X-Virus-Scanned: clean according to Sophos on Logan.com X-SpamCatcher-Score: 84 [XXX] (56%) BODY: contains an image tag with CID (44%) RECEIVED: IP not found on home country list Return-Path: Sender: To: lml Date: Fri, 02 Feb 2007 03:27:30 -0500 Message-ID: X-Original-Return-Path: Received: from mail25.syd.optusnet.com.au ([211.29.133.166] verified) by logan.com (CommuniGate Pro SMTP 5.1.5) with ESMTPS id 1805605 for lml@lancaironline.net; Thu, 01 Feb 2007 23:32:44 -0500 Received-SPF: none receiver=logan.com; client-ip=211.29.133.166; envelope-from=fredmoreno@optusnet.com.au Received: from fred (optussatellitebintb.22bjipb002.optus.net.au [59.154.24.148]) (authenticated sender fredmoreno) by mail25.syd.optusnet.com.au (8.13.1/8.13.1) with ESMTP id l124VYrn003836 for ; Fri, 2 Feb 2007 15:31:43 +1100 From: "Fred Moreno" X-Original-To: "Lancair Mail" Subject: Boost pump use X-Original-Date: Fri, 2 Feb 2007 13:32:21 +0900 X-Original-Message-ID: <020301c74683$285b7150$c211140a@fred> MIME-Version: 1.0 Content-Type: multipart/related; boundary="----=_NextPart_000_0204_01C746CE.98431950" X-Priority: 3 (Normal) X-MSMail-Priority: Normal X-Mailer: Microsoft Outlook, Build 10.0.6822 Thread-Index: AcdGgxvb6ePtNWDASBSLoM++yb3fsQ== X-MimeOLE: Produced By Microsoft MimeOLE V6.00.2900.3028 Importance: Normal This is a multi-part message in MIME format. ------=_NextPart_000_0204_01C746CE.98431950 Content-Type: multipart/alternative; boundary="----=_NextPart_001_0205_01C746CE.98431950" ------=_NextPart_001_0205_01C746CE.98431950 Content-Type: text/plain; charset="iso-8859-1" Content-Transfer-Encoding: quoted-printable Park in Phoenix, bake your airplane in the sun on the tarmac for a few = hours (or days), depart late afternoon, and then climb. At some point the = already hot fuel, when further heated on its way to the engine, is going to boil = and you will not be a happy camper. If you have not experienced it, it just means you have not truly heat soaked your fuel and then climbed high = enough. =20 I did just this during an ugly period when I had to commute to Phoenix = in my TR-182, a high wing airplane. I sometimes had engine surging as I climbed to 12,500, probably due to boiling of fuel in the carburettor = bowl.. I descended until it stopped, waited for the tanks to cool, and then = resumed the climb to cooler air (my ultimate goal) after about half an hour. = With a fuel injected low wing airplane, the problem would have been boiling = on the way to the engine-driven fuel pump, and the boost pump would have = solved it. =20 =20 The ultimate solution? Fuel pumps in the tanks. But boost pumps are = fine as long as you recognize what is going on when you visit Phoenix in July = =20 The following are extracted from the Chevron aviation fuel web site.=20 =20 http://www.chevron.com/products/prodserv/fuels/bulletin/aviationfuel/8_ag= _pe rf.shtm =20 Fred =20 =20 =20 Vapor Pressure The vapor pressure of a pure compound is defined as the pressure exerted = by its vapor in equilibrium with the liquid at a constant temperature. This pressure is independent of the amount evaporated, or vapor-liquid ratio, = as long as there is liquid remaining. Vapor pressure increases as = temperature increases. When the vapor pressure is equal to the external pressure (usually atmospheric pressure), the liquid boils. But fuels, which are mixtures of many different hydrocarbons, do = not behave the same as pure compounds. Each individual component in the fuel = has its own vapor pressure. The vapor phase over a fuel does not have the = same composition as the liquid phase. The vapor phase contains more of the = high vapor pressure (low boiling point) compounds than the liquid. As a fuel evaporates, its composition changes. The vapor pressure = of the remaining liquid decreases as the extent of evaporation increases. = For a complex mixture such as a fuel, vapor pressure is defined as the = pressure of the vapor in equilibrium with its liquid at a specified temperature, as = the vapor to liquid ratio approaches zero. This is the highest pressure that = a fuel can exert. In the petroleum industry, the true vapor pressure as defined above = is difficult to measure in practice, and is therefore not often used. = Instead, a related quantity called the Reid vapor pressure (RVP) is measured. = The RVP of a fuel is typically a few percentage points lower than the true = vapor pressure because of the way it is measured. =20 Elsewhere: Fuel Boil-Off The boiling point of a liquid is the temperature at = which its vapor pressure is equal to the local atmospheric pressure. However, atmospheric pressure decreases exponentially with increasing altitude. = At 3000 meters (10,000 feet), atmospheric pressure is only about 69 percent = as great as at sea level, and at 6000 meters (20,000 feet), it drops to 46 percent of the sea-level value. Thus liquids boil at lower temperatures = at higher altitudes.=20 Atmospheric temperature also decreases as altitude increases, which = tends to counteract the decrease in pressure. However, it takes time for fuel to = cool to ambient air temperature, while pressure equilibration is almost instantaneous since fuel tanks are vented to the atmosphere. An aircraft taking off from sea level with a fuel temperature of 38=BAC (100=BAF) = and ascending rapidly to 6000 meters (20,000 feet) may experience fuel vapor pressure that is greater than the pressure in the fuel tank, i.e., the = fuel will boil. [Emphasis added.] Any boil-off that does occur will likely be confined to the fuel tank since fuel pumps maintain the rest of the fuel system at a higher pressure. [But it can occur in the supply lines = leading up to the fuel pump, particularly if the pressure is lower in the supply line, as in sucking it up hill, and if the fuel is further heated.] If fuel does boil, the components with the highest vapor pressure = evaporate first. Loss of these lightest components changes the composition of the remaining liquid and leaves it with a lower vapor pressure. When the = fuel vapor pressure drops below the ambient pressure in the tank, boiling = will stop. Fuel boiling also lowers the temperature of the remaining liquid through evaporative cooling. Both of these effects tend to minimize loss = of fuel due to boiling. Only in extreme circumstances will loss of fuel = exceed a few percent.=20 The solubility of air dissolved in fuel also decreases as pressure decreases. Normally this air will come out of solution smoothly and not cause a problem. However, if the fuel becomes supersaturated, air can be evolved very quickly and cause frothing of the fuel. This can lead to = loss of fuel from vents, but the mechanism is different from actual fuel = boiling. Vapor Lock Vapor lock occurs when excessive gasoline vapor = accumulates somewhere in the fuel system =96 fuel pump, fuel line, carburetor or = fuel injector =96 and reduces or interrupts the fuel supply to the engine. = When the fuel supply is reduced, the fuel-air ratio becomes too lean, which may result in loss of power, knocking, surging, or backfiring. When the fuel supply is interrupted, the engine stops and may be difficult to restart until the fuel system has cooled and the vapor recondensed, or purged by boosting the fuel supply pressure.=20 While the tendency of avgas to vapor lock increases with volatility, = fuel overheating is the main cause of vapor lock. Local temperatures in the = fuel system are determined by how hard the engine is working and how well the fuel system is isolated from the heat of the engine. Fuel residence time = in the hot sections of the system, mechanical vibration, and other factors = also play a significant role in vapor lock behavior.=20 The altitude at which the engine is operating has two opposing = influences: ambient temperatures are lower at higher altitudes, which should improve fuel system cooling; but ambient pressures are also lower, making vaporization easier.=20 The design of an aircraft fuel system must take all the above factors = into account to ensure that liquid fuel, with little or no free vapor, is delivered to the engine's fuel metering system.=20 =20 =20 =20 Below is a typical distillation curve for avgas. ------=_NextPart_001_0205_01C746CE.98431950 Content-Type: text/html; charset="iso-8859-1" Content-Transfer-Encoding: quoted-printable

Park in Phoenix, bake your airplane in the sun on the tarmac for a few hours (or days), depart late afternoon, and then climb.=A0 At some point the already hot fuel, when = further heated on its way to the engine, is going to boil and you will not be a = happy camper.=A0 If you have not experienced it, it just means you have not = truly heat soaked your fuel and then climbed high enough.=A0

 

=A0I did just this during an ugly = period when I had to commute to Phoenix in my = TR-182, a high wing airplane.=A0 I sometimes had engine surging as I climbed to 12,500, = probably due to boiling of fuel in the carburettor bowl..=A0 I descended until it = stopped, waited for the tanks to cool, and then resumed the climb to cooler air = (my ultimate goal) after about half an hour. =A0=A0With a fuel injected low = wing airplane, the problem would have been boiling on the way to the = engine-driven fuel pump, and the boost pump would have solved it.=A0 =

 

The ultimate solution?=A0 Fuel = pumps in the tanks. =A0=A0But boost pumps are fine as long as you recognize what is = going on when you visit Phoenix in July =

 

The following are extracted from = the Chevron aviation fuel web site.

 

http://www.chevron.com/products/pro= dserv/fuels/bulletin/aviationfuel/8_ag_perf.shtm

 

Fred

 

 

 

Vapor Pressure
The vapor pressure of a pure compound is defined as the pressure = exerted by its vapor in equilibrium with the liquid at a constant temperature. This pressure is independent of the amount evaporated, or vapor-liquid ratio, = as long as there is liquid remaining. Vapor pressure increases as = temperature increases. When the vapor pressure is equal to the external pressure = (usually atmospheric pressure), the liquid boils.
     But fuels, which are mixtures of many = different hydrocarbons, do not behave the same as pure compounds. Each individual component in the fuel has its own vapor pressure. The vapor phase over a = fuel does not have the same composition as the liquid phase. The vapor phase contains more of the high vapor pressure (low boiling point) compounds = than the liquid.
     As a fuel evaporates, its composition = changes. The vapor pressure of the remaining liquid decreases as the extent of = evaporation increases. For a complex mixture such as a fuel, vapor pressure is = defined as the pressure of the vapor in equilibrium with its liquid at a specified temperature, as the vapor to liquid ratio approaches zero. This is the = highest pressure that a fuel can exert.
     In the petroleum industry, the true vapor pressure as defined above is difficult to measure in practice, and is = therefore not often used. Instead, a related quantity called the Reid vapor pressure (RVP) is = measured. The RVP of a fuel is typically a few percentage points lower than the = true vapor pressure because of the way it is measured.

 

Elsewhere:

Fuel = Boil-Off    The boiling point of a liquid is the temperature at = which its vapor pressure is equal to the local atmospheric pressure. However, = atmospheric pressure decreases exponentially with increasing altitude. At 3000 = meters (10,000 feet), atmospheric pressure is only about 69 percent as great as = at sea level, and at 6000 meters (20,000 feet), it drops to 46 percent of the sea-level value. Thus liquids boil at lower temperatures at higher = altitudes.

Atmospheric temperature also decreases as altitude = increases, which tends to counteract the decrease in pressure. However, it takes = time for fuel to cool to ambient air temperature, while pressure equilibration is = almost instantaneous since fuel tanks are vented to the atmosphere. An aircraft = taking off from sea level with a fuel temperature of 38=BAC (100=BAF) and = ascending rapidly to 6000 meters (20,000 feet) may experience fuel vapor = pressure that is greater than the pressure in the fuel tank, i.e., the fuel will = boil. [Emphasis = added.] = Any boil-off that does occur will likely be confined to the fuel tank since fuel = pumps maintain the rest of the fuel system at a higher = pressure. = =A0[But it can occur in the supply lines leading up to the fuel pump, particularly if = the pressure is lower in the supply line, as in sucking it up hill, and if = the fuel is further heated.]

If fuel does boil, the components with the highest = vapor pressure evaporate first. Loss of these lightest components changes the composition of the remaining liquid and leaves it with a lower vapor = pressure. When the fuel vapor pressure drops below the ambient pressure in the = tank, boiling will stop. Fuel boiling also lowers the temperature of the = remaining liquid through evaporative cooling. Both of these effects tend to = minimize loss of fuel due to boiling. Only in extreme circumstances will loss of fuel = exceed a few percent.

The solubility of air dissolved in fuel also decreases = as pressure decreases. Normally this air will come out of solution smoothly = and not cause a problem. However, if the fuel becomes supersaturated, air = can be evolved very quickly and cause frothing of the fuel. This can lead to = loss of fuel from vents, but the mechanism is different from actual fuel = boiling.

Vapor = Lock    Vapor = lock occurs when excessive gasoline vapor accumulates somewhere in the fuel = system – fuel pump, fuel line, carburetor or fuel injector – and = reduces or interrupts the fuel supply to the engine. When the fuel supply is = reduced, the fuel-air ratio becomes too lean, which may result in loss of power, knocking, surging, or backfiring. When the fuel supply is interrupted, = the engine stops and may be difficult to restart until the fuel system has = cooled and the vapor recondensed, or purged by boosting the fuel supply = pressure.

While the tendency of avgas to vapor lock increases = with volatility, fuel overheating is the main cause of vapor lock. Local temperatures in the fuel system are determined by how hard the engine is working and how well the fuel system is isolated from the heat of the = engine. Fuel residence time in the hot sections of the system, mechanical = vibration, and other factors also play a significant role in vapor lock behavior. =

The altitude at which the engine is operating has two opposing influences: ambient temperatures are lower at higher altitudes, = which should improve fuel system cooling; but ambient pressures are also = lower, making vaporization easier.

The design of an aircraft fuel system must take all = the above factors into account to ensure that liquid fuel, with little or no free = vapor, is delivered to the engine's fuel metering system.

 

 

 

Below is a typical distillation curve for = avgas.

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