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INTERCOOLERS - - ARE WONDERFUL DEVICES!

 INTERCOOLERS   - -  ARE WONDERFUL  DEVICES!

As is indicated in the previous blog on Turbochargers vs Turbonormalizers - -  intercoolers are  one of the  "secret ingredients" in the whole engineering effort  that protects  the high powered aircraft piston engine from detonation.   If you get the CHTs cooled off and you get the induction air temperature (IAT) down close to that experienced by the similar normally aspirated engine,  then you really don't threaten the engine with adverse combustion events any more than they already are with a normally aspirated engine.

The value of the intercooler is often misunderstood.  Few  pilots and mechanics  have any notion of the magnitude of  protection from detonation that is afforded by a good intercooler installation.   The data shown in the graph below helps to quantify the magnitude of protection from detonation that one obtains when good intercoolers are installed on an engine with a supercharger.  

This data in this graph is adapted from some rather excellent   WWII  era data - - all of which was originally obtained with gear driven superchargers.  But the same issues apply exactly the same way to any piston engine with a compressor - - whether it is driven from the crankshaft by a  gear  or  belt drive or whether the compressor is driven by a spinning turbine wheel sitting in the exhaust stream.   

The left hand vertical axis is in units of  horsepower.  The scale shows how much LESS horsepower is available to a detonation limited 300 Hp air cooled aircraft engine when one increases the  induction air temperature, which is shown across the bottom horizontal axis.  

In many text books and papers,  it is  common  to characterize  an engine's  margin of safety from detonation  by establishing how much additional horsepower in excess of its  rated horsepower that the engine could make - before it encounters detonation - - assuming all of the other relevant parameters are held constant.  

In this case,  we have presented the data in a slightly different manner.   This graph first establishes a reference point for a  maximum detonation free horsepower at an induction air temperature of 120 d F,  and then incrementally increases the   IAT above the  120d F  starting point.  This process establishes how much less horsepower the engine is able to make before encountering detonation as the induction air temperature is increased.    In order to have a real world example in mind,  think of this example engine as a certified engine with something like 470 cubic inches and a normal rated maximum horsepower of  260 Hp at 2700 RPM.   For our example,  we have tested this engine and found that when boosted up to 300 Hp and with the induction air temperature  measured at 120 d F,  the engine is just barely free of detonation.   This engine would have a "detonation margin" of  40 Hp (300 - 260) at  an IAT of  120 d F.

The  blue line shows the loss in detonation free horsepower for the engine operating at 2700 RPM. The red line shows the further reduction in detonation margin from the original  power that is present if the RPM is reduced to 2500 RPM. 

It is clear from the data,  that an engine that is capable of making  300 detonation free horsepower at 2700 RPM  with the induction air temperature at 120d F - - would  only be able to make about 215 to 230 Hp free of detonation if the induction air temperature is allowed to increase into the 165 to 185dF range, and the engine is operated at 2500 RPM .  This represents a loss of some 68 to 85 horsepower in the capability of the engine to operate free of detonation.  That is a loss in detonation margin of about 22 to 28% of the power of the engine.

That  22% to 28% loss in maximum detonation free horsepower  can be recovered with a good intercooler installation.

The industry,  the FAA, and the pilot community all consider it an acceptable  design configuration  for an aircraft piston engine to be able to detonate under certain power and environmental conditions.  That is why pilots are trained in engine operation and that is why we have  POH limitations that need to be followed.   Thus, if those types of engines are  inappropriately set up by the pilot with the wrong combination of  manifold pressure, RPM  & mixture, they can operate outside of  the established detonation margins.    We operate these engines with  these design constraints because it is sometimes essential in order for the aircraft to perform as they are intended.    The broad range of pilot selected operating  conditions is necessary  in order for the pilot to be able to extract the maximum horsepower from the engine during certain critical phases of flight.  

This widespread and historically successful  aircraft engine operating  paradigm  has been acceptable because the engines came with  manifold pressure, tachometer,  temperature & fuel  flow gages and the means to manipulate the values,  which, if done in accordance with the  POH, would allow the pilot to avoid engine operation in areas that would otherwise cause detonation.  

 Since harmful detonation is most likely to occur at full power during takeoff and climb.  Because,  under those conditions,  the only  "tool"  at the disposal of the pilot is the mixture control,  the FAA defines requirements for a  "margin" on the fuel  flow so that even if the fuel  flow were improperly set up by the mechanic  by some "margin"  the engine would not detonate on the unsuspecting pilot during a full power takeoff and climb.   The  certification standards  require a demonstration that the engine can be operated free of detonation with the  mixture lever positioned so that the fuel flow is as much as 12% below the specified  full power set point.

As an example,  if  one operates a stock 350 Hp  Lycoming  TIO-540J2BD (Navajo Chieftain) at full power and then foolishly brings the mixture control back to around 13 to 15% below   the   specified full rich mixture fuel flow - - then that engine is likely to begin to detonate under many environmental conditions.

On the other hand,  when operating that engine,  if one first reduces the manifold pressure by 8 to 10 inches,  then one can lean the mixture to almost any mixture and it will not detonate.   The cylinders will get hot if you lean it near peak TIT and leave it there for a while,  but it will not detonate.   

There are available  after-market  intercoolers for the Navajo Chieftain.  If they are properly installed on those engines,  then the detonation margin improves so dramatically,  that one can  "foolishly" set the mixture in that range from 13 to 15% below full rich and the chances of any detonation are dramatically reduced under almost all environmental conditions, even when the engines are operating at full power.

When we did certification testing on the TN SR 22 - -  we did that in flight.  We did that during a very hot period in June and July of  2006.  The routine daily temperatures were in excess of  100 dF.   The purpose of the testing was to  insure there were adequate margins to allow operation of the engine at full throttle with the mixture set lean of peak.  I was the PIC  for the flight tests.    

We  conducted the tests with half of the intercooler  cooling air inlet area blocked off.  At various times, we set the manifold pressure to still higher values than the  normal 29.6".  We exercised the RPM from 2700 down to much lower RPM values while maintaining  manifold pressure  well in excess of  30".    While doing that, and with the intercoolers partially blocked,  we were able to force the induction air temperature to values much higher than is possible to obtain with the intercoolers "unblocked"  and functioning normally.  

The results were fully consistent with the  predictions in the old data in the graph above:  When the induction air temperature began to rise to values in excess of  160 d F,  we were able to measure the onset of  detonation at  reduced mixture settings.

However, with the intercoolers functioning properly  we  could not force the induction air temperature above 130dF even on a hot day in a slow climb at 24,000 feet at  full power,  and detonation was never observed at any mixture setting.  

The result of the careful design  and thorough testing   - -  all born out of  a lifetime of  real world turbocharger engine operating experience  and  many years of  highly  instrumented test cell engine operation - -  has been  a robust  Cirrus "Smart Turbo"   system that is widely recognized as the  most efficient and the easiest  turbo system to operate   of any general aviation aircraft.   Ever.


Posted 13 Feb 2009 20:31 by George Braly
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Comments

Michael D. Busch wrote re: INTERCOOLERS - - ARE WONDERFUL DEVICES!
on 14 Feb 2009 21:28

George, could you post a graph that shows the relationships between OAT, CDT, and IAT as altitude varies from SL to FL250. In other words, how much temperature increase is produced by the turbocompressor and how much temperature decrease is produced by the intercooler as the aircraft climbs up to the Flight Levels?

George Braly wrote re: INTERCOOLERS - - ARE WONDERFUL DEVICES!
on 14 Feb 2009 21:59

Mike,

I can do that.  

But it is a fair amount of work to dig it out of  the files ( or model it up ).  

Can you give me a hint as to  where this is going ?  I might be able to help you with the end point easier than all the intermediate stuff ?

George

Dave Brown wrote re: INTERCOOLERS - - ARE WONDERFUL DEVICES!
on 15 Feb 2009 8:26

As a mechanial engineer flying a Cirrus I love this discourse between two smart guys.  COPA doesn't get any better than this.  I'm hanging by my thumbs waiting for the rest of this exchange.  Thanks to you both.

Brian Goldsmith wrote re: INTERCOOLERS - - ARE WONDERFUL DEVICES!
on 25 Apr 2009 8:52

George,

I'm estimating that the FAT supercharger will increase the SR22's IAT to a peak of 52F/126F when climbing to 6000 MSL from a SL airport on a ISA+30 day (45C/113F), and a peak of 45C/113F on a ISA+23 day (38C/100F).  Based on your graph, I interpret the loss of detonation-free margin to be about 28 and 15 HP, for the 113 and 100F SL temps respectively.  The fact that your graph's data was collected at 5000 MSL is fortuitous, because that elevation is very close to the FAT SC's critical altitude and hence the region of peak IAT warming.  I estimate that at peak IAT on an ISA+30 day, the SC SR22 will make 268HP WOT Best Power (86% Power).

I've based these IAT estimations on an excel model (ISA and ISA+30 SC Power and IAT Estimation_v4.xls) attached in "FAT Supercharger gets FAA approval" forum discussion.

May I ask you to review the model and comment on need for corrections or refinements?  If the model looks acceptable as a estimate of power and IAT, what would you expect to be practical implications of a loss of detonation-free margins between 15 and 28 HP?  Would an intercooler be beneficial or necessary for detonation-free flight in such conditions, or are there other engine management techniques that the pilot could exploit to stay detonation-free?

Brian

Brian Goldsmith wrote re: INTERCOOLERS - - ARE WONDERFUL DEVICES!
on 25 Apr 2009 12:09

George,

Disregard the comment above.  Reviewing your blog, I see that I initially assumed ideal (100%) compressor efficiency.  Incorporating 0.6 efficiency yields the following:

[View:www.cirruspilots.org/.../0511.ISA-and-ISA_2B00_30-SC-Power-and-IAT-Estimation_5F00_v5.xls:550:0]

The power result: on an ISA day, power drifts down from 98 to 92% as you climb from SL to 6000 feet, and then the SC engine performs like a NA flying at an altitude 3000 feet lower, with a ceiling (based on NA comparable power) of 20 to 21,000 feet.  On a very hot ISA +30 day, power drifts down from 89 to 83% as you climb from SL to 6000 feet, and then the SC engine performs like a NA flying at an altitude 3000 feet lower, with a ceiling (based on NA comparable power) of 18 to 19,000 feet.

The IAT result: on an ISA day, climbing from SL to 21,000, IAT peaks at 32C/90F at 6000 feet, decreases to 29C/84F on the way up to 16,000 feet, and then climbs again to 38C/100F at 21,000 feet.  On a very hot ISA+30 day, IAT peaks at 66C/151F at 7000 feet, decreases to 63C/145F on the way up to 14,000 feet, and then climbs again to 69C/156F at 19,000 feet.  The ISA+30 peak IAT detonation-free HP margin would decrease by 55HP (based on George's detonation-free margin vs. IAT graph).

May I ask you to review the model and comment on need for corrections or refinements?  If the model looks acceptable as a estimate of power and IAT, what would you expect to be practical implications of a loss of detonation-free margins between 55 HP?  Would an intercooler be beneficial or necessary for detonation-free flight in such conditions, or are there other engine management techniques that the pilot could exploit to stay detonation-free?

Brian

George Braly wrote re: INTERCOOLERS - - ARE WONDERFUL DEVICES!
on 25 Apr 2009 16:29

Brian,

See the  solid red line in the last graph  in my  response to Mike Busch's  question in the "Compressor IAT, CDT vs Alttiude" blog.

It depicts the performance of a  belt/gear driven compressor with a limted pressure ratio of around 1.4:1, and a compressor efficiency of around 0.60.    I think that graph is  relevant to  the numbers you are trying to generate in your spread sheet.

Your model makes the assumption that the compressor is only putting out  around ~ 30"  compressor discharge air at sea level.

For a belt/gear driven compressor that has its speed derived from the crankshaft,  that is impossible unless the inlet to the compressor is choked down.   Even then,  the compressor just continues to do its work and raise the compressor inlet ambient pressure by is rated pressure ratio (at the fixed RPM) .  That means there is,  as I understand it,  a lot more work done on the incoming airstream and therefore the  sea level standard (or hot day)  day  compressor discharge temperature will be much higher than I believe  you are using in your calculations.   If you had a variable speed compressor - -  you could arrange for the numbers to work out  to much lower  induction air temperature values as you are depicting.

Thus,  if the pressure ratio is around 1.4 at rated crankshaft speed,  then, at  sea level,  standard atmospheric pressure,  any belt/gear driven compressor is ejecting air at a compressor discharge pressure that is about ~1.4  X 29.92"  ~ =  41.9" HG.  So the heating value into that airstream is pretty large.

You might get some of that back,  when you choke down the airsupply, upstream of the throttle, with a butterfly plate controller,  but that process is also very inefficient.

This is all very different from the free shaft turbo compressor which can spin at a large variety of different RPMs, depending on the  mass  flow of air that is required.   At sea level, the typical TN  turbo compressor  discharge pressure is around 31", not 41.9" like the calculations indicate for a  belt/gear driven  compressor with a  1.4:1 pressure ratio.  

Given the routine 160dF to 175+dF temperatures that I can calculate from the thermodyamic  equations - -  the reduction in detonation margins is substantial.    

One of the ways to avoid detonation  is to require the engine to be operated at very high fuel flows while operating at higher manifold pressure settings.

I can, on the test stand,  run the induction air temperature on a normally aspirated  IO-550 at sea level up into the 160 to 170d F range and, with other parameters operating under hot day conditions,  I can, at normal fuel flows,  get it to detonate rather easily, even on 100LL that exceeds the minimum 100LL fuel octane specifications by a significant amount (ie, 104MON verses 99MON minimum spec fuel).

Let me know if I have not  answered your question,   and I will try, again.

George

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