ENCYCLOPEDIA OF RADIO ELECTRONICS AND ELECTRICAL ENGINEERING Power supply for car amplifier, 12/±20 volts 70 watts. Encyclopedia of radio electronics and electrical engineering Encyclopedia of radio electronics and electrical engineering / Power Supplies The supply voltage of the on-board network of a passenger car is 12 V. If we set the acoustic system impedance to 4 ohms, then the maximum power that can be obtained with this supply voltage will be 36 watts. This is the most theoretical maximum, assuming the bridged connection of the amplifier and zero resistance of the transistors of the output stage in the open state, that is, practically for a digital switching amplifier. For an analog amplifier, the maximum power will be no more than 20 watts per channel when bridged. To obtain more power, it is necessary either to use a pulsed output stage that generates an audio signal using the pulse-width modulation method, or it is necessary to lower the impedance of the speaker system. In the first case, the ultrasonic component from PWM will be present in the sound, as well. more complex measures to combat signal distortion will be needed. In the second case, the resistance of the voice coil will already be comparable to the resistance of the wires going to it, which, in general, can nullify such measures. There is another way - the organization of a volt-addition of power in the output stage due to the rectification of the output signal and a large storage capacity. But this is also not very good, since it is difficult to obtain a sufficiently linear frequency response, and there may be an uneven dependence of the power transfer coefficient on the input signal. Of course, all the measures listed above to increase the output power of an amplifier powered by a low-voltage source have the right to exist, and with careful and competent execution they give good results. But, there is a more traditional way to increase the power of the ULF - simply by increasing its supply voltage using a voltage converter, and even organizing bipolar power with its help. This method allows you to use in a car not a compromise automotive version of ULF, but almost any ULF circuit used in stationary equipment that can provide significantly better sound quality than ingenious powerful auto-ULF circuits, with voltage boosts on capacitors and low-impedance acoustic systems, because as they say any Hl-end lover - the best sound is given by a simple single-tube cascade without feedback circuits and with a high-impedance output. But this is of course the other extreme. Whatever the scheme of the "ordinary" ULF that you plan to use in a car, you need a power supply voltage converter for it. This converter must produce an increased bipolar voltage, in this case ± 20 V at an output current of up to 4 A. Such a power supply can supply ULF with an output power of up to 60-70 W, made according to the traditional scheme. The schematic diagram of the converter is shown in the figure. The scheme is largely typical. The master oscillator with a PWM output voltage stabilization circuit is made on the A1 chip. The nominal generation frequency is about 50 kHz (adjustable by resistor R3). The exemplary voltage from the output is fed to the input of the comparator (pin 1) and, depending on the voltage at pin 1, the comparator changes the width of the pulses generated by the microcircuit so as to maintain the output voltage stable. The value of the output voltage is precisely set by the tuning resistor R8, which will form this measuring voltage. The VD1-C3-R4-R5 circuit forms a soft start circuit. Output antiphase pulses are taken from pins 8 and 11 of A1 to be fed to the output stages, but here they first go to the output transistor driver on the A2 chip. The task of this microcircuit is to amplify the power of these pulses, since powerful field-effect transistors with a low open channel resistance are used here. Such transistors have a significant gate capacitance. To ensure sufficient speed of opening transistors, it is necessary to ensure the fastest possible charging and discharging of the capacitances of their gates, and this is what the driver on A2 serves for. Large capacitors C6 and C7 are installed along the power circuit, they must be soldered with a thick wire directly at the tap point of the primary winding of the transformer. For the option that gives a bipolar supply voltage (as in the diagram), the secondary winding has a tap from the middle. This tap through the inductance L2 is connected to a common wire. A rectifier is made on diodes VD2-VD5 (Schottky diodes), giving positive and negative voltages. In a unipolar supply circuit, the secondary winding does not have a tap, and the negative terminal of the rectifier bridge must be connected to a common minus. In this case, if a voltage of 40V is required, the resistance of the resistor R9 must be doubled compared to that indicated in the diagram. As a basis for the transformer, a neatly disassembled and unwound transformer from the power source of an old color TV of the 3-USCT line models is used. It should be noted that the core of the transformer is glued quite firmly there and not every attempt to separate its halves ends in success. In this sense, in my opinion, it is better to have two such transformers (fortunately, there are plenty of unnecessary power supplies MP-1, MP-3, etc. now). At one transformer, cut the frame along with the winding and remove it. The core remains, which, without a frame and winding, is much easier and more effective to divide. At the second transformer, carefully break and break the core so as not to damage the frame. As a result of this "barbarity" you get one good core and one good carcass. Now about winding. The winding must hold a large current, so a thick wire is needed for it. For winding the primary winding, a triple folded PEV 0,61 wire is used. For the secondary, the same wire, but folded in half. Primary winding - 5 + 5 turns, secondary - 10 + 10 turns. Coil L1 is not a coil, but a ferrite tube worn on a wire. L2 - 5 turns of a PEV 0,61 folded three times on a ferrite ring with a diameter of 28 mm. Rare FDB045AN transistors can be replaced by others, and the choice is quite large, since a maximum drain-source voltage of at least 50 V is required, a drain current of at least 70 A and an open resistance of channel 8 of no more than 0,01 Ohm. According to these parameters, you can select a lot of replacement candidates, that is, almost any FET transistor for automotive ignition switches and other things. Capacitors C11 and C12 for a voltage of at least 25 V, the remaining capacitors for a voltage of at least 16 V. Author: Gorchuk N.V. 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
02.05.2024 Advanced Infrared Microscope
02.05.2024 Air trap for insects
01.05.2024
Other interesting news: ▪ Smartphone with infinite memory ▪ Acoustics Microlab H30BT with NFC support ▪ Black caviar from Switzerland News feed of science and technology, new electronics
Interesting materials of the Free Technical Library: ▪ section of the site The most important scientific discoveries. Article selection ▪ article Nervous diseases. Lecture notes ▪ article fitter. Standard instruction on labor protection
Leave your comment on this article: Comments on the article: pasha Is there a seal? All languages of this page Home page | Library | Articles | Website map | Site Reviews www.diagram.com.ua |