Class A, AB will just suffer from all kinds of inefficiencies. however with that said, a "well designed" Class-D amplifier will handle attached load with pleasure, with very little thermal problems, and yes, it is actually a switching converter with its front-end designed to modulate to an audio signal.
Don’t think so. Keep in mind that audio amplifiers are thermally not designed to deliver continuous RMS power. They are designed to deliver temporarily maximum power in loud passages in music. Continuous average power is usually 1/10 of rated power.
Linear class AB are in general not suited, due their large inefficiency and difficulties with complex loads over 45 deg phase shift. Better are Class-D amplifiers (switch mode amplifiers). I have had good results with a 400W Hypex class-D amplifier module and a reversed 230V/32V 500VA transformer. Those can easily handle complex loads up to 90 deg phase shift, if the PSU caps are big enough (>10.000 uF). But not for long time at full load. With sufficient heat sinking the Fets are not a problem but the on board powers supply bypass caps run pretty hot and the output choke as well (over 100 deg. C).
If you want to try, always put reversed bypass diodes from the output to the supply rails to handle leakage inductance of your step-up transformer. The feedback loop is usually not fast enough to track fast high voltage transients caused by that inductance and those transients can destroy your output transistors.
I think you just re-answered me.
The class-d amplifier is far different from a traditional amplifier that uses a BJT, by design a well designed class-d output FET`s operates in their saturation region, Rds(on) dominates.
FET technology for class-d amplifiers has matured over the last 8 years dramatically. Have you seen the specification of some them? they are darn impressive.
Example
A irfb5620pbf exhibits a 72mOhm Rds(on), offers a VBRDSS of 200V and offers a gate channel capacitance of Qg of only 25nC, with this data you surely understand that if we designed a PA amplifier with a DC - bus +/-90VDC, and lets say for argument sake the supply dropped +/-89Vdc at full load, with a 2-ohm load connected, the continuous RMS rating would amount to V^2/R = 3.9kW (rms) also note I assume the FET`s are paralleled to achieve this level of power.
The thermal efficiency is very good some well designed Class-D designs requires almost no heat sinking, I've built one (a kit) where I was able to play music at loud volume at 100W (for an hour or so) with "no heat sinking" its almost unbelievable!, note this is of course achievable because of large programmed dead-time during switching times. to achieve efficiency. A commercial class-d PA amplifier using a no heat-sink approach like the Behringer iNuke amplifiers. (see attachment no heat-sink and this is rated at 2kw > @ 8ohms)
Why do you feel a Class-D configuration is incapable of delivering continuous RMS power into a load? In all reality its a switch mode converter with the same efficiency figures irrespective if it amplifiers audio, Its way more superior in efficiency than its A, AB brothers.