Practical Hand Book of Gas, Oil and Steam Engines: Stationary, Marine, Traction; Gas Burners, Oil Burners, Etc.; Farm, Traction, Automobile, Locomotive; A simple, practical and comprehensive book on the construction, operation and repair of all kinds of engines. Dealing with the various parts in detail and the various types of engines and also the use of different kinds of fuel.Rathbun, John B.
Science
Practical Hand Book of Gas, Oil and Steam Engines: Stationary, Marine, Traction; Gas Burners, Oil Burners, Etc.; Farm, Traction, Automobile, Locomotive; A simple, practical and comprehensive book on the construction, operation and repair of all kinds of engines. Dealing with the various parts in detail and the various types of engines and also the use of different kinds of fuel.
Rathbun, John B.
Internal combustion engines; Traction-engines
It should be remembered that heat is absorbed in evaporating gasoline as
well as in evaporating water, and that effects of cold weather are
greatly increased by the amount of heat absorbed, (or cold produced) by
the vaporization of the fuel. While the heat absorbed by evaporating a
given quantity of gasoline is only .45 per cent of that absorbed by an
equal amount of water, it is a fact that this heat must be supplied from
some source to prevent a reduction in the vapor density. In starting the
engine, the heat of evaporation is supplied by the atmosphere, and
should the temperature of the air be below that required for a given
vapor density, the engine will refuse to start.
By the use of two tanks and a three way valve, it is possible to use two
grades of fuel: one tank containing high gravity gasoline, and the other
low gravity; the high gravity being used for starting the engine in cold
weather, and the cheaper, low gravity, being used for continuous running
after the engine is warmed up—the change of fuels being made by throwing
over the three way valve.
The =VAPOR DENSITY= of gasoline vapor is the ratio of the weight of the
vapor compared with the weight of an equal volume of dry air at the same
temperature. If the weight of a cubic foot of gasoline vapor is divided
by the weight of a cubic foot of air at the same temperature the result
will be the vapor density of the gasoline vapor. Compared to air, the
gasoline vapor is quite heavy so that if a small quantity of gasoline is
poured on the top of a table, the vapor will flow over the edge of the
table and drop to the floor where it will remain until it has united
with the air by the process of diffusion. Experiments have shown that
pure, dry gasoline vapor has a density of about 3.28, or in other words
weighs 3.28 times as much as an equal volume of dry air. This weight of
course is the weight of pure vapor which is considerably heavier than
the mixture of vapor and air that is used in the cylinder of the engine.
Dampness, or the presence of water vapor in the air reduces the quantity
of gasoline vapor taken up by the air, but only by a small amount, the
maximum difference being only about 2 per cent. Since it is very likely
that the water vapor is broken up into its original elements, oxygen and
hydrogen, by the heat of the combustion it is likely that there is no
heat loss due to the vapor passing out through the exhaust. The
principal trouble due to dampness is the mixture of water and liquid
gasoline caused by the condensation of the water vapor.
All gasolines and oils contain water to a more or less degree, hence
provision should be made for the draining of the water which collects in
the bottom of the tank. Water in liquid fuels is the cause of much
trouble.
Water in gasoline may be detected by dropping scrapings from an
indelible pencil into a sample of the suspected fluid. If water is
present in any quantity the gasoline will assume a violet color.
Public-domain text, read in full here on John Shaqi.
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