Return-Path: Received: from [24.25.9.101] (HELO ms-smtp-02-eri0.southeast.rr.com) by logan.com (CommuniGate Pro SMTP 4.1.6) with ESMTP id 2715087 for flyrotary@lancaironline.net; Sat, 08 Nov 2003 09:06:31 -0500 Received: from o7y6b5 (clt78-020.carolina.rr.com [24.93.78.20]) by ms-smtp-02-eri0.southeast.rr.com (8.12.10/8.12.7) with SMTP id hA8E6MLR006546 for ; Sat, 8 Nov 2003 09:06:23 -0500 (EST) Message-ID: <004201c3a601$006fa240$1702a8c0@WorkGroup> From: "Ed Anderson" To: "Rotary motors in aircraft" Subject: Re: DIE LIVES! Date: Sat, 8 Nov 2003 09:02:52 -0500 MIME-Version: 1.0 Content-Type: multipart/mixed; boundary="----=_NextPart_000_003E_01C3A5D7.1734E500" X-Priority: 3 X-MSMail-Priority: Normal X-Mailer: Microsoft Outlook Express 6.00.2800.1106 X-MIMEOLE: Produced By Microsoft MimeOLE V6.00.2800.1106 X-Virus-Scanned: Symantec AntiVirus Scan Engine This is a multi-part message in MIME format. ------=_NextPart_000_003E_01C3A5D7.1734E500 Content-Type: multipart/alternative; boundary="----=_NextPart_001_003F_01C3A5D7.1734E500" ------=_NextPart_001_003F_01C3A5D7.1734E500 Content-Type: text/plain; charset="iso-8859-1" Content-Transfer-Encoding: quoted-printable =20 Hi Folks=20 =20 The reason I am e mailing you is I just found a very interesting SAE = paper written by some of the Honda motorcycle engineers back in 1970, = one by name of Shaon Yagi. A great paper overall on what design features = of an engine are of most importance in production of power. But, one = part of the paper talked about tuning by Pulse induction tuning! Well, = that got my attention! I was surprised and stunned to find out that = the equations that Yagi shows and my DIE equations are equivalents!=20 There are some differences, but I think they are related to how the = pulses are used (he only uses the "A" pulse formed by closing of the = intake valve) and his is for four stroke engines and of course the cycle = timing of the rotary on intake is like a two stroke timing wise. So I = think those differences account for most of the differences in our = equations. His equations clearly show that port timing plays a crucial role in = pulse tuning as did my independent derivation for the twin rotor. This = relevation was probably the most significant in my findings as well. I = have attached the page addressing "Pluse Tuning" from the paper for = those of you who may be interested. In any case, referencing page 10, his first equation for "t" and my = "Ta" equations are amost identical, clearly showing that port timing = places a crucial role in pulse tuning - be it 4 stroke piston engine or = rotary. I found his equation regarding "Pulse Tuning" (same as DIE) on page = 10. Yagi's equation t =3D (f*/360)*(60/Ne) Where Ne is shaft rpm and = f* is the degree of crankshaft rotation from inlet valve closure to TDC = during inlet operation of the next succeeding cycle. The formula seemed vaguely familiar, then I realized if I revised it = slightly I could express it as: t =3D f*/(360*(Ne/60)) and the reason for the familarity was readily = apparent. Recall my equation for Time Available Ta? Well with my Ad = =3Df* the two equations are equivalent=20 My Ta =3D Ad/(360*(rpm/60)) or Yagi's t =3D f*/(360*(rpm/60)) = where Ne =3D RPM Ta =3D Ad/Ars Where Ad =3D Angular Difference and Ars =3D Angular = rotational speed of the E shaft Well=20 Ars Angular Rotation Speed (Deg/Sec) =3D 360*(RPM/60)=20 which of course in Yagi's equation is the (1/360)*(60/Ne) factor. So basically my Ta =3D Ad/(360*(RPM/60) (where f* is the = equivalent of my Ad.) and Yagi's equation are equivalent. His f* and my Ad are a bit different, but I think that is because = he is working on a 4 stroke and I on the rotary which acts like a 2 = stroke in its induction cycle. Also he is having the pulse return to = the cylinder in time for the next induction cycle of that cylinder (sort = of a round trip) and mine only goes one way from rotor to rotor. Or = perhaps its simply a different arrival point is required for returning = the pulse to its generating cylinder just as it is about/begining to = open rather than as it is closing (as is the second rotor's intake in = the DIE analysis) is resonsible. His f* =3D 180deg-IC, IC =3D inlet valve closing angle expressed = as ABDC. My Ad =3D 90+IC-IO But, again I think its because he is "supercharging" the same = cylinder the pulse came from (and using the "A" pulse instead of the "B" = pulse). So his interval is from closing to opening on the same cylinder = and mine is from opening to closing on different cylinders/rotor. = Perhaps some of you folks can provide clarity on this point for a four = stroke reciprocating engine. We also have the equivalent Tr (time required) with mine Tr =3D L/vp = and his t =3D 4*L/As His As is my Vp (speed of sound). The only thing I = don't understand is why his time for the pulse to travel the length of = the intake pipe is equal to 4*L instead of my 1*L. It appears as though = he is making his pulse travel 4 times the length of the intake manifold, = but then its is not abolutely clear what his intake pipe length really = is. It may have to do with a multiple bounce of pulses. i.e. using = every 4th pulse? or perhaps because there is the "rest" stroke on a 4 = stoke cycle which the rotary does not have? Just not clear to me at this = point, why the 4*L. In any case, he eventually ends up with the equivalent of my = parametric equation! I could hardly believe it! Solving for Length of the manifold "L" = in his equation His was L =3D As* f* /gt4*(6*Ne) wereas mine was L =3D = Vp*(Ad)/6*RPM (or it could be reduced to that form) where my Ad =3D f* = and my Vp =3D his As The gt factor in his equation is a pulse selection = factor - do you want to tune by the first pulse in which case gt =3D 1 = or perhaps a 2nd or 4th pulse in which case gt =3D 2,4, etc. Since I = was only concerned with the first pulse gt became 1 and isn't a factor = in my equation. But, I think it may indicate a point that some of you = raised during the presentation (Finn?) that perhaps there are some DIE = effect at mulitples of "L" if the pulse retains sufficient energy after = several trips through the intake. The only thing that I can't explain about his equation is the factor = or "4" for his Time required for the pulse to transverse the intake = pipe. So, now more than ever, I know my orginal analysis is on solid = ground. The only other difference is that he apparently does not address = any pulse duration effect in his equation. Perhaps this is not as = critical when the pulse returns to the port that generates it? Perhaps = with the shorter L implied for the two rotor timing is more critical and = the pulse duration must be accounted for? =20 In any case, its great to find independent confirmation for my = derivations or at the very least, it clearly shows that Port timing is = crucial in pulse tuning or DIE as I showed, but which some folks = apparently still don't believe or understand. Just thought you might = like to know that the DIE analysis is on frimer ground than just based = the quality of my derivation. =20 Best Regards Ed Anderson Ed Anderson RV-6A N494BW Rotary Powered Matthews, NC eanderson@carolina.rr.com ------=_NextPart_001_003F_01C3A5D7.1734E500 Content-Type: text/html; charset="iso-8859-1" Content-Transfer-Encoding: quoted-printable
 
Hi Folks
  
The reason I am e mailing you is I = just found a=20 very interesting SAE paper written by some of the Honda motorcycle = engineers=20 back in 1970, one by name of Shaon Yagi. A great paper overall = on what=20 design features of an engine are of most importance in = production of=20 power.  But, one part of the paper talked about tuning by = Pulse=20 induction tuning!  Well, that got my attention!  I was = surprised=20 and stunned to find out that  the equations that Yagi shows and = my DIE=20 equations are equivalents! 
 
 There are some differences, = but I think=20 they are related to how the pulses are used (he only uses the "A" = pulse=20 formed by closing of the intake valve) and his is for four stroke = engines=20 and of course the cycle timing of the rotary on intake is like a two = stroke=20 timing wise.  So I think those differences account for most of = the=20 differences in our equations.
 
His equations clearly show that=20 port timing plays a crucial role in pulse = tuning=20 as did my independent derivation for the twin rotor. This relevation = was=20 probably the most significant in my findings as well.  I have = attached=20 the page addressing "Pluse Tuning" from the paper for those of you = who may=20 be interested.
 
In any case, referencing page 10, = his first=20 equation for "t" and my "Ta" equations are amost identical, clearly = showing=20 that port timing places a crucial role in = pulse=20 tuning - be it 4 stroke piston engine or rotary.
 
I found his equation = regarding "Pulse=20 Tuning" (same as DIE) on page 10.
 
 Yagi's equation = t =3D (f*/360)*(60/Ne)  Where = Ne is shaft rpm and f*  is the degree = of crankshaft=20 rotation from inlet valve closure to TDC during inlet operation of = the next=20 succeeding cycle.

The formula seemed vaguely familiar, = then I=20 realized if I revised it slightly I could express it as:

t =3D f*/(360*(Ne/60)) and the reason = for the=20 familarity was readily apparent. Recall my equation for Time = Available=20 Ta?  Well with my Ad=20 =3Df*    the = two=20 equations are equivalent

My=20 Ta =3D Ad/(360*(rpm/60)) or  Yagi's=20  t =3D f*/(360*(rpm/60)) where Ne = =3D=20 RPM

Ta =3D Ad/Ars  = Where=20 Ad = =3D Angular=20 Difference and Ars=20 =3D Angular rotational speed of the E=20 shaft

Well

Ars  Angular Rotation Speed (Deg/Sec) =3D=20 360*(RPM/60) =

which of course in Yagi's = equation is=20 the (1/360)*(60/Ne)=20 factor.

So basically my = Ta =3D Ad/(360*(RPM/60) (where = f*   is the = equivalent of=20 my Ad.)  and Yagi's equation are=20 equivalent.

His f*  and my = Ad=20 are a bit different, but I think that is = because he=20 is working on a 4 stroke and I on the rotary which acts like a 2 = stroke in=20 its induction cycle.  Also he is having the pulse return to the = cylinder in time for the next induction cycle = of that=20 cylinder (sort of a round trip) and mine only goes one way from = rotor to=20 rotor.  Or perhaps its simply a different arrival point is = required for=20 returning the pulse to its generating cylinder just as it is = about/begining=20 to open rather than as it is closing (as is the second rotor's = intake in the=20 DIE analysis) is resonsible.

His  f*  =3D 180deg-IC,   IC =3D inlet=20 valve closing angle expressed as ABDC.  = My=20 Ad =3D=20 90+IC-IO

But, again I think its because he is=20 "supercharging" the same cylinder the pulse came from (and using the = "A"=20 pulse instead of the "B" pulse).  So his interval is from = closing to=20 opening on the same cylinder and mine is from opening to closing on=20 different cylinders/rotor.  Perhaps some of you folks can = provide=20 clarity on this point for a four stroke reciprocating=20 engine.

We also have the equivalent Tr (time = required)=20 with mine Tr = =3D=20 L/vp and his

t =3D 4*L/As   His = As=20 is my Vp (speed of sound).  The only = thing I=20 don't understand is why his time for the pulse to travel the length = of the=20 intake pipe is equal to 4*L instead of my 1*L.  It appears as = though he=20 is making his pulse travel 4 times the length of the intake = manifold, but=20 then its is not abolutely clear what his intake pipe length really = is. It=20 may have to do with a multiple bounce of pulses.  i.e. using = every 4th=20 pulse? or perhaps because there is the "rest" stroke on a 4 stoke = cycle=20 which the rotary does not have? Just not clear to me at this point, = why the=20 4*L.

In any case, he eventually ends up = with the=20 equivalent of my parametric equation!

  I could hardly believe = it!  Solving=20 for Length of the manifold "L" in his equation

His was L =3D  = As* f* /gt4*(6*Ne)   = wereas mine was L =3D Vp*(Ad)/6*RPM (or it could be reduced to that = form)=20 where my Ad =3D f  and my=20 Vp =3D his As  The = gt=20 factor in his equation is a pulse selection factor - do you want to = tune by=20 the first pulse in which case gt =3D 1 or perhaps a = 2nd or=20 4th pulse in which case gt =3D 2,4, etc.  = Since I was=20 only concerned with the first pulse gt became 1 and = isn't a=20 factor in my equation.  But, I think it may indicate a point = that some=20 of you raised during the presentation (Finn?) that perhaps=20 there are some DIE effect at mulitples of "L" if the pulse = retains=20 sufficient energy after several trips through the=20 intake.

The only thing that I can't explain about = his=20 equation is the factor or "4" for his Time required for the pulse to = transverse the intake pipe.

So, now more than ever, I know my = orginal=20 analysis is on solid ground. The only other difference is that he = apparently=20 does not address any pulse duration effect in his = equation. =20 Perhaps this is not as critical when the pulse returns to the port = that=20 generates it?  Perhaps with the shorter L implied for the two = rotor=20 timing is more critical and the pulse duration must be accounted = for? =20

In any case,  its great to find = independent=20 confirmation for my derivations or at=20 the very least, it clearly shows that Port timing is = crucial in=20 pulse tuning or DIE as I showed, but which some = folks=20 apparently still don't believe or understand.  Just thought you = might=20 like to know that the DIE analysis is on frimer ground than just = based the=20 quality of my derivation. 

Best Regards

Ed Anderson

Ed Anderson
RV-6A N494BW Rotary=20 Powered
Matthews, NC
eanderson@carolina.rr.com
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