What is Inductance: understanding the basics
Inductance is one of the main basic parameters associated with any electrical or electronic circuit and inductors themsleves are used to provide specific levels of inductance within a circuit.
Inductance and Transformer Tutorial Includes:
Inductance
Symbols
Lenz's law
Self inductance
Inductive reactance calculations
Inductive reactance theory
Inductance of wire & coils
Mutual inductance
Transformers
Inductance is a fundamental parameter in electrical and electronic circuit designs. Like resistance and capacitance it is a basic electrical parameter that affects all circuits to some degree.
Inductance is used in many areas of electrical and electronic systems and circuits. The electronic components can be in a variety of forms and may be called by a variety of names: coils, inductors, chokes, transformers, . . . Each of these may also have a variety of different variants: with and without cores and the core materials may be of different types.
Understanding inductance and the different forms and formats for inductors and transformers is key to providing an understanding of what is happening within the electrical and electronic circuits.
The term inductance was coined by Oliver Heaviside in 1886. It is customary to use the symbol L for inductors shown on circuit diagrams and inductance in equations after the physicist Heinrich Lenz.
Since then the term inductor has remained in use as the primary term for describing this form of electrical parameter. Also many electronic components that have inductance as their primary parameter bear the name that was coined by Appleton.
Inductance basics
Inductance is the ability of an inductor to store energy and it does this in the magnetic field that is created by the flow of electrical current.
Energy is required to set up the magnetic field and this energy is released when the field falls.
As a result of the magnetic field associated with the current flow, inductors generate an opposing voltage proportional to the rate of change in current in a circuit.
Inductance is caused by the magnetic field generated by electric currents flowing within an electrical circuit. Typically coils of wire are used as a coil increases the coupling of the magnetic field and increases the effect.
There are two ways in which inductance is used:
Self-inductance: Self-inductance is the property of a circuit, often a coil, whereby a change in current causes a change in voltage in that circuit due to the magnetic effect of caused by the current flow. It can be seen that self-inductance applies to a single circuit - in other words it is an inductance, typically within a single coil. This effect is used in single coils or chokes.
Read more about . . . . self inductance.
- Mutual-inductance: Mutual inductance is an inductive effect where a change in current in one circuit causes a change in voltage across a second circuit as a result of a magnetic field that links both circuits. This effect is used in transformers.
Inductance unit definition
When indicating an inductor on a circuit diagram or within an equation, generally the symbol "L" is used. On circuit diagrams, inductors are generally numbered, L1, L2, etc.
The SI unit of inductance is the henry, H which can be defined in terms of rate of change of current and voltage.
Definition of the henry:
The inductance of a circuit is one henry if the rate of change of current in a circuit is one ampere per second and this results in an electromotive force of one volt.
One henry is equal to 1 Wb/A.
Inductance - what happens
When a current flows within a conductor, whether it be straight or in the form of a coil, a magnetic field builds up around it and this affects the way in which the current builds up after the circuit is made.
In terms of how inductance affects and electrical circuit, it helps to look at the way the circuit operates, first for a direct current, and then for an alternating current. Although they follow the same laws and the same effects result, it helps the explanation, the direct current example is simpler, and then this explanation can be used as the basis for the alternating current case.
• Direct current:
As the circuit is made the current starts to flow. As the current increases to its steady value the magnetic field it produces builds up to its final shape. As this occurs, the magnetic field is changing, so this induces a voltage back into the coil itself, as would be expected according to Lenz's Law.
The time constant T in seconds of the circuit which will include the inductor value L Henries and the associated circuit resistance, R Ohms can be calculated as L/R. T is the time for the current I amps to rise to 0.63 of its final steady state value of V/R. The energy stored in the magnetic field is 1/2 L I2.
When the current is switched off this means that effectively the resistance of the circuit rises suddenly to infinity. This means that the ratio L / R becomes very small and the magnetic field falls very rapidly. This represents a large change in magnetic field and accordingly the inductance tries to keep the current flowing and a back EMF is set up to oppose this arising from the energy stored in the magnetic field.
When the back EMF is set up, the very high voltages generated mean that sparks can appear across the switch contact, especially just as the contact is broken. This leads to pitted contacts and wear on any mechanical switches. In electronic circuits this back EMF can destroy semiconductor devices and therefore ways of reducing this back EMF are often employed.
• Alternating current:
For the case of the alternating current passing through an inductor, the same basic principles are used, but as the waveform is repetitive, we tend to look at the way the inductor responds in a slightly different way as it is more convenient.
By its very nature, an alternating waveform is changing all of the time. This means that the resulting magnetic field will always be changing, and there will always be an induced back EMF produced. The result of this is that the inductor impedes the flow of the alternating current through it as a result of the inductance. This is in addition to the resistance caused but he Ohmic resistance of the wire.
It means that if the Ohmic resistance of the inductor is low, it will pass direct current, DC with little loss, but it can present a high impedance to any high frequency signal. This characteristic of an inductor can be used in ensuring that any high frequency signals do not pass though the inductor.
A further aspect of inductance is that the reactance of an inductor and that of a capacitor can act together in a circuit to cancel each other out. This is known as resonance, and it is widely used in bandpass filters.
Inductance of wires and coils
Straight wires and coils have an inductance. Normally coils are used for inductors because the linking of the magnetic field between the different turns of the coil increases the inductance and enables the wire to be contained within a smaller volume.
If the wire was not coiled, then very long lengths of wire would often be needed making electronic components of this nature not viable. By coiling the wire the inductance is maximised enabling inductors to be incorporated into many electronic circuits.
However, even the inductance of a straight wire can affect some electronic circuits. For most low frequency applications, the inductance of a straight wire can be ignored, but as the frequency increases into the VHF region and beyond, the inductance of the wire itself can become significant, and interconnections need to be kept short to minimise the effects.
Calculations are available to enable the inductance of wires to be calculated quite accurately, but the inductance of coils is a little more complicated and depends upon a variety of factors including the shape of the coil and the constant of the material in and around the coil.
Inductors
There is a wide variety of inductors used to provide inductance within an electronic circuit design. These electronic components can take many forms: some may be large, others small, and they may have many formats.
These components may be used in a whole variety of electronic circuit designs, but two of the main applications are within RF circuit design where inductors are an important form of electronic component.
They are also widely used within filters for items such as EMC where electronic signals generated within an electronic items needs to be prevented from causing interference to other items of equipment. For example a simple form of inductor is often seen on computer cables where a ferrite is added around a cable to add inductance and prevent the signals from travelling along the cable and being transmitted, thereby giving rise to the possibility of interference to other systems.
Note on Inductors:
Inductors are electronic components that use inductance in an electronic circuit. These inductors are normally wound components having many turns of wire to increase the level of inductance. They may also be would on ferromagnetic cores to further increase the level of inductance.
Read more about Inductors.
For anyone undertaking any electronic circuit design, there is a very good selection of these components available that enable all sorts of different types of circuits and functions to be accommodated.
Inductance is a very important aspect of electronic circuit design. Although inductors are not so widely used in low frequency electronic circuit designs because the size of the electronic components required to give the levels of inductance needed is large, they are widely used for much higher frequencies in radio frequency designs, as well as within EMC - where filtering is used, often using inductors to ensure that any interference is not able to pass along wires and cables.
In view of this, inductance is a very important aspect of electrical and electronic science and a basic understanding is always very useful.
Written by Ian Poole .
Experienced electronics engineer and author.
More Basic Electronics Concepts & Tutorials:
Voltage
Current
Power
Resistance
Capacitance
Inductance
Transformers
Decibel, dB
Kirchoff's Laws
Q, quality factor
RF noise
Waveforms
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