Power output of tube amps compared to solid states


I'm having a hard time trying to figure out how tube amp power output relates to solid state power output. I've been looking at the classifieds for tube amps and I see lots of tube amps with 50w or 60w output, but nothing close to the 250w output typical of solid state amps.

So I have no idea what type of tube amp is required for my set up, right now I'm using totem forests with a required power rating of 150w-200w at 8ohms. The bass is so powerful on these that I have the sub crossover set to 40hz.

My question is, are tube amps so efficient that 50w from a tube sounds like 150w from a solid state? Or will 50w output from a tube severely limit how loud I can play my speakers? If so, are tubes usually meant to be driving super-high efficiency speakers?

I had previously tried a tube pre-amp with a solid state power amp (both musical fidelity) and didn't like the results because the imaging suffered greatly, even though the music sounded nicer from a distance. Now I want to try a solid state pre-amp (bryston) with a tube power amp (no idea which brand to look at), but I don't know how much power output I need or if it will even be possible with my speakers. Does anyone know what I would require?
acrossley
"Do tubes have the same "advantage" in preamplifiers?"

That's a good question! For many like me with tube-unfriendly speakers, the pre-amp (and source perhaps) are the practical places to introduce tubes.

I love my ARC sp16 tube pre-amp, but I do wonder if a good SS pre-amp could also deliver for similar cost or less once the speaker/amp optimization has been achieved.
I think they do. It would be really tricky to build a zero-feedback transistor preamp. With tubes you can do three stages of gain between the LOMC phono input and the line out, I doubt that the same can be said of transistors, at least, I've not seen any so far.

I have an additional comment about distortion that Joe mentioned- that of, shall we say, 'dynamic distortion'. Its my opinion that we need some sort of distortion test that uses a non-repeating waveform similar to what you see in real music. What Chaos Theory is saying about this is that sine waves represent a stable state in an amplifier circuit that might otherwise have chaotic response. BTW Norman Crowhurst pointed this out 50 years ago in his writings about negative feedback. Chaos Theory really seems to point to the idea that negative feedback is a destabilizing factor in amplifier circuit design, in fact, going so far as to call it non-linear.

This seems to fly in the face of traditional theory, where negative feedback occurs as something to increase linearity. But what we find by its application is that the energy of the distortion (nice calculus segue here BTW) is not changed at all- it is instead spread over the spectrum as a harmonic noise floor injected into the circuit's output. In addition, in-harmonic distortions are created due to inter-modulations at the feedback node.

The way the ear deals with this is interesting- our ears can penetrate natural noise floors like hiss or the wind blowing by about 20db, but can't do the same with this harmonic noise floor, which thus masks detail that exists below it. This is one reason why zero feedback circuits tend to be more spacious.
There are many here much more qualified than I am to answer these questions, but, it would appear to me that it really wouldn't be an issue with preamp. I would think most pre-amps have more than enough steady state power necessary to drive a power amplifier. Head room and it's duration wouldn't be a necessary consideration.
Atmasphere, would you consider a passive pre a ss device? If so, where would the feedback be there? It seems as though some of your arguments are based upon opposing theories rather than laws.
Trelja, thanks for the kind words.

Unsound, are you referring to the Threshold S/500? If so, there must be some inconsistencies around what is meant by "double its rated power for several minutes" . . . because I remember this amplifier having rather conventional headroom characteristics (but it's been at least 15 years since I've worked on one, so I may be wrong). To clarify, what I'm terming "dynamic headroom" will generally manifest itself as the ability to generate additional unclipped short-term voltage and current beyond the steady-state clipping power.

If "short term" means several minutes . . . then the limitation that keeps short-term capacity from being long-term capacity is almost surely thermal dissapation, not energy storage or output device current-limiting. The only SS amps that I can think of that exhibit this characteristic are what I would call "asymmetrical class H" operation, like the old NAD "power envelope" design. This works by having the amplifier operate from lower-voltage rails most of the time, but for large-signal peaks there is another set of commutating transistors (like conventional class G or H) that pulls the voltage up to a higher rail, and then keeps it there for a fairly long time-constant. The reason why it doesn't operate at the higher rail all the time is purely thermal . . . so I would actually consider it this design a higher-powered amp with thermal limitations, rather than a lower-powered amp with lots of headroom. But that's purely terminological I guess . . .