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    Speakers, Amplifiers, and a Few Random Thoughts

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    Post by Peter W. Thu Oct 12, 2017 8:31 am

    With a few posts going around on the differences between various VTA amps and between them and OEM Dynaco amps and more, I thought it might be useful to go over the basics on speaker efficiency, headroom and other subtleties of the hobby. As a point of departure, just keep in mind that a 24” Cymbal Crash can be as much as 124 dB, and a snare-drum rimshot the same. Momentary ‘attacks’ can exceed 130 dB in orchestral music.

    The typical speaker efficiency range - measured mostly at one (1) watt at one (1) Meter is somewhere between about 80 dB (early AR acoustic suspension devices) to 104 dB (Klipshorn). We are not discussing sports or mutants such as those based on Lowther “full range” drivers and other sad jokes with wildly distorted specifications.

    http://www.sciencewiz.com/Portal/decibel-scale.jpg

    This is a decibel scale. Helpful to compare sound levels, no more.

    Peak-to-average: The range in dB between the loudest level of a piece of music and the *average* level. NOT the lowest level, but the average. This is important as I expect that most of us listen to music at something above “conversation” and below “Lawn Mower”. Some very well recorded pieces will have an actual P/A of 30 dB. Highly compressed stuff – head-banger music – might be less than 10 dB.

    Headroom: The amount of sustained (RMS) power available from an amplifier – which will have a linear relationship to “Peak Power” and “Instantaneous Peak Power”. The former being the amount of power an amplifier can make – typically – for about one (1) second, the latter for a few milliseconds (and why there are (usually) massive capacitors in the power-supply for an amp). NOTE: OEM Dynaco Peak Power is about 180% of rated power. I know of no good study of IPP – but rule-of-thumb is about 300% - 1000%, based on various assumptions. Not very precise to measure, but easy to discern by actual results.

    Volume: For each perceived doubling of volume, ten (10) times the power is required.

    So, one is cruising along at about 75 dB (using an 85 dB speaker, that is around 0.10 watts). Comes the loud passage on the Saint-Saens Organ Symphony – about 105 dB, and all of a sudden there you are at 100 watts. Comes the cymbal crashes – and you will need peaks of 10,000 watts for a few milliseconds.

    Using the Klipschorn, or similar, and the cymbal peaks are running closer to 100 watts – a HUGE difference.

    This is a very broad-brush description of the process – and comes down to how important the combination of speakers and amp really is, and what really will make a difference. The difference between a 35 watt amp and a 60 watt amp is about 2 dB in headroom – but depending on the speaker (Klipsch vs. AR), the effect can be larger than it appears. On the other hand, for the average speaker (88 dB or so), the difference is negligible.

    For the record VTA (and most decent) tube amps are perfectly capable of reproducing a cymbal crash assuming decent speakers and a reasonable initial volume – and why the remark “by actual results” above. But at the same time, they will struggle against highly inefficient speakers at high volume with difficult signal. That is when the brute-force approach may be necessary.

    Please feel free to jump in, add/correct/delete/suggest as you see fit. There are so many approaches to this issue that my single voice by no means tells the whole story. I am from the brute-force-inefficient-speaker school historically. But I surely recognize the appeal of a Klipschorn speaker. One day....
    arledgsc
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    Post by arledgsc Thu Oct 12, 2017 11:05 am

    Recently on another forum a person mentioned they would not consider a DAC with less than 120dB s/n.  I stated my ST120 has about 95dB s/n plus my old, tired ears are about 75dB perhaps so do you really need it and can you even notice above ambient noise?  The person on the other end claimed superhuman hearing and must live in an anechoic chamber.

    I think I read long ago that to accurately reproduce a recording of the simple "snip" of a pair of scissors requires a huge s/n and a vast amount of power from an amp.  But total noise from an source/ amp/ speaker chain is the sum of all noise including ambient. (Square root of sum of the squares).  It is only as good as the weakest link in the chain.  

    Good discussion and using the ST120 has taught me that it is all about the sound and the specs above a point are essentially meaningless.
    deepee99
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    Post by deepee99 Thu Oct 12, 2017 2:35 pm

    Peter W. wrote:With a few posts going around on the differences between various VTA amps and between them and OEM Dynaco amps and more, I thought it might be useful to go over the basics on speaker efficiency, headroom and other subtleties of the hobby. As a point of departure, just keep in mind that a 24” Cymbal Crash can be as much as 124 dB, and a snare-drum rimshot the same. Momentary ‘attacks’ can exceed 130 dB in orchestral music.

    The typical speaker efficiency range - measured mostly at one (1) watt at one (1) Meter is somewhere between about 80 dB (early AR acoustic suspension devices) to 104 dB (Klipshorn). We are not discussing sports or mutants such as those based on Lowther “full range” drivers and other sad jokes with wildly distorted specifications.

    http://www.sciencewiz.com/Portal/decibel-scale.jpg  

    This is a decibel scale. Helpful to compare sound levels, no more.

    Peak-to-average: The range in dB between the loudest level of a piece of music and the *average* level. NOT the lowest level, but the average. This is important as I expect that most of us listen to music at something above “conversation” and below “Lawn Mower”. Some very well recorded pieces will have an actual P/A of 30 dB. Highly compressed stuff – head-banger music – might be less than 10 dB.

    Headroom: The amount of sustained (RMS) power available from an amplifier – which will have a linear relationship to “Peak Power” and “Instantaneous Peak Power”. The former being the amount of power an amplifier can make – typically – for about one (1) second, the latter for a few milliseconds (and why there are (usually) massive capacitors in the power-supply for an amp). NOTE: OEM Dynaco Peak Power is about 180% of rated power. I know of no good study of IPP – but rule-of-thumb is about 300% - 1000%, based on various assumptions. Not very precise to measure, but easy to discern by actual results.

    Volume: For each perceived doubling of volume, ten (10) times the power is required.

    So, one is cruising along at about 75 dB (using an 85 dB speaker, that is around 0.10 watts).  Comes the loud passage on the Saint-Saens Organ Symphony – about 105 dB, and all of a sudden there you are at 100 watts. Comes the cymbal crashes – and you will need peaks of 10,000 watts for a few milliseconds.

    Using the Klipschorn, or similar, and the cymbal peaks are running closer to 100 watts – a HUGE difference.

    This is a very broad-brush description of the process – and comes down to how important the combination of speakers and amp really is, and what really will make a difference. The difference between a 35 watt amp and a 60 watt amp is about 2 dB in headroom – but depending on the speaker (Klipsch vs. AR), the effect can be larger than it appears. On the other hand, for the average speaker (88 dB or so), the difference is negligible.

    For the record VTA (and most decent) tube amps are perfectly capable of reproducing a cymbal crash assuming decent speakers and a reasonable initial volume – and why the remark “by actual results” above.  But at the same time, they will struggle against highly inefficient speakers at high volume with difficult signal. That is when the brute-force approach may be necessary.

    Please feel free to jump in, add/correct/delete/suggest as you see fit. There are so many approaches to this issue that my single voice by no means tells the whole story. I am from the brute-force-inefficient-speaker school historically. But I surely recognize the appeal of a Klipschorn speaker. One day....

    Problem with the Klipschorns is you need about a 60-foot-long (just guessin') listening room to benefit from them. But this is indeed a very useful discussion. Correct me if I'm wrong but I think the fundamental point you're making is that there's nothing linear in the listening equation, starting with one's own ears, their age, and that increases or decreases in SPL at a given distortion level are darn near logarithmic as regards power demands & etc. The dB/watt scale is really all we've got. Then we add in the subjectivity of the human brain and there just ain't no straight-line right answer. I trust amp-makers to stand by their RMS measurements. The whole thing recalls Bob Carver's Phase Linear 700 amp of decades ago. Specs were perfect at full power but THD & etc. were horrible at nominal listening levels - that and he used lamp cord to plug the things into AC. But folks fell for it.
    arledgsc makes a good point in that "that it is all about the sound and the specs above a point are essentially meaningless." Otherwise, we're chasing ghosts.

    Peter W.
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    Post by Peter W. Thu Oct 12, 2017 3:29 pm

    Oh, MY! Yes. And then we get into speaker and driver design and the various differences between a dome, a horn, a cone; on and off-axis response, by how much; speaker plain(s) and linear/non-linear/horizontal/vertical arrays. All of these and more than a few more each had little cult followings burning incense at little altars in their worship.

    Going through the very most (and superficial) points of each:

    Cone: What we see as a ‘typical’ speaker drive. Disperses energy over about 160 degrees at some function of angle and depth of the cone and the linearity of its excursion. Older speaker with a fixed outer diameter were nowhere near as accurate as those with flexible surrounds that move as an entirety. A very large conical section of the sphere.

    Horn: Much narrower dispersion limited by the shape of the mouth.

    Dome: a speaker that disperses its energy, theoretically, at 180 degrees, a full hemisphere.

    Axis: The direct line to the center of the speaker voice-coil.
    How it fools you: A dome will have less energy per watt of input directed on-axis as it is dispersing that energy for a full hemisphere. A horn, on the other hand, may be dispersing that same energy over a tiny fraction of the same area – so much more will be perceived on-axis. Where does that measuring microphone measure – On Axis!

    Compliance: How well do the speakers flex to reproduce accurate wave-fronts. So, one wants the cone to be rigid and hard to push air accurately and evenly. One wants it also to be very light-weight so as not to under or overshoot. And one wants the suspension to be extremely soft so as not to impede the action of the voice-coil. The voice-coil also wants to be very light-weight and very narrow to fit inside a tiny little gap – so the suspension needs to be ridged enough to hold it in that gap. But the voice-coil needs to be large enough to disperse the heat it generates and the surrounding mass needs to be large enough and close enough to absorb that heat… Off to the races.

    The FTC made pretty good regulations on how amp makers measure their RMS. Nobody other than manufacturers every did much to discuss or enlighten their buyers on how speakers really work. If you read carefully the specifications and manuals for Klipschorns – you will discover that Klipsch gives an honest assessment of those differences and why it is that their speakers require their specific placement to achieve these things. Similarly Magnepan amongst planar speaker makers does the same thing. Back in the day AR went very deeply into this issue with long white-papers around the evolution of their designs from the 3 & 11 series through the 10π to the 9. The 10π addressed this issue head-on, and that learning was incorporated into the 9.

    But the bottom line came down to making sound is about vibrating (moving) air. Making loud sound requires moving a lot of air. Making loud good sound requires moving a lot of air in very complex patterns. Managing all this takes energy.

    Cutting to the chase, why it is I feel that speakers (and other transducers) are the last remaining frontier in audio where actual progress and improvement is possible – and where the limits of diminishing returns have not yet been reached. Not so of electronics at any level. Every electronic process is established science such that the best that can be expected is *more-so*.

    Back to your ears, what pleases you and what you like. Received wisdom is deadly in this hobby. Follow Rikki-Tikki-Tavi’s family motto – and I will let you search that out on your own.
    deepee99
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    Post by deepee99 Thu Oct 12, 2017 3:49 pm

    Peter W. wrote:Oh, MY! Yes. And then we get into speaker and driver design and the various differences between a dome, a horn, a cone; on and off-axis response, by how much; speaker plain(s) and linear/non-linear/horizontal/vertical arrays. All of these and more than a few more each had little cult followings burning incense at little altars in their worship.

    Going through the very most (and superficial) points of each:

    Cone: What we see as a ‘typical’ speaker drive. Disperses energy over about 160 degrees at some function of angle and depth of the cone and the linearity of its excursion. Older speaker with a fixed outer diameter were nowhere near as accurate as those with flexible surrounds that move as an entirety. A very large conical section of the sphere.

    Horn: Much narrower dispersion limited by the shape of the mouth.

    Dome: a speaker that disperses its energy, theoretically, at 180 degrees, a full hemisphere.

    Axis:  The direct line to the center of the speaker voice-coil.
    How it fools you: A dome will have less energy per watt of input directed on-axis as it is dispersing that energy for a full hemisphere. A horn, on the other hand, may be dispersing that same energy over a tiny fraction of the same area – so much more will be perceived on-axis. Where does that measuring microphone measure – On Axis!

    Compliance: How well do the speakers flex to reproduce accurate wave-fronts. So, one wants the cone to be rigid and hard to push air accurately and evenly. One wants it also to be very light-weight so as not to under or overshoot. And one wants the suspension to be extremely soft so as not to impede the action of the voice-coil. The voice-coil also wants to be very light-weight and very narrow to fit inside a tiny little gap – so the suspension needs to be ridged enough to hold it in that gap. But the voice-coil needs to be large enough to disperse the heat it generates and the surrounding mass needs to be large enough and close enough to absorb that heat… Off to the races.

    The FTC made pretty good regulations on how amp makers measure their RMS. Nobody other than manufacturers every did much to discuss or enlighten their buyers on how speakers really work. If you read carefully the specifications and manuals for Klipschorns – you will discover that Klipsch gives an honest assessment of those differences and why it is that their speakers require their specific placement to achieve these things. Similarly Magnepan amongst planar speaker makers does the same thing. Back in the day AR went very deeply into this issue with long white-papers around the evolution of their designs from the 3 & 11 series through the 10π to the 9. The 10π addressed this issue head-on, and that learning was incorporated into the 9.

    But the bottom line came down to making sound is about vibrating (moving) air. Making loud sound requires moving a lot of air. Making loud good sound requires moving a lot of air in very complex patterns. Managing all this takes energy.

    Cutting to the chase, why it is I feel that speakers (and other transducers) are the last remaining frontier in audio where actual progress and improvement is possible – and where the limits of diminishing returns have not yet been reached. Not so of electronics at any level. Every electronic process is established science such that the best that can be expected is *more-so*.

    Back to your ears, what pleases you and what you like. Received wisdom is deadly in this hobby. Follow Rikki-Tikki-Tavi’s family motto – and I will let you search that out on your own.
    I'll run and find out.
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    Post by jasn54 Thu Oct 12, 2017 5:41 pm

    A very welcome and timely post for me (thank you Peter), as I am trying to get myself comfortable with pairing my self-built ST120 and a new pair of Elac Uni-Fi UF5 towers.  Elac rates these 4 ohm speakers at 85 dB at 2.83 v/1m, which is a bit inefficient for a tube amp, I am led to believe.

    In my medium-sized room I am, for the most part, very satisfied. The speakers, using concentric-mounted midrange/tweeter, have excellent sound stage and sufficient volume with this combo.  However, from self-inflicted, web-reading overload I wonder if I have the best pairing of devices.   Pro reviewers have claimed the speakers shine best with some significant wattage behind them, virtually all solid state.  I fret that I may be flirting with overdriving the tube amp or robbing worthwhile wattage for the upper range to push bass.  Is there a method I could employ to measure/analyze the power output?

    I also read about proper mating of amps and speakers regarding damping factor.  Apparently newer speakers, of which I am assuming includes the Elacs, rely more heavily on SS amps to provide higher levels of damping, which I am also assuming to be lacking in the ST120?.  How does damping play in to the watts/efficiency debate?

    I tell myself to just trust my ears but it would be good to understand this amp/speaker relationship a little better.  BTW, this set-up is integrated in to a switchable amp/AVR configuration which lets me blend the tube amp with subs (2 x RSL Speedwoofer 10S), but I still like being able to go simple...

    Sorry if this is a thread hijack.
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    Post by corndog71 Thu Oct 12, 2017 11:40 pm

    I would recommend using the 4 ohm tap.
    Peter W.
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    Post by Peter W. Fri Oct 13, 2017 7:40 am

    Please note the interpolations.

    jasn54 wrote:A very welcome and timely post for me (thank you Peter), as I am trying to get myself comfortable with pairing my self-built ST120 and a new pair of Elac Uni-Fi UF5 towers.  Elac rates these 4 ohm speakers at 85 dB at 2.83 v/1m, which is a bit inefficient for a tube amp, I am led to believe.

    Only a bit. Unless you are into ear-bleed volumes and/or are in a very large or very 'dead' room (lots of soft furnishings and wall hangings) you will be fine under most conditions.

    In my medium-sized room I am, for the most part, very satisfied. The speakers, using concentric-mounted midrange/tweeter, have excellent sound stage and sufficient volume with this combo.  However, from self-inflicted, web-reading overload I wonder if I have the best pairing of devices.   Pro reviewers have claimed the speakers shine best with some significant wattage behind them, virtually all solid state.  I fret that I may be flirting with overdriving the tube amp or robbing worthwhile wattage for the upper range to push bass.  Is there a method I could employ to measure/analyze the power output?

    There are ways, some simple, some complex, but all of them require a certain amount of instrumentation - more importantly an understanding of what the instruments convey. On clipping (over-driving) - anything less than 10% is considered acceptable under most conditions. And tube amps clip very softly relative to SS amps. You will know absolutely when you are clipping - bass turns to mush and treble moves toward static to some degree related to the actual signal mix.

    I also read about proper mating of amps and speakers regarding damping factor.  Apparently newer speakers, of which I am assuming includes the Elacs, rely more heavily on SS amps to provide higher levels of damping, which I am also assuming to be lacking in the ST120?.  How does damping play in to the watts/efficiency debate?

    Damping (Electric Braking) is the extent to which the amp "shorts" the output to the speaker. If you have a small DC motor, try spinning it by hand. Now try it when shorting the power leads. There will be a great deal more resistance to the spin. That is how 'damping' works - by limiting the over/undershoot of voice-coil - it is, after all, a linear DC motor (think on that, NOT an AC motor). Output transformers do not pass DC (and therefore clip softly), so the damping comes more from induction - so, yes, it is lower in tube amps. Now - your speakers with the (relatively) small, low-mass 5.5" woofers do not need much damping. You will be fine. To answer your question directly - watts and efficiency have no direct and only a very indirect relationship to damping. That is a matter of amplifier design.

    I tell myself to just trust my ears but it would be good to understand this amp/speaker relationship a little better.  BTW, this set-up is integrated in to a switchable amp/AVR configuration which lets me blend the tube amp with subs (2 x RSL Speedwoofer 10S), but I still like being able to go simple...

    Sorry if this is a thread hijack.

    Not hardly.

    Now, just for giggles - try your speakers on the 8-ohm tap. You will very slightly reduce the available power to them, but you will increase the damping *and* reduce distortion at high levels. Will it be significant? Even audible? You won't know until you try - but if you do, try it with very difficult signal - trumpet, female voice, some such. I will use the Exultate Jubilate with Kiri TeKanawa, or a good recording of the Molter trumpet concerto - both very difficult pieces for amps and speakers to do well  at any kind of volume.

    On brute-force amps  - the reality with low-efficiency speakers is that after about 60 watts, you will not notice much until you are in the 200+ watt range. And then only if you are in a large room. That is - unless you are already nearly deaf or your ears are already bleeding. For 90% of the conditions out there, 60 watts/channel/RMS is just fine. For those (like me) blessed/cursed with a large room and power-pig planar speakers, brute-force is necessary.
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    Post by jasn54 Fri Oct 13, 2017 9:21 am

    Thank you Peter for the thoughtful and helpful responses (you too corndog).  That is especially informative regarding damping.

    I am fortunate to have a nicely arranged and sized media room (perhaps in need of some sound treatments), and I am playing music at much lower levels than my early days. So I am getting comfortable with the power levels I have from the ST120.  I am actually running these speakers on the 8 ohm taps per an earlier suggestion from Bob. I also bought the new three-terminal posts from Bob but have not had a chance to install them (moving can be demanding), allowing me to experiment using either the 4 or 8 ohm taps.

    Thanks as well for the music selections for testing out my gear.  I am thinking to use Holly Cole's "Girl Talk" (quite dynamic and very natural).  I'll give this all a go and report back.
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    Post by Roy Mon Jan 15, 2018 3:15 pm

    Personally I try not to let our system go much beyond 80db much at all.. As much for my own hearing as for our kid - who complains at max of 65 really..

    I had some piano lessons recently trying out a teacher that lives near us - she had an older Bosendorfer grand in her garage.. Some thick carpet on the floor, some bitumen like panels on one wall was about all the acoustic treatment there was, and  doing my thing as quietly as I could with the lid closed even   that piano just  hurt my ears..
    She said her hearing wasnt all that good anymore so it did not bother her that much =S     At home, chasing realism to the point of matching the dynamics of a full grand piano at 2 mtrs distance  just is not so attractive to my ears to be honest.
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    Post by Jim McShane Mon Jan 15, 2018 4:19 pm

    Just a small correction so everyone knows - the Acoustic Research (AR) speaker line never had a speaker with 80db efficiency. The lowest I know of was 85db.

    You can see all the specs here: AR Speaker Specifications

    That's a great page if you need specs on the AR stuff.
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    Post by Jim McShane Mon Jan 15, 2018 5:17 pm

    jasn54 wrote:I also read about proper mating of amps and speakers regarding damping factor.  Apparently newer speakers, of which I am assuming includes the Elacs, rely more heavily on SS amps to provide higher levels of damping, which I am also assuming to be lacking in the ST120?.  How does damping play in to the watts/efficiency debate?

    Damping factor is simply the relationship of the speaker resistance/impedance to the amplifier's output resistance/impedance expressed as a ratio. It is likely to vary with frequency since both the amp output and the speaker input impedances vary with frequency. Damping does not directly impact the output power or damping factor. It CAN have an indirect impact as changes made that result in different power or efficiency may also affect the damping as a "side effect".

    As an example, the Citation II amp has a damping factor of "greater than 18" (meaning a ratio of 18 to 1). That simply means the amp output impedance is 1/18th of the speaker impedance under the test conditions. So if the test was done into an 8 Ohm load hooked to the amp's 8 Ohm tap the output impedance of the amp would be 1/18th of 8, or .45 Ohms.

    So now it may be helpful to sort out what is happening at each of the taps on a tube amp's output transformer too.

    4 Ohm taps can produce the highest current but they produce the lowest voltage. Compared to the 4 Ohm tap the 8 Ohm tap produces a higher voltage but less current.

    Look at it this way... to produce 60 watts into an 8 Ohm load the amp must be able to supply about 21.91 volts into the 8 Ohm load (power = voltage squared divided by the impedance). And to supply 21.91 volts into the 8 Ohm load requires the amp to be able to provide 2.74 amps of current (current = voltage divided by impedance).

    Now do the same calculation but with a 4 Ohm tap into a 4 Ohm load. The voltage required to get 60 watts is 15.49 volts - that's less than into 8 Ohms; but the current required is higher than into 8 Ohms at 3.87 amps.

    To make this as brief as I can what that all means is that the amp has its lowest output impedance at the 4 Ohm tap and the output impedance increases at the 8 Ohm tap (and the 16 Ohm tap if it has one). So what happens when (all else being identical) we put an 8 Ohm speaker on the 4 Ohm tap is that the power is reduced since the 4 Ohm tap can't provide the voltage that the 8 Ohm tap can. But the damping factor is increased because the amp's output impedance is lower than it was on the 8 Ohm tap but the speaker impedance is the same.

    Conversely, hooking a 4 Ohm speaker to an 8 Ohm tap increases the power (assuming the amp can supply additional current); and it reduces the damping factor because the amp's output impedance is higher than it was on the 4 Ohm tap but the speaker impedance is the same.

    As usual there is a lot more to this than what I posted. But I hope this clears up a couple things I though might be getting a bit confused in the prior posts.

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