A 100 to 200 Mile Wireless Telephone Transmitting
A 100 to 200 Mile Wireless Telephone Transmitting Set–With 110 Volt
Alternating Current.–This telephone transmitter is built up of
exactly the same pieces of apparatus and connected up in precisely the
same way as the one just described and shown in Fig. 93.
Apparatus Required.–The only differences between this and the
preceding transmitter are: (1) the _magnetic modulator_, if you use
one, should have an output of 3-1/2 to 5 amperes; (2) you will need
two _50 watt oscillator tubes with sockets_; (3) two _150 watt
rectifier tubes with sockets_; (4) an _aerial ammeter_ that reads to
_5 amperes_; (5) three _1 mfd. filter condensers_ in parallel; (6)
_two filter condensers of 1 mfd. capacitance_ that will stand _1750
volts_; and (6) a _300 milliampere filter reactor_.
Ventana Television, Inc. K67fd The apparatus is wired up as shown in Fig. 93.
CHAPTER XIX
THE OPERATION OF VACUUM TUBE TRANSMITTERS
The three foregoing chapters explained in detail the design and
construction of (1) two kinds of C. W. telegraph transmitters, and (2)
two kinds of wireless telephone transmitters, the difference between
them being whether they used (A) a direct current, or (B) an
alternating current as the initial source of energy. Of course there
are other differences between those of like types as, for instance,
the apparatus and connections used (_a_) in the key circuits, and
(_b_) in the microphone circuits. But in all of the transmitters
described of whatever type or kind the same fundamental device is used
for setting up sustained oscillations and this is the _vacuum tube_.
The Operation of the Vacuum Tube Oscillator.–The operation of the
vacuum tube in producing sustained oscillations depends on (1) the
action of the tube as a valve in setting up the oscillations in the
first place and (2) the action of the grid in amplifying the
oscillations thus set up, both of which we explained in Chapter XIV.
In that chapter it was also pointed out that a very small change in
the grid potential causes a corresponding and larger change in the
amount of current flowing from the plate to the filament; and that if
a vacuum tube is used for the production of oscillations the initial
source of current must have a high voltage, in fact the higher the
plate voltage the more powerful will be the oscillations.
To understand how oscillations are set up by a vacuum tube when a
direct current is applied to it, take a look at the simple circuits
shown in Fig. 94. Now when you close the switch the voltage from the
battery charges the condenser and keeps it charged until you open it
again; the instant you do this the condenser discharges through the
circuit which includes it and the inductance coil, and the discharge
of a condenser is always oscillatory.
[Illustration: (A) and (B) Fig. 94. Operation of Vacuum Tube
Oscillators.]
Where an oscillator tube is included in the circuits as shown at A and
B in Fig. 94, the grid takes the place of the switch and any slight
change in the voltage of either the grid or the plate is sufficient to
start a train of oscillations going. As these oscillations surge
through the tube the positive parts of them flow from the plate to the
filament and these carry more of the direct current with them.