
After Class: Alternating Current Principles December 1954 Popular Electronics


December 1954 Popular Electronics
[Table of Contents]People old and young enjoy waxing nostalgic about
and learning some of the history of early electronics. Popular Electronics was published from October 1954 through April 1985. All copyrights (if any) are hereby acknowledged.

Popular Electronics wanted
to be all things to all people as far as electronics hobbyists go. From the very first edition in October of 1954
(2 prior to this one), they included articles on circuit troubleshooting, electrical theory, DIY building
projects, Amateur radio, radio control airplane enthusiasts, and much more. I don't have the first two issues yet,
but I'm guessing that the first or second After Class column covered aspects of direct current (DC), since this
installment covers alternating current (AC).
See all articles from
Popular Electronics.After Class
Alternating Current Principles
An alternating current is one which periodically reverses its direction. This is illustrated in Fig. 1. At A,
when the polarity of the line is as shown, electrons flow through the circuit in the direction indicated by the
arrows. A short time later, the polarity of the power line reverses
FIG. 1
and the direction of current also reverses as shown by the arrows in B of Fig. 1.
Usually the current
changes gradually with time from maximum in one direction to maximum in the other direction. This change can be
represented by a drawing such as shown in Fig. 2. This drawing or graph shows that the current rises from zero at
time L to its peak value at time M. The current then decreases until it reaches zero again at time N. It now
reverses direction and builds up until it reaches its maximum value in the opposite direction at time O. The
current then decreases until it once more drops to zero at time P. The variation of current between time L and
time P is known as one cycle. The
FIG. 2
number of such cycles which occur in one second is known as the frequency. For example, the usual power line
frequency is 60 cyclespersecond; this means that one complete cycle will have a duration of 1/60 second. The
frequencies used in radio and television broadcasting are much higher than the powerline frequency and are
usually specified either in kilocycles (kc.) or megacycles (mc.). A kilocycle is equal to 1000 cycles, and a
megacycle is 1,000,000 cycles.
Since the instantaneous value of an alternating current or voltage varies continually, there must be some
agreedupon way of specifying its value. Actually, there are two commonly used ways of specifying this value: peak
and r.m.s. The peak value is the maximum value reached during the cycle. For example, the 110 volt power line has
a peak value of over 155.5 volts as shown in Fig. 3. The r.m.s. value of a sine wave alternating current or
voltage is equal to .707 times the peak value. The letters r.m.s. stand for rootmeansquare, the name of the
mathematical operation by
FIG. 3
which the factor .707 is derived. The relationship between peak and r.m.s. values may be written':
Example:
What is the r.m.s. value of an alternating current whose peak value is 3 amperes?
Answer: r.m.s. = .707 peak r.m.s. = .707 X 3 r.m.s. = 2.121 amperes
Example:
What is the peak value of an alternating voltage whose r.m.s. value is 10 volts?
Answer:
Unless otherwise stated, alternating voltage or current is specified in r.m.s. values. For example, when we
speak of the 110 volt power line we mean 110 volts r.m.s. Likewise a.c. values given on a circuit diagram are
assumed to be r.m.s. unless otherwise noted. Unless designed for specialized applications, a.c. meters are
calibrated to read r.m.s. values. The r.m.s. value of voltage or current is also called the effective value, since
it gives the number of volts or amperes of d.c. which would produce the same effect, in heating, for example.
Depending upon the components of a circuit, the current and voltage may be either inphase or outofphase. When
they are inphase, current and voltage reach corresponding peaks at the same instant and pass through zero at the
same instant, as shown in Fig. 4A. If the current either leads or lags the voltage, the two are said to be
outofphase. These conditions are illustrated in Figs. 4B and 4C. The amount
FIG. 4
by which current and voltage are outofphase is known as the phase angle and is usually specified in degrees
(one complete cycle = 360°).
Phase angles are often indicated by means of drawings such as those in Fig.
5. Here, arrows instead of sine waves are used to represent the current and voltage. These arrows are known as
vectors, and the drawing itself as a vector diagram. The lengths of the vectors indicate the amounts of voltage
and current. These are often drawn on graph paper where each square represents a certain number of volts or
amperes. Vectors are considered to be pivoted in the center and rotating in a counterclockwise direction. The
three vector diagrams in Fig. 5 present exactly the same information as the three drawings of. Fig. 4. In A,
FIG. 5
the current and voltage are in phase. In B, the current lags the voltage. In C, the current leads.
The
following quiz is intended as a selfcheck. You should be able to answer all of the questions correctly if you
have mastered the foregoing text. The answers appear on page 128.
1. What is the r.m.s. value of a sine
wave having a peak of 300 volts? (a) 425 volts; (b) 212.1 volts; (c) 42.5 volts
2. A frequency of 1500
kc, is equal to: (a) 1.5 mc.; (b) 1.5 cycles; (c) 1,500,000 mc.
3. What is the peak value of a 220
volt r.m.s. power line? (a) 311 volts; (b) 155 volts; (c) 110 volts
4. At a frequency of 400
cyclespersecond, the duration of each cycle is: (a) 400 seconds; (b) .0025 second; (c) 250 seconds
5. If the frequency of an alternating current is increased but its peak value remains the same, its r.m.s,
value will:
(a) increase; (b) decrease; (c) remain the same
VANISHING VOLTS
The odd behavior of a common voltmeter when used to measure the plate potential of an electron tube amplifier is
very mystifying unless one remembers that the meter itself is a part of the circuit being measured. This idea will
be clarified by referring to the schematic diagram of the resistancecapacitance coupled amplifier shown in the
diagram.
If the amplifier is performing properly and this we shall assume  it is fair to anticipate a voltage drop
of perhaps 150 volts in the plate load resistor, R. This would leave 150 volts for the plate. A voltmeter,
connected as shown in the diagram, ought to read this voltage but, surprisingly, it will probably register a great
deal less  possibly as little as 10 or 15 volts. If your reaction to this reading is to conclude that the meter
is delinquent, forget it! You couldn't be wronger!
But the fact remains that the plate voltage has
vanished! Where?
The explanation involves two distinct considerations: first, the ordinary voltmeter generally requires about 1
ma. of current through its coil to make it read full scale; second, this additional current is being drawn through
a relatively high resistance, that of the plate load resistor R.
With the meter disconnected from the
circuit, the voltage drop across R is, as mentioned, about 150 volts. The fall of potential results from the flow
of plate current through the resistor which, of course, is in series with the tube plate circuit. Just as soon as
the meter is connected from plate to ground it, too, draws current to make its needle deflect, producing an
additional voltage drop which may be quite high. On the other hand, the decrease in plate voltage will produce
some decrease in plate current.
For example, let us suppose that our tube is the triode section of a
12SQ7GT, with 1.5 volts grid leak bias. The plate current
will be approximately 0.31 milliampere, the voltage drop across R will be 0.00031 x 500, 000, or 155 volts,
and the platetocathode voltage will be 145 volts. Now suppose we connect a 1000 ohmspervolt meter, set to its
250volt range, between the plate and cathode of the tube. The meter reading would be approximately 94 volts. With
this plate voltage and the same bias as before, the tube would draw only 0.036 milliampere. The meter, which draws
1 milliampere for a fullscale reading of 250 volts, would draw 94/250 or 0.376 milliampere. The total current
through R would be 0.376 plus 0.036, or 0.412 milliampere. The total drop across R is 0.000412 x 500,000, or 206
volts. 300 minus 206 equals 94 volts.
If we set the meter on its 100volt range, the reading would be
approximately 50 volts. With this plate voltage, and bias as before, plate current of the tube would be
practically cut off, and meter current would be 50/100, or 0.50 milliampere, which is enough to account for the
entire 250·volt drop across R. Similarly, on the 50volt range, the reading would be approximately 27 volts, and
on the 25volt range, 14 volts. The lower the range we use, the less the resistance of the meter will be, the more
current will flow through R, and the greater the voltage drop across R will be.
Colloquially, this is
known as "loading down" the circuit. The only way to avoid it is to take all such measurements with a good
vacuumtube voltmeter (v.t.v.m.), an instrument which draws practically no current at all through the plate load.
STARTING FLUORESCENTS
Modern fluorescent lighting tube emits light as a result of the excitation received by its inner, chemical
coating from the ionized gas contained within it. A somewhat unfortunate characteristic of ionization is that the
striking potential required is much greater than the operating potential. Ordinary household fluorescent lighting
fixtures must incorporate a starting scheme which applies a sudden surge of high voltage across the tube, 
voltage which is removed once the arc has been struck.
Two methods for obtaining starting potentials are
now in common use. The first, generally found in desk and floor lamps, is a manual starting system requiring a
spring pushbutton (see diagram A). A ballast coil having a relatively high inductive reactance is in series with
a filament at each end of the tube and with the starting switch. When the switch is closed, current flows through
the series circuit causing the filaments to heat and emit electrons but no arc discharge can occur between them
because the closed switch keeps the potential difference quite low. When the button is released, however, the
usual inductive voltage kickback appears across the tube of sufficiently large magnitude to initiate the
discharge. Once started, the arc continues since the voltage across the tube is in the region of 100 volts. To
extinguish the light, a separate series switch is incorporated in the line to open the circuit.
Ceiling
fixtures use an automatic starting method involving plugin starters. A starter is a rather interesting
combination of glowdischarge tube and a bimetallic element. The latter is made by bonding together two
dissimilar metals having widely different coefficients of expansion; when heated, such an element bends, with the
metal having the lower coefficient on the inside of the curve. In diagram (B), the bimetallic element is shown
straight and upright; application of heat, however, would cause it to bend toward the contact point.
When the unit is switched on, a glow discharge begins in the area indicated in the diagram. The heat from the
discharge is conducted to the bimetallic element, causing it to bend toward the contact point and close the
circuit. Now the filaments heat up since a complete circuit through the filaments has been established through the
ballast coil, but the little glow discharge ceases since the contact between the bimetallic element and the point
has shortcircuited the discharge path. The bent biopening, the same inductive kickback encountered in the
manual case appears to initiate the discharge arc. Once the lamp discharge starts, the voltage across the starter
is not high enough to restrike the glow and it remains out.
Posted
7/25/2011 


