Optocouplers are some of those things that are deceivingly easy to a beginner, but also hard to use correctly. If you are reading the datasheet carefully, you are in for a big surprise.
CTR (
Current Transfer Ratio): sensitivity of the coupler - the ratio of the transistor output current vs the LED current. e.g. for a 50% CTR, you have to drive the LED with 10mA and the transistor switches 5mA.
The CTR spec is very loose and likely this series of optocouplers are just different bins of the same parts. They don't even include a max value.
This ones show both min and max value from 100% to 200%. The following shows the part to part variation of a for a small samples of a (different) optocoupler.
CTR of a small sample of PS2021 optocoupler
Analog feedback
The optocoupler is commonly used as an analog feedback in an isolated power supply. The error voltage is pass back as a current sink or source to close a negative feedback loop of a regulator across a voltage barrier.
I played around with the isolated power supply design from previous blog with feedback from the secondary side. The voltage regulation is very tight and virtually stays at around 5V from 5mA to125mA load.
I have no idea on how well it would work with the loose CTR specs.
Passing digital signals
They are one of those things that was made with compromises. In order to make the device sensitive, they made a big photo-transistor at the expense of large parasitic capacitance (
Millar Capacitance) and and suffers from slow speed.
It'll be pretty sad day if I don't try to make something slow to go fast. I played around with LTSpice and came up with something that is not covered by the app. note.
The values I used are determined by the optocoupler CTR.
Optocoupler circuits: simple, medium and complex
To see their performance, I put them side by side and feed each of these circuits with the same 5 pulses of 100kHz signal (200kbps data rate).
Top trace: Input (cyan), bottom traces outputs from optocoupler circuits
Simple coupler circuit (green)
CBC (base collector capacitance) aka
Millar Capacitance. It slows down the transistor. Datasheet typically uses 10V and a load resistor of 100R as their test circuit. CBC is low at higher voltages and the small pull up value help with the rise time.
Note: the scale from Low to high (left in log scale) is very different from High to low (right in linear)
The speed is much slower when you use a large pull up resistor and lowering the voltage. The values I picked is might be useful for low data rate may be lower tens of kilobits per second. e.g. asynchronous serial. It should only be used with a Schimtt Trigger input to clean up the slow rise and fall time.
The middle circuit (blue)
The optocoupler is the first stage of inverter that drives a transistor of a second stage inverter. Its output range is clamped to a diode drop of the transistor base voltage. The operating point is not a good spot for low CBC.
Input (Cyan), Q1 base voltage (Purple), Output (Blue)
In spite of that, it only take about 100mV change in base voltage for the transistor to turn on or off. It is a good compromise to squeeze an extra bit of bandwidth out of the old optocoupler. There is a bit of inconsistency in the timing. A timing analysis should be made for setup/hold time for protocols that require coordination of multiple signals e.g. SPI.
The more complex circuit (Red)
It bypasses the Miller effect as it uses the transistor junction as a photo diode. The comparator threshold is set to about mid point of the input (~100mV). The speed (propagation around 500ns) is limited by the $0.20 LM393 type of comparator that is used to amplify the signal.
You can speed up the photodiode even more by using a
transimpedance amplifier. Because of the feedback, the voltage across the diode junction is maintained around 0V, the switch time is greatly minimized. However high speed amplifiers cost more and I don't have a whole lot of them.
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