I felt, this deserved it's own thread-
At the risk of more flames and becoming an outcast, I'd just like to flesh out a couple more points on this very contentious subject.
I read John Fields comments in the "common base thread" about the audio amplifier matching (thanks for that). But as I pondered it later on, I decided I needed to look at this further. It was keeping me up at night.
And audioph00ls just need to know. ;-)
Two nagging questions remained:
- What then is the role of the output transformer in a tube amplifier, if not for impedance matching?
- What is the design procedure for arriving at the turns ratio of the transformer? So I dug out a few old books on tube design. For the sake of discussion, consider a simple 1-tube class A stage:
The statement that I _did_ find was:
"The step-down ratio n for an output transformer should approximate a value such that n squared times the load resistance equals the resistance to be _presented_ to the tube." [1]
So then the important question became:
What is the value to be "presented to the tube"?
I eventually found an answer in a problem's solution, stating:
"For maximum undistorted power output, the load impedance for a 3-electrode tube should be equal to about twice the plate resistance." [2]
Ah ha! So the key word is "undistorted"!
So under ideal conditions, you might match to the plate resistance Rp but in order to avoid distortion, you match to
2 * Rp. I am of course, ignoring real transformer properties here but this only slightly influences.From this I have to conclude there is indeed impedance matching involved but it is purposely _not matched exactly_. For vacuum tube amplifiers the 2Rp mismatch is done for the sake of improved distortion characteristics. From a power perspective, this is suboptimal but the distortion factor overrules.
Comments?
As a secondary point, it would appear that by using a 4 ohm speaker on a
8 ohm speaker [tube] amplifier, you may in fact get more power delivered. This is because the presented load at the primary exactly matches Rp. BUT with higher distortion. Consider:If Rp = 4k ohms, and RL=8 ohms, then n~=32
SQRT(2Rp/RL) ~= 32
Attaching RL=4 ohms, results in 4*32^2 ~= 4k ohms being presented to the tube. This matches Rp=4k for max power (but with more distortion).
Warren
[1] Chapter 5 Vacuum-tube Amplifiers, Section 9. Output Transformers and Other Coupling Arrangements for Class A Power Amplifiers, Radio Engineer's Handbook, by Fredrick Emmons Terman, McGraw-Hill Book Company, Inc, 1943 [2] Article 461 solution, in Radio Physics Course: An Elementary Text Which Explains the Principles of Electricity and Radio, 2nd Edition, by Alfred A. Ghirardi (1932).