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Very nice, thanks!Hy run,
Here is a circuit for an opto receiver:
See further proof women are a bad idea! Shame they are not more like Oscilloscopes and then you could switch them on only when needed.Hi run.
Sorry the circuit took so long, but my missus gets unreasonable and expects me to do non-technical things from time to time, so ended up shopping in Bristol most of yesterday.
Not 100% certain what you mean, but I want to measure different light intensities to monitor and compare them (with two or more detectors) at the same time (at the same freq as the uv pulses from the other circuit).Hi again run- only a question:
(1) Do you need to monitor the light received power all the time while data is being received
(2) or would it be acceptable if you could switch to either datamode or light received power measurement mode.
I think I know your answer (1), but thought I would ask just in case.
spec
Just a rookie, sorryrunarh. you seem to be avoiding specs. Is there a reason?
To detect intensity requires a a peak detector not included which can introduce distortion if not buffered from the signal. Generally a verty high gain limiter(comparator) is used for front end and thus intensity cannot be derived from the output. You would need a linear wideband amp as the front end to measure it's analog peak, perhaps with very high GBW such as my previous post suggestion, depending on your data rate.Very nice, thanks!
What changes would I have to do to allow it to detect the intensity of the light, as it should give different outputs if the light is brighter/weaker?
I should have specified this earlier, sorry.
To detect intensity requires a a peak detector not included
This is just s meaningless unqualified statement about 101 circuit design. The OPA192 has a very high impedance input so the peak detector is isolated from the signal.which can introduce distortion if not buffered from the signal.
Not correct with this diode which produces a current. A current to voltage converter is used to get a workable voltage signal. Feeding the current into a virtual earth point means that no parasitic capacitances need to be charged up and down. Thus speed is optimized and distortion is minimized.Generally a verty high gain limiter(comparator) is used for front end and thus intensity cannot be derived from the output.
You keep on about specifications but you do not seem to use specifications yourself. The OP has stated that his data rate is 1K baudYou would need a linear wideband amp as the front end to measure it's analog peak, perhaps with very high GBW such as my previous post suggestion, depending on your data rate.
This is another generalization without any figures. It is perfectly acceptable to use an op amp as a peak detector, in fact in the main they are. And in this case the opa192 has a minimum source and sink current of 65mA, a gain bandwidth of 10MHz and a slew rate of 20V/us rate. It also has a minute indecision window around 7uV, so it is no slouch. I do agree that a comparator would be faster but that is unnecessary in this application. Also, finding a fast comparator to to handle a 12V peak signal would be a challenge.Since Comparators don't use feedback and are thus inherently stable ( if supply and Vref is clean, and thus are designed with much higher slew rates than Op Amps like OPA192
Hardly any circuits have specification included with the circuits posted on ETO. But at least I give you the data sheets so you can work out the performance of the circuit for yourself. But you will have to get all the facts from the data posted in the thread to see what the OPs requirement are. You will also have to make an attempt to see how the circuit works. If you don't understand, or need clarification, just ask like most other members.We still don't have a spec for your slew rate, data rate or signal level. (big hint)
Hello Tony,
spec
Hello Spec,
Yes I am aware of the parasitic positive feedback potential for spurious resonance in high speed comparators.
I may have assumed too much. I expected ultrafast fluorescence spectroscopy from the question with UV stimulated green light, which is performed in nano or fempto seconds.
The solution I was thinking of for in-situ probe detection ( OE conversion) is the same used in camera photo detectors with a CIE eye-corrected flat response and is fairly accurate with a dark current well under 1uA.
They are cheap and readily available at D-K. I used many of them in a design of an optical light meter for testing LEDs of any visible colour straight into a built-in portable cheap DMM.
I suggested this approach on the assumption that the user might not know how to design the optical interface with an optical splitter between emitter and detector for reflected fibre endoscopic detection. With this approach a better defined volume of medium. With an in-situ emitter<>detector, a controlled volume of medium for a transmission method can be conducted. This avoids the Lambertian Response of an endoscopic method of unknown volume of medium.
The circuit is trivial with a low power 5V three terminal low-current regulator, a defined resistor or switchable set of values and a multi-meter (DMM) or ADC data collection system.
The package is the same as the 5mm LEDs.
View attachment 98669
View attachment 98667
I would choose a 10 ms UV pulse with whatever duty cycle is desired and then use the Analog output for the experimental data with an accuracy of < 1% after calibration with a known light source.
If one does not need optical corrected intensity vs wavelength , then any old Sharp/Vishay PD will do with 0.5uA/uW.
I tend to think of overall requirements, not just what an inexperienced OP asks for.