kelly0303
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Thank you for this! I actually found this: https://ned.ipac.caltech.edu/level5/Leo/Stats4_5.html I think this is what I was looking for.Dale said:Ok, so having reviewed the NIST document and your post I think that I understand the “official” procedure.
Ok, so this is a type A uncertainty with a standard uncertainty of ##u_s = 100##. If you are trying to measure the mean of the signal then this uncertainty contributes to the uncertainty of the measurement. But if you are trying to measure an individual value of this signal then this uncertainty is not relevant since it is part of the measurand.
This is then a type B uncertainty with a standard uncertainty ##u_1 = 50/2\sqrt{3}=14##
Which is a type B standard uncertainty of ## u_2 = 200/2\sqrt{3} = 58##
So if your goal is to measure the individual signal value you would use the propagation of errors. For that the combined uncertainty is ##u_c = \sqrt{u_1^2+u_2^2}/2 = 30##
But if your goal was to measure the mean of the signal then I am not certain, but I think that the combined uncertainty would be ##u_c = \sqrt{u_s^2 + u_1^2/4 + u_2^2/4} = 104##
I am not confident about that last one.