is the expression for the induced rms voltage in loop A?