20 × 80 = 1,600 kilogrammeters.

If we admit a product of 50 per cent., we shall have in the two cases,

for the power actually necessary:

600

---- = 1,200 kilogrammeters, or 16 H.P.

0.05

1,600

----- = 3,200 kilogrammeters, or 43 H.P.

0.05

Such are the limits within which the power of the motor should be able

to vary.

After successively examining all the different systems of engines now

in existence, and finding none which, in a plain form, was capable of

fulfilling the conditions imposed, Mr. E.D. Farcot decided to study

out one for himself. Almost from the very beginning of his researches

in this direction, he adopted the Woolf system, which is one that

permits of great variation in the expansion, and one in which the

steam under full pressure acts only upon the small piston. There are

many types of this engine in use, all of which present marked defects.

In one of them, the large cylinder is arranged directly over the small

one so as to have but a single rod for the two pistons; and the two

cylinders have then one bottom in common, which is furnished with a

stuffing-box in which the rod moves. With this arrangement we have but

a single connecting rod and a single crank for the shaft; but, the

stuffing-box not being accessible so that it can be kept in a clean

state, there occur after a time both leakages of steam and entrances

of air.

Mr. Farcot has further simplified this last named type by suppressing

the intermediate partition, and consequently the stuffing-box. The

engine thus becomes direct acting, that is to say, the steam acts

first upon the lower surface of the small piston during its ascent,

and afterward expands in the large cylinder and exerts its pressure

upon the upper surface of the large piston during its descent.

Moreover, the expansion may be begun in the small cylinder, thanks to

the use of a slide plate distributing valve, devised by the elder

Farcot and slightly modified by the son.

As the volume comprised between the two pistons varies with the

position of the latter, annoying counter-pressures might result

therefrom had not care been taken to put the chamber in communication

with a reservoir of ten times greater capacity, and which is formed by

the interior of the frame. This brings about an almost constant

counter-pressure.

The type of motor under consideration, which we represent in the

accompanying plate, is possessed of remarkable simplicity. The number

of parts is reduced to the extremest limits; it works at high speed

without perceptible wear; it does not require those frequent repairs

that many other cheap engines do; and the expansion of the steam is

utilized without occasioning violent shocks in the parts which

transmit motion. Finally, the plainness of the whole apparatus is

perfectly in accordance with the uses for which it was devised.

[Illustration: FARCOT'S IMPROVED WOOLF COMPOUND ENGINE.]

_Details of Construction._--Figs. 1 and 2 represent the motor in

vertical section made in the direction of two planes at right angles.

Figs. 3 and 4 are horizontal sections made respectively in the

direction of the lines 1-2 and 3-4.

The frame, which is of cast iron and entirely hollow, consists of two

uprights, B, connected at their upper part by a sort of cap, B¹, which

is cast in a piece with the two cylinders, C and _c_. The whole rests

upon a base, B², which is itself bolted to the masonry foundation.

Each of the uprights is provided internally with projecting pieces for

receiving the guides between which slides the cross-head, _g_, of the

piston rod. The slides terminate in two lubricating cups designed for

oiling the surfaces submitted to friction.

The cross-head carries two bearings, _g¹_, to which is jointed the

forked extremity, D, of the connecting rod, whose opposite extremity

receives a strap that embraces the cranked end of the driving shaft,

A. It will be remarked that the crank, A¹, and the bearings, _g¹_,

are very long. The end the inventor had in view in constructing them

thus was to diminish friction.

To the shaft, A, are keyed the coupling disks, Q, which are cast solid

at a portion of their circumference situated at 180° with respect to

the parts, A², of the cranked shaft, the object of this being to

balance the latter as well as a portion of the connecting rod, D.

The shaft, A, also receives the eccentric, E, of the slide valve, the

rod, _e_, of which is jointed to the slide valve rod through the

intermedium of a cross-head, _e¹_, analogous to that of the pistons,

and which, like the latter, runs on guides held by the support, b.

The two pistons, _p_ and P, are mounted very simply on the rod, T, as

shown in Fig. 1, and slide in cylinders, _c_ and C, whose diameters

are respectively equal to 270 and 470 millimeters.

The slide valve box, F, is bolted to the cap-piece, B¹, as seen in

Fig. 4. As for the slide valve, _t_, its arrangement may be

distinguished in section in Fig. 2. Its eccentric is keyed at 170° so

as to admit steam into the small cylinder during the entire travel,

which latter is 470 mm.

To permit of the expansion beginning in the small cylinder, Mr. Farcot

has added a sliding plate, _t¹_, which abuts at every stroke against

the stops, _s_. These latter are affixed to the rod, S, whose lower

extremity is threaded, and which may be moved vertically, as slightly

as may be desired, through the medium of the pinions, S¹, when the

hand-wheel, V, is revolved. A datum point, _v_, and a graduated

socket, _v¹_, allow the position of the stops, _s_, and consequently

the degree of expansion, to be known.

Steam is introduced into the small cylinder through the conduit, _i_,

and its passage into the large one is effected through the conduit,

_f_. The escape into the interior of the frame is effected, after

expansion, through the horizontal conduit, _h_. The pipe, H, leads

this exhaust steam to the open air.

The pipe, I, leads steam into the jacket, C¹, of the large cylinder,

this latter being provided in addition with a casing of wood, C², so

as to completely prevent chilling.

The regulator, R, is after the Büss pattern, and is set in motion by a

belt which runs over the pulleys, _a_ and _a¹_. It is mounted upon a

distributing box, R¹, to which steam is led from the boiler by the

pipe, _r¹_. After traversing this box, the steam enters the slide

valve box through the pipe, _r²_, its admission thereto being

regulated by the hand-wheel, R², which likewise serves for stopping

the engine.

The cocks, _x_, are fixed at the base of the uprights, B, for drawing

from the frame the condensed water that has accumulated therein.

The lubricating apparatus, V, which communicates, through the tube,

_u_, with the steam port, _r¹_, permits oil to be sent to the large

and small cylinders through the tubes, _u¹_ and _u²_.

Mr. Farcot has recently adapted this type of motor to the direct

running of electric machines that are required to make 400 revolutions

per minute.--_Publication Industrielle._

* * * * *

Scientific American Supplement, No. 388, June 9, 1883 · 第 13 / 79 题