An inductor
is a passive element designed to store energy in its magnetic field. They find
numerous applications in electronics and power systems. For example, they are
used in transformers, radios, TVs, radars and electric motors.
![](https://blogger.googleusercontent.com/img/b/R29vZ2xl/AVvXsEgVCLhnu1MjKHj6oEUMHGJ4Yy8Ht4NY6wPQPMa9UVF0UD_AqMO_YoRtkH_AfogzCl7Fdb-FTJzqVYLdQ1WppMtH-c-PIOJdWCY_3PWtJINPNsdYaBX5Wo2eaUWmDtF3OB05SBPRRXN7L1o/s320/inductors.png)
It was in
the early 1800s, that English experimentalist Michael Faraday and American
inventor Joseph Henry discovered almost simultaneously that a changing magnetic
field could produce a voltage in a neighboring circuit. They showed that this
voltage was proportional to the time rate of change of current which produced
the magnetic field. That constant of proportionality is called inductance and
is denoted by L.
\[v=L\frac{di}{dt}\]
The unit of
inductance is Henry (H).
Now, what is Inductance?
Inductance
is the property of the coil by virtue of which it opposes any change in the
current flowing through it.
The
inductance of an inductor depends on its physical dimensions and construction.
Inductance of a solenoid (inductor) is given by
\[L=\frac{\mu
{{N}^{2}}A}{l}\]
Where, N =
number of turns
l = length
A = cross-sectional area
$\mu
$= permeability of the core
Inductance
can be increased by increasing N,$\mu
$, and A or by reducing l.
TYPES OF INDUCTORS-
Inductors
are available in different types ranging from large high current iron- cored
chokes to tiny low current coils.
Air-cored
coils are wound on a tubular insulating material such as cardboard, fiber, hard
rubber, Bakelite etc. Such coils find use in electronic circuits working at
high frequencies. Their inductance values are in millihenry (mH) and microhenry
($\mu
$H) range.
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Solenoidal wound inductor |
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Toroidal inductor |
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Chip inductor |
Iron-cored
chokes may have laminated iron core or powdered iron cores. They are mainly
used at AC power frequency (50Hz) and at audio frequencies (20Hz to about 10
kHz). Such chokes have inductance of a few henry's.
HOW TO MAKE AN INDUCTOR VARIABLE?
An inductor
can be made variable, by having tapped coils (taps are brought out at several
points in the winding), by having a slider (similar to a rheostat), or by
having a movable core. Standard symbols of different types of inductor are
shown in the figure given below.
ENERGY STORED IN AN INDUCTOR-
We know
induced voltage v, in an inductor is given by
\[v=L\frac{di}{dt}\]
\[\Rightarrow
di=\frac{1}{L}vdt\]
Integrating
gives, \[i=\frac{1}{L}\int\limits_{-\infty
}^{t}{v(t)dt}\]
or\[i=\frac{1}{L}\int\limits_{{{t}_{o}}}^{t}{v(t)dt+i({{t}_{0}})}\]
Where i(t0)
is the total current for -$\infty
$<t<t0 and i(-$\infty
$)=0. This argument is reasonable because there must be time
in the past when there was no current in the inductor.
Power
delivered to inductor is p = vi = $\left( L\frac{di}{dt} \right)i$
Energy
stored is $w=\int\limits_{-\infty }^{t}{pdt}=\int\limits_{-\infty }^{t}{\left(
L\frac{di}{dt} \right)idt}$
\[=L\int\limits_{-\infty
}^{t}{idt}=\frac{1}{2}L{{i}^{2}}(t)-\frac{1}{2}L{{i}^{2}}(-\infty )\]
Since, i($-\infty
$)=0,
\[w=\frac{1}{2}L{{i}^{2}}\]
PROPERTIES OF AN INDUCTOR-
Following
are the important properties of an inductor –
- Voltage across an inductor is zero when the current is constant which can be inferred from the equation, $v=L\frac{di}{dt}$ . Thus, inductor acts like a short circuit to DC.
- The current through an inductor
cannot change instantaneously. Thus, an inductor opposes abrupt change in
current through it.
Current through an inductor (i) allowed, (ii) not allowed; an abrupt change is not possible. - An ideal inductor does not dissipate energy. The energy stored in it can be retrieved at a later time. It takes power from the circuit when storing energy and delivers power to the circuit when returning previously stored energy.
- A practical, non-ideal inductor has a
significant resistive component as shown in the figure given below.
Circuit model of a practical inductor
The presence of Rw, makes it both an energy storage device and
an energy dissipation device.
Since Rw is small, it is ignored in most cases. The non-ideal
inductor also has a winding capacitance Cw due to the capacitive
coupling between the conducting coils. Cw is small and can be
ignored in most cases, except at high frequencies.