I need some help deciphering the circuit
I know that P1 controls the voltage and P2 controls the current, but I can't figure out how the opamps work.
My instructor wants me to build it, but I want to understand it first.
A universal power supply unit
So that we don't always have to rely on batteries for experiments and testing our circuits, we should get a universal power supply unit for our workshop. As true hobbyists, we will of course build it ourselves. As a blueprint for this, I offer my laboratory power supply, which I built more than 30 years ago and which still works today.
The terms voltage source and current source are often used in the same context. Strictly speaking, however, they are two different things. A voltage source provides a stable output voltage that does not change when the load at the output changes. A current source supplies a constant output current and regulates the voltage required for this. For our laboratory power supply, it is desirable if it combines both properties. It supplies a constant voltage to operate our circuits. However, if a certain maximum current is reached, it no longer allows the current to increase further. In this way, we can prevent the components from being destroyed by excessive current in the event of errors in the test circuit. In addition, our power supply unit is not affected by a short circuit.
At the time, I opted for a power supply unit that delivers two independent voltages of 1-30V at a maximum current of 1A. The circuit described is therefore completely duplicated.
A few comments on the circuit. The power transformer with an M102a core is self-wound. The choice of active components is actually quite uncritical as long as the limit values for voltage, current and power dissipation are adhered to. A Graetz bridge 3PM1 was used as the rectifier. Of course, you can also use 4 individual rectifier diodes. This is followed by a large charging capacitor. When selecting it, remember that it charges with the peak voltage of the AC voltage before rectification. At 40V effective AC voltage, this is about 56.6V! The Z-diode SZX21/1 at the input of the first operational amplifier supplies a reference voltage of approx. 0.75V. As Z diodes cannot be manufactured for such low voltages, this is actually a normal forward biased silicon diode. I have simply used the base-emitter diode of a miniplast transistor for this.
A rotary switch can be used to preset the desired maximum current in 5 stages (10mA, 30mA, 100mA, 300mA, 1A). The fine adjustment is made with the potentiometer P2. The output voltage can be set with P1. At the time, I did not use precisely calibrated scales and always set the desired values beforehand using a measuring device. Of course, you could also integrate suitable measuring instruments in the housing. The two power transistors (SU 169 and SD 337) are screwed onto aluminum heat sinks for heat dissipation. Of course, sufficient ventilation must also be ensured in the housing. The resistors on the output switch must be designed for the power losses that occur there, especially in the high current ranges.
Here is the Link to the German Website:
https://technik.reicke.de/bauanl1.phpAlso, if anyone could explain to me how you go about deciphering schematics that you might not quite understand at first, I'd be grateful!