The Steam Engine Familiarly Explained and Illustrated: With an historical sketch of its invention and progressive improvement; its applications to navigation and railways; with plain axioms for railway speculatorsLardner, Dionysius
History
The Steam Engine Familiarly Explained and Illustrated: With an historical sketch of its invention and progressive improvement; its applications to navigation and railways; with plain axioms for railway speculators
Lardner, Dionysius
Steam-engines -- Early works to 1850
Now since 7-1/2 pounds is very nearly the 300th part of a ton, it
follows that if an inclination upon a railroad rises at the rate of 1
foot in 300, or, what is the same, 17-1/2 feet in a mile, such an
acclivity will add 7-1/2 pounds per ton to the force of traction. This
acclivity therefore would require a force of traction twice as great
as a level. In like manner a rise of 35 feet in a mile would require
three times the force of traction of a level, 52-1/2 feet in a mile
four times that force, and so on. In fact, for every 7 feet in a mile
which an acclivity rises, 3 pounds per ton will be added to the force
of traction. If we would then ascertain the power necessary to pull a
load up any given acclivity upon a railroad, we must first take 7-1/2
pounds as the force necessary to overcome the common resistance of the
road, and then add 3 pounds for every 7 feet which the acclivity rises
per mile. For example, suppose an acclivity to rise at the rate of 70
feet in a mile, the force of traction necessary to draw a ton up it
would be thus calculated:--
Friction 7-1/2 lbs.
70 feet = 10 times 3 lbs. 30
------
Total force 37-1/2
It will be apparent, therefore, that if a railroad undulates by
inclined planes, even of the most moderate inclinations, the
propelling power to be used upon it must be of such a nature as to be
capable of increasing its intensity in a great degree, according to
the elevation of the planes which it has to encounter. A plane which
rises 52-1/2 feet per mile presents to the eye scarcely the appearance
of an ascent, and yet requires the power of traction to be increased
in a fourfold proportion.
It is the property of animal power, that within certain limits its
energy can be put forth at will, according to the exigency of the
occasion; but the intensity of mechanical power, in the instance now
considered, cannot so conveniently be varied, except indeed within
narrow limits.
In the application of locomotive engines upon railways the difficulty
arising from inclined planes has been attempted to be surmounted by
several methods, which we shall now explain.
1. Upon arriving at the foot of the plane the load is divided, and the
engine carries it up in several successive trips, descending the
plane unloaded after each trip. The objection to this method is the
delay which it occasions,--a circumstance which is incompatible with a
large transport of passengers. From what has been stated, it would be
necessary, when the engine is fully loaded on a level, to divide its
load into four parts, to be successively carried up when the incline
rises 52 feet per mile. This method has been practised in the
transport of merchandise occasionally, when heavy loads were carried
on the Liverpool and Manchester line, upon the Rainhill incline.
Public-domain text, read in full here on John Shaqi.
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