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Subject: Re: [FlyRotary] Re: cooling system troubeshooting
Date: Thu, 28 Dec 2017 21:11:24 +0800
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Hi Guys
In search of cooler running this is what we did today and plan to do =
next.
Any insights/thoughts welcome.

Today we:
1. Installed a new pressurised tank with 21psi cap at the highest point =
possible. It is fed from:
 A. Rear Iron.=20
 B. Top of the coolant out manifold (engine heading for radiator).=20
 C. Top of radiator inlet tank
It returns to the pump inlet via a hose with a 1/8=E2=80=9D restriction.
It overflows into an expansion tank accessible via a hatch in the top =
cowl

2. Tested new config:
A. I wondered why she wasn=E2=80=99t running as sweet as usual and =
realised the Leading plugs weren=E2=80=99t firing so fixed the problem.
	With an OAT of ~ 80F after 20 mins of idle at 1800 rpm water =
gets to over 225 and I shut it down. (No significant change from last =
setup)
B. Measured Cowl pressure at a point between water radiator and cowl =
flap referenced to Static -=20
	At idle the pressure is 0 inches of water
	At 6000rpm (fine pitch) it hits about negative 1/2 inch of water =
(the exit shape, exhaust augmenter and cowl flap appear to be producing =
some negative pressure in the cowl)
	I=E2=80=99ve currently stuffed the gear opening full of pillows =
and rags to emulate the gear being up and door closed.

So here is the detail:
The 193 inch^3 oil cooler is fed by a 7.4 inch^2 inlet well below the =
spinner and into a trumpet diffuser.=20
The 540 inch^3 water cooler is fed by the 16.5 inch^2 right cheek inlet =
very close to the spinner and into a trumpet and then wedge diffuser. =
(Tried to copy Tracy=E2=80=99s RV8 cooler design)
Ive put a matrix of wool tufts over the back of the water cooler and =
distribution appears quite even.
See photo showing oil cooler inlet below spinner vs cheeks.
Currently the oil temps lag the water temps by a good 30F.

So next opportunity I=E2=80=99m thinking:
1. Because its a quick and easy test, I=E2=80=99m planning to close off =
part of the oil cooler inlet and see what this does to the water temps.
Will this provide a better balance between oil and water with the water =
rad getting a better share of the exit air flow?

2. Seek to plot a set of pressure measurements at various locations =
around the cowl and diffusers for various;
1. RPM=E2=80=99s
2. Cowl Flap position
3. Gear door open / closed (stuffed full of pillow and rag).

Many thanks for your ponderings and any of your thoughts.

Cheers

Steve
Perth Western Australia
Glasair Super IIRG - Renesis 4 port RD1C EC3 EM3=20



=09
=20
> On 28 Dec 2017, at 7:37 am, Stephen Izett stephen.izett@gmail.com =
<flyrotary@lancaironline.net> wrote:
>=20
> Hi Steve
>=20
> Aeroplane has not flown. We are still testing on the ground in OAT=E2=80=
=99s of 80-100F
> At idle (1900rpm) Delta T=E2=80=99s across Oil coiler - 18F, Water =
coiler - 8F
>=20
> We are seeking to do two things:
> 1. Review our design - have we made a clear mistake somewhere -
> a. We managed to not have an air bleed at the engine coolant in/out =
which is the highest point!
> We only have returns to the pressurised expansion tank/cap from rear =
iron and one from the top of the radiator in tank (returning to pump =
in).
> b. We do not have a small hole in the Renesis bypass which we plugged.
> c. Lynn uses a restrictor in the outlet to make sure the pump isn=E2=80=99=
t cavitating. Our coolant out plumbing has far less restriction than the =
stock setup (All be it the radiator is a dual pass so presents  =
significantly more resistance)
> d. We have just finished building a cowl flap in an attempt to control =
cowl pressure.
>=20
> 2. Do the science and seek to measure what the air and water are =
doing.
> a. Not sure how to measure the water flow easily.=20
> b. We are testing today to see what air pressures exist around the =
diffusers and cowl.
>=20
> Cheers
>=20
> Steve
>=20
>> On 28 Dec 2017, at 3:00 am, Steven W. Boese SBoese@uwyo.edu =
<flyrotary@lancaironline.net> wrote:
>>=20
>> Simply determining radiator coolant delta T may be useful in =
troubleshooting the cooling system.  The water cooling system is a =
closed system with two heat exchangers: one is the engine putting heat =
into the coolant and the other is the radiator removing heat from the =
coolant.  When all of the coolant flows through the engine and radiator =
(coolant bypass passage blocked by either a plug or a fully open =
thermostat) the engine and radiator must have the same coolant delta T.  =
At a given power level and coolant flow rate we all should see similar =
delta T's since we are using very similar engines.  At sea level full =
throttle, that coolant delta T should be close to 15 degrees F.  Since =
the heat exchanger characteristics of a clean engine are essentially =
fixed, a coolant delta T of much more than15 degrees F at full throttle =
would most likely be a result of insufficient coolant flow rate through =
the system.  This could result from a defective water pump or too much =
coolant bypassing the radiator such as due to an incompletely closed =
thermostat bypass passage, too large air bleeds from engine coolant high =
points, or an open cabin heater coolant loop.  An EWP would introduce an =
additional variable. =20
>>=20
>> With proper coolant flow rate, when the radiator cannot remove enough =
heat from the system, the overall coolant temperature will rise until =
one of two conditions are achieved.  First, the radiator may be capable =
of removing enough heat with a greater delta T between the coolant and =
the air.   The system will stabilize, but the delta T's of the coolant =
across the engine and across the radiator will remain essentially equal =
and unchanged.  This type of behavior is demonstrated in the attached =
data plot for a full throttle climb from 7,000 to 14,0000 ft msl with a =
typical OAT decrease.
>>=20
>> The second condition would be to boil the coolant and remove heat due =
to the phase change.  This may not maintain a closed system and the =
stable condition would then, of course, be temporary.
>>=20
>> The goal of designing the radiator side of the cooling system is to =
size the radiator and air flow through its core to achieve the desired =
overall coolant temperature.  Trying to change the coolant delta T at a =
given RPM and power level will prove frustrating.
>>=20
>> The same would be true of the oil cooling system if the oil flow rate =
was consistent between our systems.  However, if part of the oil flow is =
returned to the sump at the front cover relief valve, comparisons =
between different setups will be of limited value unless the actual oil =
flow rates through the oil coolers are known. =20
>>=20
>> Steve Boese
>> RV6A, 1986 13B NA, RD1A, EC2
>>=20
>>=20
>> <coolant delta T.jpg>--
>> Homepage:  http://www.flyrotary.com/
>> Archive and UnSub:   =
http://mail.lancaironline.net:81/lists/flyrotary/List.html
>=20
>=20
> --
> Homepage:  http://www.flyrotary.com/
> Archive and UnSub:   =
http://mail.lancaironline.net:81/lists/flyrotary/List.html


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<html><body style=3D"word-wrap: break-word; -webkit-nbsp-mode: space; =
-webkit-line-break: after-white-space;">Hi Guys<div class=3D"">In search =
of cooler running this is what we did today and plan to do =
next.</div><div class=3D"">Any insights/thoughts welcome.</div><div =
class=3D""><br class=3D""></div><div class=3D"">Today we:</div><div =
class=3D"">1. Installed a new pressurised tank with 21psi cap at the =
highest point possible. It is fed from:</div><div class=3D"">&nbsp;A. =
Rear Iron.&nbsp;</div><div class=3D"">&nbsp;B. Top of the coolant out =
manifold&nbsp;(engine heading for radiator).&nbsp;</div><div =
class=3D"">&nbsp;C. Top of radiator inlet tank</div><div class=3D"">It =
returns to the pump inlet via a hose with a 1/8=E2=80=9D =
restriction.</div><div class=3D"">It overflows into an expansion tank =
accessible via a hatch in the top cowl</div><div class=3D""><br =
class=3D""></div><div class=3D"">2. Tested new config:</div><div =
class=3D"">A. I wondered why she wasn=E2=80=99t running as sweet as =
usual and realised the Leading plugs weren=E2=80=99t firing so fixed the =
problem.</div><div class=3D""><span class=3D"Apple-tab-span" =
style=3D"white-space:pre">	</span>With an OAT of ~ 80F after 20 =
mins of idle at 1800 rpm water gets to over 225 and I shut it down. (No =
significant change from last setup)</div><div class=3D"">B. Measured =
Cowl pressure at a point between water radiator and cowl flap referenced =
to Static -&nbsp;</div><div class=3D""><span class=3D"Apple-tab-span" =
style=3D"white-space:pre">	</span>At idle the pressure is 0 inches =
of water</div><div class=3D""><span class=3D"Apple-tab-span" =
style=3D"white-space:pre">	</span>At 6000rpm (fine pitch) it hits =
about negative 1/2 inch of water (the exit shape, exhaust augmenter and =
cowl flap appear to be producing some negative pressure in the =
cowl)</div><div class=3D""><span class=3D"Apple-tab-span" =
style=3D"white-space:pre">	</span>I=E2=80=99ve currently stuffed =
the gear opening full of pillows and rags to emulate the gear being up =
and door closed.</div><div class=3D""><br class=3D""></div><div =
class=3D"">So here is the detail:</div><div class=3D"">The 193 inch^3 =
oil cooler is fed by a 7.4 inch^2 inlet well below the spinner and into =
a trumpet diffuser.&nbsp;</div><div class=3D"">The 540 inch^3 water =
cooler is fed by the 16.5 inch^2 right cheek inlet very close to the =
spinner and into a trumpet and then wedge diffuser. (Tried to copy =
Tracy=E2=80=99s RV8 cooler design)</div><div class=3D"">Ive put a matrix =
of wool tufts over the back of the water cooler and distribution appears =
quite even.</div><div class=3D"">See photo showing oil cooler inlet =
below spinner vs cheeks.</div><div class=3D"">Currently the oil temps =
lag the water temps by a good 30F.</div><div class=3D""><br =
class=3D""></div><div class=3D"">So next opportunity I=E2=80=99m =
thinking:</div><div class=3D"">1. Because its a quick and easy test, =
I=E2=80=99m planning to close off part of the oil cooler inlet and see =
what this does to the water temps.</div><div class=3D"">Will this =
provide a better balance between oil and water with the water rad =
getting a better share of the exit air flow?</div><div class=3D""><br =
class=3D""></div><div class=3D"">2. Seek to plot a set of pressure =
measurements at various locations around the cowl and diffusers for =
various;</div><div class=3D"">1. RPM=E2=80=99s</div><div class=3D"">2. =
Cowl Flap position</div><div class=3D"">3. Gear door open / closed =
(stuffed full of pillow and rag).</div><div class=3D""><br =
class=3D""></div><div class=3D"">Many thanks for your ponderings and any =
of your thoughts.</div><div class=3D""><br class=3D""></div><div =
class=3D"">Cheers</div><div class=3D""><br class=3D""></div><div =
class=3D"">Steve</div><div class=3D"">Perth Western Australia</div><div =
class=3D"">Glasair Super IIRG - Renesis 4 port RD1C EC3 =
EM3&nbsp;</div><div class=3D""><br class=3D""></div><div class=3D""><br =
class=3D""></div><div class=3D""><br class=3D""></div><div =
class=3D""><span class=3D"Apple-tab-span" style=3D"white-space:pre">	=
</span><img apple-inline=3D"yes" =
id=3D"E499FF19-1E2B-4534-9290-773BEF50664F" =
src=3D"cid:6AA6B0B7-2A1A-4BC4-A430-C2782EDC2359" class=3D""></div><div =
class=3D"">&nbsp;</div><div class=3D""><blockquote type=3D"cite" =
class=3D"">On 28 Dec 2017, at 7:37 am, Stephen Izett <a =
href=3D"mailto:stephen.izett@gmail.com" =
class=3D"">stephen.izett@gmail.com</a> &lt;<a =
href=3D"mailto:flyrotary@lancaironline.net" =
class=3D"">flyrotary@lancaironline.net</a>&gt; wrote:<br class=3D""><br =
class=3D"">Hi Steve<br class=3D""><br class=3D"">Aeroplane has not =
flown. We are still testing on the ground in OAT=E2=80=99s of 80-100F<br =
class=3D"">At idle (1900rpm) Delta T=E2=80=99s across Oil coiler - 18F, =
Water coiler - 8F<br class=3D""><br class=3D"">We are seeking to do two =
things:<br class=3D"">1. Review our design - have we made a clear =
mistake somewhere -<br class=3D"">a. We managed to not have an air bleed =
at the engine coolant in/out which is the highest point!<br class=3D"">We =
only have returns to the pressurised expansion tank/cap from rear iron =
and one from the top of the radiator in tank (returning to pump in).<br =
class=3D"">b. We do not have a small hole in the Renesis bypass which we =
plugged.<br class=3D"">c. Lynn uses a restrictor in the outlet to make =
sure the pump isn=E2=80=99t cavitating. Our coolant out plumbing has far =
less restriction than the stock setup (All be it the radiator is a dual =
pass so presents &nbsp;significantly more resistance)<br class=3D"">d. =
We have just finished building a cowl flap in an attempt to control cowl =
pressure.<br class=3D""><br class=3D"">2. Do the science and seek to =
measure what the air and water are doing.<br class=3D"">a. Not sure how =
to measure the water flow easily.&nbsp;<br class=3D"">b. We are testing =
today to see what air pressures exist around the diffusers and cowl.<br =
class=3D""><br class=3D"">Cheers<br class=3D""><br class=3D"">Steve<br =
class=3D""><br class=3D""><blockquote type=3D"cite" class=3D"">On 28 Dec =
2017, at 3:00 am, Steven W. Boese <a href=3D"mailto:SBoese@uwyo.edu" =
class=3D"">SBoese@uwyo.edu</a> &lt;<a =
href=3D"mailto:flyrotary@lancaironline.net" =
class=3D"">flyrotary@lancaironline.net</a>&gt; wrote:<br class=3D""><br =
class=3D"">Simply determining radiator coolant delta T may be useful in =
troubleshooting the cooling system. &nbsp;The water cooling system is a =
closed system with two heat exchangers: one is the engine putting heat =
into the coolant and the&nbsp;other is the radiator removing heat from =
the coolant. &nbsp;When all of the coolant flows through the engine and =
radiator (coolant bypass passage blocked by either a plug or a fully =
open thermostat) the engine and radiator must have&nbsp;the same coolant =
delta T. &nbsp;At a given power level and coolant flow rate we all =
should see similar delta T's since we are using very similar engines. =
&nbsp;At sea level full throttle, that coolant delta T should be close =
to 15 degrees F.&nbsp;&nbsp;Since the heat exchanger characteristics of =
a clean engine are essentially fixed, a coolant delta T of much more =
than15 degrees F at full throttle would most likely be a result of =
insufficient coolant flow rate through the system.&nbsp;&nbsp;This could =
result from a defective water pump or too much coolant bypassing the =
radiator such as due to an incompletely closed thermostat bypass =
passage, too large air bleeds from engine coolant high points, or an =
open cabin&nbsp;heater coolant loop. &nbsp;An EWP would introduce an =
additional variable. &nbsp;<br class=3D""><br class=3D"">With proper =
coolant flow rate, when the radiator cannot remove enough heat from the =
system, the overall coolant temperature will rise until one of two =
conditions are achieved. &nbsp;First, the radiator may be capable of =
removing&nbsp;enough heat with a greater delta T between the coolant and =
the air. &nbsp; The system will stabilize, but the delta T's of the =
coolant across the engine and across the radiator will remain =
essentially equal and unchanged. &nbsp;This type of&nbsp;behavior is =
demonstrated in the attached data plot for a full throttle climb from =
7,000 to 14,0000 ft msl with a typical OAT decrease.<br class=3D""><br =
class=3D"">The second condition would be to boil the coolant and remove =
heat due to the phase change. &nbsp;This may not maintain a closed =
system and the stable condition would then, of course, be temporary.<br =
class=3D""><br class=3D"">The goal of designing the radiator side of the =
cooling system is to size the radiator and air flow through its core to =
achieve the desired overall coolant temperature. &nbsp;Trying to change =
the coolant delta T at a given RPM and power&nbsp;level will prove =
frustrating.<br class=3D""><br class=3D"">The same would be true of the =
oil cooling system if the oil flow rate was consistent between our =
systems. &nbsp;However, if part of the oil flow is returned to the sump =
at the front cover relief valve, comparisons between different =
setups&nbsp;will be of limited value unless the actual oil flow rates =
through the oil coolers are known. &nbsp;<br class=3D""><br =
class=3D"">Steve Boese<br class=3D"">RV6A, 1986 13B NA, RD1A, EC2<br =
class=3D""><br class=3D""><br class=3D"">&lt;coolant delta =
T.jpg&gt;--<br class=3D"">Homepage: &nbsp;<a =
href=3D"http://www.flyrotary.com/" =
class=3D"">http://www.flyrotary.com/</a><br class=3D"">Archive and =
UnSub: &nbsp; <a =
href=3D"http://mail.lancaironline.net:81/lists/flyrotary/List.html" =
class=3D"">http://mail.lancaironline.net:81/lists/flyrotary/List.html</a><=
br class=3D""></blockquote><br class=3D""><br class=3D"">--<br =
class=3D"">Homepage: &nbsp;<a href=3D"http://www.flyrotary.com/" =
class=3D"">http://www.flyrotary.com/</a><br class=3D"">Archive and =
UnSub: &nbsp; <a =
href=3D"http://mail.lancaironline.net:81/lists/flyrotary/List.html" =
class=3D"">http://mail.lancaironline.net:81/lists/flyrotary/List.html</a><=
br class=3D""></blockquote><br class=3D""></div></body></html>=

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