X-Virus-Scanned: clean according to Sophos on Logan.com Return-Path: Received: from cdptpa-omtalb.mail.rr.com ([75.180.132.120] verified) by logan.com (CommuniGate Pro SMTP 5.2c2) with ESMTP id 2470520 for flyrotary@lancaironline.net; Tue, 13 Nov 2007 16:16:09 -0500 Received-SPF: pass receiver=logan.com; client-ip=75.180.132.120; envelope-from=eanderson@carolina.rr.com Received: from edward2 ([24.74.103.61]) by cdptpa-omta06.mail.rr.com with SMTP id <20071113211524.MWBE507.cdptpa-omta06.mail.rr.com@edward2> for ; Tue, 13 Nov 2007 21:15:24 +0000 Message-ID: <001b01c8263a$9c70b590$2402a8c0@edward2> From: "Ed Anderson" To: "Rotary motors in aircraft" References: Subject: Re: [FlyRotary] Re: Rebutal to the rebutal {:>) Thick vs Thin was : Diffuser Configuration Comparison Date: Tue, 13 Nov 2007 16:17:34 -0500 MIME-Version: 1.0 Content-Type: multipart/related; boundary="----=_NextPart_000_0017_01C82610.B33D9970"; type="multipart/alternative" X-Priority: 3 X-MSMail-Priority: Normal X-Mailer: Microsoft Outlook Express 6.00.2900.3138 X-MIMEOLE: Produced By Microsoft MimeOLE V6.00.2900.3138 This is a multi-part message in MIME format. ------=_NextPart_000_0017_01C82610.B33D9970 Content-Type: multipart/alternative; boundary="----=_NextPart_001_0018_01C82610.B33D9970" ------=_NextPart_001_0018_01C82610.B33D9970 Content-Type: text/plain; charset="iso-8859-1" Content-Transfer-Encoding: quoted-printable Sorry, Al, I disagree in this case. =20 1st addressing your statement regarding the inlet sizing. =20 Assuming that selecting your inlet opening size controls mass flow is = incomplete. It is the total pressure loss for the entire duct (and = core) which combined with the available freestream kinetic energy (due = to velocity) that determines mass flow. I can make changes to any of = the intake, diffuser, core, and outlet and make changes in the mass flow = - so its not just the inlet. =20 In fact, Mr. Horner in his tome on Fluid Dynamics states on page 9-2 = states ".... I mean what's the point in reading all this stuff if you can't name drop = {:>) 2nd regarding the deltaT "swap" I made: We are comparing apples and oranges, one is a thin large frontal area = core and the other is a smaller (frontal area) but thicker core, so = their heat transfer capability are going to be different. I do not agree that you need to compare on the basis of same mass flow = or deltaT - the only factor that really matters is that the needed heat = be removed. There are a large combinations of mass flow and deltaT that = will remove X amount of heat. =20 I personally don't see how you can change a core's fundamental = characteristics and dimension and then assume you are going to still = have the same mass flow or deltaT.=20 I mean if I reduce the dimensions of the diffuser, down sizing it to = meet the smaller cross sectional area of the thick core,and if I double = the thickness of that core (at least) and certainly change its pressure = drop characteristics and yet there is supposedly not suppose to be any = change? You may be correct, Al, but I just don't see it. From what I have = studied, its fairly clear to me that mass flow in a actual system is = NOT independent of the core characteristics, so if I change the core , = it sure seems to me that I have affected the mass flow - be it up or = down. =20 I was going to name drop again, and call on the spirits of K&W citing = pressure and heat transfer coefficients, but I don't think there would = be any point. Perhaps my light bulb will come on in the near future = {:>).=20 Again, always value your viewpoint, Al Ed From: Al Gietzen=20 To: Rotary motors in aircraft=20 Sent: Tuesday, November 13, 2007 2:49 PM Subject: [FlyRotary] Re: Rebutal to the rebutal {:>) Thick vs Thin was = : Diffuser Configuration Comparison Sorry; Ed, your argument is bogus. You changed horses in the middle = of the stream, and that is not allowed. You cannot suddenly change your = assumed delta T, because that also requires changing the inlet scoop, = which changes the mass flow rate. You size the inlet scoop to give you a mass flow needed at a given = delta T. If I expand that air to a large, thin core, it's velocity is = slow, and I get the given delta T. If I now expand the air half as much = for a frontal area that is half as large and the velocity is double, To = get the same delta T (whatever that thickness is, probably double) I = will get a pressure drop about 4 times as high for the same delta T. You have to compare them based on the same heat removal - same mass = flow, same delta T Al=20 -----Original Message----- From: Rotary motors in aircraft [mailto:flyrotary@lancaironline.net] = On Behalf Of Ed Anderson Sent: Tuesday, November 13, 2007 10:06 AM To: Rotary motors in aircraft Subject: [FlyRotary] Rebutal to the rebutal {:>) Thick vs Thin was : = Diffuser Configuration Comparison Hi Dave, Sure had me going for a spell, however, I got out the equations and = believe I can point out a different view point. If I understood you correctly, your basic assertion is that the same = mass flow is required for both thin and thick radiators and since the = thicker radiator has a smaller frontal area it must therefore have a = higher velocity air flow to generate the same mass flow to remove the = same heat. Furthermore the higher velocity also translates into more = drag (even with the reduced frontal area due to the drag being = proportional to the square of the velocity) - but all the above is not = necessarily true. In fact I found a NACA study where they looked at the effects of = using thicker radiators and I have worked out the equations on a = spreadsheet which I believe sheds some concrete facts on the old thin Vs = Thick debate - but, it is complex and I'll wait a bit before springing = it {:>). =20 However back to your contention that both radiators the thin and the = thick required the same mass flow to remove the same amount of heat - it = just isn't so and here is why. =20 First, we have two radiators one is 1" thick and 1 square ft in = frontal area, the second one is 1/2 square feet of frontal area and = twice (or more) as thick. Now turning to our trusty equation for heat = rejection and mass flow. Q =3D m*Cp*DeltaT is the basic equation that tells us how much heat we = remove for a mass flow "m", a specific heat (air =3D 0.24) and = temperature increase in the medium (air) or DeltaT. =20 Taking a specific example of say - 5000 Btu/min (which is about the = amount of heat an NA 13B generates at 175 HP that needs to be rejected = by the coolant). We know the Cp so that leaves the DeltaT and that is = what makes the difference. We have to assume a DeltaT, lets say 50F = (yes, it could easily be different but bear with me) then we have m =3D 5000/(0.24)*(50)/60 =3D 6.94 lbm/sec of mass flow . and lets = say we have a 1 square foot radiator to get rid of that heat. Then the = velocity requires V1 =3D m/(p1A1) =3D 6.94 lbm/min/(.0765*1) =3D 90 = ft/sec =3D 61.36 mph through the 1 square foot radiator. Perhaps a bit = higher than desirable but that's what we get. Now if I understood you correctly your point is that the same mass = flow is also required for the smaller radiator (1/2 sq ft) to remove the = same amount of heat and therefore since frontal area is 1/2 the size, = the velocity must be double that of the larger radiator to get the same = mass flow and remove the same quantity of heat. But, it just isn't = necessarily so. Taking the same conditions as before, except this time I use a DeltaT = of 100F (hey! its permitted as I'm using a different core here{:>) see = further discussion on effects of thickness on DeltaT). Now we have m = =3D 5000/(0.24)*100/60 =3D 3.47 lbm/sec of mass flow is required. That = is 1/2 of the mass flow required with a DeltaT of 50F. Therefore even with 1/2 the frontal area, I can use the same air = velocity as before and remove the same amount of heat with 1/2 the mass = flow and with LESS drag because my frontal area is now 1/2 that of the = thinner larger radiator and the velocity is the same. Now you can say I = cheated by having a different radiator, but that is certainly what you = would do - as that is what we are discussing are the relative merits of = thinner vs thicker for our application. But, If you reduce the frontal area of the radiator, then you must = increase the thickness (or add more fins, turbulators, etc) to increase = its Heat transfer coefficient to continue to reject sufficient heat to = the air flow. Therefore, The air temperature coming out of a thicker = radiator is going to be higher than a thin radiator. The reason is both = radiators are flowing at the same velocity (remember I did used the = same velocity for both radiators), and since the velocity of the flow is = the same for both radiators, the air spends more time (twice, three, = four times depending on the thickness) in the thicker core of the = smaller radiator. The longer duration of the air in the thicker core = causes it to be absorb more heat and be raised to a higher temperature = than the thinner radiator, therefore the higher deltaT (for the same = velocity air). This probably did not/and will not convince you of the merits of the = thicker vs thinner and besides I know your reservations about my = deductive reasoning {:>). So I am working on understanding fully the = Naca study I found that addresses the effect of thickness on required = mass flow and heat rejection. I believe it would be considered a fairly = credible source and will hopefully enable all to reach their own = conclusion. I think its going to blow the socks off this thick vs thin = debate - but, then I've been wrong before {:>) Boy, this is fun!!! Sure keeps the old brain working (hopefully). Anyhow, Dave, I respectively disagree with your assertion (see above) = {:>) Best Regards Ed ----- Original Message -----=20 From: "Ernest Christley" To: "Rotary motors in aircraft" Sent: Tuesday, November 13, 2007 9:19 AM Subject: [FlyRotary] Re: Thick vs Thin was : Diffuser Configuration = Comparison > David Leonard wrote: >> Why is it going slower? BECAUSE YOU HAVE DESIGNED YOUR THIN = RADIATOR SYSTEM >> DUCTS SUCH THAT AN EQUAL AMOUNT OF AIR PASSES THROUGH AN EQUAL = VOLUME OF >> RADIATOR AS WOULD OCCUR ON A THICK RADIATOR SYSTEM. (This is the = big if... >> system design... but bear with me). ie, equal amount of air, equal = volume >> of radiator - in the thin radiator system the air will be flowing = more >> slowly. >> =20 >=20 > I agree with your concept, Dave, but I think you underestimate the=20 > difficulty of fitting a large faced radiator into the physical=20 > constraints of the area available in a small airplane. I worked on=20 > trying to use a large, 1" thick radiator for a while, and this was = in a=20 > delta planform. I had comparitively HUGE amounts of volume to work=20 > with. I eventually gave up, as there was just no reasonable way to = get=20 > a duct built around it that would slow the air down. As you = increase=20 > the face area, you increase the size of the duct necessary to expand = the=20 > air without separation. The best radiator and duct ever created = will be=20 > useless if we have to leave it on the ground because it doesn't fit = in=20 > the airplane. >=20 > I think the flow chart for sizing a radiator for our needs should = follow=20 > something like this: >=20 > 1) Mark out a space for the largest volume that you can fit a = radiator=20 > and its associated ducting into. Insure that routing for the hoses = will=20 > be convenient, and the ducting can be made something resembling = efficient. >=20 > 2) Visit one of the websites like frigidair.com and find a radiator = that=20 > meets the dimensional specs you came up with. Or contact Jerry and = have=20 > him make you one of that size. >=20 > 3) If the core volume is less than 700 cubic inches, add another. >=20 > 4) Go fly. If it is to cool (<160F), choke off the inlet a little. = If=20 > it is to hot (>200F), fiddle with the ducting. >=20 > -- > Homepage: http://www.flyrotary.com/ > Archive and UnSub: = http://mail.lancaironline.net:81/lists/flyrotary/List.html ------=_NextPart_001_0018_01C82610.B33D9970 Content-Type: text/html; charset="iso-8859-1" Content-Transfer-Encoding: quoted-printable
Sorry, Al, I disagree in this case. =20
 
 1st addressing your statement regarding = the inlet=20 sizing. 
 
Assuming that selecting your inlet opening size = controls=20 mass flow is incomplete.  It is the total pressure loss for = the entire=20 duct (and core) which combined with the available = freestream kinetic energy=20 (due to velocity) that  determines mass flow  I can = make changes=20 to any of the intake, diffuser, core, and outlet and make changes in the = mass=20 flow - so its not just the inlet. 
 
In fact, Mr. Horner in his tome on Fluid = Dynamics=20 states on page 9-2  states "....
3D""
 
 
I mean what's the point in reading all this = stuff if you=20 can't name drop {:>)
 
 
2nd regarding the deltaT "swap" I = made:
 
We are comparing apples and = oranges, one=20 is a thin large frontal area core and the other is a smaller (frontal = area) but=20 thicker core, so their heat transfer capability are going to be=20 different.
 
I do not agree that you need to compare on the = basis of=20 same mass flow or deltaT - the only factor that really matters is that = the=20 needed heat be removed.  There are a large combinations of mass = flow and=20 deltaT that will remove X amount of heat. 
 
 I personally don't see how you can change = a core's=20 fundamental characteristics and dimension and then assume you = are=20 going to still have the same mass flow or deltaT. 
 
  I mean if I reduce the dimensions of the = diffuser,=20 down sizing it  to meet the smaller cross sectional area of the = thick=20 core,and if I double the thickness of that core (at least) and = certainly=20 change its pressure drop characteristics  and yet there is = supposedly not=20 suppose to be any change?
 
 You may be correct, Al, but I just don't = see=20 it.  From what I have studied, its fairly clear to me that  = mass flow=20 in a actual system is NOT independent of the core characteristics, = so if I=20 change the core , it sure seems to me that I have affected the mass flow = - be it=20 up or down.
 
I was going to name drop again, and call on = the=20 spirits of K&W citing pressure and heat transfer coefficients, but I = don't=20 think there would be any point.  Perhaps my  light bulb = will come=20 on in the near future {:>). 
 
Again, always value your viewpoint, = Al
 
Ed
 
From: Al Gietzen
 
Sent: Tuesday, November 13, = 2007 2:49=20 PM
Subject: [FlyRotary] Re: = Rebutal to the=20 rebutal {:>) Thick vs Thin was : Diffuser Configuration = Comparison

Sorry; = Ed, your=20 argument is bogus.  You changed horses in the middle of the = stream, and=20 that is not allowed.  You cannot suddenly change your assumed = delta T,=20 because that also requires changing the inlet scoop, which changes the = mass=20 flow rate.

 

You size = the inlet=20 scoop to give you a mass flow needed at a given delta T.  If I = expand=20 that air to a large, thin core, it=92s velocity is slow, and I get the = given=20 delta T.  If I now expand the air half as much for a frontal area = that is=20 half as large and the velocity is double, To get the = same delta T = (whatever=20 that thickness is, probably double) I will get a pressure drop about 4 = times=20 as high for the same delta=20 T.

 

You have = to compare=20 them based on the same heat = removal =96=20 same mass = flow,=20 same delta=20 T

 

Al=20

 

-----Original=20 Message-----
From: = Rotary=20 motors in aircraft [mailto:flyrotary@lancaironline.net] On Behalf Of Ed = Anderson
Sent:
Tuesday, = November=20 13, 2007 10:06=20 AM
To: Rotary motors in = aircraft
Subject: [FlyRotary] Rebutal to = the=20 rebutal {:>) Thick vs Thin was : Diffuser Configuration=20 Comparison

 

Hi = Dave,

 

Sure had me going for a = spell,=20 however, I got out the equations and believe I can point out a = different view=20 point.

 

If I understood you = correctly,=20 your basic assertion is that  the same mass flow is required for = both=20 thin and thick radiators and since the thicker radiator has = a=20 smaller frontal area  it must therefore have a higher velocity = air flow=20 to generate the same mass flow to remove the same =  heat. =20 Furthermore the higher velocity also translates into more drag (even = with the=20 reduced frontal area due to the drag being proportional to the square = of the=20 velocity) - but all the above is not necessarily=20 true.

 

  In fact I found a = NACA=20 study where they looked at the effects of using thicker radiators and = I have=20 worked out the equations on a spreadsheet which I believe sheds some = concrete=20 facts on the old thin Vs Thick debate - but, it is complex and I'll = wait a bit=20 before springing it {:>). 

 

However  back to = your=20 contention that both radiators the thin and the thick required the = same mass=20 flow to remove the same amount of heat - it just isn't so and here is=20 why. 

 

First, we have two = radiators one=20 is 1" thick and 1 square ft in frontal area, the second one is 1/2 = square feet=20 of frontal area and twice (or more) as thick.  Now turning to our = trusty=20 equation for heat rejection and mass flow.

 

Q =3D m*Cp*DeltaT is the = basic=20 equation that tells us how much heat we remove for a mass flow "m", a = specific=20 heat (air =3D 0.24) and temperature increase in the medium (air) or=20 DeltaT. 

 

Taking a specific = example of say -=20 5000 Btu/min (which is about the amount of heat an NA 13B generates at = 175 HP=20 that needs to be rejected by the coolant).  We know the Cp so = that leaves=20 the DeltaT and that is what makes the difference.  We have to = assume a=20 DeltaT, lets say 50F (yes, it could easily be different but bear with=20 me)  then we have

 

m =3D = 5000/(0.24)*(50)/60=20  =3D 6.94  lbm/sec of mass flow  . and = lets say we=20 have a 1 square foot radiator to get rid of that heat.  Then the = velocity=20 requires V1 =3D m/(p1A1) =3D 6.94 lbm/min/(.0765*1) =3D 90 ft/sec = =3D 61.36 mph=20 through the 1 square foot radiator.  Perhaps a bit higher than = desirable=20 but that's what we get.

 

  Now if I = understood you=20 correctly your point is that  the same mass flow is = also required=20 for the smaller radiator (1/2 sq ft) to remove the same amount of heat = and=20 therefore since frontal area is 1/2 the size,  the velocity must = be=20 double that of the larger radiator to get the same mass flow and = remove the=20 same quantity of heat.  But, it just isn't necessarily=20 so.

 

Taking the same = conditions as=20 before, except this time I use a DeltaT of 100F (hey! its permitted as = I'm=20 using a different core here{:>) see further discussion on effects = of=20 thickness on DeltaT).  Now we have m =3D 5000/(0.24)*100/60 =3D = 3.47 lbm/sec=20 of mass flow is required.  That is 1/2 of the mass flow required = with a=20 DeltaT of 50F.

 

Therefore even with 1/2 = the=20 frontal area, I can use the same air velocity as before and remove the = same=20 amount of heat with 1/2 the mass flow and with LESS drag because my = frontal=20 area is now 1/2 that of the thinner larger radiator and the velocity = is the=20 same.  Now you can say I cheated by having a different radiator, = but that=20 is certainly what you would do - as that is what we are discussing are = the=20 relative merits of thinner vs thicker for our=20 application.

 

But,  If you reduce = the=20 frontal area of the radiator,  then you must increase the = thickness (or=20 add more fins, turbulators, etc) to increase its Heat transfer=20 coefficient to continue to reject sufficient  heat to the = air=20 flow.  Therefore, The air temperature coming out of a thicker = radiator is=20 going to be higher than a thin radiator.  The reason is both = radiators=20 are flowing at the same velocity (remember I did used  the = same=20 velocity for both radiators), and since the velocity of the flow is = the same=20 for both radiators, the air spends more time (twice, three, four times = depending on the thickness) in the thicker core of the smaller=20 radiator.  The longer duration of the air in the thicker core = causes it=20 to be absorb more heat and be raised to a higher temperature than the = thinner=20 radiator, therefore the higher deltaT (for the same velocity=20 air).

 

This probably did = not/and will not=20 convince you of the merits of the thicker vs thinner and besides I = know your=20 reservations about my deductive reasoning {:>).  So I am = working on=20 understanding fully the Naca study I found that addresses the effect = of=20 thickness on required mass flow and heat rejection.  I believe it = would=20 be considered a fairly credible source and will hopefully enable all = to reach=20 their own conclusion.  I think its going to blow the socks off = this thick=20 vs thin debate - but, then I've been wrong before=20 {:>)

 

Boy, this is = fun!!!  Sure=20 keeps the old brain working (hopefully).

 

Anyhow, Dave, I = respectively=20 disagree with your assertion (see above) = {:>)

 

Best=20 Regards

 

Ed

 

 

 

 

 

 

----- Original Message = -----=20

From: "Ernest Christley" = <echristley@nc.rr.com>

To: "Rotary motors in = aircraft"=20 <flyrotary@lancaironline.net>

Sent: Tuesday, November = 13, 2007=20 9:19 AM

Subject: [FlyRotary] Re: = Thick vs=20 Thin was : Diffuser Configuration = Comparison

 

> David Leonard=20 wrote:
>> Why is it going slower?  BECAUSE YOU HAVE = DESIGNED=20 YOUR THIN RADIATOR SYSTEM
>> DUCTS SUCH THAT AN EQUAL AMOUNT = OF AIR=20 PASSES THROUGH AN EQUAL VOLUME OF
>> RADIATOR AS WOULD OCCUR = ON A=20 THICK RADIATOR SYSTEM.  (This is the big if...
>> system = design... but bear with me).  ie, equal amount of air, equal=20 volume
>> of radiator - in the thin radiator system the air = will be=20 flowing more
>> slowly.
>>  
> =
> I=20 agree with your concept, Dave, but I think you underestimate the =
>=20 difficulty of fitting a large faced radiator into the physical =
>=20 constraints of the area available in a small airplane.  I worked = on=20
> trying to use a large, 1" thick radiator for a while, and = this was in=20 a
> delta planform.  I had comparitively HUGE amounts of = volume to=20 work
> with.  I eventually gave up, as there was just no=20 reasonable way to get
> a duct built around it that would slow = the air=20 down.  As you increase
> the face area, you increase the = size of=20 the duct necessary to expand the
> air without = separation.  The=20 best radiator and duct ever created will be
> useless if we = have to=20 leave it on the ground because it doesn't fit in
> the=20 airplane.
>
> I think the flow chart for sizing a = radiator for=20 our needs should follow
> something like this:
>
> = 1) Mark=20 out a space for the largest volume that you can fit a radiator =
> and=20 its associated ducting into.  Insure that routing for the hoses = will=20
> be convenient, and the ducting can be made something = resembling=20 efficient.
>
> 2) Visit one of the websites like = frigidair.com=20 and find a radiator that
> meets the dimensional specs you came = up=20 with.  Or contact Jerry and have
> him make you one of = that=20 size.
>
> 3)  If the core volume is less than 700 = cubic=20 inches, add another.
>
> 4) Go fly.  If it is to = cool=20 (<160F), choke off the inlet a little.  If
> it is to = hot=20 (>200F), fiddle with the ducting.
>
> --
>=20 Homepage: 
http://www.flyrotary.com/
> Archive and=20 UnSub:   http://mail.lancaironline.net:81/lists/flyrotary/List.html<= /FONT>

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