ENCYCLOPEDIA OF RADIO ELECTRONICS AND ELECTRICAL ENGINEERING Charger for nickel-cadmium batteries. Encyclopedia of radio electronics and electrical engineering Encyclopedia of radio electronics and electrical engineering / Chargers, batteries, galvanic cells At present, miniature MP3 players are very popular, especially among young people, as well as electronic cameras that are powered by a voltage source of 1,2 ... 1,5 V. The use of galvanic disposable cells is hardly justified here - the current consumption is high, and even with prolonged continuous operation. Ordinary cells of the "AAA" type have to be changed several times a day in this mode, which is quite expensive, but the battery can save you a lot of nerves and money. In order for the battery to serve for a long time, it is necessary to ensure its optimal mode, both charging and discharging. Nickel-cadmium batteries are characterized by the so-called "memory effect". Consisting in the fact that if you charge an incompletely discharged battery, then during further discharge it will give only part of the energy, starting from the level from which charging began. Therefore, before starting charging, it is advisable to discharge the battery to a voltage of less than 1 V. And only after that start charging. The figure shows a diagram of a charger - an attachment to a laboratory power source that measures the voltage on the battery, discharges the battery to 1 V before charging and charges it to 1,4 V. The charger itself consists of a current stabilizer at A1. The value of the charging current can be set to 60mA, 80mA or 120mA with switch S2. The charger is turned on and off using transistors VT3 and VT4. To start charging to the VT3 base, you need to apply a logical zero. And to stop charging - one (through resistor R14). The discharge circuit is made on a transistor key on VT5 and VT6, connected according to the circuit of a composite transistor. The discharge load is resistor R16. The voltage on the battery (G1) is measured by the meter on the A1 polycomparator chip. LEDs HL1-HL6 indicate the voltage on the battery, and the cascades on VT1 and VT2 form logic levels for supplying information about the voltage on the battery to a simple control logic circuit on two RS-flip-flops made on the elements of the K561LE5 microcircuit. Now consider the operation of the scheme as a whole. When the battery is connected, the A1 chip measures the voltage on it. The measurement result can be seen on a display of six LEDs. The measurement is made without load. To find out the voltage under load, you need to press the "Start" button S1. In this case, the RS flip-flop D1.3-D1.4 is set to a state with a logical unit at the output D1.4. The transistor key VT5-VT6 opens and loads the battery with resistor R16. If at the same time the voltage on the battery drops to 1 V and one of the diodes VD1-VD3 opens below, which leads to the opening of the transistor VT2. A logical unit voltage appears on its emitter, which, after some time (R8-C2), switches the RS flip-flop D1.3-D1.4 to the opposite state. The load (R16) from the battery is disconnected. At the same time, the unit that occurred at the output of D1.3 sets the trigger D1.1-D1.2 to a state with a logical zero at the output of D1.2. This causes the charger to turn on. A2 (VT4 opens). Battery charging starts. If the loaded battery voltage is greater than 1V, it will be held under load until the voltage across it is 1V or less. And only after that the charging will start. Charging will continue until the voltage on the battery reaches 1,4 V. After that, the transistor VT1 will open and the voltage of the logical unit level will be set on its collector RS-trigger D1.1-D1.2 will switch to a state with a unit at the output D1.2 .XNUMX and battery charging will stop. The disadvantage of this scheme is that only one battery can be charged at the same time. Batteries cannot be charged. Even if you make a switchable divider at the input of the A1 microcircuit, the charger will not be able to work well with the battery, since it is impossible to determine how discharged one or the other battery included in it is by the total battery voltage. Therefore, if you need to charge several batteries at the same time, you need to make an appropriate number of such circuits. The K561LE5 chip can be replaced by a domestic analogue K176LE5 or any foreign analogue. The LM3914 chip can be replaced with some kind of analogue, but subject to a linear indication (not logarithmic) using the running point method. Or assemble a comparator circuit on operational amplifiers. The adjustment consists in setting the charging current by selecting the resistances R10-R12 and calibrating the voltage meter by adjusting the resistor R2. Another point - when the HL6 LED is off, the voltage across R4 should be zero. If this is not the case, you need to include a diode of the KD1 type in the emitter circuit VT522, in the forward direction. The same applies to the transistor VT2 (the voltage on its collector should be zero when the LEDs HL1, HL2, HL3 are off). Author: Zamkov V.S. See other articles Section Chargers, batteries, galvanic cells. Read and write useful comments on this article. Latest news of science and technology, new electronics: Air trap for insects
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