X-Virus-Scanned: clean according to Sophos on Logan.com Return-Path: Received: from ispmxmta09-srv.alltel.net ([166.102.165.170] verified) by logan.com (CommuniGate Pro SMTP 5.0.8) with ESMTP id 1032899 for flyrotary@lancaironline.net; Mon, 13 Mar 2006 18:42:09 -0500 Received-SPF: pass receiver=logan.com; client-ip=166.102.165.170; envelope-from=montyr2157@alltel.net Received: from Thorstwin ([166.102.185.184]) by ispmxmta09-srv.alltel.net with SMTP id <20060313234114.JFXG16513.ispmxmta09-srv.alltel.net@Thorstwin> for ; Mon, 13 Mar 2006 17:41:14 -0600 Message-ID: <000901c646f7$a1d11b20$01fea8c0@Thorstwin> From: "M Roberts" To: Subject: NACA cooling additional thoughts Date: Mon, 13 Mar 2006 17:41:20 -0600 MIME-Version: 1.0 Content-Type: multipart/related; type="multipart/alternative"; boundary="----=_NextPart_000_0005_01C646C5.56F8B7C0" X-Priority: 3 X-MSMail-Priority: Normal X-Mailer: Microsoft Outlook Express 6.00.2900.2180 X-MimeOLE: Produced By Microsoft MimeOLE V6.00.2900.2180 This is a multi-part message in MIME format. ------=_NextPart_000_0005_01C646C5.56F8B7C0 Content-Type: multipart/alternative; boundary="----=_NextPart_001_0006_01C646C5.56F8B7C0" ------=_NextPart_001_0006_01C646C5.56F8B7C0 Content-Type: text/plain; charset="iso-8859-1" Content-Transfer-Encoding: quoted-printable Just some more napalm for the bonfire: Ever stop to think about the real cause of cooling drag? It seems that = there is this bedrock truth out there with all these superfluous = arguments swirling about all around it in a cloud of incomprehensible = gibberish.=20 Whenever encountering such conundrums it is best to start over from = scratch and think things through. The bottom line is making pressure costs you drag. I think there was a = guy named Bernoulli who had something to say about this. He has a fairly = famous equation that is good to know. I says basically :No matter what = type of catchers mitt you hang out into the stream of baseballs in order = to catch a few, you are going to feel it.=20 Don't let the con artists tell you that external diffusion is the holy = grail. Don't believe me? Try this experiment: Drive down the road at 100 = mph and place your palm flat to the onslaught. Do you feel anything? = Yes!- external diffusion.=20 Now place your hand at a knife edge into the wind. Is there a = difference? Coolers, be they cooling fins around a cylinder or cooling fins in a = radiator require some amount of pressure to get the baseballs through = the sieve. The amount of pressure for a given flow of baseballs is the = key. If you inhale a lot of baseballs at a low pressure (Mack truck = radiator) or a few baseballs at a high pressure (thick rad) you = have....drumroll please......DRAG!!! TA--DA!! Now some would argue that you close the outlet and let the baseballs = stack up until you are pushing this pile of baseballs, so that baseballs = are bouncing off the pile and going around the outside, totally screwing = up the baseball flow. Remember the hand! Does this sound like the route to low drag Nirvana? This all sounds very simple until some smarty pants thermo guy comes = along and starts yakking about the P-51 and all the thrust they made = with their special catchers mitt and gets everybody all hot and = bothered. The keyboards begin to click away as arm chair aerodynamicists = the world over imagine infinite speed from a lawnmower engine in their = very own laminar light plane. flying at 250 mph on a teaspoon-full of = gasoline per hour. Talk of exotic devices like augmentation tubes and = flush inlets are flung about with reckless abandon. (I have my own = theories about why male pilots are ever fascinated by these devices ;-). So how does this work?? The theory is: If I can throw the baseballs away = faster than I catch them, I can make thrust! Even better, If I can keep = all the energy I get when I catch it and put it back in I won't have to = throw so hard. Imagine I catch it and let my arm fly around in a circle = and let it go in the opposite direction. EUREKA! I can just snatch = baseballs out of the air and throw them away and propel my self about = the room! So lets say I have this really slick design and I want to use this = principle to go really fast. Lets say I have an airplane which will do = 200 mph on 100hp. There are a few that can so this is within the realm = of possibility.=20 Now the P51 went closer to 400 mph so lets say this is how fast we want = to go to keep the math simple.=20 The energy in the baseballs we are catching is proportional to the = square of the speed V^2. This means the baseballs the P-51 is catching = have 4 times the energy of the baseballs I am catching at 200.=20 Which is a lot. But it gets worse. To go 400 mph I would need more = power. How much? Power increases with the CUBE! So I will need 2^3 or = 2*2*2=3D8 or 800 hp! This means I have 4 times the energy and 8 times = the heat rejection to work with by simply doubling the speed. So = something that is significant at 400 mph is decimal dust below 200mph. = We just don't have energetic enough baseballs or a big enough arm to = help ourselves out here.=20 So how does this help us. We have now eliminated 50% of the cloud of = incomprehensible gibberish. You are not going to make a jet engine from = your piston single no matter how hard you try. There is still some confusion about the catchers mitt however that = results in much argument.=20 Some want the catchers mitt hung right out in the flow of baseballs, = some want it cleverly hidden so the baseballs just roll into it. One = group says that only real men fly with their catchers mitt in the air = the others are just out to lunch.=20 Remember the hand! Making pressure cost you no matter how you do it. The ideal inlet, = whether flush or conventional, will be sized to catch just the right = amount of air with a diffuser to build the pressure AFTER the inlet. = There is NO external diffusion. The problem is the ideal inlet is only = ideal for 1 flight condition. Change the temperature, pressure, = altitude, speed, or engine operating point and it is now less than = ideal.=20 Most airplanes have a flight envelope, not a flight point. It turns out that you need a bigger inlet for climb, because you are = going slow and making a lot of power. Then you get to altitude and speed = up and make less power. The ideal inlet changes. The typical way to deal = with this is to size for climb with an open cowl flap. Then close the = flap and tolerate some mild external diffusion in cruise. This works = regardless of the inlet type.=20 Either inlet will make more pressure at lower inlet velocity ratios. = Vi/Vo is how much slower the air going in the inlet is vs. how fast the = airplane is flying. So if I am flying at 100 mph and my velocity ratio = is .8 then the air through my inlet is doing 80mph. Now not all = airplanes have a convenient place to put a pitot inlet and this = necessitates a scoop type inlet. the scoop has a lot of drag because it = messes up the airflow all around and behind it plus it adds a lot of = wetted area in order to properly fair it. If you decrease the inlet = velocity ratio so that you start getting a lot of external diffusion, = and you do this on a laminar wing or cowl, you really make a mess.=20 The following graphs may be found in NACA RM A7I30 The problem with the flush inlet is that it makes up 85% of the free = stream pressure at around .2-.6 inlet velocity ratios.=20 FIG 18 Now this is pressure before the diffuser. When they placed a long = diffuser on the inlet they got more losses at the higher inlet velocity = ratios. This is easily attributable to mixing losses. There is some low = hanging fruit here if you use one of the shorter diffuser types. Now look at the drag FIG 25 =20 At an inlet velocity ratio of .8 the drag is ZERO!! And I can make at = least 75% of the free stream pressure with the proper inlet size. Now at = reasonable altitudes and cruise speeds that means 75% of around 8 in of = water. So I can make around 5 in water at 200 mph with no inlet drag. = Now I am still catching baseballs and they are still scrubbing along the = ductwork and it is still making drag, I am just not disturbing the = external flow or making a mess around the inlet. You can do this with a = pitot or scoop inlet as well, and you will get a higher pressure = recovery with a well designed diffuser, but you have to hang your mitt = out in the air and disturb all those other baseballs. Now to size this for cruise, it will be woefully small for full power = climb. You will have to figure out a way to deal with that to make this = work. If you size it for climb you will be able to make more pressure at = cruise, but your inlet velocity ratio will go down and your drag will go = up, just like it would with a scoop or pitot inlet. If you use an = augmenter to increase your inlet velocity ratio above 1 you may even get = some THRUST! or negative drag from the inlet! Now you still caught the = baseball and it is still scrubbing along the duct work so you probably = will not make thrust overall, but you will definitely make less drag! = Now this is not only true of the flush inlet, but is also true of the = pitot or scoop. You will have less pressure recovery with the flush = inlet the higher the inlet velocity ratio IF YOU USE A LONG DIFFUSER! = Note, that is where the loss occurs, in the diffuser. This is due to = mixing. If you use a shorter diffuser and use the turbulence to your = advantage you may get better results.=20 Now if you can tell me where on a typical single engine airplane you can = place a pitot type inlet with a proper diffuser leading to a vertical = radiator and then have a perfect exit duct without making a mess on the = wing or the front of the airplane, I would agree that it would be the = ideal setup. The only place I can think of to do this is on a twin = engine pusher. Then you might be able to put the Ideal setup to work. = Otherwise it is all a compromise dependent on what you want the airplane = to do. So there is no free lunch. But you can make a NACA flush inlet work and = you can even do it without VGs, protruding lips or other Band-Aids. Your mileage may vary. Monty =20 ------=_NextPart_001_0006_01C646C5.56F8B7C0 Content-Type: text/html; charset="iso-8859-1" Content-Transfer-Encoding: quoted-printable
Just some more napalm for the = bonfire:
 
Ever stop to think about the real = cause of=20 cooling drag? It seems that there is this bedrock truth out = there with=20 all these superfluous arguments swirling about all around it in a cloud = of=20 incomprehensible gibberish.
 
Whenever encountering such conundrums = it is best to=20 start over from scratch and think things through.
 
The bottom line is making pressure = costs you=20 drag. I think there was a guy named Bernoulli who had something to = say=20 about this. He has a fairly famous equation that is good to know. I says = basically :No matter what type of catchers mitt you hang out into the = stream of=20 baseballs in order to catch a few, you are going to feel it. =
 
Don't let the con artists tell you that = external=20 diffusion is the holy grail. Don't believe me? Try this experiment: = Drive down=20 the road at 100 mph and place your palm flat to the onslaught. Do you = feel=20 anything? Yes!- external diffusion.
 
Now place your hand at a knife edge = into the=20 wind. Is there a difference?
 
Coolers, be they cooling fins = around a=20 cylinder or cooling fins in a radiator require some amount of pressure = to get=20 the baseballs through the sieve. The amount of pressure for a given flow = of=20 baseballs is the key. If you inhale a lot of baseballs at a low pressure = (Mack=20 truck radiator) or a few baseballs at a high pressure (thick rad) you=20 have....drumroll please......DRAG!!! TA--DA!!
 
Now some would argue that you close the = outlet and=20 let the baseballs stack up until you are pushing this pile of baseballs, = so that=20 baseballs are bouncing off the pile and going around the outside, = totally=20 screwing up the baseball flow. Remember the hand!
 
Does this sound like the route to low = drag=20 Nirvana?
 
This all sounds very simple until some = smarty pants=20 thermo guy comes along and starts yakking about the P-51 and all the = thrust they=20 made with their special catchers mitt and gets everybody all hot and = bothered.=20 The keyboards begin to click away as arm chair aerodynamicists the world = over=20 imagine infinite speed from a lawnmower engine in their very own laminar = light=20 plane. flying at 250 mph on a teaspoon-full of gasoline per hour. Talk = of exotic=20 devices like augmentation tubes and flush inlets are flung = about with=20 reckless abandon. (I have my own theories about why male = pilots are=20 ever fascinated by these devices ;-).
 
So how does this work?? The theory is: = If I can=20 throw the baseballs away faster than I catch them, I can make thrust! = Even=20 better, If I can keep all the energy I get when I catch it and put it = back in I=20 won't have to throw so hard. Imagine I catch it and let my arm fly = around=20 in a circle and let it go in the opposite direction. EUREKA! I can = just=20 snatch baseballs out of the air and throw them away and propel my self = about the=20 room!
 
So lets say I have this really slick = design and I=20 want to use this principle to go really fast. Lets say I have an = airplane which=20 will do 200 mph on 100hp. There are a few that can so this is within the = realm=20 of possibility.
 
Now the P51 went closer to 400 mph so = lets say this=20 is how fast we want to go to keep the math simple.
 
The energy in the baseballs we are = catching is=20 proportional to the square of the speed V^2. This means the baseballs = the P-51=20 is catching have 4 times the energy of the baseballs I am catching at = 200.=20
 
Which is a lot. But it gets worse. To = go 400 mph I=20 would need more power. How much? Power increases with the CUBE! So I = will need=20 2^3 or 2*2*2=3D8 or 800 hp! This means I have 4 times the energy and 8 = times the=20 heat rejection to work with by simply doubling the speed. So something = that is=20 significant at 400 mph is decimal dust below 200mph. We just don't have=20 energetic enough baseballs or a big enough arm to help ourselves out=20 here. 
 
So how does this help us. We have now = eliminated=20 50% of the cloud of incomprehensible gibberish. You are not going to = make a jet=20 engine from your piston single no matter how hard you try.
 
There is still some confusion about the = catchers=20 mitt however that results in much argument.
 
Some want the catchers mitt hung right = out in the=20 flow of baseballs, some want it cleverly hidden so the baseballs just = roll into=20 it. One group says that only real men fly with their catchers mitt in = the air=20 the others are just out to lunch.
 
Remember the hand!
 
Making pressure cost you no matter how = you do it.=20 The ideal inlet, whether flush or conventional, will be sized to catch = just the=20 right amount of air with a diffuser to build the pressure AFTER the = inlet. There=20 is NO external diffusion. The problem is the ideal inlet is = only ideal=20 for 1 flight condition. Change the temperature, pressure, altitude, = speed, or=20 engine operating point and it is now less than ideal.
 
Most airplanes have a flight envelope, = not a flight=20 point.
 
It turns out that you need a bigger = inlet for=20 climb, because you are going slow and making a lot of power. Then you = get to=20 altitude and speed up and make less power. The ideal inlet changes. The = typical=20 way to deal with this is to size for climb with an open cowl flap. Then = close=20 the flap and tolerate some mild external diffusion in cruise. This works = regardless of the inlet type.
 
Either inlet will make more pressure at = lower inlet=20 velocity ratios. Vi/Vo is how much slower the air going in the inlet is = vs. how=20 fast the airplane is flying. So if I am flying at 100 mph and my = velocity ratio=20 is .8 then the air through my inlet is doing 80mph.  Now not all = airplanes=20 have a convenient place to put a pitot inlet and this necessitates a = scoop type=20 inlet. the scoop has a lot of drag because it messes up the airflow all = around=20 and behind it plus it adds a lot of wetted area in order to properly = fair it. If=20 you decrease the inlet velocity ratio so that you start getting a lot of = external diffusion, and you do this on a laminar wing or cowl, you = really make a=20 mess.
 
 
The following graphs may be found in = NACA RM=20 A7I30
 
The problem with the flush inlet is = that it makes=20 up 85% of the free stream pressure at around .2-.6 inlet velocity = ratios.=20
3D""
 
FIG 18
 
Now this is pressure before the = diffuser. When they=20 placed a long diffuser on the inlet they got more losses at the higher = inlet=20 velocity ratios. This is easily attributable to mixing losses. There is = some low=20 hanging fruit here if you use one of the shorter diffuser = types.
 
3D""
 
Now look at the drag
3D""
 
FIG 25 
 
 
At an inlet velocity ratio of .8 the = drag is ZERO!!=20 And I can make at least 75% of the free stream pressure with the proper = inlet=20 size. Now at reasonable altitudes and cruise speeds that means 75% of = around 8=20 in of water. So I can make around 5 in water at 200 mph with no inlet = drag. Now=20 I am still catching baseballs and they are still scrubbing along the = ductwork=20 and it is still making drag, I am just not disturbing the external flow = or=20 making a mess around the inlet. You can do this with a pitot or scoop = inlet as=20 well, and you will get a higher pressure recovery with a well designed = diffuser,=20 but you have to hang your mitt out in the air and disturb all those = other=20 baseballs.
 
Now to size this for cruise, it will be = woefully=20 small for full power climb. You will have to figure out a way to deal = with that=20 to make this work. If you size it for climb you will be able to make = more=20 pressure at cruise, but your inlet velocity ratio will go down and your = drag=20 will go up, just like it would with a scoop or pitot inlet. If you use = an=20 augmenter to increase your inlet velocity ratio above 1 you may even get = some=20 THRUST! or negative drag from the inlet! Now you still caught the = baseball and=20 it is still scrubbing along the duct work so you probably will not make = thrust=20 overall, but you will definitely make less drag! Now this is not only = true of=20 the flush inlet, but is also true of the pitot or scoop. You will have = less=20 pressure recovery with the flush inlet the higher the inlet velocity = ratio IF=20 YOU USE A LONG DIFFUSER! Note, that is where the loss occurs, in the = diffuser.=20 This is due to mixing. If you use a shorter diffuser and use the = turbulence to=20 your advantage you may get better results.
 
Now if you can tell me where on a = typical single=20 engine airplane you can place a pitot type inlet with a proper diffuser = leading=20 to a vertical radiator and then have a perfect exit duct without making = a mess=20 on the wing or the front of the airplane, I would agree that it would be = the=20 ideal setup. The only place I can think of to do this is on a twin = engine=20 pusher. Then you might be able to put the Ideal setup to work. Otherwise = it is=20 all a compromise dependent on what you want the airplane to = do.
 
So there is no free lunch. But you can = make a NACA=20 flush inlet work and you can even do it without VGs, protruding lips or = other=20 Band-Aids.
 
Your mileage may vary.
 
Monty
 
 
 
 
 
 
 
 
 
 
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