ENCYCLOPEDIA OF RADIO ELECTRONICS AND ELECTRICAL ENGINEERING Generators and shapers of impulses. Encyclopedia of radio electronics and electrical engineering Encyclopedia of radio electronics and electrical engineering / Beginner radio amateur Based on the logic elements of digital devices, a variety of pulse generators can be designed. Here are some specific examples. The generator according to the circuit in Figure 1 (open-collector 2I-NOT elements are used) generates pulses in a wide frequency range - from units of hertz to several kilohertz. The dependence of the frequency f (kHz) on the capacitance of the capacitor C1 (pF) is expressed by the approximate formula f"3*105/C1. The pulse voltage duty cycle is almost equal to 2. When the power supply voltage is reduced by 0,5 V, the frequency of the generated pulses decreases by 20%.
In the generator according to the circuit in Figure 2, the pulse duration can be controlled by a variable resistor R2 (duty cycle varies from 1,5 to 3), and the frequency by resistor R1. For example, in a generator with C1 \u0,1d 2 μF, with the exception of resistor R1, only resistor R8, the frequency of the generated pulses can be changed from 125 to 1 kHz. To obtain a different frequency range, it is necessary to change the capacitance of the capacitor CXNUMX.
A wide change in the frequency of the generated pulses (about 50 thousand times) provides a device assembled according to the circuit in Figure 3. The minimum pulse frequency here is about 25 Hz. The duration of the pulses is regulated by the resistor R1. The repetition frequency can be determined by the formula: f=1/(2R1C1) f - frequency Hz, R1 - resistance Ohm, C1 - capacitance farad.
When implementing digital devices for various purposes, it is often necessary to form short pulses along the fronts of the input signal. In particular, such pulses are used to reset counters as synchronization pulses when writing information to registers, etc. Figure 4 shows the circuit and timing diagrams of a short negative pulse shaper based on a positive voltage drop at its input. When the voltage Uin changes from low to high, this difference without delay enters the input 13 of the element DD1.4. At the same time, at the input 12 of the element DD1.4, a high-level voltage is maintained during the signal propagation time through the elements DD1.1-DD1.3 (about 75 ns). As a result, the output of the device remains low during this time. Then, at the input 12, the voltage is set to a low level, and the output of the device is set to high. Thus, a short negative pulse is formed, the edge of which coincides with the front of the input voltage. In order to use such a device to form a negative pulse at the cutoff of the input signal, it must be supplemented with another inverter (Figure 4).
Figure 5 shows a diagram and a timing diagram of the operation of the pulse shaper along the front and edge of the input signal. The duration of each generated pulse is equal to tи1=tи2=nt1,0зд.р.+(n+1)t0,1зд.р. Here n is an even number of elements involved in signal delay. The principle of operation of this shaper is similar to the principle of operation of the previously described short pulse shapers. The shaper of short pulses has become widespread, the circuit and timing diagram of which are shown in Figure 6. At a low-level voltage at the input of the device, capacitor C1 is charged through resistors R1 and R2. In this case, the output voltage of the device is low. When a high-level voltage appears at the input of the shaper, capacitor C1 begins to discharge through resistor R2. Until the voltage across the capacitor drops to a low level, both inputs of the DD1.2 element, and, consequently, at the output of the shaper, have high voltage levels. As soon as the voltage on the capacitor becomes less than 0,4 V, the level at the output of the shaper changes (Figure 6, b). The pulse duration is proportional to the capacitor discharge time constant and is equal to ti=3R2*С1.
Pulse shapers are also included in the K155 series microcircuits. So, the K155AG1 microcircuit is a single vibrator with three inputs, direct and inverse, outputs and leads for connecting external timing circuits, Figure 7. The single vibrator can be triggered by both positive and negative drops in input signals at a certain voltage, independent of the duration of the input pulses. The one-shot switch is switched by a negative edge of the input signal applied to one of the inputs A, while a high level voltage is applied to the input B, or a positive edge applied to the input B, if a low level voltage is present at one of the inputs A or A1.
With the maximum resistance of the resistor Rin = 40 kOhm, the duration of the output pulse should not exceed 0,9T, where T is the repetition period of the input pulses. The duration of the output pulse depends on the resistance Rin=(0-40) kOhm and C=(0-1000) uF and is determined by the formula: ti=RC1n2. Here R \u2d 2k + Rin, XNUMXk is the resistance of the internal resistor. The K155 series also includes the K155AGZ chip. It contains two single vibrators in one housing. The options for connecting external timing elements and the timing diagram of the one-shot operation are shown in Figure 8. The one-shot is also triggered either by a negative (input signal drop at input A at a high level at inputs B and R), or positive by a positive voltage drop at input B at a low level at the input A and a high level at the input R. The pulse duration ti1 is determined by the time constant of the timing circuit, but can be reduced by applying a low-level voltage to the input R at ti2 ti1. . Author: -=GiG=-, gig@sibmail; Publication: cxem.net See other articles Section Beginner radio amateur. Read and write useful comments on this article. Latest news of science and technology, new electronics: Alcohol content of warm beer
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