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The Operational Amplifier
The name is literal. John Ragazzini and his colleagues at Columbia coined it in a paper of May 1947 about wartime work on gun directors, and the amplifiers in question were called operational because they performed mathematical OPERATIONS - adding, scaling, integrating, differentiating - inside a machine that solved the differential equations of a shell in flight while the shell was still in the gun.
The circuit is Black's feedback amplifier with the loop closed by two impedances instead of two resistors, and the argument for it needs no electronics at all. Give the amplifier enormous gain and an inverting input. For the output to sit anywhere sensible, that input must be within microvolts of zero, so no current goes into the amplifier and whatever arrives through the input resistor has to leave through the feedback element. That is Kirchhoff, and it means the answer is a ratio of two components. Put a capacitor in the feedback path and the same argument gives you an integral.
It is the same integral the wheel-and-disc machine performed with friction sixteen years earlier, and it wins for a reason that has nothing to do with accuracy: both are good to about a tenth of a per cent, and one takes a day of gearing to set up while the other takes a few minutes of patch cords.
It loses on one column, and that is worth knowing. A friction wheel parked at a radius stays there all day; a charged capacitor leaks, and the amplifier's own offset voltage and bias current are integrated along with the signal. A general-purpose bipolar op-amp integrating onto a microfarad will hit the supply rail in under two minutes with no input at all. That is why every analogue computer has a reset button and no differential analyser ever needed one.
මධ්යම
3 hours
උපදෙස්
1
1
Two resistors decide everything
Two resistors decide everything
Wire a TL072 as an inverting amplifier, 1k in and 100k back, on a split supply. Feed it 100 mV at 1 kHz and check the output is 10 V peak and upside down.
Now measure the voltage at the summing junction itself with the scope on its most sensitive range. It barely moves - a few hundred microvolts while the output swings twenty. That stillness is the entire circuit.
Materials for this step:
TL072 JFET Op-Amp (10-Pack)1 පැකට්
1/4W Resistor Kit (600pcs, 30 Values)1 කට්ටලය
Ceramic Capacitor Kit1 කට්ටලයTools needed:
Breadboard - Classic
DDS Signal Generator (1Hz-65MHz)
Digital Oscilloscope
Bench Power Supply (30V/5A)2
2
Integrate, and watch it walk away
Integrate, and watch it walk away
Swap the feedback resistor for a 1 uF capacitor and feed the input a square wave: the output is a triangle, which is the integral.
Now disconnect the input entirely and watch the output with a stopwatch. It ramps away to a rail with nothing applied. Time it, and you have measured the amplifier's offset and bias current with two components and a clock.
Materials for this step:
Electrolytic Capacitor Kit (200pcs, 15 Values)1 කට්ටලය
1/4W Resistor Kit (600pcs, 30 Values)1 කට්ටලයTools needed:
TL072 JFET Op-Amp (10-Pack)
LM741 Op-Amp (10-Pack)
Digital Oscilloscope
Stopwatch
Breadboard - Classic3
3
Virtual earth, integrator drift, and four integrators
Virtual earth, integrator drift, and four integrators
Loading Jupyter Notebook...
Tools needed:
Desktop Computer4
4
Compendium: why it needs a capacitor inside it
Compendium: why it needs a capacitor inside it
An amplifier with a hundred decibels of gain and three internal stages has three lags, and by Bode's rule those give it a slope of sixty decibels per decade well before the gain reaches unity. Close a unity-gain loop round that and it oscillates - which is exactly what the earliest monolithic op-amps did, and why they shipped with a table of external compensation capacitors and a warning about which gains were safe. The 741 of 1968 put a single 30 pF capacitor on the chip to create one dominant pole at about 10 Hz, so the gain falls at twenty decibels per decade all the way to unity and the part is stable at any gain, straight out of the tube. It is the second row of blueprint 8's table, cast in silicon and sold ten million times.
The bill arrives as a specification everybody quotes without noticing what it is. Gain times bandwidth is constant on a twenty-decibel-per-decade slope, so a 1 MHz part gives a hundred times of gain out to 10 kHz and ten times out to 100 kHz - and that is not a limitation of the transistors, it is the compensation capacitor doing precisely the job it was put there for. Slew rate is the same capacitor seen from the other side: the internal stage can only charge it so fast, so a large fast signal stops obeying the small-signal bandwidth entirely and the output goes into a straight-line ramp.
Tools needed:
Notebook and Pencilද්රව්ය
4- TL072 JFET Op-Amp10% කොමිස්1 පැකට්ස්ථානගත
- 1/4W Resistor Kit10% කොමිස්2 කට්ටලයස්ථානගත
- Ceramic Capacitor Kit10% කොමිස්1 කට්ටලයස්ථානගත
- Electrolytic Capacitor Kit10% කොමිස්1 කට්ටලයස්ථානගත
අවශ්ය මෙවලම්
9- Breadboard - Classic10% කොමිස්$10.00
- ස්ථානගත
- TL072 JFET Op-Amp10% කොමිස්ස්ථානගත
- LM741 Op-Amp10% කොමිස්ස්ථානගත
- Desktop Computer100% කොමිස්ස්ථානගත
- Notebook and Pencil10% කොමිස්ස්ථානගත
සම්බන්ධ බ්ලූප්රින්ට්
මෙම බ්ලූප්රින්ට් දැනුම බෙදා ගනී — ශිල්ප ක්රම, ද්රව්ය හෝ මූලධර්ම
CC0 පොදු වසම
මෙම බ්ලූප්රින්ට් CC0 යටතේ නිකුත් කර ඇත. ඔබට අවසර නොමැතිව පිටපත් කිරීම, වෙනස් කිරීම, බෙදා හැරීම සහ භාවිතා කිරීම කළ හැක.
බ්ලූප්රින්ට් හරහා නිෂ්පාදන මිලදී ගැනීමෙන් නිර්මාතෘට සහාය වන්න නිර්මාතෘ කොමිසම විකුණුම්කරුවන් විසින් නියම කළ, හෝ මෙම බ්ලූප්රින්ට්හි නව අනුවාදයක් සාදා ආදායම බෙදා ගැනීමට ඔබේ බ්ලූප්රින්ට්හි සම්බන්ධතාවයක් ලෙස ඇතුළත් කරන්න.



