This is a third and final installment of my in-depth review and analysis of Yaqin MC-100B amplifier. It will cover my attempts to improve measured performance and (hopefully) sound. First two installments can be found here http://www.audiokarma.org/forums/showthread.php?t=429993 and here http://www.audiokarma.org/forums/showthread.php?t=430109.
To make sure that amplifier works best in all power range from zero to clipping, I measured it at three points of output power – 1W, 8 Watts and at clipping point (whatever those limits were for every modification). I also disconnected global feedback circuit assuming that if I will be able to make amplifier most linear without it, I will always improve results by adding it back. So all tweaking was done without global feedback and measured numbers reflect that.
At first I measured Yaqin distortion values in stock form. Here is what I got (all numbers are in dB relative to main signal):
At 1 kHz 2nd harmonic 3rd harmonic
1 W -54 -60
8 W -43 -43
32W -24 -34
At 8 kHz
1W -43
8W -28
32W -19
I didn’t measure second harmonic for 8 kHz signal, as it is outside of measurement range for 48 kHz sampled EMU interface.
Now after I modified circuit based on best simulation results I got:
At 1 kHz 2nd harmonic 3rd harmonic
1W -51 -59
8W -35 -41
32W -32 -34
At 8 kHz
1W -41
8W -24
32W -24
Here goes simulation… As you can see we have some improvement at maximum power, but poor results anywhere else. I repeated simulation with different tube models, but still didn’t get anything better than stock, when I measured it. I do not know if it is deficiency of simulator, or tubes parameters are too far from ones used in models. But it looks like simulation is not very helpful for tube based designs (I never had so bit discrepancies in transistor circuits).
Now it was time to decide what to do without relying on simulation. First thing I decided to try was based on lower than expected B+ level. I decided to increase plate voltage at least in first three stages. It is easy to do in Yaqin, since it has two RC filters to clean power for input tubes. I decided to start with R14 and R15. I shorted R14. This resulted in increase of plate voltage from 338 to 365 Volts on Q3. All other plate voltage increased too. From oscilloscope picture it was clear that I could get higher peak-to-peak signal at grid of KT88 before onset of distortion. Increase was about 20%, which I would consider significant. Another thing to consider was final stage bias. 50 to 60 mA range specified by Yaqin is reasonable when you have plate voltage at 500 Volts. KT88 is specified to have 35-40 Watts (depends on version) of maximum plate dissipation. For 500 Volts on the plate it means 70 mA. It is recommended to use 70-80% of it at idle for AB class amplifier, which translates into 50–55 mA of recommended idle current. This is in line with what Yaqin recommends. But if we have only 400-410 Volts at plate, we can increase idle current if there is a value. I tried all range between 55 and 85 mA, measuring THD at 1 kHz, and found that the best results I can get was at 85mA. This is a little high (34 Watts), but considering that KT88-98 tubes used in Yaqin are relatively cheap, I can live with lower tubes’ life expectancy.
Another change I tested was to make Schottky circuit plate load different as usually recommended. When I reduced R6 to 43 KOhm I noticed improvement in second harmonic level of about 5 dB. I tried to get it even lower, but result was worse. So I decided to stay with 43/47 KOhm pair.
Now I did a final round of measurements with all changes implemented. Now I had:
At 1 kHz 2nd harmonic 3rd harmonic
8W -49 -51
32W -44 -43
I also noticed that I can get better output level at 8 kHz before onset of clipping from 18 to 21 Watts.
Now it was time to restore global feedback and test amplifier as a whole. I did full test and found that I can get at least 35W before obvious signs of clipping at 1 kHz. At 15 Watts I got THD level at 0.03% and IMD at 0.12% for 60+6000 Hz signal. At higher power levels THD slowly increased to 1% and IMD to 5 %. But overall useful power (under 1% IMD) was below 35 Watts at 1 kHz and about 25 Watts for 8 kHz. These are respectable numbers and should provide good listening experience for almost all types of music and relatively sensitive (over 90 dB) speakers.
Finally I was going to address ringing in amplifier after applying global feedback. From simulation I noticed that there is not enough of phase reserve at high frequencies. This is a common problem with tube amplifiers which use output transformers. I verified that there is no phase problem in the first three stages. Thus all my attention was concentrated on the final stage with a pair of KT88. I did some research and found one possible solution – shunt primary winding of the output transformer with capacitor and resistor. One practical example from 1950th for KT88 based amplifiers included 1000 pF capacitor in series with 1 KOhm resistor between plate and screen grid connection of output transformer (it has to be applied to both tubes in push-pull circuit). I decided to follow this example. The result was positive. It reduced ringing from 4-5 to 2 cycles. It also visibly reduced overshoot to fronts for at least 50%. I decided that it is enough of improvement, and didn’t try to get it any better.
Now it was time for listening tests again. I used the same disks as before, but added some old vinyl records from 60th and early 70th. What should I say – now there was no difference between my solid state amplifier and Yaqin at all. I tried all records on which I used to hear artifacts before, but there was nothing now. Until I got to power level over 35W (my power amplifier has peak meters), there was no way I could distinguish Yaqin from my solid state rig.
Now I can say that tube amplifier, when it operates within power limits and loaded with moderately easy to rive speakers has no difference in sound from competent solid state amplifier. Again there are could be many different reasons why someone chooses tube rig today, but sound shouldn’t be one of them.
The End.
Comments are welcome.
To make sure that amplifier works best in all power range from zero to clipping, I measured it at three points of output power – 1W, 8 Watts and at clipping point (whatever those limits were for every modification). I also disconnected global feedback circuit assuming that if I will be able to make amplifier most linear without it, I will always improve results by adding it back. So all tweaking was done without global feedback and measured numbers reflect that.
At first I measured Yaqin distortion values in stock form. Here is what I got (all numbers are in dB relative to main signal):
At 1 kHz 2nd harmonic 3rd harmonic
1 W -54 -60
8 W -43 -43
32W -24 -34
At 8 kHz
1W -43
8W -28
32W -19
I didn’t measure second harmonic for 8 kHz signal, as it is outside of measurement range for 48 kHz sampled EMU interface.
Now after I modified circuit based on best simulation results I got:
At 1 kHz 2nd harmonic 3rd harmonic
1W -51 -59
8W -35 -41
32W -32 -34
At 8 kHz
1W -41
8W -24
32W -24
Here goes simulation… As you can see we have some improvement at maximum power, but poor results anywhere else. I repeated simulation with different tube models, but still didn’t get anything better than stock, when I measured it. I do not know if it is deficiency of simulator, or tubes parameters are too far from ones used in models. But it looks like simulation is not very helpful for tube based designs (I never had so bit discrepancies in transistor circuits).
Now it was time to decide what to do without relying on simulation. First thing I decided to try was based on lower than expected B+ level. I decided to increase plate voltage at least in first three stages. It is easy to do in Yaqin, since it has two RC filters to clean power for input tubes. I decided to start with R14 and R15. I shorted R14. This resulted in increase of plate voltage from 338 to 365 Volts on Q3. All other plate voltage increased too. From oscilloscope picture it was clear that I could get higher peak-to-peak signal at grid of KT88 before onset of distortion. Increase was about 20%, which I would consider significant. Another thing to consider was final stage bias. 50 to 60 mA range specified by Yaqin is reasonable when you have plate voltage at 500 Volts. KT88 is specified to have 35-40 Watts (depends on version) of maximum plate dissipation. For 500 Volts on the plate it means 70 mA. It is recommended to use 70-80% of it at idle for AB class amplifier, which translates into 50–55 mA of recommended idle current. This is in line with what Yaqin recommends. But if we have only 400-410 Volts at plate, we can increase idle current if there is a value. I tried all range between 55 and 85 mA, measuring THD at 1 kHz, and found that the best results I can get was at 85mA. This is a little high (34 Watts), but considering that KT88-98 tubes used in Yaqin are relatively cheap, I can live with lower tubes’ life expectancy.
Another change I tested was to make Schottky circuit plate load different as usually recommended. When I reduced R6 to 43 KOhm I noticed improvement in second harmonic level of about 5 dB. I tried to get it even lower, but result was worse. So I decided to stay with 43/47 KOhm pair.
Now I did a final round of measurements with all changes implemented. Now I had:
At 1 kHz 2nd harmonic 3rd harmonic
8W -49 -51
32W -44 -43
I also noticed that I can get better output level at 8 kHz before onset of clipping from 18 to 21 Watts.
Now it was time to restore global feedback and test amplifier as a whole. I did full test and found that I can get at least 35W before obvious signs of clipping at 1 kHz. At 15 Watts I got THD level at 0.03% and IMD at 0.12% for 60+6000 Hz signal. At higher power levels THD slowly increased to 1% and IMD to 5 %. But overall useful power (under 1% IMD) was below 35 Watts at 1 kHz and about 25 Watts for 8 kHz. These are respectable numbers and should provide good listening experience for almost all types of music and relatively sensitive (over 90 dB) speakers.
Finally I was going to address ringing in amplifier after applying global feedback. From simulation I noticed that there is not enough of phase reserve at high frequencies. This is a common problem with tube amplifiers which use output transformers. I verified that there is no phase problem in the first three stages. Thus all my attention was concentrated on the final stage with a pair of KT88. I did some research and found one possible solution – shunt primary winding of the output transformer with capacitor and resistor. One practical example from 1950th for KT88 based amplifiers included 1000 pF capacitor in series with 1 KOhm resistor between plate and screen grid connection of output transformer (it has to be applied to both tubes in push-pull circuit). I decided to follow this example. The result was positive. It reduced ringing from 4-5 to 2 cycles. It also visibly reduced overshoot to fronts for at least 50%. I decided that it is enough of improvement, and didn’t try to get it any better.
Now it was time for listening tests again. I used the same disks as before, but added some old vinyl records from 60th and early 70th. What should I say – now there was no difference between my solid state amplifier and Yaqin at all. I tried all records on which I used to hear artifacts before, but there was nothing now. Until I got to power level over 35W (my power amplifier has peak meters), there was no way I could distinguish Yaqin from my solid state rig.
Now I can say that tube amplifier, when it operates within power limits and loaded with moderately easy to rive speakers has no difference in sound from competent solid state amplifier. Again there are could be many different reasons why someone chooses tube rig today, but sound shouldn’t be one of them.
The End.
Comments are welcome.
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