Output power: 100W (RL = 4Ω, K = 0.1%) or 70W (RL = 8Ω, K = 0.1%) (continuous sinusoidal signal)
Power in relation to frequency: <10Hz-100KHz at 100W
Distortion: 0.1% at 20Hz-20KHz at 100W
Intrinsulation: 0.28% measured at 40Hz and 10KHz at a 4: 1 ratio and Pa = 100W
Signal/Noise (SIN): 70 dB
Input sensitivity: 0.775V
Input resistance: 100KΩ
Output resistance: 0.052 Ω (in 1KHz)
Minimum load: 4Ω
Power supply: 80V symmetrical (+ 40V, 0, -40V)
Current consumption: 2.5A max at RL = 4Ω
Peak current: 50mA
The input stage, is a differential amplifier with main elements the transistors T1 and T2. Then we have a lead step with T4 whose collector is connected to the T3 emitter. This works like an adjustable Zener diode and regulates the resting current. The final step follows with two completely complementary transistors T7 and T8 (Darlington).
An advantage of the symmetrical voltage, is that the electrolytic capacitor is avoided at the circuit.
The amplifier has a fairly high input resistance that exceeds 100KΩ since before C4 we have R2, and since the input resistance of T1 is too high.
Negative feedback (both for DC and for AC) we have with resistance R6. The DC negative feedback section produces almost zero potential at the output. The feedback section AC determines the amplification and is dependent on R6, C4 and R3. The amplification is determined by the formula:
Uo/Ui = (R3 + R6)/R3 = 3420/120 = 28.5
The stage with T4 leads the T7 and T8, but because they are darlington they need very little base current, so for T4 we do not need a heatsink.
Transistor T3 together with resistors R18 and R19 stabilizes the output current of the output transistors. The voltage drop on R18 and R19 is determined by the position of P1 because it controls the collector voltage from the T3 transmitter. R11 in conjunction with C5 capacitor increases the AC boost of the drive.
The heart of the output stage is the Darlington transistors BDX66 and BDX67. At 25°C this series has the following characteristics:
If the collector current becomes 10A then the collector voltage from the transmitter becomes 2V and the amplification at DC is about 1000. When the collector current is 5A then the voltage is between 0.4V and 0.5V and the amplification is about 4000.
With these characteristics these transistors are ideal for such circuits. Regardless of how "good" the transistors are, they need protection from short circuits.
The voltage drop on the collector resistors R18 and R19 gives us the magnitude of the collector current through the transmitter. If the current passing through the resistors R18 and R19 passes a certain limit, then they will start to drive the transistors T5 and T6 since the voltage on the dividers R16, R14 and R15, R17 parallel to R18 and R19. Thus the currents passing through the diodes D2 and D3 will reduce the base currents of T7 and T6, which will also reduce the collector currents.
The various other elements R and C serve different purposes. C1 limits the input bandwidth. This avoids a portion of noise. C3 is responsible for 3dB at 100KHz, that is to say, it is inclined to the characteristic of the frequency response. C6, C7 and C8 are Miller capacities. C9 and R20 stabilize the output. The C10 / R21, C12, C11 / R22 and C13 cut off the various peaks at the RF frequencies coming from the power supply.
The circuit has no difficulty and its construction is relatively easy. With some luck, the amplifier can give 120W of power at 4Ω, but unfortunately the deformation reaches about 1%. But at 100W (again at 4Ω) the deformation is less than 0.1%.
From the following figure we see that the deformation remains constant and is less than 0.1% at frequencies from 40Hz to 20KHz. For full performance the input must be greater than 0.775V. This level is given by almost all preamplifiers. If a higher output device is used then a 10KΩ potentiometer must be fitted at the input of the amplifier.
It is known that the performance of the amplifier depends on the quality of the power supply. The amplifier needs a symmetrical voltage of ± 40V. At full power (100W at 4Ω) the current is 2.5A and at load 8Ω with power 70W the current is 1.1A. For economy and simplicity, we use a non-stabilized power supply. By its nature, however, such a power supply will have a fluctuation in voltage.
If the power supply at full power output is 40V it means that with less power the supply voltage will tend to increase. However, since the output elements have a maximum operating voltage of 100V, which means ± 50V, the design should be done so that these limits are not exceeded. For this reason, we define the power supply voltage to ± 46V so that we also have a safety margin. However, the ± 46V only leaves a margin of 6V between maximum and minimum load. However, this means that the internal resistance of the power supply must be very small. A good way to get a little resistance is to use a good transformer.
Given the good transformer, a bridge-rectifying bridge and some electrolytic capacitors and we have the power supply we need. The fuses on each power line are used to protect the circuit from short circuits, because the T7 and T8 protection circuits are only short-lived until the fuses are blown. For stereo performance we need two amplifiers and therefore two power supplies.
Resistors R18 and R19 must have a PCB spacing of at least 5mm. This generates a good bleed and hence good heat dissipation. Transistors T7 and T8 as well as capacitors C7 and C8 are mounted on the heatsink.
The heatsink must be 1.2 ° C / W. If a heat-conducting paste is applied on both sides, then a heatsink with 1.8 ° C / W is sufficient. It is known that if more than one transistor is placed on a heatsink then we have to divide the thermal resistance of the heatsink with the number of transistors. Therefore, if both transistors (T7 and T8) are placed on a heatsink, then the type should be 0.6 ° C / W or 0.9 ° C / W.
In no case should there be direct contact of the transistor with the heatsink, because the collector is connected to the transistor cover and thus would cause short circuits. For this reason, insulators such as, for example, Mica.
Before connecting the capacitors C7 and C8 (see Fig. 4), insulate their terminals by placing eg. Plastic macaroni.
The connections to the printed circuit must be made with the shortest possible copper wire.
The input jack must be connected to an AF cable in the printed circuit (coaxial cable should be grounded). The best way to connect the ground to the amp printed box is to ground the input jack. The cable and the plug must be positioned as far as possible from the other components and cables to reduce the possibility of back-up and noise from the 220V network.
The two windings of the secondary are completely separate. That means four wires will remain in our hands. To see where we connect each one we get two in luck and unite them. Then we measure the voltage in the other two. If the voltage between them is 60V AC, then connect the two wires together with the earth of the power supply and the other two in the remaining free points. If the voltage is 0V, then we need to change one of the edges we've joined with a free one. Electrolytic capacitors must be attached (due to size) to the PCB with a plastic collar or the like.
Remove F2 from the power supply after short-circuiting the input and making sure the output is not connected to anything else. Then put a multimeter in the 1A DC region at the ends of the fuse block, and with the (+) in its side with C2.
Turn the potentiometer to its end in a direction opposite to the clock. Check all connections and connect the power adapter to the network. The multimeter should point around 0A. If the reading is greater then an error must be present and you must immediately stop the power supply. In good condition the current should be about 100mA which with P1 must be set to 80mA. This means that the resting current in the power transistors will be about 50mA.
This is the whole process of adjusting the amplifier. We replace F2 fuse, after first shutting down the power supply. If an error has occurred, we can easily correct it by comparing the voltages at different points in the circuit. These voltages have been measured with the speaker connected and the input disconnected.
R1 = 120k | R2,R5,R6 = 3k3 | R3 = 120Ω | R4,R8 = 680Ω | R7 = 1k5 | R9 = 5k6 | Α10 = 1k2 | R11 = 2k7 | R12,R13 = 270Ω | R14,R15 = 15Ω | R16,R17 = 220Ω | R18,R19 = 1Ω/9W | R20 = 10Ω | R21,R22 = 1Ω | Ρ1 = 1k
C1 = 470 pF | C2 = 10μF/63V | C3 = 150pF | C4 = 1000μ/4V | C5 = 220μ/40V | C6 = 47pF | C7,C8 = 560pF | C9 = 47nF | C10,C11 = 680nF | C12,C13 = 100nF
Τ1,Τ2 = BC556Α | Τ3,Τ5 = BC547B | Τ4 = BC639 | Τ6 = BC557B | Τ7 = BDX67B,BDX67C | Τ8 = BDX66B,BDX66C | D1 = 9V1/1.3W | D2,D3 = 1Ν4148,1Ν914,BAW62
2 heatsinks 1.2 ° C / W or 1.8 ° C / W (see text) | Insulators for power transistors (mica)
R1, R2 = 3k3 / 1W
C1 = 100nF | C2, C3 = 4700μF / 63V
D1, D2 = LED | B1 = B80C 3200/5000 Rectifier (Bridge)
F1 = 1.4A (approx.) | F2, F3 = 2.5A (approximately)
Toroidal transformer = Secondary 2 x 30V - 2x 3,75A | S1 = bipolar switch | Two fuses for PCB | A fuse box for 220V