ENCYCLOPEDIA OF RADIO ELECTRONICS AND ELECTRICAL ENGINEERING Tri-state power amplifier. Encyclopedia of radio electronics and electrical engineering Encyclopedia of radio electronics and electrical engineering / Power Supplies The article describes a non-reversible power amplifier operating on direct current in the mode of switching to an active-inductive load. In order to reduce power consumption after actuation of the actuator, the load is transferred from the rated DC voltage to the third state - a pulsed power supply mode with an unregulated duty cycle. Active-inductive loads (solenoids, clutches, electromagnets, relays, etc.) operating on direct current are widely used both in production and in everyday life. Most of these loads operate in an on-off mode, they are connected through amplifiers, and they do not require reverse (change the sign of the output voltage). Typically, such an amplifier operates in relay mode, when the control signal takes only two extreme values, corresponding either to the absence of current in the load, or to the rated current. The value of the traction force of the actuator is provided by the rated load current. After the actuator has worked, the conductivity of its magnetic circuit increases, and in order to maintain it in working condition, the load current must be reduced, just twice as compared to the rated current, which will save electricity. The relay mode of operation of the amplifier, as it were, excludes the third state of the load circuit without an additional ballast resistor, which extinguishes part of the load voltage, or without an additional power source with a voltage equal to half of the nominal one. Such amplifiers are described, for example, in [1], and are known under different names. The presence of a ballast or an additional power source is the main disadvantage of such circuits. The devices described below, after switching to the rated current mode, after a certain specified time, pass into the third state, in which a part of the rated voltage is set on the load, and the unregulated value of the latter is obtained as a result of a change in the relative duration of the pulse voltage on the load, i.e. by pulse-width modulation (PWM) amplifier. The amplifier is controlled by a PWM modulator operating at a certain frequency, depending on the load time constant. The main technical characteristics of the device:
The device (Fig. 1) consists of a power amplifier (PA) based on transistors VT1 and VT2, operating in the switching mode, and a DD1 logic circuit that controls it, made on the same package of the K561LN2 microcircuit. The microcircuit is powered from the input signal, and there must be no bounce of the input signal for reliable operation of the device. On inverters DD1.1 and DD1.4, an input signal delay circuit is made, on inverters DD1.2, DD1.3 and DD1.5, a rectangular pulse generator circuit that can provide both the required frequency (capacitor C2) and the relative pulse duration (resistors R3, R4). The VD4 diode acts as an anti-coincidence circuit, and the DD1.6 inverter is used to obtain the required magnitude and phase of the signal that controls the PA. Diodes VD5, VD6 protect the amplifier in the event of a short circuit of the load, which is shunted by the reverse diode VD7. The device works as follows. In the initial state, the input voltage is not applied, the microcircuit is not powered, the control voltage is not supplied to the PA input, the load is de-energized. When the control voltage is applied to the input of the device, the supply voltage is supplied to DD1, the charge of the capacitor C1 begins, and until the voltage equal to the inverter switching threshold voltage appears on the capacitor (ton = 0,7R1C1), the voltage at output 12 is log. "0". At the same time, a rectangular voltage appears at the output 6 of the generator with a duty cycle equal to 2, but until the delay circuit is triggered, the voltage log "10" is maintained at the output 1.6 of the inverter DD1. The PA turns on, the load is powered by the rated voltage. This voltage is held on the load until the end of transients and can vary from tenths of a second to several seconds by choosing capacitor C1. After the delay circuit is triggered at log "1" at the output 6 of the generator, a log "1" appears at the input 11 of the inverter DD1.6 and, accordingly, log "0" at its output 10. The PA closes, the voltage is removed from the load. The appearance of a log. "0" at the output of the generator will again turn on the PA, the load Y1 will again be energized, etc. If the generator output has rectangular pulses with a duty cycle of 2, then the load will have a voltage equal to 0,5 Unom. The load is powered by pulsed voltage modulated in duration with a constant repetition rate. As is known [2], in an active-inductive load, the current can flow continuously through the transistor from the power source, and when the transistor is closed, under the action of self-induction EMF, it can flow through the diode shunting the load. The average voltage at the load is not depending on the value of the inductance Un = kUp, where k is the pulse duration in relation to the pulse repetition period (the reciprocal of the duty cycle); Up - load power supply voltage. With an increase in the ratio of the load time constant τ = Ln/Rn to the pulse repetition period, the mode of continuous load currents begins. Taking into account the minimum current ripple in the load, the pulse duration should be ti = τ/(5...7). (one) The pulse frequency is selected in the range from several tens to several hundreds (and even thousands) Hz, depending on the time constant τ.
The main technical characteristics of the device according to Fig. 2:
In the devices shown in Fig. 1 and Fig. 2, the pulse frequency is 50 Hz, which is suitable for a large class of active-inductive loads, for which condition (1) is met. In the circuit of Fig.2 in module A1 in relation to the circuit of Fig.1 it is necessary to: 1) remove the jumper 4-5; 2) install jumper 4-6; 3) install a jumper in place of the VD4 diode; 4) set R5 = R6 = 9,1 kOhm. This device works similarly to the one described above in Fig.1. The circuits shown in Fig.3,4,5 are variants of the main circuit of Fig.1, but with the following changes in module A1: For Fig.3 in module A1 it is necessary to: 1) remove jumper 4-5; 2) install jumper 4-6; 3) install a jumper in place of the VD4 diode; 4) set R5 = R6 = 3,9 kOhm; C1 \u0,47d 2 uF; C0,01 = XNUMX uF. For Fig.4 in module A1 it is necessary to: 1) remove jumper 4-5; 2) install jumper 4-6; 3) install a jumper instead of the VD4 diode, instead of the resistors R5, R6, install the diodes with the cathode to the output of the microcircuit; 4) set C1 = 0,47 uF; C2 = 0,01 uF. For Fig.5 in module A1 it is necessary to: 1) remove jumper 4-5; 2) install jumper 4-6; 3) install a jumper in place of the VD4 diode; 4) set C1 = 10 uF; C2 = 0,1 uF; R5 \u6d R3,9 \uXNUMXd XNUMX kOhm. The circuit in Fig. 3 was tested with a load in the form of a REN34 relay (passport KhP4.500.030-01) with a nominal voltage of 12 V, a winding resistance of 75 Ω, and a trip current of 160 mA. When a capacitor C1 = 1 μF was installed in the circuit of module A0,1, a rectangular voltage with a frequency of 50 Hz was set at the generator output. At the same time, the relay vibrated. When, instead of resistors R3, R4, a variable resistor with a resistance of 220 kOhm was soldered, a voltage was established on the relay winding with a pulse duration of 15 ms, pauses of 25 ms, and the relay bounce stopped, the current in the relay winding became continuous (140 mA), the average value of the voltage on the winding was 10,4 .2 V (economical mode is not achieved). If you set the ratings: R82 \u3d 200 kOhm; R2 = 0,01 kOhm; C400 \u6d 80 μF, then a rectangular voltage follows with a frequency of XNUMX Hz, there is no contact bounce. The average value of the voltage on the winding is XNUMX V, the current in the winding is continuous and equal to XNUMX mA. In this case, the efficiency of the regime has been achieved. The circuit in Fig. 4 can be used to control a low-power active-inductive load, the operating current of which corresponds to the input current at log "0" at the output of the microcircuit. The circuit in Fig. 5 can be used to control an incandescent lamp. First, part of the voltage is supplied to the load, and after the filament has warmed up, the voltage becomes nominal. Details. All resistors in MLT type circuits. The 0,25 W resistors in the A1 module can be replaced with 0,125 W resistors, but this will not reduce the dimensions of the module. Low-power diodes can be replaced with KD102, KD103, KD226 diode - with KD213A. Capacitors type K739, K73-17, MBM. Electrolytic capacitor C1 type K52, K53, K50-16, K50-24. It is convenient to choose the oscillator frequency with capacitor C2. The devices described above can be used in production for various types of actuators, but the reliability of their operation in non-rated modes must be verified in practice. In particular, their use depends on the intermittent mode of operation of the actuator. References:
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