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T EVIS i - AmericanRadioHistory.Com

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further condenser failures have occurred.<br />

The addition of C, (Fig. 4)<br />

also eliminated a slight genemotor ripple<br />

which was previously apparent on<br />

the carrier.<br />

For the sake of clarity in the circuit<br />

diagram (Fig. 5), several dual condensers<br />

were given widely separated<br />

numbers for their two sections. Obviously<br />

if sections in separate functions<br />

like C, -C.; were called "C, -C:.."<br />

the reader's eye would have to travel<br />

all over the diagram to follow the<br />

parts list. Naturally. when the transmitter<br />

is assembled it will be found<br />

that the connections of the two sections<br />

of any dual unit are adjacent,<br />

or nearly so. Dual units were used<br />

to save badly needed space, although<br />

single units will probably fit fairly<br />

easily in some places.<br />

The antenna changeover relay, RL,,<br />

Fig. 5. is a surplus item. Originally<br />

designed for 12 -volt d.c. operation, it<br />

was rewound for 6 volts. Those contacts<br />

not required for antenna switching<br />

are wired to the octal power plug<br />

P. on the rear of the chassis and<br />

can he used to disable the receiver<br />

whenever the transmitter goes on the<br />

air.<br />

Crystal control may be employed<br />

by plugging a crystal into the socket<br />

on the front panel and then tuning<br />

the v.f.o. dial slightly higher than<br />

the crystal frequency. The v.f.o.- crystal<br />

switch, S., should be thrown to crystal<br />

and the final then tuned in the normal<br />

manner. Since the setting of the v.f.o.<br />

dial has some effect on the crystal's<br />

frequency, the carrier can be "rub -<br />

bered" a kilocycle or so when dodg-<br />

ing QRM. On 20, 15, 11, and 10 meters,<br />

40 -meter crystals should be used,<br />

and for 80- and 40 -meter operation,<br />

160 -meter crystals are required.<br />

Since the crystal socket is wired in<br />

the hot portion of the oscillator grid<br />

circuit, whenever a crystal is in the<br />

socket, the v.f.o. frequency will be<br />

shifted slightly due to stray capacity<br />

effects. As a consequence, during<br />

v.f.o. operation it pays to remove the<br />

crystal from the socket.<br />

This nuisance will he minimized if<br />

you can locate a BC -746A tuning unit.<br />

The socket from a BC -746A is designed<br />

to accommodate two crystals<br />

and can be wired so that only two of<br />

its four contacts are live. Then. when<br />

using the v.f.o., a crystal may be<br />

placed in the dead section of the<br />

socket for storage.<br />

Both the final tuning condenser and<br />

the loading condenser have a rating<br />

of 140 µµtd. They, too, are salvaged<br />

from BC -746A tuning units. Since the<br />

plate voltage is not very high, no<br />

arcing difficulties should be experienced,<br />

despite the small plate spacing<br />

of these condensers.<br />

After trying several different types<br />

of final coil switching, a method employed<br />

by W2AEF' was finally put to<br />

use. The coils are mounted at right<br />

angles to one another, and therefore<br />

little loss is introduced into the circuit<br />

as the coils are shorted when<br />

switching from one band to another.<br />

The 20- mete[- coil, L.., is tapped for<br />

15 -meter operation and the 80 -meter<br />

coil, L., is tapped for 40 meters. No<br />

difficulty should be experienced in soldering<br />

a tap to L.,, but working with<br />

L., may not be so easy because of the<br />

small spacing between turns. After<br />

choosing the proper location for the<br />

40 -meter tap, take a thin jackknife<br />

blade and push the adjacent turns<br />

aside far enough to allow room for<br />

easy soldering. Once the tap is in<br />

place, use the knife blade to readjust<br />

the position of any turns which<br />

may have been deformed by the pre-<br />

vious operation. Make certain that<br />

there are no shorts between turns and<br />

then apply two or three coats of polystyrene<br />

coil dope to the area sur-<br />

rounding the tap. This will keep<br />

shorts from developing while the<br />

tapped coil is being wired in place.<br />

Although the 10- and 20 -meter final<br />

coils are self- supporting, the wire in<br />

the 80 -meter one is not strong enough<br />

for this purpose. Therefore, two<br />

pieces of polystrene must be cemented<br />

between the latter coil and the terminal<br />

strips to which it is soldered in<br />

order to provide the required amount<br />

of support.<br />

When wiring the final, be sure to<br />

keep all plate leads well removed<br />

from the grid circuit. Use the rear<br />

deck of the bandswitch for plate coil<br />

switching and be sure that the final<br />

grid circuit switching takes place at<br />

least two decks away. About the only<br />

other wiring precaution that need be<br />

observed is to make all bypass condenser<br />

leads as short as possible. If<br />

these steps are taken, no parasitic<br />

or fundamental oscillation problems<br />

should arise.<br />

The transmitter can be aligned<br />

without difficulty, providing you have<br />

the proper test equipment at hand. An<br />

accurately calibrated receiver, a 100 -<br />

kc. frequency standard, a grid dip oscillator<br />

covering all the bands from<br />

160 through 10 meters, and a 0 -5 ma.<br />

meter are "musts." Without these<br />

items you'll find yourself floundering<br />

helplessly, but if you have them, the<br />

job can be performed with a minimum<br />

of effort and wasted time.<br />

First, switch to the 10 -meter band<br />

and adjust C.:. until the oscillator just<br />

hits 7 mc. with the plates of C,. fully<br />

meshed. The grid dip oscillator should<br />

be coupled to L and the slug of this<br />

coil adjusted for resonance at 14.5 mc.<br />

L; should then be peaked at 29 mc.<br />

Tune C., until the v.f.o.'s fourth harmonic<br />

falls on 29.1 mc. Peak L. and<br />

L; for maximum final grid current.<br />

Tune C,. to 28.9 mc. and repeak L:,<br />

then tune to 29.3 mc. and repeak L.<br />

Grid current will then hold fairly constant<br />

from 28.6 mc. to 29.6 mc. It<br />

should be at least 21_ ma. over most<br />

of this range and shouldn't drop below<br />

2 ma. at the extremes. If this is<br />

not the case, readjust L: and L: until<br />

optimum operation is achieved.<br />

Throw S: to 11 meters and tune the<br />

v.f.o. to 6775 kc. Either compress or<br />

expand the turns of L, and L, until<br />

maximum final grid current is obtained.<br />

15 meters is next. Adjust L; to<br />

approximately 7100 kc. by means of<br />

the dipper. Tune the v.f.o. to the same<br />

frequency and either squeeze or expand<br />

the turns of L.. for maximum<br />

deflection of the grid current meter.<br />

On 20, tune the v.f.o. to 7100 kc.<br />

and peak L... at 14,200 kc.<br />

(Continued on pure 104)<br />

Fig. 6. Top view of the transmitter chassis. Parts placement<br />

is compact but not crowded. Note the right -angle mounting of<br />

the output coils, and Bakelite strips on the modulator choke.<br />

Fig. 7. Bottom view of the chassis. Slug tuned coils are so<br />

arranged that adjacent units do not tune to same frequency.<br />

thereby minimizing interaction and aiding unit's stability.<br />

46 RADIO & TEL<strong>EVIS</strong>ION NEWS

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