Larry,
Good points. Your reference was specifically to linear supplies so that the point at which the rectifier conducts, and stops conducting, influences the shape of the pulse. And to some extent, the inductive leakage of the associated power transformer might have a strong influence. With a bridge rectifier in a linear supply, we are conducting on some portion of the |sine| and the larger the capacitance, the sharper the transition. I guess I should have added the inevitable 'all things being equal', and to make those things actually equal, one would pad to compensate for the lowering of esr (ignore the esl, multiple inductances in parallel, or assume we're not adding multiple of capacitors, but just substituting a bigger cap with equivalent inductance) so that we could see only the effect of increased capacitance which would be grossly wrt noise, a lowering of pole frequency of the formed filter.
But in the context of a switching supply, assuming some form of PWM, we already know shape of the rectified pulse, prior to any inductive or capacitive massaging its a rectangular shape, and its the spectral content of those sharply defined edges that is so frigg'n problematic in switching supplies.
So I'm digging myself deeper and deeper into this hole of power supply design in which I can't claim any particular expertise. My point is simply that first order appoximations and off the cuff calculations are a poor substitute for actual empirical verification. All I can say is that I've yet to meet a component that didn't benefit from the proper power conditioning.
Has any one ever tried a string of car batteries to run a power amp?
Actually, Gordy has build a stereo UCD 400 poweramp powered by dual 48v rails of gell cell batteries