Class A means all the current, all the time, so "less demanding" is a matter of definition. What is different about Class D is the amount of HF energy they require, all the time, and the fact that the power supply rails can directly modulate the output signal, something not true in Class A or AB amps (within reason, the reason being the PSRR of the amp).
For cap models, most manufacturers provide static ESR and self-resonance; some provide shunt conductance as well. You can use those to derive a simple RLC(G) model of the caps:
Series R = ESR
Shunt R = 1/G
C = nominal C value
L = series L to create the self-resonance point for the series LC
HTH - Don
OK,
I'll give this a try although I feel really lost trying to use LTSpice for the moment.
Please bear with me, as I am almost feeling like doing painting by numbers...
The datasheet does not provide any "direct" information concerning self-resonance as far as I can tell.
After reading up a little I found the following formula for calculating the self-resonance of a capacitor:
1/(2*pi*sqrt(L*C))
ESR as per datasheet: 0,016 Ohm
ESL as per datasheet: typically 16nH
Capacitance @ 100hz: 15000µF
giving me: 1/(2*pi*sqrt(0,000000016 H * 0,015 F)) = 16137,4306091976 Hz
If I get it right my capacitor is capacitive up to roughly 16 kHz, resistive at the calculated frequency and inductive from there on..
Should I just model a capacitor using the ESR for R, the ESL for L and the capacitance @100 Hz for C ?
I actually found a capacitor model for Spice, the above is for my better understanding only.. or non-understanding.
Max