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.
Inductor Package Styles
The property of inductance that opposes a change in 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 drawing) or parallel (right drawing) 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 the parallel circuit (right), 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 left. 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. SPICE-type
simulators use this or an even more sophisticated model to facilitate more accurate calculations over a wide range of frequencies.
Related Pages on RF Cafe
- Inductors &
- Inductance Conversions
Standard Inductor Values
HamWaves.com website has a very sophisticated calculator for coil
inductance that allows you to en9ter the conductor diameter.
Equations (formulas) for combining inductors in series and parallel are given below. Additional equations are given for inductors of various
Total inductance of series-connected inductors is equal to the sum of the individual inductances. Keep units constant.
Closely Wound Toroid
Coaxial Cable Inductance
Straight Wire Inductance
These equations apply for when the length of the wire is much longer than the wire diameter
(look up wire diameter here). The ARRL Handbook presents the equation for
units of inches and µF:
For lower frequencies - up through about VHF, use this formula:
Above VHF, skin effect causes the ¾ in the top equation to approach unity (1), so use this equation:
Straight Wire Parallel to Ground Plane w/One End Grounded
The ARRL Handbook presents this equation for a straight wire suspended above a ground plane, with one end grounded to the plane:
a = wire radius, l = wire length
parallel to ground plane
h = height of wire above ground plane to bottom of wire
Parallel Line Inductance
Multi-Layer Air-Core Inductance
Total inductance of parallel-connected inductors is equal to the reciprocal of the sum of the reciprocals of the individual inductances.
Keep units constant.
Inductance Formula Constants and Variables
The following physical constants and mechanical dimensional variables apply to equations on this page. Units for equations are shown inside
brackets at the end of equations; e.g., means lengths are in inches and inductance is in Henries. If no units are indicated, then any may be used
so long as they are consistent across all entities; i.e., all meters, all µH, etc.
C = Capacitance
L = Inductance
N = Number of turns
W = Energy
εr = Relative permittivity (dimensionless)
ε0 = 8.85 x 10-12 F/m (permittivity of free space)
µr = Relative permeability (dimensionless)
µ0 = 4π x 10-7 H/m (permeability
of free space)
1 meter = 3.2808 feet <—> 1 foot = 0.3048 meters
1 mm = 0.03937 inches <—> 1 inch = 25.4
Also, dots (not to be confused with decimal points) are used to indicate multiplication in order to avoid ambiguity.
Inductive reactance (XL, in Ω) is proportional to the frequency (ω, in radians/sec, or f, in Hz) and inductance (L,
in Henries). Pure inductance has a phase angle of 90° (voltage leads current with a phase angle of 90°).
Energy Stored in an Inductor
Energy (W, in Joules) stored in an inductor is half the product of the inductance (L, in Henries) and the current (I, in amp) through the
Voltage Across an Inductor
The inductor's property of opposing a change in current flow causes a counter EMF (voltage) to form across its terminals opposite in polarity
to the applied voltage.
Quality Factor of Inductor
Quality factor is the dimensionless ratio of reactance to resistance in an inductor.
Single-Layer Round Coil Inductance
Wheeler's Formula for d >> a:
In general for a = wire radius:
Note: If lead lengths are significant, use the straight wire calculation to add that inductance.
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.