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ENCYCLOPEDIA OF RADIO ELECTRONICS AND ELECTRICAL ENGINEERING
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Experiments with a quartz supergenerator. Encyclopedia of radio electronics and electrical engineering

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Encyclopedia of radio electronics and electrical engineering / Knots of amateur radio equipment. Generators, heterodynes

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Figure 1 shows the scheme that was used for the experiments. The frequencies of the quartz in the studies were 14.218 MHz. The main element that was changed in the experiment is the inductor L. A 22 kΩ resistor was added in parallel to it to eliminate frequency dips within the range. The transistor in the generator has a cutoff frequency of 80 MHz. As a buffer stage - a field-effect transistor amplifier. The bias resistor Rb for the first transistor is 100 kΩ (with this value, the emitter current is 9 mA). Capacitors C1 and C2 150 pF each. At the end of the experiment, there was an attempt to change the values ​​of Rb, C1 and C2. The variable capacitor is plate-type and has a value from a few pF to 100 pF. The transformer T is wound on a ferrite ring with a diameter of 7 mm. The winding is made of folded and twisted three wires PELSHO 0.2 and contains 3...4 turns. The ends of each winding are connected according to the scheme.

Experiments with a quartz supergenerator. Scheme
Ris.1

Figure 2 shows the generator frequency adjustment ranges when the capacitance of the TS capacitor changes from the minimum value to 100 pF. For measurements, we used a set of inductors L with ratings of 5.6, 8.2, 10, 10.39, 11, and 12 μH. To obtain an inductance of 10.39 μH, two 10+0.39 μH coils connected in series were used, and for 11 μH, 10+1 μH. For clarity, the curve (X1 only) for a generator with one quartz is shown. As can be seen from the graph, for a conventional generator, the frequency changes slightly with increasing inductance. At the same time, for the supergenerator, the frequency adjustment range rapidly increases up to 300 kHz (!) with L=12 μH. However, we must be careful with such a wide frequency adjustment range due to the deterioration of stability.

Experiments with a quartz supergenerator
Ris.2
Figure 2 shows the frequency drift for three inductance values ​​L=10, 10.39, and 11 µH. In this case, both quartz are connected in parallel, and the capacitance of the variable capacitor is TC=100 pF. The measurements were carried out 25 min after soldering the corresponding circuit. After that, the power to the generator was turned on and the time was recorded. As can be seen, acceptable stability over time was observed for L=10 μH. For values ​​with L=10.39 and 11 µH, the frequency drifts over a wider range. This is most dependent on the temperature coefficient of the inductances. Therefore, in my practice, I settled on the maximum value of L = 10 µg. Ultimately, you can get better stability with longer warm-up times and using inductors with small temperature coefficients.

Experiments with a quartz supergenerator
Ris.3

Now I change capacitances C1 and C2 a little. All other parameters are set as follows: Rb=100 kOhm, L=10 µH, and X1, X2 in parallel connection. Fig.4 shows the frequency range as a function of capacitance C1 and C2. C1 and C2 changed simultaneously. The graph shows that the frequency range is wider with increasing capacitance. Measurements with C1=C2=330pF were not possible because Vout (output voltage at the counter) was too low as shown in Fig.5. The values ​​​​of C1 and C2 in 100 and 150 pF are the most acceptable in practice in this circuit.

Experiments with a quartz supergenerator
Ris.4

And, finally, the value of the base resistor Rb was changed. The other elements were: C1=C2=150pF, L=10uH, and X1, X2 in parallel. Initially, Rb was set to 100 kΩ with an emitter current of 9 mA. This time, Rb is set to 200 kΩ, with the emitter current reduced to 5.2 mA. The frequency range did not change although Vout (output voltage) decreased from 0.7 V to 0.3 V. Further, Rb was increased to 470 kΩ, the emitter current decreased to 2.4 mA. However, Vout was too low, less than 0.1 V. Therefore, the counter could not measure the frequency of the signal.

Experiments with a quartz supergenerator
Ris.5

Finally, a frequency range of about 100 kHz was obtained with L=10 µH, C1=C2=150 pF, X1 and X2 connected in parallel and Rb=100 kΩ. The stability was acceptable, but worsened as the coil inductance L increased. The frequency range was wider because C1 and C2 were set to high values ​​but did not depend on the bias resistor Rb.

It should be emphasized that these results are more or less specific and depend on the quartz used in this experiment. The optimum was estimated for L, C1 and C2 and may differ from the values ​​obtained in this experiment if the quartz has other parameters or other frequencies. Therefore, you can experiment to optimize the parameters for your quartz resonator.

Author: MINOWA, Makoto, 7N3WVM; Translation and publication: N. Bolshakov, rf.atnn.ru

See other articles Section Knots of amateur radio equipment. Generators, heterodynes.

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