Subject: Turbo-compounding -update
From: ACRE
Date: 9/3/2004, 1:19 AM


Monty.

I understand your points well. Thanks for bringing them up for
everyone.
It
has occurred to me (and Paul is way ahead of me on this) that we
would
need
to compromise performance on the turbo compound side even with  a
special
oversized turbine and some sort of gearing. Logically two turbines
as
described above would be a good way to test the turbo compound
concept
limits. It would give us an idea of much power can be recovered
from the
13B. without choking the engine. I believe  a moderately boosted
turbo
charged Renesis engine should put out about 300Hp  near 7900 rpm.
55%
cruise power means 165hp. and 4345 e-shaft rpm. with a lot of
exhaust
energy
still available. If our power turbine can pick up even a paltry 10
ft./lbs
of torque at this low end range and transfer it at 90% efficiency,
that
would mean we'd have an additional 10.8 hp. I would be happy.

If we can pick up  35 ft./lbs like Paul L. suggested at 90%
transfer
efficiency we would have about 38 Hp increase in power. Paul would
be so
happy he wouldn't sleep at night:)  The heavy Renesis engine would
suddenly
be a possible choice for pilots desiring a 300hp engine that would
have
a
better BSFC than the Lycoming IO540.  We aren't re engineering the
engine
per se. I would like to think we are just mining the waste.

I would be ecstatic to find a small power axial turbine designed
to work
well in the  40 to 50K rpm range or even 10K faster. Monty if you
could
point me to a source for turbines in this range I would be
grateful. We
could get easily get a 10:1  reduction (300mmų  down to 30mmų)
with
belts
and a large pulley, or a motorcycle chain and sprocket mounted
where the
flywheel is now.  I agree with you that we would have to match
rpms and
that
can be done using a rather new but seemingly simple technology and
very
basic electronics.

Go here for details.    http://www.magnadrive.com/

The units as shown are to heavy.  We would have to  redesign the
clutch
and
perhaps arrange the magnets in a different polar configuration for
more
attraction but less slippage.  Simply explained; the mag./clutch
is
designed
to slip from 100% down to about 3% by varying the gap between the
magnets
and the copper conductor.  The input power rpms are always larger
than
the
output rpms. in its intended design applications.  However this
might
get us
into trouble or be a benefit in our application.  Have to test it.
Torque
stays the same though.

The  micro toroid CVT. is our other option for matching rpms as
well as
being a disconnect clutch, affording wider range of turbo speed
ratios
rpms., and perhaps a few other goodies. I am now designing a few
variations
of this device on paper.

This work is approaching a bench test on certain parts.  Paul is
busy
spinning gears and planning Hollywood stunt work  while I am
playing
with
colored pencils and magnets:)

Doug in Japan

Doug,

I would love to direct you to a source of turbines. Unfortunately you
are
going to have to roll your own. If you find a source I would love to
know
about it, as I need one myself. The problem (one of many) with
turbomachinery is that the components must be matched to the
application and
to each other. It is very hard (impossible) to design a set of stock
components. Radial inflow turbines seem to tolerate operation off
design
point without loosing too much efficiency. They can also be "trimmed"
to
give different characteristics using the same casting. You change the
inducer and exducer dia. and the area ratio of the scroll to get
different
behavior. Radial turbines are also more tolerant of sloppy tip
clearances.
They just have lousy stalled torque characteristics, and the
efficiency will
suffer vs. a radial or axial turbine designed specifically for the
application. Because of this "tune-ability", ability to use a series
of
stock castings, and less sensitivity to manufacturing tolerances, most
of
the small dia. high RPM turbocharger turbines are radial inflow.

 With axial turbines there are also structural problems at high rpm
and the
flow rates needed for most turbocharger applications.  Axial turbines
are
also more of a point design and there is no easy way to "trim" them
for
different applications. Axial and radial turbines, if designed
specifically
for an application are virtually identical regarding efficiency. They
work
best a different wheel speeds relative to flow and are not
interchangeable
in application. The other option is the "mixed" flow turbine which is
a
hybrid of the two designs. Having designed/developed several mixed
flow
devices, I cannot recommend this, unless you have CFD, a lot of time,
and a
lot of money. Or really, really, good luck. I'll just say this: throw
away
the text books and the equations, because they are worthless. Add to
this
mix different percentages of reaction vs. impulse and you have a
really
exciting time ahead, ummm,,,,, I mean, rewarding design experience.

The apparent contradiction in the radial turbine not loosing
efficiency as
quickly off design point and the fact that it makes a lousy power
turbine is
due to the stalled torque characteristics, not the thermodynamic eff.
While
the radial turbine will not loose thermodynamic efficiency off design
point
as rapidly, its ability to produce torque over a broad operating range
is
inferior. Perversity of nature is the accepted explanation.;-)

To address Paul's comments on radial inflow turbines. They will work
over a
very narrow operating range. Like a diesel. The Solar unit also uses a
radial inflow wheel. The PTO is directly off of the single shaft
engine. It
is confined to a very narrow operating range. This is acceptable for
an APU.
For your application I think you would be better off simplifying the
PTO
drive equipment and using an axial flow turbine. The more favorable
off-design torque characteristics should make this possible. If you
want to
go to higher shaft speeds, you will probably have to use a radial
inflow
turbine. If you do you will either have to design it for cruise only
and
just accept that it is inefficient off design or go with a variable
NGV to
broaden the range. You will also find that the manufacturers of these
turbocharger turbines hold their cards pretty close to their vest. If
you
were working with MAZDA, have a track record and are willing to sign a
lot
of paperwork, Garrett might let you see their turbine maps. Perhaps
you
would have better luck working with one of the Japanese manufacturers.
Otherwise trying to engineer a system that works well is going to be
pretty
tough without reverse engineering the components first, or designing
and
developing your own.

4345 X 10 = 43,450 This should be a workable speed for a small axial
turbine
about 6-8 inches in dia. Let me know what the mass flow rate is and
what the
TIT is. It is fairly easy to have an RP of a wax pattern made. A
vacuum melt
investment casting can be made in inconel from the pattern relatively
inexpensively. Depending on the blade profile, you might also be able
to
machine one from a billet, although machining inconel is not for the
faint
of heart. I would make it a blisk and try to avoid furnace brazing a
lot of
separate components. 90% eff is high, though possible. I would use a
100%
impulse turbine and forget about the reaction stuff. A single impulse
stage
can achieve efficiencies as high as 90%, I would plan on more like 85%
unless you want to spend a lot of time on development.

If you are going to be at Tracy's we should have some face time to
talk
about all this. I have some Ideas regarding magnets and such we should
talk
about.

Monty

PS. attached is a cutaway pic of the CF700, the engine I think Vance
was
describing.

Opss forgot to attach the gif. Here it is.

Monty, there is lots of modern design info in this book on radial inflow
turbines
used in turbo chargers.

____________________________________________________________________________
_________
For some historical background on the coming wave of electric assisted
turbochargers,
turbo compound and hybrid turbo generators for cars I recommend
Turbocharging
and Turbochargers. Published by the  I Mech E 1982 ISBN 0 85298 491 X
Much more in depth than the Hugh MacInnes book. Also some of the
original
work on the variable vane turbochargers now widely used on European
diesel
engine powered cars. Many technical papers on work done world wide.

Paul Lamar

___________________________________________________________________________

Turbine efficiencies are are above 70% from velocity ratios of .6 to .9
with a peak
at 80%. A 200 net HP rotary is wasting 200 HP in the exhaust max.
Lets say as a wild ass guess half is unrecoverable heat energy and the
other half is
gas kinetic energy that is 100 HP max in gas kinetic energy alone.

70% of that is potentially 70 HP max from your typical Mazda turbo charger
turbine over that velocity ratio range. Since we are using a CVT and can
optimize the turbo charger RPM for the available flow rate I feel
confident we can extract significant HP over the rotary engine
HP range of 55% to 75% power mentioned by Doug. Assuming of course
we can maintain these heat loss ratios.

In this first chart effective heat is net HP out.
Note the second chart is at very low net power out levels.

Paul Lamar

Daniel Gagnon wrote:

Did anybody ever think of direct drive Tesla turbine, no real restriction,
excellent heat extraction of the exhaust, light, just a tought.

Daniel Gagnon

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