October 1935 Short Wave Craft
Wax nostalgic about and learn from the history of early electronics. See articles
from Short Wave Craft,
published 1930 - 1936. All copyrights hereby acknowledged.
A while back I was using
the familiar analogy that relates water pressure, hose diameter, and flow rate to
electrical voltage, resistance, and current, respectively†, in an explanation
to my daughter regarding why the water characteristics in her house changed after
the well supply pipe and indoor plumbing changed. The cause, I proposed, was due
to an increased distance between well and house, and the use of the plastic PEX
tubing with a smaller inside diameter than the old copper pipe, respectively. The
submersible pump and holding tank still supply the same 50 psi as before, but
since that pressure now has to force the water through a path inside the house with
more resistance to water flow, the delivery rate to fixtures is now lower. When
I hold the contacts closed on the pump control relay, the most I can get is about
55 psi. Raising the pressure will require replacing the submersible pump, which
is probably a good idea since it is a 115 volt, ½-HP job sitting about 100
feet down in the ground. A 1-HP version that operates on 220 volts will be an easy
swap since it can use the same size electric cable as the existing one (12-2).
I mention all that because this article's author goes to great lengths to create
mechanical analogies based on hydraulic systems and little elfin men throwing electrons
around inside a vacuum tube. It's definitely a unique approach, and the drawings
are pretty good to boot!
See Part 1,
2, and Part 3
Radio Amateur Course: No.2 - How the Vacuum Tube Works
This is the second lesson in the Radio Amateur
Course, which has been especially prepared for the readers of Short Wave Craft.
Future lessons will take up "inductance and capacity," and explain how oscillatory
The entire radio industry as it stands today, owes its success and magnitude
to the electron tube, or vacuum tube, if you prefer; the well-known bulb which is
used in every type of present-day radio. The electron tube is not only used today
for radio, but in other industries and serves a vast number of other purposes.
For instance, with the aid of the photoelectric cell (a special form of vacuum
tube) or electric eye, color measurements are made and it is possible to match colors
perfectly with this instrument, where previously the entire matching of colors was
dependent upon the human eye.
It is the vacuum tubes used in radio, however, which we intend to discuss in
this lesson. The starting point in the construction or analyzing the construction
of the electron tube, is the source of electrons, which is technically termed the
cathode. This cathode is made of a material which when heated gives off a quantity
of electrons. In Fig. 1, we see the filament type cathode, wherein the wire
used for constructing the filament contains a certain amount of material which will
provide (emit) electrons when heated by an electric current passing through it.
If this filament were exposed to the atmosphere and heated it would decompose
or "burn out," as it is commonly termed. However, when enclosed in a glass envelope
from which all air has been exhausted or removed, this filament will glow for a
long time without damage.
Diagrams above-Figs. 1 to 4A, show filament and cathode heater
units; how current flow is opposite to the electron flow (3); rectification of A.C.
passing through an electron tube (4); hook-up of full-wave rectifier tube (4A);
detail of tube elements (4B).
In Fig. 2 we have what is termed an indirectly heated cathode, which consists
of a small tube through the center of which is run the heating wire or resistor.
The outside of this tube is usually coated with some metal oxide. When it is heated
to a sufficient temperature, electrons are then emitted from the outside coating
and it is entirely independent of the heater unit.
As the electrons are emitted from this cathode they form what is termed an "electron
cloud" around the cathode and within the envelope in which it is enclosed. These
electrons can only be attracted to some object which is positively charged. Now,
if we insert in this tube and around the cathode, a piece of metal or some other
conducting material, and charge it positively, we can draw or attract the electrons
In Fig. 3 we show the action which takes place in a tube having a cathode
and a plate or anode, as the plate is technically termed. By connecting a battery
between the anode and cathode with the positive terminals of the battery connected
to the plate, we attract electrons to this plate or anode. Current will then flow
between the anode and cathode, remembering always that the current flow is also
opposite to the electron flow.
If we insert a meter in series with the circuit we will find that it will show
the amount of current flowing in the circuit. This tube, as shown in Fig. 3,
is known as the diode or one having two elements. If we remove the battery from
the circuit and connect the negative side of the battery to the plate and the positive
side to the cathode, no current will flow, because the negatively charged plate
will reject the electrons.
Effect of A.C. on Tube
So far, we have considered a constant polarity of voltage applied between the cathode
and anode. Now, if we were to apply an alternate voltage between these two elements
(see Lesson 1 for explanation of alternating current electricity), the plate will
be alternately charged positive and negative, which means that current will only
flow through the circuit during the period when a positive voltage is applied to
the anode. When the anode side of the circuit becomes negative, current does not
flow. In Fig. 4 we illustrate what is termed rectification.
Simple hydraulic analogy to illustrate how the grid in an electron
tube acts like a valve to regulate or control the amount of current (water) passing
between the plate (motor) and the cathode (pump). The water reservoir in the analog
diagram corresponds to the "B" battery or power supply unit in a radio circuit.
The input circuit is indicated as alternating current while the output circuit
shows current flowing in only one direction during half of the time of the input
cycle. We have flowing in the output circuit then, an interrupted direct current
or what would otherwise be termed half-wave rectification. All tubes of the diode
type are therefore termed half-wave rectifiers. The 281 is an example of this type
By using two anodes we can obtain full-wave rectification. This is shown in Fig. 4A.
A rectifier of this type is termed a full-wave rectifier and an example is the 280
Returning to Fig. 3 we can readily understand that as we change the degree
of positive potential (voltage) applied to the plate, we will change the volume
of electrons which are attracted to it. A low potential will attract a small amount
of electrons, while a high potential or high voltage will attract a greater number
of electrons. An important point to bear in mind is that a negative potential repels
electrons, while a positive potential attracts them. (Unlike charges attract and
How the "Grid" Works
To have a better control over the amount of current flow in the plate circuit
of the vacuum tube, we may insert a third element, known as the grid. Tubes having
three elements are termed triodes, the prefix "tri" meaning three. This grid consists
of a form of screen between the anode and cathode through which electrons must pass
in order to reach the plate.
This grid being located nearer to the cathode or source of electrons, will have
a greater effect upon the electron stream when it is charged either positively or
negatively. In Fig. 5, we have the same circuit as in Fig. 3, excepting
for the addition of the grid. Because of the great effect this grid has upon the
electron flow, it is called the control grid.
Fig. 5 shows action of triode tube; 5A, how A.C. input
is changed into a rectified, pulsating direct current by an electron tube; 6, arrangement
of the elements in a screen-grid tube; how elements are arranged in a pentode at
We may now apply either a positive or a negative potential to this grid and obtain
a change in plate current or a change in the number of electrons reaching the plate,
because if the grid is charged negatively, it will tend to repel or retard the flow
of electrons between the cathode and the plate. This grid can be made so negative
(biased) that it will entirely cut off the flow of electrons, reducing the plate
current to zero.
As this grid becomes more positively, charged, an increase in the flow of electrons
to the plate will take place. That is, providing the potential (voltage) of the
grid is not as great as that of the plate. As this grid becomes entirely positive,
relative to the cathode, it will then collect a certain amount of electrons from
the stream and return them to the cathode, causing current to flow in the grid circuit.
In receiving circuits the output of the vacuum tube depends upon the plate current
change, that is, the increase and decrease in amplitude or, more simply stated,
the magnitude of the change. So, we can readily see that by using this control grid,
which is located close to the filament, we can effect great changes in the current
flowing in the plate circuit of the vacuum tube with relatively small changes in
the potential of the grid and thus obtain considerable amplification in radio circuits.
The simple analogy above is an attempt to show the action taking
place in the vacuum or electron tube used in radio circuits. Note that the shutters
(corresponding to the grid in the tube) control the number of balls hurled through
it toward the target (or plate). In a similar way, the grid in a vacuum tube controls
the amount of current passing from the plate to the cathode (or filament).
In Fig. 5a we show what happens when A.C. is applied to the input circuit
of a triode, biased (bias usually means applying a fixed negative or positive charge,
independent of the signal voltage, to the grid of the tube) so that the plate current
is of fairly low value, but nowhere near the cut-off point. We show the input signal
to the grid as alternating current, where it rises above and falls below the zero
mark. As the input signal swings the grid more positive, or better stated - less
negative - the plate current begins to rise above what is commonly termed the "no-signal"
(static) plate current value; that is, the normal value of plate current with no
This constitutes one-half of the cycle of the input signals. On the other half
of the input-signal cycle, the grid becomes more negative, causing the plate current
to fall below its normal no-signal value. (See previous explanation under "How the
Grid Works.") Now, in the plate circuit, we have apparently the same wave form as
the input signal. The input signal was A.C.; however, A.C. does not flow in the
plate circuit of the tube. This fluctuating replica of the input signal is termed
the alternating component of the plate current. ("Plate current" is the current
flowing through the circuit from plate to filament, or heater, when the electron
stream is established by heating the filament.)
If we were to connect earphones in series with the plate circuit, we would be
able to hear the incoming signal reproduced and amplified in the plate circuit,
that is if it was of low enough frequency to come within the range of the human
The fluctuating plate current or the alternating component of the plate current
would cause the diaphragm of the earphone to vibrate due to the varying current
flowing through the phones and the change in the magnetic pull on the diaphragm.
So long as the voltage of the incoming signal does not exceed the value of the
bias battery, there will be no grid current flowing, because the grid will never
go completely positive. On the positive half of the input signal the grid, in reality,
becomes just less negative.
If we were to insert a resistor (R) in series with the plate circuit, the fluctuating
current flowing through this resistor would cause a voltage drop across the resistor,
varying directly with the plate current. The ratio of this varying voltage drop
to the input signal voltage, is known as the gain of the tube or the voltage amplification.
Tubes Have Capacity Between Elements
In all types of vacuum tubes, we have in reality a number of small condensers
in that there is a definite electrical capacity, for instance, between the plate
and the grid, between the grid and cathode, and also between the plate and cathode,
for the simple reason that each of these elements can be likened to the plates of
a small condenser (current absorber). The grid to cathode capacitance is termed
the input capacitance. The output capacitance is the capacity between the plate
and cathode. In many very "high-gain" circuits, it is necessary to neutralize the
plate to grid capacity in order that energy will not be fed back from the plate
circuit to the grid circuit.
This can be accomplished either by external methods of neutralizing, which will
be explained in a later lesson, or by inserting a shield or a screen between "the
plate of the tube and the grid. This is commonly termed the screen-grid and tubes
having a control grid and a screen-grid, together with the anode and cathode, are
This screen-grid is so designed that it will effectively shield the plate from
the grid. While the plate to grid capacity of a triode may be as great as 8 mmf.,
the plate to grid capacitance of a screen-grid tube may be reduced to a value as
low as 0.007 mmf. This screen must be constructed so that it will not materially
obstruct" the flow of electrons between the cathode and plate; therefore, it is
made in the form of wire mesh.
It also must not be negatively charged because the flow of electrons would also
be impeded. Therefore, a positive potential is in most cases applied to the screen-grid
in order to accelerate the flow of electrons to the plate. This screen being an
electrostatic shield must be bypassed with a condenser to the cathode in order to
be grounded, in so far as high frequency currents are concerned.
The voltage applied to the screen is usually lower than the plate voltage. The
stream of electrons going to the plate being greatly accelerated by the screen-grid,
may strike the plate at such a terrific speed that they will dislodge other electrons,
which may be attracted to the screen, which is the nearest positively charged element.
This is known as secondary emission and limits the output capabilities of the tube.
This condition can be overcome by inserting between the screen and the plate another
element which will not obstruct the flow of electrons to the plate but prevent them
from returning to the screen.
In order to accomplish this, the third grid or suppressor is usually connected
directly to the cathode in order that electrons dislodged from the plate may continue
back via the suppressor to the cathode.
In some tubes such as the types 34 and 39 this suppressor is connected directly
to the cathode of the tube internally. However, tubes such as types 57 and 58 have
a separate pin on the base for this suppressor grid, in order that in special circuits
a positive or a negative voltage may be applied to it. The values, of course, will
be dependent upon the circuit requirements. In large transmitting tubes of the pentode
type (pentode is a name given to all tubes having 5 elements), this suppressor is
positively charged to the order of 30 or 40 volts.*
Hydraulic analogs showing action of half- and also full-wave
rectifiers, the detector tube in a receiving circuit acting as a rectifier. The
first diagram shows how a single-action pump and a check valve permits water to
pass through the pipe up into the tank on each half stroke, while any counter water
pressure is prevented from passing back into the pump by the check-valve. The second
diagram shows how two half-wave rectifiers (pumps), with the aid of two check-valves
cause a "full-wave" pressure to be developed in the main water line. When one is
not working, the other is.
*Some excellent books covering the electron theory and the operation of electron
"Electrons at Work," by Charles R. Underhill.
"Radio Receiving Tubes," by Moyer & Wostrel. The RCA Tube Manual also contains
a wealth of information covering the operation of various types of vacuum tubes.
"Principles of Radio Communication," Prof. John H. Morecroft.
"Modern Vacuum Tubes and How They Work," by Robert Hertzberg.
† As a side note, a 100-foot-tall column of water in a 1" (i.d.) pipe weighs
x 1200"] x [0.03606 lb/in3] = 34 pounds. Here is a useful paper on
selecting a submersible pump with calculations incorporating depth,
pipe resistance, pump flow rating, etc. Here are a couple articles on the electricity-water
Electrical Quantities, December 1942 Radio-Craft
Posted September 22, 2020
(updated from original post on 4/23/2015)