Earlier in this thread I mentioned that I had an A500 coming in from a client for work to be performed, and that I would take some measurements not only for this project, but also to show how far Jack's work went over the original design. Here's a few of the highlights from the results of those tests as based the original design, and measured from a loaded 16Ω tap:
1. The design provides 14.5 db of Positive Feedback from the cathode of the inverter to the cathode of the AF amplifier stage -- this to maximize the gain of the AF stage and therefore OL gain of the power amp section to achieve the desired sensitivity sought for this section after the Global NFB loop is closed.
2. With the PFB loop in place, 9 db of feedback is produced by the global NFB loop. I had originally estimated this at 6 db earlier -- fairly close.
3.The sensitivity of the power amp section is .32 vac (rms) to produce maximum power output (25 watts measured with only one channel operating).
4. A 10 kHz square wave is provided with the signal injected at the top of the balance control. This not only eliminates the effect of those controls and earlier stages, but also, accounts for the fact that the balance control (when centered) represents a 78KΩ series resistance at the AF amplifier's input grid (which is paralleled with a 2700 pF cap). This network is part of the power amplifier section, so its effects needed to be included with the testing. All the test results provided here were generated with the signal injected in this manner.
5. With 9 db of NFB, the internal output impedance of the amplifier is a whopping 8.37Ω, which is to be expected. With a pentode output stage and a limited amount of NFB applied, this would be the result -- not unlike that which guitar amplifier's produce. A benefit of this reduced NFB level however, is that the amplifier is completely stable whether loaded, unloaded, or into any kind of cap only load.
While this result seems rather extreme, the reduced DF produced (1.91) -- as calculated in the classic vintage manner -- is a quality that many folks favor, with its tendency being to add increased body to the sound. I have no doubt it is a significant reason why the A500 receives much of the praise it does. If the speaker's DC resistance is included in the calculation, the real DF then is even lower.
6. The output transformers are the golden nugget of the design that Jack took advantage of. Even with the limited amount of the NFB provided in the original design, the transformers could easily deliver 25 watts of power at 20 Hz (one channel at a time of course) without visable distortion, which is a real credit to HK's efforts with this amplifier. At 20 kHz, they deliver 22.5 watts under the same conditions.
7. I always measure output transformer impedance without loading the measured winding, since loading produces copper losses that distort the determination of turns ratio. Others have a different opinion on this which I respect. My own belief is that measuring the turns ratio in this manner delivers the most accurate turns ratio results, while the difference between that and the apparent increased turns ratio produced when loading the measured winding is more accurately a measure of the transformer's losses when in circuit. Whether it is really losses, or indicative of a higher actual reflected impedance, either way results in reduced power output versus that which a no load turns ratio test indicates. Measured using the method described, the output transformer reflected a 3,543Ω impedance from the 16Ω winding.
10. The real downfall of the original design is the biasing method used -- that being the use of the 12 volt heaters series connected in the three phono preamp and line stage tubes. With the quiecent heater voltage set at 29 vdc across the string as indicated on the schematic, it rises to a whopping 47 vdc with both channels at a full boil, with notable crossover distortion appearing at just over 14 watts in each channel. The 3 12AX7 heaters surely can't like that! But with an 18 volt increase in bias, there would surely be cross over distortion indeed! It's for that reason however that the B+ only drops 15 volts from quiescent to maximum power output in both channels, and the power output dropoff is so significant. The voltage doubler power supply is good -- but not that good! This design screams for at least zeners to be added across the heater string in the same way I published for them to be added to certain Fisher amplifiers using the same biasing approach. I'll be working on that soon.
Against the original design, I have no doubt that Jack's project produced very fine results indeed!
Dave
