Radio Broadcast - 1925, February - 113 Pages ... - VacuumTubeEra
Radio Broadcast - 1925, February - 113 Pages ... - VacuumTubeEra
Radio Broadcast - 1925, February - 113 Pages ... - VacuumTubeEra
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722<br />
<strong>Radio</strong><br />
<strong>Broadcast</strong><br />
fore be wound with wire that will safely carry<br />
this current, and referring to Fig. 7 we find<br />
that this is No. 33.<br />
Multiplying the volts, 300, by the amperes,<br />
.04, will give youthe number of secondary voltamperes.<br />
In a perfect transformer this would<br />
be exactly the volts-amperes inputted to the<br />
primary. However, efficiency must be considered,<br />
and so we multiply this VA rating 12,<br />
by 1.2 the product being close to the volts<br />
times amperes in the primary circuit. Therefore,<br />
primary volts multiplied by primary<br />
amperes equals 14.4, or *&<br />
is the number<br />
of amperes flowing in the primary under full<br />
load. The primary current then is .122.<br />
Again referring to the table we find that the<br />
correct primary wire is about No. 28.<br />
In all cases, of course, a larger size wire may<br />
be used for convenience or other reasons.<br />
LABORATORY HINTS<br />
EDISON element storage B batteries can be<br />
charged at comparatively high charging<br />
rates without harm. Most B battery chargers<br />
using electric light bulbs as a series resistance<br />
only charge at a rate of about 75 to 100 milliamperes,<br />
which is quite correct for the majority<br />
of lead plate cells. However, on Edison cells<br />
this rate may be considerably increased by the<br />
substitution of a soldering iron or an electric<br />
iron for the lamp. Fig. 8 shows a commercial<br />
type of charger the "Unitron" an efficient<br />
bulb rectifier for charging both A and B batteries<br />
without the purchase of additional apparatus,<br />
charging a Todd B battery through a<br />
COIL<br />
FLEXIBLE-''<br />
CORD<br />
FIG. 9<br />
A half inch of spaghetti keeps the silk from fraying<br />
standard 500 watt electric iron. The complete<br />
battery is charged as a forty-five volt<br />
unit at close to a one-half ampere rate. Three<br />
hours running completely charges the battery,<br />
and after six months of repeated charging no<br />
ill effects of the comparatively high rate can<br />
be observed. If anything, the battery is in<br />
better condition than when originally obtained.<br />
CIGURE 9 shows a wiring kink that<br />
r solves<br />
in a neat and efficient manner the tendency<br />
of flexible cables to fray at the ends.<br />
Flexible wires, generally of the ordinary lamp<br />
cord type, are indispensable to the wiring of<br />
most receivers employing variable coupling,<br />
such as the Roberts. Moving coils are connected<br />
to the stationary bus-bars by means of<br />
these leads. If a small piece a half inch or<br />
so of spaghetti tubing<br />
is slipped over the<br />
ends of the flexible cables, forming a "cuff," a<br />
permanently neat job is assured.<br />
FIG. 8<br />
A flat iron can be substituted for the usual carbon lamp when high charging<br />
rates are desired. An electric toaster will pass approximately the same current