Prev: Fun with positive feedback
Next: IEEE was Re: Photodiode readout without transimpedance amplifier
From: john on 13 Jan 2010 12:00 On 12 Jan, 10:22, Ian Bell <ruffreco...(a)yahoo.com> wrote: > Suppose you have a simple pot divider consisting of two equal value > resistors, say 10K each. Across the upper one you connect a series LC > circuit that resonates at 3KHz or thereabouts. If you drive this network > from a low impedance source and plot the response across the bottom > resistor, the Q of the resulting peak is not the Q of the series LC but > rather is determined by the pair of LC values. For example, choosing > l=150mH and C=18nF gives a Q of just over 2. Choosing L= 1.5H and > C=1.8nF gives a much higher Q. > > What I need is a simple means of calculating L and C given the pot > divider resistor value and desired Q and f (assuming the Q of the LC > itself is much higher). > > Cheers > > Ian I'd see it as a Q 'definition' oddity. If the pot is set at say the 80%, ie 4k/16k position then there's an output baseline of 0.8V which simply can't be measured using the normal method of 71% of peak voltage. The skirts are just too high and the resulting curve shape 'looks' decidedly low Q. But, subtract the 0.8V offset and remeasure Q as normal, this gives the 'real' working Q value of XL/R. ('R' in this case appears as 3200ohms hence the real Q is simply proportional to to the L or C reactance value at resonance. ). Set the pot at say the 10% position and the standard Q definition becomes more and more valid.
First
|
Prev
|
Pages: 1 2 3 4 Prev: Fun with positive feedback Next: IEEE was Re: Photodiode readout without transimpedance amplifier |