ENCYCLOPEDIA OF RADIO ELECTRONICS AND ELECTRICAL ENGINEERING Electronic phase meter. Encyclopedia of radio electronics and electrical engineering Encyclopedia of radio electronics and electrical engineering / Measuring technology The phase meter is designed to measure the phase shift angles between two periodically changing electrical oscillations and can be used in amateur radio practice in the development, adjustment and operation of electronic and electrical apparatus and devices. The proposed electronic phase meter simultaneously provides information about the sign and magnitude of the phase shift angle, which makes it more visual. In the device, it was possible to significantly simplify the nodes for selecting the magnitude and sign of the angle and to combine the functions of individual elements. Main technical characteristics:
The schematic diagram of the electronic phase meter is shown in fig. one. Input voltages Uin1 and Uin2 of arbitrary shape (for example, sinusoidal) from the measured circuits through the dividers R1VD1VD2 and R2VD3VD4 are fed to the input of the shapers DA1 and DA2 (voltage comparators) and are converted into unipolar rectangular pulses with fairly steep rises and falls. The width of the pulses corresponds to the duration of the half-cycle of the input signal, which is illustrated by the timing diagrams shown in Fig.2.
The dynamic D-trigger (DD1) selects the sign of the phase shift angle, i.e., at the moment of formation of the pulse front of the second measuring channel used in this circuit as a synchronizing (clocking) signal, the leading or lagging nature of the signal of the first measuring channel, the output of which is connected to the information input of the D-flip-flop. In this case, the synchronizing pulse, with its front, transfers the D-flip-flop to a state determined by the voltage level at its information input at a given time. Therefore, if the input voltage Uin1 is in phase with the voltage Uin2, then the direct output of the D-flip-flop (pin 9 DD1.1) is set to a voltage corresponding to a logical unit, and the inverse output is set to a logical zero. The phase shift angle meter is implemented on the basis of a coincidence element (DD2.2), one of the inputs of which is connected directly to the output of the DA2 shaper, and the second is connected through the DD2.1 inverter with the measuring channel shaper DA1. The width of the generated pulse at the output of such an element is proportional to the angle of mutual overlap of the input pulses, i.e., the phase shift angle between the voltages Uin1 and Uin2, which is confirmed by the timing diagrams in Fig. 2. Combining information about the magnitude and sign of the angle in the scheme under consideration is carried out by introducing into its composition one more coincidence element (DD2.3), which performs the same functions of measuring the magnitude of the angle as described above. However, each of these 3I-NOT elements (DD2.2 and DD2.3) is connected by one of its inputs, respectively, to the direct and inverse outputs of the D-flip-flop, as a result of which the latter determines at the output of which of the coincidence elements a pulse is emitted, in width equal to the phase shift angle. The PA1 measuring device is connected between the outputs of the coincidence elements DD2.2 and DD2.3, thus forming a differential circuit, as a result of which its arrow will deviate in the direction determined by the sign of the angle, and by an angle corresponding to the phase shift angle between the voltages Uin1 and Uin2. Capacitor C1, connected in parallel with the PA1 indicator, is designed to reduce the pulsation of the arrow when measuring at low frequencies. The construction of the input circuits of the phase meter allows you to measure the phase angle not only between two voltages, but also between current and voltage or between two currents, for which the input dividers are equipped with appropriate leads. The electronic phase meter is made as a separate unit. The front panel displays the input terminals of the measuring channels, a microammeter, the scale of which is calibrated in el. deg., and a power switch. The elements of the device are mounted on a printed circuit board made of one-sided foil fiberglass 1,5 mm thick and fixed directly on the measuring clamps of the microammeter. The connections of the printed circuit board with the input terminals of the device are made with a shielded wire, which is caused by ensuring its noise immunity. The device uses resistors MLT and SP3-16 (R5), capacitor C1 - type MBM, and as an indicator PA1 - microammeter type M906 with a two-sided scale of 50-0-50 μA. Instead of those indicated in the device, microcircuits of other series of a similar functional purpose can be used with an appropriate choice of their supply voltage. Unipolar pulse shapers DA1 and DA2 can be made not only on the basis of K554CA3 or 521CA3 functional microcircuits, but also on operational amplifiers or transistor stages operating in the key mode and providing the required steepness of the generated pulse fronts. Diodes VD1 - VD4 are selected from the conditions of the flow of a long-term measured current through them. If the phase meter is designed to measure the phase shift between two voltages only, then these diodes can be replaced by any others without presenting requirements for current and reverse voltage. The device is powered from a single source of unipolar stabilized voltage (Fig. 3).
The expansion of the measurement limits for the voltage of the input signal can be carried out by proportionally changing the parameters of the resistors R1 and R2. If there is no need to measure the sign of the phase angle, then the dynamic D-trigger can be excluded from the circuit, and the phase angle difference signal extraction unit (Fig. 4) can be connected directly to the outputs of comparators DA1 and DA2. In this device, the DD1.4 element implements a differential switching circuit for the PA1 indicator and provides compensation for the logic zero voltage.
As an indicator of the controlled parameter PA1, an electronic oscilloscope or a digital voltmeter can be used, this will significantly improve the accuracy of reproduction of the measured value. The electronic phase meter has a linear scale, which makes it easy to calibrate. To do this, two linear voltages of a three-phase network should be taken as calibration voltages (the phase angle of the linear voltages is 120 el. deg.). In the process of calibration, it is necessary to match the calibration voltages with the permissible level of input voltages. The value of deviations of the indicator needle and the required scale mark is carried out by resistor R5. 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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