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Radio Broadcast - 1925, February - 113 Pages ... - VacuumTubeEra

Radio Broadcast - 1925, February - 113 Pages ... - VacuumTubeEra

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eceiving<br />

In the R. B. Lab. 719<br />

It is assumed that the resonant absorption<br />

coil will be wound on a form approximating<br />

the diameter of the secondary, perhaps alongside<br />

the secondary, or on a tube that may be<br />

slipped within the grid coil. This being the<br />

case, the absorption coil should be wound with<br />

one half the number of turns on the secondary,<br />

and the condenser C should have a value of<br />

.00025 m W. A Micadon will do nicely. This<br />

method of mounting the coil and condenser is<br />

illustrated in Fig. 3. The absorption coil has<br />

been wound alongside of the secondary.<br />

The absorption coil should be wound with<br />

no smaller than No. 26 wire. The differential<br />

effect is curiously curtailed by the use of very<br />

small wire sizes, for the high-frequency resistance<br />

of the wire increases with the frequency,<br />

which appreciably cuts down the absorption<br />

where it is most wanted. In a few cases when<br />

the absorption coil tunes over sharply, that is<br />

when the circuit oscillates above and below the<br />

maximum absorption point, the difficulty can<br />

be remedied by winding two or three turns of<br />

the coil with resistance wire from a rheostat.<br />

This added resistance tends to increase the<br />

decrement of the absorption circuit making it<br />

tune more broadly, which allows the receiver<br />

to cover a larger wave band.<br />

It is advisable to experiment with the<br />

coupling between the resonant absorption coil<br />

and the circuit. When .<br />

properly<br />

adjusted (though the adjustment is not critical<br />

and is easily effected), the set can just be<br />

FIG. 3<br />

A tuned radio transformer on the primary of which<br />

a stabilizing coil has been wound. The shunt condenser<br />

fits nicely within the tube<br />

made to oscillate by filament rheostat variation,<br />

thus permitting regeneration control that<br />

desirable and effective. When oscil-<br />

is<br />

very<br />

lations occur on such an adjustment they are<br />

almost invariably generated in the second<br />

tube, seldom, if ever, in the first bulb. Ape-<br />

FIG. 4<br />

The circuit of the de luxe six-tube Roberts Knockout receiver

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