nicklockard
Torque Dorque
Hmmm, I just intuitively thought it should show up in the pressure relationships somehow. Oh well.
If the pressure relationship is constant, yes, it would, but as has been shown, it's not.nicklockard said:Hmmm, I just intuitively thought it should show up in the pressure relationships somehow. Oh well.
Scratch that thought.TDIMeister said:Maybe taking derivatives of F_U_B's EMP and IMP pressure (after dealing with the buzziness of the data) and measuring the time deltas between a positive turbine pressure gradient and the corresponding positive compressor pressure gradient.......
Insightful analysis on precompressor fumigation, IMO.quoted from [URL="http://www.aquamist.co.uk/phpBB2/viewtopic.php?t=1364" said:http://www.aquamist.co.uk/phpBB2/viewtopic.php?t=1364[/url]]
WI on a duramax
I have spent much of the last year working through a problem with coolant overheating on GM diesel work vehicles. Since some of my findings are applicable to this effort, I will elaborate.
What I found was that the smallish compressor was working in the northeast part of the map, and in some thermal conditions, "off the page". On further investigation, the temperature of the compressure discharge emerged at near 600 F. I calculated efficiency around the 50% mark. Needless to say, this is in a word, ridiculous! Further investigation led me to question what the effect of this heatup (and expansion) is on the downstream plumbing. Something told me that I was seeing extaordinary head losses with this huge heatup. In other words, the velocity in the IC/CAC plumbing would be increasing dramatically, leading to higher frictional losses. It turned out, the difference between the compressor discharge pressure (work) and the intake plenum pressure (downstream) was nearly 6 psi! This at a plenum requirement of 32 psi. On the diesel this is around 60-65 lb/min of airflow.
Now hopefully I have not lost you. The plumbing restrictions when considering the 2.5" IC plumbing and the IC itself, totalled 6 psi. (2.5" is way too small)
After working through the compressible flow equations in a 2.5" conduit, it turns out the increased discharge temp was creating much of this loss, via increased air flow velocity. With fluid flow, there is apoint where the force required to push the fluid (air) through the straw (or IC pipe) becomes exponential, the curve quickly rising vertically at some flow rate. When this happens it is time for a diameter increase from the engineers. (what in fact happened, is that GM reduced the diameter from 3.0" in previous models, and to this day there is no known explanation why)
Adding insult to injury, that high temp product was leading to dramatic ambient temp increases behind the grill. The IC sits in front of the radiator, and measured ambient in front of the radiator, on the hot side of the IC, was 240 degrees! So the CAC was acting like a torch to heat coolant. I calculated something like 290,000 BTU/hr of heat exchange with the IC. Nuts!
But back to hot discharge product. The predictions for this non-adiabatic behavior, show that velocity increases dramatically, and adds a lot of added restriction in the plumbing. Clearly cooling the charge increases density, reduces velocity, and hence pressure losses. This means that, for a given desired intake plenum boost pressure, less work (discharge pressure) is required. This compressor now works less, which means higher efficiency. The improvement is cyclical in nature.
it appears that pre-compressor WI, PCWI, can be a performer or a deterent to performance. If you already operate in the efficient islands, on a humid day, then cooling charge can move you to lower efficiency on the left. It also leads to huge condensation effect in the IC. So PCWI would have limited usefulness on a properly designed forced induction platform with large stock amounts of charge cooling. But the undersized compressor, operating on a dry day, with excessive air box temps, should benefit big.
From my point of view, I do not share the idealized concept that WI provides quasi-isothermal compression. I believe that all the inefficiencies of non-adiabatic compression are in place even with WI. But naturally the beneficial impact of cooler charge can be seen in my explanation. But I don't believe that WI improves the efficiency of the compressor, from a purist sense. This assumes that there is no appreciable evaporation prior to compressor, as is the case in an axial mount nozzle in front of the nut.
_________________
Michael Patton (aka Killerbee)
1: Mass airflow's unit is mg per engine volume, so it's clear that at high engine rpm the VE of the engine dropts due pumping losses atc, so the cilinder filling is less complete..nicklockard said:Why are the vanes snapping shut so rapidly? I thought the whole point of VNT was fine control. Is that a consequence of his tune strictly? I mean if someone with a different tune logged data it could look dramatically different?
Questions:
- How can mass air flow be falling while he is still accelerating? Is the car just overfueling and smoking?
- Why do the vanes suddenly slam open at 4450 rpm's when he is still accelerating? Is the ECU trying to prevent an overspeed?
- Between 3300-3800 rpm, EMP>IMP. Is the turbo crossing over efficiency islands/holes?
Peak acceleration occurs at ~2400 rpm's and not at peak power which is hugely interesting in and of itself.
No, I think it will just do the opposite, because the compressor is more efficient, comp out temp will be lower, so IAT too, so air will be more dense, this means more mass flow at the same PR, this means we move to the right on the compressor map, away from the surge line..nicklockard said:Devil, or anyone:
Does pre-compressor water/methanol injection exacerbate turbo surge at low rpm?
Thank youRub87 said:No, I think it will just do the opposite, because the compressor is more efficient, comp out temp will be lower, so IAT too, so air will be more dense, this means more mass flow at the same PR, this means we move to the right on the compressor map, away from the surge line..
This is also why on a hot day, or when the intercooler is heat soaked surge will occur more frequently..
Nick - Yes, the ecu in my brain is trying to prevent overspeed by lifting my right foot . My appologies for not correcting the above graph in the other threads that it's in. The above picture has about a 2 second offset in the analog pressure measurements versus the VagLog data. This thread has all the results from the 4-5 setups that I've tested thus far and they are much more synchronous (same data, just with the time offest removed).nicklockard said:Why are the vanes snapping shut so rapidly? I thought the whole point of VNT was fine control. Is that a consequence of his tune strictly? I mean if someone with a different tune logged data it could look dramatically different?
Questions:
- How can mass air flow be falling while he is still accelerating? Is the car just overfueling and smoking?
- Why do the vanes suddenly slam open at 4450 rpm's when he is still accelerating? Is the ECU trying to prevent an overspeed?
- Between 3300-3800 rpm, EMP>IMP. Is the turbo crossing over efficiency islands/holes?
Peak acceleration occurs at ~2400 rpm's and not at peak power which is hugely interesting in and of itself.
Fix_Until_Broke said:Nick - Yes, the ecu in my brain is trying to prevent overspeed by lifting my right foot . My appologies for not correcting the above graph in the other threads that it's in. The above picture has about a 2 second offset in the analog pressure measurements versus the VagLog data. This thread has all the results from the 4-5 setups that I've tested thus far and they are much more synchronous (same data, just with the time offest removed).
Sorry for the confusion. I have some spare exhaust flanges that just need to be drilled out so I can measure post turbo pressures as well. Current setup will measure any 4 pressures, but can easily be expanded up to 16 with no problem. I have all these things that I want to do, but just not enough time to do them all .
above link said:Did you ever think about what happens in the combustion chamber when you inject water into the charge air? In addition to cooling the air, they are many other things going on. The presentation below, taken from a web site with the authors permission, I might add, describes in understandable terms what happens in the combustion chamber. Wish I was smart enough to have written it!
I wish to thank the author for letting me use his words. Every little bit of knowledge helps us to run faster without blowig any thing up and scattering car parts all over the track.
"[Reformatted slightly for readability, but otherwise as posted.]
From: Robert Harris
To: DIY_EFI@lists.diy-efi.org
Subject: Water and its effect on combustion.
Date: Mon, 10 Jul 2000 10:24:08 -0700
Message-ID: <9ptjms0uu4oe292mpk6a6vhm2hn8bu9h1j@4ax.com>
Let us take a quick look at ignition. Those who have a Heywood can look it up
- mines on loan so going by memory. The first thing that happens is a plasma
cloud is formed by the arc consisting of super heated electron stripped atoms.
When this cloud "explodes" a ball of high energy particles is shot outward.
The highest energy particles are the hydrogen atoms - and they penetrate the
charge about 5 times as far as the rest of the particles. As they lose energy
and return to normal temps - about 5000 k - they begin to react chemically
with any surrounding fuel and oxygen particles. The effectiveness of spark
ignition is directly related to the availability of free hydrogen. Molecules
containing tightly bound hydrogen such as methanol, nitromethane, and methane
are far more difficult to ignite than those with less bonds.
During combustion - water - H2O ( present and formed ) is extremely active in
the oxidation of the hydrocarbon. The predominate reaction is the following:
OH + H ==> H2O
H2O + O ==> H2O2
H2O2 ==> OH + OH
Loop to top and repeat.
The OH radical is the most effective at stripping hydrogen from the HC
molecule in most ranges of combustion temperature.
Another predominate process is the HOO radical. It is more active at lower
temperatures and is competitive with the H2O2 at higher temps.
OO + H ==> HOO
HOO + H ==> H2O2
H2O2 ==> OH + OH
This mechanism is very active at both stripping hydrogen from the HC and for
getting O2 into usable combustion reactions.
Next consider the combustion of CO. Virtually no C ==> CO2. Its a two step
process. C+O ==> CO. CO virtually drops out of early mid combustion as the O
H reactions are significantly faster and effectively compete for the available
oxygen.
Then consider that pure CO and pure O2 burns very slowly if at all. Virtually
the only mechanism to complete the oxidization ( Glassman - Combustion Third
Edition ) of CO ==> CO2 is the "water method".
CO + OH ==> CO2 + H
H + OH ==> H20
H2O + O ==> H2O2
H2O2 ==> OH + OH
goto to top and repeat.
This simple reaction accounts for 99% + of the conversion of CO to CO2. It is
important in that fully two thirds of the energy of carbon combustion is
released in the CO ==> CO2 process and that this process occurs slow and late
in the combustion of the fuel. Excess water can and does speed this
conversion - by actively entering into the conversion process thru the above
mechanism.
The peak flame temperature is determined by three factors alone - the energy
present and released, the total atomic mass, and the atomic ratio - commonly
called CHON for Carbon, Hydrogen, Oxygen, and Nitrogen. The chemical
reactions in combustion leading to peak temperature are supremely indifferent
to pressure. The temperatures and rates of normal IC combustion are
sufficient to cause most of the fuel and water present to be dissociated and
enter into the flame.
As can be seen above, water is most definitily not only not inert but is a
very active and important player in the combustion of hydrocarbon fuel.
Ricardo and others have documented that under certain conditions ( normally
supercharged ) water can replace fuel up to about 50% and develop the same
power output, or that the power output can be increased by up to 50% addition
of water. This conditions were investigated by NACA and others for piston
aircraft engines. It is important to note that these improvements came at the
upper end of the power range where sufficient fuel and air was available to
have an excess of energy that could not be converted to usable pressure in a
timely manner.
As a side note - Volvo recently released some SAE papers documenting the use
of cooled EGR to both reduce detonation and return to a stoic mixture under
boost in the 15 psi range - while maintaining approximately the same power
output. Notice - they reduced fuel and still get the same power output.
When you consider that EGR consists primarily of nitrogen, CO2, and water ( to
the tune of about two gallons formed from each gallon of water burned ), you
might draw the conclusion that it also was not "inert". They peaked their
tests at about 18% cooled EGR - which would work out to about 36% water
injection and got about the same results under similar conditions that the
early NACA research got."
Fix_Until_Broke said:I have some spare exhaust flanges that just need to be drilled out so I can measure post turbo pressures as well. Current setup will measure any 4 pressures, but can easily be expanded up to 16 with no problem. I have all these things that I want to do, but just not enough time to do them all .