[sdiy] phaser cv law
JH.
jhaible at debitel.net
Wed Feb 14 14:25:19 CET 2007
>One thing about incandescent vactrols though, is the
>thermal inertia of the filament, which has a considerable
>effect on the overall current/resistance transfer, particularly
>at high frequencies.
Yes, absolutely.
Some non-optoelectronic phasers approximate this with an RC low pass, but
it's only an approximation.
My Compact A clone (I don't know if the original has this or not) shows a
crazy extra effect: The front panel lamp (which indicates the inverse of the
lamp that drives the LDRs) sometimes "jumps" a little before it gets to its
maximum brightnes / sweep turning point. This only happens _sometimes_,
every few cycles. I suspect it's a self-heating thermal effect - Vbe of the
driving transistor decreasing with temperature, look at these crazy
shematics! - and gives a nice randomizing effect.
>One popular phaser LFO waveform is derived by taking
>a sine wave, full wave rectifying it, and inverting the
>result (giving a slowly swept botom & fast swept peak).
I bet it's quite close to the Tau / Aries 1/x function. (or law?)
This helps to achieve a thru-zero modulation effect. And it (1/x at least)
would be the best approximation for a moving sound source, i.e. rotary
speaker effect.
The Compact A and Mutron, as far as I can tell, are doing just the opposite
of this, though. Where -abs(sinwt) modulation or a triangle modulation with
1/x law accelerate the frequency sweep towards the high range, an
incandescent lamp would decelerate.
JH.
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