Showing posts with label 6080. Show all posts
Showing posts with label 6080. Show all posts

Thursday, October 18, 2018

RH6080HE (Headphones Edition)



It’s been years since I have posted any new projects on my blog – it’s not due to a lack of inspiration or ideas, rather I was too busy to build any new projects – or publish what I was working on. In the meantime my interests and experiences have evolved towards fields that I have been less involved in during the past years, and the general lack of time has made me rethink some of my building practices towards more time-efficient solutions.


Headphones and Speakers

While like most of my generation I have experienced first hand the advent of mobile audio in the form of the first “Walkman” devices (cassette players with and without FM radio) and thus grew accustomed to using headphones, I was never particularly taken by headphones listening – always preferring speakers. Over the years, this preference has basically cost me a lot in terms of musical pleasures not experienced: everyone can hear what (and how loud) you are listening when you use speakers, which implies that your family willing or nilling takes part of your musical and audiophile life. If your tastes include rather hermetic music, or hard bop, post bop, modal, classical – you name it, basically whatever is not mainstream commercial… in other words not suitable for everyone and not necessarily acceptable to others – you will likely listen to less music than you might have had, or will have to avoid some of the music you like. That’s where headphones enter the life of the regular music lover and audiophile.
The main reason why I prefer speakers to headphones is space – the music otherwise being confined to one’s head and thereabouts. Furthermore, the subjective sound quality being (perceived as) far higher with speakers – which might be a surprise to those who are aware or at least convinced that headphones are far superior in terms of transducers (no need for crossovers, little or no limitations due to available power, etc). Well, most probably that was due to the fact that we used to listen to headphones connected to the headphones connectors of our (integrated) amplifiers and receivers, or CD players and cassette decks: simply put, driven by a handful of small transistors, or op-amps. The advent of the new generation of often USB capable DACs, of which some were marketed as headphones amplifiers, did little or nothing – for me, at least – to change the perception of headphones sound quality as inferior to speakers in a good system. Well, I guess the words “good system” are the key to this perception – just like trying to compare some integrated solid state amplifier with a good (or much better than good, for that matter) tube preamplifier matched to some SE tube amps, with good cables to boot and all the possible amenities – on the same set of speakers. I needed to listen to more music, and it became obvious to me that there must be a way to equalize the perceived sound quality between speakers and headphones – let’s search for it in the missing link, the amplification.

Design Choices

Headphones do not need a lot of power – so far I have not had any planar magnetic headphones, but even these should probably do well with a couple of good watts… while most headphones are actually rated for less than 2W of power (i.e. they can handle that much power before being destroyed – assuming that your ears are not involved in the ordeal as they would make it painfully obvious that the power is too high).
What headphones do need is a high quality amplifier with low (lowish, actually) output impedance. Besides the most obvious choice of active element (tubes and solid state), and the quality of the power supply, passive elements are also relevant to the perceived sound quality of the amplifier – most notably capacitors and transformers. I guess it’s more than obvious that I would not choose solid state active elements to build an amplifier for my headphones, and with tubes there are basically 2 design options – with or without output transformer.



While there are lots of amp designs and ideas all around us on the net when it comes to using tubes to drive headphones without an output transformer, almost all reasonably feasible (and repeatable in terms of performance) alternatives must use a coupling capacitor between the headphones and the amplifying stage. I prefer to avoid coupling capacitors in the signal path, and my designs are centered on using the least number of gain stages and therefore coupling caps. Furthermore, when it comes to headphones, the values of the coupling caps have to be rather high if one is after a reasonable response in the lower frequencies: this is particularly true for most “modern” headphones which tend to be anywhere between 32 and 150 ohms impedance. The large value implies the use of electrolytic capacitors: while it is possible to parallel film caps to some extent, this will almost always end up in a very costly and physically large compromise. Caps will tend to leak, and that’s just another problem one is facing with output caps in a headphone amp. I have the feeling that the headphones are not really safe with a capacitor coupled output, although that is probably irrelevant to most: you only live once, so who cares…
As I already mentioned, most currently available dynamic headphones are between 32 and 150 ohms impedance, where above 80 ohms the choice becomes rather slim, at least in terms of variety. While these lower impedance headphones are relatively easily driven with solid state devices, they represent a taxing load for tubes and the possible solutions are either push-pull circuits, or the usual highly inefficient cathode follower compromises that are quite good at driving higher impedance headphones (300 - 600 ohms) but cover the fact that they are struggling to drive lower impedance headphones regardless of the inefficient high idle current draw and relatively high output power (relatively high – that is in terms of headphones power handling capabilities).
Some well-known amps and kits resort on 6080 or 6AS7 in cathode followers drawing high currents and running their cathode resistors rather hot: I have considered this option with 2k 25W cathode resistors and was not happy with the high current that would have to be drawn, the heat generated by these cathode resistors, the compromise when driving anything else than high impedance headphones – and last but not least, the output capacitors. OK, let’s put this straight – amplifier size or power consumption was the least of my concerns; I do not like unnecessary heat in an amp, and I do not like output coupling capacitors – but what I hate most is the compromise involved. While I own several headphones, most are low or lower impedance, and I guess most DIY-ers and audiophiles are facing the same choice of headphones. Last but not least, I like universal solutions (does the word ring some bell?) and dislike compromises that can be avoided.


RH Amplifier – Headphones Edition

Once we leave the output capacitor path behind, the only way to go is with an output transformer. While some would consider the output transformer as another compromise in quality, similar to the capacitor, I would beg to differ. The transformer does not leak, unlike the capacitor, and headphones are safe unless abused: the only regular problem that comes to mind is the pops and clicks when powering up or powering down the amplifier, but that can be avoided in more ways than one. The limitations of output transformers are known, and in this case due to the fact that headphones do not require a lot of power, can easily be solved with larger cores than strictly necessary. A core that would be good for a decent 5W SE amplifier is more than good for a headphones amplifier that will in most cases deliver less than ½W of power. On the other hand, transformers can be rather universal devices that offer flexibility – just like the 4, 8, and 16 ohm taps on some output transformers, there can be 32, 64, 128… ohm taps on the output transformer for headphones, matching the impedance of the headphones at hand, or better – the impedance groups of headphones.
Now that the decision is made – go with an output transformer – an amplifier is needed. Well, in my case that can only be an RH amp, otherwise I would not be true to myself. Over the years I had several times been asked if the RH84 could be used as a headphones amp, provided the appropriate output transformer is installed – and I have replied that it most certainly can, but it was not designed, or optimized, for this role. The purpose of the RH84 is to drive speakers with as much power as can be had from the EL84 while not sacrificing the sound quality – actually, trying to solve that design task better than most other amps.


For the headphones RH amp, I chose to design something “new and different”, although the resemblance to my other designs is striking. This amp does not need to produce more than a couple of Watts of power, but needs to yield excellent sound quality, and absolutely needs to be quiet – i.e. no noise is allowed because the headphones being on the listener’s ears are quite sensitive to noise and hum. Last but not least, the optimization needs to be easy, taking into account the intrinsic differences between the imperfect devices that tubes are, and the variations possible even within the same batch.
One additional element that needed to be taken into account is the lowest sensitivity possible without resorting to additional volume potentiometers, while the amp needs to be able to easily accommodate various use cases with simple modifications. Lowest sensitivity possible – this implies that while it might be beneficial for a low power SE amp to get to its full power of 3W with an input of 0.775mV RMS, this would be totally impractical for the same SE amp used as a headphones amp. As I said several times already, this amp will not be used at 2W output power by most users!
The design centers around the 6080/6AS7 tube which is a dual triode just like the ECC81 or the 6SN7, but the two triodes inside the envelope have 12W anode dissipation each, and mu is very low – lower than 2A3 or 300B. Obviously, the low sensitivity requirement excludes all the usual pentodes that come to mind -  EL84, 6V6, and the smaller “siblings” like EL85 or EL95 which can still be found and had at low prices – although all of these tubes would have more than enough power for the task. Even if those pentodes were used as triodes (something that I personally don’t do) their resulting mu as pseudo-triodes would still be too high. The 2A3, 6BG4, or 300B might be used, and would probably be capable of interesting results – but they are all directly heated and thus would require additional attention (and circuitry) to avoid filament hum. The 6080/6AS7 tubes are rather plentiful and therefore still cheap, and will not require any additional attention to heating – being indirectly heated triodes.
The driver is the usual ECC81 that I use for all my other RH amps – I guess by now it does not need any introduction. Let me just reiterate that this tube has a relatively high mu (reasonably high internal impedance) combined with a relatively high transconductance – two characteristics that make it especially suitable for the role it is supposed to have – driving the output tube to desired results.
As mentioned at the beginning, the lack of time has driven me towards different solutions than previously adopted: installing sockets and doing a hard-wired installation might be the best solution for most people, provided they had the time to do it. Additionally, while a hard wired installation is expected to yield better sound quality and last longer, it is quite impractical for servicing and adaptations, let alone re-use or recycling in other projects. On the other hand, my recent preamplifier revalidation has shown that even PCBs I have drawn and etched manually have lasted more than a decade without any problems whatsoever, and continue to perform well in spite of the servicing and modification changes (change of component values to suit other tubes). Thus when building a new preamplifier I have redesigned the PCBs and this time had them etched instead of doing it myself.
In accordance with the experience gained using the old preamplifier for more than a decade, and having just built a new version, I have decided to design an amplifier board that I named RH6080 – generally suitable for application of most noval tubes as drivers, and the 6080/6AS7 family of tubes in the output position octal socket. The two channels are basically dual-mono except for the common ground on the board, and the fact that the tubes are dual triodes: in theory, even the B+ could come from a different source or be of different value, although that is highly unlikely.


I can use the same board to build other projects that I have in mind – an 8W SE amp for loudspeakers, PP RH amps – and even a driver amplifier that can push large output tubes into class A2… projects awaiting to happen in the future.

Performance and Optimization


As shown in the simulation, this amplifier is capable of 3.2W output power with an input of 2.5V RMS. As such, with an appropriate output transformer it could be used to drive speakers – rivaling classic SE amps with 2A3 output tubes, usually specified as 3.5W output power. The 6080/6AS7 output impedance is lower than that of the 2A3, and combined with the RH specific feedback – this translates into quite low output impedance for an SE amp: what DIY-ers who have built RH amps have previously experienced with the amps they built would be adequately replicated by this amp. Simulations are just as good as the models used, and the models I am using both for ECC81 (accuracy comparison shown in the RH813 post) and the 6080/6AS7G are as accurate as possible. By that I mean – the models were created based on a sets of curves shown in the datasheets – to get the results with 100% accuracy one would have to generate curves from the batch of tubes used, and create models based on these curves. The accuracy achievable with datasheets curves should be considered as “as accurate as possible” – unless one is in the “laboratory measurements” hobby as opposed to the “designing and building amplifiers” hobby.
This amplifier is supposed to be used as regular amplifier for loudspeakers – the only difference being that headphones are connected to it instead of the loudspeakers. Therefore, there is no volume potentiometer except for the one on the preamplifier. My current preamplifier has 20dB of line stage gain, giving it a reasonably ample range of volume adjustment with my power amplifiers into my speakers, where the amps are not particularly sensitive, and the speakers are reasonably efficient. When operating the RH6080HE I have found that the volume adjustment range on the preamplifier pot is twice as limited – basically, at 9 o’clock the volume with most headphones is at the limit of my comfort zone in terms of loudness, i.e. output power. In practice, this means that with the addition of a volume potentiometer and eventually a selector it can be used without a line stage preamplifier, or connected to the tape output of the preamplifier (without line stage gain).


A slight modification to the input circuitry where the cathode resistor coupling cap is removed decreases input sensitivity further to almost 3V RMS needed for full output, while the remaining parameters are the same – this increases the range of volume adjustment on the potentiometer, and makes it easier to find the adequate volume for listening. I guess in this case use without a preamplifier as explained above is still borderline possible and will depend on the output voltage of the source used – a CD or DAC at 2V RMS output should be amply sufficient to exceed comfort zone volumes with headphones, but lower output sources might lead to insufficient volume and/or a lack of fullness in the sound.
This is a single ended, i.e. SE amp – thus absolutely suitable to drive any headphones without the need for any strange or non-standard connectors. Nevertheless, as the output transformers totally isolate the headphones from signal or power ground, and even the left from the right channel, I have chosen to adopt as standard a 4-pin XLR socket, basically the same as used by some manufacturers to connect headphones in balanced mode. Needless to say, I have chosen to implement the same pin connection standard as used by the manufacturers, mainly to simplify potential issues with cables compatibility.


Balanced headphones connection requires a separation of ground returns between channels, hence the need for 4 connections instead of the usual 3 (common ground). Thus a pair of headphones configured for balanced connection can easily be connected to this amplifier, as the grounds are galvanically isolated – although obviously they will be driven in single-ended mode since the amplifier is SE. In order to connect headphones with regular 6.3mm jacks and 3 connections (common ground) an adapter is sufficient where the ground connections are shorted: this might be even dangerous with a balanced amplifier, but is absolutely normal with this SE amplifier. Therefore I have decided against having an additional 6.3mm jack terminal next to the 4-pin XLR and to use a custom-made adapter instead.


The knob visible on the facia of the amplifier is not a volume potentiometer – rather a selector. The purpose is to choose the secondary of the output transformer based on the impedance of the headphones connected to the amplifier. While the type pictured is good enough for the task and works fine in practice, it is sub-optimal and I suggest a better selector is installed – besides mechanical stability the clue regarding it’s adequacy for the task is declared current/power capability.

The Power Supply

The initial version was built with a rather simple CLC power supply that would be suitable for an SE amplifier that drives speakers – basically, if this amp was used to power loudspeakers, there would be no audible hum or noise audible at 1m and even less from the speakers. But, this amp is used with headphones, and absolutely all sound effects can be heard – down to the eventual propensity to microphonics of some tubes (even the output tubes), and this includes all sorts of hum that come to mind. As usual, I have had no problems with the wiring or ground loops, but in the absence of music clean low frequency (100Hz, twice the mains frequency) hum could be heard. At that point it became clear that the power supply is either going to be large (marginally too large for the box in which I was building it), elaborate, and expensive – or regulated.
Having had excellent results with the power supply I have recently developed for a new iteration of my classic preamplifier (some might remember the RPA, not available on the net any more as the old site has disappeared), I decided to modify the voltage setting resistors ratio to match the needs of the RH6080HE and populate a spare PCB etched for the preamplifier project that I had at hand. It took me literally minutes to build it, as opposed to hard-wiring capacitors and finding a way to keep them fixed…  This power supply works perfectly with the phono stage, both in terms of hum and noise, as in terms of perceived sound quality.


Needless to say, as expected, the amplifier became dead quiet – it all boils down to tubes quality now, as some driver tubes (ECC81) might be less quiet than needed – and even some 6AS7 can be noisier than a perfectionist would accept. The power supply uses a hybrid bridge composed of a dual rectifier tube and two solid state diodes – the rectifier tube is slower and dictates the behavior of the solid state diodes, with the result being sonically equal to what the rectifier tube would yield in a pure tube rectification circuit. The active pass element is a TL783, a device similar to the LM317 but with a much higher input-output voltage differential of 125V. Another difference is the pass element which in the TL783 is not bipolar rather FET. The same circuit can be built with an LM317, but in some circumstances the input-output voltage differential might be higher than 35V (highly unlikely but possible) most probably killing the LM317 instantly… no harm would happen to the tubes, obviously, but the hum would immediately rise to unacceptable levels pointing out that something needs to be done about it… Another difference is the quality of the TL783, which unlike most LM317 is not noisy. The difference in price is irrelevant in DIY terms and the TL783 should be relatively easy to come by.



Some would probably object to the solid state regulator, as the solid state pass element is expected to mask the “sound” of the tube rectifier. As I already said, this power supply has proven its worth in the preamplifier project, and rectifier tube rolling with this power supply is more than effective in fine-tuning the sound. The only issue for tube rolling might be the possibly large difference in output voltage between different rectifier types (actually, the difference in diode voltage drop) – precluding the use of 5R4 and 5Y3 tubes in this circuit (input-output differential too low and the regulator is not working properly, with high hum as a result). Of course, that can be circumvented with a higher secondary AC voltage (for instance, 360V instead of 330V) but in that case when using more efficient rectifiers like the 5Z4 the input-output differential across the regulator element will increase to probably 30 or 40V, which combined with 100mA current draw for the amplifier circuits yields 3-4W of dissipation – precluding the use of more efficient rectifiers and limiting reasonable operation with a higher voltage secondary to the 5Y3 or 5R4 rectifier tubes. In that case, a good heatsink capable of at least 5W dissipation is necessary: I prefer keeping the dissipation below 1.5W. It goes without saying that both the TL783 used in the power supply, and the regulators used as current sinks below the cathodes of the output tubes must be heatsinked, although the heat-sinks do not need to be particularly large (adequate for up to 2W dissipation).

The Output Transformers and Sound Quality

Well, so far so good – it’s just a regular RH amp with output transformers that are adequate for headphones, and can be build on PCBs – making it esier for DIY-ers… but most SE output transformers are actually designed and manufactured for loudspeakers, with 4 and 8 ohm taps. They are not adequate for 32 ohm headphones, let alone high impedance types at 300 or more.
The output transformers used for this project were manufactured by Heyboer in the US based on project requirements – and provided by a fellow DIY-er: Larry Granger. I would like to thank him for finding the subject interesting, and for his kindness in providing the output transformers – without those, the project would just be dead drawings on (electronic) paper.


The primary was chosen to be 5k – this is perfectly suitable in general for tubes drawing 40-50mA, and a value generally suitable for most low power pentodes and tetrodes, like the EL84 or the 6V6. While this value seems too high for use with 6080/6AS7, the assumption is not particularly correct. The output tube in this circuit is used at a rather unusual operating point, constantly drawing 50mA and having just above 200V across the tube (cathode to anode). The output tube in practice operates at around 10W anode dissipation, which is absolutely acceptable for this type of tube and guarantees a long operating life. On the other hand, output power maximization is not necessary – and it is already done with the particular feedback applied which includes the characteristics of the driver tube.


The core of the transformer would be absolutely suitable for a high quality SE amplifier in the range 3-5W, and most manufacturers would market it as a 10W core: thus it is expected to behave very well in terms of bandwidth. The higher than usual primary impedance for  the tube, and the low output impedance of the circuit mean that with this transformer there should be no bandwidth constraints, particularly at 1W output power and below. While not having any planar magnetics to try, I expect that even the slightly higher power requirements of such headphones would be served nicely.
The secondary windings were chosen to be multiples of 32 ohms – 32 ohms being the de-facto standard value with headphones nowadays. Thus the values are 32 – 128 – 256 – 512 ohms, and as such will accommodate a wide range of headphones from 32 to 600 ohms. Connecting 600 ohm headphones to the 512 ohm secondary will result in lower primary impedance seen by the output tube as 4.2k instead of 5k – but as explained above, this tube and the circuit can easily handle 20% differences in primary load, while 450 ohm headphones will again fit the 512 ohm tap very well. Similarly, connecting 300 ohm headphones to the 256 ohm tap is absolutely fine. Most 70 or 80 ohm headphones actually show impedance charts around 100 ohms, and they can be well served by the 128 ohm tap, just like the 150 ohm headphones. I am deliberately not mentioning the brand names of the “usual suspects”, and I expect most headphones enthusiasts know well which brand still manufactures 300 and 600 ohm headphones, and eventually proposes new “improved” models of 150 ohm impedance…


Last but not least, the sound quality: much better than expected, actually. While my amplifiers perform very well in my room driving the reasonably efficient speakers that I use, with the RH6080HE power is not a relevant topic, at least in terms of loudness and dynamics. Having much more power than needed imparts an ease and effortlessness in the presentation of music, and the most important characteristics that I have found is what I was missing most with headphones – space, or rather the sense of space. It is common knowledge that open headphones convey a better sense of space, frequently at the expense of less depth and definition in the bass notes. With this amplifier, I have found improvements on both: closed headphones have an excellent and unexpected rendition of space, while even those bass-heavy among them show a very controlled low register. On the other hand, the sense of space with open headphones is amazing, while the rendition of bass notes is so effortless and well defined that it easily rivals listening on loudspeakers.
More importantly – how does this amplifier compare to commercial alternatives? Well, first of all, I am not aware that there are many commercially available tube amps with output transformers and multiple secondaries – and not having listened to any such amps, I can only believe that the difference is proportional to what can be had when a “regular” loudspeaker driving RH amp is compared to commercial alternatives of similar power. On the other hand, there is literally no comparison with most if not all commercial solid state device powered alternatives that I have had the possibility to try: the difference in sound quality is quite pronounced and it becomes quite obvious that the tube amp is in a league of its own. But, as a good friend nicely puts it – one can take along most of these amps and DACs in one’s pocket and carry them along enjoying music everywhere, while I cannot take this amplifier, rather heavy and the size of a regular SE amplifier, and use it on the go. Still, the purpose of this design has never been portability, but sound quality rivaling listening to a good system with loudspeakers – and that goal has been amply achieved.

Friday, February 7, 2014

RH2A3 – An Amplifier With a Twist!



During the final development stages of the RH300B amplifier a similar schematics for use with 2A3 tubes has imposed itself as quite feasible and logical. The 2A3 is a DHT tube just like the 300B, of similar general characteristics: mu is around 4 in both cases, while plate resistance is between 700 and 800 ohms. The main difference between these two tubes, heaters voltage aside, is maximum ratings – dissipation and voltage. Thus slight downscaling of operating voltage and current to create operating conditions acceptable for 2A3 tubes has been done before with several popular schematics.

This would be the general RH2A3 schematics – almost a mini-RH300B. With lower B+ and current consumption, cheaper to build due to lower power requirements, different heater voltage for the output tubes, and lower power with the same or similar output transformers. Just as in the case of the RH300B, at 5.1W and 1% distortion, output power exceeds expectations – and will probably be discussed and questioned in the future by all who have not built the amplifier themselves and thus ascertained whether the promise has been fulfilled.


As the schematics is strikingly similar to the RH300B, I shall not repeat all considerations related to the schematics itself – the only appoint that should be made, or rather repeated, is that the operating point of the cathode follower tube is determined by the directly coupled grounded cathode driver tube. Thus it will draw the same current regardless of tube type used – and this time I have chosen to adopt an octal socket, accommodating 6SN7 tubes, but 6SL7, ECC35, and other similar tubes can be used as well – you can go as far as 6BL7, 6BX7… even 6AS7 (or 5998). While it might elude logic to employ 6AS7, 6080, or 5998 (WE421 by TungSol) due to the relatively low current draw, and keeping in mind that these tubes have very high heater current requirements which would have to be taken into account – the sonic results obtainable with these tubes reflects their known sonic characteristics, and are quite interesting in the scope of this amplifier.

The twist


The RH2A3 can be built with regular 2A3 tubes, either NOS or current production: it seems that just like the current production of 300B, modern 2A3 tubes are good sounding, reliable, and meet the “single anode” construction so much sought after by some DIY-ers and audiophiles. And of course, that is the most logical way to go…


But I have built mine with “unusual” 2A3 tubes – on octal base. While the 2A3 tube was manufactured as well with 6.3V heaters and UX4 base (6A3), and further developed into a version with 6.3V heaters and octal base known as 6B4G – I am referring to “special edition” 2A3 tubes, with 2.5V heaters, mounted on octal base. The most notable application of these tubes have been the Audio Innovations First and Second amplifiers, as it seems that 2A3 tubes were custom ordered on octal base due to a lack of UX4 sockets at the time. In my personal opinion, while this is a plausible answer, I guess that commercial concerns were important as well, channeling the supply of spare tubes for the amplifiers.
Anyway, a different base just needs a particular socket, and besides complicating life a little bit trying to source 2A3 tubes on octal bases, this would not be much of a twist. In keeping with the inherent universality of my designs, at this point the 1619 enters the stage. The 1619 is a direct heated beam tetrode tube on octal socket. It has 2.5V heaters just like the 2A3, and is pin-compatible with the octal socket used for octal 2A3 tubes – pins 2 and 7 for the filamentary cathode, 3 for the anode, and 5 for the control grid.


So far so good - but what about the second grid and the beam forming plates? While the 1619 is used by some in triode configuration, with g2 connected to the anode – this application is almost reserved for the old radio collectors market. The 1619 is seen as a cheap replacement for expensive 45 tubes, and relatively elaborate adapters are being made or sold to allow plugging the 1619 in old radio receivers. In the case of the RH2A3/1619 amplifier, the second grid on pin 4 is connected via a zener diode to B+ (56V 5W zener recommended, setting the g2 voltage at approximately 250V), while the beam forming plates (pin 8) are connected to the shield (pin 1) and directly to ground. Furthermore, pin 6 – which is missing on 1619 tubes – is used as the “virtual cathode” point. Pins 4, 6, 8, and 1 are NC on 2A3 octal base tubes, just like they are NC (not connected) on 6B4G tubes (as a matter of fact, the octal base of the 2A3 octal is identical to the 6B4G base). Thus when a 2A3 is plugged into the socket, it is indifferent to the connection of these pins.



How to make it all work?


Both tubes have 2.5V heaters with similar current consumption, and 15W anode dissipation ratings. But the bias voltage of the 2A3, i.e. the potential of the cathode in respect to ground, is much higher than that of the 1619. At the foreseen operating condition of approximately 250V across the tube and (exactly) 60mA of current draw, the bias voltage of the 2A3 exceeds the ratings of the LM317 regulator. While this could be solved by adopting a TL783 regulator which is safe for input voltages of up to 125V (the main and probably only relevant difference between these two regulators is the adoption of a DMOS output transistor in the TL783) – the bias voltage times the current draw will require a relatively large heat-sink and lead to a potential overheating problem. The resistor shown in the schematics absorbs most of the voltage differential and lowers heat-sinking requirements for the active element (LM317), leading to more stable operation. I just somehow prefer to run solid state components as cool as possible, and leave the heat to the high power ceramic resistors. In order to operate the 1619 tube, the resistor must be excluded from the circuit, which is easily done bypassing it with a switch.


The difference in voltage across the tube will be dealt with naturally by the difference in tube type: since the 1619 is a tetrode, the total current draw is the sum of anode and screen grid current. Thus anode current will not be 60mA as with the triode 2A3, but about 54mA – as approximately 6mA will be drawn by the second grid. Changing tubes and excluding the voltage dropping resistor by switching it off will lead to a different set of operating conditions which suits the 1619 just as well as the other set of operating conditions (with voltage dropping resistor) suits the 2A3.

The output transformer


Another important difference between 2A3 and 1619 is the optimal anode load: while the 2A3 triode will perform at its best at values between 2.5k to 3k, the 1619 beam tetrode would require a load between 5k and 6k. To achieve this goal, we need a very versatile output transformer which would allow us to change anode loading at the flip of a switch (or switches).
The Lundahl LL1623 output transformer used in this amplifier, besides the highest build and materials quality, has a probably unique versatility and adaptability to various circuits, since both the primary and the secondary windings can be arranged to suit a wide range of currents and transformation ratios.


While the primary windings could be arranged in parallel to double the maximum current capability, this would lead to lowering the inductance, and since the gap is already set at the factory to suit for 60mA, 90mA, or 120mA of DC current across the primary – the best solution is to connect all primary windings in series, as shown in the datasheet. Thus the inductance of the primary will be defined by the chosen gap, i.e. required DC current value. Quite logically, the optimal gap for the RH2A3 amplifier is as set for 60mA DC current across the primary.
The secondary windings can be combined to achieve standard foreseen anode loads of 1.6k, 3k, and 5.6k – for an insertion loss that varies between 0.2dB and 0.8dB. Bearing in mind that all the above combinations are possible for 4, 8, and 16 ohm loudspeakers – it is obvious that the possible anode load is actually even more varied.
While the user might exercise his (or her) wits by finding alternative connection possibilities, an application sheet is available on the Lundahl site showing possible secondary winding connections that allow switching between “adjacent” anode loads by use of switches or bridges. Since my application is with 8 ohm speakers, I have chosen to prepare the output transformers for B/C, i.e. 5.6k and 3k loads into 8 ohm outputs.


While for the connections of the primaries I have chosen to solder pieces of wire, the much more elaborate secondary connections seem to require a different approach: hence the wire harness showed in the pictures. The three switches allow the choice between 3k anode load (suitable for 2A3) and 5.6k anode load (suitable for 1619). While the wiring harness looks complicated, and indeed requires a couple of hours to complete and check – there is no need to rush while building an amp. The building experience is indeed a source of pleasure, and once you finish building the amp, you will probably be using it for years to come: what would be the point of building it in one afternoon?
I feel confident with the solution I have adopted – but a further simplification and expedient could be a custom PCB, foreseen to be simply mounted and soldered on the pins of the secondary windings, greatly simplifying the build and avoiding the need to check and re-check.


Thus, to recapitulate: one switch to include/exclude the voltage dropping cathode resistor (2A3/1619) and three switches to select the optimal anode load for the tube (3k/5.6k). I guess that is not too much to do in order to enjoy two (slightly) different amplifiers from a single box?
Of course, the switch for the dropping resistor can be omitted if TL783 is used with an adequate heat-sink (dissipation will reach 2.5W with 2A3 tubes) – and with that touch the only possibility for error would be avoided: because, if you insert a 2A3 tube without the voltage dropping resistor, you will most probably kill your LM317 – and if you insert a 1619 tube with the voltage dropping resistor in circuit, it will not be able to draw the specified current, leading to possible overvoltage conditions for the power supply caps (which is why those are not rated for a tempting 400V that looks to be just fine, but would be easily exceeded if the output tubes do not draw current for any given reason). On the other hand, if you forget to set the correct load for the output tubes, the lack of power and early clipping will harmlessly remind you to check the switches…

How does it sound (and compare)?


I used to have for quite a long time a 6B4G SE “no feedback” amp that I enjoyed quite a lot and used it as a “reality check” at the time of the initial RH designs – RH84 and RH807. The amp was very straightforward and classic, I had conceived it as a two stage design with 6SN7 (grounded cathode, bypassed cathode resistor, resistor loaded anode, 6mA current) driver and 6B4G output (automatic bias via bypassed cathode resistor, 300V across the tube, 50mA current draw, 3.5k load). While the “no feedback” designation is a nonsense per se – as particularly in triodes, plate current is dependent on the plate to cathode voltage differential: as the signal tries to pull the control grid positive it causes a rise in anode current, but the anode to cathode voltage differential decreases at the same time, trying to pull the anode current down. Since anode and control grid are pulling in opposite directions, this is negative feedback by definition… (to put it as straightforward as possible, though simplified to the point of easy criticism) While the behavior of the triode suggests an “inbuilt” feedback mechanism, the term “no feedback” is more of a common lingo expression reflecting the fact that cathode degeneration was “avoided” throughout by adoption of bypass caps on cathode resistors (avoided, that is, from the high pass frequency on), as well as the lack of NFB either local or overall. While the feedback nonsense should be left aside, the reality check comparison is something I frequently do, and can only suggest it to everyone – as a means of avoiding the proud of ownership (or craftsmanship, or own design) syndrome and illusions about the perceived quality or quantity. The mentioned amp was a classic 3.5W 2A3 class amp (with good quality black anode 6B4G tubes) and represents a valid statement to compare the performance of the RH2A3 with.


One important detail is the hum inherent with AC heating operation of direct heated tubes: the hum level is proportional to the heater voltage, and the gain of the tube. Thus the most obvious advantage of the 2A3 in comparison with the 6B4G is AC related hum. In RH amplifiers, hum is obviously reduced by the application of feedback – so much so that it can be barely heard on the RH300B (5V heaters), and it becomes virtually inaudible on 88dB/W/m speakers with 2A3 tubes (2.5V heaters). On the other hand, the hum of a “no-feedback” 6B4G amp can be easily heard on the same speakers, although it might not be so distracting at the listening position (“humming pot” or not, it could be heard between songs during quiet night hours). If a 6B4G is used instead of 2A3 in this circuit, AC hum would be more apparent, but much less pronounced than in a classic “no-feedback” circuit.
First of all, the power output of this amp is nothing short of awesome, from a 2A3 amp – that is. While 5W will not rock most houses (unless those houses are equipped with very efficient speakers), it definitely (re)produces music much louder than a classic 2A3 amp – to the point that, depending on your listening taste, you would probably not need anything more powerful 95% of the time, even with 88dB/W/m loudspeakers. Obviously, the RH300B can go much louder – and does so effortlessly after the point where the RH2A3 clips – showing that there is a definite difference in output power, quite adequate to the 5W vs. 12W comparison.


This gap in power is reduced when 1619 tubes are used. While lacking good models for the 1619 I can only estimate the power to be about 7.5W – and the best comparison probably is the RH307A Super. While the curves of the 307A look more promising than those of the 1619, both are 15W anode dissipation tubes, and the difference in curves probably stems as well from the difference in internal construction – while the 307A is a direct heated pentode, the 1619 is a direct heated beam tetrode. The direct comparison shows similar power for both amplifiers… which is quite logical to me. Thus the option to use 1619 tubes does extend the possibility to enjoy music with this amplifier.
In operation, what makes this amplifier so nice and user friendly is current consumption and heat. If you sum up the requirements for the various secondary windings on the power transformer, it becomes apparent that a nice 100VA unit will be just fine for the task – which translates into nice and small, particularly in the realm of toroids. Not to mention further size decrease if you choose to wind two transformers, of which one for the tube heaters (allowing easy and cheap modification to use i.e. 6B4G output tubes). Current draw is slightly less than 140mA, allowing you to employ a nice smallish choke… while the schematics calls for a 10H 150mA choke, I have used a 5H 150mA unit without any ill effects (like hum). Cold and relaxed in operation, particularly when compared to larger amps, you can just forget about it once you have powered it up, and concentrate on the music (or whatever else you are doing that is just being complemented by the music).


How about the sound? While the amplifier quite predictably sounds remarkably similar to other RH amplifiers, it does present some unique characteristics due to the very high quality of the output transformers used. While the socket play is an interesting feature, in a way the amplifier is built around the LL1623 output transformers – allowing for easy adaptation to the optimal load for each tube used. The low insertion loss and high intrinsic quality of the transformer are clearly felt in the sound, compared to other good quality and large size, both EI laminations and double C (4C in fact – it should be called quadruple C, I guess) core output transformers used in the RH300B and RH307A, respectively.
An initial premise about the sound in the 2A3 version is dictated by the specific output tubes. Since I am not aware of other 2A3 octal base tubes beside the Shuguang, this is probably a limiting option for tube rolling and synergistic combinations. The “old type contemporary” double anode 2A3 tubes are probably inferior in quality to the best contemporary “mono-plate” 2A3 tubes, and the “fake mesh” 300B (most probably made in the same factory) which were sold under various brand names during the years, and are known for a specific sound signature favoring great highs and mids. The RH2A3 (with 2A3 tubes) sounds remarkably similar to the RH300B, albeit with lower power. Besides unexpectedly high listening volumes when compared to other 2A3 amps, the most striking points are great, well defined, and extended bass notes – as well as great mids, particularly lower mids. We could say that the amplifier does a great performance in the “melody range”. Differing from the “fake mesh” 300B, the RH2A3 sounds more similar to the sound of the RH300B used with EH300B tubes – but the bass is even better defined, the mids finer chiseled: I guess that with the extreme similarity of the schematics, and with the same or very similar drivers used, as well as the same rectifier tube, the merit clearly goes to the Lundahl LL1623 output transformers, easily outperforming the nicely wound and rather large (and heavy, too) EI105 lamination output transformers used in my RH300B. This is an assertion that I hope to check in the future by substituting the output transformers in the RH300B.
The 1619 is a direct heated beam tetrode, and beside an increase in power, few would expect it to introduce an improvement in sound quality… but as a matter of fact, it does. Compared to the Shuguang 2A3 octal tube, the black metal 1619 tubes are visually inferior, but their sound is better balanced overall. While the bass is slightly less pronounced, it is by no means inferior due to the increase in power – but the most striking difference is less pronounced mids, and an improvement in upper mid and highs quality. The mids are less in evidence, and the general tone is even more listenable and involving. Output power is on a par with the RH307A Super, and comparing to the large 4C output transformers in that amp, the LL1623 shows even greater finesse in the upper mids, a clearness of tone that becomes particularly apparent when listening to LP records. When clear and clean upper mids are mentioned, the first thing that comes to mind is a possible exaggeration of these tones when vinyl is reproduced – but it is quite the opposite, as the upper mids and highs are not exaggerated at all, while the impression is one of increased listen-ability. The upper mids and highs result extremely clear and clean, not intrusive or evidenced.

What if?


As already mentioned, the only 2A3 octal base I know of are the older production Shuguang made specifically for Audio Innovation, which one might already own, or find a means to acquire somewhere. On the other hand, the 1619 is basically a sleeper tube – visually unattractive, odd heater voltage, direct heated, and commanding relatively low prices (mostly driven by the radio collectors market). Besides the possibility to opt for building it as a classic UX4 socket amp – which is always a good solution per se, but leads to a loss of 1619 functionality – one possibility could be adopting UX4 to octal adapters, similar to those employed to make use of 5Z3 tubes in octal sockets.


Making such an adapter should be very simple and straightforward once you procure the parts necessary – after all, it is about soldering wires between the correct pins, and fastening the two parts together – and it would allow to listen to the amp with modern 2A3 tubes as well as the highly regarded mono-plates of times long passed.  I guess employing adapters would be much easier than changing the bases on 2A3 tubes (once you unsolder the pins and dilute the “glue”, it is easy to detach the base on any given DHT… all you would need to do would be fitting the wires into the proper pins on the octal base, gluing the base and soldering the pins. A good option to glue the base could be thermally stable silicone (for heating applications)… but that might mean pushing it too far, for most!


Another very simple alternative would be to build the amp for 6B4G tubes, which can still be found at low and affordable prices (Russian 6C4C – i.e. 6S4S) – and use 6L6 tubes as an alternative. By 6L6 tubes I mean specifically the metal 6L6Y, the glass ST version 6L6, and the several Russian 6П3С, i.e. 6P3S types – all those 6L6 types are rated between 15 and 19W anode dissipation, thus perfectly suitable to be used in the circuit instead of the 1619, not to mention the possibility to employ 6V6 and 6F6 types as well – and all that with just a few circuit differences (simple modifications to be performed on an already built RH2A3-1619) as shown in the schematics.


Besides 6.3V heater windings for the output tubes (6L6 types draw 0.9V which is almost identical to the 1A drawn by the 6B4G), the main difference is the cathode connection: instead of choosing between keeping or excluding the resistor in the circuit, this time it is about choosing between “virtual cathode” (made on pin 6 – which path includes the voltage dropping resistor) or indirect heated cathode (on pin 8). Pin 1 can remain connected to ground, thus the metal envelope on 6L6Y tubes will be grounded, and EL34 tubes might be used as well with their g3 correctly grounded via pin 1.

I would like to thank Mr. Per Lundahl of Lundahl transformers, Sweden, for his kind assistance, help, and support in the realization of this project.