From: "Saved by Internet Explorer 11" Subject: Auto-Bias SE & PP Output Stages Date: Wed, 8 Apr 2015 11:44:44 -0700 MIME-Version: 1.0 Content-Type: multipart/related; type="text/html"; boundary="----=_NextPart_000_006A_01D071F1.68255B00" X-MimeOLE: Produced By Microsoft MimeOLE V6.1.7601.17609 This is a multi-part message in MIME format. ------=_NextPart_000_006A_01D071F1.68255B00 Content-Type: text/html; charset="iso-8859-1" Content-Transfer-Encoding: quoted-printable Content-Location: http://www.tubecad.com/2012/09/blog0243.htm =20 =20 Auto-Bias SE & PP Output Stages =20 =20 =20 =20 =20 =20 =20
=20
John=20 Broskie's Guide to Tube Circuit Analysis & Design =

18 September = 2012

=20

Interconnect & = Speaker=20 Cable: Long or Short?
Your speakers stand 20 = feet=20 away from your line stage amplifier, so there are (roughly) three = ways=20 that you can arrange your system: use long 19-foot interconnects = to=20 deliver the line stage's signal to the two monobloc power = amplifiers, each=20 of which sits behind the speaker it drives through an = embarrassingly short=20 1-foot length of speaker cable; or use 1-foot interconnects to the = two=20 power amplifiers and 19-foot lengths of speaker cable; or use = 10-foot=20 interconnects and 10-foot speaker cables, placing the power = amplifier in=20 the middle of the wires. Which is best? It depends is probably the = correct=20 answer.

If I had to choose, I would prefer long = interconnects=20 and short speaker cables. But what would make me happier still = would be=20 long interconnects and a very-hot line stage amplifier, which = could put=20 out 40Vpk of clean signal, more than enough to drive a unity-gain = power=20 buffer situated behind or, perhaps, located within the = loudspeaker. Why? A=20 variety of reasons, such as the pursuit of novelty and simplicity. =

Tubes work well with high voltages and can = easily=20 swing big voltages, so using a tube-based line stage makes a lot = of sense,=20 if you desire huge output swings. For example, an Aikido line = stage based=20 on a 12AX7 input tube will provide a gain of about 50 (or +34dB), = which is=20 plenty. (Of course, a flea-power power buffer, say one that put = out only=20 4W, would need only 8Vk of input signal; 50Vpk into an 8-ohm load = equals=20 156W, real watts, not peak-power watts.)

In addition, power amplifiers, be they = tube-based or=20 solid-state-based, have enough work to do by having to deliver = high=20 current into a speaker; adding voltage amplification to its lists = of tasks=20 just complicates its design and construction. And why duplicate = functions?=20 Why cascade two voltage gain stages when one will do? Freed of the = job of=20 voltage amplification, building a solid-state power buffer is = easier than=20 building the equivalent solid-state power voltage amplifier, as = the=20 unity-gain power buffer can consists of only an emitter-follower = or=20 source-follower output stage, only one stage, not the typical = three:=20 voltage-amplification stage (VAS), driver stage, and output stage. =

Or, if you fancy MOSFETs over bipolar = transistors, then=20 the LT1166=20 might be the answer.

=20

Note the 1-ohm load; with an 8-ohm load, much = higher=20 power-supply rails can be used. See Blog =20 211 for more details.

Even a single stage tube-based unity-gain, = power buffer=20 can be built, but not in a cathode-follower topology, alas. = indeed, with=20 tube power buffers, things get a bit more complicated. For = example, the=20 following tube power buffer uses a grounded-cathode amplifier. = Thus,=20 although the same amount of output voltage develops as input = voltage=20 enters, say 10Vpk in and 10Vpk out, it does so because the output=20 transformer steps down the plate voltage swings. For example, = 10Vpk goes=20 in and the plate swings 50Vpk, but the output transformer=92s 5:1 = winding=20 ratio reduces the 50Vpk to 10Vpk at the secondary.

=20

A closer approximation to a true tube-based = power=20 buffer would require at least one more stage. A tube-based,=20 negative-feedback-based, unity-gain power buffer might look like = the=20 following.

This circuit appeared in Blog=20 68, whose topic was tube power buffers. But tube and = solid-state=20 unity-gain, power buffers have been covered here countless times = (well, at=20 least countless times as far as I am willing to count). For = example, here=20 is an interesting balanced power buffer from Blog=20 190.

=20

Note the pentode topology and the = constant-current=20 source, which auto-biases the output tubes (matched tubes). = Normally, a=20 pentode output stage presents a very high output impedance, which = requires=20 that the input stage apply a big dollop of negative feedback to = reduce Zo.=20 But in this tube power buffer, the feedback is applied directly at = the=20 output tube's cathodes. Also note that the center-tapped secondary = sits at=20 the bias voltage, +36Vdc, not 0Vdc.

What appeals to me most is the simplicity of = these=20 designs. =93Simplicity is the ultimate sophistication,=94 so said = Leonardo da=20 Vinci. Less can be more, although it can just as easily be a = bore. Well,=20 I have been thinking about a stereo system that held a high-gain,=20 tube-based, line-stage amplifier and long interconnects and = monobloc=20 unity-gain power buffers, with short lengths of speaker cable. = Thus, this=20 type of circuit interested me. And as I can never leave any = circuit=20 unmodified, I have come up with a clever modification of the = single-ended=20 inverted amplifier. As Leonardo also put it so well, =93Art is = never=20 finished, only abandoned.=94

 

Auto-Bias = Single-Ended Output=20 Stages
Having just written the above = section, I must=20 quickly announce that the following design idea is not limited to = power=20 buffers; it just that power buffers were what I was examining when = the=20 idea came to me. What is this idea? It is a two-barrel affair that = solves=20 two tube-based amplifier problems, automatically biasing the = output tube=20 and improving the amplifier's PSRR. But first, let's quickly = review the=20 inverted, single-ended output stage. In a conventional = single-ended output=20 stage the output transformer sits atop the tube=92s plate, as we = saw in the=20 grounded-cathode amplifier shown before. If we do not =93ground=94 = the power=20 supply, letting it float, then we can move the output transformer = to=20 output tube=92s cathode.

It may not look right, offending the eye and = long-held=20 custom, but the amplifier functions identically to its more = conventional=20 brother. It is still a grounded-cathode amplifier, not a cathode = follower;=20 it offers the same output impedance and voltage gain; and if we = strip away=20 the two-capacitor Aikido trick from the conventional single-ended = output=20 stage, the same PSRR obtains. What we have acquired from this = inversion is=20 a slightly more efficient use of the available B+ voltage, as the = voltage=20 that the output transformer=92s primary will displace, due to its = DCR, is no=20 longer wasted, as it now serves to cathode bias the output tube. = But this=20 advantage is minor and the primary=92s DCR is no better than a = cathode=20 resistor in establishing a precise idle current. Achieving a = steady fixed=20 idle current will require a constant-current source.

The constant-current source will = automatically adjust=20 the output tube=92s grid-to-cathode voltage to maintain a fixed = idle=20 current. The large-valued electrolytic capacitor that shunts the = output=20 tube and output transformer will allow the output stage to amplify = audio=20 signals. The high-voltage battery is just a placeholder for a more = complex=20 floating power supply. In fact, this entire schematic is rather = idealized,=20 as a truly functional circuit will require more parts and more = complexity.=20 But before moving on, let=92s examine how the constant-current = source=20 shields the output stage from power-supply noise.

In this example, as long as the power-supply = noise does=20 not exceed 12Vpk, the constant-current source will vary its = voltage drop=20 with the ripple, so the output stage sees a fixed voltage window = to=20 operate within.

Okay, that=92s great, no power-supply noise = at idle, but=20 what about amplifying music? How can the output tube amplify, if = its plate=20 and cathode see a fixed DC voltage? Actually, only the cathode = sees a=20 fixed voltage, as the plate is free to move up and down in voltage = as=20 prompted by the grid signal. For example, a positive input voltage = will=20 provoke an increase in the tube=92s current conduction, which will = pull down=20 its plate voltage, just as it would in a conventional single-ended = plate=20 amplifier=97the power supply is floating after all. As the plate = pulls down=20 100V, the output transformer=92s primary sees an additional 100V = voltage=20 drop. Conversely, as the tube conducts less, its plate voltage = will=20 increase causing the output transformer=92s primary to see voltage = reversal,=20 as the electrolytic capacitor pulls it connection to the primary = upward.=20 Because the power supply is floating, each channel will require = its own=20 power supply.

What does the constant-current source see = with these=20 big plate-voltage swings? Essentially, nothing much: just the 12V = voltage=20 drop and the power-supply ripple. Relative to ground, the = constant-current=20 source is swinging up and down with the big voltage swings; but=20 differentially, the constant-current source sees the same = low-voltage=20 drop. Okay, ideally it sees the same 12V drop. But a speaker cable = breaking contact or shorting can provoke a huge primary voltage = that can=20 overwhelm the constant-current source. The workaround is a 50 cent = zener=20 diode.

Now that it has been fleshed out, I admit = that this=20 schematic looks much more complicated. The battery has been = replaced with=20 an actual high-voltage power supply. Two 270=B5F capacitors are = placed in=20 series, which halves the capacitance, but doubles the voltage = rating. The=20 two 100k resistors shunting the power supply capacitors work to = establish=20 a true voltage division between power-supply capacitors.

If the power transformer is center tapped, = then the two=20 voltage-divider resistors are not required, as the center tap will = halve=20 the voltages for us.

The LM317 is an adjustable, three-pin, = voltage=20 regulator that has been configured as a constant-current source.=20 Internally, the LM317 holds a voltage reference, an OpAmp, and a = power NPN=20 transistor. The internal OpAmp constantly monitors the voltage at = its=20 =93adjust=94 pin, comparing it to the voltage reference=92s = output.

If the adjust pin voltage falls below the = reference=20 voltage, the OpAmp increases the transistor=92s current = conduction; if the=20 adjust pin voltage climbs above the reference voltage, the OpAmp = decreases=20 the transistor=92s current until the adjust pin voltage falls = enough to=20 match the reference voltage. In other words, the LM317 strives to = maintain=20 a fixed voltage drop across 12.5-ohm resistor. Thus, if a constant = voltage=20 exists across the resistor, a constant current must flow though = the=20 resistor. The maximum voltage the LM317 can withstand is 37V; a=20 high-voltage version is available, the LM317-HV, which can = withstand 57V.=20 The 30V zener protects the LM317 against inductive kickbacks that = can=20 produce huge voltage swings on the output transformer=92s primary = and=20 against the 100=B5F capacitor's slow charge up at turn on. If the = zener sees=20 more than +30V, it begins conducting, halting the voltage increase = to 30V;=20 if the zener sees a negative voltage, it begins conducting like a = normal=20 rectifier, with a fixed voltage drop of about 0.7V. In other = words, the=20 zener sets an operational voltage window of +30V to -0.7V for the = LM317 to=20 work within.

The 0.68=B5F capacitor is needed to prevent = the=20 power-supply noise and the huge signal voltage swings from = dragging down=20 the signal source. The 200k resistor and 0.68=B5F capacitor define = a=20 low-pass RC filter with transition frequency of about 1Hz. Thus, = the DC=20 voltage gets through as though the capacitor was not there, but AC = signals=20 above 1Hz are greatly attenuated. The effective input impedance is = not=20 300k (100k + 200K) as we might guess, but 100k.

The input coupling capacitor is needed to = isolate the=20 negative-bias voltage from the signal source. The 10k grid-stopper = resistor is essential, as it prevents the output tube from = oscillating at=20 some super-sonic frequency. The 100=B5F/450V capacitor stores the = voltage=20 charge that the output tube and output transformer will work = within; it=20 can be (and should be) bypassed by a high-quality film or PIO = capacitor.=20 Since the output stage operates in single-ended, class-A, this = capacitor=20 has little work to do, as the output stage draws a fairly constant = current=20 on average.

The output transformer=92s primary is part = of the=20 biasing setup, as its DCR helps bias the output tube. With a 100mA = of idle=20 current flow, the 200-ohm DCR will drop 20Vdc, leaving it to the = LM317 to=20 drop the needed 12Vdc to establish the required -32Vdc for the = tube=92s grid=20 relative to its cathode.

 


Pure-Tube or=20 Nothing
Are you insane? Solid-state rectifiers and = voltage=20 regulators! My tube guru says that just adding an LED power = indicator to a=20 tube amplifier is enough to ruin the tone. It=92s pure tube or = nothing for=20 me. Okay, but don=92t let me catch you connecting your = pure-tube=20 amplifier to a solid-state DAC or tuner or iPod. Building a more = retro=20 version is easy enough, but we will have to forgo the better = auto-bias=20 control offered by the LM317.

The LM317 has been replaced by an inductor (a = choke)=20 and its DCR combined with the output transformer=92s primary=92s = DCR=20 effectively create a 320-ohm cathode-bias resistor. An inductor = functions=20 much like a constant-current source to AC signals, as it opposes a = change=20 in current flow through it. The 5AR4 tube rectifier replaces the=20 solid-state rectifiers and charges up the 47=B5F power-supply = capacitor. Why=20 so low a capacitor value? Too big a capacitor will damage the tube = rectifier. Remember that the bigger the capacitor, the greater the = peak=20 charging current. The zener is no longer needed, although I would = still=20 use one, just to play it safe. In many ways, this topology is = similar to=20 the old single-ended, para-feed (choke-loaded, = transformer-coupled)=20 topology.

 

Push-Pull Inverted=20 Auto-Bias
Yes, it is possible. A push-pull = version=20 will require two isolation transformers and two RC filters, one = for each=20 grid.

The constant-current source sets the idle = current, with=20 each output tube getting half, assuming matched tubes. In = addition, the=20 constant-current source filters away the power-supply noise. = Because the=20 constant-current source limits the maximum current flow, this = amplifier=20 must be run in strict, no nonsense, non-glossy-ad, real-thing, = class-A=20 mode. (The zener might actually help out here, as it could allow = the=20 amplifier to break out of the class-A envelope of operation and = intrude=20 into class-B territory, but at the cost of requiring some = tweaking.) The=20 output stage is configured as a push-pull grounded-cathode = amplifier, not=20 a cathode follower, appearances to the contrary. In other words, = the same=20 output impedance and voltage gain as if the output transformer had = been=20 located at the plates.

The zener offer the same over-voltage = protection for=20 the constant-current source. The 100=B5F power-supply capacitor = holds the=20 420V charge that defines the B+ voltage for the output stage. The = two 300k=20 grid resistors and the two 1=B5F decoupling capacitors are needed = to provide=20 a DC path to the -12Vdc and to tightly couple the isolation = transformer=92s=20 secondaries to the cathodes. Remember that the output tube will = produce=20 gain, so if 30Vpk of signal goes in the primary, 300Vpk might = develop at=20 the cathode.

One danger with any two-output-tube design, = either PP=20 or parallel SE, is that if one tube is missing from its socket = while its=20 brother is inserted, the engaged tube will conduct twice the idle = current,=20 which could damage the tube. The workaround is to place both = output tube=20 heaters in series and use a 12.6V (or 10V for 300B tubes) heater = voltage.=20 Thus, much like Christmas tree lights, if one tube is missing, the = other=20 will not heat up.

Okay, here is your homework assignment: How = could this=20 circuit be reconfigured as a power cathode follower?*


Next = Time
=20 I hope to have some good news about restocked PCBs.

 

 

* Answer:

Mind you, the isolation transformers may not = be needed,=20 but truly huge input swings, say +/-300Vpk, will be. How does one = get such=20 a huge differential input signal? One solution would be to build = an ES=20 headphone amplifier, tube-based of course. And, of course, you = could=20 switch between driving ES headphones, such as those made by Stax, = or=20 driving the following cathode-follower power output stage, which = in turn=20 would drive speakers.

=20

//JRB

     

 

=20 =20 =20 =20

 

Kit User Guide PDFs
= Click=20 image to download

<= IMG=20 width=3D"288" height=3D"425" = src=3D_http_/www.tubecad.com/2008/02/21/Attenuator%20PDF.html border=3D"0">

<= IMG=20 width=3D"290" height=3D"373" = src=3D_http_/www.tubecad.com/2011/11/25/Unbalancer%20Cover.html border=3D"0">


E-mail from GlassWare Customers = =20

Hi John,

I received the Aikido PCB today - thank you for the first = rate=20 shipping
speed.

Wanted to let you know that this is simply the best PCB I = have had in=20 my hands, bar none. The quality is fabulous, and your = documentation is=20 superb. I know you do this because you love audio, but I think = your=20 price of $39 is a bit of a giveaway! I'm sure you could charge = double=20 and still have happy customers.

Looking forward to building the Aikido, will send some = comments when=20 I'm done!

Thank you, regards,
Gary.

And=20 =20

Mr Broskie,

I bought an Aikido stereo linestage kit from you some days = ago, and I=20 received it just this Monday. I have a few things to say about = it.=20 Firstly, I'm extremely impressed at the quality of what I've = been sent.=20 In fact, this is the highest quality kit I've seen anywhere, of=20 anything. I have no idea how you managed to fit all this stuff = in under=20 what I paid for it. Second, your shipping was lightning-quick. = Just more=20 satisfaction in the bag, there. I wish everyone did business = like=20 you.

Sean H.


High-quality, double-sided, extra thick, = 2-oz traces,=20 plated-through holes, dual sets of resistor pads and pads for two = coupling=20 capacitors. Stereo and mono, octal and 9-pin printed circuit = boards=20 available.

   Designed by John Broskie = & Made=20 in USA

Aikido PCBs for as = little as=20 $24

http://glass-ware.stores.yah= oo.net/

 



Only=20 $9.95
to start=20 designing
tube-based=20 crossovers
and much more... =
=20

TCJ Filter Design

The Tube CAD Journal's first companion = program, TCJ=20 Filter Design lets you design a filter or crossover (passive, = OpAmp or tube) without having to check out = thick=20 textbooks from the library and without having to breakout the = scientific=20 calculator. This program's goal is to provide a quick and easy = display not=20 only of the frequency response, but also of the resistor and = capacitor=20 values for a passive and active filters and crossovers. =

TCJ Filter Design is easy to use, but not lightweight, = holding=20 over 60 different filter topologies and up to = four filter=20 alignments:

        Bessel, =
        =
Butterworth,=20
        = Gaussian,=20
       =20 Linkwitz-Riley.

While the program=92s main concern is active filters, = solid-state=20 and tube, it also does passive filters. In fact, it can be used to = calculate passive crossovers for use with speakers by entering 8 = ohms as=20 the terminating resistance. Click on the image below to see the = full=20 screen capture.

Tube crossovers are a major part of this program; both = buffered=20 and un-buffered tube based filters along with mono-polar and = bipolar power=20 supply topologies are covered. Available on a CD-ROM and a = downloadable=20 version (4 Megabytes).

Download or CD ROM
= Windows=20 95/98/Me/NT/2000/XP

 
www.tubecad.com =20         =20 Copyright =A9 1999-2012=20 GlassWare       =20    All=20 Rights Reserved

 

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