Kenji's K5000 Message Board Digest - Overview K5000 Resources - Overview
The Eat at Joe's K5000 Wav Resynthesis Project
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The gap between theory and reality
Saturday, 07-Mar-98 15:27:58 

     130.67.2.99 writes:

     Someone please explain to me why any attempt to translate bookish knowledge
     into sound seems to backfire on this synth. For instance, I have tried to
     emulate the behavior of a string plucked at 1/4 of its length. For the first
     24 harmonics I have used these levels:

     127, 115, 102, 0, 90, 90, 82, 0, 76, 78, 72, 0, 68, 70, 64, 0, 62, 64, 59,
     0, 57, 60, 55, 0

     Getting the attack right is a problem, of course. But it seems that no matter
     what sort of attack I use, whether or not I let the high harmonics decay faster
     than the low ones, etc., I am still miles away from the sound of a real string
     being plucked.

     In particular, I am worried about the murky sound I get with series of harmonics
     like the one above. It reminds me of the sound you get if you play a
     guitar where part of the wrapping on the wound strings is loose, if you have
     ever tried such a thing. I wonder if any of you understand precisely when and
     why this murkiness comes about.

     Could this have any connection with the incorrect phases that result when we
     enter absolute values for the levels? The series above is calculated using the
     amplitude formula sin(PI/4 * n)/n^2 - where n is the harmonic number - which
     is alternately positive and negative. The complete formula is:

     127 + 8 * ln abs(sin(PI/4 * n)/n^2/sin(PI/4)))/ln2

     Negative values do not have logarithms, so I have to use that abs() function.
     But how does this affect the composite wave function? It seems to me that a
     sum of positive terms and a sum of alternately positive and negative terms
     ought to add up to two different waves, but I am probably wrong here since
     everyone, it seems, is doing it this way. If any of you Fourier experts out
     there know the deeper reason for why the abs() values can be used, I would
     like to hear more about it.

     In any case, the murkiness is there, and the only cure that I have found is
     to avoid sustained sounds with many neighboring harmonics of comparable
     amplitude. Fortunately, this cure is at least POSSIBLE on the K5000, which is
     not the case with a number of other synths. But it would still be nice to get
     some sort of theoretical handle on sound formation on this machine.

     I hope everyone will share their thoughts and experiences with the K5000 on
     this board. It would be interesting to see more people telling about their
     work with sound formation, both the positive and negative aspect of it.

     Tore 

     tl001@online.no 

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Re: The gap between theory and reality
Sunday, 08-Mar-98 03:15:16 

     199.86.33.43 writes:

     I don't recognise the formula, but the series of harmonics looks like a 25% pulse.
     The amplitude of harmonic n for a 25% pulse should be:

     A=abs(sin(.25*Pi*n))/n

     This looks like part of your formula, but I don't recognise the rest. (Although
     it doesn't mean much that I don't).

     I got the theory to work on a few things, though. The 127-8logA formula posted
     here is very accurate. The most geometrically perfect saw I've seen
     from any of the machines I have is by applying that formula and using all
     128 harmonics. 65-128 actually make a big difference! I'll post more on that
     later.


     leiter@skypoint.com 

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Re: Re: The gap between theory and reality
Sunday, 08-Mar-98 10:07:32 

     130.67.65.106 writes:

     It may well be that the 25% pulse and a string plucked at 1/4 of its length have
     something in common. I presume that you mean to use amplitudes relative
     to the max amplitude, which makes it necessary to divide by sin(PI/4*1).
     The formula for A/Amax for a 25% pulse would then be
     abs(sin(PI/4*n)/n/sin(PI/4)). The only difference from the plucked string
     formula here is that n is not squared.

     If anyone wonders about the meaning of these formulas, it may help to to
     consider the terms A and Amax separately before they are entered into Jens'
     formula for the Level:

     Level = 127 + 8 * log2(A/Amax)

     I tried your pulse 25% for 128 harmonics, and the upper 64 harmonics do make
     a difference in the bass. This is not the case, however, for the plucked
     string sound, where the upper levels are very feeble due to that n^2 term.

     The plucked string formula may be correct for the sustain phase of that sound.
     But one probably needs a bunch of loud high harmonics that decay quickly
     in the attack phase.

     Tore

     tl001@online.no 

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Re: Re: Re: The gap between theory and reality
Sunday, 08-Mar-98 19:24:30 

     199.86.33.82 writes:

     QUOTE 
     I presume that you mean to use amplitudes relative to the max amplitude, which
     makes it necessary to divide by sin(PI/4*1). The formula for A/Amax for
     a 25% pulse would then be abs(sin(PI/4*n)/n/sin(PI/4)).
     UNQUOTE

     That gives the amplitude relative to the first harmonic, but the first isn't
     the max in a 25% pulse, the second is. As pulses get narrower, the amplitude of
     the fundamental approaches zero. 

     QUOTE
     The plucked string formula may be correct for the sustain phase of that sound.
     UNQUOTE

     Now that I think of it, narrower pulses can sound a lot like harpsichords. They
     also sound a lot like reed instruments.

     leiter@skypoint.com 

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Pulses & Plucked Strings
Monday, 09-Mar-98 04:23:25 

     130.67.2.210 writes:

     QUOTE 
     The formula for A/Amax for a 25% pulse would then be abs(sin(PI/4*n)/n/sin(PI/4)).
     UNQUOTE

     QUOTE
     That gives the amplitude relative to the first harmonic, but the first isn't the
     max in a 25% pulse, the second is.
     QUOTE

     According to my calculator:

     sin (PI/4*1)/1 = 0.707 (maximum)
     sin (PI/4*2)/2 = 0.5
     sin (PI/4*3)/3 = 0.236

     There has GOT to be some misunderstanding here.

     +-+-+-+

     QUOTE
     Now that I think of it, narrower pulses can sound a lot like harpsichords.
     UNQUOTE

     The plucked string formula presupposes that you start the vibration by pulling
     the string to one side and then let go of it. Needless to say, this is not a
     realistic picture of what happens, even on instruments that are literally "plucked". 

     I'd like to know more about what the actual sound event looks like in detail.
     Unfortunately, even the SHARC database does not seem to have that sort
     of data in it. Maybe some of you know other web sites that have raw data on
     acoustic sounds of the sort that would be of interest to K5K users.

     Tore

     tl001@online.no 

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Re: Pulses & Plucked Strings
Monday, 09-Mar-98 11:37:22 

     192.28.2.19 writes:

     QUOTE
     According to my calculator:
     sin (PI/4*1)/1 = 0.707 (maximum)
     sin (PI/4*2)/2 = 0.5
     sin (PI/4*3)/3 = 0.236
     There has GOT to be some misunderstanding here.
     UNQUOTE

     Oops, I left out the 1/n; I was just thinking about the sin(Pi/4*n) part. If you
     go out to a 10% pulse or a 5% pulse--the first harmonic is still biggest. How
     'bout that. Learn something new everyday. I guess the sin(Pi/4*n) part never
     overcomes the 1/n part.

     leiter@skypoint.com 

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Re: The gap between theory and reality
Sunday, 08-Mar-98 22:15:32 

     199.86.33.82 writes:

     QUOTE
     Negative values do not have logarithms, so I have to use that abs() function.
     But how does this affect the composite wave function? It seems to me that a
     sum of positive terms and a sum of alternately positive and negative terms
     ought to add up to two different waves, but I am probably wrong here since
     everyone, it seems, is doing it this way.
     UNQUOTE

     With a triangle wave, which also has a 1/n^2 amplitude profile, every other
     harmonic is supposed to be negative phase. If you leave them positive phase,
     the resulting wave form is like a sine that bulges out on the sides instead of
     being flattened on the sides. But--it sounds the same. (At least by itself; there
     are probably some subtle differences when you combine waves.) 

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Re: Re: The gap between theory and reality
Tuesday, 10-Mar-98 05:43:28 

     130.67.66.36 writes:

     Leafing through some books, I find that already Helmholtz asserted that we are
     not able to hear phase, so I guess this is an established fact since it has
     survived for more than a century.

     But I would like to know more about those "subtle effects". Some of you may
     have found that additive organ tones can be a strain on the K5000. (They
     can, in fact, be a strain on humans too.) I wonder if this is a matter of
     sustained amplitude only or whether the phase issue could have something to do
     with it.

     Tore

     tl001@onlin.no 

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Re: Re: Re: The gap between theory and reality
Tuesday, 10-Mar-98 11:41:15 

     192.28.2.19 writes:

     I don't know how you could hear the phase of a single harmonic, but with two
     identical harmonics the phase determines whether they cancel or reinforce.
     By subtle effects I meant the way, say, two notes in an interval interact:
     some pairs of harmonics cancel when others reinforce and vice versa.

     As far as ear strain, BBE makes an "enhancer" box that corrects for the phase
     shifts caused by electronic circuits like amplifiers. It definitely sweetens the
     sound. (Some Aiwa home stereos have this curcuit now, too.) The "enhancer" in
     the effects section of the K5k is supposed to be like the BBE box; I
     haven't tried it much yet. (The "exciter" is different, it's supposed to add
     soft distortion to the high frequency portion of the signal to generate high
     frequency even harmonics.)

     leiter@skypoint.com 

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Re: The gap between theory and reality
Monday, 09-Mar-98 07:23:09 

     12.68.130.71 writes:

     I think it is extremely cool that folks are really trying to use additive
     synthesis for what it is and not being scared by theory! 

     The plucked string, like all continuous musical events is a hard equation to
     formulate because there are really several "time blocks" of events which
     occurr. The pluck of the string itself is a deformation of the music wire which
     travels down the wire in opposite directions, reflects, passes through itself
     (adding or subtracting due to a linear domain here) until we arrive at steady
     state. The moment that is in question is actually quite fleeting --- consider that
     the attack of a violin is very different than its' steady state...the same for
     the piano...The piano undergoes a very large relative decay within 50mS of its
     attack--steady state is radically different than the first 50mS of "attack"
     (where a lot of stuff is happening to the string and it is "sorting out" to steady
     state")

     In other words, the plucked string may be correct, its placement in the whole
     scheme of the patch may be treating it as the wrong part of the steady state
     in the time domain analysis.

     ALSO- The division you are plucking at, lets say 1/5 of the strings length will
     supress the n=5 harmonic in the Fourier Analysis coefficients.

     I would try Morph Mode and making the pluck a transient event that melts into a
     simple 7 or 9 harmonic saw or square to see if it gets you closer. Also
     don't forget that the soundboard of a real instrument alters everything the
     books say about spectra of the source due to the coupling between the source
     (wire) and the amplifier (soundboard).

     For those who care try this book for a reference:
     "The Physics of Musical Instruments" by N. Fletcher and T. Rossing published
     by Springer-Verlag. (2 ISBN's???) - ISBN 0-387-94151-7 and ISBN 3-540-94151-7 

     Myself-I just figured out that all my "loud spectra" are too soft (my El_Piano
     patch is wicked guilty of this fault).

     Pete

     favant@worldnet.att.net 

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Re: "The Physics of Musical Instruments" and Plucked Strings
Tuesday, 10-Mar-98 23:56:35 

     199.86.33.88 writes:

     QUOTE
     For those who care try this book for a reference: "The Physics of Musical
     Instruments" by N. Fletcher and T. Rossing published by Springer-Verlag. (2
     ISBN's???) - ISBN 0-387-94151-7 and ISBN 3-540-94151-7 
     UNQUOTE

     Excellent book. I'm sending in an Accoustic Guitar Patch based on the
     information in the book and Jens' Formula.

     leiter@skypoint.com 


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Re: New website - new downloads
Sunday, 15-Mar-98 13:42:50 

     193.172.21.195 writes:

     I like the new layout of your page very much! I only found one bug. When i click
     on the k5000 link there opens a panel at the left. On my 15 inch monitor i
     can't see the message digest knob. I know it's there but i can't see it. Just
     want to let you know. 

     About the patches, the Zamber patch is routed to the individual out port. I
     didn't hear anything when i tried the patch. After looking in the patch data i've
     changed the out part and i could play with the patch. 

     The acoustic guitar patch works fine. I think Leiter really succeeded in programming
     the harmonics of a guitar. It's only working right in the middle section of
     my keyboard. When i play on the lower part of my keyboard, the harmonics sounding
     different. Maybe Leiter can explain why the k5k is behaving that way
     with his patch. I don't really understand this.

     Quiffy


     tcoh@hotmail.com 

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Re: Re: New website - new downloads
Sunday, 15-Mar-98 15:15:05 

     199.86.40.85 writes:

     QUOTE
     The acoustic guitar patch works fine. I think Leiter really succeeded in programming
     the harmonics of a guitar. It's only working right in the middle section of
     my keyboard. When i play on the lower part of my keyboard, the harmonics sounding
     different. Maybe Leiter can explain why the k5k is behaving that way
     with his patch. I don't really understand this.
     UNQUOTE

     Thanks. The usual guitar range is E2 up to about E5, although I think this patch
     gets too "tight" above A5. The harmonics that come through the FF are
     different for every note, e.g., around G2 and G3 the fundamental booms a bit.
     What ranges do you mean?


     leiter@skypoint.com 


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Re: Re: K5000X discontinued
Saturday, 21-Mar-98 04:43:48 

     153.34.231.34 writes:

     Maybe they are still in "selling a piano" marketing mode, and they think that the
     hardware is the selling point. I wonder if the marketing is more aggressive in
     Japan? Since we haven't heard from any Japanese users here (I have seen a link
     to my site from the Japanese page) I don't really know how popular the
     instrument is over there.

     I agree that it's very interesting how they describe the instrument - the formant
     filter particularly - in terms of how it can be used to synthesize acoustic
     instruments, and then none of the patches do just that. 

     Here's a quote from their website:

     "This new Formant Filter can be used to simulate naturally occurring tonal
     characteristics (such as the tube of a clarinet or the body of an acoustic guitar)."

     Hmmmm... I haven't gotten my K5000 back to look at the patch yet, but is this
     what Leiter's acoustic guitar patch does?


     -Kenji 

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Leiter's acoustic guitar patch
Saturday, 21-Mar-98 08:29:40 

     130.67.2.235 writes:

     Leiter employs the formant filter very actively in that patch. In fact, rather
     too actively IMO, because there are sudden changes in the amplitude in the middle
     of the keyboard. I wonder about his rationale for doing that. 

     I have some issues of "Journal of Guitar Acoustics" - in fact, I might have all
     the issues of this short-lived (?) journal. I could probably get a lot of relevant
     information out of them, I just haven't got around to it yet. Frequency response
     is one of the few things that are properly discussed from several angles in that
     magazine. The information that is sorely missing here and elsewhere (at SHARC
     e.g.) is a thorough discussion of onset transients, which are crucial for getting
     the right sound color.

     Leiter's patch seems to use the same harmonics that I had tried when I complained
     about "The gap between theory and reality". I found out afterward that I
     could improve the sound by cleaning up my envelopes. Having done this, it sounds
     a lot like a lute or classical guitar. That's OK in a way, but I would like to
     have a steel string guitar, and there is no way I can make it resemble a steel
     string just be choosing another PCM attack. Also, the "classical guitar" I get has
     gut strings all over. How to get the sound of wound strings is beyond me at present.

     Getting a good steel string guitar might be a suitable warming up exercise to
     the challenge of piano and harpsichord sounds, which are probably the hardest
     types of acoustic sound we could try for.

     Meanwhile, I am looking into FFT theory. I hope to make a program that extracts
     information from .WAV files and stuffs it directly into K5K patches. We'll
     see.

     Tore

     tl001@online.no 

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Re: Leiter's acoustic guitar patch
Saturday, 21-Mar-98 12:41:13 

     199.86.33.77 writes:

     QUOTE
     Leiter employs the formant filter very actively in that patch. In fact, rather
     too actively IMO, because there are sudden changes in the amplitude in the middle
     of the keyboard. I wonder about his rationale for doing that. 
     UNQUOTE

     I was following the chart on p.223 of Fletcher & Rossing. Some notes on a guitar
     boom a bit, for others the higher harmonics come through better, so it
     sounded natural enough.

     Looking through Fletcher and Rossing, it seems like many acoustic instruments
     have similar body resonances, with a few large spikes and valleys in the
     fundamental range and shallower, closer peaks further up the scale. See pp. 268,
     303.

     QUOTE
     Leiter's patch seems to use the same harmonics that I had tried when I complained
     about "The gap between theory and reality".
     UNQUOTE

     Yes, that was the right formula: A=sin(20%*Pi*n)/n^2. (Fletcher & Rossing p. 42).
     The waveform that amplitude profile creates is supposed to resemble the
     shape of the string before it's released, i.e. an unequal triangle. (It's the
     deriviative of a 20% pulse, sloping up for 20% of the cycle and sloping down for
     80%.)

     F&R at p. 61 (sorry for all the cites, but it's a great book!) discusses
     vibrations in strings that have stiffness, which is a major difference between
     steel and gut strings. With stiffer strings, the upper harmonics are "stretched"
     upward in pitch. It says this is one reason why stretch tuning is used on a piano,
     so the harmonics of lower strings don't beat with the upper strings.

     Unfortunately this can't be done continuously on the K5k, only stepwise, using
     another ADD for each step. I'll stop typing and give it a try.

     P.S. Long live the K5k!

     leiter@skypoint.com 

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Re: Re: Leiter's acoustic guitar patch
Saturday, 21-Mar-98 13:00:44 

     199.86.33.77 writes:

     QUOTE
     (It's the deriviative of a 20% pulse, sloping up for 20% of the cycle and sloping
     down for 80%.)
     UNQUOTE

     Ooops; integral, not derivative.

     leiter@skypoint.com 

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Re: Re: Leiter's acoustic guitar patch
Saturday, 21-Mar-98 15:50:52 

     130.67.2.249 writes:

     QUOTE
     Looking through Fletcher and Rossing, it seems like many acoustic instruments
     have similar body resonances, with a few large spikes and valleys in the
     fundamental range and shallower, closer peaks further up the scale. See pp. 268,
     303.
     UNQUOTE

     Come to think of it, we probably accept many such irregularities on "face value"
     without thinking about it whenever we actually hold and play a guitar. Maybe
     we are more disposed to hearing them when we get the same sound out of a
     keyboard, which is supposed to be more even in its response.

     Tore

     tl001@online.no 

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Re: Leiter's acoustic guitar patch
Saturday, 21-Mar-98 15:27:35 

     153.34.205.186 writes:

     For a "natural" sounding guitar, the additive sources would also need to change
     with the B String (or the D String for some guitars I guess) to simulate the
     transition between wound strings and nylon or steel strings - right? It seems to me
     (just from listening closely) that it's not only the attack transient that differs,
     but the harmonic series seems brighter for the unwound steel strings as opposed to
     the wound ones. What do the books say?

     Also, the attack "transients" on the unwound strings seem to take quite a long
     time to die out. My strings start out with a subtle, almost buzzing sound which
     takes a few seconds to decay (but still decays before the rest of the tone). The
     wound strings do not seem to have this characteristic. Then again, I have a
     slightly unusual sounding acoustic guitar.

     Again, this is just from listening, so I don't know how accurate I am.


     -Kenji 

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Re: Re: Leiter's acoustic guitar patch
Saturday, 21-Mar-98 15:50:07 

     130.67.2.249 writes:

     QUOTE
     For a "natural" sounding guitar, the additive sources would also need to change
     with the B String (or the D String for some guitars I guess) to simulate the
     transition between wound strings and nylon or steel strings - right?
     UNQUOTE

     Right. Personally I don't care whether or not I manage to program such subtleties
     in a guitar sound, but it will a problem to get this right in a piano sound. I
     wish Kawai had given us four sets of harmonics, i.e. low/soft, low/loud, high/soft
     high/loud, with seamless cross-fading between all four of them. I guess the
     solution is to use two or more sources.

     Tore

     tl001@online.no 


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Re: Re: Leiter's acoustic guitar patch
Saturday, 21-Mar-98 18:11:44 

     199.86.40.85 writes:

     Yep, synths never know what "string" you're playing on. It makes the most
     difference with a 12-string patch, where the first four strings are tuned in octaves
     and the last two are in unison. Let's call it a "feature" instead of a "bug".

     I'm sending a Folk Guitar patch that's similar to the Acoustic (gut-string) Guitar
     patch. It uses three ADD's (instead of one) for the string, seperating low, mid,
     and high harmonics to shift their pitch and "flange" them off each other. It uses
     three PCM's (instead of one) for the attack, one set on "Folk Guitar Attack",
     one to add more body on the fundamental, and one to add a metalic transient.

     leiter@skypoint.com 


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Plucked Strings
 Wednesday, 01-Jul-98 17:29:23 

      209.160.126.144 writes:

      Do I understand correctly that if a string, on a guitar for example, is plucked
      at a particular node, that harmonic will not sound? I measured the string length
      of the second string of my Les Paul (24.75 inches). I then measured the
      approximate point where the string would be plucked (3.5 inches). Dividing these
      two numbers, I got 7.07. Does this mean that the 7th harmonic will not sound?
      What about those one octave or more above it? 

      Leslie 

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Re: Plucked Strings
 Thursday, 02-Jul-98 01:12:31 

      199.86.40.75 writes:

      >Do I understand correctly that if a string, on a guitar for example, is plucked
      >at a particular node, that harmonic will not sound?

      Yep.

      >I measured the string length of the second string of my Les Paul (24.75 inches).
      >I then measured the approximate point where the string would be plucked
      >(3.5 inches). Dividing these two numbers, I got 7.07. Does this mean that the
      >7th harmonic will not sound? What about those one octave or more above it? 

      Every seventh harmonic will be missing; 7, 14, 21, etc.

      Theoretically, the force the plucked string exerts against the bridge follows a
      pulse wave. If you pluck it at 1/7 of it's length from the bridge, it's a 1/7th
      (14.3%) pulse. For anything natural sounding, though, you usually have to tone
      down the high end.


      leiter 

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Re: Re: Plucked Strings
 Thursday, 02-Jul-98 14:55:48 

      209.160.126.138 writes:

      While we are on the subject, I know that a string is intially sharp after it's been
      plucked. Generally speaking, is there more to it than that? Does the string go
      flat at all after the attack? 

      Leslie 

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Re: Re: Re: Plucked Strings
 Friday, 03-Jul-98 05:17:06 

      194.172.230.108 writes:

      Generally speaking, is there more to it than that?
      Yes. The wave that propagates along the string loses energy. The biggest energy
      loss occurs each time the wave is reflected at the bridge. The further way of
      this energy portion is: guitar body movement and then: sound. What makes it
      complicated (and pleasing to the ear) is that the energy transfer (and its overall
      decay) is frequency-dependent and that the body has resonances.
      Most people are here to talk about the K5000, so let's apply that theory to the K.
      For a good guitar emulation you need that 1/7th (or whatever) pulse
      wave spectrum, the harmonic envelopes set to a faster decay for the higher harmonics
      and a formant filter tuned to the correct resonances. Exact values can
      probably be found in the literature - I am sure someone has measured it all. I
      think Leiter mentioned a book... 

      Jens Groh 

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Re: Re: Re: Re: Plucked Strings
 Friday, 03-Jul-98 13:26:13 

      209.160.126.93 writes:

      Since the Les Paul I mentioned is a solid body electric guitar, I wonder if body
      resonaces play a lesser role than with acoustic guitars. This might make the
      waves an electric guitar produces closer to theory than their acoustic counterparts. 

      When I create a plucked sound, I use a pitch envelope to sharpen the sound at the
      onset. I was wondering what approach some of you take with the attack.


      Leslie 

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Re: Re: Re: Re: Re: Plucked Strings
 Saturday, 04-Jul-98 20:03:57 

      199.86.40.88 writes:

      >Since the Les Paul I mentioned is a solid body electric guitar, I wonder if
      >body resonaces play a lesser role than with acoustic guitars. This might make the
      >waves an electric guitar produces closer to theory than their acoustic counterparts. 

      The body still matters, but it's a lot more subtle. Some guitar players say they
      know whether they'll like a solid guitar's sound by playing it acoustically, before
      they plug it in.

      The pickups are more important; using the formant filter to model the pickup's
      frequency response would be a good idea. (And since you own an LP you
      know how important the amp is.)

      The position of the pickup must cancel harmonics just like the position that you
      pluck: harmonics with nodes directly over the pickup shouldn't be picked up;
      harmonics with maxima over the pickup are enhanced. This probably matters less
      with an LP becuase you have a two-coil humbucker pickup; one is picking
      up some of what the other misses.

      I think the pickup sees a different kind of pulse than the bridge, but I've gotta
      think about that.

      >When I create a plucked sound, I use a pitch envelope to sharpen the sound at
      >the onset. I was wondering what approach some of you take with the
      >attack.

      Same, or else a very quick /\_ . (i.e. starting from zero and quickly going sharp
      and then back.) I don't remember why I did the second one! 

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Re: Re: Re: Re: Re: Re: Plucked Strings
 Saturday, 04-Jul-98 21:00:26 

      209.160.126.111 writes:

      On the subject of attacks: In a book I have, called "A Synthesis Guide To Acoustic
      Instruments", the authors talked about the "thud" you hear in the attack
      of acoustic guitars. They put its frequency at around 100hz. I remember trying
      to recreate this by centering some inharmonic partials at 100hz and giving
      them a fast decay. I fixed the pitch of the "thud" so it would stay the same
      regardless of what key was played. I also rate scaled the amplitude so it wouldn't
      be as loud in the upper ranges. Layering this sound with the rest of my guitar patch
      made it sound much more realistic. The trick was to balance the sound so
      it wouldn't get to "boomy". 

      Leslie 

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Re: Re: Re: Re: Re: Re: Re: Plucked Strings
 Saturday, 04-Jul-98 22:56:10 

      199.86.40.89 writes:

      More on the waveform: I think a guitar pickup responds to the _velocity_ of the
      string, since it takes motion to induce a current. In that case, the pickup sees
      a positive pulse, then zero, then a negative pulse, then zero. Here's the formula:

      A(n)=(1/n)*(sin(Pi*n*X%))*(sin(Pi*n*Y%))

      where X% is the position that you pluck the string (as a percent of the whole
      length of the string) and Y% is the position of the pickup. 

      leiter 

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Re: Re: Re: Re: Re: Re: Re: Re: Plucked Strings
 Sunday, 05-Jul-98 01:24:46 

      209.160.126.137 writes:

      I measured the length of the lead pickup (since that's the one I use most of the
      time) and got 1.5 inches from its center to where the second string meets the
      bridge. So far that makes: 
      24.75 inches-total length of the second string
      3.5 inches-plucking position
      1.5 inches-center of lead pickup to bridge
      I'll plug these numbers into you're equations and see what I get. I put the
      finishing touches on my "Les Paul" guitar patch and it sounded pretty good,
      especially in the mid-range. It will be interesting to see how the new numbers work.

      "A Synthesist's Guide to Acoustic Instruments" is by Howard Massey with Alex Noyes
      and Daniel Shklair. It was published in 1987 by Amsco Publications
      (I don't know if it's still in print). It shows how to emulate various instruments
      with analog, phase distortion, and FM synthesis. There's enough general info to
      make it useful for additive synthesis. It's not really a rigoruos treatement of
      the subject, but more of a practical guide to synthesis. 

      Leslie 

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Re: Re: Re: Re: Re: Re: Re: Re: Plucked Strings
 Sunday, 05-Jul-98 06:07:54 

      209.160.126.149 writes:

      Well folks, I just got through doing the calcultions using leiter's equations
      combining the pluck position with the pickup position (actually I wrote a program
      for my old Atari St to do the calculations for me). To say I was amazed at the
      results would be an understatement. Once I finished entering all the numbers
      and adjusting the envelopes, I had a "Les Paul" sound that rivals a sample (I
      should know because I've sampled my LP several times). This is with an old K5
      keyboard to; just think what you can do with your K5000!

      By the way, the position of the Rhythem pickup is 5.5 inches from the bridge. I'm
      going to do that sound next. 

      Leslie 

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Re: Re: Re: Re: Re: Re: Re: Re: Plucked Strings
 Sunday, 05-Jul-98 10:52:05 

      195.232.55.162 writes:

      You can get the string velocity by taking the derivative of the string
      displacement. Shouldn't the 1/n term vanish then? 


      Jens Groh 

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Re: Re: Re: Re: Re: Re: Re: Re: Re: Plucked Strings
 Sunday, 05-Jul-98 13:41:55 

      199.86.33.43 writes:

      The motion above the pickup is a trapezoidal pulse, (1/n^2)(sinX%)(sinY%). As you
      approach the bridge, Y goes to 0 and the waveform approaches a
      rectangular pulse. There's no string motion at the bridge, but the force on the
      bridge is proportional to the angle the string makes as it inserts at the bridge. 

      leiter 

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Re: Re: Re: Re: Re: Re: Re: Re: Re: Re: Plucked Strings
 Sunday, 05-Jul-98 15:41:45 

      199.86.33.43 writes:

      > The motion above the pickup is a trapezoidal pulse, (1/n^2)(sinX%)(sinY%). As
      > you approach the bridge, Y goes to 0 and the waveform approaches a
      > rectangular pulse. There's no string motion at the bridge, but the force on the
      > bridge is proportional to the angle the string makes as it inserts at the bridge.

      Come to think of it, that would be the natural way to roll off the high end for
      an accoustic guitar; instead of (1/n)(sin~15%), use (1/n^2)(sin~15%)(sin~4%).
      But I think for an electric it's still (1/n)(sin~15%)(sin~21% or ~8%) 

      leiter 


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Re: Re: Re: Re: Re: Re: System Exclusive and the K500
 Friday, 10-Jul-98 03:12:43 

      209.160.126.94 writes:

      Sounds like a good idea to me; I'll try it.

      By the way leiter, have you created any sounds with the equation you came up
      with for the electric guitar? I'm still amazed at how that Les Paul patch
      sounded. One thing I noticed is that by setting the pluck position at 50% and
      the pickup position at 33% you get an almost bell like tone. Using the setings
      40% and 33% gives a sort of soft jazz guitar sound. Amazing.



      Leslie 


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Two Electric Guitar Patches
 Friday, 10-Jul-98 22:28:02 

      199.86.40.86 writes:

      I'm sending two electric guitar patches:

      Jangle: Rickenbacker 12-string electric emulation
      Twang: Telecaster lead pickup emulation

      All of the guitar emulations I've done so far have a drawback: they sound too
      harsh above about an A4. That's at least partly because the waveform is made
      on the assumption that you're plucking the string at about 1/6th its length.
      But as you play up the neck, you're plucking nearer and nearer the center of the
      vibrating string. You could put in a second ADD for plucking at about 1/3d the
      length and split the keyboard, but I haven't bothered yet.

      The FF in both of these patches is supposed to reflect the characteristics of
      the pickup. Generally, guitar pickups act like lowpass filters with a resonant
      peak. There's some good 
      information on various types of pickups at:

      http://www.seymourduncan.com/tonechart.html 

      leiter 

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And One More
 Friday, 10-Jul-98 22:58:55 

      199.86.40.86 writes:

      Here's one more:

      Jangle18: Identical to "Jangle", except it adds one more ADD detuned from the
      other two, so it's like an 18-string electric guitar.

      _This_ is what the K5k is for! :-)


      leiter 


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