The voltage induced in an inductor is represented as
Product of its inductance and rate of change of current through it
An inductor is a passive electrical component that stores energy in a magnetic field when electric current flows through it. The fundamental property of an inductor is its inductance, usually denoted by \(L\), which is a measure of its ability to oppose changes in the current flowing through it.
When the current passing through an inductor changes, a voltage is induced across the inductor. This phenomenon is a direct consequence of Faraday's Law of Induction and Lenz's Law. The magnitude of this induced voltage is directly proportional to the inductance of the inductor and the rate at which the current changes with respect to time.
The voltage induced in an inductor is mathematically represented by the following formula:
\(V_{L} = -L \frac{dI}{dt}\)
Let's break down each term in this formula:
Considering the magnitude of the induced voltage, it is the product of the inductance and the rate of change of current through it.
Let's analyze the given options in the context of the induced voltage:
Therefore, the voltage induced in an inductor is indeed the product of its inductance and the rate of change of current through it.
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