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Inductors & Inductance Calculations |
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Inductors are passive devices used in electronic circuits to store energy in the form of a magnetic field. They are the compliment of capacitors, which store energy in the form of an electric field. An ideal inductor is the equivalent of a short circuit (0 ohms) for direct currents (DC), and presents an opposing force (reactance) to alternating currents (AC) that depends on the frequency of the current. The reactance (opposition to current flow) of an inductor is proportional to the frequency of the current flowing through it. Inductors are sometimes referred to as "coils" because most inductors are physically constructed of coiled sections of wire.
The property of inductance that opposes current flow is exploited for the purpose of preventing signals with a higher frequency component from passing while allowing signals of lower frequency components to pass. This is why inductors are sometimes referred to as "chokes," since they effectively choke off higher frequencies. A common application of a choke is in a radio amplifier biasing circuit where the collector of a transistor needs to be supplied with a DC voltage without allowing the RF (radio frequency) signal from conducting back into the DC supply.
  When used in series (left) or parallel (right) with its circuit compliment, a capacitor, the inductor-capacitor combination forms a circuit that resonates at a particular frequency that depends on the values of each component. In the series circuit, the impedance to current flow at the resonant frequency is zero with ideal components. In parallel circuits (right), the impedance to current flow is infinite with ideal components.
 Real-world inductors made of physical components exhibit more than just a pure inductance when present in an AC circuit. A common circuit simulator model is shown to the right. It includes the actual ideal inductor with a parallel resistive component that responds to alternating current. The DC resistive component is in series with the ideal inductor, and a capacitor is connected across the entire assembly and represents the capacitance present due to the proximity of the coil windings.
Equations (formulas) for combining inductors in series and parallel are given below. Additional equations are given for inductors of various configurations.
| Parallel Inductors | | Inductors in parallel combine in the same manner as parallel resistors. |
| Straight Wire | At high frequencies where skin effect
negates internal inductance
z = length, r = radius
Look up wire diameter here.
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| Coaxial Cable |  | D = outer radius
d = inner radius |  | z = length (ft) |  | z = length (m) |
| Closely Wound Toroid |  
(units in inches)
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Single-Layer Air-Core
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| Wheeler's
Formula
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(units in inches)
| Where: | d and z are in inches
N = number of turns | | Note: | If lead lengths are significant, use the straight wire calculation to add that inductance. |
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| Multilayer Air-Core Coil | Inductance[μHenry] =  ,
L = inductance (µH)
r = mean radius of coil (in)
z = physical length of coil winding (in)
N = number of turns
d = depth of coil (outer radius minus inner radius) (in) |
| | Inductive Reactance |
XL=jωL
| | Series Inductors | Inductors in series combine in the same manner as series resistors.
Ls = L1 + L2 + ··· + Ln  W = 1/2 Li 2  X L = 2 π f L L = inductance (H) v = voltage (V) W = energy (J) |
| "Q" Factor | - Q = F0/F3db
- Q = Estored / Eloss_per_cycle
- Parallel Circuit:
Q = R/(2*π*F0*L) - Series Circuit:
Q = (2*π*F0*L)/R - 1/Qload = 1/Qext + 1/Qtank
| | Where: | L = inductance
E = energy
ext = external
| | Finding the Equivalent "RQ" | Since the "Q" of an inductor is the ratio of the reactive component to the  resistive component, an equivalent circuit can be defined with a resistor in parallel with the inductor. This equation is valid only a a single frequency, "f," and must be calculated for each frequency of interest.
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Webmaster: Kirt Blattenberger, BSEE, UVM 1989 | |
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