CHAPTER VII

Why Lubrication Is Necessary--Friction Defined--Theory of

Lubrication--Derivation of Lubricants--Properties of Cylinder

Oils--Factors Influencing Lubrication System Selection--Gnome

Type Engines Use Castor Oil--Hall-Scott Lubrication System--Oil

Supply by Constant Level Splash System--Dry Crank-Case System

Best for Airplane Engines--Why Cooling Systems Are Necessary--

Cooling Systems Generally Applied--Cooling by Positive Pump

Circulation--Thermo-Syphon System--Direct Air-Cooling Methods--

Air-Cooled Engine Design Considerations.

WHY LUBRICATION IS NECESSARY

The importance of minimizing friction at the various bearing surfaces of

machines to secure mechanical efficiency is fully recognized by all

mechanics, and proper lubricity of all parts of the mechanism is a very

essential factor upon which the durability and successful operation of

the motor car power plant depends. All of the moving members of the

engine which are in contact with other portions, whether the motion is

continuous or intermittent, of high or low velocity, or of rectilinear

or continued rotary nature, should be provided with an adequate supply

of oil. No other assemblage of mechanism is operated under conditions

which are so much to its disadvantage as the motor car, and the tendency

is toward a simplification of oiling methods so that the supply will be

ample and automatically applied to the points needing it.

In all machinery in motion the members which are in contact have a

tendency to stick to each other, and the very minute projections which

exist on even the smoothest of surfaces would have a tendency to cling

or adhere to each other if the surfaces were not kept apart by some

elastic and unctuous substance. This will flow or spread out over the

surfaces and smooth out the inequalities existing which tend to produce

heat and retard motion of the pieces relative to each other.

A general impression which obtains is that well machined surfaces are

smooth, but while they are apparently free from roughness, and no

projections are visible to the naked eye, any smooth bearing surface,

even if very carefully ground, will have a rough appearance if examined

with a magnifying glass. An exaggerated condition to illustrate this

point is shown at Fig. 75. The amount of friction will vary in

proportion to the pressure on the surfaces in contact and will augment

as the loads increase; the rougher surfaces will have more friction than

smoother ones and soft bodies will produce more friction than hard

substances.

FRICTION DEFINED

Friction is always present in any mechanism as a resisting force that

tends to retard motion and bring all moving parts to a state of rest.

The absorption of power by friction may be gauged by the amount of heat

which exists at the bearing points. Friction of solids may be divided

into two classes: sliding friction, such as exists between the piston

and cylinder, or the bearings of a gas-engine, and rolling friction,

which is that present when the load is supported by ball or roller

bearings, or that which exists between the tires or the driving wheels

and the road. Engineers endeavor to keep friction losses as low as

possible, and much care is taken in all modern airplane engines to

provide adequate methods of lubrication, or anti-friction bearings at

all points where considerable friction exists.

THEORY OF LUBRICATION

The reason a lubricant is supplied to bearing points will be easily

understood if one considers that these elastic substances flow between

the close fitting surfaces, and by filling up the minute depressions in

the surfaces and covering the high spots act as a cushion which absorbs

the heat generated and takes the wear instead of the metallic bearing

surface. The closer the parts fit together the more fluid the lubricant

must be to pass between their surfaces, and at the same time it must

possess sufficient body so that it will not be entirely forced out by

the pressure existing between the parts.

[Illustration: Fig. 75.--Showing Use of Magnifying Glass to Demonstrate

that Apparently Smooth Metal Surfaces May Have Minute Irregularities

which Produce Friction.]

Oils should have good adhesive, as well as cohesive, qualities. The

former are necessary so that the oil film will cling well to the

surfaces of the bearings; the latter, so the oil particles will cling

together and resist the tendency to separation which exists all the time

the bearings are in operation. When used for gas-engine lubrication the

oil should be capable of withstanding considerable heat in order that it

will not be vaporized by the hot portions of the cylinder. It should

have sufficient cold test so that it will remain fluid and flow readily

at low temperature. Lubricants should be free from acid, or alkalies,

which tend to produce a chemical action with metals and result in

corrosion of the parts to which they are applied. It is imperative that

the oil be exactly the proper quality and nature for the purpose

intended and that it be applied in a positive manner. The requirements

may be briefly summarized as follows:

First--It must have sufficient body to prevent seizing of the parts to

which it is applied and between which it is depended upon to maintain an

elastic film, and yet it must not have too much viscosity, in order to

minimize the internal or fluid friction which exists between the

particles of the lubricant itself.

Second--The lubricant must not coagulate or gum; must not injure the

parts to which it is applied, either by chemical action or by producing

injurious deposits, and it should not evaporate readily.

Third--The character of the work will demand that the oil should not

vaporize when heated or thicken to such a point that it will not flow

readily when cold.

Fourth--The oil must be free from acid, alkalies, animal or vegetable

fillers, or other injurious agencies.

Fifth--It must be carefully selected for the work required and should be

a good conductor of heat.

DERIVATION OF LUBRICANTS

The first oils which were used for lubricating machinery were obtained

from animal and vegetable sources, though at the present time most

unguents are of mineral derivation. Lubricants may exist as fluids,

semifluids, or solids. The viscosity will vary from light spindle or

dynamo oils, which have but little more body than kerosene, to the

heaviest greases and tallows. The most common solid employed as a

lubricant is graphite, sometimes termed "plumbago" or "black lead." This

substance is of mineral derivation.

The disadvantage of oils of organic origin, such as those obtained from

animal fats or vegetable substances, is that they will absorb oxygen

from the atmosphere, which causes them to thicken or become rancid.

Such oils have a very poor cold test, as they solidify at comparatively

high temperatures, and their flashing point is so low that they cannot

be used at points where much heat exists. In most animal oils various

acids are present in greater or less quantities, and for this reason

they are not well adapted for lubricating metallic surfaces which may be

raised high enough in temperature to cause decomposition of the oils.

Lubricants derived from the crude petroleum are called "Oleonaphthas"

and they are a product of the process of refining petroleum through

which gasoline and kerosene are obtained. They are of lower cost than

vegetable or animal oil, and as they are of non-organic origin, they do

not become rancid or gummy by constant exposure to the air, and they

will have no corrosive action on metals because they contain no

deleterious substances in chemical composition. By the process of

fractional distillation mineral oils of all grades can be obtained. They

have a lower cold and higher flash test and there is not the liability

of spontaneous combustion that exists with animal oils.

The organic oils are derived from fatty substances, which are present in

the bodies of all animals and in some portions of plants. The general

method of extracting oil from animal bodies is by a rendering process,

which consists of applying sufficient heat to liquefy the oil and then

separating it from the tissue with which it is combined by compression.

The only oil which is used to any extent in gas-engine lubrication that

is not of mineral derivation is castor oil. This substance has been used

on high-speed racing automobile engines and on airplane power plants. It

is obtained from the seeds of the castor plant, which contain a large

percentage of oil.

Among the solid substances which may be used for lubricating purposes

may be mentioned tallow, which is obtained from the fat of animals, and

graphite and soapstone, which are of mineral derivation. Tallow is

never used at points where it will be exposed to much heat, though it

is often employed as a filler for greases used in transmission gearing

of autos. Graphite is sometimes mixed with oil and applied to cylinder

lubrication, though it is most often used in connection with greases in

the landing gear parts and for coating wires and cables of the airplane.

Graphite is not affected by heat, cold, acids, or alkalies, and has a

strong attraction for metal surfaces. It mixes readily with oils and

greases and increases their efficiency in many applications. It is

sometimes used where it would not be possible to use other lubricants

because of extremes of temperature.

The oils used for cylinder lubrication are obtained almost exclusively

from crude petroleum derived from American wells. Special care must be

taken in the selection of crude material, as every variety will not

yield oil of the proper quality to be used as a cylinder lubricant. The

crude petroleum is distilled as rapidly as possible with fire heat to

vaporize off the naphthas and the burning oils. After these vapors have

been given off superheated steam is provided to assist in distilling.

When enough of the light elements have been eliminated the residue is

drawn off, passed through a strainer to free it from grit and earthy

matters, and is afterwards cooled to separate the wax from it. This is

the dark cylinder oil and is the grade usually used for steam-engine

cylinders.

PROPERTIES OF CYLINDER OILS

The oil that is to be used in the gasoline engine must be of high

quality, and for that reason the best grades are distilled in a vacuum

that the light distillates may be separated at much lower temperatures

than ordinary conditions of distilling permit. If the degree of heat is

not high the product is not so apt to decompose and deposit carbon. If

it is desired to remove the color of the oil which is caused by free

carbon and other impurities it can be accomplished by filtering the oil

through charcoal. The greater the number of times the oil is filtered,

the lighter it will become in color. The best cylinder oils have flash

points usually in excess of 500 degrees F., and while they have a high

degree of viscosity at 100 degrees F. they become more fluid as the

temperature increases.

The lubricating oils obtained by refining crude petroleum may be divided

into three classes:

First--The natural oils of great body which are prepared for use by

allowing the crude material to settle in tanks at high temperature and

from which the impurities are removed by natural filtration. These oils

are given the necessary body and are free from the volatile substances

they contain by means of superheated steam which provides a source of

heat.

Second--Another grade of these natural oils which are filtered again at

high temperatures and under pressure through beds of animal charcoal to

improve their color.

Third--Pale, limpid oils, obtained by distillation and subsequent

chemical treatment from the residuum produced in refining petroleum to

obtain the fuel oils.

Authorities agree that any form of mixed oil in which animal and mineral

lubricants are combined should never be used in the cylinder of a gas

engine as the admixture of the lubricants does not prevent the

decomposition of the organic oil into the glycerides and fatty acids

peculiar to the fat used. In a gas-engine cylinder the flame tends to

produce more or less charring. The deposits of carbon will be much

greater with animal oils than with those derived from the petroleum base

because the constituents of a fat or tallow are not of the same volatile

character as those which comprise the hydro-carbon oils which will

evaporate or volatilize before they char in most instances.

FACTORS INFLUENCING LUBRICATION SYSTEM SELECTION

The suitability of oil for the proper and efficient lubrication of all

internal combustion engines is determined chiefly by the following

factors:

1. Type of cooling system (operating temperatures).

2. Type of lubricating system (method of applying oil to the moving

parts).

3. Rubbing speeds of contact surfaces.

Were the operating temperatures, bearing surface speeds and lubrication

systems identical, a single oil could be used in all engines with equal

satisfaction. The only change then necessary in viscosity would be that

due to climatic conditions. As engines are now designed, only three

grades of oil are necessary for the lubrication of all types with the

exception of Knight, air-cooled and some engines which run continuously

at full load. In the specification of engine lubricants the feature of

load carried by the engine should be carefully considered.

_Full Load Engines._

1. Marine.

2. Racing automobile.

3. Aviation.

4. Farm tractor.

5. Some stationary.

_Variable Load Engines._

1. Pleasure automobile.

2. Commercial vehicle.

3. Motor cycle.

4. Some stationary.

Of the forms outlined, the only one we have any immediate concern about

is the airplane power plant. The Platt & Washburn Refining Company, who

have made a careful study of the lubrication problem as applied to all

types of engines, have found a peculiar set of conditions to apply to

oiling high-speed constant-duty or "full-load" engines. Modern airplane

engines are designed to operate continuously at a fairly uniform high

rotative speed and at full load over long periods of time. As a sequence

to this heavy duty the operating temperatures are elevated. For the

sake of extreme lightness in weight of all parts, very thin alloy steel

aluminum or cast iron pistons are fitted and the temperature of the thin

piston heads at the center reaches anywhere between 600 deg. and 1,400 deg.

Fahr., as in automobile racing engines. Freely exposed to such intense

heat hydro-carbon oils are partially "cracked" into light and heavy

products or polymerized into solid hydro-carbons. From these facts it

follows that only heavy mineral oils of low carbon residue and of the

greatest chemical purity and stability should be used to secure good

lubrication. In all cases the oil should be sufficiently heavy to assure

the highest horse-power and fuel and oil economy compatible with perfect

lubrication, avoiding, at the same time, carbonization and ignition

failure. When aluminum pistons are used their superior heat-conducting

properties aid materially in reducing the rate of oil destruction.

The extraordinary evolutions described by airplanes in flight make it a

matter of vital necessity to operate engines inclined at all angles to

the vertical as well as in an upside-down position. To meet this

situation lubricating systems have been elaborated so as to deliver an

abundance of oil where needed and to eliminate possible flooding of

cylinders. This is done by applying a full force feed system,

distributing oil under considerable pressure to all working parts.

Discharged through the bearings, the oil drains down to the suction side

of a second pump located in the bottom of the base chamber. This pump

being of greater capacity than the first prevents the accumulation of

oil in the crank-case, and forces it to a separate oil reservoir-cooler,

whence it flows back in rapid circulation to the pump feeding the

bearings. With this arrangement positive lubrication is entirely

independent of engine position. The lubricating system of the

Thomas-Morse aviation engines, which is shown at Fig. 76, is typical of

current practice.

[Illustration: Fig. 76.--Pressure Feed Oiling System of Thomas Aviation

Engine Includes Oil Cooling Means.]

GNOME TYPE ENGINES USE CASTOR OIL

The construction and operation of rotative radial cylinder engines

introduce additional difficulties of lubrication to those already

referred to and merit especial attention. Owing to the peculiar

alimentation systems of Gnome type engines, atomized gasoline mixed with

air is drawn through the hollow stationary crank-shaft directly into the

crank-case which it fills on the way to the cylinders. Therein lies the

trouble. Hydrocarbon oils are soon dissolved by the gasoline and washed

off, leaving the bearing surfaces without adequate protection and

exposed to instant wear and destruction. So castor oil is resorted to as

an indispensable but unfortunate compromise. Of vegetable origin, it

leaves a much more bulky carbon deposit in the explosion chambers than

does mineral oil and its great affinity for oxygen causes the formation

of voluminous gummy deposit in the crank-case. Engines employing it need

to be dismounted and thoroughly scraped out at frequent intervals. It is

advisable to use only unblended chemically pure castor oil in rotative

engines, first by virtue of its insolubility in gasoline and second

because its extra heavy body can resist the high temperature of

air-cooled cylinders.

HALL-SCOTT LUBRICATION SYSTEM

[Illustration: Fig. 77.--Diagram of Oiling System, Hall-Scott Type A 125

Horse-Power Engine.]

The oiling system of the Hall-Scott type A-5 125 horse-power engine is

clearly shown at Fig. 77. It is completely described in the instruction

book issued by the company from which the following extracts are

reproduced by permission. Crank-shaft, connecting rods and all other

parts within the crank-case and cylinders are lubricated directly or

indirectly by a force-feed oiling system. The cylinder walls and wrist

pins are lubricated by oil spray thrown from the lower end of connecting

rod bearings. This system is used only upon A-5 engines. Upon A-7a and

A-5a engines a small tube supplies oil from connecting rod bearing

directly upon the wrist pin. The oil is drawn from the strainer located

at the lowest portion of the lower crank-case, forced around the main

intake manifold oil jacket. From here it is circulated to the main

distributing pipe located along the lower left hand side of upper

crank-case. The oil is then forced directly to the lower side of

crank-shaft, through holes drilled in each main bearing cup. Leakage

from these main bearings is caught in scuppers placed upon the cheeks of

the crank-shafts furnishing oil under pressure to the connecting rod

bearings. A-7a and A-5a engines have small tubes leading from these

bearings which convey the oil under pressure to the wrist pins.

A bi-pass located at the front end of the distributing oil pipe can be

regulated to lessen or raise the pressure. By screwing the valve in, the

pressure will raise and more oil will be forced to the bearings. By

unscrewing, pressure is reduced and less oil is fed. A-7a and A-5a

engines have oil relief valves located just off of the main oil pump in

the lower crank-case. This regulates the pressure at all times so that

in cold weather there will be no danger of bursting oil pipes due to

excessive pressure. If it is found the oil pressure is not maintained at

a high enough level, inspect this valve. A stronger spring will not

allow the oil to bi-pass so freely, and consequently the pressure will

be raised; a weaker spring will bi-pass more oil and reduce the oil

pressure materially. Independent of the above-mentioned system, a small,

directly driven rotary oiler feeds oil to the base of each individual

cylinder. The supply of oil is furnished by the main oil pump located in

the lower crank-case. A small sight-feed regulator is furnished to

control the supply of oil from this oiler. This instrument should be

placed higher than the auxiliary oil distributor itself to enable the

oil to drain by gravity feed to the oiler. If there is no available

place with the necessary height in the front seat of plane, connect it

directly to the intake L fitting on the oiler in an upright position. It

should be regulated with full open throttle to maintain an oil level in

the glass, approximately half way.

An oil pressure gauge is provided. This should be run to the pilot's

instrument board. The gauge registers the oil pressure upon the

bearings, also determining its circulation. Strict watch should be

maintained of this instrument by pilot, and if for any reason its hand

should drop to 0 the motor should be immediately stopped and the trouble

found before restarting engine. Care should be taken that the oil does

not work up into the gauge, as it will prevent the correct gauge

registering of oil pressure. The oil pressure will vary according to

weather conditions and viscosity of oil used. In normal weather, with

the engine properly warmed up, the pressure will register on the oil

gauge from 5 to 10 pounds when the engine is turning from 1,275 to 1,300

r. p. m. This does not apply to all aviation engines, however, as the

proper pressure advised for the Curtiss OX-2 motor is from 40 to 55

pounds at the gauge.

The oil sump plug is located at the lowest point of the lower

crank-case. This is a combination dirt, water and sediment trap. It is

easily removed by unscrewing. Oil is furnished mechanically to the

cam-shaft housing under pressure through a small tube leading from the

main distributing pipe at the propeller end of engine directly into the

end of cam-shaft housing. The opposite end of this housing is amply

relieved to allow the oil to rapidly flow down upon cam-shaft, magneto,

pinion-shaft, and crank-shaft gears, after which it returns to lower

crank-case. An outside overflow pipe is also provided to carry away the

surplus oil.

DRAINING OIL FROM CRANK-CASE

The oil strainer is placed at the lowest point of the lower crank-case.

This strainer should be removed after every five to eight hours running

of the engine and cleaned thoroughly with gasoline. It is also advisable

to squirt distillate up into the case through the opening where the

strainer has been removed. Allow this distillate to drain out thoroughly

before replacing the plug with strainer attached. Be sure gasket is in

place on plug before replacing. Pour new oil in through either of the

two breather pipes on exhaust side of motor. Be sure to replace strainer

screens if removed. If, through oversight, the engine does not receive

sufficient lubrication and begins to heat or pound, it should be stopped

immediately. After allowing engine to cool pour at least three gallons

of oil into oil sump. Fill radiator with water after engine has cooled.

Should there be apparent damage, the engine should be thoroughly

inspected immediately without further running. If no obvious damage has

been done, the engine should be given a careful examination at the

earliest opportunity to see that the running without oil has not burned

the bearings or caused other trouble.

Oils best adapted for Hall-Scott engines have the following properties:

A flash test of not less than 400 deg. F.; viscosity of not less than 75

to 85 taken at 21 deg. F. with Saybolt's Universal Viscosimeter.

_Zeroline heavy duty oil_, manufactured by the Standard Oil Company of

California; also,

_Gargoyle mobile B oil_, manufactured by the Vacuum Oil Company, both

fulfill the above specifications. One or the other of these oils can be

obtained all over the world.

Monogram extra heavy is also recommended.

OIL SUPPLY BY CONSTANT LEVEL SPLASH SYSTEM

The splash system of lubrication that depends on the connecting rod to

distribute the lubricant is one of the most successful and simplest

forms for simple four- and six-cylinder vertical automobile engines, but

is not as well adapted to the oiling of airplane power plants for

reasons previously stated. If too much oil is supplied the surplus will

work past the piston rings and into the combustion chamber, where it

will burn and cause carbon deposits. Too much oil will also cause an

engine to smoke and an excess of lubricating oil is usually manifested

by a bluish-white smoke issuing from the exhaust.

A good method of maintaining a constant level of oil for the successful

application of the splash system is shown at Fig. 78. The engine base

casting includes a separate chamber which serves as an oil container and

which is below the level of oil in the crank-case. The lubricant is

drawn from the sump or oil container by means of a positive oil pump

which discharges directly into the engine case. The level is maintained

by an overflow pipe which allows all excess lubricant to flow back into

the oil container at the bottom of the cylinder. Before passing into the

pump again the oil is strained or filtered by a screen of wire gauze and

all foreign matter removed. Owing to the rapid circulation of the oil it

may be used over and over again for quite a period of time. The oil is

introduced directly into the crank-case by a breather pipe and the level

is indicated by a rod carried by a float which rises when the container

is replenished and falls when the available supply diminishes. It will

be noted that with such system the only apparatus required besides the

oil tank which is cast integral with the bottom of the crank-case is a

suitable pump to maintain circulation of oil. This member is always

positively driven, either by means of shaft and universal coupling or

direct gearing. As the system is entirely automatic in action, it will

furnish a positive supply of oil at all desired points, and it cannot be

tampered with by the inexpert because no adjustments are provided or

needed.

DRY CRANK-CASE SYSTEM BEST FOR AIRPLANE ENGINES

[Illustration: Fig. 78.--Sectional View of Typical Motor Showing Parts

Needing Lubrication and Method of Applying Oil by Constant Level Splash

System. Note also Water Jacket and Spaces for Water Circulation.]

In most airplane power plants it is considered desirable to supply the

oil directly to the parts needing it by suitable leads instead of

depending solely upon the distributing action of scoops on the

connecting rod big ends. A system of this nature is shown at Fig. 77.

The oil is carried in the crank-case, as is common practice, but the

normal oil level is below the point where it will be reached by the

connecting rod. It is drawn from the crank-case by a plunger pump which

directs it to a manifold leading directly to conductors which supply the

main journals. After the oil has been used on these points it drains

back into the bottom of the crank-case. An excess is provided which is

supplied to the connecting rod ends by passages drilled into the webs of

the crank-shaft and part way into the crank-pins as shown by the dotted

lines. The oil which is present at the connecting rod crank-pins is

thrown off by centrifugal force and lubricates the cylinder walls and

other internal parts. Regulating screws are provided so that the amount

of oil supplied the different points may be regulated at will. A relief

check valve is installed to take care of excess lubricant and to allow

any oil that does not pass back into the pipe line to overflow or

bi-pass into the main container.

[Illustration: Fig. 79.--Pressure Feed Oil-Supply System of Airplane

Power Plants has Many Good Features.]

A simple system of this nature is shown graphically in a phantom view of

the crank-case at Fig. 79, in which the oil passages are made specially

prominent. The oil is taken from a reservoir at the bottom of the engine

base by the usual form of gear oil pump and is supplied to a main feed

manifold which extends the length of the crank-case. Individual

conductors lead to the five main bearings, which in turn supply the

crank-pins by passages drilled through the crank-shaft web. In this

power plant the connecting rods are hollow section bronze castings and

the passage through the center of the connecting rod serves to convey

the lubricant from the crank-pins to the wrist-pins. The cylinder walls

are oiled by the spray of lubricant thrown off the revolving crank-shaft

by centrifugal force. Oil projection by the dippers on the connecting

rod ends from constant level troughs is unequal upon the cylinder walls

of the two-cylinder blocks of an eight- or twelve-cylinder V engine.

This gives rise, on one side of the engine, to under-lubrication, and,

on the other side, to over-lubrication, as shown at Fig. 80, A. This

applies to all modifications of splash lubricating systems.

When a force-feed lubricating system is used, the oil, escaping past the

cheeks of both ends of the crank-pin bearings, is thrown off at a

tangent to the crank-pin circle in all directions, supplying the

cylinders on both sides with an equal quantity of oil, as at Fig. 80, B.

WHY COOLING SYSTEMS ARE NECESSARY

The reader should understand from preceding chapters that the power of

an internal-combustion motor is obtained by the rapid combustion and

consequent expansion of some inflammable gas. The operation in brief is

that when air or any other gas or vapor is heated, it will expand and

that if this gas is confined in a space which will not permit expansion,

pressure will be exerted against all sides of the containing chamber.

The more a gas is heated, the more pressure it will exert upon the walls

of the combustion chamber it confines. Pressure in a gas may be

created by increasing its temperature and inversely heat may be created

by pressure. When a gas is compressed its total volume is reduced and

the temperature is augmented.

[Illustration: Fig. 80.--Why Pressure Feed System is Best for

Eight-Cylinder Vee Airplane Engines.]

The efficiency of any form of heat engine is determined by the power

obtained from a certain fuel consumption. A definite amount of energy

will be liberated in the form of heat when a pound of any fuel is

burned. The efficiency of any heat engine is proportional to the power

developed from a definite quantity of fuel with the least loss of

thermal units. If the greater proportion of the heat units derived by

burning the explosive mixture could be utilized in doing useful work,

the efficiency of the gasoline engine would be greater than that of any

other form of energizing power. There is a great loss of heat from

various causes, among which can be cited the reduction of pressure

through cooling the motor and the loss of heat through the exhaust

valves when the burned gases are expelled from the cylinder.

The loss through the water jacket of the average automobile power plant

is over 50 per cent. of the total fuel efficiency. This means that more

than half of the heat units available for power are absorbed and

dissipated by the cooling water. Another 16 per cent. is lost through

the exhaust valve, and but 33-1/3 per cent. of the heat units do useful

work. The great loss of heat through the cooling systems cannot be

avoided, as some method must be provided to keep the temperature of the

engine within proper bounds. It is apparent that the rapid combustion

and continued series of explosions would soon heat the metal portions of

the engine to a red heat if some means were not taken to conduct much of

this heat away. The high temperature of the parts would burn the

lubricating oil, even that of the best quality, and the piston and rings

would expand to such a degree, especially when deprived of oil, that

they would seize in the cylinder. This would score the walls, and the

friction which ensued would tend to bind the parts so tightly that the

piston would stick, bearings would be burned out, the valves would warp,

and the engine would soon become inoperative.

[Illustration: Fig. 81.--Operating Temperatures of Automobile Engine

Parts Useful as a Guide to Understand Airplane Power Plant Heat.]

The best temperature to secure efficient operation is one on which

considerable difference of opinion exists among engineers. The fact that

the efficiency of an engine is dependent upon the ratio of heat

converted into useful work compared to that generated by the explosion

of the gas is an accepted fact. It is very important that the engine

should not get too hot, and on the other hand it is equally vital that

the cylinders be not robbed of too much heat. The object of cylinder

cooling is to keep the temperature of the cylinder below the danger

point, but at the same time to have it as high as possible to secure

maximum power from the gas burned. The usual operating temperatures of

an automobile engine are shown at Fig. 81, and this can be taken as an

approximation of the temperatures apt to exist in an airplane engine of

conventional design as well when at ground level or not very high in the

air. The newer very high compression airplane engines in which

compressions of eight or nine atmospheres are used, or about 125 pounds

per square inch, will run considerably hotter than the temperatures

indicated.

COOLING SYSTEMS GENERALLY APPLIED

There are two general systems of engine cooling in common use, that in

which water is heated by the absorption of heat from the engine and then

cooled by air, and the other method in which the air is directed onto

the cylinder and absorbs the heat directly instead of through the medium

of water. When the liquid is employed in cooling it is circulated

through jackets which surround the cylinder casting and the water may be

kept in motion by two methods. The one generally favored is to use a

positive circulating pump of some form which is driven by the engine to

keep the water in motion. The other system is to utilize a natural

principle that heated water is lighter than cold liquid and that it will

tend to rise to the top of the cylinder when it becomes heated to the

proper temperature and cooled water takes its place at the bottom of the

water jacket.

Air-cooling methods may be by radiation or convection. In the former

case the effective outer surface of the cylinder is increased by the

addition of flanges machined or cast thereon, and the air is depended on

to rise from the cylinder as heated and be replaced by cooler air. This,

of course, is found only on stationary engines. When a positive air

draught is directed against the cylinder by means of the propeller slip

stream in an airplane, cooling is by convection and radiation both.

Sometimes the air draught may be directed against the cylinder walls by

some form of jacket which confines it to the heated portions of the

cylinder.

COOLING BY POSITIVE WATER CIRCULATION

[Illustration: Fig. 82.--Water Cooling of Salmson Seven-Cylinder Radial

Airplane Engine.]

A typical water-cooling system in which a pump is depended upon to

promote circulation of the cooling liquid is shown at Figs. 82 and 83.

The radiator is carried at the front end of the fuselage in most cases,

and serves as a combined water tank and cooler, but in some cases it is

carried at the side of the engine, as in Fig. 84, or attached to the

central portion of the aerofoil or wing structure. It is composed of an

upper and lower portion joined together by a series of pipes which may

be round and provided with a series of fins to radiate the heat, or

which may be flat in order to have the water pass through in thin sheets

and cool it more easily. Cellular or honeycomb coolers are composed of a

large number of bent tubes which will expose a large area of surface to

the cooling influence of the air draught forced through the radiator

either by the forward movement of the vehicle or by some type of fan.

The cellular and flat tube types have almost entirely displaced the

flange tube radiators which were formerly popular because they cool the

water more effectively, and may be made lighter than the tubular

radiator could be for engines of the same capacity.

[Illustration: Fig. 83.--How Water Cooling System of Thomas Airplane

Engine is Installed in Fuselage.]

The water is drawn from the lower header of the radiator by the pump and

is forced through a manifold to the lower portion of the water jackets

of the cylinder. It becomes heated as it passes around the cylinder

walls and combustion chambers and the hot water passes out of the top of

the water jacket to the upper portion of the radiator. Here it is

divided in thin streams and directed against comparatively cool metal

which abstracts the heat from the water. As it becomes cooler it falls

to the bottom of the radiator because its weight increases as the

temperature becomes lower. By the time it reaches the lower tank of the

radiator it has been cooled sufficiently so that it may be again passed

around the cylinders of the motor. The popular form of circulating pump

is known as the "centrifugal type" because a rotary impeller of

paddle-wheel form throws water which it receives at a central point

toward the outside and thus causes it to maintain a definite rate of

circulation. The pump is always a separate appliance attached to the

engine and driven by positive gearing or direct-shaft connection. The

centrifugal pump is not as positive as the gear form, and some

manufacturers prefer the latter because of the positive pumping

features. They are very simple in form, consisting of a suitable cast

body in which a pair of spur pinions having large teeth are carried. One

of these gears is driven by suitable means, and as it turns the other

member they maintain a flow of water around the pump body. The pump

should always be installed in series with the water pipe which conveys

the cool liquid from the lower compartment of the radiator to the

coolest portion of the water jacket.

[Illustration: Fig. 84.--Finned Tube Radiators at the Side of Hall-Scott

Airplane Power Plant Installed in Standard Fuselage.]

WATER CIRCULATION BY NATURAL SYSTEM

Some automobile engineers contend that the rapid water circulation

obtained by using a pump may cool the cylinders too much, and that the

temperature of the engine may be reduced so much that the efficiency

will be lessened. For this reason there is a growing tendency to use the

natural method of water circulation as the cooling liquid is supplied to

the cylinder jackets just below the boiling point and the water issues

from the jacket at the top of the cylinder after it has absorbed

sufficient heat to raise it just about to the boiling point.

As the water becomes heated by contact with the hot cylinder and

combustion-chamber walls it rises to the top of the water jacket, flows

to the cooler, where enough of the heat is absorbed to cause it to

become sensibly greater in weight. As the water becomes cooler, it falls

to the bottom of the radiator and it is again supplied to the water

jacket. The circulation is entirely automatic and continues as long as

there is a difference in temperature between the liquid in the water

spaces of the engine and that in the cooler. The circulation becomes

brisker as the engine becomes hotter and thus the temperature of the

cylinders is kept more nearly to a fixed point. With the thermosyphon

system the cooling liquid is nearly always at its boiling point, whereas

if the circulation is maintained by a pump the engine will become cooler

at high speed and will heat up more at low speed.

With the thermosyphon, or natural system of cooling, more water must be

carried than with the pump-maintained circulation methods. The water

spaces around the cylinders should be larger, the inlet and discharge

water manifolds should have greater capacity, and be free from sharp

corners which might impede the flow. The radiator must also carry more

water than the form used in connection with the pump because of the

brisker pump circulation which maintains the engine temperature at a

lower point. Consideration of the above will show why the pump system is

almost universally used in connection with airplane power plant cooling.

DIRECT AIR-COOLING METHODS

The earliest known method of cooling the cylinder of gas-engines was by

means of a current of air passed through a jacket which confined it

close to the cylinder walls and was used by Daimler on his first

gas-engine. The gasoline engine of that time was not as efficient as the

later form, and other conditions which materialized made it desirable to

cool the engine by water. Even as gasoline engines became more and more

perfected there has always existed a prejudice against air cooling,

though many forms of engines have been used, both in automobile and

aircraft applications where the air-cooling method has proven to be very

practical.

The simplest system of air cooling is that in which the cylinders are

provided with a series of flanges which increase the effective radiating

surface of the cylinder and directing an air-current from a fan against

the flanges to absorb the heat. This increase in the available radiating

surface of an air-cooled cylinder is necessary because air does not

absorb heat as readily as water and therefore more surface must be

provided that the excess heat be absorbed sufficiently fast to prevent

distortion of the cylinders. Air-cooling systems are based on a law

formulated by Newton, which is: "The rate for cooling for a body in a

uniform current of air is directly proportional to the speed of the air

current and the amount of radiating surface exposed to the cooling

effect."

AIR-COOLED ENGINE DESIGN CONSIDERATIONS

[Illustration: Fig. 85.--Anzani Testing His Five-Cylinder Air Cooled

Aviation Motor Installed in Bleriot Monoplane. Note Exposure of Flanged

Cylinders to Propeller Slip Stream.]

There are certain considerations which must be taken into account in

designing an air-cooled engine, which are often overlooked in those

forms cooled by water. Large valves must be provided to insure rapid

expulsion of the flaming exhaust gas and also to admit promptly the

fresh cool mixture from the carburetor. The valves of air-cooled engines

are usually placed in the cylinder-head, in order to eliminate any

pockets or sharp passages which would impede the flow of gas or retain

some of the products of combustion and their heat. When high power is

desired multiple-cylinder engines should be used, as there is a certain

limit to the size of a successful air-cooled cylinder. Much better

results are secured from those having small cubical contents because the

heat from small quantities of gas will be more quickly carried off than

from greater amounts. All successful engines of the aviation type which

have been air-cooled have been of the multiple-cylinder type.

An air-cooled engine must be placed in the fuselage, as at Fig. 85, in

such a way that there will be a positive circulation of air around it

all the time that it is in operation. The air current may be produced by

the tractor screw at the front end of the motor, or by a suction or

blower fan attached to the crank-shaft as in the Renault engine or by

rotating the cylinders as in the Le Rhone and Gnome motors. Greater care

is required in lubrication of the air-cooled cylinders and only the best

quality of oil should be used to insure satisfactory oiling.

The combustion chambers must be proportioned so that distribution of

metal is as uniform as possible in order to prevent uneven expansion

during increase in temperature and uneven contraction when the cylinder

is cooled. It is essential that the inside walls of the combustion

chamber be as smooth as possible because any sharp angle or projection

may absorb sufficient heat to remain incandescent and cause trouble by

igniting the mixture before the proper time. The best grades of cast

iron or steel should be used in the cylinder and piston and the machine

work must be done very accurately so the piston will operate with

minimum friction in the cylinder. The cylinder bore should not exceed

4-1/2 or 5 inches and the compression pressure should never exceed 75

pounds absolute, or about five atmospheres, or serious overheating will

result.

As an example of the care taken in disposing of the exhaust gases in

order to obtain practical air-cooling, some cylinders are provided with

a series of auxiliary exhaust ports uncovered by the piston when it

reaches the end of its power stroke. The auxiliary exhaust ports open

just as soon as the full force of the explosion has been spent and a

portion of the flaming gases is discharged through the ports in the

bottom of the cylinder. Less of the exhaust gases remains to be

discharged through the regular exhaust member in the cylinder-head and

this will not heat the walls of the cylinder nearly as much as the

larger quantity of hot gas would. That the auxiliary exhaust port is of

considerable value is conceded by many designers of fixed and fan-shaped

air-cooled motors for airplanes.

Among the advantages stated for direct air cooling, the greatest is the

elimination of cooling water and its cooling auxiliaries, which is a

factor of some moment, as it permits considerable reduction in

horse-power-weight ratio of the engine, something very much to be

desired. In the temperate zone, where the majority of airplanes are

used, the weather conditions change in a very few months from the warm

summer to the extreme cold winter, and when water-cooled systems are

employed it is necessary to add some chemical substance to the water to

prevent it from freezing. The substances commonly employed are

glycerine, wood alcohol, or a saturated solution of calcium chloride.

Alcohol has the disadvantage in that it vaporizes readily and must be

often renewed. Glycerine affects the rubber hose, while the calcium

chloride solution crystallizes and deposits salt in the radiator and

water pipes.

One of the disadvantages of an air-cooling method, as stated by those

who do not favor this system, is that engines cooled by air cannot be

operated for extended periods under constant load or at very high speed

without heating up to such a point that premature ignition of the charge

may result. The water-cooling systems, at the other hand, maintain the

temperature of the engine more nearly constant than is possible with an

air-cooled motor, and an engine cooled by water can be operated under

conditions of inferior lubrication or poor mixture adjustment that would

seriously interfere with proper and efficient cooling by air.

Air-cooled motors, as a rule, use less fuel than water-cooled engines,

because the higher temperature of the cylinder does not permit of a full

charge of gas being inspired on the intake stroke. As special care is

needed in operating an air-cooled engine to obtain satisfactory results

and because of the greater difficulty which obtains in providing proper

lubrication and fuel mixtures which will not produce undue heating, the

air-cooled system has but few adherents at the present time, and

practically all airplanes, with but very few exceptions, are provided

with water-cooled power plants. Those fitted with air-cooled engines are

usually short-flight types where maximum lightness is desired in order

to obtain high speed and quick climb. The water-cooled engines are best

suited for airplanes intended for long flights. The Gnome, Le Rhone and

Clerget engines are thoroughly practical and have been widely used in

France and England. These are rotary radial cylinder types. The Anzani

is a fixed cylinder engine used on training machines, while the Renault

is a V-type engine made in eight- and twelve-cylinder V forms that has

been used on reconnaissance and bombing airplanes with success. These

types will be fully considered in proper sequence.

Aviation Engines: Design—Construction—Operation and Repair · 第 7 / 15 章