ENCYCLOPEDIA OF RADIO ELECTRONICS AND ELECTRICAL ENGINEERING Reducing the heating of transformers of low-power power supplies. Encyclopedia of radio electronics and electrical engineering Encyclopedia of radio electronics and electrical engineering / Power Supplies When making low-power mains-powered electronic devices on their own, radio amateurs often encounter a situation where the mains transformer turns out to be the only noticeably heating element of the device, dissipating power in the form of heat, sometimes several times higher than the useful one. The thing is that industrially manufactured transformers, having suitable dimensions and voltage, are sometimes made so "economically" that even the no-load current causes them to heat up. Especially often transformers manufactured in Southeast Asia have this drawback [1]. They are more suitable for countries where the mains voltage is 220 V with a frequency of 60 Hz, but for normal operation in a network with a frequency of 50 Hz, the number of turns of the mains winding is insufficient. On fig. 1 shows the dependence of the no-load current on the mains voltage of some transformers. Curve 1 corresponds to transformers from universal adapters "SANWALL" and "BELLSONIC" with a power of 5 W, with a maximum load current of 300 mA, an output voltage of 3 ... 12 V, having magnetic circuits with a cross section of 1,4 cm2. For comparison, curves 2 and 3 are transformers of domestic production TP - 133 and TP - 321, in which the cross-sectional area of the magnetic conductors is 2 and 1,6 cm2, respectively. Given that the mains voltage, especially in cities, can exceed 235 V for a long time, and an increase in voltage above the nominal causes a disproportionately large increase in no-load current, the use of such transformers, especially in devices designed for long-term operation without supervision (timers, thermostats, antenna amplifiers, etc.) should be approached with great care. There is a way out in this situation. It is necessary to include an active or reactive ballast resistance in the primary winding circuit of the mains transformer to reduce the voltage on it by 20 ... 30 V. The no-load current and heating of the transformer will noticeably decrease. Of course, this reduces the secondary voltage and power of the transformer. However, if the power consumed by the device is much less than the overall power of the transformer, then this is quite acceptable. Usually resistors or capacitors are used for such purposes [2]. The main disadvantage of a resistive ballast is its heating, which limits the scope of this method. Moreover, the voltages on the primary winding of a lightly loaded transformer and on the resistor have different phases (the phase shift can reach up to 70 ... 80 degrees), so the voltage across the resistor is usually higher than expected. For example, with a mains voltage of 220 V and on the primary winding of an unloaded transformer of 195 V, the voltage across the resistor can reach up to 45 V. When the load of the transformer increases to values close to the nominal value, the phase shift decreases almost to zero. Capacitive ballast practically does not generate heat, but as practice shows, it is most advisable to use capacitors when the voltage on the transformer windings needs to be reduced by more than 25 ... 30%. In any case, if capacitors are used, it is necessary to make sure that when the load and supply voltage change in the primary circuit, there are no resonant phenomena when the voltage across the transformer can increase sharply [3]. In the case of using an inductive ballast, such phenomena do not occur, since the voltage phases are almost the same, heat is released only on the active resistance of the ballast winding, which is several times less than that of an equivalent ballast resistor. It is convenient to use DC electromagnetic relays for an operating voltage of more than 20 V as inductive ballasts, for example, PCM, RES6, RES9, RES22, etc. To reduce their dimensions, the relay can be disassembled and only a coil with a magnetic circuit can be used. To eliminate chatter, the relay armature should be fixed in the attracted state by bending or using a pointed match and glue. When choosing a relay, it is necessary to take into account the maximum current in the primary circuit of the transformer, which must not exceed the rated operating current of the relay. Curve 4 in Fig. 1 shows the change in the no-load current of the transformer (dependence 1 in Fig. 1) with an inductive ballast (relay PCM-2 for a voltage of 24 V with a winding resistance of 750 Ohm, a rated operating current of 35 mA). On fig. 2 shows the load characteristics of the same transformer (voltage at the output of the rectifier with a filter): curve 1 - without ballast; 2 - with inductive ballast (relay PCM-2); 3 - with an equivalent (for a load current of 20 mA) resistive ballast - a resistor with a resistance of 3 kOhm and a power of 4 W. The large load capacity of a transformer with an inductive ballast compared to an equivalent resistive ballast is apparently due to a decrease in the ballast inductance due to saturation of the magnetic circuit with an increase in the flowing current. This is noticeable by the characteristic change in the curvature of dependence 2 in relation to graphs 1 and 3 at a load current of 150...200 mA. Literature
Author: V. Andreev, Tolyatti, Samara region. See other articles Section Power Supplies. Read and write useful comments on this article. Latest news of science and technology, new electronics: Machine for thinning flowers in gardens
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