Z = R + jXl -jXc
Yeah, it's something like that (i've "misplaced" my memory of the exact formulae- I'm a firm believer of deriving things from first principals)
However, this totally neglects the fact taht this is a complex function.
Becuase you've got an oscillating supply, and a phase/frequency dependant component (the capicitor) you've got to factor in that little i (you know, the sqrt(-1) fellow).
If you ignore the complex part, then you get these simple equations like Z = R + jXl - jXc, which I think comes from something like Z = R + jcis(fl) + 1/jcis(fc) or some crap like that. If you're doing simple electronics for homework, then the equations you're loooking at will be fine.
If, however, you want to use this in the design of audio gear, then you cannot ignore the complex part of this equation, as it deals with phase shifts etc. This is one of the reasons that most frequency-dependant analouge resistors (EQs, HPF/LPFs) rarely go above +/-24dB / octave, as the phase shifitng becomes uncontrollable.
It's also why expensive EQs sound better, they don't taint the phase so much as cheap ones that jsut have simple vRLC or RLvC cuircits
Once again, duty calls, so I must away, however if this thread is still alive I'll fire up the brain and write out some lengthy, dry RLC posts if you want...