Barkhausen tubes and other unicomponent oscillators

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The discussion centers on the Barkhausen-Kurz oscillator, highlighting its characteristics as an active device rather than a single component oscillator. The output frequency is influenced by the applied voltage and current, with the oscillator typically producing a sinewave output due to bandwidth limitations at microwave frequencies. Participants explore the potential for electron tube relaxation oscillators driven by DC inputs and discuss the construction of such devices. There is also a comparison between vacuum tube oscillators and semiconductor alternatives, with opinions on the advantages of tubes in specific applications like audio electronics. The conversation emphasizes the historical and practical significance of electron tubes in oscillator design.
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So in my insatiable curiosity about electron tubes(I've been struggling to find a comprehensive textbook that discusses them-any title suggestions?)I came across the Barkhausen-Kurz Oscillator. So my questions is as follows:


1. What is the equation(based on applied voltage and current) for the oscillator output frequency?

2. I presume that this is a sinusoidal oscillator. Are there any electron tube relaxation oscillators that can be driven by a DC input? If not, how would a single component relaxation oscillator tube be constructed?
 
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This was my "go to" tube reference back in the day.

$_35.JPG


For a downloadable pfd file of the 1936 edition go here: "www.tubebooks.org/Books/arrl_1936.pdf"
 
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A Barkhausen tube is not really a single component oscillator. It is an active device that has gain and a self resonance that can be physically tuned to a centre frequency in a specific range. By loading it with a tuned network it can be stabilised and power extracted at the wanted frequency.

Since the bandwidth of the loading at microwave frequencies is usually insufficient to pass the second harmonic, only the fundamental is available so it will have a sinewave output.

The relative voltages on the electrodes decide the gain and whether it will oscillate or not. Operating voltages also decide the DC current and the output power available.

If you are into historical microwave oscillators then I would recommend you get a copy of; Volume 7. KLYSTRONS AND MICROWAVE TRIODES, in “The MIT Radiation Laboratory Series”. Vol 7 is available as a 24 Megabyte pdf download from Jefferson Lab. https://www.jlab.org/ir/MITSeries/V7.PDF

Adjust V7 in the above link for volumes V3 through to V28, the series index.

Massachusetts Institute Of Technology, Radiation Laboratory Series.
1. RADAR SYSTEM ENGINEERING — Ridenour (Use https://www.jlab.org/ir/MITSeries/V1-1.pdf )
2. RADAR AIDS TO NAVIGATION — Hall (Use https://www.jlab.org/ir/MITSeries/V2.pdf )
3. RADAR BEACONS — Roberts
4. LORAN — Pierce, McKenzie and Woodward
5. PULSE GENERATORS — Glasoe and Lebacqz
6. MICROWAVE MAGNETRONS — Collins
7. KLYSTRONS AND MICROWAVE TRIODES — Hamilton, Knipp and Kuper
8. PRINCIPLES OF MICROWAVE CIRCUITS — Montgomery, Dicke and Purcell
9. MICROWAVE TRANSMISSION CIRCUITS — Ragan
10. WAVEGUIDE HANDBOOK — Marcuvitz
11. TECHNIQUE OF MICROWAVE MEASUREMENTS — Montgomery
12. MICROWAVE ANTENNA THEORY AND DESIGN — Silver
13. PROPAGATION OF SHORT RADIO WAVES — Kerr
14. MICROWAVE DUPLEXERS — Smullin and Montgomery
15. CRYSTAL RECTIFIERS — Torrey and Whitmer
16. MICROWAVE MIXERS — Pound
17. COMPONENTS HANDBOOK — Blackburn
18. VACUUM TUBE AMPLIFIERS — Valley and Wallman
19. WAVEFORMS — Chance, Hughes, MacNichol, Sayre and Williams
20. ELECTRONIC TIME MEASUREMENTS — Chance, Hulsizer, MacNichol and Williams
21. ELECTRONIC INSTRUMENTS — Greenwood, Holdam and MacRae
22. CATHODE RAY TUBE DISPLAYS — Soller, Starr and Valley
23. MICROWAVE RECEIVERS — Van Voorhis
24. THRESHOLD SIGNALS — Lawson and Uhlenbeck
25. THEORY OF SERVOMECHANISMS — James, Nichols and Phillips
26. RADAR SCANNERS AND RADOMES — Cady, Karelitz and Tutner
27. COMPUTING MECHANISMS AND LINKAGES — Svoboda
28. SERIES INDEX — Linford

You can usually find a printed copy by searching http://www.bookfinder.com with the title and first author's name.

The Information Resources of Jefferson Lab is often worth a visit. https://www.jlab.org/ir/
 
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If you want the ultimate vacuum tube application handbook, 1500 pages in 25MByte, google;
radiotron designer's handbook H4 pdf
 
Baluncore said:
If you want the ultimate vacuum tube application handbook, 1500 pages in 25MByte, google;
radiotron designer's handbook H4 pdf
Just downloaded it. Awesome. Is there anything about tubes it doesn't explain?

BTW Check out page 3 and note the Olathe Kansas Public Library stamp. That's just down the road from one of our mentors and about a 45 minute drive for me. Curious.

Anyway, thanks. I've got a couple vintage tube products that's on my list to restore. It may come in handy.
 
Thanks likewise - old jim
 
Baluncore said:
A Barkhausen tube is not really a single component oscillator. It is an active device that has gain and a self resonance that can be physically tuned to a centre frequency in a specific range. By loading it with a tuned network it can be stabilised and power extracted at the wanted frequency.

Since the bandwidth of the loading at microwave frequencies is usually insufficient to pass the second harmonic, only the fundamental is available so it will have a sinewave output.

The relative voltages on the electrodes decide the gain and whether it will oscillate or not. Operating voltages also decide the DC current and the output power available.

If you are into historical microwave oscillators then I would recommend you get a copy of; Volume 7. KLYSTRONS AND MICROWAVE TRIODES, in “The MIT Radiation Laboratory Series”. Vol 7 is available as a 24 Megabyte pdf download from Jefferson Lab. https://www.jlab.org/ir/MITSeries/V7.PDF

Adjust V7 in the above link for volumes V3 through to V28, the series index.

Massachusetts Institute Of Technology, Radiation Laboratory Series.
1. RADAR SYSTEM ENGINEERING — Ridenour (Use https://www.jlab.org/ir/MITSeries/V1-1.pdf )
2. RADAR AIDS TO NAVIGATION — Hall (Use https://www.jlab.org/ir/MITSeries/V2.pdf )
3. RADAR BEACONS — Roberts
4. LORAN — Pierce, McKenzie and Woodward
5. PULSE GENERATORS — Glasoe and Lebacqz
6. MICROWAVE MAGNETRONS — Collins
7. KLYSTRONS AND MICROWAVE TRIODES — Hamilton, Knipp and Kuper
8. PRINCIPLES OF MICROWAVE CIRCUITS — Montgomery, Dicke and Purcell
9. MICROWAVE TRANSMISSION CIRCUITS — Ragan
10. WAVEGUIDE HANDBOOK — Marcuvitz
11. TECHNIQUE OF MICROWAVE MEASUREMENTS — Montgomery
12. MICROWAVE ANTENNA THEORY AND DESIGN — Silver
13. PROPAGATION OF SHORT RADIO WAVES — Kerr
14. MICROWAVE DUPLEXERS — Smullin and Montgomery
15. CRYSTAL RECTIFIERS — Torrey and Whitmer
16. MICROWAVE MIXERS — Pound
17. COMPONENTS HANDBOOK — Blackburn
18. VACUUM TUBE AMPLIFIERS — Valley and Wallman
19. WAVEFORMS — Chance, Hughes, MacNichol, Sayre and Williams
20. ELECTRONIC TIME MEASUREMENTS — Chance, Hulsizer, MacNichol and Williams
21. ELECTRONIC INSTRUMENTS — Greenwood, Holdam and MacRae
22. CATHODE RAY TUBE DISPLAYS — Soller, Starr and Valley
23. MICROWAVE RECEIVERS — Van Voorhis
24. THRESHOLD SIGNALS — Lawson and Uhlenbeck
25. THEORY OF SERVOMECHANISMS — James, Nichols and Phillips
26. RADAR SCANNERS AND RADOMES — Cady, Karelitz and Tutner
27. COMPUTING MECHANISMS AND LINKAGES — Svoboda
28. SERIES INDEX — Linford

You can usually find a printed copy by searching http://www.bookfinder.com with the title and first author's name.

The Information Resources of Jefferson Lab is often worth a visit. https://www.jlab.org/ir/



The wikipedia entry on the Barkhausen-Kurz tube describes it as a self-oscillating RF electron tube. Is this not correct? Moreover...What is the response of a Barkausen-Kurz tube to a DC voltage input from experimental data?

I did see an article from the late 40s or early 50s about a Barkausen oscillator that used an electromagnet to accelerate electrons from the cathode and another electromagnet further down the tube with the opposite polarity to deflect electrons back and create bunched electron clouds.

Now for a relataxion tube oscillator, I'd imagine it to be some kind of thyratron tube with high plate capactitance.
 
By definition, no “component” is ever used “stand alone”. Just as Barkhausen tubes once were, Gunn diodes for example, are used with other circuit components and tuning networks.

You appear to be looking for a single active component that somehow has the exact frequency and waveform characteristic you want without any external control.

Why build plate capacitance into the vacuum tube when you can attach it externally and retain the flexibility of design and later adjustment? I do not understand what incentive there can be to to build the frequency determining network inside the glass envelope of the active device.
 
  • #10
Baluncore said:
By definition, no “component” is ever used “stand alone”. Just as Barkhausen tubes once were, Gunn diodes for example, are used with other circuit components and tuning networks.

You appear to be looking for a single active component that somehow has the exact frequency and waveform characteristic you want without any external control.

Why build plate capacitance into the vacuum tube when you can attach it externally and retain the flexibility of design and later adjustment? I do not understand what incentive there can be to to build the frequency determining network inside the glass envelope of the active device.


Good point. What I meant by a unicomponent oscillator wasn't a "standalone" component, but an electron tube which can generate a self-sustaining oscillating output from a DC input where the frequency depends on the input voltage supplied to it. Cavity magnetrons are a good example of the type of component I am talking about. What originally inspired my curiosity is how a self-oscillating electron tube that uses a DC input could be tuned to oscillate at much lower frequency ranges, like audio frequency, and so that is why I need to know how the frequency of a Barkhausen-Kurz tube is determined.
 
  • #11
EinsteinKreuz said:
Cavity magnetrons are a good example of the type of component I am talking about.
Unfortunately, cavity magnetron frequency is controlled by the cavity dimensions. Voltage or current operating point, or the magnetic field, have little effect on frequency. The most significant frequency variation of microwave oven magnetrons is from thermal expansion of the structure. They are designed for 2450. MHz and sweep about 100. MHz, that is 4%, in a couple of seconds when power is applied.

There is no need for vacuum tubes. The CMOS CD4046 chip contains a VCO that would meet your requirements.
 
  • #12
Baluncore said:
Unfortunately, cavity magnetron frequency is controlled by the cavity dimensions. Voltage or current operating point, or the magnetic field, have little effect on frequency. The most significant frequency variation of microwave oven magnetrons is from thermal expansion of the structure. They are designed for 2450. MHz and sweep about 100. MHz, that is 4%, in a couple of seconds when power is applied.

There is no need for vacuum tubes. The CMOS CD4046 chip contains a VCO that would meet your requirements.



Yes, and cavity magnetrons ≠ electron tubes. The thing about tube oscillators is that there are such things as Backwards Wave Oscillators(which are electron tubes with a zigzag wave guide) that can oscillate at frequencies in the terahertz range beyond what semiconductor oscillators are currently capable of. Vacuum tube oscillators, if I recall correctly, have greater frequency stability and tubes in general are less noisy than transistors. I am a firm believer in the supremacy of tubes to semiconductors when it comes to audio electronics and what brought this up is a project I am embarking on to build a vacuum tube synthesizer.
 
  • #13
Vacuum tubes still have their uses in modern equipment but having designed, built and repaired very complex tube devices for 30+ years I can tell you there is nothing 'supreme' about tubes other than they help warm the room when it's cold.

If you need some audio source ideas for your project do a search for thyratron VCO.
http://www.allaboutcircuits.com/vol_3/chpt_7/2.html
 
  • #14
I am a firm believer in the supremacy of tubes to semiconductors when it comes to audio electronics

now there'd be an interesting topic for the general discussion forum, because it's so largely subjective.

Personal theories are discouraged here on PF, BUT -------

there are interesting articles from 1980's where scientific measurements were made the harmonic content of tube vs opamp amplifiers driven into distortion,

and the high output impedance of tube amps vs low output impedance of solid state has to contribute to different transient behavior of the speaker cone(it's a linear motor).

Yes, it's subjective. A neighborhood Guitar-zan youth once showed me an old Dynaco solid state amplifier which he said "...has an unusual warmth , for a solid state amp". Looking into it i found it took most of its feedback from output current not voltage, so as to mimic a tube amp's high Zout.

There are articles published in respectable journals. If you find some, maybe mentors would allow such a thread.

No hijack intended.

old jim
 
  • #15
EinsteinKreuz said:
I am a firm believer in the supremacy of tubes to semiconductors when it comes to audio electronics
I am a firm believer that both tubes and semiconductors have their place when it comes to audio electronics. I am pragmatic and able to make the design decisions needed to select appropriate components to meet the specifications. There is nothing special about a FET with a pilot lamp.


EinsteinKreuz said:
cavity magnetrons ≠ electron tubes
Magnetrons are vacuum tubes. They support a vacuum, have a filament and a plate current.
Fleming first invented the vacuum tube rectifier. Lee DeForest added the control grid to make an amplifier. http://en.wikipedia.org/wiki/Fleming_valve

As a good example of a tunable vacuum tube oscillator you might consider the gyrotron. http://en.wikipedia.org/wiki/Gyrotron
 
  • #16
EinsteinKreuz said:
I am a firm believer in the supremacy of tubes to semiconductors when it comes to audio electronics and what brought this up is a project I am embarking on to build a vacuum tube synthesizer.

jim hardy said:
there are interesting articles from 1980's where scientific measurements were made the harmonic content of tube vs opamp amplifiers driven into distortion,
and the high output impedance of tube amps vs low output impedance of solid state has to contribute to different transient behavior of the speaker cone(it's a linear motor).

There are also some interesting psycho-acoustic experiments that showed that people in general actually prefer listening to sound reproduced with a restricted frequency range and added distortion, compared with the undistorted original.

The experiments used listening tests with music played first by human musicians hidden behind a screen (so the subjects didn't know it was a live performance) who were also recorded, followed by playback of a distorted version of the recording that had just been made.

The conclusion was that many people preferred the low quality sound that they were familiar with from their own audio equipment, rather than the "real thing".

I guess this is still true, considering how many people listen to low-bitrate MP3 files played through cheap earbuds!
 
  • #17
AlephZero said:
There are also some interesting psycho-acoustic experiments that showed that people in general actually prefer listening to sound reproduced with a restricted frequency range and added distortion, compared with the undistorted original.

I have a fairly good home theater (with acoustic room treatments, etc..) in the house with 8 large speakers of mine that look impressive but are actually vintage Radio-Shack enclosures with new speaker components and crossovers. I've found over the years that a new persons response on how they sound varies with what brand I say they are. I usually start a showing with the lights down so they can't see the equipment and they usually ask sometime during or after the movie. I'm still amazed at how subjective sound quality can be with different expectations. I'm also amazed on how people think electronics can fix a bad rooms sound. In a room designed and build for fine sound a cheap boom-box sounds good.
 
  • #18
nsaspook said:
Vacuum tubes still have their uses in modern equipment but having designed, built and repaired very complex tube devices for 30+ years I can tell you there is nothing 'supreme' about tubes other than they help warm the room when it's cold.

If you need some audio source ideas for your project do a search for thyratron VCO.
http://www.allaboutcircuits.com/vol_3/chpt_7/2.html



Nice to hear from someone who has worked with these things! :approve:

FWIW, a big part of what intrigues me about electron tubes is the ability of certain tubes to self-oscillate when supplied with a DC input voltage. Like the cavity magnetron(@baluncore I stand corrected! Never thought of magnetrons as electron tubes but indeed they are even though the ones I've seen are shaped more like a thick disk), the Barkhausen tube, and the Gyrotron.

In particularly, I've become interested in Terahertz oscillators to which often use Backward Wave Oscillator tubes. Now in the case of transistors for audio devices like amplifiers, isn't there an issue of base-emitter breakdown(leading to unwanted noise) when the amplifier power is increased to a high enough level?
 
  • #19
EinsteinKreuz said:
Now in the case of transistors for audio devices like amplifiers, isn't there an issue of base-emitter breakdown(leading to unwanted noise) when the amplifier power is increased to a high enough level?
Yes and No. That is a truism. By definition, anything “increased to a high enough level” can turn bad.
 
  • #20
EinsteinKreuz said:
In particularly, I've become interested in Terahertz oscillators to which often use Backward Wave Oscillator tubes.

We used 'twits' in the electronic warfare and jamming equipment I worked on.
http://en.wikipedia.org/wiki/AN/SLQ-32_Electronic_Warfare_Suite

This is one area where tubes might still be 'supreme'. :devil:
Even the new gear still uses tubes.
 

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  • #21
nsaspook said:
We used 'twits' in the electronic warfare and jamming equipment I worked on.

Damn. You really are a spook. Awesome. :thumbs:
 
  • #22
dlgoff said:
Damn. You really are a spook. Awesome. :thumbs:

I was just another grunt keeping things running but I was one of those guys who could fix anything. It was a nice toy but we all knew if the crap hit the fan the Russians would just launch everything they had at once to wipe us off the planet and we had a very short lead time to do the same thing.
The TWT type tubes are unique in their ability to generate high power across a wide band of radar frequencies and when designed as a LNA, provide a very low noise amplification front-end for receivers that made them perfect for a wide-band radar detector that's also resistant to EMP. They are still being used in communication satellite transponders today.

http://www.r-type.org/articles/art-030.htm
http://www3.alcatel-lucent.com/bstj/vol42-1963/articles/bstj42-4-1703.pdf
 
  • #23
nsaspook said:
They are still being used in communication satellite transponders today.
Just because you're an "old spook" doesn't take away from you being awesome. :approve:
 
  • #24
As it turns out, Vacuum tubes are making a comeback at a much tinier scale. But technical books about them are extremely scarce and usually >50 years old(out-of-print)!

I have found a plethora of books on amazon dot com about audio frequency vacuum tube amplifiers, but pretty much nothin about vacuum tube oscillators(audio frequency OR radio frequency)which is frustrating since the latter are what interest me.
 
  • #25
From 20Hz to 20kHz is a factor of 1000, so audio amplifiers need to have a very wide flat response. Oscilloscope vertical deflection amplifiers and radar receivers also required wide bandwidth.

In about 1897, Sir Oliver Lodge in London invented radio frequency tuning. Vacuum tubes followed soon after, so RF amplifiers and oscillators using VTs are usually relatively narrow band circuits with high Q. They often employ deliberate narrow band selectivity.

Since WW2 we have gradually migrated to spread spectrum and digital, both of which require wide bandwidth. But we do not use VTs since semiconductors are more reliable and use less power for signal processing.

There is plenty of VT narrow band amplifier and oscillator theory out there. Begin with the older ARRL or RSGB handbooks. Download the RMIT Rad Lab books from my earlier link if you want theory. Vol 18, Vacuum Tube Amplifiers. Vol 28, Series Index, has 3 pages indexing VT oscillators of all sorts from audio through to microwave.
 
  • #27
Understanding the interaction of phase, gain and feedback are very important in amplifier design.

Since VT amplification became available, many aspiring amplifier designers have failed in an attempt to design a stable wide-band, high-gain amplifier. Some, such as; Barkhausen-Kurz, Butler, Clapp, Colpitts, Cutton-Touly, Franklin, Gill-Morell, Hartley, Mesny, Pierce, Robert Dollar, Squire, and Vacker, have turned failure into success by giving their names to oscillators.
 
  • #28
Baluncore said:
From 20Hz to 20kHz is a factor of 1000, so audio amplifiers need to have a very wide flat response. Oscilloscope vertical deflection amplifiers and radar receivers also required wide bandwidth.

In about 1897, Sir Oliver Lodge in London invented radio frequency tuning. Vacuum tubes followed soon after, so RF amplifiers and oscillators using VTs are usually relatively narrow band circuits with high Q. They often employ deliberate narrow band selectivity.

Since WW2 we have gradually migrated to spread spectrum and digital, both of which require wide bandwidth. But we do not use VTs since semiconductors are more reliable and use less power for signal processing.

There is plenty of VT narrow band amplifier and oscillator theory out there. Begin with the older ARRL or RSGB handbooks. Download the RMIT Rad Lab books from my earlier link if you want theory. Vol 18, Vacuum Tube Amplifiers. Vol 28, Series Index, has 3 pages indexing VT oscillators of all sorts from audio through to microwave.


Will do(downloads). But what about Backward Wave Oscillators? Semiconductors have hit the lower limit for size and are almost to the upper limit for oscillator frequency. I know of no physical reason why electron tube backward wave oscillators couldn't be designed to oscillate at frequencies with multiples of 10 to 100 Thz...beyond. Did you see the link I posted about microscopic vacuum tubes?
 
  • #29
EinsteinKreuz said:
Semiconductors have hit the lower limit for size and are almost to the upper limit for oscillator frequency.

There are semiconductor designs that extend the range into the thz range with quantum mechanical effects.

http://en.wikipedia.org/wiki/Resonant-tunneling_diode
 
  • #30
@EinsteinKreuz.
A research news item constitutes a dream, not a movement. I still work with VTs in the real world and I do not have your rosy view. I put my effort into removing relays, monostables and VTs rather than looking for opportunities where I might bring them back.

Making free running oscillators is not the problem, we now need to generate and receive modulated data streams. Optical data links employ semiconductor transducers, so they really can not need VTs. VTs will never match a FET semiconductor on speed, or noise figure at room temperature. How might you cool a VT amplifier to 5°K.

There are situations where VTs are still the answer. There are also situations where a VT has no application. For example, there are “non-linear transmission lines” made from semiconductors that sharpen pulse edges and make data links, sampling mixers and oscilloscopes with quite ridiculous speed and resolution. That cannot possibly be done with VTs.
 
  • #31
In the end it's tubes that get the last laugh. Every transistors daddy is a tube, it might be a big tube with lots of vacuum pumps and controllers but most of the machines that form the basic layers and do the doping have the basics of filaments, cathodes, control grids, suppression grids or plates and anodes in their guts.
 
  • #32
Baluncore said:
@EinsteinKreuz.
A research news item constitutes a dream, not a movement. I still work with VTs in the real world and I do not have your rosy view. I put my effort into removing relays, monostables and VTs rather than looking for opportunities where I might bring them back.

Making free running oscillators is not the problem, we now need to generate and receive modulated data streams. Optical data links employ semiconductor transducers, so they really can not need VTs. VTs will never match a FET semiconductor on speed, or noise figure at room temperature. How might you cool a VT amplifier to 5°K.

There are situations where VTs are still the answer. There are also situations where a VT has no application. For example, there are “non-linear transmission lines” made from semiconductors that sharpen pulse edges and make data links, sampling mixers and oscilloscopes with quite ridiculous speed and resolution. That cannot possibly be done with VTs.



Well yes. These microscopic vacuum tubes are still in the R&D phase and haven't fully been put into use. And I do not dispute that there are electronics applications where VTs aren't useful and can only be done with semiconductors. And do not misunderstand me: I was not saying that semiconductors are useless!
 
  • #33
nsaspook said:
There are semiconductor designs that extend the range into the thz range with quantum mechanical effects.

http://en.wikipedia.org/wiki/Resonant-tunneling_diode


True. But the thing is that electrons in semiconductors have certain allowed energy states(energy bands)whereas free electrons can have any energy. The higher the oscillation frequency of an electron or a photon the higher the energy it carries( E = h\nu)so if you want to go up to frequencies that are in the 100 Thz or Petahertz range and beyond it would be easier to accomplish this with free electron tubes. There is a team of scientists in Deutschland developing an opto-electronic petahertz oscillator using femtosecond laser pulses.
 
  • #34
Baluncore said:
Since WW2 we have gradually migrated to spread spectrum and digital, both of which require wide bandwidth. But we do not use VTs since semiconductors are more reliable and use less power for signal processing.
In the case of audio electronics, digital will never truly replace analog because without conversion back into analog, you wouldn't be able to hear digitized recorded sound!
The problem with analog transistor amplifiers is that semiconductors are nonlinear in terms of the output current response to input voltages( collector current plotted against base-emitter voltage) and have very low impedance. This causes unwanted distortion of large signals(the clipping effect which is very unpleasant to the human ear). To minimize the distortion of large signals you need bypass capacitors and swamping resistors. Buuuuuuuuuuuuuuuuut...this has a filtering effect which can remove desirable frequencies from the signal.

VTs, when operated below their maximum voltage rating, have a linear response to changes in input voltages with the notable exception of the Tetrode. So while their power requirements are larger, you have much higher fidelity to the input signal unless you overdrive your tubes the way a guitar amp does(where distortion is desirable). The intentional distortion of triode guitar amps is pleasing to the human ear which is why tube amps are preferred to transistor amps. I've also noticed as an audiophile the superior sound of tube stereo amplifiers when playing records because there isn't that obnoxious humming sound coming through.
nsaspook said:
In the end it's tubes that get the last laugh. Every transistors daddy is a tube, it might be a big tube with lots of vacuum pumps and controllers but most of the machines that form the basic layers and do the doping have the basics of filaments, cathodes, control grids, suppression grids or plates and anodes in their guts.

I'm with you. And the advantage of tubes for high voltage AC, RF, and military electronics is that semiconductors are highly sensitive to electromagnetic interference. This makes them vulnerable to electromagnetic weapons and in the case of high-voltage semiconductors used in the power grid, geomagnetic storms. The reliance of solid state high powered switches makes the US power grid extremely vulnerable to EMP weapons and large Solar Flares.
 
  • #36
EinsteinKreuz said:
In the case of audio electronics, digital will never truly replace analog because without conversion back into analog, you wouldn't be able to hear digitized recorded sound!
Not true. That is where the semiconductor H-bridge, class D amplifier, works well.

EinsteinKreuz said:
The problem with analog transistor amplifiers is that semiconductors are nonlinear in terms of the output current response to input voltages( collector current plotted against base-emitter voltage) and have very low impedance. This causes unwanted distortion of large signals(the clipping effect which is very unpleasant to the human ear).
Not true. You are assuming class A, without feedback. In reality, analogue transistor amplifiers are way more linear than VT amplifiers. That is because the circuit can be designed using many more integrated transistors than could possibly be done with VTs. It it possible to build ultra-linear SC amplifiers that require only milliwatts of power. Saturation of any device will always cause harmonic distortion. VTs and SCs both have the same saturation problem.

EinsteinKreuz said:
To minimize the distortion of large signals you need bypass capacitors and swamping resistors.
Semiconductors do not require coupling capacitors or level-shifting because two polarities of device are available.
A VT is an N-channel FET with a pilot lamp. There is no equivalent to the P-channel FET in VTs.

It is a mistake to argue that VTs are better than SCs. There are places where each has it's place.
Emotions are not rational. People who think VTs are better will buy higher priced VT audio amplifiers.
 
  • #37
Baluncore said:
Not true. That is where the semiconductor H-bridge, class D amplifier, works well.Not true. You are assuming class A, without feedback. In reality, analogue transistor amplifiers are way more linear than VT amplifiers. That is because the circuit can be designed using many more integrated transistors than could possibly be done with VTs. It it possible to build ultra-linear SC amplifiers that require only milliwatts of power. Saturation of any device will always cause harmonic distortion. VTs and SCs both have the same saturation problem.

Semiconductors do not require coupling capacitors or level-shifting because two polarities of device are available.
A VT is an N-channel FET with a pilot lamp. There is no equivalent to the P-channel FET in VTs.

It is a mistake to argue that VTs are better than SCs. There are places where each has it's place.
Emotions are not rational. People who think VTs are better will buy higher priced VT audio amplifiers.
Well when it comes to emotions and the sound quality of audio amplifiers, what matters in this context is which is more pleasing to the human ear. Conversion from analog to digital results in a loss of information because an ADC has a *finite* sampling rate(whereas if it had a countably infinite number of clock cycles per second it would be essentially continuous)and so values between those sampling points will not be discarded. Now with respect to your claims about Class-D amplifiers, I can't say that I'm entirely convinced about the sound quality and & I'm evidently not alone.

Now in the case of saturation and harmonic distortion, the kind that is produced in transistors is known to be very unpleasant to the human ear(clipping, crossover, and in the worst case avalanche noise)compared to that produced by thermionic valves.
 
  • #38
Audio amplifier quality is all quite off topic for "barkhausen-tubes-and-other-unicomponent-oscillators".
EinsteinKreuz said:
Conversion from analog to digital results in a loss of information because an ADC has a *finite* sampling rate(whereas if it had a countably infinite number of clock cycles per second it would be essentially continuous)and so values between those sampling points will not be discarded.
That is a complete fallacy. The bandwidth of an audio amplifier limits the highest frequencies present. You clearly do not understand the Nyquist–Shannon sampling theorem, it says that if the data rate is more than twice the audio bandwidth, then there should be no difference between analogue and reconstructed digital signals. Your ears limit the bandwidth more than the technology. http://en.wikipedia.org/wiki/Nyquist–Shannon_sampling_theorem

EinsteinKreuz said:
Now in the case of saturation and harmonic distortion, the kind that is produced in transistors is known to be very unpleasant to the human ear(clipping, crossover, and in the worst case avalanche noise)compared to that produced by thermionic valves.
Saturation or clipping does not happen in a properly designed and operated amplifiers. Clipping should never occur, (except deliberately in some guitar amplifiers).

Harmonic distortion is evidence of non-linearity. It is easier to design and build an ultra-linear SC amplifier than a linear VT amplifier. Harmonic distortion is quite irrelevant to the VT versus SC argument.

Crossover noise is only a problem when an amplifier is driving a load with higher impedance than it was designed to drive. Again it is quite irrelevant to the VT versus SC argument.

Avalanche noise is produced by reverse biassed SC junctions in breakdown. That is why Zener diodes should not be used for voltage references or level shifting in audio amplifiers without sufficient low-pass filtering. Avalanche noise is not a problem.

If you name enough possible problems you will cause unfounded fears, uncertainty and doubt in the uneducated. When something fails because of poor design or out-of-spec operating conditions then that cannot be used as evidence in an argument between VTs and SCs.
 
  • #39
One needs to compare analog to digital using same program material.

I have Fiedler;s "Pops Roundup" on both vinyl and CD.
MI0002431447.jpg


That is a classic recording because the quality is so good.
Tony Salvatore was the recording engineer.

When RCA made the CD they restored the original Ampex vacuum tube tape recorder they'd used to make the original masters... digitized that analog signal
so the quality of both is about as good as either medium can get.

The CD version just plain outshines the vinyl even though both come from same master recording played on same equipment..
i think it's because the dynamic range that's available on a CD exceeds what you can do with a needle and groove
irrespective of whether the speaker cone is driven by class A, AB or D .

Doubtless cheap digital won't be as good as expensive analog.

Is my test flawed?

old jim
 
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  • #40
Baluncore said:
Audio amplifier quality is all quite off topic for "barkhausen-tubes-and-other-unicomponent-oscillators".

That is a complete fallacy. The bandwidth of an audio amplifier limits the highest frequencies present. You clearly do not understand the Nyquist–Shannon sampling theorem, it says that if the data rate is more than twice the audio bandwidth, then there should be no difference between analogue and reconstructed digital signals. Your ears limit the bandwidth more than the technology. http://en.wikipedia.org/wiki/Nyquist–Shannon_sampling_theorem
Yes, I am aware of the celebrated Nyquist theorem but there again, that is a mathematical theorem which has been proven mathematically but electrical engineering is not pure mathematics and the theory doesn't always correspond with real data.

Also, speaking of wikipedia, did you see the section on Aliasing in the article were analog and digital recording technologies are compared?
From the article:

Technical difficulty arises with digital sampling in that all high frequency signal content above the Nyquist frequency must be removed prior to sampling, which, if not done, will result in these ultrasonic frequencies "folding over" into frequencies which are in the audible range, producing a kind of distortion called aliasing. The difficulty is that designing a brick-wall anti-aliasing filter, a filter which would precisely remove all frequency content exactly above or below a certain cutoff frequency, is impractical.[8] Instead, a sample rate is usually chosen which is above the theoretical requirement. This solution is called oversampling, and allows a less aggressive and lower-cost anti-aliasing filter to be used.

Unlike digital audio systems, analog systems do not require filters for bandlimiting. These filters act to prevent aliasing distortions in digital equipment. Early digital systems may have suffered from a number of signal degradations related to the use of analog anti-aliasing filters, e.g., time dispersion, nonlinear distortion, temperature dependence of filters etc. (Hawksford 1991:8). Even with sophisticated anti-aliasing filters used in the recorder, it is still demanding for the player not to introduce more distortion.
 
  • #41
I have built my share of both vacuum-tube and solid-state amplifiers, and I have a couple of comments to the "Hi-Fi debate" that is starting to show. here.

As to harmonic distortion: The link in my previous post refers to the "Williamson amplifier", widely known as the best tube amplifier ever. Look at the schematic. After the tube amplifier sits the output transformer. Big and heavy. And - as all iron-core transformers - introducing a fair amount of distortion due to hysteresis, leakage inductance and wiring capacitance. Yes, we tried to do feedback around the output transformer, but it was not very successful.

As to other kinds of distortion: Read through this paper: http://www.linearaudio.nl/linearaudio.nl/images/pdf/otala%20low%20tim%20amp.pdf
This is the famous paper by Matti Ottala that discusses Transient Intermodulation Distortion and shows an example of an amplifier with very little TIM.

As to digital vs. analog audio: Yes, digital audio is sampled - this introduces a digitizing noise floor of -84dB. But vinyl is not without its problems either - the signal is run through a complex high-pass filter before engraving, and must therefore be run through a matching low-pass filter (the well-known RIAA stage) before amplification. This circuit is not easy to design.
 
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  • #42
EinsteinKreuz said:
Yes, I am aware of the celebrated Nyquist theorem
It is actually “Shannon's sampling theorem”. It should not be referred to as the “Nyquist Theorem”. Others have attached Nyquist's name to parameters such as the “Nyquist frequency” and the “Nyquist rate”.

EinsteinKreuz said:
theory doesn't always correspond with real data.
That is a problem with competency to take measurements of real data, or an inability to understand and apply the theory correctly. This is a Physics Forum, so the real data and the theory do correspond. If they did not, then I would want to know why. Can you give an example where “theory doesn't always correspond with real data”.

Wiki said:
Unlike digital audio systems, analog systems do not require filters for bandlimiting.
Wiki is correct. Analogue circuits are inherently low-pass filters so they do not need filtering. Band limiting immediately prior to digitisation is part of the analogue to digital conversion process. It takes place at such a high frequency that it is well outside the audio band.
 
  • #43
Svein said:
I have built my share of both vacuum-tube and solid-state amplifiers, and I have a couple of comments to the "Hi-Fi debate" that is starting to show. here.

As to harmonic distortion: The link in my previous post refers to the "Williamson amplifier", widely known as the best tube amplifier ever. Look at the schematic. After the tube amplifier sits the output transformer. Big and heavy. And - as all iron-core transformers - introducing a fair amount of distortion due to hysteresis, leakage inductance and wiring capacitance. Yes, we tried to do feedback around the output transformer, but it was not very successful.

As to other kinds of distortion: Read through this paper: http://www.linearaudio.nl/linearaudio.nl/images/pdf/otala%20low%20tim%20amp.pdf
This is the famous paper by Matti Ottala that discusses Transient Intermodulation Distortion and shows an example of an amplifier with very little TIM.

As to digital vs. analog audio: Yes, digital audio is sampled - this introduces a digitizing noise floor of -84dB. But vinyl is not without its problems either - the signal is run through a complex high-pass filter before engraving, and must therefore be run through a matching low-pass filter (the well-known RIAA stage) before amplification. This circuit is not easy to design.

Regarding Vinyl, I have no doubt that these circuits are not easy to design. But Hi-Fi stands for High Fidelity(the accuracy to the original sound/recording).

That being said, I just got a brand new tube amp for my record player and WOW! I can definitely hear big improvement in sound quality to a transistor amplifier when it comes to vinyl. Playing a record through transistor amplifiers that I've heard results in an obnoxious, low frequency hum coming from the turntable whereas with a tube amp that noise is completely eliminated. I'm definitely sticking with VTs for audio amplifiers.
 
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  • #44
EinsteinKreuz said:
Playing a record through transistor amplifiers that I've heard results in an obnoxious, low frequency hum coming from the turntable whereas with a tube amp that noise is completely eliminated.
Well - either the hum comes from the turntable or it does not.
  • If the hum comes from the turntable it should be reproduced by a good amplifier. If the hum isn't present through the tube amplifier I suspect a 60Hz high-pass filter somewhere, since tube amplifiers usually had problems with hum (the filaments used AC, and that AC had a tendency to insert itself in the audio chain).
  • If the does not come from the turntable, it is harder to say what happens. It depends on the pickup, the cable and whether or not the RIAA stage is inside the amplifier or outside. A relevant test is to short-circuit the phono inputs on the amplifiers and listen for hum.
As an aside: Hi-fi pickups are usually very low-impedance things. Therefore, using shielded cables does not keep hum from entering the wires, you need good quality twisted pair cables. For the same reason tube preamps have a hard time handling raw pickup signals.

Observe: I do not say that transistor amplifiers are "better" than tube amplifiers. What I try to say is that a tube amplifier is a voltage amplifier, and needs an impedance transformer to match the low-impedance loudspeakers. A transistor amplifier is a current amplifier and has a very low impedance output, interfacing nicely with the loudspeakers.

I am somewhat surprised that no one has mentioned MOSFET-based amplifiers. A MOSFET has the same voltage-amplifier characteristics as a tube, can operate at high voltages and can interface directly with loudspeakers.
 
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