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Friday, October 30, 2009

PN Junction

A PN junction is made from a single piece of semiconductor that is made to have two differing areas. One end is made to be P-type and the other N-type. This means that both ends of the PN-junction have different properties. One end has an excess of electrons whilst the other has an excess of holes. Where the two areas meet the electrons fill the holes and there are no free holes or electrons. This means that there are no available charge carries in this region. In view of the fact that this area is depleted of charge carriers it is known as the depletion region.

PN junction with no bias applied

The semiconductor diode PN junction with no bias applied

The depletion region is very thin - often only few thousandths of a millimetre - but this is enough to prevent current flowing in the normal way. However it is found that different effects are noticed dependent upon the way in which the voltage is applied to the junction.

PN junction with forward bias applied

The semiconductor diode PN junction with forward bias

  • Current Flow - If the voltage is applied such that the P type area becomes positive and the N type becomes negative, holes are attracted towards the negative voltage and are assisted to jump across the depletion layer. Similarly electrons move towards the positive voltage and jump the depletion layer. Even though the holes and electrons are moving in opposite directions, they carry opposite charges and as a result they represent a current flow in the same direction.

  • No current flow - If the voltage is applied to the PN junction in the opposite sense no current flows. The reason for this is that the holes are attracted towards the negative potential that is applied to the P type region. Similarly the electrons are attracted towards the positive potential which is applied to the N type region. In other words the holes and electrons are attracted away from the junction itself and the depletion region increases in width. Accordingly no current flows across the PN junction.

PN junction with reverse bias

The semiconductor diode PN junction with reverse bias

How a PN Junction Diode Works

summary of the basics or a tutorial of how a PN junction or diode works showing how does the current flow in only one direction, and how diodes can be used on their own and in transistors


Before reading this page, it is worth reading the page entitled "What is a semiconductor" - see the related articles list below the left menu. This will explain some of the basics of semiconductors and some of the terms used on this page.

The PN junction is one of the most important structures in today's electronics scene. It forms the basis of today's semiconductor technology, and was the first semiconductor device to be used. The first semiconductor diode to be used was the Cat's Whisker wireless detector used in early wireless sets. It consisted of a wire placed onto a material that was effectively a semiconductor. The point where the wire met the semiconductor then formed a small PN junction and this detected the radio signals.

The diode or PN junction was the first form of semiconductor device to be investigated in the early 1940s when the first real research was undertaken into semiconductor technology. It was found that small point contact diodes were able to rectify some of the microwave frequencies used in early radar systems and as a result they soon found many uses.

Today, the PN junction has undergone a significant amount of development. Many varieties of diode are in use in a variety of applications. In addition to this, the PN junction forms the basis of much of today's semiconductor technology where it is used in transistors, FETs, and many types of integrated circuit.

The PN junction is found in many semiconductor devices today. These include:

  • Diode

  • Bipolar transistor

  • Junction FET

  • Diac

  • Triac

The PN junction has the very useful property that electrons are only able to flow in one direction. As current consists of a flow of electrons

Conductors and Non-Conductors

Conductors and Non-Conductors

An electric current occurs when there is a flow of electrons in a certain direction. As electrons have a negative charge, their movement means that charge is flowing from one point to another and this is what an electric current is.

To enable the current to flow the electrons must be able to move freely within the material. In some materials electrons are moving freely around the lattice, although the number of electrons and the available spaces for them balances out so the material itself does not carry a charge. In these materials the electrons are moving freely but randomly. By placing a potential difference across the conductor the electrons can be made to drift in one direction and this constitutes an electric current. Many materials are able to conduct electricity, but metals form the most common examples.

Unlike metals, there are many other materials in which all the electrons are firmly bound to their parent molecules and they are not free to move. Accordingly when a potential is placed across the substance very few electrons will be able to move and very little or no current will flow. These substances are called non-conductors or insulators. They include most plastics, ceramics and many naturally occurring substances like wood.


Semiconductors

Semiconductors do not fall into either the conductor or non-conductor categories. Instead they fall in between. A variety of materials fall into this category, and they include silicon, germanium, gallium arsenide, and a variety of other substances.

In its pure state silicon is an insulator with no free electrons in the crystal lattice. However to understand how it acts as a semiconductor first look at the atomic structure of silicon in its pure state. Each molecule in the crystal lattice consists of a nucleus with three rings or orbits containing electrons, and each electron has a negative charge. The nucleus consists of neutrons that are neutral and have no charge, and protons that have a positive charge. In the atom there are the same number of protons and electrons so the whole atom has no overall charge.

The electrons in the silicon, as in any other element are arranged in rings with strict numbers of electrons in each orbit. The first ring can only contain two, and the second has eight. The third and outer ring of the silicon has four. The electrons in the outer shell are shared with those from adjacent atoms to make up a crystal lattice. When this happens there are no free electrons in the lattice, making silicon a good insulator. A similar picture can be seen for germanium. It has two electrons in the inner most orbit, eight in the next, 18 in the third, and four in the outer one. Again it shares its electrons with those from adjacent atoms to make a crystal lattice without any free electrons.


Impurities

In order to make silicon or any other semiconductor into a partially conducting material it is necessary to add a very small amount of impurity into the material. This considerably changes the properties.

If traces of impurities of materials having five electrons in the outer ring of their atoms are added they enter the crystal lattice sharing electrons with the silicon. However as they have one extra electron in the outer ring, one electron becomes free to move around the lattice. This enables a current to flow if a potential is applied across the material. As this type of material has a surplus of electrons in the lattice it is known as an N-type semiconductor. Typical impurities that are often used to create N-type semiconductors are phosphorous and arsenic.

It is also possible to place elements with only three electrons in their outer shell into the crystal lattice. When this happens the silicon wants to share its four electrons with another atom with four atoms. However as the impurity only has three, there is a space or a hole for another electron. As this type of material has electrons missing it is known as P-type material. Typical impurities used for P-type material are boron, and aluminium.


Holes

It is easy to see how electrons can move around the lattice and carry a current. However it is not quite so obvious for holes. This happens when an electron from a complete orbit moves to fill a hole, leaving a hole where it came from. Another electron from another orbit can then move in to fill the new hole and so forth. The movement of the holes in one direction corresponds to a movement of electrons in the other, hence an electric current.

From this it can be seen that either electrons or holes can carry charge or an electric current. As a result, they are known as charge carriers, holes being the charge carriers for a P-type semiconductor and electrons for an N-type semiconductor.

Semiconductors basics

Semiconductors basics


what semiconductors are and the way in which current is able to flow in them

Semiconductors and semiconductor technology forms the basis of most of the electronics industry these days. Transistors, diodes, integrated circuits and many more devices all have semiconductor technology in common. As a result of the enormous degree of flexibility that semiconductor technology provides, it has enabled electronics to take over many areas of daily life, that fifty years ago could not have been conceived.

The first step in looking at semiconductor technology is to see what types of material there are in terms of their electrical properties. Basically there are three types:

  • Conductors

  • Non-conductors

  • Semiconductors

In order to understand what semiconductors are and why they are a distinct group on their own, it is necessary to look first at why some materials conduct electricity (conductors) and why others do not (non-conductors).

Types of diode

There is a host of different types of diode that are manufactured and used in today's electronics. Each type has different properties and this makes them suitable for different applications or jobs.

  • Cat's whisker: As already mentioned, this type of diode was the earliest type to gain widespread acceptance. It consisted of a small wire placed on a piece of mineral crystal. This created a small point contact diode, which although unreliable was sufficiently good to enable radio transmissions to be heard when used in a "crystal set."

  • Laser diode: This type of diode is different to the ordinary light emitting diode in that it produces laser (coherent) light. They are used in many applications including CD and DVD drives. Although much cheaper than other forms of laser generators, these diodes are more expensive than ordinary LEDs.

  • Light emitting diodes: The light emitting diode or LED is one of the most popular types of diode. When forward biased with current flowing through the junction, light is produced. The diodes use component semiconductors, and can produce a variety of colours, although the original colour was red.

  • Photodiode: When light strikes a PN junction it can create electrons and holes, causing a current to flow. As a result it is possible to use semiconductors to detect light. These types of diodes can also be used to generate electricity. For some applications, PIN diodes work very well as photodetectors.

  • PIN diode: This diode type has areas of P-type and N-type silicon, but between them there is an area of intrinsic semiconductor (i.e. no doping). This increases the size of what is termed the depletion region. This type of diode is used in a number of applications including radio frequency switches and as photodiodes.

  • Point contact diode: This type of diode performs in the same way as a simple PN junction diode, but the construction is much easier. They consist of a piece of n-type semiconductor, onto which a sharp point of a specific type of metal wire (group III metal for chemists) is placed. Some of the metal migrates into the semiconductor and produces a PN junction. These diodes have a very low level of capacitance and are ideal for many radio frequency (RF) applications. They also have the advantage that they are very cheap to manufacture, although their performance is not particularly repeatable.

  • PN Junction: The standard PN junction may be thought of as the normal or standard type of diode in use today. These diodes can come as small signal types for use in radio frequency, or other low current applications, or other types may be high current and high voltage ones that can be used for power applications.

  • Schottky diodes: This type of diode has a lower forward voltage drop than ordinary silicon PN junction diodes. At low currents the drop may be somewhere between 0.15 and 0.4 volts as opposed to 0.6 volts for a silicon diode. To achieve this performance they are constructed in a different way to normal diodes having a metal to semiconductor contact. They are widely used as clamping diodes, and in RF applicat

Friday, October 16, 2009

Varicap or varactor diode

Varactor or varicap diodes are used mainly in radio frequency (RF) circuits to be able to provide a capacitance that can be varied by changing a voltage in an electronics circuit. This can be used for tuning circuits including radio frequency oscillators and filters.

Although both names: varactor and varicap diode are used, they are both the same form of diode. The name varactor meaning variable reactor, or reactance, and varicap meaning variable capacitance (vari-cap).


Operation of a variable capacitor

They key to understanding how a varactor or varicap diode works is to look at what a capacitor is and what can change the capacitance. As can be seen from the diagram below, a capacitor consists of two plates with an insulating dielectric between them

... the capacitance and the amount of charge that can be stored depends on the area of the plates and the distance between them....

Basic concept of a capacitor

.

... the capacitance and the amount of charge that can be stored depends on the area of the plates and the distance between them....

Basic concept of a capacitor

The capacitance of the capacitor is dependent upon the area of the plates - the larger the area the greater the capacitance, and also the distance between them - the greater the distance the smaller the level of capacitance.

A reverse biased diode has no current flowing between the P-type area and the N-type area. The N-type region and the P-type regions can conduct electricity, and can be considered to be the two plates, and the region between them - the depletion region is the insulating dielectric. This is exactly the same as the capacitor above.

As with any diode, if the reverse bias is changed so does the size of the depletion region. If the reverse voltage on the varactor or varicap diode is increased, the depletion region of the diode increases and if the reverse voltage on varactor diode is decreased the depletion region narrows. Therefore by changing the reverse bias on the diode it is possible to change the capacitance.


Change of varactor diode capacitance with reverse bias


Varactor or varicap circuit symbol

The varactor diode or varicap diode is shown in circuit diagrams or schematics using a symbol that combines the diode and capacitor symbols. In this way it is obvious that it is being used as a varacor or varicap capacitor rather than a rectifying diode.


Circuit symbol for a varactor diode / varicap diode

When operated in a circuit, it is necessary to ensure the varactor diode remains reverse biased. This means that the cathode will be positive with respect to the anode, i.e. the cathode of the varactor will be more positive than the anode.


Varactor circuits

It is impossible to show all the circuits in which varactor / varicap diodes may be used. However it is worth providing one example to show how these diodes may be used in a typical circuit. Effectively a capacitor is replaced with the varactor diode, but it is necessary to also ensure that the tune voltage, i.e. the voltage used to set the capacitance of the diode can be inserted into the circuit, and that no voltages such as bias voltages from the circuit itself can affect the varactor diode.


Voltage controlled oscillator using a varactor diode

Within this circuit D1 is the varactor diode that is used to enable the oscillator to be tuned. C1 prevents the reverse bias for the varactor or varicap diode being shorted to ground through the inductor, and R1 is a series isolating resistor through which the varactor diode tuning voltage or bias is applied.


Specifications

The most important characteristics of the diode are its capacitance and the range of capacitance that can be achieved. Normally two voltage points are specified, one at the top of the range and the other near the bottom at the minimum useable voltage. It is obviously important to select a diode which combines the correct capacitance range for the available tuning voltage range. The higher voltage specified is normally the maximum reverse bias and this should not be exceeded otherwise breakdown may occur.

Diodes typically operate with reverse bias ranging from around a couple of volts up to 20 volts and higher. Some may even operate up to as much as 60 volts, although at the top end of the range comparatively little change in capacitance is seen.

Some varactor circuits can use quite high voltages. With voltages of 60 volts

What is a Zener Diode

Zener diode basics

Zener diodes are sometimes referred to as reference diodes as they are able to provide a stable reference voltage for many electronics circuits. The diodes themselves are cheap and plentiful and can be purchased in virtually every electronics components store.

Zener diodes have many of the same basic properties of ordinary semiconductor diodes. They conduct in the forward direction and have the same turn on voltage as ordinary diodes. For silicon this is about 0.6 volts.

In the reverse direction, the operation of a Zener diode is quite different to an ordinary diode. For low voltages the diodes do not conduct as would be expected. However, once a certain voltage is reached the diode "breaks down" and current flows. Looking at the curves for a Zener diode, it can be seen that the voltage is almost constant regardless of the current carried. This means that a Zener diode provides a stable and known reference voltage.


Zener diode markings

There are many styles of package for a Zener diode. Some are used for high levels of power dissipation and others are contained within surface mount formats. For home construction, the most common type is contained within a small glass encapsulation. It has a band around one end and this marks the cathode.

It can be seen that the band around the package corresponds to the line on the diode circuit symbol and this can be an easy way of remembering which end is which. For a Zener diode operating in its reverse bias condition the band is the more positive terminal in the circuit.

Zener diode markings, symbol and package outlines

Zener diode markings, symbol and package outlines


How a Zener diode works

The Zener diode is particularly interesting in the way that it operates. There are actually two mechanisms that can cause the breakdown effect that is used to provide the voltage reference effect:

  1. Zener breakdown: Although the physics behind the effect is quite complicated, it can be considered that this effect occurs when the electric field within the semiconductor crystal lattice is sufficiently high to pull electrons out of the lattice to create a hole and electron. The electron then moves under the influence of the field to provide an electric current.

  2. Impaction ionisation: Again this effect occurs when there is a high level of electric field. Electrons are strongly attracted and move towards the positive potential. In view of the high electric field their velocity increases, and often these high energy electrons will collide with the semiconductor lattice. When this occurs an electron may be released, leaving a hole. This newly freed electron then moves towards the positive voltage and is accelerated under the high electric field, and it to may collide with the lattice. The hole, being positively charged moves in the opposite direction to the electron. If the field is sufficiently strong sufficient numbers of collisions occur so that an effect known as avalanche breakdown occurs. This happens only when a specific field is exceeded, i.e. when a certain reverse voltage is exceeded for that diode, making it conduct in the reverse direction for a given voltage, just what is required for a voltage reference diode.

It is found that of the two effects the Zener effect predominates above about 5.5 volts whereas impact ionisation is the major effect below this voltage.

The two effects are affected by temperature variations. This means that the Zener diode voltage may vary as the temperature changes. It is found that the impact ionisation and Zener effects have temperature coefficient in opposite directions. As a result Zener diodes with reverse voltages of around 5.5 volts where the two effects occur almost equally have the most stable overall temperature coefficient as they tend to balance each other out for the optimum performance.


Zener diode circuits

The most basic Zener diode circuit consist of a single Zener diode and a resistor. The Zener diode provides the reference voltage, but a series resistor must be in place to limit the current into the diode otherwise a large amount of current would flow through it and it could be destroyed.

The value of the resistor should be calculated to give the required value of current for the supply voltage used. Typically most low power leaded Zener diodes have a maximum power dissipation of 400 mW. Ideally the circuit should be designed to dissipate less than about half this value, but to operate correctly the current into the Zener diode should not fall below about 5 mA or they do not regulate correctly.


Basic Zener diode circuit

Basic Zener diode circuit


Design example

Take the case where a Zener diode is used to supply a regulated 5.1 Volt rail consuming 2 mA, from an input voltage supply of 12 volts. The following easy steps can be used to calculate the resistor required:

  1. Calculate the difference in voltage across the series resistor

    12 - 5.1 = 6.9 volts


  2. Determine the resistor current. Choose this to be 15 mA. This will allow sufficient margin above the minimum Zener diode current for some variation in the load current.

  3. Check the Zener diode power dissipation. At a current of 15 mA and a voltage across the power dissipation is:

    15 mA x 5.1 volts = 76.5 mW


    This is nicely within the maximum limit for the diode

  4. Determine the current through the series resistor. This is 15 mA for the Zener diode plus 2 mA for the load, i.e. 17 mA.

  5. Determine the value of the series resistor. Using Ohms law this can be calculated from the voltage drop across it and the total current through it:

    6.9 / 17 mA = 0.405 kohm


    The nearest value is 390 ohms

  6. Determine the wattage of the series resistor. This can be determined using the value for the current through the resistor and the voltage across it calculated earlier:

    V x I = 6.9V x 17mA = 117mW


    The resistor needs to be able to dissipate this level of heat. A quarter watt resistor should be adequate for this.

Basics of how does a transistor work

Basics of how does a transistor work


Short transistor history

Semiconductor technology is now well established but it has been used for over a hundred years. The first semiconductor effects were noticed back in the early 1900s when the first wireless or radio sets were being used. Various ideas were being investigated as detectors. Thermionic valve or vacuum tube technology was introduced in 1904, but these devices were expensive, and also required powering by a battery. Soon afterwards the Cat's Whisker detector was discovered. This consisted of a thin wire placed onto one of a number of types of material. Today we know these were all semiconductors. As a result these created the first diodes.

Other semiconductor effects were also discovered. In 1908 H J Round investigating Cat's Whisker diodes discovered that when a current was passed through a detector using a particular material, light was emitted. He reported the fact in a magazine of the day, but little was done.

During the 1920s and 1930s much of the work undertaken into electronics devices was focussed on thermionic valve or vacuum tube technology. However there was also some original work being undertaken into particle physics. Although not directed towards electronics technology, this was to provide the foundations upon which semiconductor technology would be built.

With the development of radar in World War II, there was a growing need for high performance microwave components. Detectors were a particular need. It was soon realised that developments of what was effectively a cat's Whisker performed well at these frequencies, and using the early work done into semiconductor physics, these diodes were developed further as point contact diodes.

After the war, much research continued. In particular Bell Labs in the USA invested heavily, and one of their groups with three engineers, Bardeen, Brattain, and Shockley stated to investigate a three terminal device in which the voltage on one terminal would affect the current flow through a semiconductor path - effectively a field effect device. The device did not work and therefore they turned their research towards another idea. We now know this device as the bipolar transistor.

The transistor effect was first observed on 23rd December 1947 at Bell Labs in the USA, and it was then demonstrated to senior management of the company on Christmas Eve. Little did they know what an impact the device would have on the lives of billions of people around the world.

The original idea they were investigating - the field effect transistor had to wait until semiconductor material technology had advanced and allowed the semiconductors to be refined further and processed more accurately before it could be made to work. Nevertheless the foundations that enabled semiconductor had now taken place, enabling semiconductors to become the dominant technology ousting tubes or valves from a place they had occupied for around 50 years.


Basic transistor structure

The transistor is a three terminal device and consists of three distinct layers. Two of them are doped to give one type of semiconductor and the there is the opposite type, i.e. two may be n-type and one p-type, or two may be p-type and one may be n-type.. They are arranged so that the two similar layers of the transistor sandwich the layer of the opposite type. As a result transistor are designated either P-N-P (PNP) types of N-P-N (NPN) types according to the way they are made up.

Transistor diagrammatic structure and circuit symbols

The centre region is called the base and gains its name from the fact that in the very earliest transistors it formed the "base" for the whole structure. The other two connections are called the emitter and collector. These names result from the way in which they either emit or collect the charge carriers. It is also essential that the base region is very thin if the device is to be able to operate. In today's transistors the base may typically be only about 1 mm [micrometre] across. It is the fact that the base region of the transistor is thin that is the key to the operation of the device


Transistor operation

A transistor can be considered as two P-N junctions placed back to back. One of these, namely the base emitter junction is forward biased, whilst the other, the base collector junction is reverse biased. It is found that when a current is made to flow in the base emitter junction a larger current flows in the collector circuit even though the base collector junction is reverse biased.

For clarity the example of an NPN transistor is taken. The same reasoning can be used for a PNP device, except that holes are the majority carriers instead of electrons.

When current flows through the base emitter junction, electrons leave the emitter and flow into the base. However the doping in this region is kept low and there are comparatively few holes available for recombination. As a result most of the electrons are able to flow right through the base region and on into the collector region, attracted by the positive potential.

Transistor structure and circuit symbols

Only a small proportion of the electrons from the emitter combine with holes in the base region giving rise to a current in the base-emitter circuit. This means that the collector current is much higher. The ratio between the collector current and the base current is given the Greek symbol b. For most small signal transistors this may be in the region 50 to 500. In some cases it can be even higher. This means that the collector current is typically between 50 and 500 times that flo

Transistor Specifications Explained

Transistor Specifications Explained


There is a huge number of transistors available which have been designed to fulfil a variety of different applications. In order to define the parameters of a transistor there is a variety of different specifications that are used. These transistor specifications define an aspect of the performance of a transistor.

Transistor manufacturers issue specification sheets for their transistors. These transistor specification sheets may be available on the Internet, or they may be found in transistor manuals issued by the manufacturers over the years. Today, most of the transistor data is available on the manufacturers' Internet sites as paper based data books are expensive to produce and not as easy to disseminate.

When choosing a transistor using the transistor specification or data sheets, it is necessary to be able to understand what the different transistor specifications mean.


Transistor specification parameters

There are a number of standard parameters with abbreviations that are used to define the performance of a transistor. The definitions of these parameters are outlined in the table below:

Term Definition and details
Type number The type number of the device is a unique identifier given to each type of transistor. There are three international schemes that are widely used: European Pro-Electron scheme; US JEDEC (numbers start with 2N for transistors); and the Japanese system (numbers start with 2S). [see the page on Transistor and Diode Numbering Codes].
Case There is a wide variety of case styles. They often start with TOxx for leaded devices or SOTxxx for surface mount devices.
Polarity There are two types of transistor: NPN and PNP. It is important to choose the correct type otherwise all the circuit polarities will be wrong.
Material The two main types of material used for transistors are germanium and silicon. Other materials are used, but in very specialised transistors. A knowledge of the type of material used is important because it affects many properties, e.g. forward bias for the base emitter junction is 0.2 - 0.3 V for germanium and ~0.6 V for silicon.
VCEO Collector to Emitter breakdown voltage. This is the maximum voltage that can be placed from the collector to the emitter. It is normally measured with the base open circuit - hence the letter "0" in the abbreviation. The value should not be exceeded in the operation of the circuit otherwise damage may occur. Note that for circuits using inductors in the collector circuit, the collector voltage may rise to twice the rail voltage.
VCBO Collector to base breakdown voltage. This is the maximum collector base voltage - gain it is generally measured with the emitter left open circuit. This value should not be exceeded in the operation of the circuit.
IC Collector current, normally defined in milliamps, but high power transistors may be quoted in amps. The important parameter is the maximum level of collector current. This figure should not be exceeded otherwise the transistor may be subject to damage.
VCEsat The collector emitter saturation voltage, i.e. the voltage across the transistor (collector to emitter) when the transistor is turned hard on. It is normally quoted for a particular base and collector current values.
Hfe This is the current gain of the transistor. It is effectively the same as b.
FT Frequency Transition - the frequency where current gain falls to unity. The transistor should normally be operated well below this frequency.
Ptot Total power dissipation for the device. It is normally quoted for an ambient external temperature of 25C unless other wise stated. The actual dissipation across the device is the current flowing through the collector multiplied by the voltage across the device

Transistor and diode numbering

Transistor and diode numbering


Semiconductor numbering schemes

There are many different ways of organising a numbering scheme. In the early days of thermionic valve (vacuum tube) manufacture, each manufacturer gave a number to the types they manufactured. In this way there were vast numbers of different numbers for devices many of which were virtually identical. It soon became obvious that a more structured approach was required, so that the same device could be bought regardless of the manufacturer.

The same is true for semiconductor devices, and manufacturer independent numbering schemes are used for both diodes and transistors. In fact there are two main semiconductor numbering schemes in use:

  1. Pro-electron scheme This diode and transistor numbering scheme was originated in Europe and is widely used for transistors developed and manufactured here.


  2. JEDEC scheme This diode and transistor numbering scheme was originated in the USA and it is widely used for diodes and transistors that originate from North America.


Using these diode and transistor numbering schemes it is possible to look at the part number and identify certain properties it will possess and what applications it may be used for. In particular, the Pro-electron diode and transistor numbering scheme makes it possible to broadly identify the capabilities of the transistor. For example parameters such as the transistor being intended for low frequency power, RF, etc can be determined.

The JEDEC semiconductor numbering system details far less, being intended to be purely a numbering system. From the number it can be determined how many PN junctions are in the device.


Pro-Electron Numbering or Coding System

First Letter
Specifies semiconductor material
Second Letter
Specifies type of device
Subsequent Characters
A Germanium
B Silicon
C Gallium Arsenide
R Compound materials
A Diode - low power or signal
B Diode - variable capacitance
C Transistor - audio frequency, low power
D Transistor - audio frequency, power
E Tunnel diode
F Transistor - high frequency, low power
G Miscellaneous devices
H Diode - sensitive to magnetism
L Transistor - high frequency, power
N Photocoupler
P Light detector
Q Light emitter
R Switching device, low power, e.g. thyristor, diac, unijunction
S Transistor - switching low power
T Switching device, low power, e.g. thyristor, triac
U Transistor - switching, power
W Surface acoustic wave device
X Diode multiplier
Y Diode rectifying
Z Diode - voltage reference
The characters following the first two letters form the serial number of the device. Those intended for domestic use have three numbers, but those intended for commercial or industrial use have letter followed by two numbers, i.e. A10 - Z99.

This a BC107 is a low power audio transistor and a BBY10 is variable capacitance diode for industrial or commercial use.


JEDEC Numbering or Coding System

First Number Second LetterSubsequent numbers
1 = Diode

2 = Bipolar transistor

3 = FET
N Serial
number
of
device

Thus a 1N4148 is a diode and a 2N706 is a transistor.

Choosing Transistor Replacements

Choosing Transistor Replacements


When working with electronics equipment, either to design, build or repair it is sometimes necessary to choose a replacement transistor. Either the type of transistor may not be to hand, or it may not be available. Fortunately it is normally possible to use a replacement transistor type as there is often a considerable degree of overlap between the specifications of different types of transistor, and by looking at the basic specifications it is normally possible to choose the correct transistor replacements.

This explanation is focussed on bipolar transistors, but it is possible to apply similar logic to field effect transistors to ensure that suitable replacements can be found.

When looking for suitable transistor replacements it is necessary to look at the main specifications for the transistor. Once the transistor specifications and parameters have been ascertained, it is possible to check for other replacement transistor types with similar parameters that will be able to operate within the circuit in question.

When considering any possible replacement transistors, it is necessary to look at a variety of parameters. These will include the basic parameters of the transistor operation performance. They will also include the environmentally related parameters, and the physical parameters. All these need to be taken into account when choosing a suitable replacement transistor.

JFET - Junction Field Effect Transistor

JFET - Junction Field Effect Transistor


The junction field effect transistor or JFET is widely used in electronics circuits. The junction field effect transistor is a reliable and useful circuit component that can be used very easily in a variety of electronic circuits ranging from JFET amplifiers to JFET switch circuits.

The junction field effect transistor is freely available, and JFETs can be bought for very little money. This makes them ideal for use in many circuits where cost and performance are of interest.


JFET history

The idea of the field effect transistor or FET has been in existence for many years. The idea for this type of device first appeared in a proposal made by Lilienfield in 1926. Later in 1935 the idea re-surfaced in a paper presented by a researcher named Heil.

However it was during the 1940s at Bell Laboratories that real progress towards the field effect transistor or FET was made. At this time they set up a semiconductor research group that investigated a number of areas pertaining to semiconductors, one of which was a device that would modulate the current flowing in a semiconductor channel buy placing an electric field close to it.

Unfortunately the idea for the field effect transistor did not work initially and even after repeated attempts to discover the cause of the problem no progress was made. As a result this failure the group investigating this device turned their sights in other directions and ultimately invented the bipolar transistor in 1948.

After the discovery of the bipolar transistor much of the semiconductor research was focussed on improving this device, and the idea for the field effect transistor was not fully investigated for some years.

One of the main reasons why the idea for the field effect transistor did not work initially was that the materials could not be refined sufficiently. However as work progressed on improving semiconductor materials for the bipolar transistor, this also enabled work to proceed with the field effect transistor. This resulted in the successful implementation of the field effect transistor or FET, and gained widespread acceptance during the 1960s when these devices became more widely available.


Basic JFET structure and circuit symbols

Basically a field effect transistor or FET consists of a section of silicon whose conductance is controlled by an electric field. The section of silicon through which the current flows is called the channel, and it consists of one type of silicon, either N-type or P-type.

The connections at either end of the device are known as the source and drain. The electric field to control the current is applied to a third electrode known as a gate.

Junction field effect transistor circuit symbols

Junction field effect transistor circuit symbol

MOSFET - Metal Oxide Semiconductor Field Effect Transistor

MOSFET - Metal Oxide Semiconductor Field Effect Transistor


Field effect transistors, FETs are widely used in electronics circuits in today's equipment. They provide advantages over other types of transistors in many circuits and applications. As a result they are used in vast quantities, as well as being incorporated into integrated circuits.

There are a number of different types of field effect transistor. The junction field effect transistor or JFET was the first to be developed, but the other major type of FET that is in widespread use today is the MOSFET. The term MOSFET stands for Metal Oxide Semiconductor Field Effect Transistor.


MOSFET development

The concept of the MOSFET has been known for many years but they only became important in mid to late 1960s. In fact when the first bipolar transistor was invented, the researchers had initially been looking at developing field effect devices. Unfortunately they did not work and they could not discover why - it was later discovered that the problem lay in the purity of the semiconductors. However once the bipolar transistor was discovered it took the centre stage in the development arena. Nevertheless developments in processing the raw semiconductor materials enabled the field effect transistor to be developed.

One of the major problems experienced with MOSFETs themselves was associated with the insulating oxide layers and their fabrication. These were only overcome as the semiconductor materials and processing technology improved and in the late 1960s MOSFET technology became more widespread.

Now MOSFET technology is one of the most widely used semiconductor techniques, having become one of the principle elements in integrated circuit technology. Their performance has enabled power consumptions in ICs to be reduced. This has reduced amount of heat being dissipated and enabled the large ICs we take for granted today to become a reality. As a result of this the MOSFET is the most widely used form of transistor in existence today.


MOSFET Basics

Within the MOSFET family of devices there are a number of categories into which the devices can be split. The first categories depends on the type of channel use:

  1. N-channel


  2. P-channel

In the case of the N-channel MOSFET, the major carrier type is electrons, but for the P-channel type the major carrier is holes. Of the two types of device, the N-channel is more commonly used on its own as a discrete device, although both types are widely used in integrated circuits.

There are also two further categories into which the MOSFET family of devices can be split:

  1. Depletion mode MOSFET


  2. Enhancement mode MOSFET

As the name suggests the depletion mode MOSFET acts by depleting or removing the current carriers from the channel, whereas the enhancement type increases the number of carriers according to the gate voltage.

What is a Thyristor, SCR?

What is a Thyristor, SCR?


Thyristors or silicon controlled rectifiers (SCR) as they are sometimes known may appear to be unusual electronics components in many ways, but they are particularly useful for controlling power circuits. As such these electronics components are often used for applications such as light dimmers, and there may be thyristor circuits used in many power supply applications. Thyristors are simple to use and cheap to buy and often thyristor circuits are easy to build and use. All these reasons make thyristors ideal components to consider for many applications.

The idea for the thyristor is not new. The idea for the device was first put forward in 1950 by William Shockley, one of the inventors of the transistor. Although some later investigation of the device was undertaken by others a couple of years later, it was not until the early 1960s when they became available. After the introduction of the thyristor, they soon became popular for power supply circuits.


What is a thyristor?

The thyristor may be considered a rather an unusual form of electronics component because it consists of four layers of differently doped silicon rather than the three layers of the conventional bipolar transistors. Whereas conventional transistors may have a p-n-p or n-p-n structure with the electrodes named collector, base and emitter, the thyristor has a p-n-p-n structure with the outer layers with their electrodes referred to as the anode (n-type) and the cathode (p-type). The control terminal of the SCR is named the gate and it is connected to the p-type layer that adjoins the cathode layer.

Structure of a thyristor or silicon controlled rectifier (SCR)

Structure of a thyristor or silicon controlled rectifier (SCR)

Thyristors are usually manufactured from silicon, although, in theory other types of semiconductor could be used. The first reason for using silicon for thyistors is that silicon is the ideal choice because of its overall properties. It is able to handle the voltage and currents required for high power applications. Additionally it has good thermal properties. The second major reason is that silicon technology is well established and it is widely used for a variety of semiconductor electronics components. As a result it is very cheap and easy for semiconductor manufacturers to use.


How does a thyristor work?

The way in which a thyristor operates is different to other devices. Normally no current flows across the device. However if a supply is connected across the device, and a small amount of current is injected into the gate, then the device will "fire" and conduct. It will remain in the conducting state until the supply is removed.

To see how the thyristor operates, it is worth looking at a thyristor equivalent circuit. For the sake of an explanation, the thyristor circuit can be considered as two back to back transistors. The first transistor with its emitter connected to the cathode of the thyristor is an n-p-n device, whereas a second transistor with its emitter connected to the anode of the thyristor, SCR is a p-n-p variety. The gate is connected to the base of the n-p-n transistor as shown below.

Thyristor equivalent circuit

Thyristor equivalent circuit

When a voltage is applied across a thyristor no current flows because neither transistor is conducting. As a result there is no complete path across the device. If a small current is passed through the gate electrode, this will turn "on" the transistor TR2. When this occurs it will cause the collector of TR2 to fall towards the voltage on the emitter, i.e. the cathode of the whole device. When this occurs it will cause current to flow through the base of TR1 and turn this transistor "on". Again this will now try to pull the voltage on the collector of TR1 towards its emitter voltage. This will cause current to flow in the emitter of TR2, causing its "on" state to be maintained. In this way it only requires a small trigger pulse on the gate to turn the thyristor on. Once switched on, the thyristor can only be turned off by removing the supply voltage.

It can be seen that current will only flow in one direction through the thyristor. If a reverse voltage is applied, then no current will flow, even if some gate current is applied. In this way for thyristor circuits used for AC, operation only occurs over one half of the AC waveform. For the other half of the cycle the device remains inoperative and no current can flow.


Thyristor symbol

The thyristor symbol is easy to recognise. Like the circuit symbols for most electronic components, the symbols may vary slightly dependent upon who has generated them, but in general it is as shown below. The thyristor symbol effectively shows a diode rectifier symbol with a control gate.

Thyristor symbol used in circuit diagrams

Thyristor symbol used in circuit diagrams


Thyristor circuit

There are many thyristor circuits that are in common use. They can be sued in many applications from AC control as in the case of motor or light dimmers to other circuits including power supply crowbar circuits.

The circuit below shows a power supply crowbar circuit. It can be used to protect circuitry within the main equipment from the effects of the failure of the series regulator in a power supply. If the series regulator fails short circuit, then high voltages can be paled on the power rail inside the equipment and this could result in serious damage to the overall equipment.

Thyristor over voltage crowbar circuit

Thyristor overvoltage crowbar circuit

The SCR over voltage crowbar or protection circuit is connected between the output of the power supply and ground. The zener diode voltage is chosen to be slightly above that of the output rail. Typically a 5 volt rail may run with a 6.2 volt zener diode. When the zener diode voltage is reached, current will flow through the zener and trigger the silicon controlled rectifier or thyristor. This will then provide a short circuit to ground, thereby protecting the circuitry that is being supplied form any damage.

What is a Diac?

What is a Diac?


A diac is a full-wave or bi-directional semiconductor switch that can be turned on in both forward and reverse polarities. The name diac comes from the words Diode AC switch. The diac is an electronics component that is widely used to assist even triggering of a triac when used in AC switches and as a result they are often found in light dimmers such as those used in domestic lighting. These electronic components are also widely used in starter circuits for fluorescent lamps.

Although the term is not often seen, they may also be called symmetrical trigger diodes - a term resulting from the symmetry of their characteristic curve.


Diac symbol

The diac symbol used to depict this electronic component in circuit diagrams can be remembered as a combination of what may appear to be two diodes in parallel with each other but connected in opposite directions.

Circuit symbol for the diac

Circuit symbol for the diac

Owing to the fact that diacs are bi-direction devices the terminals cannot be labelled as anode and cathode as they are for a diode. Instead they may be labelled as A1 and A2 or MT1 ("Main Terminal") and MT2.


Diac operation

Diac circuits use the fact that a diac only conducts current only after a certain breakdown voltage has been exceeded. The actual breakdown voltage will depend upon the specification for the particular component type.

When the diac breakdown voltage occurs, the resistance of the component decreases abruptly and this leads to a sharp decrease in the voltage drop across the diac, and a corresponding increase in current. The diac will remain in its conducing state until the current flow through it drops below a particular value known as the holding current. When the current falls below the holding current, the diac switches back to its high resistance, or non-conducting state.

Diacs are widely used in AC applications and it is found that the device is "reset" to its non-conducting state, each time the voltage on the cycle falls so that the current falls below the holding current. As the behaviour of the device is approximately equal in both directions, it can provide a method of providing equal switching for both halves of an AC cycle, e.g for triacs.

Most diacs have a breakdown voltage of around 30 volts, although the exact specifications will depend upon the particular type of device.. Interestingly their behaviour is somewhat similar to that of a neon lamp, although they offer a far more precise switch on voltage and thereby provide a far better degree of switching equalisation.


Diac applications

One of the major uses of diacs within triac circuits. The diac is placed in series with the gate of a triac to provide a more symmetrical switching characteristic. It is found that triacs do not fire symmetrically as a result of slight differences between the two halves of the device. This results in harmonics being generated, and the less symmetrical the device fires, the greater the level of harmonics produced. It is generally undesirable to have high levels of harmonics in a power system.

To help in overcoming this problem, a diac is often placed in series with the gate. This device helps make the switching more even for both halves of the cycle. This results from the fact that the diac switching characteristic is far more even than that of the triac. Since the diac prevents any gate current flowing until the trigger voltage has reached a certain voltage in either direction, this makes the firing point of the triac more even in both directions. In view of their usefulness, diacs may often be built into the gate terminal of a triac.

What is a Triac?

What is a Triac?

riacs are widely used in AC power control applications. They are able to switch high voltages and high levels of current, and over both parts of an AC waveform. This makes triac circuits ideal for use in a variety of applications where power switching is needed. One particular use of triac circuits is in light dimmers for domestic lighting, and they are also used in many other power control situations including motor control.

The triac is a development of the thyristor. While the thyristor can only control current over one half of the cycle, the triac controls it over two halves of an AC waveform. As such the triac can be considered as a pair of parallel but opposite thyristors with the two gates connected together and the anode of one device connected to the cathode of the other, etc..


Triac symbol

The basic triac symbol used on circuit diagram indicates its bi-directional properties. The triac symbol can be seen to be a couple of thyristor symbols in opposite senses merged together.

Triac symbol for use in circuit diagrams

Triac symbol for use in circuit diagrams

Like a thyristor, a triac has three terminals. However the names of these are a little more difficult to assign, because the main current carrying terminals are connected to what is effectively a cathode of one thyristor, and the anode of another within the overall device. There is a gate which acts as a trigger to turn the device on. In addition to this the other terminals are both called Anodes, or Main Terminals These are usually designated Anode 1 and Anode 2 or Main Terminal 1 and Main Terminal 2 (MT1 and MT2). When using triacs it is both MT1 and MT2 have very similar properties.


How does a triac work?

Before looking at how a triac works, it helps to have an understanding of haow a thyristor works. In this way the basic concepts can be grasped for the simpler device and then applied to a triac which is more complicated. The operation of the thyristor is covered in the article in this section and accessible through the "Related Articles" box on the left of the page and below the main menu.

For the operation of the triac, it can be imagined from the circuit symbol that the triac consists of two thyristors in parallel but around different ways. The operation of the triac can be looked on in this fashion, although the actual operation at the semiconductor level is rather more complicated.

Equivalent circuit of a triac

Equivalent circuit of a triac

When the voltage on the MT1 is positive with regard to MT2 and a positive gate voltage is applied, one of the thyristors conducts. When the voltage is reversed and a negative voltage is applied to the gate, the other thyristor conducts. This is provided that there is sufficient voltage across the device to enable a minimum holding current to flow.

Types of Connector

Types of Connector

here is a huge variety of different connector types that can be used in a wide number of different applications. Some connector types may be intended for use where a single connection is required, whereas other connectors may be used where a very large number of connections is required. Other requirements may include elements such as the size of the connector, the intended use, and many other elements. As a result many types of connector are available.

Connector basics and key parameters

As might be expected there is an amount of terminology and specifications associated with connectors. The different connector types as well as the basic formats and the different types of specification.

  • Plugs and sockets One of the basic concepts of connectors is that there are two different formats for connectors. One is the male, or plug, and the other is the mating half that is the socket, receptacle or female section. The male section has pins, and these are often exposed and therefore plugs are never used to supply power. This would mean that when not connected the accessible pins would be live and there would be a significant risk of them becoming shorted. Instead the female connector can supply power. The contacts in the female connector are more protected and therefore it is safer to have power on them while there is no mating connection.


  • Number of pins When choosing any connector type it is necessary to determine how many pins will be required. This may not only determine the actual connector part, but also the series of connector to be used. When choosing a particular connector it is standard practice to ensure there are a few spare pins for any future unforeseen requirements.


  • Number of insertions All connectors have a finite life. It is obvious that they will wear each time they are connected and disconnected. Often the life of a connector is specified in terms of the number of mating cycles, i.e. a connection and disconnection. Some connectors that are intended to enable a piece of equipment to be assembled and then are intended only to be disconnected for service and repair may only have a small number of mating cycles. Others for more general use will have a much larger number. This specification may obviously affect the type of connector chosen for a particular applications.


  • Mechanical considerations There are a number of mechanical considerations when choosing connectors. Physical size and shape is an important factor, but there may also be environmental requirements. Will it operate over a given temperature range, or withstand moisture. These and other mechanical aspects need to be considered when choosing the type of connector.


  • RF and screened connectors Sometimes there are special electrical requirements. One particular case is where the connector requires screening to be contiguous through the connector, or for more exacting requirements where the connector forms part of an RF feeder. In these cases the connector may need to be coaxial in nature, where the two conductors are manufactured so that one surrounds the other. For RF connectors the requirements may be more exacting because the characteristic impedance of the feeder needs to be maintained through the connector.


  • Current capability An important element for any type of connector is its current capability. Some connectors are only designed to carry small currents, whereas others are able to carry much larger levels. Normally it is only necessary to consider higher current levels, as most connectors can take a few milliamps without a problem. However when looking at low current elves it is necessary to ensure that a good quality connector is used. Some low cost varieties may form oxide layers that need a certain level of current to flow to enable a good low resistance contact to be made. If currents of a few milliamps or microamps are to be carried, they may not perform well. Often gold plated contacts may be required for the more exacting applications.

    It is often found that the current carrying capacity of a pin is not quite adequate. One solution that is often used is to use two contacts instead of one. The drawback is that the current may not be shared equally between the two contacts and one may exceed its rating. When adopting this approach it is best to leave a large overall margin to ensure that all pins will operate well within their capability.


  • Voltage capability there is a maximum operating voltage for connectors. Above a certain voltage it is not safe to operate a connector. While virtually all connectors will be suitable for low voltages, when they rise to what may be termed hazardous voltages, care needs to be taken as insulation may fail, or there may be flash over. Accordingly it is always worth ensuring that the maximum voltage is not exceeded. Specifications may be provided for AC and DC.


  • Insertion force When connectors mate, there is a certain level of friction between the contacts. This enables good contact to be made, and the contacts to be cleaned. For many small connectors, this is not a problem. But for many larger connector types with a large number of pins, the force per contact is multiplied by the number of pins used, and this can result in a large amount of force being required to connect and disconnect the connectors. This can be a problem in some instances, and may need to be considered. For some specialist applications where very large numbers of pins are required, what are termed "Zero Insertion Force" (ZIF) connectors may be used. When mating, the female connector does not allow the male pins to contact the female mating pins, thereby considerably reducing the force. A lever on the side of the female connector brings them into contact once the two halves have mated. This reduces the insertion force to a very small value.

The choice of connector can play an important part in the deign of any equipment. Even when using connectors for home applications it is often useful to have a good understanding of their capabilities and an idea of the key specifications for differe

D-type connector

D-type connector

The D-type range of connectors has been in widespread use for many years. They were first developed in 1952 by Cannon which is now part of ITT. The D-type connector has been used in many applications as a multi-way connector, but it is probably most widely known as the connector used for RS-232 serial links. In fact the D-type connector was used for the serial link on most computers for many years, and today variations of D-type connectors are still found on most computers.

The D-type connector was originally termed a sub-miniature connector, and often today the connectors may be referred to as D sub-miniature connectors. Although these connectors were small when they were first introduced, the can no longer be thought of as true sub-miniature connectors.


D-type connector mechanical outline

D-type connectors most commonly consist or two parallel rows of connections. As there is an odd number of pins in each D-type connector, one row has one more pin than the other. This basic construction is used for the more common configurations of connector, namely 9, 15, 25, and 37 way connectors. High pin counts and higher pin densities can be achieved using more rows of pins.

The pins in the D-type connector are surrounded by a metal shield or casement that provides mechanical support and protection and this also provides some degree of electromagnetic shielding that can help reduce radiated interference and pickup levels. This metal surround is broadly in the shape of a D and this gives the connector its name. It also ensures the correct orientation of the plug when mating

The pins in the more common connector types with two rows of pins (e.g. 9, 15, 25 and 37 way) are spaced approximately 0.108 inch (2.74 mm) apart with the rows spaced 0.112 inch (2.84 mm) apart.

IEC power connector

IEC connector

is the common name for the set of thirteen power line connectors. They are defined by the International Electrotechnical Commission (IEC) specification IEC 60320, and these IEC connectors are widely used for the power connections on electrical and electronic equipment.

There is a total of thirteen different types of IEC power connector that are defined. The IEC power connectors include variants with two and three conductors as well as different current variants to enable power to be connected into different types of electrical and electronic equipment.

These power connectors are widely sued for domestic equipment ranging from products including small mains powered radios through computers to items such as electrical kettles and the like. The fact that there is a wide range of IEC connectors means that the same series can be sued for a very wide variety of applications while still having an overall specification to detail the connectors.


Basic IEC power connector types

The main types of IEC power connectors are outlined below:

Connector
designation
Basic
description
Current
capability (A)
Further details
C1 2 conductor 0.2 Non-polarised
C3 2 conductor 2.5
C5 3 conductor 2.5
C7 2 conductor 2.5 Non -polarised although there is also a polarised version.
C9 2 conductor 6 Non-polarised
C11 2 conductor 10
C13 3 conductor 19
C15 3 conductor 10 120 °C maximum temperature
C15A 3 conductor 10 120 °C maximum temperature
C17 2 conductor 16
C19 3 conductor 16
C21 3 conductor 16 155 °C maximum temperature
C23 2 conductor 16

Most common forms of IEC Power Connector


IEC power connector summary

IEC power connectors are now the standard form of power connector used on electronic and electrical equipment. Being a standard format, it is easy to buy ready constructed leads and this makes them very attractive for equipment manufacturers whoa re able to buy off the shelf items very cheaply because the quantities that are manufactured overall. In addition to this the connectors themselves are freely available and low cost. Additionally a wide variety of filtered connectors is available, again at low cost, enabling filtering and other functions to be incorporated using standard components. These and many other advantages mean that IEC power connectors are an ideal choice for many electronics equipment design applications

Jack connectors

Jack connectors

The jack plug and socket are a very common form of connector. They may also be referred to as the phone plug. They have been in use for very many years, being originally designed in the 1878 for use with telephone circuits - they were widely used in telephone switchboards. In view of their long period of service, this makes them the oldest form of electronics connector in regular use today.

The jack, phone, or telephone connectors are able to provide very reliable service, although they are only suitable for low frequency operation and they are not suitable for connections above 20 kHz or so. Accordingly they are widely used for audio applications. Virtually every set of headphones or earpieces will use a jack connector of one size of another. While they may not represent the very latest in connector technology, their use is so embedded in consumer audio, that they are unlikely to be replaced for very many years to come.


Jack connector standards and specifications

Jack connector sizes
There are a number of standard sizes for jack connectors in use these days. They are:

  • 1/4" jack (6.35 mm) or standard jack

  • 3.5mm also known as the miniature jack

  • 2.5mm also known as the subminiature jack

Mono and stereo variants
In addition to the basic size there are other variations to the jack plugs and jack sockets. The main one of that there are variants to cater for mono and also for stereo applications. Mono and stereo variants of jack plugs and sockets are available in all sizes.

The basic mono format was the first to be used. This only required the use of a line or signal connection and an earth or return. Mono jack connectors therefore only possess two connections, the tip and the body. Mono jack connectors were the first types to be designed and manufactured.

With the introduction of stereo in the 1950s and 1960s it became necessary to be able to modify the basic mono jack connector to be able to carry stereo signals. Stereo requires the use of an earth or return as well as one signal line for each of the two stereo channels. Thus a total of three connections are required instead of the two provided by the original "mono" jack connector. The additional connection is accommodated by providing a "ring" between the connection at the tip, and the body or earth connection.

Jack connectors with switches
Many jack sockets incorporate switches so that when the plug is inserted some switch contacts are made or broken. The original requirement for this arose so that when the jack plug was inserted to enable headphones to be used, then the speaker output was disconnected. For switched jack sockets, there is one set of contacts for each channel, i.e. one for a mono socket, and two for a stereo socket.


Standard jack connections

In view of the huge number of these connectors used for applications such as headphones, etc where it is anticipated that they can be plugged in and work, it is essential that a common connection standard is adopted. The connections that are invariably used are given in the table below. By adopting this convention it is possible to plug almost any item using one of these connectors in to a relevant item of equipment and it will work.

Pin Unbalanced Balanced Stereo
Tip Signal Signal +
i.e. 'hot' signal
Left
Ring Not present Signal -
i.e. negative phase
Right
Sleeve Ground / return Ground /shield Ground / shield

XLR connector series

The XLR series of connectors

is widely used for audio and video applications. The XLR connectors provide a rugged series of connectors that can be used for professional as well as semi-professional applications. As an indication of this, XLR connectors are used on most serious audio mixing desks, and on high quality microphones, as well as for many other audio applications.

The XLR series connectors started life as the Cannon X series of connectors. The original versions had no method of retaining the connectors, and later a latch was added to prevent accidental disconnection, and the resultant connector was known as the XL connector. A further medication incorporated the use of a rubber based compound surrounding the contacts, and the designation XLR was given to them.


Standard XLR connections

Pin Signal line
1 Shield
2 Signal +
3 Signal -

RF Coax Connectors

here are a number of commonly available RF connectors that are used with coax cable to provide screened connections. These connectors are used in a number of areas whether to carry RF or radio frequency signals or just to provide a much higher level of screening than would be possible if more ordinary "open" connectors were used.

RF connectors are used in many areas. Naturally their main uses are associated with RF applications. Everything from domestic television, through CB and ham radio to the large number of commercial and industrial applications. However RF or coaxial connectors are also used in areas where screening is one of the major priorities rather than the fundamental RF properties. Coaxial connectors are widely used with a variety of test instruments. For example RF connectors are used on oscilloscopes. These and many other applications all use RF connectors.


RF connector basics

Many connectors, such as the D-type connectors and many other multiway connectors consist of a series of pins with connections in parallel to each other. RF coaxial connectors need to retain the coaxial nature of the cable they are used with. As a result they consist of a central pin for the inner of the coax cable, and then an outer connection around the inner for the outer conductor on the cable. This makes these RF connectors very different to other, more "traditional" connectors.

Coaxial cable has a number of properties, one of which is the characteristic impedance. In order that the maximum power transfer takes place from the source to the load, the characteristic impedances of both should match. Thus the characteristic impedance of a feeder is of great importance. Any mismatch will result in power being reflected back towards the source. It is also important that RF coaxial cable connectors have a characteristic impedance that matches that of the cable. If not, a discontinuity is introduced and losses may result.

There is a variety of connectors that are used for RF applications. Impedance, frequency range, power handling, physical size and a number of other parameters including cost will determine the best type for a given applications.


RF connector types

There is a large host of different types of RF connector. Some are in widespread use whereas others are les widely used. Some of those in widespread use and likely to be encountered in the standard electronics laboratory or by the hobbyist are:

  1. BNC The BNC coax connector is widely used in professional circles being used on most oscilloscopes and many other laboratory instruments. The BNC connector is also widely used as an RF connector, being used on RF test equipment, transmitters, receivers and almost any RF equipment. The BNC connector has a bayonet fixing to prevent accidental disconnection while being easy to disconnect when necessary.

    Electrically the BNC coax cable connector is designed to present a constant impedance and it is most common in its 50 ohm version, although 75 ohm ones can be obtained. It is recommended for operation at frequencies up to 4 GHz and it can be used up to 10 GHz provided the special top quality versions specified to that frequency are used.


  2. N-type The N-type connector is a high performance RF coaxial connector used in many RF applications. The N-type RF connector is larger than the BNC connector and it has a threaded coupling interface to ensure that it mates correctly. It is available in either 50 ohm or 75 ohm versions. These two versions have subtle mechanical differences that do not allow the two types to mate. The connector is able to withstand relatively high powers when compared to the BNC connector. The standard versions are specified for operation up to 11 GHz, although precision versions are available for operation to 18GHz.

BNC Connector

The BNC coax connector is one of the most widely used RF connectors today. It is very easy and convenient to use, and offers a very high level of performance. The BNC connector is used on test equipment for everything from oscilloscopes to audio generators, and power meters to function generators. In fact BNC connectors are used in applications where coaxial or screened cable is required, and particularly for RF applications.

The BNC connector has many attributes. One its chief mechanical attributes is that it uses a bayonet fixing. This is particularly useful because it prevents accidental disconnection if the cable is pulled slightly or repeatedly moved.

The BNC is also what is termed a constant impedance connector. This means that it has the same characteristic impedance across the whole of the connector. Coax cable has what is called a characteristic impedance. Accordingly any RF signals travelling along a coax cable will not see any impedance changes as they pass through the BNC connector. This is particularly important for RF applications as it will result in few reflections and a lower level of loss.


BNC development

The BNC connector was developed in the late 1940s and it gains its name from a combination of the fact that it has a bayonet fixing and from the names of the designers, the letters BNC standing for Bayonet Neill Concelman. In fact the BNC connector is essentially a miniature version of the C connector which was in turn a bayonet version of the N-type connector.

The BNC connector was developed as a result of the need to provide a high quality, robust connector that would be capable of being used in a wide variety of applications. Additionally it needed to be smaller than either the N-type or C-type connectors which were much larger


BNC specifications

The specifications of the BNC connector naturally vary from one manufacturer to another and it is always best to ensure that the particular component being purchased is suitable for the intended application. However there are a number of guidelines that can be used. The connector comes in two basic types:

  • 50 ohm

  • 75 ohm

Of the two versions of the BNC connector, the 50 ohm version is more widely used. Often the BNC connector is specified for operation at frequencies up to 4 GHz and it can be used up to 10 GHz provided the special top quality versions specified to that frequency are used. However it is wise to fully check the specification.

N-type Connector

The N-type connector is a high performance RF coaxial connector. The N-type RF connector is used in many applications, particularly where RF performance is of paramount importance. Although not used as widely in small laboratories and hobbyist applications, the N-type connector is particularly good where high power s and high performance is required. Being physically larger than other types of connector such as the BNC connector, the N-type connector is more suited to use with the larger low loss cables.

... the N-type connector is used in many applications where RF performance is of paramount importance....

N-type RF connector

N-type development

The N-type connector has been in use for many years. It was originally designed by Paul Neill of Bell Laboratories, and it gained its name from the first letter of his surname. Its development arose out of the need for a high performance RF connector with a constant impedance. Since its first introduction, it has found many applications in areas where good RF performance is needed, along with the ability to carry high levels of power, and to be used with the larger sized coaxial cables.


N-type performance

The connector has a threaded coupling interface to ensure that it mates correctly to provide the optimum performance.

There are two versions of the N-type connector that are available:

    • 50 ohm


    • 75 ohm


Of the two versions of this RF connector that are available, it is the 50 ohm N-type connector that is by far the most widely used. This results from the fact that 75 ohm systems are only rarely used in commercial and professional systems these days.

The two versions of the N-type connector have subtle mechanical differences that do not allow the two types to mate. This can be an advantage in preventing the wrong standard connectors being used by mistake.

The connector able to withstand relatively high powers when compared to the BNC or TNC connectors. The standard versions are specified for operation up to 11 GHz, although precision versions are available for operation to 18GHz.

The N-type coaxial connector is used for many radio frequency applications including broadcast and communications equipment where its power handling capability enables it to be used for medium power transmitters, however it is also used for many receivers and general RF applications.


Connector formats

N-type connectors come in a variety of formats. Not only are there plugs and sockets but there are also adapters and also other items such as attenuators.

N-type plugs are designed not only for the required impedance, but also to accept a particular coax cable format. In this way all the internal piece parts are compatible with the coaxial cable used. It is therefore necessary to specify the N-type plug for use the cable to be used. Although there is some latitude, it is naturally best to select the correct cable format.

N-type connectors are often used where performance is of paramount importance, and under these circumstances large cables are often needed to ensure the levels of loss are minimised. In view of the fact that N-type connectors are slightly larger than either BNC or TNC connectors this makes them ideal for these applications. Accordingly a variety of N-type connector versions capable of accommodating larger types of coax cable are available.

In addition to this there are straight and right angled variants. Of these the straight connectors are the most widely used, although right angled connectors where the cable leaves the plug at right angles to the centre of the connector centre line are also available. These are ideal in many applications where the cables need to leave the connector in this manner to ensure cables are in a tidy fashion, or where space is at a premium. Unfortunately right-angled connectors have a marginally higher level of loss than their straight through counterparts. This may not be significant for most applications, but at frequencies near the operational limit of the connector there may be a small difference.

The sockets or female N-type connectors also come in a number of flavours. In view of the fact that TNC connectors are normally used for RF applications, bulkhead mounting connectors where coaxial cable entry is provided are normally used. Again