Hello Spehro and Dave, Spehro says: > RC time constant is just R * C, your formula is correct for 1/f (Xc = R, so > 3dB down), or lose the 2*Pi and calculate f in radians/sec. Dave says: > Actually, what we refer to as the "RC time constant" is usually the > product T = RC, without multiplying by 2*pi. oh, big confusion here. Now it clarified. Thanks. Dave says: >This product is used when calculating the time-domain response of an RC >circuit such as above: when a voltage step is presented to the input, >going from zero volts to some voltage Vin, the output waveform is >described by the expression > Vout = Vin * (1 - (e^(-t/T))), >where t is the time elapsed since the input voltage step and T = RC. Sorry for my math ignorance but what's that "e" in the formula? >(I'm not disputing your frequency calculation, just clarifying the usage >of the term "time constant".) thank you again for clarifying this. Dave says: >> IN----R1----*-----*----OUT >> | | >> C R2 >> | | >> GND GND >The way to do this is to consider R1 and R2 to be in parallel with one >another with regard to AC, since R1 is connected from C to a circuit >node (the input) which has zero impedance with respect to ground (that >is, the input is driven by a voltage source), just as is R2. So in >terms of the resistance that the capacitor "sees", R1 and R2 are in >parallel. Great explanation. Spehro says: > If you're not familiar with this method, here's a web page > that 'splains it fairly well: > http://hyperphysics.phy-astr.gsu.edu/hbase/electric/thevenin.html thank you again. Great site. Spehro says: > > IN----R1----*-----*----R3----OUT > > | | > > C R2 > > | | > > GND GND > > The same as above unless there is loading on the circuit. ;-) > If you short the output to ground and look at the current, then the > 3dB down frequency would be > > f = 1/( 2 * Pi *C * R1 || R2 || R3) > > where A || B || C = 1/(1/A + 1/B + 1/C) Good. Dave says: >And finally, if R3 is feeding into a load resistance Rload which is >neither infinite nor zero, then you do the calculation as above but with >(R3+Rload) replacing R3 in the formula. Actually it's connected to the non-inverting input of a comparator. I think this makes the calculation more complex as we have the input impedance of the comparator, the positive-feedback resistance (schmitt trigger) and the pull-up resistor at the comparator output. But your lesson give me clues of what to do and what to expect. Thank you very much again, Brusque ----------------------------------------------------------------- Edson Brusque C.I.Tronics Lighting Designers Ltda Researcher and Developer Blumenau - SC - Brazil Say NO to HTML mail www.citronics.com.br ----------------------------------------------------------------- -- http://www.piclist.com#nomail Going offline? Don't AutoReply us! email listserv@mitvma.mit.edu with SET PICList DIGEST in the body