ENCYCLOPEDIA OF RADIO ELECTRONICS AND ELECTRICAL ENGINEERING Quartz chaotic oscillator. Encyclopedia of radio electronics and electrical engineering Encyclopedia of radio electronics and electrical engineering / Measuring technology The construction of self-oscillators with "chaotic behavior" is based on the interaction of interconnected linear and nonlinear oscillators. The scheme of a "chaotic" oscillator usually contains three main elements:
The nature of the processes in the nonlinear circuit of a chaotic self-oscillator is determined by both the frequency and the amplitude of the impact on it. Complex signals at the output of a non-linear circuit after passing through the self-oscillator feedback circuit become a source of perturbation of the same non-linear circuit. With repeated circulation of the signal, the dynamics of such an oscillator becomes chaotic. A diagram of a quartz chaotic oscillator, where quartz is used as linear circuits, is shown in Fig. 1. Here, the linear oscillatory circuit is formed by quartz, and the non-linear circuit is formed by elements L1-VD1. Depending on the polarity and level of the RF voltage applied to the varactor diode VD1, its capacitance changes, therefore, the natural (resonant) frequency of the L1-VD1 circuit also changes.
With certain parameters of the system (values of radio components), the oscillations in it become chaotic, and the spectrum of oscillations, discrete up to this point (Fig. 2), becomes continuous (Fig. 3).
To build a chaotic self-oscillator, the well-known classical scheme of a capacitive "three-point" was used. Transistor VT2 forms a buffer stage, which is necessary for decoupling the oscillator on VT1 and its load (for example, measuring instruments with 50-ohm inputs). The circuit in Fig. 1 uses two quartz. This is caused by the following. As shown by preliminary experiments, chaotic oscillations are realized in the presence of the L1-VD1 circuit and only one quartz, however, this mode of operation of the oscillator turns out to be extremely unstable. When the power is turned off and then turned on, the oscillator stops working in a chaotic mode and becomes a "normal" crystal oscillator. A return to the chaotic mode is possible in this case by briefly connecting the second quartz to the one already working in the oscillator. With the parallel inclusion of several quartzes and the absence of a nonlinear circuit L1-VD1, complex (multi-frequency), but deterministic oscillations occur in the circuit. By connecting a spectrum analyzer to the output of the oscillator, in this case one can see only a certain number of peaks of different heights (Fig. 2). In the presence of two quartz with different frequencies, the oscillations of one quartz modulate the oscillations of the other due to the non-linearity of the amplifier on VT1. The result is an AM signal and a series of harmonics. The more complex the shape of the oscillations affecting the linear circuit L1-VD1, the more likely the chaotic mode. It should be noted that the type of case and the execution of quartz must be identical, and they must differ only in frequency - this is one of the conditions for the oscillator to generate immediately at the frequencies of the quartz installed in it. The frequencies of quartz should differ by about 1,3 ... 1,5 times. In this case, it is necessary to use quartz with a frequency ratio close to an irrational number. In other words, it is desirable to use quartz with incommensurable frequencies. To obtain chaotic oscillations, if necessary, it is necessary to select the inductance L1 (as L1, the author used an industrial-made drop-shaped choke with two leads). If chaotic oscillations still do not work, you should try to select capacitors C2 and C3, or change the DC mode of the transistor VT1 using R1. Having installed a multi-band receiver with AM bands near the oscillator under study and connecting a piece of wire 10 ... The presence of strong noise in a wide frequency band with "inserts" of very powerful carriers indicates that it is the chaotic mode of operation that is implemented. Instead of a receiver, you can use a special device that allows you to control even the moment of transition from deterministic to chaotic oscillations. The circuit of such a device - an indicator of chaotic oscillations (Fig. 4) - is a detector receiver of AM signals with a 50-ohm RF input and a highly sensitive ultrasonic frequency loaded on headphones.
The indicator is adjusted by selecting the value of the resistor R5 until a voltage of +4 ... 8 V is obtained at the VT2 collector. The indicator input is connected to the generator output. In the presence of chaotic oscillations in the oscillator under study, a very loud noise is heard in the headphones, resembling the "super noise" of a super-generative receiver. As experiments have shown, in the frequency band 1 ... 25 MHz, the noise power of a quartz chaotic oscillator is 104... 106 times more noise power than the classical zener diode noise generator circuit! This makes it possible to use the quartz chaotic self-oscillator as a heavy-duty noise generator for various measurements. Literature
Author: V.Artemenko, UT5UDJ, Kiev; Publication: radioradar.net See other articles Section Measuring technology. Read and write useful comments on this article. Latest news of science and technology, new electronics: The world's tallest astronomical observatory opened
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