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Energy stored in an inductor is considered one the most difficult concept.
11 Questions around this concept.
What is the time at which the rate of dissipation of energy (Joule's heat) across the resistance is equal to the rate at which magnetic energy is stored in the inductor?
Rate of increment of energy in an inductor with time in series LR circuit getting charged with a battery of e.m.f. E is best represented by: [ inductor has initially zero current ]
A 0.1 m long conductor carrying a current 50 A is held perpendicular to a magnetic field 1.25 mT . The mechanical power required to move the conductor with a speed of $1 \mathrm{~ms}^{-1}$ is:
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A current of 1 A through a coil of inductance of 200 mH is increasing at a rate of $0.5 \mathrm{~A} \mathrm{~s}^{-1}$. The energy stored in the inductor per second is:
Shown in the figure is a parallel R, L, and C circuit with keys K1 closed and K2 opened. When K1 is opened and K2 is closed simultaneously, The maximum charge stored in it is:
In the shown network the energy stored in the inductor in a steady state will be
The energy stored in a conductor is U. What will be the value of the energy stored if the value of the current is halved by the previous value-
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Energy stored in an inductor (U)-
In building a steady current in the circuit, the source emf has to do work against of self-inductance of the coil and whatever energy
consumed for this work stored in the magnetic field of coil this energy called as magnetic potential energy (U) of the coil.
When an electric current i is flowing in an inductor, there is energy stored in the magnetic field. Considering a pure inductor L, the instantaneous power which must be supplied to initiate the current in the inductor is
$
P=i v=L i \frac{d i}{d t}
$
The work done by the voltage source during a time interval $d t$ is
$
d W=P d t=i L \frac{d i}{d t} d t=\text { Lidi }
$
total work $W$ done in establishing the final current $I$ in the inductor
$
\mathrm{W}=\int_0^t P d t=\int_0^I L i d i=\frac{1}{2} L I^2
$
So Energy stored in the magnetic field of the inductor is given as
$
U=\frac{1}{2} L I^2
$
The energy density (u)/Energy per unit volumeusing $U=\frac{1}{2} L I^2$
for the solenoid field, we can write
\begin{aligned}
& U=\frac{1}{2}(L i) i=\frac{N \phi i}{2} \\
& u=\frac{U}{V}=\frac{B^2}{2 \mu_0}
\end{aligned}
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