Late model wide case exhausts

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Sam
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Re: Late model wide case exhausts

Postby Sam » Sat Feb 07, 2015 8:54 pm

ecurbruce wrote:Not meaning to but-in on your conversation, but...
Harvey, I read that book some 20+ years ago, and it's all you say it is!
Back then I used it's principals to tune exhaust on racing go-cart with some success. Messed with pipe lengths and megaphone tapers. These well known principals have been around for a long time, this book just gives a good explanation.

Bruce


I see calculations as a base line, a friend used to build race exhausts for a living, on one occasion we fabricated an exhaust with given/calculated lengths then tested on his dyno. The exhaust was formed using slip joints which enabled us to move lengths slightly then re-dyno checking progress as we went with gained power. We also messed with taper headers back in the very early ninety's (two stroke technology on a four stroke) which in turn gave better scavange.
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DewCatTea-Bob
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Re: Matters Concerning Power-band Exhaust-tuning

Postby DewCatTea-Bob » Sat Feb 07, 2015 11:16 pm

DCT-Bob wrote:__ Now I next present the actual math.figuring-steps normally needed to reach the ACTUAL bottom-line inch-length figure !...
_ First, I divide the 6500-RPM established figure by 2, to get 3250 ex.valve openings per minute...
Step-2 _ Then divide that 3250 by 60 to get 54.167 v.openings per-second,, which when divided into 1-second, thus converts to .01846-sec (for 1 complete 720-degree Otto-cycle).
Step-3 _ Then-next determine the number of degrees between the exhaust & intake valve opening-times, (which after choosing the std.DESMO-cam valve-timing), thus providing length-duration of 80+110 (with respect to BDC), plus half of the 'overlap' period, gives a total-result of 257-degrees ave.duration.
Step-4 _ Then-next, that result in degrees has to be divided by the 720-degrees (of the single Otto-cycle) to get the resulting fraction-factor of '.35694'.
Step-5 _ Then-next that resulted-factor must be applied against the .01846-sec (time of the 1 Otto-cycle at 6500RPM), in order to get the actual time that the sound-speed wave-fronts have to make the round-trip,, which is: .0065897-sec.
Step-6 _ Then-next, that fraction of time is actually how long the accepted speed of sound has (to make the round-trip through the ex.pipe-length),, which if "1500ft/sec"-(18000in/sec), it then travels 118.6-inches, or if rather "1700ft/sec"-(20400in/sec), then it travels 134.4-inches (for the round-trip).
Step-7 _ Lastly,, the actual tuned-pipe/exhaust-length obviously rather has to be half that 'round-trip' distance, which thus means that the exhaust-pathway needs to have a tuned-length of 59 to 67 inches long (depending on whichever the speed of sound actually is, through the ex.pipe full of hot ex.gas) !
__ So if we logically*split-up the Conti's 22-inch length in-half (* as was also done with the overlap-duration),, then the ex.header-length itself can be shorter by 11-inches, (and-so the ex.header-length should be about 52-inches +/- 4"),, thus-then allowing the full-cone of the Conti to come-into-play centered over the center of the overlap-period of the DESMO-cam !
__ This unexpected out-of-the-ballpark result -(referring-to the rather extensive 59 ~ 67 inch 'tuned-length'), leads me to suspect that there must be another factor that slows-down the speed of sound,, and so I'm now suspecting that the speed of the ex.gas-flow may significantly work against the sound-speed.
____ I've now seen that I've fallen-behind in this thread and have another new post by Harvey to respond to. _ So I'll now quite this post at this point and move-on, (and perhaps finish-up my current/leftover thoughts within another post later).
____ It's just as well that I had let Harvey's posting interrupt the continuing-on of my post (of 2-days ago), as that post was already getting too-long then anyhow.
Now to continue-forth from where I had left-off before and finish-up my leftover thoughts...
__ At 6500-RPM, a 450's piston must travel near 640-inches per second, so I figure that produces an ex.gas flow-rate of 4100in/sec. _ (I think I recall that Harvey had stated that the ex.flow-rate was limited to just 300ft/sec -[3600in/sec], but I don't see how that could be possible,, cuz even at just 6500-RPM, such a bottleneck flow-rate would then soon curtail cylinder-purging due-to exhaust-pressure constantly building-up higher & higher while trying to keep-up, [after the 450's revs surpass 5700RPM]).
So if the speed of sound -(19200in/sec [average]) is actually slowed-down by the full 4100in/sec, then that yields a resulting reduced sound-speed of 15,100in/sec. _ Which means the tuned-length* for the exhaust-pathway is near 50-inches (* for 6500RPM),, and-so if that tuned-point is placed in the center of the 22" Conti-cone, that means the ex.header-pipe would need to be near-about 39-inches long.
__ This extra-added math-figuring now brings the bottom-line result into the expected ballpark range.
So-thus it would seem that the ex.gas flow-rate must indeed be a worthy speed-factor that works against the speed of sound within the ex.pipe.


Next...
Harvey wrote:We work the length out with the formula: 180 X 1600 / 6500 = pipe length in ".
The 180 is the number of engine degrees for the sound wave to do the return run down and back to the cylinder, the 1600 is for the speed of sound in that gas temp. The 6500 is the engine rpm that we want the maximum torque to occur.

There are a few variables here, if we accept the speed of sound in the pipe to be 1600ft/sec, we then have to settle on how many degrees for the trip.
We say 180* as that is approximately the number of degrees from the exhaust valve opening, to over-lap. So if the effective exhaust timing is open at 70* BBDC and the inlet opens at 30* BTDC, it is about 180*.

____ Now next, to apply the DESMO-cam valve-timing into Harvey's presented formula...
__ The ex.valve opens 80-degrees before BDC, and the in.valve opens 110-degrees later (after BDC / ['70 BTDC']),, so that's a total duration of 190-degrees (instead of his "180" example). _ And with the '190' rather plugged-in to "the formula", 190x1600/6500 = 46.77, would indicate that the tuned-length for the exhaust-pathway ought be near 47-inches long.
____ That result seems acceptably close enough to my-own 50-inch bottom-line result, but there's actually more difference than just that 3-inch discrepancy...
__ Of-course it makes good/logical sense that Harvey's presented formula directly addresses the specific point at which the intake-valve opens, (which even just that alone, is a pretty-good point in time to have the neg.pressure-front/boost-punch reach all the way back through & in that far), since a megaphone's center-point located at the 47-inch ex.length point would then evenly spread-out the boost-punch's arrival-timing and-thus also spread the tuned-enhanced power-band equally out-over both sides of the chosen 6500-RPM rev.point (so that the otherwise narrow tuned-band then becomes widened-out [rather well beyond either side of the 6500] to end-up covering an expanded RPM.range [rather than merely-just near-about the 6500-point]).
__ However it's my understanding that the tuned/timed-arrival of the desired neg.pressure/boost-punch is not only beneficial just as the in.valve opens, but also ANY-time during the v.overlap-period.
So by tuning the exhaust-pathway length so that the neg.boost-punch is rather timed to arrive at the center-point of the overlap-period, then allows the tuned power-band to be widened equally on either side of the chosen 6500-RPM target-point.
And that's the arrival-time difference which MAY possibly account for the 3-inch -(50 vs. 47) discrepancy, (although presently, I'm sorta doubting that notion).

____ Unfortunately I've recently received phone-calls & a visitation interrupting my posting/thoughts (and-thus delaying the orderly completion of the last-half of this post),
and have since become too sleepy. _ So now I need to ponder this stuff some more
later, (to figure-out whether it's good or not to have both power-band widening efforts* concentrated [or rather only slightly overlapping]).
(* concerning that provided by the megaphone-effect, and-also that of centering within the overlap-period)


Tillater,
-Bob
PLEASE NOTE... If this-post is not-yet signed-off with '-Bob', then I'm still in the process of completing it,, and if not also included with 'DCT' near bottom as well, then I may edit this post's wording at a later time. - Dct.Bob

Harvey
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Re: Late model wide case exhausts

Postby Harvey » Sun Feb 08, 2015 3:25 am

Bob said:
So I suppose it may be fair to call that wave-front a 'sound-wave',, but I'd really think not, since areal sound-wave is much same as a 'double-edged sword', in that along with it's neg.side, must follow a pos.side, (or-else it can't really be considered as a true sound-wave !). _ And what of that-pos.side, and it's effect on exhaust-flow ??


Well if you replace "'double-edged sword", with an "AC voltage wave", you can see that the cycle starts with a rising positive sign, (at valve opening) dropping to "zero crossing" at the expansion point, changing to a rising negative sign, to reduce to "zero crossing", with the closing of the valve. A Complete wave cycle, what happens after that, does not matter as the exhaust valve has closed.

__ When I began that prior post, I had awakened from a good long nap and then found nothing on TV worthy of distracting me for the time I had presumed it would take me to work-out the math-figuring which I had before mentioned I would get-around to tackling.
But after working on step-numbers 3 thru 6 (longer than expected, [as I then had-to settle a choice of cam.model for the figuring-example]),, getting past step-7 then began to really bog-down my posting, since TV.programing starting competing for my mind's attention by that time !
__ Sorry for not being ready for your posting, (you must get-up pretty-early over on your side of the globe) !


Oh come on Bob :D ,,,,,,,you can't fool us,,,,,,,,,,the truth is that you are snowed in over there :shock: ,,,,,,,,,,,can't get out,,,,,,,,,,,,cabin fever :cry: ........ Got to talk to some body about anything. :D :D

Now to continue-forth from where I had left-off before and finish-up my leftover thoughts...
__ At 6500-RPM, a 450's piston must travel near 640-inches per second, so I figure that produces an ex.gas flow-rate of 4100in/sec. _ (I think I recall that Harvey had stated that the ex.flow-rate was limited to just 300ft/sec -[3600in/sec], but I don't see how that could be possible,, cuz even at just 6500-RPM, such a bottleneck flow-rate would then soon curtail cylinder-purging due-to exhaust-pressure constantly building-up higher & higher while trying to keep-up, [after the 450's revs surpass 5700RPM]).
So if the speed of sound -(19200in/sec [average]) is actually slowed-down by the full 4100in/sec, then that yields a resulting reduced sound-speed of 15,100in/sec. _ Which means the tuned-length* for the exhaust-pathway is near 50-inches (* for 6500RPM),, and-so if that tuned-point is placed in the center of the 22" Conti-cone, that means the ex.header-pipe would need to be near-about 39-inches long.
__ This extra-added math-figuring now brings the bottom-line result into the expected ballpark range.
So-thus it would seem that the ex.gas flow-rate must indeed be a worthy speed-factor that works against the speed of sound within the ex.pipe.


I can see you love to do the maths, but you are assuming too much, and using factors that don't count. What has the piston speed got to do with the speed of the gas pressure front? The gas expansion rate is not dependant on the piston speed, they are two different events.
Harvey.

Harvey
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Re: Late model wide case exhausts

Postby Harvey » Sun Feb 08, 2015 3:26 am

ecurbruce wrote:Not meaning to but-in on your conversation, but...
Harvey, I read that book some 20+ years ago, and it's all you say it is!
Back then I used it's principals to tune exhaust on racing go-cart with some success. Messed with pipe lengths and megaphone tapers. These well known principals have been around for a long time, this book just gives a good explanation.

Bruce


Thanks Bruce another "true believer ". :) My copy is 1962, right as we were trying to get 15hp out of a 125 BSA Bantam !
Wow, were our eyes opened.
Harvey.

DewCatTea-Bob
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Re: Late model wide case exhausts

Postby DewCatTea-Bob » Sun Feb 08, 2015 6:56 am

[quote= Harvey ...
" Well if you replace "'double-edged sword", with an "AC voltage wave", you can see that the cycle starts with a rising positive sign, (at valve opening) dropping to "zero crossing" at the expansion point, changing to a rising negative sign, to reduce to "zero crossing", with the closing of the valve. A Complete wave cycle, "

____ If that explanation is actually applicable, then it's a concept to be taken into consideration.
However the likening of it to an AC.wave ought really be rather more-so as a 'square-wave' (which wouldn't be so natural sounding).



DCT-B wrote: (I think I recall that Harvey had stated that the ex.flow-rate was limited to just 300ft/sec -[3600in/sec],

" What has the piston speed got to do with the speed of the gas pressure front? The gas expansion rate is not dependant on the piston speed, they are two different events. "

____ Alright then, it seems I was mistaking about exactly what you were actually specifically referring-to that had the 300ft/sec speed-limit. _ (I should've gone-back & reread all your associated wording once-again, before trusting what I thought I recalled !)
I now gather that you were actually referring-to the ex.gas 'expansion-rate' (which becomes allowed once the ex.valve opens).
__ However, I thought my post-wording was fairly clear that I was rather in reference to the speed of the ex.gas being EXPELLED from out-of the cylinder, (instead of it's 'expansion-rate').
So to answer your question, piston-speed probably has very-little to do with the rate that the ex.gas 'expands' and moves out forth-ward, (but it's rate of forward speed has-to be enhanced at-least a little, compared to expanding-out from a cylinder with a stopped piston).
__ Now I have to think of how this overlooked 'expansion-rate' may effect the speed of sound within the ex.pipe.
I'm now wondering what percentage of it's maximum 3600in/sec speed might ought-to be added to the speed of the piston-expelled ex.gas !? _ (Perhaps just enough to pretty-much exactly make-up for the 3-inch discrepancy ?)
Opinions anyone ?
( It was so much easier to calculate the bottom-line result by just plugging-in the accepted standard speed-of-sound -(13500in/sec) into the math-figuring ! - [Then maybe Harvey's "41.5" would finally become confirmed ?] )
UPDATE: I've since gone-ahead & plugged-in/substituted the rather commonly-known speed-of-sound -(1126ft/sec) into the math-figuring (as in 'Step-6')...
And while the result actually didn't end-up confirming Harvey's original "41.5" figure, it did however pretty-much match the same result as his presented formula came-up with ! ...
Harvey's formula: "180x1600/6500" results with 44.3-inches,, while the actual math-figuring with the regular speed-of-sound, results with 44.5-inches !
Now what's-up with that ?
Harvey's mysterious "formula" leaves me doubting that those matching results are no coincidence. _ But are they actually indeed so, Harvey ?




____ Also, still left wondering how you account for the discrepancy between your originally stated "41.5" and the 44.3-inch results from your presented formula ?


Disenchanted-Cheers,
DCT-Bob
PLEASE NOTE... If this-post is not-yet signed-off with '-Bob', then I'm still in the process of completing it,, and if not also included with 'DCT' near bottom as well, then I may edit this post's wording at a later time. - Dct.Bob

machten
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Re: Late model wide case exhausts

Postby machten » Sun Feb 08, 2015 10:47 am

Apologies for stepping out of this thread for nearly a week. I've had the combination of some work issues to deal with, and more significantly, it was my 25th wedding anniversary last week (or more importantly, it was my wife's 25th wedding anniversary last week ;) ) and my better half had other plans for me and motorcycle activities were banned! (well, perhaps not "banned", but the consequences of spending too much time on it didn't bear consideration). I have managed a few illicit peeks, but that's all. Give me a few days to digest what's here.

Kev

machten
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Re: Late model wide case exhausts

Postby machten » Tue Feb 10, 2015 1:18 pm

I've ordered the book, Harvey.

Bob, I'll keep my powder dry on calcs for the moment. I will say this this however...

    I've seen and played with some simple internet exhaust length calculators
    I've looked at your own maths

I don't think the physics are anywhere near so perfect a model. IMHO There's a good reason people argue about this. There are a lot of variables and it isn't simple. What seems to me to compound this is the language people use to describe it.

I need to read some more to understand it. I'll need some time and at the end of that time, I still may not understand it...but at least I think I'll know by then the right questions to ask.

Kev

Harvey
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Re: Late model wide case exhausts

Postby Harvey » Tue Feb 10, 2015 10:29 pm

Bob wrote;
UPDATE: I've since gone-ahead & plugged-in/substituted the rather commonly-known speed-of-sound -(1126ft/sec) into the math-figuring (as in 'Step-6')...
And while the result actually didn't end-up confirming Harvey's original "41.5" figure, it did however pretty-much match the same result as his presented formula came-up with ! ...
Harvey's formula: "180x1600/6500" results with 44.3-inches,, while the actual math-figuring with the regular speed-of-sound, results with 44.5-inches !
Now what's-up with that ?
Harvey's mysterious "formula" leaves me doubting that those matching results are no coincidence. _ But are they actually indeed so, Harvey ?



____ Also, still left wondering how you account for the discrepancy between your originally stated "41.5" and the 44.3-inch results from your presented formula ?


Disenchanted-Cheers,
DCT-Bob


I can clear that up Bob, I have used the lower road bike sound speed, of 1500 ft/sec. My blue, not paying attention. :oops:
Harvey.

DewCatTea-Bob
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Matters Concerning Power-band Exhaust-tuning

Postby DewCatTea-Bob » Wed Feb 11, 2015 8:18 am

[quote= machten ...
" Bob, I'll keep my powder dry on calcs for the moment. I will say this this however...
I've seen and played with some simple internet exhaust length calculators "

____ It would've been of interest if you had provided links to any of those which you found to be possibly worthy of further examination by the rest of us.
__ Did you compare any of their answers using the sample*example that Harvey chose (and which I've maintained as the accepted working-example -[* DESMO-cam @ 6500RPM]) ? _ As it would be of interest to learn if any of their result-answers matched closely or not !



" I've looked at your own maths "

____ I assume that since you haven't pointed-out any math-errors, that you must not have found any ?
Anyhow, it doesn't really matter if you-yourself bothered to check that all my math was actually correct,, as I know it's all without errors, (just as anyone-else with a calculator could realize) ! _ It's just that those who don't have a clue,, could've been more assured, with the likes of yourself confirming that the math is all good.




" I don't think the physics are anywhere near so perfect a model. "

____ There's actually no legitimate arguing with the perfection of the actual math-logic ! _ However I do believe you're quite correct to imply that all the involved physics seem too complex to pin-down to the degree of perfection that yields result-answers within fractions of an inch (or perhaps even within a half-foot, with much certainty) !
__ What actually makes it next to impossible for the math-result to reach the actual factual bottom-line answer,, is that the speed of sound within the ex.pipe, just can't seem to be pinned-down to a good/solid known to be absolutely true degree.
And whatever that actual sound-speed boils-down to,, it's so very fast, that in any case,
no matter how tight it's tolerance-range is fairly kept limited down-to,, it's varied result range is just-simply too great (to trust the bottom-line result [in inch-increments*] as being near perfect enough) !
(Meaning that while we might be able to trust result-figures in 'yard' or 'meter' increments, inch-increments however imply an accuracy that's really not trustworthy, [for bike-exhausts with their limited pipe-lengths].)



Harvey wrote:I can clear that up Bob, I have used the lower road bike sound speed, of 1500 ft/sec.
____ That's a perfect answer, Harvey !
Instead of you seemingly having not used your-own presented formula (for attaining your posted "41.5" result), you actually rather had simply plugged-in a lower sound-speed into that formula.
(I had just assumed that you'd stuck-with the same '1600' ft/sec sound-speed that you had seemed to've settled-on.)



____ I've been fairly suspicious of that seemingly oversimplified formula (that Harvey has presented), but I've recently since found that it's end-result has provided the same result/answer as that achieved with the long/drawn-out math-figuring...
Just as plugging-in the '190' duration (of the DESMO-cam's 80+110 degrees) into that formula yielded 46.76+ inches,, the long-math method I perform, also resulted with '46.76+', just as-well (when I did the math-figuring with merely just the 190-degree duration) !
__ However I still find there to be an issue with the directions for exactly what valve-timing numbers should be entered into that formula (to figure the desired length of ex.pipe for a particular RPM.range)...
__ By only entering merely-just the number of degrees existing between the opening of the ex.valve & the opening of the in.valve, (such as the 190-degrees of the DESMO-cam), the neg.sound-wave will arrive back at the intake-valve just as it's begun opening, (which is the good intention of the formula).
However the chosen RPM entered into the formula will then tend to be misleading because...
For instance, with '6500' desired as the target-RPM to prefer max.torque to center-peak at,, the 'result' of the-formula will rather be off-target (to the lower-edge of the actual enhanced power-band's beginning-point [that starts immediately above 6500]) !
That's because at any lower RPM than 6500, the neg.sound-wave will then return too-soon before the in.valve opens (and then not able to fully perform it's useful effect [anywhere below the 6500-point]). _ And-also (with that raw formula), the v.overlap-range will only allow the power-band to be enhanced just within the RPM.range directly above the target-RPM only !
So in the example-case of a DESMO-cam & 6500-RPM, the enhanced RPM.range will BEGIN at 6500 and extend to 11,100-RPM* (due-to the D.cam's 135-degree overlap-period), rather than center-around the 6500-RPM !
(* As by 11100RPM, the ex.valve will then be closed by the time the neg.sound-wave returns [from the tuned-end of the ex.pipe].)
__ So if anyone expects to use that formula to rather find the 'bull's-eye' of the target-RPM power-band, (instead of simply the RPM.point at which it merely begins),, then ya have-to include half of the v.overlap-degrees in addition to the duration between the valve-openings ! _ In that way, the entered RPM will then be rather centered within the targeted enhanced power-band range. _ And-so with the chosen (DESMO-cam) example-case of picking 6500-RPM as the preferred center-point for the enhanced power-band,
the 6500-point will then be centered within the 4600-RPM power-bandwidth (with a 2300 rev.range left on both sides, [instead of all 4600 left only above the 6500-point]).


Enlightening-Cheers,
DCT-Bob
PLEASE NOTE... If this-post is not-yet signed-off with '-Bob', then I'm still in the process of completing it,, and if not also included with 'DCT' near bottom as well, then I may edit this post's wording at a later time. - Dct.Bob

Ventodue
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Re: Late model wide case exhausts

Postby Ventodue » Tue May 10, 2016 5:15 pm

machten wrote:As I understand it, Sil Motor produced two structural versions of the later Silentium long silencer. The first one was a two piece tube consisting of the primary baffle and a separate slice encapsulating a secondary baffle, joined together with the use of a ring clamp. You can see that here in this Ducati brochure for a front drum brake Desmo :

Image.

I am uncertain of the IGM (Ispettorato Generale Motorizzazione) number on these as I don’t have one. Later, Sil Motor produced for Ducati a slightly different construction silencer which was one piece although still with a separate primary and secondary baffle. See below my 74 450 Mark 3 which is labelled “Moto Ducati I.G.M 1984 S”. <snip>


I'm reviving this thread (... and returning to Kevin's original question :D ), because I found this while having a clear-out today:

Image

Working solely from the IGM number, "1984/R" (see the photo insert), I hazard this could be the early, 2-piece, silencer mentioned by Kevin.

P.s And if anyone wants it, please let me know! Otherwise it will shortly be going on ebay :) ! Please note, I don't have the ring clamp.

Craig


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