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ENCYCLOPEDIA OF RADIO ELECTRONICS AND ELECTRICAL ENGINEERING
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Hi-Fi amplifier QUAD-405. Encyclopedia of radio electronics and electrical engineering

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Encyclopedia of radio electronics and electrical engineering / Transistor power amplifiers

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For decades, the "QUAD-405" has been one of the best known quality amplifiers. With the application of innovations born of technology, its parameters have been repeatedly improved. We will get acquainted with its modified version, in which the emphasis is on increasing power.

The purpose of the modification was to double the power of the "basic version" of "QUAD", i.e. up to 200 W, while maintaining all its output parameters. This task is not an easy one, since it entails, first of all, an increase in the supply voltage. To get 200W sinusoidal power into a 4-ohm load, you need an 80V peak-to-peak signal. This signal level requires a supply voltage of approximately ±50. .55 V. The situation is even more complicated in the case of 8-ohm loudspeakers. when the output signal swing needs to be increased to 115 V. The supply voltage required for it increases to ± 60 ... 65 V.

From the above examples, it is clear that increasing power requires considerable discretion in solving both circuitry and technological problems. The correct choice of transistors is a necessary but not sufficient condition for the correct solution of this problem.

Scheme "QUAD-405/200"" is shown in Fig.1.

Hi-Fi amplifier QUAD-405
(click to enlarge)

The AC voltage gain is determined in the 1C operational amplifier by the ratio of the resistances R6 and R3. Negative feedback, due to the presence of capacitor C3, begins to act above a frequency of 1 Hz. Through the R5-R3 circuit, 100% negative DC feedback is carried out from the output of the amplifier. Since the amplifier has unity gain with respect to DC, the resulting offset (offset) is the same as the bias voltage of the operational amplifier.

The amplification of the AC voltage and the operation of the class "A" amplifier on the transistor T2 at high frequency is determined mainly by the elements of the bridge. Capacitor C9, together with this amplifier, forms a high-speed integrator, while it simultaneously serves as one of the bridge elements. The next element of the bridge is R37. Control over the output stage current (dumper) is carried out by the third element of the bridge - inductance L2. The fourth element of the bridge is the equivalent resistance of the parallel chain of resistors R16-R17, which, with the help of R15, sets the voltage gain of the cascade at T2, contributing to a very good linearity of the characteristic.

In the same way, voltage is supplied to T2, which compensates for the error that occurs due to the voltage drop across L2 due to the output current. This error signal passes through the amplifier and appears at the output with the same amplitude, but with the opposite phase compared to the signal occurring at 12. After the two error signals are canceled out at the loudspeaker, a slight mismatch of the bridge creates an excellent output signal without distortion. . System performance is affected by Class A distortion, bridge mismatch, and NE5534 op amp distortion.

Limiting the frequency range of the signal arriving at T2 is provided by the integrating chain R11-C6. This places an upper limit on the bandwidth of the amplified frequencies and is one of the simplest ways to protect against intermodulation distortion. About the proper phase shift of the amplifier on T2. in addition to C9, the chain C8-R14, as well as the capacitor C10, also "takes care of". Excessive phase shift that occurs during the turn-on of the output stage is compensated by the chains L3-R33 and L1-R36.

Amplifier "QUA0-405/200" is placed on a single-sided printed circuit board, the drawing of which is shown in Fig. 2, and the location of the elements - in Fig. 3.

Hi-Fi amplifier QUAD-405

Mounting parts on the board begins with resistors (parts are installed in ascending order of their height). This prevents the soldered part from moving out of place when the board is turned over. Resistors are recommended to be measured with an ohmmeter, rather than identified by a color code printed on them. Powerful resistors should be installed a few millimeters above the board so that they cool better. Inductors L1...L3 each contain 22 turns of winding wire 01 mm wound on a mandrel 013 mm (L1, L3) and 016 mm (L2).

Next, an operation is carried out that particularly affects the reliability of the amplifier: the installation of terminal transistors. Let's think about the following: with an efficiency of 70% and a sinusoidal signal, approximately 90 W of thermal power must be diverted so that the instantaneous temperature of the semiconductors does not approach a critical value! In catalogs, this temperature is usually indicated in the range of 120 ... 140 ° C. This can only be achieved by installing transistors T7 ... T10 on a radiator with very good heat transfer (with heat-conducting paste).

Upon completion of the assembly, we carefully examine the entire circuit again. Using an ohmmeter, we check the insulation between the transistors and the radiator. If everything is in order, you can make the first inclusion. You should not rush, because in the case of a powerful amplifier it is impossible to unambiguously determine how it will behave when the operating point setting is not yet known. By working with due care, the so-called "smoke effect" can be avoided. To do this, we include ammeters in the positive and negative power circuits. It is necessary in one way or another to limit the maximum current of the power supply so that in the event of a short circuit there is no trouble.

Basically, two cases are possible. In the first of them, the final stage functions normally, in the second it “smokes” due to some kind of malfunction. In the first case, the current consumption is about 100 mA. In the second case, there is some kind of anomaly, the current is much larger (it is limited only by the internal resistance of our power supply). In light of this, it is desirable to have a protection with such a characteristic that the impedance at low currents could be neglected, while at high currents it would increase abruptly. This characteristic has a conventional incandescent lamp.

We will include in the positive and negative branches of the power supply by a lamp (a series chain of lamps), the voltage of which is not less than the supply voltage. The protective ability of an incandescent lamp is based on the property that there is a difference of more than one order of magnitude between its cold and hot resistance. If the amplifier is working well, the quiescent current is about 100 mA. With such a current, an incandescent lamp due to the small "cold" resistance is equivalent to a short circuit, as if it were not there. In other words, when it is off, everything is fine. Otherwise, if the pump is on, this indicates a large current and the presence of some kind of malfunction in the system. However, the disaster did not happen, and there is little chance that any part failed. Experience has shown that high current is usually due to improper resistor placement, board defects, poor soldering, high frequency self-excitation, and, much less frequently, poor parts.

With a lamp, troubleshooting is simplified because the circuit can remain on for a longer time. During this time, the defective part will warm up well, and it is easy to detect it by touch. If this does not help, measurements with instruments will be needed. This method of protection using an incandescent lamp is successfully applicable to any amplifier.

So, we connect the supply voltage to the appropriate contacts. Its value is not critical: ±45 ... 55 V. We look at the lamps; if they are off, we control the current in both branches of the supply voltage using ammeters, and then the voltage at the output of the amplifier. This should be around 0V. Current below 100mA and the presence of zero at the midpoint indicates that the DC operating point is set correctly and dynamic control can be exercised. As a precaution, incandescent lamps with a small signal can be left. It should be borne in mind that they limit the output power, and, depending on the magnitude of the signal, they flash and “put down” the power, as in the event of a malfunction, therefore, they are not used with a large signal.

We control signal transmission without load using an audio frequency generator and an oscilloscope. If, after turning on the amplifier without a signal and load, any lamp lights up, immediately turn off the power and engage in a systematic search for errors. Unfortunately, no exact recipe can be given here, as any mistake can affect nutrition. We examine the amplifier again, paying increased attention to the board tracks (presence of breaks, short circuits, etc.), soldering (shorting neighboring points, "unsoldered"). polarity of installed diodes, capacitors, etc.

It is advisable to supplement such an amplifier with an appropriate protective circuit - a "knock silencer". First of all, this protects the speaker system from voltage surges that occur during turning off and on the amplifier, as well as the appearance of a constant voltage at the output in case of a possible malfunction. When finalizing before the output amplifier, you need to turn on some kind of preamplifier and tone control to adjust the level and tone of the sound.

It is advisable to power the amplifier from a structurally simple supply unit (transformer-bridge-capacitor of a high-capacity filter). To achieve an output power of 200 W with a good approximation, a mains transformer of at least 300 W is required. The amplifier can be connected to the power supply using contact connections. The signal input on the board is made in the form of a soldering patch, since it is more expedient to directly solder the shielded cable from the preamplifier here.

See other articles Section Transistor power amplifiers.

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a guest
"The AC voltage gain is determined in the 1C operational amplifier by the ratio of the resistances R6 and R3." Not entirely accurate, it is difficult to agree with this with reservations. "Negative feedback, due to the presence of capacitor C3, begins to act above a frequency of 1 Hz." Here is already a gross mistake, eloquently speaking about the qualifications of the writer. You don't have to read further...


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