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Switching voltage stabilizer on KT825. Encyclopedia of radio electronics and electrical engineering

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Encyclopedia of radio electronics and electrical engineering / Surge Protectors

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Due to the high efficiency, switching voltage stabilizers have recently become more widespread, although they are usually more complicated than traditional ones and contain a larger number of elements. So, for example, a simple switching regulator (Fig. 5.6) with an output voltage lower than the input voltage can be assembled on only three transistors, two of which (VT1, VT2) form a key regulatory element, and the third (VT3) is an error signal amplifier.

Switching voltage stabilizer on KT825

The device operates in self-oscillating mode. The positive feedback voltage from the collector of the transistor VT2 (it is composite) through the capacitor C2 enters the base circuit of the transistor VT1. Transistor VT2 periodically opens up to saturation with current flowing through resistor R2. Since the base current transfer coefficient of this transistor is very large, it saturates at a relatively small base current. This allows you to choose the resistance of the resistor R2 rather large and, therefore, increase the transfer coefficient of the regulating element.

The voltage between the collector and emitter of a saturated) transistor VT1 is less than the opening voltage of transistor VT2 (in a composite transistor, as you know, two p-n junctions are connected in series between the base and emitter terminals), therefore, when the transistor VT1 is open, VT2 is securely closed.

The element of comparison and the amplifier of the error signal is a cascade on the transistor VT3. Its emitter is connected to a reference voltage source - the zener diode VD2, and the base - to the output voltage divider R5 ... R7.

In switching stabilizers, the regulating element operates in the key mode, so the output voltage is regulated by changing the duty cycle of the key. In the device under consideration, the transistor VT2 controls the opening and closing of the transistor VT3 according to the signal of the transistor VT1. At the moments when the transistor VT2 is open, in the inductor L1, due to the flow of load current, electromagnetic energy is stored. After closing the transistor, the stored energy through the diode VD1 is given to the load.

Despite its simplicity, the stabilizer has a fairly high efficiency. Thus, at an input voltage of 24 V, an output voltage of 15 V, and a load current of 1 A, the measured efficiency was 84%.

The inductor L1 is wound on a K26x16x12 ring made of ferrite with a magnetic permeability of 100 wire with a diameter of 0,63 mm and contains 100 turns. The inductance of the inductor at a bias current of 1 A is about 1 mH. The characteristics of the stabilizer are largely determined by the parameters of the transistor VT2 and the diode VD1, the speed of which should be as high as possible. In the stabilizer, transistors KT825G (VT2), KT313B, KT3107B (VT1), KT315B, (VT3), a diode KD213 (VD1) and a zener diode KC168A (VD2) can be used.

Author: Semyan A.P.

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