Ed Anderson told me he will make a presentation on intake manifold
design using this theory at the up coming Shady Bend Rotary engine
powered airplane fly in on October 24th, 25th and 26th.
It appears at this time major improvements in intake
manifold tuning MIGHT be possible using this theory.
One of the best internet references I have found so far
is this one.
http://www.ae.gatech.edu/~comblab5/Publications/RobEJASAApril2003.pdf
There may be other good ones. If you find a better one please let me
know.
Read up on the theory so you can ask Ed intelligent questions.
I am sure Ed will jump on here and fill us in some more
before Shady Bend.
Paul Lamar
Thanks Paul, (I think {:>))
Finite-Amplitude-Waves (FAW) are indeed at the heart of the
Dynamic
Intake Effect (DIE) or "Dynamic Supercharging" as the Mazda Marketers
often
refereed to it. Found on the NA 13Bs from around 1884 through at
least 1992
or so. Fortunately, to understand the DIE effect which makes use of
the
characteristic features of a FAW, you do NOT have to understand the
higher
theoretical basis of FAW. Original solutions of FAW reactions in a
tube/duct involved Hyperbolic Partial Differential Equations (which
are just
about analytically impossible to solve for real world applications)
which
only became solvable with Numerical Techniques (the digital computer).
Now
you may feel comfortable with Hyperbolic Partial Differential
Equations, but
they are pretty tough animals and I, for one, intend to avoid them.
No,
you won't have to bring your computer either {:>).
So, certainly read all that you are interested in reading about FAW -
BUT,
if you come expecting anything close to the study done in Paul's
reference
above - YOU WILL be disappointed {:>}. The highest math that you will
need
to understand what I am going to present is high school algebra. Even
that
is probably not absolutely necessary - but it makes it a bit easier.
Paul makes a good point, the DIE will not make a "silk purse out of a
sow's
ear". If you don't have a basically good induction/exhaust system to
start
with then DIE won't pull the fat out of the fire. The Mazda engineer's
spent
a lot of time getting a good basic induction system developed to
provide the
characteristics they desired. Available information I have (mostly
provided by sources from Paul, thanks, Paul) indicates that somewhere
around
a 15% increase is probably the maximum obtainable. My own calculations
also
indicate that 15% approximate power increase over that produced by a
good
induction system.
For those of you pursuing "Forced Induction" designs this information
will
be of limited interest. For those of you which hope to eke out every
last
HP residing in the NA rotary, this will probably get your attention.
Right
now the Analysis only addresses the two rotor engine - sorry you 20B
guys.
I do have some initial thoughts on DIE and the three rotor, but they
require
some more investigation.
The main focus of my presentation is to show the derivation of the
significant variables that affect the DIE operating points and their
interrelationships (via some simple algebraic equations). Some of it
will
come as no surprise to many of you, but I think other areas will be
eye
opening. The bottom line is that I have used parametric equations
derived
from my analysis to show the relationship between manifold length and
these
other variables of the DIE and have produced graphs of these
parametric
curves and compared the results with what little specific we have from
Mazda
on the DIE. So you will be able to judge the validity of the analysis
for
yourself.
So ED's DIE presentation (as contrasted with something Mazda might own
up to
{:>)) will consist of three parts:
A very short lead-in on what got me started down this path
I. A short overview of the DIE as implemented by Mazda to bring
everyone up
to a minimum level of understanding of the DIE system
II. The analysis and derivation of the variables and equations that
govern
the DIE (this is where the algebra comes in)
III. The comparison of the results of these equations with what we
know from
Mazda about DIE
The presentation consists of approx 65 slides at this point, so bring
your
pillow - this may be the most relaxing time you'll have at Shady Bend.
For those of you who can not make the Shady Bend flyin. This
information
will be make available to you (assuming that I survive the tomatoes
{:>))
after Shady Bend. If Paul becomes convinced (yet to be determined)
that the
results are meaningful - who knows, they might even show up on his Web
page.
If they do not then, you will have Paul's de facto assessment of my
Analysis
{:>)
That is all that will be revealed before Shady Bend - thanks for the
announcement, Paul.
Best Regards
Ed Anderson
Ed sent two other web sites that are somewhat more geared towards laymen
but IMHO do not adequately make the connection between organ pipe theory
and Finite
Amplitude Waves. They do mention FAW however. Also IMHO some of their
command of fluid dynamics knowledge is questionable. So I would take this
one with a grain of salt.
http://www.racetech.com.au/faqinertia.htm
This second web site appears to be an organ pipe simulation. They want to
charge
a bunch of money for it. No mention of Finite Amplitude Waves is made on
the main
page.
http://www.dynomation.com/
At Seven Stock I bought a book called RX8 by J.Yamaguchi & J.Dinkel ISBN
4-947659-02-5
Published by Mazda Motor Corp.
This is a quasi technical book covering in detail some of the intake
manifold
design of the RX8. No mention is made of Finite Amplitude Waves or FAW and
the
Mazda PR department is found of using catchy acronyms when ever possible.
There is no evidence that Mazda ever used this principle in any of the
intake systems Mazda ever built. That is not to say it is not happening
and I think that is what Ed is out to prove.
As I understand it now Finite Amplitude Wave effects occur with precise
changes in runner cross sectional areas such as a trumpet shape or
a bellows shaped duct.
Paul Lamar
Yes, some very interesting things happens when the FAW meets a discontinuity
and those things depend on the type of change in discontinuity such as
increasing/decreasing cross sections, bell shape cross-sections, stepped
cross-sections, etc. Also what happens depends not only on the type of
change, but the degree of change. Interesting phenomona without doubt.
You may be correct about Mazda, Paul. I have seen no direct reference to
Finite-Amplitude-Waves in any of the papers. The theory has apparently been
around for decades. The FAW theory is not needed to explain DEI (although
knowledge that the wave of energy is converted to dynamic pressure when it
terminates at the intake port is crucial - but that can be empirically
measured as Mazda apparently did, showing the intake pressure increase in
Fig 5.0 of the SAE paper due to the FAW pulse of energy)
Want to make one thing clear. My presentation is NOT about FAW - its about
DEI. Although I do briefly mention it to explain a couple of its
characteristics that are germane to DEI. I think 2-3 slides out of the 65
mention FAW. The presentation is about DEI and the variables involved and
their relationships (equations) of which FAW is only one factor - a crucial
one in that without the FAW effect there would be no DEI, but again only one
factor.
In fact, the only two things I can think of real importance regarding FAW
and understanding DEI is that the energy wave travels at the Speed of sound
in the manifold and that it generates high pressures at its termination end
(near the intake port). So if you consider those two characteristics
adequately explained by other theories and can accept it without the need of
FAW theory, then you don't need FAW to explain DEI at all.
So not out to prove anything about FAW and DEI, just to present the results
of my analysis - which of course, anyone is free and welcome to form their
own conclusions about.
From my initial analysis, it appears that if you want understand how the
Dynamic Chamber functions to broaden the DEI torque curve, then there are
several other characteristics of FAW that are germane to the Dynamic Chamber
operation. But as the Dynamic Chamber is not required for DEI that is not
part of the DEI presentation. I assume the function of the Dynamic Chamber
can possibly be explained by other theories - don't know, have tried a
couple and just haven't gotten far with them. But, the FAW predicted
reaction to the Dynamic chamber appears pretty straight forward as far as I
can see and does provide an explanation for how the chamber broadens the
Torque curve.
Since I don't have anymore on the simulation than what you see on the 2nd
web page and what is in the book I have, I can't comment. But, the
simulation is generally described in the book and the book claims it is
based on FAW. However, I'm not going to spend $600 to find out, nor do I
have any stock in the company{:>)
Again, the focus of the presentation is DEI not FAW. Anyhow, I am off now.
Won't be back online until Sunday or Monday.
Best Regards
Ed Anderson
A slug of air moving down a tube suddenly encountering a closed intake port will
increase in pressure due to just plain old inertia effects. It is like a ballon filled
with air and will bounce like a ballon. As the slug of air travels
back along the tube a drop in pressure will occur behind the slug. Particularly
if it encounters an increase in tube cross sectional area such as a sudden
opening. Nature abhors a vacuum so air rushes in to fill the vacuum in
the tube starting another slug of air flowing down the tube.
The same effect will occur if the slug encounters a T a Y or a branch
in the pipe.
This happens as long as the port remains closed. If the port opens just as
the new slug arrives the engine will benefit from the increased air
density of the new slug. It will draw that air in and then some causing
the start of a new slug at the other end of the tube. Generally speaking
the slug travels at the speed of sound.
A slug of air is high pressure and high density by definition. Air molecules
are always moving around locally. They move faster and run in to each other
and the container walls more often when the pressure is increased. This is
because there are more air molecules in a smaller space.
This is called the Kinetic Molecular Model Of An Ideal Gas.
KMMOIF for short :)
An analogy is the dynamic pressure phenomena. As you move a flat plate
perpendicular to the air stream pressure is built up on the plate.
This we recognize as the aerodynamic drag phenomena.
Now if the tube is of a non uniform cross section like a trumpet
not only is the inertia of the air increasing the density and pressure
but the decreasing cross sectional area of the tube is also tending to increase
the pressure and density. This I think is the main Finite Amplitude Wave effect.
The question remains. Will the engine really get more air?
I also want to point out there are no dynamic chambers in the 3rd gen
and RX8 intake systems. Just T's, Y's or branches in the runners.
BTW Back in the days when I studied Physics our text books were not
well illustrated compared to today's standards. 3D computer programs
have gone a long way towards making physical phenomena much
easier to visualize. I highly recommend University Physics
by Hugh D. Young. ISBN 0-201-52981-5
Paul Lamar
The AirCraft Rotary Engine NewsLetter. Powered by Linux.
ACRE NL web site. http://home.earthlink.net/~rotaryeng/
Copyright 1998-2003 All world wide rights reserved.