Let me first recommend that you do not use
ambient or DC-biased illumination for the
photodiodes to receive. This just begs for
modulated-optical noise pickup from
lighting, windows (picking up vibrations and
turning them into reflection-modulated
light). Using a carrier frequency like 1MHz
(or higher) to drive D1-D6, a narrowband filter
and AM-demodulating would be better. This
is a common approach to IR beam-break
detectors and such, to tamp down ambient
light "spoofing" and any attempts to defeat
by a simple flashlight. Might be good to have
a DC "baseline" that keeps diodes slightly
lit, and a 1MHz square wave summed in
(laser diodes have a threshold current; LEDs
have their own "threshold" (Vf) and would
probably behave better if you didn't put them
full dark every half cycle).
Now your photodiodes (D7-D12) appear to
have no DC bias. That means they must
work in photovoltaic mode, but that will crush
optical-electrical voltage gain. You'd be better
off with a reasonable reverse bias and resistor
load (might make this adjustable, until you
find the range on your illuminator / filter /
demod) to use photoconductive mode for
much higher signal (hence better SNR).
Voltage is a relative measure. Thus a voltmeter has two wires: the black one as reference, the red one as measurement input.Google tells me I want to apply negative voltage to the diode, But I've only got +9 Volts. And biasing the op-amp at half that. Would using ground be the negative in my case? as it is relatively below my bias voltage.
I posted an article from National Semiconductor who says that reverse bias increases noise and photo-voltaic reduces noise. Sharp Electonics says the same.At this point I can't tell if people are contradicting each other. I thought my current setup was photovoltaic like #13. But some people are telling me to reverse bias the diode for photoconductive operation to improve SNR.
I posted an article from National Semiconductor who says that reverse bias increases noise and photo-voltaic reduces noise. Sharp Electonics says the same.
You can ground the anode of the photodiodes when you have a dual-polarity supply.
You say grounded "one side" of the photo-diodes but which side?
You "flipped" connected the cathodes to ground??
It does not make sense. Please sketch a schematic.
I think shorting together all the photodiodes causes shadows on some of them to affect the level of a string that you are playing. Use a separate opamp for each photodiode and mix them with the 2.2k resistors.
Hi,
Circuits have benefits and drawbacks.
When audioguru says that the non biased photodiodes are less noisy then this will be correct.
Non biased there will be much distortion, rectifying style. I can't imagine that it will work satisfactory.
Noise:
There will be voltage noise, current noise,
... noise from the photodiodes, resistors, Opamp
... noise from power supply or induced
... noise from the ambient light
When you say the noise does not change, then maybe the noise source is not the photodiode circuit, maybe the noise comes from elsewhere.
Thus I recommend to analyze the noise. Use your audio card, samplee the noise with still guitar strings in a dark room.
Then run an FFT on the sampled data and show the result. Free tools are available.
Klaus
Could you explain why six amplifiers would be better? Wouldn't the signals and noise get summed all the same?
In my opinion, the benefits of summing random noise to attempt a zero average is not worth the effort. Yes, there will be some noise reduction but your underlying problem is trying to amplify such a tiny voltage from the outset. The more you have to amplify, the greater the resulting noise will be, that's electronics (or is it physics?) for you.Lower noise op amps are for sure something I need to try, but the question is if I should keep a parallel setup or not.
1. Each string vibration is recorded by one photodiode; the frequency and amplitude must be correlated with the photodiode output signal. Due to positioning (in)accuracies or signal amplifications etc (there can be many other reasons), we need to normalize the output from each string (as seen from the photodiode output). If you sum all the signals, this information may be lost.
2. The photodiode is not looking at the whole string; it is looking only at a very small part of it. For example, the photodiode may see at the middle of the string which is good for the fundamental but not for the odd harmonics. The positioning of the photodiodes is therefore very critical in my opinion.
3. The output from string instruments is polarised and this cannot be caught by a single photodiode; you need at least two per string in quadrature.
4. The phase of the outputs must be corrected before you add them and send it to the final amplifier. Each amplifier may have produced different phases because different strings may produce different frequencies.
5. The body of the instrument may act as a resonator and you need to apply frequency corrections for each photodiode because it catches only the motion of the string.
In my opinion, the benefits of summing random noise to attempt a zero average is not worth the effort. Yes, there will be some noise reduction but your underlying problem is trying to amplify such a tiny voltage from the outset. The more you have to amplify, the greater the resulting noise will be, that's electronics (or is it physics?) for you.
I think with a suitably designed optical sensor you should get tens if not hundreds of mV directly from the sensor, enough to drive a final power amplifier with little or no other amplifier stages. C_mitra's comments are very valid though, at least for acoustic guitars. I'm not sure how the solid body of an electric guitar influences the sound it makes.
Just an idea, if it is practical to implement - have you considered an interruptive sensor rather than a reflective one. I had the idea of using a slotted optocoupler with the string passing through the gap.
Brian.
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