years have passed since I sat in a college classroom to learn about
transistor fundamentals. The industry had long moved past germanium
transistors and was solidly into silicon. Having been formally introduced
to transistors in the USAF, I was familiar with their functionality
from a technician's perspective of checking for gain, proper bias (as
indicated on "educated" schematics), and determining go-no-go health
by performing a front-to-back resistance measurement using an ohmmeter.
Holes, energy bands, gate widths, and doping levels were first encountered
in solid state physics class, however. This article does a nice job
of introducing the terms and concepts at a layman's level.
|August 1957 Radio & TV News
of Contents]These articles are scanned and OCRed from old editions of the Radio & Television
News magazine. Here is a list of the
Radio & Television News articles
I have already posted. All copyrights
(if any) are hereby acknowledged.
actually found the vacuum tube circuits in our radar unit easier to
troubleshoot than transistor circuits, partially because I had a little
experience with them prior to enlistment and also because the point-to-point
component mounting made it easy to isolate or remove components from
the rest of the circuit. It was rare to destroy a vacuum tube by shorting
out or improperly installing another component in the circuit. Today's
field techs typically swap out circuit board assemblies after the system's
built-in-test (BIT) advises corrective action on a computer monitor.
See all available vintage
Radio News articles.
Northwestern Television and Electronics Institute
For a true understanding of semiconductors,
you must be able "to speak the language". Here is how.
has now ceased to be an experimental device and has become, instead,
a commercial reality. The technician who fails to recognize this fact
and does not prepare himself accordingly, faces a future as limited
as that of an automobile mechanic who does not acquaint himself with
automatic transmissions. In his attempts to read up on transistors,
the technician too often finds himself engulfed in a fog of unfamiliar
terminology. Such terms as injected carriers, intrinsic semiconductor,
trivalent impurity, etc. are from the vocabulary of the semiconductor
physicist and to the average technician are as meaningless as Sanskrit.
It is the purpose of this article to define, in terms familiar to the
technician, the terminology of transistor physics.
In some substances,
the atoms are arranged in neat, orderly geometric patterns, like oranges
in a newly packed crate. These are known as crystalline substances in
order to distinguish them from materials in which the atoms, like grains
of sand on a beach, have no regular pattern of arrangement. Because
of the geometric orientation of their atoms, crystalline substances
have characteristic shapes. A familiar example is the six-sided rod
of quartz in its natural state.
Germanium is a crystalline substance whose electrical resistance is
too great to permit ·its use as a conductor and too low to be used as
an insulator. For this reason, germanium is classified as a semiconductor.
In each atom of germanium, 32 electrons revolve around the nucleus.
These planet-like electrons are located in four orbits or rings. The
outer orbit, known as the valence ring, contains four of the electrons.
In a germanium crystal, the four valence ring electrons of each atom
are associated with the valence ring electrons of adjacent atoms. These
associations or partnerships of outer orbit electrons are known as valence
bonds or covalent bonds. To illustrate the concept of valence bonds
with a purely mechanical analogy, consider a floor made up of hexagonal
tiles as shown in Fig. 1. It is apparent that tiles of this particular
shape will fit together perfectly, and that each tile is associated
with six adjacent tiles. An analogous relationship exists in the atomic
structure of a germanium crystal. As shown in Fig. 1, each outer orbit
electron is associated with an outer orbit electron of an adjacent atom.
Since no outer orbit electron is without a mate, the atoms (like the
tiles) fit together perfectly. The chemist describes this situation
by saying that all of the valence bonds are satisfied. As is common
practice, only the outer orbit or valence electrons are shown in the
drawing of Fig. 1 shown below.
Fig. 1. Hexagonal tiles fit together perfectly. Each tile
is associated with six adjacent tiles. Atoms of germanium fit
together perfectly. The four outer orbit electrons of each atom
are associated with outer orbit electrons of adjacent atoms.
Such associations are called "valence" bonds.
Fig. 2. Since boron has only three valence electrons,
one of the valence bonds is left unsatisfied when an atom of
boron is added to germanium. The "missing" electron creates
a hole in the crystal structure. When arsenic is added to germanium,
each atom contributes a surplus electron.
Consider now the consequence
of replacing one of the tiles of Fig. 1 with a tile having a different
number of sides. It is immediately apparent that such a tile will not
fit. Either it will, overlap adjacent tiles or will leave empty spaces.
These structural defects have analogies in the transistor. If one of
the atoms of Fig. 1 is replaced with an atom having either too many
or too few outer orbit electrons, this impurity atom will not properly
fit into the structure of the crystal. Either there will be an overlap
(extra electron) or an empty spot (hole) in the structure, depending
upon the number of valence electrons in the impurity atom. Under these
conditions, all of the outer orbit electrons do not have mates. In the
language of the chemist, all of the valence bonds are not satisfied.
In transistor physics, such structural imperfections are known as lattice
defects and are intentionally created by introducing impurity atoms
into the semiconductor material. By definition, an impurity atom is
one having either more or less valence electrons than the atoms of the
semiconductor to which it is added.
When the chemical impurity
added to a semiconductor material has fewer valence electrons than the
atoms of the semiconductor, the impurity is known as an acceptor. For
example, boron is an acceptor when added to germanium because it has
only three outer orbit electrons as compared to four for germanium.
As a consequence, each boron atom will rob or accept a valence electron
from an atom of germanium. The site formerly occupied by the stolen
electron is known as a hole. Because it is the consequence of a missing
electron, the hole possesses the properties of a positively charged
particle. This condition is shown schematically in Fig. 2. Since its
atoms contain three valence electrons, boron is known as a trivalent
impurity. Indium, gallium, and aluminum are also trivalent and therefore
are acceptors with respect to germanium. Germanium to which acceptor
impurities have been added is characterized by an abundance of holes
and is therefore known as positive or p-type germanium.
the chemical impurity added to the semiconductor material has more valence
electrons than the atoms of the semiconductor, the impurity is known
as a donor. For example, arsenic is a donor when added to germanium
because it has five outer orbit electrons as compared to four for germanium.
As a result, each arsenic atom provides one extra electron which is
not in valence bond and therefore free to act as a current carrier.
This condition is shown schematically in Fig. 2. Since its atoms contain
five valence electrons, arsenic is known as a pentavalent impurity.
Germanium, to which donor impurities have been added, is characterized
by an abundance of electrons and is therefore known as negative or n-type
Since its atoms contain four valence electrons, germanium
is known as a tetravalent element. When the germanium is pure or when
it contains equal amounts of donor and acceptor impurities, it is referred
to as intrinsic germanium.
A junction diode is made up of n-type
and p-type germanium as shown in Fig. 3. When the negative terminal
of a battery is connected to the n-type (electron-rich) layer of the
junction, and the positive terminal is connected to the p-type (hole-rich)
layer, the diode is biased in the forward direction. Under these conditions,
the electrons in the n-type layer are repelled by the negative terminal
of the battery and move toward the junction. At the same time, the holes
in the p-type layer are repelled by the positive terminal of the battery
and also move toward the junction. At the junction, the electrons and
the holes effectively neutralize each other and permit current flow.
This represents the low resistance direction of the junction diode.
When the polarity of the battery is reversed, the electrons in the n-type
layer and the holes in the p-type layer move away from the junction.
Very little current can now flow across the junction because there are
few current carriers in this region. This is referred to as reverse
bias and represents the high resistance direction of the junction diode.
The junction transistor consists of two back-to-back junction
diodes with the center layer (known as the base) participating in both
junctions. The input junction (emitter and base) is biased in the forward
direction, and the output junction (collector and base) is biased in
the reverse direction. The transistor shown in Fig. 3C consists of a
layer of p-type germanium between two layers of n-type germanium. This
is known as an n-p-n transistor. An opposite arrangement is used in
the p-n-p transistor and the battery polarities must be opposite those
shown in Fig. 3C.
In some respects, the emitter of a transistor is comparable to the cathode
of a vacuum tube since both emit or inject the current carriers. In
the transistor, the injected carriers may be either electrons or holes.
In the operation of an n-p-n transistor, a negative potential is applied
to the emitter and electrons are repelled from emitter to base. The
emitter has thus injected carriers into the base region. The emitter
of a p-n-p transistor is made positive with respect to base. Each electron
attracted towards the positive terminal of the battery leaves a hole
at its former location. The hole then captures an electron from an adjacent
atom, creating another hole farther back toward the base. In effect,
the emitter has injected holes into the base region.
Fig. 3. The base-collector junction of the transistor
is biased in the reverse direction, but current flow is increased
by the presence of carriers injected by emitter. Input current
therefore controls output current.
Fig. 4. Resistor R determines the magnitude of the d.c.
bias current. The input signal swings this current around the
operating point, causing related variations in output current.
junction is biased in the reverse direction and the current flow is
therefore relatively small. This current, however, is increased by the
presence of the additional carriers injected by the emitter. When an
input signal is applied to the transistor, it varies the number of carriers
injected into the base region and therefore varies the collector current.
The ratio of the change of collector current to the change of emitter
current (with collector voltage held constant) is known as the alpha
of the transistor. Since it specifies the ratio of the output to input
current, alpha is the current gain of the transistor. Alpha is defined
with respect to the common base circuit, a configuration in which the
base is common to both the input arid the output circuit. The alpha
of a junction transistor is less than unity because some of the carriers
injected by the emitter are neutralized in the base region and therefore
do not reach the collector. For example, some of the electrons injected
by the emitter of an n-p-n transistor are neutralized in the hole-rich
base region. In the p-n-p transistor, the injected carriers are holes,
and some of them are neutralized in the electron-rich base. It is for
this reason that the output current is less than the input current.
The alpha of junction transistors commercially available is in the range
of 0.80 to 0.99. The higher values of alpha (approaching unity) are
obtained when the base layer of the transistor is made very thin. The
injected carriers then pass through the base in less time and fewer
of them are neutralized.
Because the alpha of a transistor is
less than one does not mean that it is incapable of producing voltage
gain. The feature of the transistor that makes voltage gain possible
is the high output resistance as compared to the input resistance. Even
though the output current is slightly less than the input current, it
flows through a higher value of resistance and therefore produces a
signal voltage of greater magnitude than that of the input signal. For
the same reason, the transistor is capable of power gain.
a transistor is connected in a common emitter circuit, the input signal
is applied to the base and the output is taken from the collector. With
this configuration, a current gain greater than unity can be achieved.
This base-to-collector current gain is known as beta, and values of
30 to 40 are common for commercially available transistors, The beta
of a transistor is related to its alpha as follows: beta = alpha/(1
- alpha). From this relationship, it is apparent that the beta of a
transistor becomes greater as its alpha approaches unity.
vacuum tube is a voltage-operated device and bias voltage is used to
establish the desired operating point. The input signal then swings
the grid around this operating point, The transistor, however, is a
current-operated device. A steady d. c. bias current is used to establish
the initial condition and the input signal then swings this current
around the operating point. In the common emitter circuit, the input
signal is applied to the base of the transistor, The steady bias current,
upon which the signal current is superimposed, is known as the base
bias current. In the common emitter circuit shown in Fig. 4A, battery
B1 supplies the base bias
current, and battery B2
is used to bias the collector circuit. Fig. 4B is a circuit arrangement
which uses a single battery for biasing both input and output circuits.
Resistor R determines the magnitude of the base bias current and therefore
establishes the operating point.
The collector of a transistor
is biased in the reverse (high-resistance) direction. Consequently,
current in the collector circuit is relatively small. This current,
however, is increased by the presence of injected carriers and therefore
varies in accordance with the variations of input signal. Even with
the input current reduced to zero, some small amount of current will
flow in the collector circuit. This is known as collector current cut-off.
It is not a true cut-off condition such as can be obtained in a vacuum
tube because the collector draws some current even with reverse bias
and with no injected carriers. The current, however, is sufficiently
small to justify the use of the term cut-off.
The amount of
power that can be dissipated in the collector of a transistor is limited
by the possibility of damage or serious change of characteristics as
a result of overheating. Except for specially designed power transistors,
collector dissipation is usually in the range of 50 to 150 milliwatts.
Numerically, collector dissipation is equal to the product of collector
current and collector voltage. The transistor must be so operated that
this product does not exceed the maximum dissipation rating. For example,
if the maximum collector dissipation of a transistor is 100 milliwatts
and the collector voltage is 25, the collector current must not exceed
4 ma. If the collector voltage is reduced to 20 volts, the permissible
collector current will be 5 ma. Naturally, the operating range of the
transistor should be so limited that at no point will the rated maximums
of collector voltage and collector current be exceeded.
Posted November 27, 2013