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Frequency multiplier on phase shifters. Encyclopedia of radio electronics and electrical engineering

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Encyclopedia of radio electronics and electrical engineering / Digital technology

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Unlike conventional frequency multipliers, phase shifter multipliers can provide a spectrally clean, filter-free output signal. Using broadband phase-difference circuits for phase splitting, it is possible to implement frequency-independent multipliers operating in a range that spans many octaves.

The principle of operation of multipliers of this type is shown in Fig. 1a. The frequency of the sinusoidal signal is multiplied by N by dividing the input voltage into N different phases equidistant from each other over a range of 360°. N signals with different phases drive N transistors operating in class C mode, the output signals of which are combined to form a pulse every 360°/N degrees. By using N transistors, the input signal power can be N times the power required to saturate the transistor.

Frequency multiplier on phase shifters
Fig.1a (click to enlarge)

The described audio frequency multiplier by 4 (Fig. 1b) contains frequency-dependent 90° phase shifters R1C1 and R2C2. Transistors Q1 and Q4 form pulses that are phase-shifted at the output by 0 and 90 °. The phase inversion of the pulses is carried out by transistors Q5 and Q6, which control transistors Q2 and Q3, as a result of which pulses with a phase shift of 180 and 270 ° are formed at the output of the latter. The 90° phase-shifted output pulses are combined to form a quadruple frequency. The audio range multiplier quadruples frequencies from 625 to 2500 Hz.

Frequency multiplier on phase shifters
Fig. 1b (click to enlarge)

The amplitude of the input signal is set to the required value on the basis of the transistor Q4. In addition, resistors R3, R4 and R5 can adjust the signal amplitude for transistors Q1, Q2 and Q3. The waveform shows high quality output signal when multiplied by 4 input frequency of 2500 Hz.

Compared to conventional devices, frequency multipliers based on phase shifters have less subharmonics at high frequencies. Figure 2a shows a high-frequency version of such a multiplier (also by 4), in which a simple phase shifter in the form of an LCR circuit is used to shift the phase by 90° (Fig. 2b). An interesting property of such a circuit is that for equal values ​​of reactances, the phase shift between the input and output is 90 °, regardless of the resistance R. This allows you to adjust both the amplitude (by changing R) and the phase (by changing L or C) of the signal.


Fig.2a (click to enlarge)


Rice. 2b

The inductance L is formed by the primary winding of the transformer T1; from the secondary winding, transistors Q1 and Q2 receive signals shifted by 90 and 270 °, respectively. Phase shifts of 0 and 180° are carried out by transformer T2, which is connected to transistors Q3 and Q4.

The U-shaped inductive circuit at the output provides optimum matching to a 50-ohm load and low sub-harmonic rejection. Unlike conventional devices, this multiplier suppresses subharmonics and does not require filtering at the output.

As measurements with a spectrum analyzer show, the second and third harmonics can be easily suppressed by more than 50 dB relative to the level of the useful fourth harmonic.

Author: Fred Brown; Publication: N. Bolshakov, rf.atnn.ru

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