Electronic Transformer Coupled Oscillators

Posted on Feb 5, 2014

Transformer OCL and capacitor C1 form a tank circuit, to which are coupled sufficient turns to drive the grid in the lower left-hand winding. The output circuit is coupled by a separate winding. For good wave shape in such an oscillator, triodes and class B operation are preferable. The ratio of turns between anode and grid circuits is determined

Electronic Transformer Coupled Oscillators
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by the voltage required for class B operation of the tube as if it were driven by a separate amplifier stage. Single tubes may be used, because the tank circuit maintains sinusoidal wave shape over the half-cycle during which the tube is not operating. Grid bias is obtained from the RC2 circuit connected to the grid. In such an oscillator, tube load equals transformer loss plus grid load plus output. In small oscillators, transformer loss may be an appreciable part of the total output. This loss consists of core, gap, and copper loss. copper loss is large because of the relatively large tank current, and the wire size in the anode winding is larger than would be normally used for an ordinary amplifier. The gap is necessary to keep the inductance down to a value determined by the tank circuit Q or volt-amperes. This in turn is dictated by the required harmonic content. The use and selection of core materials are approximately the same as those indicated in Filter Inductor Design and Powdered iron Cores. Class C oscillators are less desirable for very low harmonic requirements, because of the difficulty of designing tank circuits with sufficiently high Q. Where large harmonic values can be tolerated, the transformer can be designed for low Q, but the wave form becomes non-sinusoidal. Transformer grid circuit turns are large, approximately the same as plate turns, and the grid voltage would be high if grid current did not...

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