Component:  Inductor 
Image Upright:  1.15]] 
First Produced:  Michael Faraday (1831) 
An inductor, also called a coil, choke, or reactor, is a passive twoterminal electrical component that stores energy in a magnetic field when electric current flows through it.^{[1]} An inductor typically consists of an insulated wire wound into a coil.
When the current flowing through the coil changes, the timevarying magnetic field induces an electromotive force (e.m.f.) (voltage) in the conductor, described by Faraday's law of induction. According to Lenz's law, the induced voltage has a polarity (direction) which opposes the change in current that created it. As a result, inductors oppose any changes in current through them.
An inductor is characterized by its inductance, which is the ratio of the voltage to the rate of change of current. In the International System of Units (SI), the unit of inductance is the henry (H) named for 19th century American scientist Joseph Henry. In the measurement of magnetic circuits, it is equivalent to weber/ampere. Inductors have values that typically range from 1µH (10^{−6}H) to 20H. Many inductors have a magnetic core made of iron or ferrite inside the coil, which serves to increase the magnetic field and thus the inductance. Along with capacitors and resistors, inductors are one of the three passive linear circuit elements that make up electronic circuits. Inductors are widely used in alternating current (AC) electronic equipment, particularly in radio equipment. They are used to block AC while allowing DC to pass; inductors designed for this purpose are called chokes. They are also used in electronic filters to separate signals of different frequencies, and in combination with capacitors to make tuned circuits, used to tune radio and TV receivers.
\Phi_{B}
I
L
L:=
\Phi_{B}  
I 
The inductance of a circuit depends on the geometry of the current path as well as the magnetic permeability of nearby materials. An inductor is a component consisting of a wire or other conductor shaped to increase the magnetic flux through the circuit, usually in the shape of a coil or helix, with two terminals. Winding the wire into a coil increases the number of times the magnetic flux lines link the circuit, increasing the field and thus the inductance. The more turns, the higher the inductance. The inductance also depends on the shape of the coil, separation of the turns, and many other factors. By adding a "magnetic core" made of a ferromagnetic material like iron inside the coil, the magnetizing field from the coil will induce magnetization in the material, increasing the magnetic flux. The high permeability of a ferromagnetic core can increase the inductance of a coil by a factor of several thousand over what it would be without it.
Any change in the current through an inductor creates a changing flux, inducing a voltage across the inductor. By Faraday's law of induction, the voltage induced by any change in magnetic flux through the circuit is given by
l{E}=
d\Phi_{B}  
dt 
.
Reformulating the definition of above, we obtain
\Phi_{B}=LI.
l{E}=
d\Phi_{B}  
dt 
=
d  
dt 
(LI)=L
dI  
dt 
.
for independent of time, current and magnetic flux linkage.
So inductance is also a measure of the amount of electromotive force (voltage) generated for a given rate of change of current. For example, an inductor with an inductance of 1 henry produces an EMF of 1 volt when the current through the inductor changes at the rate of 1 ampere per second. This is usually taken to be the constitutive relation (defining equation) of the inductor.
The dual of the inductor is the capacitor, which stores energy in an electric field rather than a magnetic field. Its current–voltage relation is obtained by exchanging current and voltage in the inductor equations and replacing L with the capacitance C.
In a circuit, an inductor can behave differently at different time instant. However, it's usually easy to think about the shorttime limit and longtime limit:
See main article: Lenz's Law. The polarity (direction) of the induced voltage is given by Lenz's law, which states that the induced voltage will be such as to oppose the change in current.^{[6]} For example, if the current through an inductor is increasing, the induced voltage will be positive at the current's entrance point and negative at the exit point, tending to oppose the additional current.^{[7]} ^{[8]} ^{[9]} The energy from the external circuit necessary to overcome this potential "hill" is being stored in the magnetic field of the inductor. If the current is decreasing, the induced voltage will be negative at the current's entrance point and positive at the exit point, tending to maintain the current. In this case energy from the magnetic field is being returned to the circuit.
One intuitive explanation as to why a potential difference is induced on a change of current in an inductor goes as follows:
When there is a change in current through an inductor there is a change in the strength of the magnetic field. For example, if the current is increased, the magnetic field increases. This, however, does not come without a price. The magnetic field contains potential energy, and increasing the field strength requires more energy to be stored in the field. This energy comes from the electric current through the inductor. The increase in the magnetic potential energy of the field is provided by a corresponding drop in the electric potential energy of the charges flowing through the windings. This appears as a voltage drop across the windings as long as the current increases. Once the current is no longer increased and is held constant, the energy in the magnetic field is constant and no additional energy must be supplied, so the voltage drop across the windings disappears.
Similarly, if the current through the inductor decreases, the magnetic field strength decreases, and the energy in the magnetic field decreases. This energy is returned to the circuit in the form of an increase in the electrical potential energy of the moving charges, causing a voltage rise across the windings.
The work done per unit charge on the charges passing the inductor is
l{E}
I
W
dW  
dt 
=l{E}I
l{E}=L
dI  
dt 
dW  
dt 
=L
dI  
dt 
⋅ I=LI ⋅
dI  
dt 
dW=LI ⋅ dI
In a ferromagnetic core inductor, when the magnetic field approaches the level at which the core saturates, the inductance will begin to change, it will be a function of the current
L(I)
W
I_{0}
This is given by:
W=
I_{0}  
\int  
0 
L_{d(I)}IdI
L_{d(I)}
L_{d}=
d\Phi_{B}  
dI 
\begin{align} W&=
I_{0}  
L\int  
0 
IdI\\ W&=
1  
2 
L
2 \end{align}  
{I  
0} 
For inductors with magnetic cores, the above equation is only valid for linear regions of the magnetic flux, at currents below the saturation level of the inductor, where the inductance is approximately constant. Where this is not the case, the integral form must be used with
L_{d}
The constitutive equation describes the behavior of an ideal inductor with inductance
L
A real inductor's capacitive reactance rises with frequency, and at a certain frequency, the inductor will behave as a resonant circuit. Above this selfresonant frequency, the capacitive reactance is the dominant part of the inductor's impedance. At higher frequencies, resistive losses in the windings increase due to the skin effect and proximity effect.
Inductors with ferromagnetic cores experience additional energy losses due to hysteresis and eddy currents in the core, which increase with frequency. At high currents, magnetic core inductors also show sudden departure from ideal behavior due to nonlinearity caused by magnetic saturation of the core.
Inductors radiate electromagnetic energy into surrounding space and may absorb electromagnetic emissions from other circuits, resulting in potential electromagnetic interference.
An early solidstate electrical switching and amplifying device called a saturable reactor exploits saturation of the core as a means of stopping the inductive transfer of current via the core.
The winding resistance appears as a resistance in series with the inductor; it is referred to as DCR (DC resistance). This resistance dissipates some of the reactive energy. The quality factor (or Q) of an inductor is the ratio of its inductive reactance to its resistance at a given frequency, and is a measure of its efficiency. The higher the Q factor of the inductor, the closer it approaches the behavior of an ideal inductor. High Q inductors are used with capacitors to make resonant circuits in radio transmitters and receivers. The higher the Q is, the narrower the bandwidth of the resonant circuit.
The Q factor of an inductor is defined as, where L is the inductance, R is the DCR, and the product ωL is the inductive reactance:
Q=
\omegaL  
R 
Q increases linearly with frequency if L and R are constant. Although they are constant at low frequencies, the parameters vary with frequency. For example, skin effect, proximity effect, and core losses increase R with frequency; winding capacitance and variations in permeability with frequency affect L.
At low frequencies and within limits, increasing the number of turns N improves Q because L varies as N^{2} while R varies linearly with N. Similarly increasing the radius r of an inductor improves (or increases) Q because L varies with r^{2} while R varies linearly with r. So high Q air core inductors often have large diameters and many turns. Both of those examples assume the diameter of the wire stays the same, so both examples use proportionally more wire. If the total mass of wire is held constant, then there would be no advantage to increasing the number of turns or the radius of the turns because the wire would have to be proportionally thinner.
Using a high permeability ferromagnetic core can greatly increase the inductance for the same amount of copper, so the core can also increase the Q. Cores however also introduce losses that increase with frequency. The core material is chosen for best results for the frequency band. High Q inductors must avoid saturation; one way is by using a (physically larger) air core inductor. At VHF or higher frequencies an air core is likely to be used. A well designed air core inductor may have a Q of several hundred.
Inductors are used extensively in analog circuits and signal processing. Applications range from the use of large inductors in power supplies, which in conjunction with filter capacitors remove ripple which is a multiple of the mains frequency (or the switching frequency for switchedmode power supplies) from the direct current output, to the small inductance of the ferrite bead or torus installed around a cable to prevent radio frequency interference from being transmitted down the wire. Inductors are used as the energy storage device in many switchedmode power supplies to produce DC current. The inductor supplies energy to the circuit to keep current flowing during the "off" switching periods and enables topographies where the output voltage is higher than the input voltage.
A tuned circuit, consisting of an inductor connected to a capacitor, acts as a resonator for oscillating current. Tuned circuits are widely used in radio frequency equipment such as radio transmitters and receivers, as narrow bandpass filters to select a single frequency from a composite signal, and in electronic oscillators to generate sinusoidal signals.
Two (or more) inductors in proximity that have coupled magnetic flux (mutual inductance) form a transformer, which is a fundamental component of every electric utility power grid. The efficiency of a transformer may decrease as the frequency increases due to eddy currents in the core material and skin effect on the windings. The size of the core can be decreased at higher frequencies. For this reason, aircraft use 400 hertz alternating current rather than the usual 50 or 60 hertz, allowing a great saving in weight from the use of smaller transformers.^{[12]} Transformers enable switchedmode power supplies that isolate the output from the input.
Inductors are also employed in electrical transmission systems, where they are used to limit switching currents and fault currents. In this field, they are more commonly referred to as reactors.
Inductors have parasitic effects which cause them to depart from ideal behavior. They create and suffer from electromagnetic interference (EMI). Their physical size prevents them from being integrated on semiconductor chips. So the use of inductors is declining in modern electronic devices, particularly compact portable devices. Real inductors are increasingly being replaced by active circuits such as the gyrator which can synthesize inductance using capacitors.
An inductor usually consists of a coil of conducting material, typically insulated copper wire, wrapped around a core either of plastic (to create an aircore inductor) or of a ferromagnetic (or ferrimagnetic) material; the latter is called an "iron core" inductor. The high permeability of the ferromagnetic core increases the magnetic field and confines it closely to the inductor, thereby increasing the inductance. Low frequency inductors are constructed like transformers, with cores of electrical steel laminated to prevent eddy currents. 'Soft' ferrites are widely used for cores above audio frequencies, since they do not cause the large energy losses at high frequencies that ordinary iron alloys do. Inductors come in many shapes. Some inductors have an adjustable core, which enables changing of the inductance. Inductors used to block very high frequencies are sometimes made by stringing a ferrite bead on a wire.
Small inductors can be etched directly onto a printed circuit board by laying out the trace in a spiral pattern. Some such planar inductors use a planar core. Small value inductors can also be built on integrated circuits using the same processes that are used to make interconnects. Aluminium interconnect is typically used, laid out in a spiral coil pattern. However, the small dimensions limit the inductance, and it is far more common to use a circuit called a gyrator that uses a capacitor and active components to behave similarly to an inductor. Regardless of the design, because of the low inductances and low power dissipation ondie inductors allow, they are currently only commercially used for high frequency RF circuits.
Inductors used in power regulation systems, lighting, and other systems that require lownoise operating conditions, are often partially or fully shielded.^{[13]} ^{[14]} In telecommunication circuits employing induction coils and repeating transformers shielding of inductors in close proximity reduces circuit crosstalk.
The term air core coil describes an inductor that does not use a magnetic core made of a ferromagnetic material. The term refers to coils wound on plastic, ceramic, or other nonmagnetic forms, as well as those that have only air inside the windings. Air core coils have lower inductance than ferromagnetic core coils, but are often used at high frequencies because they are free from energy losses called core losses that occur in ferromagnetic cores, which increase with frequency. A side effect that can occur in air core coils in which the winding is not rigidly supported on a form is 'microphony': mechanical vibration of the windings can cause variations in the inductance.
At high frequencies, particularly radio frequencies (RF), inductors have higher resistance and other losses. In addition to causing power loss, in resonant circuits this can reduce the Q factor of the circuit, broadening the bandwidth. In RF inductors, which are mostly air core types, specialized construction techniques are used to minimize these losses. The losses are due to these effects:
To reduce parasitic capacitance and proximity effect, high Q RF coils are constructed to avoid having many turns lying close together, parallel to one another. The windings of RF coils are often limited to a single layer, and the turns are spaced apart. To reduce resistance due to skin effect, in highpower inductors such as those used in transmitters the windings are sometimes made of a metal strip or tubing which has a larger surface area, and the surface is silverplated.
See also: Magnetic core.
Ferromagneticcore or ironcore inductors use a magnetic core made of a ferromagnetic or ferrimagnetic material such as iron or ferrite to increase the inductance. A magnetic core can increase the inductance of a coil by a factor of several thousand, by increasing the magnetic field due to its higher magnetic permeability. However the magnetic properties of the core material cause several side effects which alter the behavior of the inductor and require special construction:
Lowfrequency inductors are often made with laminated cores to prevent eddy currents, using construction similar to transformers. The core is made of stacks of thin steel sheets or laminations oriented parallel to the field, with an insulating coating on the surface. The insulation prevents eddy currents between the sheets, so any remaining currents must be within the cross sectional area of the individual laminations, reducing the area of the loop and thus reducing the energy losses greatly. The laminations are made of lowconductivity silicon steel to further reduce eddy current losses.
See main article: Ferrite core. For higher frequencies, inductors are made with cores of ferrite. Ferrite is a ceramic ferrimagnetic material that is nonconductive, so eddy currents cannot flow within it. The formulation of ferrite is xxFe_{2}O_{4} where xx represents various metals. For inductor cores soft ferrites are used, which have low coercivity and thus low hysteresis losses.
See also: Carbonyl iron. Another material is powdered iron cemented with a binder.
See main article: Toroidal inductors and transformers.
In an inductor wound on a straight rodshaped core, the magnetic field lines emerging from one end of the core must pass through the air to reenter the core at the other end. This reduces the field, because much of the magnetic field path is in air rather than the higher permeability core material and is a source of electromagnetic interference. A higher magnetic field and inductance can be achieved by forming the core in a closed magnetic circuit. The magnetic field lines form closed loops within the core without leaving the core material. The shape often used is a toroidal or doughnutshaped ferrite core. Because of their symmetry, toroidal cores allow a minimum of the magnetic flux to escape outside the core (called leakage flux), so they radiate less electromagnetic interference than other shapes. Toroidal core coils are manufactured of various materials, primarily ferrite, powdered iron and laminated cores.^{[15]}
Probably the most common type of variable inductor today is one with a moveable ferrite magnetic core, which can be slid or screwed in or out of the coil. Moving the core farther into the coil increases the permeability, increasing the magnetic field and the inductance. Many inductors used in radio applications (usually less than 100 MHz) use adjustable cores in order to tune such inductors to their desired value, since manufacturing processes have certain tolerances (inaccuracy). Sometimes such cores for frequencies above 100 MHz are made from highly conductive nonmagnetic material such as aluminum.^{[16]} They decrease the inductance because the magnetic field must bypass them.
Air core inductors can use sliding contacts or multiple taps to increase or decrease the number of turns included in the circuit, to change the inductance. A type much used in the past but mostly obsolete today has a spring contact that can slide along the bare surface of the windings. The disadvantage of this type is that the contact usually shortcircuits one or more turns. These turns act like a singleturn shortcircuited transformer secondary winding; the large currents induced in them cause power losses.
A type of continuously variable air core inductor is the variometer. This consists of two coils with the same number of turns connected in series, one inside the other. The inner coil is mounted on a shaft so its axis can be turned with respect to the outer coil. When the two coils' axes are collinear, with the magnetic fields pointing in the same direction, the fields add and the inductance is maximum. When the inner coil is turned so its axis is at an angle with the outer, the mutual inductance between them is smaller so the total inductance is less. When the inner coil is turned 180° so the coils are collinear with their magnetic fields opposing, the two fields cancel each other and the inductance is very small. This type has the advantage that it is continuously variable over a wide range. It is used in antenna tuners and matching circuits to match low frequency transmitters to their antennas.
Another method to control the inductance without any moving parts requires an additional DC current bias winding which controls the permeability of an easily saturable core material. See Magnetic amplifier.
A choke is an inductor designed specifically for blocking highfrequency alternating current (AC) in an electrical circuit, while allowing DC or lowfrequency signals to pass. Because the inductor resistricts or "chokes" the changes in current, this type of inductor is called a choke. It usually consists of a coil of insulated wire wound on a magnetic core, although some consist of a donutshaped "bead" of ferrite material strung on a wire. Like other inductors, chokes resist changes in current passing through them increasingly with frequency. The difference between chokes and other inductors is that chokes do not require the high Q factor construction techniques that are used to reduce the resistance in inductors used in tuned circuits.
The effect of an inductor in a circuit is to oppose changes in current through it by developing a voltage across it proportional to the rate of change of the current. An ideal inductor would offer no resistance to a constant direct current; however, only superconducting inductors have truly zero electrical resistance.
The relationship between the timevarying voltage v(t) across an inductor with inductance L and the timevarying current i(t) passing through it is described by the differential equation:
v(t)=L
di(t)  
dt 
\begin{align} i(t)&=I_{P\sin(\omega}t)\\
di(t)  
dt 
&=I_{P\omega}\cos(\omegat)\\ v(t)&=LI_{P\omega}\cos(\omegat) \end{align}
In this situation, the phase of the current lags that of the voltage by π/2 (90°). For sinusoids, as the voltage across the inductor goes to its maximum value, the current goes to zero, and as the voltage across the inductor goes to zero, the current through it goes to its maximum value.
If an inductor is connected to a direct current source with value I via a resistance R (at least the DCR of the inductor), and then the current source is shortcircuited, the differential relationship above shows that the current through the inductor will discharge with an exponential decay:
i(t)=I
 
e 
The ratio of the peak voltage to the peak current in an inductor energised from an AC source is called the reactance and is denoted X_{L}.
X_{L=}
V_{P}  
I_{P} 
=
\omegaLI_{P}  
I_{P} 
Thus,
X_{L=}\omegaL
where ω is the angular frequency.
Reactance is measured in ohms but referred to as impedance rather than resistance; energy is stored in the magnetic field as current rises and discharged as current falls. Inductive reactance is proportional to frequency. At low frequency the reactance falls; at DC, the inductor behaves as a short circuit. As frequency increases the reactance increases and at a sufficiently high frequency the reactance approaches that of an open circuit.
In filtering applications, with respect to a particular load impedance, an inductor has a corner frequency defined as:
f_{3dB}=
R  
2\piL 
When using the Laplace transform in circuit analysis, the impedance of an ideal inductor with no initial current is represented in the s domain by:
Z(s)=Ls
where
L
s
If the inductor does have initial current, it can be represented by:
See main article: Series and parallel circuits. Inductors in a parallel configuration each have the same potential difference (voltage). To find their total equivalent inductance (L_{eq}):
1  
L_{eq} 
=
1  
L_{1} 
+
1  
L_{2} 
+ … +
1  
L_{n} 
The current through inductors in series stays the same, but the voltage across each inductor can be different. The sum of the potential differences (voltage) is equal to the total voltage. To find their total inductance:
L_{eq}=L_{1}+L_{2}+ … +L_{n}
These simple relationships hold true only when there is no mutual coupling of magnetic fields between individual inductors.
Mutual inductance occurs when the magnetic field of an inductor induces a magnetic field in an adjacent inductor. Mutual induction is the basis of transformer construction.
M=\sqrt{L_{1L}_{2}}
M\leq\sqrt{L_{1L}_{2}}
M=K\sqrt{L_{1L}_{2}}
The table below lists some common simplified formulas for calculating the approximate inductance of several inductor constructions.
Construction ! Formula  Notes   ! Cylindrical aircore coil^{[17]}  L=\mu_{0}KN^{2}
\pi
 K ≈ 1   ! rowspan="2"  Straight wire conductor^{[20]}  L=
\ell\left(A  B +C\right) where: \begin{align} A&=ln\left(
+\sqrt{\left(
\right)^{2}+1}\right)\\ B&=
\pi
\tfrac{\mu_{0}{2\pi}}  Exact if ω = 0, or if ω = ∞. The term B subtracts rather than adds.    L=
\ell\left[ln\left(
\right)1\right] L=
\ell\left[ln\left(
\right)
\right]
\tfrac{\mu_{0}{2\pi}}  Requires ℓ > 100 d^{[23]} For relative permeability μ_{r} = 1 (e.g., Cu or Al).   ! Small loop or very short coil^{[24]}  L ≈
N^{2}\piD\left[ln\left(
\right)+\left(ln82\right)\right] +\sqrt{
\ell_{c} ≈ N\piD
\tfrac{\mu_{0}{2\pi}}  Conductor μ_{r} should be as close to 1 as possible  copper or aluminum rather than a magnetic or paramagnetic metal.   ! Medium or long aircore cylindrical coil^{[26]} ^{[27]}  L=
 Requires cylinder length ℓ > 0.4 r: Length must be at least of the diameter. Not applicable to singleloop antennas or very short, stubby coils.   ! Multilayer aircore coil^{[28]}  L=
⋅
  ! rowspan="2"  Flat spiral aircore coil^{[29]} ^{[30]} ^{[31]}  L=
   L=
 Accurate to within 5 percent for d > 0.2 r.   ! rowspan="2"  Toroidal core (circular crosssection)  L=0.01595N^{2}\left(D\sqrt{D^{2}d^{2}\right)}
   L ≈ 0.007975{d^{2}N^{2}\overD}
 Approximation when d < 0.1 D   ! Toroidal core (rectangular crosssection)  L=0.00508N^{2}hln\left({


\piD