Showing posts with label ECC83. Show all posts
Showing posts with label ECC83. Show all posts

Sunday, November 17, 2013

The RH300B Story



The RH300B project was the first envisaged in the 2nd generation series, but the last to be developed. The development of this amplifier was long stalled by material reasons, mostly because I had no 300B tubes to build and breadboard it. Thanks to the generosity of a DIY friend who sent me two pairs of these DHT tubes, I was finally able to breadboard, troubleshoot, and finalize the project.
While an initial circuitry was published on some forums and sent to some DIY-ers back in 2005, when the time came to finalize the project some design choices were to be reconsidered. Thus the RH300B introduces a different driver stage in respect to all previous RH amplifiers, while simplification was introduced in the power supply section.

 
For the first time, I was hesitant and reluctant to publish the schematics of this amplifier. A lot of work, knowledge, and insight have gone into the design of the amplifier, and the various difficulties encountered on the way clearly show that these projects are not to be taken lightly. Good ideas and lots of knowledge are not enough; building an amp definitely requires some material means. RH amplifiers have met the criticism of all those who felt threatened by the publicity gained in particular by the RH84, and while many DIY-ers have built and enjoyed one of the several designs, the RH series has also spawned lots of copy-cats, and word is out that some are building RH amps for their local clients – mostly DIY-ers without the time at hand, or the experience required to build their own amps: while the clients should not be judged for feeling challenged by the prospect of building a tube amplifier, since it is among other issues dangerous as well (these voltages could kill you), the “hired builders” should at least give some credit to the original designer and avoid changing important parts just to make it look different at first site. There is a site (I will not paste shortcuts, but you can easily find it based on the description) showcasing a parallel SE amplifier with 807 tubes which is basically a copy of the original RH807 adopting 2nd generation solutions taken from the RH88, while the only difference is fixed biasing with negative voltage instead of a cathode resistor under the output tubes; the site owner has reluctantly agreed to mention my work by adding a blurred statement how his amp is in fact inspired by work of a compatriot of his, whose triode connected 807 amp (sic!) was in turn inspired by one of my designs… is there any shame left in people? Thus this amplifier represents the last in the 2nd generation series, published for all DIY-ers.

The Schematics


As it is evident from the schematics, the driver section now has a cathode follower directly coupled to the driver itself. While the driver is a rather standard choice for RH amplifiers – an ECC81 family tube, with anode-to-anode feedback connection to the output tube – the cathode follower portion of the driver is not. The cathode resistor of the driver tube is split in two, of which one resistor is bypassed with a capacitor – which is also a first in RH amps. This particular split is necessary in order to maintain a correct biasing of the driver tube while increasing the gain, in order to keep the input sensitivity below 2V RMS for full output (as declared at 1% distortion).
The cathode follower is not strictly necessary, as the driver tube is well capable of driving the output tube on its own. This particular detail appeared as a necessity while contemplating biasing methods for the output tube, since fixed bias requires the adoption of a grid resistor lower than 50k. With such a load, the driver was not capable to perform its task adequately, and the cathode follower represents the best way to solve the problem, since it does not invert the signal nor add any gain, while it is possible to couple it directly to the driver tube – avoiding additional capacitors in the signal path.
In the end, fixed bias was discarded, since the only apparent benefit would have been a lower B+ voltage. On the other hand, the negative bias power supply represents and additional cost, complication, and a source of potential trouble for the DIY-er. Furthermore, it would require checking the bias voltage of the tubes from time to time, as well as adjustments every time the output tubes are changed. All the amplifiers I have designed so far were easy to build and straight-forward in use, which to me represents an important feature – thus fixed bias (i.e. bias by negative voltage applied to the grid) was discarded as it brings more potential problems than eventual benefits.
Lowering the output impedance and increasing the current draw has enabled lowering the B+ voltage which mostly compensates for the only possible gain from fixed bias – as a result, DC RMS voltages are never higher than 470V (with 5U4 rectifiers) which helps keep costs down while the second cap in the power supply remains safely in the 500V WKG category (of course, with both channels operating, i.e. drawing current).
Finally, the cathode follower has remained in the schematics, since it obviously helps the driver tube perform its task, and keeps distortions at even lower levels. While the driver tube should be an ECC81 family member (12AT7, ECC801, 6201, CV4024, etc.), the cathode follower can be almost any small signal triode tube – almost, because once you choose the socket and the basing connections, there is little variation possible – 5687 is one example - and of course you have to keep in mind the operating conditions for this tube, which preclude some choices (most ECC88 tubes cannot be used, and even E88CC types are not advisable). But if we stick to the more common noval tubes, it could be an ECC82/12AU7, ECC81/12AT7, even an ECC83/12AX7 – while in the octal domain, a 6SN7 would do the job perfectly well (12SN7 would suit just as well, but you will have to provide 12.6V for the heaters, and connect the heaters of the driver tube in series mode instead of parallel). Whichever tube you choose, as the cathode follower section is directly coupled to the driver tube it will be biased to approximately the same conditions. What will vary is the bias voltage of the CF tube (grid to cathode differential) as well as the input impedance (approximately ranging from 2meg to 5meg) and the gain (in CF slightly lower than 1, depending on the mu of the tube used). It is thus not unimportant which tube is chosen or used – as it will have an impact on the sound of the amplifier.
The cathode follower section requires referencing the heaters supply for the driver tubes at approximately 20% B+ voltage. Most datasheets recommend not exceeding the heater-cathode differential of tubes by more of 100V DC, thus it would not be a good idea to have the cathode of the CF tube at approximately 160V DC without doing something about the potential of the heaters. The best option is to reference the heaters to a potential between the cathodes of the two driver tubes, and a 220k/47k voltage divider will perform this task perfectly well.
Of course, having two triodes per channel helps employ one double triode per channel in a mono-block amplifier configuration… there is no reason why you could not use the ECC81 as the CF tube as well, and as a matter of fact it provides the highest input impedance among all the proposed tubes.


The output tube, as you already know, is the 300B. NOS 300B tubes are probably extinct by now, or too expensive, and I cannot expect that DIY-ers – people who are not ready (willing, or able, choose your game) to spend 5 figures in USD or EUR on Hi-End amplifiers (Hi-Cost no doubt, the Hi-End sound is in the ear of the beholder) – would spend 4 figures on the output tubes alone. Thus the amplifier was designed, bread-boarded, and finalized keeping in mind the current production 300B tubes.
The biasing of the output tube is automatic as customary in RH amplifiers, set by a current source (or sink, if you like) made by a simple LM317 and current setting resistor. Regardless of the tube inserted in the socket, the current draw will always remain the same, and since this is a triode, there is no second grid to take into account – all current drawn is “anode current”. The current is set in such manner as to be near the upper limit for 300B tubes, while the voltage drop across the tube, deriving from the combination of current draw and B+ voltage, puts the anode dissipation between 30.5W and 33W, depending on the chosen rectifier tube (5R4 or 5U4 types). The anode dissipation is on the upper conservative level, which basically means that you will not unnecessarily shorten tube life while enjoying the best sound those tubes can provide. This relatively low anode dissipation is certainly adequate for the mesh anode types, either “mesh anode” or “plate with holes”. Those seeking additional thrills can always use a GZ34 (5AR4) rectifier for higher B+ voltages resulting in higher anode dissipation (about 36W) – this is feasible but not at all necessary.
As for heat and tube life, I have measured the temperature on the hottest point on the glass of the globe “mesh” 300B tubes after several hours of operation at approximately 33W dissipation, and it does not exceed 100⁰C. Real datasheets for current production 300B varieties do not present the same richness of data as the datasheets from the golden age of tubes, but I guess that an output tube in an SE amplifier, operating at temperatures lower than that of the rectifier tube in the same amplifier, where the rectifier tube is definitely running inside the safe envelope of operation, means that the output tube is not stressed and will not encounter a premature end – at least due to anode dissipation – regardless of what some tube dealers would like you to believe. On the other hand, filament defects (breakage) are definitely not caused by the ability of the anode to disperse heat, and should be addressed in a different manner.
Last but not least, the output tube cathode circuitry is virtually the same as the configuration already explained for the RH307A amplifier. Since the LM317 can only handle up to 35V input, the inserted resistor keeps the environment safe for the current regulator. Regardless of 300B type, or rectifier used, the voltage across the regulator cannot exceed 30V. Another solution would be the TL783, which is good for up to 125V input – but besides being relatively difficult to source, it would have to dissipate up to 7W, requiring a very serious heat-sink (temperatures inside the amplifier should be taken into account as well). The voltage dropping resistor should be powerful enough to withstand up to 5W dissipation for a long period of time (11W types and higher recommended).


The heating circuitry is AC, but 50Hz hum is absolutely low and completely inaudible on my speakers, due to the cathode circuitry solution and the general schematics of the amplifier. Even on more efficient speakers the AC heaters hum should not be prominent enough to annoy the listener. While the question which heaters power solution provides the best sound – AC, DC, unregulated, voltage regulated, or current regulated – it is my opinion the AC probably sounds best due to the fact that the whole filament is kept at the same potential level. But leaving this discussion aside, since each and every amplifier should be regarded as a whole, another great advantage of AC powered heaters is the simplicity of the solution. If the inevitable mains frequency hum is not an issue (in this amplifier it should definitely not be a problem), AC is the best, cheapest, and most practicable solution by far.

The Power Supply

As already mentioned, the power supply is simplified in respect to previous RH amplifiers. This is a normal cap input power supply, where the rectifier is combined with solid state diodes in a hybrid bridge. The hybrid bridge is more efficient than the standard full wave with central tap rectifier, and puts less stress on the rectifier tube. It is also by far less complicated to set and use than an all tube bridge rectifier, which would require more tubes and additional secondary windings. The sound (contribution to the sound of the amplifier) of the hybrid bridge is virtually identical to the sound of the same rectifier tube used in a classic central tap arrangement, providing a win-win combination. Rectifiers can be switched easily, either to tune the sound of the amplifier, or to increase (or decrease) anode dissipation. Since output tube biasing is automatic and always the same (set by CCS), there is no need to adjust anything when changing either output tubes or the rectifier tube.
The power supply is cap input, and this first cap should be a 600V poly or oil type – a good choice would be motor run caps rated at least 400V AC. The second cap should be a 500V type, and it can be a good quality electrolytic. There is no need to bypass any of the two caps with smaller caps. The choke is not critical as the only important element is DC current handling – a 200mA type is the minimum requirement. As for inductance, 5H or more is recommended for a good level of filtering.

The Transformers

The RH300B can be built with just one power transformer, or with several, depending on the size of the enclosure and the willingness of the DIY-er to order custom wound transformers. I have built mine employing a 150VA custom wound toroid for the high tension and rectifier heaters, and another smaller custom wound 30VA toroid for the heaters of the output tubes and the drivers. The two cannot be squeezed in a 150VA core, but could be wound on a 200VA core which would probably be a more expensive solution due to the large number of secondary windings. This even larger toroid would also require more space, both as sheer physical size, and probably due to the more complicated placing of the secondary windings output wiring. There is absolutely no need for a more powerful high tension secondary than provided by the schematics: while the DC current draw of the B+ is slightly above 210mA, the AC current draw as measured on the HT secondary is 270mA – less than foreseen by PSUD2 or calculated using the usual formulas. The temperature of the transformers in operation is up to 60⁰C and 40⁰C, respectively, in the box, after several hours of operation – thus it can be regarded as absolutely recommended.


While the schematic requires 5V secondary windings for the output tubes, it is advisable to adopt 6.3V secondary windings and drop the voltage to 5V across 0.56 ohm resistors on each leg. This will limit the current drawn by the cold filaments at power-up and definitely increase the life of the tubes, since filament failure through breakage at power-up is a common problem with many current production direct heated tubes.
A word about the output transformers – as shown in the schematics, those should be 2.5k primary impedance types. The secondary, of course, should be adequate to the nominal impedance of the speakers used. As for size, while size does matter, manufacturers tend to rate their amplifiers as output power, which is a relative point of view. You could build a 2A3 amp and a 300B amp using the same output transformer, as both tubes would work into 2.5k loads – but while a classic SE 2A3 amp will provide approximately 3W, the 300B will provide approximately 8.5W, thanks to its higher anode dissipation, and in particular due to the higher current draw.
Thus the most important part when choosing output transformers for the RH300B should be whether they are built to operate with 100mA DC current across the primary winding. If that request is met, all the remaining details (physical size, DC resistance of the primary, etc.) will work towards achieving a more or less extended and defined output, introducing additional distortion and loss in a more or less pronounced manner. While the RH300B thanks to the circuitry will have an excellent damping factor (DF), and will sound perfectly well on most output transformers that are fit for the current, primary impedance, and output power – since this is really a top-notch project, you should try not to spare on the output transformer. What is true of the RH84, re-built by many with high quality parts and output transformers to enjoy its qualities even more, relates even more to this amplifier, as the parts quality will be rewarded with increased sound quality.

End Results and Remarks

This long awaited amplifier, while being the first to be designed in the 2nd generation series, was the last to be finalized and built. The RH amps started as an alternative to classic DHT SE amps, succeeding in offering better sound and at least similar output power, step by step, DHT by DHT. The RH Universal easily over-powers classic 300B amps while providing better bass and definition, while the RH307A offers approximately the same power of classic SE 300B amps from a less expensive tube (while providing better bass and definition), and adds the thrill of direct heating, the particular sound of direct heated tubes… What is to be expected of the RH300B, since this is the tube mostly addressed by previous RH amplifiers with pentode (and beam tetrode) output tubes?
All RH amplifiers sound quite similar – since they have been designed by the same person adopting the same scheme type, which is quite rigorous on the tubes, imparting a particular type of sound. The main difference, beside output power, is the output tube itself, as the intrinsic sound quality of the tube will define the overall sonic quality of the amplifier. Direct heated tubes definitely have some interesting edge when it comes to sound, and the 300B is probably the most coveted of all DHTs – due to its intrinsic sound qualities, and the relatively high power it can provide, which is necessary in our world of relatively inefficient speakers spawned by several decades of powerful transistor amplifiers rule on the commercial Hi-Fi market.

Well, this amplifier is virtually a nail in the coffin of classic SE DHT amps. Whatever the 300B tube used (since there is currently a relative multitude of current production 300B types, and of course the almost extinct NOS WE) would provide in a classic SE design, it will do better and provide more in the RH300B amplifier. This is not any more the case of comparing pentodes with the 300B – but using the same “weaponry”. As a matter of fact, this was an easy win.


The simulation clearly shows 12W output at 1% distortion, with almost 2V RMS input sensitivity. I do not have any equipment that I could use to provide measurements, so DIY-ers will have to believe my word – or the simulation presented. Nevertheless, what matters is the sound, and the relative loudness that the amplifier can achieve in a system. In practice, the RH300B goes just as loud as the RH Universal does – on my normal real-world 88dB/W/m speakers – quite loud by anyone’s standards. There is no hint of the usual syrupy sound of SE 300B amps, which is so good for taming wild high efficiency horn speakers… instead, the sound is extremely detailed and controlled, with great bass definition and depth. Such statements are not to be taken lightly, but those who have successfully built any of the previous RH amplifiers probably know that their expectations will be met and exceeded.
If you ask me, my only regret is the fact that the 300B, being a triode, does not have a second grid that I could use to my advantage, like a lever to increase performance even further… It is interesting how many attempts have been made to copy the 300B, including indirect heated prototypes, curve clones, that were made out of pentodes in which the second and third grid were missing, not wound on their supports during manufacturing. All this trouble to construct a good triode, when there is so much to be had from pentodes – only because the knowledge required for that task has been lost or misplaced. Humans sometimes find it easier to replace an object, or resource, than to learn how to use it properly.

What Next?

This amplifier represents in a way the end of the 2nd generation series. The next, 3rd generation of RH amps will strive to go further, including different and maybe unexpected output tubes, and the circuitry solutions necessary to make these tubes work at their best.
Designing these amps takes a lot of time and thought, as I try to see the eventual problems in advance and design including simpler and more effective solutions, never straying from the path of excellence: the sound comes first, since those amplifiers are designed to enable enjoyment when listening to music, not winning awards. Bread-boarding an amplifier requires resources which are neither cheap nor easy to source (particularly in my country). The RH300B exemplifies this more than any of my previous amplifiers, as it was not possible to bread-board and build the finalized amp without the output tubes, and the lack of other resources, like output transformers and chokes, hit me more than ever before: for instance, the output transformers had to be extracted from the RH307A (those are 2.5k into 4/8 ohm transformers, when connected to 8 ohm speakers they present a 5k load to the output tube – the same ones pictured in the RH84 PPE prototype), and I had to find a way to design a good sounding power supply using only one choke in a cap input configuration…

There are no publicity banners, nor a Pay-Pal button on this blog. My efforts have always been totally non-commercial. But without help from DIY-ers who respect my work, I am not going to be able to continue designing and sharing amplifiers. All those who would like to help with output transformers, chokes, tubes, sockets, caps… are welcome to contact me.

Monday, July 22, 2013

CRITICISM AND SUPERFICIALITY



Since the DIY community has discovered the first RH amplifiers published on the net, back at the beginning of 2001, there has been a lot of appraisal by those who built with success the various amps (in particular the RH84 and RH807) – and a line of critics has emerged as well, which is both healthy and normal: without criticism, mankind would not have accomplished so much.

Most of the criticism falls in the following categories:
1.       RH amps are not original – there were a lot of amplifiers in the past that with plate to plate feedback (Schade and other examples).
2.       RH amps are not optimal – the driver should be a pentode (because most of the above mentioned sources say so).

There is a widespread misunderstanding among the critics that I claim the invention of anode to anode feedback, in spite of the fact that in the tube era the feedback path was known and applied in various forms. Just as usual (and how conveniently for the critics, if I might add) I cannot reply since I have no access to the forum – it is a fact that responding to harsh criticism, protesting copycats, and posting with arguments showing facts instead of empty words, leads to banning and expulsion. The conflict of interest between forum stakeholders – people who defend their arguments by saying, basically, “I am the authority because I say so”, or “because I build amps in that way (and I do it for money, so do not step on my toes)” is more than evident to all those who are willing to consider it.

While I have never actually claimed the “invention” of a certain feedback path, I was in all sincerity not even aware of the existence of the literature mentioned (like the RDH 4th edition which is often mentioned, or the famous work of Schade for RCA, which is basically an addendum to the datasheets and application data for the RCA beam tubes) – and have read none of the works mentioned at the time when I designed the first RH amps. The well-fed cannot fully understand the hungry – or what hunger actually is: living in the USA or Canada, it is very hard to imagine that such (seminal?) works (most examples are actually very common or normal books, but tend to be exalted by those who find it is in their interest to do so) were neither available nor accessible in socialist countries! Furthermore, in 2000 we still had dial-up (expensive dial-up, if I might add) and downloading a couple MB worth of tube datasheets was considered a feast! Besides, I do not recall being able to download the RDH 4th edition back in 2000, or the work of Schade regarding beam tubes. Thus, in a way, I had no examples to draw on for inspiration except my own ideas: that is maybe the reason why I keep defending this notion – my ideas are my own.

What I claim is that my designs are fresh and different, and up to the point when it comes to feasibility and results. The freshness and difference comes from the fact that before 2001 there have been no similar amplifiers published on the net, as far as I am aware (original designs done by the person sharing it, not books or magazines shared with or without the consent of the authors). The feasibility and good results come from what those who have built any of the published RH amplifiers have so far reported, both on forums and in direct e-mail communication. Due to the latter (reported good results), copycats started appearing since 2004, but became much more commonplace near 2009. The 2nd generation amps, characterized by having only the Rfb resistor (the classic anode resistor has disappeared) were first published in forums around 2005, when I built the original RH88 breadbord. Fresh and different ideas, and designs with a high degree of feasibility and success in obtaining good results, that is what is mostly lacking to the critics and their friends – at least when shared and publicised work is concerned.

The latest post linked above mentions “Hugo Gernsback's 1947 Amplifier Builder's Guide”. I have never heard of it, so I did some searching and quite easily found references to it, and – like always when the zealous critics (whose identity in most cases remains hidden behind pseudonims) have something to point out – it is not exactly what they are assuming it to be. In this case, Hugo Gernsback is actually the editor, or publisher – the copyright holder, anyway – of the Radio Craft Library (No. 33): Amplifier Builder’s Guide prepared by the editors. The amplifier mentioned (PA 8W amplifier) is not by H. Gernsback, but rather by Andrew Tait… so much for the attention to detail.

I have so far avoided direct comparison with old designs (while I do sometimes point out the flaws or inaccuracies in copycat designs) because I both felt there was no need, and due to having respect for the work of people who lived in a different era. Like I already stated, the well-fed cannot understand the hungry, and just like RDH or Schade were SF to me before the internet era, and throughout the dial-up internet era – until the moment when kind people shared those works with us – spice simulation and computers were mere science-fiction to the designers of the tube-era (maybe even beyond the imaginable)!

Nevertheless, this time I am going to make an exception, both because I cannot reply otherwise, and because I guess most blog readers will find the comparison interesting. Thus I apologize to the (most probably) late Mr. Tait for dissecting his work in this manner.

The amplifier in question which allegedly resembles the RH amps due to the fact that it shares the same feedback principle is basically a combination of 6L6G output tube and 6SF5 driver. While I have no model available for the 6SF5 (and no intention of writing one specifically) I will use the ECC83 model instead, since the two tubes are very similar – the 6SF5 is (almost exactly) half an ECC83 placed in an octal envelope: so much so, that any good ECC83 would probably test just as good if it could be used as 6SF5 replacement. While the correct operating voltages are not mentioned, the 6L6G is the old 6L6 type tube with 19W dissipation, meaning that with a 200 ohm cathode resistor it will draw approximately 70mA of anode current and 5mA of cathode current with a B+ of 300V (expected anode voltage across the tube of 274V and anode dissipation of 19.18W – too much in practice, but just about adequate to show the principle at work). Maybe a power supply simulation might show higher B+ (leading to improvement in results) but it is quite unreasonable to assume 25 or 30W dissipation capability in a 19W anode dissipation tube.


As the simulation shows, the amplifier is capable of 1.5W output at 3% distortion, with an input sensitivity of 83.33mV RMS (120mV peak).


Pushing the volume up to the 8W limit (actually, the article states 8-10W), the THD is 7.7%, which is much more distortion than would be acceptable for a relaxing listening session in your living room?! . It is important to point out that this happens with an input of 199mV RMS (287mV peak), which you could probably achieve with a tuner or ceramic cartridge.

From the two simulations above, it can be deducted that while the feedback is really taken from the anode of the output tube and fed to the grid (as the author simplifies) by connecting it to the anode of the driver tube, it is not very effective… maybe that is because of the decoupling on the cathode resistor of the driver tube?


Well, after removing that cap the distortion is slightly lower at 7%, but still not adequate for your living room. On the other hand, notice that the input is now 722.22mV RMS (1,04V peak) which cannot be achieved with the above mentioned sources without additional gain (would be fitting for a reel-to-reel tape deck, actually, with a standard 775mV RMS output at 0dB… but I guess those were not available back in 1947?).



Now for a much different approach: this would be (almost) an RH amplifier, and more careful readers might have noticed that the resistors applied to the ECC83 (6SF5, for that matter) are now identical to the combination shown in the RH Universal version 2. All other elements are kept identical for comparison purposes. While some critics have tried to imply high distortion in RH amplifiers, or that RH amp fans are “distortion loving” (freaks?), that is nowhere near the case. I sincerely think that the two amplifiers (RH and original PA) are not the same, although sharing the feedback approach: it is not about the principle, but how well do you apply it. The difference in design is profound to me, from the driver operating point all the way to the feedback resistor and the lack of decoupling cap on the g2 of the output tube - if I went a few steps further, to me the amps would be so far apart that a real comparison in terms of simulation would be pointless - but that does not stop the critics from mixing apples and oranges. Thus the simulation comparison is basically limited to details of the driver circuitry.


At 8W output the circuit of the PA amplifier modified as per RH amplifier principles now has a much more acceptable (although still far from desired) distortion figure of 4.4% - but the input has to be approximately 1V RMS, which would require an additional gain stage in the amplifier to allow for use with the sources that were available at the time. The AC response has also improved in the transition from the 1947 PA amp to RH mod, although the coupling cap has been kept at (nowadays unnecessarily low) 50nF.

This is not an attempt to denigrate the amplifiers of the golden age of tubes: the sources were different, and spice models were definitively SF to the designers of that age. The components at hand were also far from what we have today, both as values and quality. It is often simplified that at a moment in time we have rediscovered tubes and SE amps, and some criticize this move as backward thinking, the senseless embracing of flea powered 50’s amplifiers – but the truth is that modern tube amplifiers have very little in common with their ancestors (less than catches the eye), and the less they have in common - usually the better they sound (cheap clones and copycats excluded). Components have gone a long way since the golden age of tubes, designing has become very easy with spice models and analysis – easy that is, for those who have good ideas and enough knowledge to transform ideas into designs.

Let me now address the other issue – pentode driver. Indeed, why not a pentode driver in RH amps? There has been so much criticism both on the choice of 12AT7 (ECC81) as “driver par excellence” in the RH amplifiers, and the fact that the driver must get out of steam because it is not a pentode…


OK – here is your pentode driver in action, applied to this PA amp. While most components remain with the original (nowadays pointlessly low) values, like the 50nF coupling cap – a few others have been replaced for different values that were not easy to apply in 1947. It is obvious that this amplifier outperforms the original design at 3% distortion for 7.3W of output – and the reason why a pentode should be applied is input sensitivity: at 290mV it is low-ish for the era, but still quite feasible! The larger coupling caps and the removed unnecessary cap from g2 to ground on the output 6L6G help creating a very good AC response – and since the pentode driver is less affected by the absence of “cathode degeneration” feedback due to the decoupling of the cathode resistor, input sensitivity is retained even with the much higher feedback involved.

This pentode driver modification is obviously unobtainium back in 1947, since 6AU6 was still not made – but similar results could probably be achieved with 6J7 or similar tubes. This should explain once and for all "why Langford-Smith (and all the Langford-Smiths that populate the dreams and reality of critics) preferred a pentode driver" (“…did Langford-Smith really understand how the circuit worked? And where did he get off on saying pentode is preferred in the V1 position, I mean really…”): input sensitivity was paramount in order to avoid an additional gain stage. They did not have digital audio and op-amps, the equipment at hand did not have a standard 2V RMS output! On the other hand, what good is 290mV sensitivity in power amplifiers today – unless you are “active-preamplifier challenged”, or prefer using a passive preamp with your analogue FM tuner (because you do not need that much sensitivity with your CD player)?

The pentode driver will actually yield no improvement in distortion at 8W power (compared to the triode driver RH mod of this PA amp), and while representing a viable alternative, it remains to be seen how good it would actually sound. Because, schematics do not produce sound – while the actual components do. Just like several different make or sub-type tubes from the ECC81 family will measure approximately the same but will have a different sound (just to mention a garden variety ECC81 compared to 6021) – how is the 6AU6 going to fare? How many 6AU6 types are there to be found and tried, compared to ECC81? The most important point is that that there will be no improvement in power output, because that will be limited by the output tube – how much power can you extract from an EL84 in SE mode? What is more limiting, the type of driver (relevant mainly to the nowadays unnecessary input sensitivity) or the output tube (where an EL34 with 25W anode dissipation will indeed have twice the output of an EL84 with 12W anode dissipation). Let me remind you that we are not talking about low to medium triodes with a bias of 80V, but pentodes and beam tetrodes with a bias voltage of 8-18V! Last but not least, what is the difference between 5W and 10W? If you own high efficiency speakers (at least 96dB/W/m) you might probably miss the difference… but if you own low efficiency multi-driver speakers (i.e. 86dB/W/m) it will mean the difference between listening to some music, and trying to listen at low levels! This fact goes a long way towards explaining the huge success of the 211 and 845 amplifiers at the beginning of the SE revival in Hi-End audio: at 20-25W output power, we are basically just enough on the loudness target even with the lower sensitivity Hi-End speakers of the 90s!

That said, maybe the critics should concentrate on claiming that a 45 (or 10Y for that matter) cannot be beat and what you need is a pair of efficient 104dB/W/m speakers. The correct reply would probably have to be somewhere between the price of the two music reproduction combinations, taking as well into account the space (cost of rental, or cost of additional mortgage funds related to a larger living room) needed to house a pair of Klipschorns.

Just a last remark on RHD 4th edition and page 333 showing various anode-to-anode feedback arrangements… I wonder whether the critics of RH amps have actually done any of the math shown on that same page, or just strolled along with their eyes, finding similar looking resistors? Are they sure where would the math lead them?

Sunday, May 19, 2013

RH Universal v.2 – Totally Universal



The RH Universal is a derivative of the pilot 2nd generation RH amplifier project – the RH88. When I was working on the 2nd generation design, my main goal was stunning simplicity and lowest possible parts count. The concept was tested on 6550 tubes, both tetrode and triode connected, confirming in practice the auspicious simulation results, and showing that there is no difference in sound between triode and tetrode connection, except for the lower power obtainable in triode mode. While this makes operation of tetrode/pentode tubes in triode mode just a waste of available power, it does however open the possibility to adopt the 2nd generation circuit with triodes, as in the pilot project RH300B.


The 2nd generation circuit however requires relatively high voltages, basically excluding many possible driver tubes and making it unsuitable for many output tubes. The original RH Universal pushes this concept to the limit by making it possible to create adequate operating conditions for a range of tetrode/pentode tubes: with a fixed current draw, anode voltage is simply adjusted by means of changing rectifier type. Thus a wide range of output tubes can be used to full output power – at the expense of strict driver tube limitation (ECC81, eventually ECC82), and low input sensitivity. While low input sensitivity should not be a problem when a good active preamp is used, the driver inflexibility is in stark contrast with the output tube universality.


With a couple of modifications to the original RH Universal circuit, here comes a version 2 – now (almost) totally universal! The basic differences are:
  1. Application of 1st generation driver circuitry – the classic anode resistor returns, allowing more freedom in operation to the driver tube which is not limited by the swing of the output tube.
  2. Adjustable Rfb allowing the circuit to be perfectly tuned for the ECC81 family of double triodes (high-ish mu, relatively high transconductance) – or for the ECC83 family of double triodes (high mu, relatively low transconductance).



The advantages of this version 2 can be summarized as:
  • Total universality – a very wide range of output tubes can be successfully implemented: at the flip of a switch the circuit can be optimized for either of the two different tube types, making it possible to use a wide range of tubes which fit the same socket (and pinout) type, even adding the possibility to combine tube-rolling with different operating points and feedback. Some of the now usable driver tube types may be odd, rare, or low cost types – a personal favorite of mine is a 12BZ7 used as a substitute for ECC83. 
  •  Technical perfection (as far as possible) for the two optimized tube types, and near perfection for similar driver types, allowing for 10-11W output power at approximately 1% distortion levels (with KT88/6550). It goes without saying that maximum output power is higher… and depends on tube type.
A further advantage of the driver universality is the possibility to make an “all octal” version of the amplifier, as 6SN7 and 6SL7 can be alternated with excellent results – and similar tubes like the Mullard ECC35 can be used as well.


While modification of original RH Universal amplifiers is quite simple – the basic difference is one switch and two added resistors per channel – the v2 does not supplant the original. Besides being simpler, maybe more elegant, the original has a slightly different sound due to the 2nd generation driver circuit. The v2 sounds like an RH84 with lots of power, while the original version offers a slightly different nuance to the sound. It goes without saying that nuances are to be heard and judged based on the same passive and active components – the output transformers, caps, and resistors have an important sonic character which cannot be circumvented by simply changing the active components. The perfect combination may be completely individual, and the RH Universal allows for a wide range of active components alternatives on the same passive platform – a range now considerably widened with the version 2 update.