The Inductor
| An inductor can be a single turn of wire: | |
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| or many turns: | |
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. . . on a metal core, or an air core:
An inductor can be almost any size or shape and is the most complex component in electronics.
Even winding a toroid is an amazing process. Here is a diagram of a toroid winding machine:
There are 3 main symbols for an inductor:
Inductance is measured in Henries.
One Henry is a large unit.
An inductor of 1 Henry would be a few cm in diameter and a few cm long and have many turns of wire on a ferrite core.
An inductance of one Henry (or any value of inductance) does not tell you anything about the size of the device, its current capability (the amount of current that can flow through the winding without the device overheating) or any of the other features we need to know about it. That's why you need to know the PRACTICAL side of selecting an inductor.
In electronics, we normally use smaller units: mH µH and nH (m = milli µ = micro n = nano)
Surface mount inductors are measured in nH - nanoHenries and "µH" - microHenries.
See the table below for the very important way chip inductors are identified. Take special note of the letter "R" in the 3-digit code, for a 100nH or 1,000nH device. Do not get confused with a chip resistor as the two devices look almost identical and a resistor of "1R0" is one ohm.
| 1,000mH = 1H 1,000,000µH = 1H 1,000,000,000nH = 1H thus: 1,000µH = 1mH 1,000nH = 1µH Here are some typical values: 1nH = 0.001µH = 1N0 on a surface-mount component 10nH = 0.01µH = 10N " " " " 100nH = 0.1µH = R10 " " " " 1,000nH = 1µH = 1R0 " " " " 10,000nH = 10µH = 100 " " " " 100,000nH = 100µH = 101 " " " " 1,000,000nH = 1,000µH = 1mH = 102 10,000,000nH = 10,000µH = 10mH = 103 100,000,000nH = 100,000µH = 100mH = 0.1H = 104 1,000,000,000nH = 1,000,000µH = 1,000mH = 1H = 105 3.3nH = 0.0033µH = 3N3 on a surface-mount component 33nH = 0.033µH = 33N " " " " 330nH = 0.33µH = R33 " " " " 3,300nH = 3.3µH = 3R3 " " " " 33,000nH = 33µH = 0.033mH = 330 330,00nH = 330µH = 0.33mH = 331 3,300,00nH = 3,300µH = 3.3mH = 332 33,000,00nH = 33,0000µH = 33mH = 333 Note: 102, is the 3-digit identification on a surface-mount inductor. It means the figure "ten" and "two zero's" = 10 0 0 = 1,000µH = 1mH Surface mount inductors are measured in nH - nanoHenries and "µH" - microHenries. ((All surface mount capacitors are measured in "p" - picofarads)) Note: 102 is not 102 102 is 10 to the power "2" or "ten squared." 102 or 103 or 105 is "ten" then the third digit gives the number of "zeros." |
150 = 15uH (15 and no zero's)
471 = 470uH (47 and 1 zero)
100 = 10uH (10 and no zeros)
102 = 1,000uH = (10 and two zeros) = 1mH
Here are some more inductors:
In addition, the thickness of the wire has very little effect on the inductance and is only used to allow a high current to flow.
The value of an inductor cannot be determined by the way it looks. The value depends on a number of things including the core material, number of turns and the type of magnetic path. The best type of magnetic path is a closed loop such as the toroid (doughnut) shown in the photos at the top of the article or other type of closed magnetic path such as a pot-core. If the magnetic path contains an air gap, a lot of the magnetic flux will be lost when it "crosses the air gap" and the value of inductance will be reduced. For a simple inductor, a rod will be ok.
Inductors can have lead termination (called fly-leads), wire termination for through-hole mounting or as a "chip" for surface-mounting on a PC board.
The inductors above are identified in microHenry (µH), but the value marked on a surface-mount "chip inductor" can be nH - nanoHenries or "µH" - microHenries and you need to refer to the table above for the complete range of values as the letters N and R are also used to assist with the decade ranges (from 1nH to 9,999nH).
OTHER NAMES
An inductor can be called a "coil." There is no particular difference between a "coil" and an "inductor" and it mainly depends on where and how it is used. A coil generally refers to turns of wire on a former with an air core. When the core is metal (such as ferrite or soft iron or simply "iron"), it becomes an INDUCTOR.
In certain applications an inductor is called a CHOKE.
The term choke is used when the inductor is designed to prevent a signal passing through the winding or when the coil is designed to reduce a particular waveform - such as ripple. The following circuit shows a choke in operation. The circuit is called an L-C filter (or more-accurately a pi filter). The waveform on the left of the inductor (L) contains ripple as shown by the sinewave. The voltage emerging from the inductor has a smaller value of ripple. This is partially due to the filtering provided by C1 and C2 and also the effect of the choke.
The voltage entering the choke is mainly DC and this passes through the winding without any alteration. Any ripple contained within the DC creates an increasing magnetic flux and this cuts the turns of the winding to produce a reverse voltage. This acts against the ripple and effectively reduces it. The result is a lower value of ripple emerging from the inductor.
A resistor could be used in place of the inductor. The inductor has two advantages. It will produce a lower output ripple and a smaller voltage will be "lost" across the inductor.
An inductor is not the preferred choice for modern designs as a voltage regulator such as 7805, will provide the same results at a lower cost and will take up less board space.
We have used the inductor as an example, to show one of its characteristics. It has fallen out of favor with the introduction of the "3-terminal regulator" (we are talking about 50Hz power supplies).
In the following circuit, the signal emerges from the transistor and is prevented from flowing to earth by the "choke." The inductor provides a low resistance path for the biasing of the transistor while preventing the signal flowing to the 0v rail.
If the choke is replaced by a resistor, some of the signal will be lost in the resistor (we say "across the resistor") and the voltage dropped across the resistor will be higher than a choke.
If a winding on a coil or
"former" is designed to pull a metal rod into the centre of the coil
when a current flows, it is called a SOLENOID.
If the coil is wound on a metal core and attracts metal objects (such as the contacts of a relay, picking up scrap metal in a junk-yard, or to make a bell ring), it is called an ELECTROMAGNET.
The following diagram shows the operation of the electromagnet in a bell:
If the coil is wound on a metal core and attracts metal objects (such as the contacts of a relay, picking up scrap metal in a junk-yard, or to make a bell ring), it is called an ELECTROMAGNET.
The following diagram shows the operation of the electromagnet in a bell:
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HOW A BELL WORKS When the contacts are closed, current flows through the two windings (this is called a horseshoe electromagnet) and creates magnetic flux that pulls the arm (called the clapper) towards the electromagnet. This makes the hammer hit the bell and at the same time the contacts are opened. This causes the current to stop flowing and the magnetic flux ceases (collapses). The arm is returned (via a small piece of springy wire at the pivot-point) to a position where the contacts are closed and the current flows again to repeat the action. |
When it is operating (when an increasing voltage is applied), it produces a voltage in the opposite direction to the applied voltage (actually due to the increasing current) and the size of this voltage makes the inductor do amazing things.
This voltage is called a back-voltage or back-EMF. Its size depends on how the inductor is manufactured and its value in Henries (or millihenries, microhenries or nanohenries) and how it is activated in the circuit.
When an inductor is used in electronic circuit, the ratio of the back-voltage to the applied voltage is called the "Q-factor." This voltage can also be detected as the "spark" between the contacts of the bell above and it can be felt as a "kick-back" between your fingers when you remove an inductor from the supply voltage.
This voltage can be used to produce a very high voltage and is sometimes called a "fly-back" voltage.
This voltage is not wanted in some circuits and must be suppressed. The voltage produced by the coil of a relay (when it is de-energised) can damage the driving transistor and must be "snubbed" (removed) by placing a reverse-biased diode across the coil as shown in the diagram below:
So, there we have it.
In many instances an inductor will produce a high "reverse-voltage" when it is de-activated. The size of this voltage depends on the way the inductor is manufactured and many other things.
You cannot work out the size of the voltage from any formulae, so experimentation is the only way. At last we can put aside mathematics and get out the soldering iron.
There are basically two ways to use an inductor.
1. Pass a magnet over one end and detect (read) the voltage. A voltage is only produced when the magnet is moving. This is the basis of a GENERATOR.
2. Apply a voltage to the coil. This voltage can be a steady voltage (called DC) or a varying voltage (called AC). Different results will be produced in each case. This is the basis of a MOTOR.
If the voltage is steady (DC) the coil will produce STEADY magnetic flux and create an ELECTROMAGNET. We draw this flux as concentric lines around each conductor. They pass through the centre of the coil an emerge at one end. The emerging lines are said to create the NORTH pole of the electromagnet. The "magnetism" (the magnetic lines) are strongest in the centre of each turn of the coil and if the coil has air in the centre, only a small number of lines can be present before the air is SATURATED. If a metal such as iron (called soft iron) or ferrite (they are basically the same thing - with ferrite suitable for high frequency inductors) is placed in the centre, the magnetic lines can become more concentrated (1,000 - 2,500 times or more) before the core is saturated.
In many instances an inductor will produce a high "reverse-voltage" when it is de-activated. The size of this voltage depends on the way the inductor is manufactured and many other things.
You cannot work out the size of the voltage from any formulae, so experimentation is the only way. At last we can put aside mathematics and get out the soldering iron.
There are basically two ways to use an inductor.
1. Pass a magnet over one end and detect (read) the voltage. A voltage is only produced when the magnet is moving. This is the basis of a GENERATOR.
2. Apply a voltage to the coil. This voltage can be a steady voltage (called DC) or a varying voltage (called AC). Different results will be produced in each case. This is the basis of a MOTOR.
If the voltage is steady (DC) the coil will produce STEADY magnetic flux and create an ELECTROMAGNET. We draw this flux as concentric lines around each conductor. They pass through the centre of the coil an emerge at one end. The emerging lines are said to create the NORTH pole of the electromagnet. The "magnetism" (the magnetic lines) are strongest in the centre of each turn of the coil and if the coil has air in the centre, only a small number of lines can be present before the air is SATURATED. If a metal such as iron (called soft iron) or ferrite (they are basically the same thing - with ferrite suitable for high frequency inductors) is placed in the centre, the magnetic lines can become more concentrated (1,000 - 2,500 times or more) before the core is saturated.
If the driving voltage is AC (such as a sinewave) an electromagnet will
be produced but the magnetism of the electromagnet will increase and
decrease as the voltage varies.
Hundreds of different results can be produced from the examples above, by creating inductors with a different number of turns, different shape, different core material, different speed of movement of the magnet and different frequencies for the AC voltage.
Hundreds of different results can be produced from the examples above, by creating inductors with a different number of turns, different shape, different core material, different speed of movement of the magnet and different frequencies for the AC voltage.
Watch the needle on the meter when the loop changes
from a "forward" direction to a "reverse" direction. This
is when the flux changes direction.
When the two coils are stationary, the "centre-reading"
meter indicates "zero." This is because the magnetic
flux in not increasing or decreasing.
Watch the needle when the movement of the coil
ceases. This is when the magnetic flux is
stationary - "not increasing or decreasing."
Watch the needle when the coil is moving
away from the detecting loop.
In this discussion we are going to keep everything simple by saying this:
You can create almost any type of inductor by experimentation. You do not need to know any of the formulae or any of the theory. It can be created by simple "trial and error."
I admit a formulae will get you started but it will not tell you the type or size of former to use or the thickness of wire.
The best approach is to copy something similar to the type you need and modify it by adding or removing turns.
In this way you will be able to "peak" the inductor and be sure you have used the optimum number of turns.
This may seem to be a simplistic way to create an inductor, however it is successful. You finish up with an item that WORKS!
Now that we have simplified the approach, let's start with the THEORY:
The simplest inductor is a single turn of stiff wire with air in the centre (air core).
If a metal object is placed in the centre of the turn, the inductance is increased.
If additional turns are added, the inductance is increased.
If the diameter of the turn is increased, the inductance is DECREASED.
If the turns are stretched apart, the inductance of the coil DECREASES.
INDUCTORS IN PARALLEL AND SERIES
I have never had to place inductors in parallel or series in a final design, but during experimentation, it is handy to know what is happening.
Basically, they behave the same as RESISTORS.
In series, the inductance is increased and in parallel the overall inductance of the circuit is reduced.
You can create almost any type of inductor by experimentation. You do not need to know any of the formulae or any of the theory. It can be created by simple "trial and error."
I admit a formulae will get you started but it will not tell you the type or size of former to use or the thickness of wire.
The best approach is to copy something similar to the type you need and modify it by adding or removing turns.
In this way you will be able to "peak" the inductor and be sure you have used the optimum number of turns.
This may seem to be a simplistic way to create an inductor, however it is successful. You finish up with an item that WORKS!
Now that we have simplified the approach, let's start with the THEORY:
The simplest inductor is a single turn of stiff wire with air in the centre (air core).
If a metal object is placed in the centre of the turn, the inductance is increased.
If additional turns are added, the inductance is increased.
If the diameter of the turn is increased, the inductance is DECREASED.
If the turns are stretched apart, the inductance of the coil DECREASES.
INDUCTORS IN PARALLEL AND SERIES
I have never had to place inductors in parallel or series in a final design, but during experimentation, it is handy to know what is happening.
Basically, they behave the same as RESISTORS.
In series, the inductance is increased and in parallel the overall inductance of the circuit is reduced.
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| The total inductance is: 10 + 20 + 50 = 80µH |
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| The total inductance is: 10µH |
Note: A gold stripe in the 1st 2nd or third location represents a decimal point. When a decimal point is used, there is no multiplier.
DRIVING AN INDUCTOR
There are two ways to drive an inductor.
1. It can be driven with a SINEWAVE
2. It can be driven with a PULSE
In the diagram below, the inductor is driven by a sinewave from the driving transistor:
There are two ways to drive an inductor.
1. It can be driven with a SINEWAVE
2. It can be driven with a PULSE
In the diagram below, the inductor is driven by a sinewave from the driving transistor:
This is purely an experimental circuit as the inductor does not perform
any "feature." The voltage across the inductor is simply a reproduction
of the sinewave produced by the transistor. It does not produce the
"fly-back" voltage we mentioned above.
The reason is as follows: The magnetic flux is GRADUALLY increasing and decreasing during the cycle and although this flux cuts the turns of the coil it does not produce a voltage that is higher than the applied voltage.
If another winding (called the SECONDARY) is placed over the existing winding, it will produce a larger or smaller sinewave, according to the number of turns on the secondary. The inductor becomes a TRANSFORMER and this has been covered in another article.
A typical example of a component that looks like an inductor, but is really a transformer, is a "trigger transformer." It has a primary winding of about 30 to 100 ohms and a secondary consisting of 1,000 or more turns.
It has three leads and this may be confusing. The start winding and secondary winding are connected internally and this turns it into a type of transformer called an 'AUTO TRANSFORMER." It means the primary and secondary are connected and thus it does not provide insulation between windings - one of the most important reasons why a transformer is used to power an electronic device - when connected to the "mains."
The diagram below shows a trigger transformer:
The reason is as follows: The magnetic flux is GRADUALLY increasing and decreasing during the cycle and although this flux cuts the turns of the coil it does not produce a voltage that is higher than the applied voltage.
If another winding (called the SECONDARY) is placed over the existing winding, it will produce a larger or smaller sinewave, according to the number of turns on the secondary. The inductor becomes a TRANSFORMER and this has been covered in another article.
A typical example of a component that looks like an inductor, but is really a transformer, is a "trigger transformer." It has a primary winding of about 30 to 100 ohms and a secondary consisting of 1,000 or more turns.
It has three leads and this may be confusing. The start winding and secondary winding are connected internally and this turns it into a type of transformer called an 'AUTO TRANSFORMER." It means the primary and secondary are connected and thus it does not provide insulation between windings - one of the most important reasons why a transformer is used to power an electronic device - when connected to the "mains."
The diagram below shows a trigger transformer:
If an inductor is driven by a pulse, the applied voltage is turned off at
some point in the cycle and this causes the driving current to cease.
In the diagram below, the inductor is driven by pulses:
In the diagram below, the inductor is driven by pulses:
The magnetic flux that is present at the time when the transistor turns
off collapses immediately and creates a voltage in the winding that
has the opposite polarity to the driving voltage. If there is a lot of
magnetic flux (stored in the iron or ferrite core) the voltage produced
will be very high.
We are not getting something for nothing. In the first instance, the multiplication of the supply voltage and current produces a certain value of stored energy. This stored energy is converted from a low-voltage/high-current to a high-voltage/low-current.
This effect can be used to produce a high voltage from a low voltage supply. It is commonly called the "fly-back" effect. The output from the inductor are spikes of very high voltage. These are passed through a diode and stored in a capacitor. The diode prevents the voltage on the capacitor feeding back into the winding of the inductor and discharging the capacitor.
We are not getting something for nothing. In the first instance, the multiplication of the supply voltage and current produces a certain value of stored energy. This stored energy is converted from a low-voltage/high-current to a high-voltage/low-current.
This effect can be used to produce a high voltage from a low voltage supply. It is commonly called the "fly-back" effect. The output from the inductor are spikes of very high voltage. These are passed through a diode and stored in a capacitor. The diode prevents the voltage on the capacitor feeding back into the winding of the inductor and discharging the capacitor.
HOW DO YOU
DESIGN AN INDUCTOR?
Basically you can't.
In most cases you have no idea how an inductor should appear for a particular application, its size or how many turns are required.
You need to see an example.
Disassemble a sample, count the number of turns and measure the diameter of the wire.
Carefully note any features such as the thickness and type of insulation and the way the inductor has been wound.
Jumble-winding or layer-winding does not alter the inductance but if it is required to produce an extremely high "fly-back" voltage, the voltage between any two turns must not be higher than 80v.
This means the turns must be wound in layers with very good insulation between layers.
If the inductor is to be used in a high-frequency situation, the core material must be a high-frequency ferrite such as F24.
If you intend to copy an inductor, it is best to have two samples. One sample is dismantled and the other is used as a reference, to compare with your prototype.
Basically you can't.
In most cases you have no idea how an inductor should appear for a particular application, its size or how many turns are required.
You need to see an example.
Disassemble a sample, count the number of turns and measure the diameter of the wire.
Carefully note any features such as the thickness and type of insulation and the way the inductor has been wound.
Jumble-winding or layer-winding does not alter the inductance but if it is required to produce an extremely high "fly-back" voltage, the voltage between any two turns must not be higher than 80v.
This means the turns must be wound in layers with very good insulation between layers.
If the inductor is to be used in a high-frequency situation, the core material must be a high-frequency ferrite such as F24.
If you intend to copy an inductor, it is best to have two samples. One sample is dismantled and the other is used as a reference, to compare with your prototype.
WHAT TYPE OF INDUCTOR?
Suppose you have been shown a circuit requiring a 10nH choke.
Can any type of 10nH choke (inductor) be used?
How many different types of 10nH inductors are there?
How do you know which type to use?
The answer to this very complex. There are many different 10nH inductors and most circuit diagrams do not provide sufficient information for you to get (or make) the correct type.
The value "10nH" is like saying a resistor is "1k." It does not tell you all the features you need to know such as wattage or tolerance.
The same with a 10nH inductor. The value tells you nothing about its physical size, the size of the winding etc.
A 10nH inductor can be created by winding thick wire or thin wire onto a core of magnetic material. The inductor using thick wire will be larger and the resistance of the coil will be less.
The two 10nH inductors will perform completely differently when connected to some circuits.
The following circuit shows a typical use for an inductor.
It is connected across a piezo diaphragm.
The collapsing magnetic field of the inductor produces a very high voltage and this is passed to the piezo diaphragm to produce a very load output.
For a 12v supply, this voltage can be as high as 120v.
If the inductor has a low resistance, you will have to drive the transistor very hard during a part of each cycle, to produce a current-flow in the inductor.
If the resistance (called the DC resistance) of the inductor is high, the transistor will not have to be driven as hard and thus the circuit will be more efficient.
Suppose you have been shown a circuit requiring a 10nH choke.
Can any type of 10nH choke (inductor) be used?
How many different types of 10nH inductors are there?
How do you know which type to use?
The answer to this very complex. There are many different 10nH inductors and most circuit diagrams do not provide sufficient information for you to get (or make) the correct type.
The value "10nH" is like saying a resistor is "1k." It does not tell you all the features you need to know such as wattage or tolerance.
The same with a 10nH inductor. The value tells you nothing about its physical size, the size of the winding etc.
A 10nH inductor can be created by winding thick wire or thin wire onto a core of magnetic material. The inductor using thick wire will be larger and the resistance of the coil will be less.
The two 10nH inductors will perform completely differently when connected to some circuits.
The following circuit shows a typical use for an inductor.
It is connected across a piezo diaphragm.
The collapsing magnetic field of the inductor produces a very high voltage and this is passed to the piezo diaphragm to produce a very load output.
For a 12v supply, this voltage can be as high as 120v.
If the inductor has a low resistance, you will have to drive the transistor very hard during a part of each cycle, to produce a current-flow in the inductor.
If the resistance (called the DC resistance) of the inductor is high, the transistor will not have to be driven as hard and thus the circuit will be more efficient.
The same situation occurs with a high-voltage generating circuit, using an
inductor, as shown in the diagram below.
If the inductor has a high resistance, the output from the circuit will be very high and the transistor will not have to be driven very hard. In other words, the efficiency of the circuit will be high.
If the inductor has a high resistance, the output from the circuit will be very high and the transistor will not have to be driven very hard. In other words, the efficiency of the circuit will be high.
THE "Q-FACTOR"
The "Q-factor" or Quality-factor refers to the voltage generated by an oscillatory circuit made up of a coil and capacitor. In the circuit below, the coil and capacitor are connected in parallel and this is called an L-C circuit (parallel L-C circuit). When this circuit is added to an FM transmitter, it is given the name '"TANK CIRCUIT."
The two components we are discussing are the coil and capacitor. The transistor is merely the driving component and has nothing to do with the feature of producing the high voltage.
We have already explained how an inductor produces a high voltage when the magnetic flux collapses and this is why the L-C circuit will produce a voltage higher than the supply.
The ratio of the generated-voltage to the supply voltage gives the Q-factor. This can be as low as 1 or 2 for a poorly designed circuit, up to100 or more. The quality depends on how much magnetic flux is produced and how effectively it cuts the turns of the coil.
As the frequency of a circuit increases, the effectiveness of ferrite as a core material decreases. The maximum frequency for ferrite is about 100MHz - 200MHz. At this frequency the difference between air and ferrite is very small. For this reason, air-cored coils are often used.
These are just a few of the uses for an
inductor.
The main point of this article is to make you aware of the need to check the resistance of an inductor to see if a high resistance or low resistance version will improve the output of the circuit.
And remember the SECRET . . .
The inductor produces a REVERSE VOLTAGE when the supply is TURNED OFF:
The main point of this article is to make you aware of the need to check the resistance of an inductor to see if a high resistance or low resistance version will improve the output of the circuit.
And remember the SECRET . . .
The inductor produces a REVERSE VOLTAGE when the supply is TURNED OFF:
Slow-motion showing showing the
"reverse voltage" pulse produced by the
inductor when the supply is removed.
When a
capacitor is added to the circuit, the energy flows from the inductor to
the capacitor, and back to the inductor, when the supply is removed, to
produce an "oscillatory effect."
The end result is a sinewave output.
The animation below shows the energy flowing between the components with the "centre-reading" voltmeter detecting the voltage:
The end result is a sinewave output.
The animation below shows the energy flowing between the components with the "centre-reading" voltmeter detecting the voltage:
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TERMINOLOGY: A coil can be used as a "pick-up" to detect magnetic or metal objects. It can be called a TRANSDUCER, Inductive transducer, magnetic transducer, coil, pick-up, inductor, magnetic coil, pickup coil, inductive loop, inductive sensor, magnetic sensor, metal detector, comparator, gold detector, crack detector - to detect cracks in welds etc, head - as in a tape recorder. It can have a core made of iron or ferrite and be called an INDUCTOR. It can have a moving iron core and be called a SOLENOID. An inductor can be used to smooth the ripple in a supply, or it can be used to generate a voltage higher than the supply and it can be wound on "poles" to create a motor. It can have an adjacent winding and become a transformer, isolator or step-up device. It can be a current transformer, or even a linear motor. And there are possibly dozens more . . . |
THE INDUCTOR AS A "PICK-UP."
Now we come to an important feature of a coil when it is used as a SENSOR.
When a magnet passes a coil (this includes the action of moving towards or away from a coil), a voltage is generated in the turns in the form of a sinewave.
We use the term "sinewave" to indicate the approximate shape of the waveform to distinguish it from other shapes such as "square wave," "exponential" or "glitch." A sinewave is a continuing waveshape with a gradual rise and fall as shown in the following example:
Now we come to an important feature of a coil when it is used as a SENSOR.
When a magnet passes a coil (this includes the action of moving towards or away from a coil), a voltage is generated in the turns in the form of a sinewave.
We use the term "sinewave" to indicate the approximate shape of the waveform to distinguish it from other shapes such as "square wave," "exponential" or "glitch." A sinewave is a continuing waveshape with a gradual rise and fall as shown in the following example:
The same type of waveform is produced if the magnet passes the end of the coil, into and
out of the end of the coil or if the magnet passes through the centre.
If the magnet is moved rapidly, the amplitude of the waveform INCREASES (and there will be more "up's ad down's" in the same time-interval on the diagram above).
The amplitude is also determined by the strength of the magnet.
If the magnet is moved rapidly, the amplitude of the waveform INCREASES (and there will be more "up's ad down's" in the same time-interval on the diagram above).
The amplitude is also determined by the strength of the magnet.
There are three important points to note.
The first is the voltage produced by the coil as it passes the end of the coil.
When the magnet is directly opposite the end of the coil, the change in magnetic flux is zero and thus the voltage produced by the coil is zero.
The second point is the change in voltage produced by the coil. The output voltage changes from positive to negative during the very small portion of excursion when the magnet moves from a forward to reverse direction as seen by the end of the coil.
The third point is the coil produces zero voltage when the magnet is not moving.
If the magnet moves at a faster rate, the voltage produced by the coil will be greater as shown by the animation below:
The first is the voltage produced by the coil as it passes the end of the coil.
When the magnet is directly opposite the end of the coil, the change in magnetic flux is zero and thus the voltage produced by the coil is zero.
The second point is the change in voltage produced by the coil. The output voltage changes from positive to negative during the very small portion of excursion when the magnet moves from a forward to reverse direction as seen by the end of the coil.
The third point is the coil produces zero voltage when the magnet is not moving.
If the magnet moves at a faster rate, the voltage produced by the coil will be greater as shown by the animation below:
If two or more coils are placed in close proximity
with one or more coils providing a magnetic field, when a magnet or metal
object is passed through the field, the waveform produced by the
sensing coil is altered. The size and shape may be very small but amplifying stages
can produce amazing information.
This is the principle of a metal detector (gold detector) or a coin detector in a vending machine.
The resulting waveform can discriminate between a coin and a "slug," an aluminium can, a "pull ring" or a gold nugget. This type of detector is beyond this discussion. We will only be discussing how to detect the frequency of the pulses and the amplitude of the voltage from a single coil.
For an inductive pick-up to be successful, the magnet passing the end of the coil must be powerful and pass near to the end of the coil.
The output of a coil will generally be less than 700mV and must be AC coupled to a transistor so that the voltage produced by coil will modify the biasing of the transistor as shown in the diagram below:
This is the principle of a metal detector (gold detector) or a coin detector in a vending machine.
The resulting waveform can discriminate between a coin and a "slug," an aluminium can, a "pull ring" or a gold nugget. This type of detector is beyond this discussion. We will only be discussing how to detect the frequency of the pulses and the amplitude of the voltage from a single coil.
For an inductive pick-up to be successful, the magnet passing the end of the coil must be powerful and pass near to the end of the coil.
The output of a coil will generally be less than 700mV and must be AC coupled to a transistor so that the voltage produced by coil will modify the biasing of the transistor as shown in the diagram below:
In the diagram below, the magnet is passing the coil and when it is
receding from the coil, the voltage produced by the coil turns the
transistor OFF and the voltage on the collector rises.
The coil can be connected to a two-transistor arrangement to produce a
square-wave output, suitable for circuits that require a noise-free
signal:
A very simple circuit using a coil is shown in the diagram below. It is
our METAL DETECTOR -1.
It uses a 16 turn coil (approx 6" dia) to detect metal objects such as coins etc. The circuit oscillates at approx 140kHz and the frequency produced is picked up by an AM radio to produce a quiet spot on the dial. When a piece of metal is placed near the coil, the frequency of the circuit is altered and this is picked up by the radio as a low frequency tone. The circuit is extremely sensitive and a shift in frequency of as little as a few hertz will be clearly heard.
It uses a 16 turn coil (approx 6" dia) to detect metal objects such as coins etc. The circuit oscillates at approx 140kHz and the frequency produced is picked up by an AM radio to produce a quiet spot on the dial. When a piece of metal is placed near the coil, the frequency of the circuit is altered and this is picked up by the radio as a low frequency tone. The circuit is extremely sensitive and a shift in frequency of as little as a few hertz will be clearly heard.
ROTATION
A motor is an example of a rotating inductor. Most small motors are 3-pole (the minimum number of poles for self-starting) and if a motor is used as a generator, the output will correspond to the speed of rotation.
For a 3-pole motor, three waveforms are produced for each revolution and the following diagram shows the type of waveform produced:
A motor is an example of a rotating inductor. Most small motors are 3-pole (the minimum number of poles for self-starting) and if a motor is used as a generator, the output will correspond to the speed of rotation.
For a 3-pole motor, three waveforms are produced for each revolution and the following diagram shows the type of waveform produced:
If the motor increases in RPM, the waveform changes:
A detecting circuit can be used to count the pulses and determine the
RPM.
By putting fan blades on the shaft of a motor, you can measure wind velocity and the output of heating and cooling systems etc.
The output from the motor can be calibrated by placing the fan outside the window of a car traveling at a known velocity.
THE INDUCTOR AS A FILTER - also known as a CHOKE
When an inductor is placed in a circuit and reduces the ripple, as it does in the circuit below, it is also known as a CHOKE - it "chokes off" the ripple. This is old terminology and is called Jargon. (Jargon are words or sentences that are only understood by those who work in the particular field or "area" or job.)
We have already covered this feature at the beginning of this article but since it is so important, we will go over it again.
This time we will cover some of the features of a coil and one of its hidden "magical properties." This magical property is the ability of a coil (inductor) to produce a BACK VOLTAGE or REVERSE VOLTAGE that opposes an increasing or decreasing voltage.
This is how the inductor smoothes (reduces) the ripple in the voltage emerging from the rectifier.
It all starts when a voltage increases (or decreases) in amplitude.
Any increasing voltage allows an increasing current to flow and this current increases the magnetic flux produced by the coil and this flux cuts all the other turns of the coil to produce a "back voltage."
This is the situation with the inductor "L" in the circuit below:
By putting fan blades on the shaft of a motor, you can measure wind velocity and the output of heating and cooling systems etc.
The output from the motor can be calibrated by placing the fan outside the window of a car traveling at a known velocity.
THE INDUCTOR AS A FILTER - also known as a CHOKE
When an inductor is placed in a circuit and reduces the ripple, as it does in the circuit below, it is also known as a CHOKE - it "chokes off" the ripple. This is old terminology and is called Jargon. (Jargon are words or sentences that are only understood by those who work in the particular field or "area" or job.)
We have already covered this feature at the beginning of this article but since it is so important, we will go over it again.
This time we will cover some of the features of a coil and one of its hidden "magical properties." This magical property is the ability of a coil (inductor) to produce a BACK VOLTAGE or REVERSE VOLTAGE that opposes an increasing or decreasing voltage.
This is how the inductor smoothes (reduces) the ripple in the voltage emerging from the rectifier.
It all starts when a voltage increases (or decreases) in amplitude.
Any increasing voltage allows an increasing current to flow and this current increases the magnetic flux produced by the coil and this flux cuts all the other turns of the coil to produce a "back voltage."
This is the situation with the inductor "L" in the circuit below:
When current flows, the
voltage-waveform after the inductor, will be smaller than
the waveform entering the inductor. The size of the waveform from the
bridge
will depend on the ripple from the transformer. The diagram above shows
a waveform before and after the inductor but this is just a
representation. It is not a true indication of the size of the waveform.
A power supply contains electrolytic called filter electrolytics and the diagram below shows one placed before the inductor and one after the inductor.
A power supply contains electrolytic called filter electrolytics and the diagram below shows one placed before the inductor and one after the inductor.
This discussion is very
complex because we are constantly discussing voltage waveforms then
current waveforms. But this is the way it has to be.
The other thing that is hard to understand is the term "DC." When we say "DC" we mean a steady or unchanging voltage or current. Even though the real meaning of DC is "Direct Current" we still refer to an unchanging voltage as "DC." Again this is jargon and that's why you need to understand the meaning of the words.
The voltage waveform entering the inductor will actually be something like 10v DC with a ripple of say 300mV and 9.5v with a ripple of 50mV leaving the inductor.
This is shown on the diagram below:
The other thing that is hard to understand is the term "DC." When we say "DC" we mean a steady or unchanging voltage or current. Even though the real meaning of DC is "Direct Current" we still refer to an unchanging voltage as "DC." Again this is jargon and that's why you need to understand the meaning of the words.
The voltage waveform entering the inductor will actually be something like 10v DC with a ripple of say 300mV and 9.5v with a ripple of 50mV leaving the inductor.
This is shown on the diagram below:
The size of the "output" waveform (from the inductor) will
depend on the inductance of L and the value of the load. If the load is
an amplifier, the current will be changing all the time according to the
level of music or speech. If the load is a globe, we call the load a
"steady load." By this we mean the current is steady.
Even if you are supplying a steady load such as a globe, the waveform (ripple) entering the inductor will create a "back-voltage" in the inductor that will reduce the peaks and increase the "lows." This is due to the input waveform have a "ripple component." If the input voltage was "pure DC," the inductor would not be needed. This is just an example of the operation of the inductor. There will be a voltage drop across the indicator due to the resistance of the winding. This can be proven by connecting the inductor to a battery (such as a car battery) and measuring the voltage drop across it for any given load.
Now we go back to our example: The output ripple is not constant. As the current is increased, the output ripple will increase. This is due to a number of factors.
The transformer will not be able to supply the higher current and its output voltage will drop. The electrolytics will provide less filtering at the higher current (see circuit below) and the inductor will become "magnetically saturated" and not produce the same filtering. All these characteristics will combine to produce a varying ripple voltage on the output.
There is another factor to consider.
You simply cannot select an inductor by inductance alone. For instance, you cannot simply say "use a 10,000uH choke." Not all 10,000uH chokes are the same. Here is an example of 3 different 10,000uH chokes.
But before we do, remember this:
Ten thousand microhenries is the same as 10 millihenries.
1,000nH = 1µH
1,000µH = 1mH
1,000mH = 1Henry
The following photos show different types of chokes. All have the same inductance (10,000uH) but they will all produce a different output because they have different coil-resistances. The second inductor seems to be up-side-down, but the two ends are soldered to the PC board. It is a surface-mount item.
Even if you are supplying a steady load such as a globe, the waveform (ripple) entering the inductor will create a "back-voltage" in the inductor that will reduce the peaks and increase the "lows." This is due to the input waveform have a "ripple component." If the input voltage was "pure DC," the inductor would not be needed. This is just an example of the operation of the inductor. There will be a voltage drop across the indicator due to the resistance of the winding. This can be proven by connecting the inductor to a battery (such as a car battery) and measuring the voltage drop across it for any given load.
Now we go back to our example: The output ripple is not constant. As the current is increased, the output ripple will increase. This is due to a number of factors.
The transformer will not be able to supply the higher current and its output voltage will drop. The electrolytics will provide less filtering at the higher current (see circuit below) and the inductor will become "magnetically saturated" and not produce the same filtering. All these characteristics will combine to produce a varying ripple voltage on the output.
There is another factor to consider.
You simply cannot select an inductor by inductance alone. For instance, you cannot simply say "use a 10,000uH choke." Not all 10,000uH chokes are the same. Here is an example of 3 different 10,000uH chokes.
But before we do, remember this:
Ten thousand microhenries is the same as 10 millihenries.
1,000nH = 1µH
1,000µH = 1mH
1,000mH = 1Henry
The following photos show different types of chokes. All have the same inductance (10,000uH) but they will all produce a different output because they have different coil-resistances. The second inductor seems to be up-side-down, but the two ends are soldered to the PC board. It is a surface-mount item.
 |
 |
 |
|
10milliHenry
2R7 Max current 3A |
10milliHenry
15R Max current 2mA |
10milliHenry 33R Max current 20mA |
The photos above do not show the real size of the components but you can see
each has a maximum current rating.
The current rating is the dominant factor.
That's why a 10mH choke can have so many different sizes.
THE INDUCTOR IN A POWER SUPPLY
An inductor can be used in a power supply to reduce the ripple.
In most power supplies this is done with electrolytics, however we will explain how the inductor operates.
The inductor only operates on the fluctuating part of the voltage.
If the voltage rises, it increases the magnetic flux and this is called expanding flux. This flux cuts all the turns of the coil and produces a voltage in the turns that is opposite to the incoming voltage.
Thus the increasing voltage does not enter the inductor.
This is how the inductor reduces the ripple on the output.
In the following circuit, the output has a reduced ripple due to the inductor:
The current rating is the dominant factor.
That's why a 10mH choke can have so many different sizes.
THE INDUCTOR IN A POWER SUPPLY
An inductor can be used in a power supply to reduce the ripple.
In most power supplies this is done with electrolytics, however we will explain how the inductor operates.
The inductor only operates on the fluctuating part of the voltage.
If the voltage rises, it increases the magnetic flux and this is called expanding flux. This flux cuts all the turns of the coil and produces a voltage in the turns that is opposite to the incoming voltage.
Thus the increasing voltage does not enter the inductor.
This is how the inductor reduces the ripple on the output.
In the following circuit, the output has a reduced ripple due to the inductor:
The following diagram shows an inductor with a closed magnetic circuit. The "magnetic circuit" is shown via the arrows:
An
"open" magnetic circuit is shown above via the colour-coded inductor.
The "magnetic circuit" is the core but the flux does not form a
continuous loop. This type of magnetic circuit is very inefficient and
has high losses. But it is quite acceptable if the magnetic flux is kept
to a low level where the core is not saturated.
DESIGNING AN INDUCTOR AS A FILTER (choke)
Designing an inductor for the above application is a very complex mathematical problem. We do not know the ripple on the input to the inductor or any of the voltage values as a small transformer as show in the diagram has a very poor regulation factor and the output can be up to 60% higher than the stated output so that the voltage drops to the required level on full output current.
The best thing is to have a range of inductors and try them.
If you are winding your own inductor it is best to add too many turns to a core and gradually remove them as needed.
Nothing beats "actual application" as there are too many variables to be able to design something from a chart.
If you don't know where to start, look at a power supply. Remember the frequency of this power supply is either 50Hz or 60Hz. It is not a 40kHz design. The inductance will be much higher than for a 40kHz circuit.
The same approach is recommended for any type of inductor.
An inductor is very difficult to design.
Projects do not always consume a constant current and the ripple present on the unfiltered side of a power supply needs to be viewed on a CRO.
Rather than using complex mathematical formulae to work out the value of an inductor, the easiest way is to try different values.
THE WIRE
The size of the wire (the thickness) is an important factor when designing an inductor.
It is always best to use the thickest wire for the application.
WHY?
The thickest wire produces the best result.
But finding the best thickness (gauge) is a complex problem.
Let's explain:
In some cases the wire-size is easy to work out. For a transformer, the size of the former (the plastic bobbin on which the wire is wound) and the area (space for the winding) is already known. You will also know the number of turns required for each volt and thus the total number of turns will be known. The size (gauge) of wire can be found from a table.
But an electromagnet (or solenoid) is different. This is basically a DC component, although it will work on AC (say 50Hz or 60Hz).
These devices are designed to produce magnetic flux (to pull in an armature or core or collect scrap metal - such as in a metal-yard) and the flux is produced by multiplying the number of turns by the current flowing though the coil. This is called AMP-TURNS.
Theoretically, the same flux can be produced by one turn and 100amps or 100 turns and one amp or 500 turns and 200mA.
But the current will depend on the gauge of the wire (as thin wire has a higher resistance - and this will limit the amount of current that will flow).
So, the maximum flux will depend on selecting a wire-size. Working out how many turns can be fitted onto the former (wound on the bobbin) and thus the total length of wire can be determined. This will give you the resistance of the coil and thus the current (use a table to find the resistance and Ohm's Law to find the current). Multiply the number of turns by the current. Select another gauge of wire and eventually you will get a table of values. From this table you will see a maximum value.
If you are designing an inductor for an AC voltage or any fluctuating or changing voltage, you will utilizing the coils: "magic property." This is the fact that the expanding or collapsing flux from each turn cuts all the other turns of the coil to produce a voltage in the opposite direction. This is called the INDUCTANCE of the coil and it means the coil does not only produce magnetic flux as described in the electromagnet or solenoid above, but it also has an effect of limiting or reducing the current you can deliver to the coil. This is because a coil, solenoid or inductor always limits or reduces the current at the instant you apply the voltage.
If you are constantly utilizing this feature by supplying a rising and falling voltage, the coil will behave completely differently to a solenoid (that has a DC supply connected to it for a long period of time).
This means you must treat the coil completely differently to a solenoid.
It will produce completely different results, however it is best to use the thickest gauge available.
WHY?
The thick wire allows more of the flux to pass through the wire and thus produce a higher reverse voltage.
In addition, it will have a lower resistance and this will allow a higher current to flow and thus create more flux.
THE INDUCTOR IN "FLYBACK"
We mentioned above, one of the "magical properties" of an inductor is its ability to produce a "back-voltage" or "reverse voltage."
There is an even-more-magical extension to this.
If a voltage is applied to an inductor and then removed, the back-voltage will be VERY HIGH. It can be 100 times (or more) higher than the applied voltage.
This is the principle of the ignition system in a car. The distributor connects the ignition-coil to the battery of the car via the points and then the points open.
The collapsing magnetic filed in the ignition-coil is passed from the end of the coil to the distributor rotor-cap, and this is the rotating part of the distributor. It sends the 20,000v to the appropriate spark-plug.
So, the collapsing property of an inductor has been known for a long time and it has also been used in electronics for many applications.
Uses such as electric fences, high voltage generators, EHT circuits in TV's, switch-mode power supplies.
This back-voltage is also produced by relays, motors, door-latches and where-ever a coil is energised.
In most cases this voltage is higher than the operating voltage of the components in the circuit and it must be prevented from damaging them.
In the case of relay, the back-emf, (this is what the back-voltage is called) is snubbed (reduced) by the diode. The back-voltage has the opposite polarity to the supply and this voltage is placed directly across the diode and it forms a very low resistance path to absorb the energy.
DESIGNING AN INDUCTOR AS A FILTER (choke)
Designing an inductor for the above application is a very complex mathematical problem. We do not know the ripple on the input to the inductor or any of the voltage values as a small transformer as show in the diagram has a very poor regulation factor and the output can be up to 60% higher than the stated output so that the voltage drops to the required level on full output current.
The best thing is to have a range of inductors and try them.
If you are winding your own inductor it is best to add too many turns to a core and gradually remove them as needed.
Nothing beats "actual application" as there are too many variables to be able to design something from a chart.
If you don't know where to start, look at a power supply. Remember the frequency of this power supply is either 50Hz or 60Hz. It is not a 40kHz design. The inductance will be much higher than for a 40kHz circuit.
The same approach is recommended for any type of inductor.
An inductor is very difficult to design.
Projects do not always consume a constant current and the ripple present on the unfiltered side of a power supply needs to be viewed on a CRO.
Rather than using complex mathematical formulae to work out the value of an inductor, the easiest way is to try different values.
THE WIRE
The size of the wire (the thickness) is an important factor when designing an inductor.
It is always best to use the thickest wire for the application.
WHY?
The thickest wire produces the best result.
But finding the best thickness (gauge) is a complex problem.
Let's explain:
In some cases the wire-size is easy to work out. For a transformer, the size of the former (the plastic bobbin on which the wire is wound) and the area (space for the winding) is already known. You will also know the number of turns required for each volt and thus the total number of turns will be known. The size (gauge) of wire can be found from a table.
But an electromagnet (or solenoid) is different. This is basically a DC component, although it will work on AC (say 50Hz or 60Hz).
These devices are designed to produce magnetic flux (to pull in an armature or core or collect scrap metal - such as in a metal-yard) and the flux is produced by multiplying the number of turns by the current flowing though the coil. This is called AMP-TURNS.
Theoretically, the same flux can be produced by one turn and 100amps or 100 turns and one amp or 500 turns and 200mA.
But the current will depend on the gauge of the wire (as thin wire has a higher resistance - and this will limit the amount of current that will flow).
So, the maximum flux will depend on selecting a wire-size. Working out how many turns can be fitted onto the former (wound on the bobbin) and thus the total length of wire can be determined. This will give you the resistance of the coil and thus the current (use a table to find the resistance and Ohm's Law to find the current). Multiply the number of turns by the current. Select another gauge of wire and eventually you will get a table of values. From this table you will see a maximum value.
If you are designing an inductor for an AC voltage or any fluctuating or changing voltage, you will utilizing the coils: "magic property." This is the fact that the expanding or collapsing flux from each turn cuts all the other turns of the coil to produce a voltage in the opposite direction. This is called the INDUCTANCE of the coil and it means the coil does not only produce magnetic flux as described in the electromagnet or solenoid above, but it also has an effect of limiting or reducing the current you can deliver to the coil. This is because a coil, solenoid or inductor always limits or reduces the current at the instant you apply the voltage.
If you are constantly utilizing this feature by supplying a rising and falling voltage, the coil will behave completely differently to a solenoid (that has a DC supply connected to it for a long period of time).
This means you must treat the coil completely differently to a solenoid.
It will produce completely different results, however it is best to use the thickest gauge available.
WHY?
The thick wire allows more of the flux to pass through the wire and thus produce a higher reverse voltage.
In addition, it will have a lower resistance and this will allow a higher current to flow and thus create more flux.
THE INDUCTOR IN "FLYBACK"
We mentioned above, one of the "magical properties" of an inductor is its ability to produce a "back-voltage" or "reverse voltage."
There is an even-more-magical extension to this.
If a voltage is applied to an inductor and then removed, the back-voltage will be VERY HIGH. It can be 100 times (or more) higher than the applied voltage.
This is the principle of the ignition system in a car. The distributor connects the ignition-coil to the battery of the car via the points and then the points open.
The collapsing magnetic filed in the ignition-coil is passed from the end of the coil to the distributor rotor-cap, and this is the rotating part of the distributor. It sends the 20,000v to the appropriate spark-plug.
So, the collapsing property of an inductor has been known for a long time and it has also been used in electronics for many applications.
Uses such as electric fences, high voltage generators, EHT circuits in TV's, switch-mode power supplies.
This back-voltage is also produced by relays, motors, door-latches and where-ever a coil is energised.
In most cases this voltage is higher than the operating voltage of the components in the circuit and it must be prevented from damaging them.
In the case of relay, the back-emf, (this is what the back-voltage is called) is snubbed (reduced) by the diode. The back-voltage has the opposite polarity to the supply and this voltage is placed directly across the diode and it forms a very low resistance path to absorb the energy.
Another way to prevent the high voltage damaging the circuit is to
provide high-voltage insulation and shielding. Apart from
spike-suppression capacitors across the chips, there is no other way to
prevent high voltages damaging a circuit.
THE SECRET
The following circuit uses an inductor to separate the 3.6v across a 1 watt LED from a 15v power supply.
This circuit explains the secret: "HOW AN INDUCTOR WORKS."
The resistance of the inductor is less than one ohm and it sees about 14v on the left lead and 3.6v on the right lead.
So . . . how does it work?
How does it allow 14v to be present on one side and 3.6v on the other side. The 1R resistor between the inductor and LED only has about 0.3v across it.
Obviously the resistance of the inductor is not creating the 14 - 3.6 = 10.4volts across the leads.
It must be something to do with the turns of wire on the ferrite core.
On the right lead of the inductor is a 100u electrolytic. This capacitor has the effect of preventing the voltage rising or falling. It keeps the voltage fixed and stable.
When the BC327 transistor turns ON, it sends a pulse of current to the left lead of the inductor. This current enters the inductor and produces magnetic flux that cuts all the turns of wire and produces a voltage in the opposite direction.
This voltage is nearly the same value as the voltage entering the coil and the result is very little current will flow though the inductor.
This current is exactly the correct amount to fully illuminate the LED.
The inductor can only prevent too much current flowing FOR A VERY SHORT PERIOD OF TIME.
That's why the oscillator is a very HIGH FREQUENCY.
That's the secret behind the operation of the inductor.
It creates a voltage across it that limits the current flowing through the turns.
Of course the inductor must be selected to have the correct number of turns and the correct wire-size and correct ferrite-size.
The following circuit uses an inductor to separate the 3.6v across a 1 watt LED from a 15v power supply.
This circuit explains the secret: "HOW AN INDUCTOR WORKS."
The resistance of the inductor is less than one ohm and it sees about 14v on the left lead and 3.6v on the right lead.
So . . . how does it work?
How does it allow 14v to be present on one side and 3.6v on the other side. The 1R resistor between the inductor and LED only has about 0.3v across it.
Obviously the resistance of the inductor is not creating the 14 - 3.6 = 10.4volts across the leads.
It must be something to do with the turns of wire on the ferrite core.
On the right lead of the inductor is a 100u electrolytic. This capacitor has the effect of preventing the voltage rising or falling. It keeps the voltage fixed and stable.
When the BC327 transistor turns ON, it sends a pulse of current to the left lead of the inductor. This current enters the inductor and produces magnetic flux that cuts all the turns of wire and produces a voltage in the opposite direction.
This voltage is nearly the same value as the voltage entering the coil and the result is very little current will flow though the inductor.
This current is exactly the correct amount to fully illuminate the LED.
The inductor can only prevent too much current flowing FOR A VERY SHORT PERIOD OF TIME.
That's why the oscillator is a very HIGH FREQUENCY.
That's the secret behind the operation of the inductor.
It creates a voltage across it that limits the current flowing through the turns.
Of course the inductor must be selected to have the correct number of turns and the correct wire-size and correct ferrite-size.
CONCLUSION
This discussion has covered only a fraction of the mysteries of the inductor. There are special ways to wind an inductor for high voltage circuits. There are special ways to reduce the inductance and there are special cores to increase the inductance.
There are ways to tap an inductor to get all sorts of results such as high current, high impedance, low impedance and impedance-matching. You can add a second, third and fourth winding to get isolation, impedance-matching, high voltage or high current. Inductors can be made long, short, fat or any shape to fit onto a circuit.
That's why there are so many shapes, sizes and pin-outs.
To understand "the Inductor" you need to make a simple circuit that you can adjust and change the physical properties of the inductor.
The following circuit is a perfect example for experimenting. It uses a single 1.5v cell to illuminate a white LED. We know a white LED requires at least 3.2v for it to illuminate, so the circuit is "magically" increasing the 1.5v to a higher voltage.
The coil (the two coils) is actually a transformer and it is acting in FLYBACK MODE.
It has no core (just air) and you can separate the turns and see what effect it has on the operation.
This bike flasher uses a single transistor to flash two white LEDs from a single cell. And it has no core for the transformer - just AIR!
All Joule Thief circuits you have seen, use a ferrite rod or toroid (doughnut) core and the turns are wound on the ferrite material. But this circuit proves the collapsing magnetic flux produces an increased voltage, even when the core is AIR. The fact is this: When a magnetic filed collapses quickly, it produces a higher voltage in the opposite direction and in this case the magnetic field surrounding the coil is sufficient to produce the energy we need.
Wind 30 turns on 10mm (1/2" dia) pen or screwdriver and then another 30 turns on top. Build the first circuit and connect the wires. You can use 1 or two LEDs. If the circuit does not work, swap the wires going to the base.
Now add the 10u electrolytic and 100k resistor (remove the 1k5). The circuit will now flash. You must use 2 LEDs for the flashing circuit.
BIKE FLASHER - AMAZING!
THE IMPROVED BIKE FLASHER CIRCUIT
The original 30 turns + 30 turns coil is
shown on the right. The circuit took 20mA to illuminate two LEDs.The secret to getting the maximum energy from the coil (to flash the LEDs) is the maximum amount of air in the centre of the coil. Air cannot transfer a high magnetic flux so we provide a large area (volume) of low flux to provide the energy. The larger (20mm) coil reduced the current from 20mA to 11mA for the same brightness. This could be improved further but the coil gets too big. The two 30-turn windings must be kept together because the flux from the main winding must cut the feedback winding to turn ON the transistor HARD.
When the transistor starts to turn on via the 100k, it creates magnetic flux in the main winding that cuts the feedback winding and a positive voltage comes out the end connected to the base and a negative voltage comes out the end connected to the 100k and 10u. This turns the transistor ON more and it continues to turn ON until fully turned ON. At this point the magnetic flux is not expanding and the voltage does not appear in the feedback winding.
During this time the 10u has charged and the voltage on the negative lead has dropped to a lower voltage than before. This effectively turns off the transistor and the current in the main winding ceases abruptly. The magnetic flux collapses and produces a voltage in the opposite direction that is higher than the supply and this is why the two LEDs illuminate. This also puts a voltage through the feedback winding that keeps the transistor OFF. When the magnetic flux has collapsed, the voltage on the negative lead of the 10u is so low that the transistor does not turn on. The 100k discharges the 10u and the voltage on the base rises to start the next cycle.
You can see the 100k and 1k5 resistors and all the other parts in a "birds nest" to allow easy experimenting.
Note: Changing the turns to 40t for the main winding and 30t for the feedback (keeping the turns tightly wound together by winding wire around them) reduced the current to 8-9mA.
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