Water Lifted By Compressed Air
For Municipal, Manufacturing, Irrigation or Other Water Supply
År: 1905
Forlag: The Ingersoll-Sergeant Drill Company
Sted: New York
Udgave: 1
Sider: 96
UDK: 621.65-69
Catalog No 73
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So
tered the pressures per square inch of these
water columns or layers. Thus the pressure
per square inch of column 1 is seen to be 1.74
pounds; that of 2, consisting of two columns
or layers 1 and 2, each 4.02 feet long, to be
0.40 pounds, and that of 10, consisting of nine
columns or layers of water 1 to 9, inclusive,
4.02 feet long, and one of 3.80—viz., layer
10—feet in length to be 17.35 pounds, and the
aggregate length of the layers of waler is 39.08
teet in a total length of ninety-one feet of
pipe. It will be noted that the length of pipe
KK tle surface of the water in the well is
°0-o and that the difference between this
mnme. aggregate length of the water layers
wa.as) is 15.52 feet—that is, on equal areas
Pressure outside of the pipe is greater
~>nan A .e Pressure on the inside by the weight
due this difference of level, which is 47165
pounds for the end of the discharge-pipe. It
is this difference of 15.52 feet, acting as a
nead that supplies the water-pipe, puts the
contents of the pipe in motion, and overcomes
tne resistance m the pipe. In general the
water layers are equal each to each, and the
pressure upon any layer of air is due to the
number of water layers above it. Thus the
Pressure upon the bottom layer of air 10 in
the drawing's is due to all the layers of water
in the pipe, (17.35 pounds,) and the pressure
upon the uppermost layer of air 1 is due to
the single layer of water I at the moment ot
its discharges beginning—viz., 1.74 pounds
per square inch. As this discharge pro-
gresses this is lessened, until at the comple-
tion of the discharge of the water layer the
air layer Is of the same tension as the normal
atmosphere.
The quantitative relations of the air to wa-
ter are determinable, but vary with the rela-
tions of submergence to lift, diameter of pipe,
temperature, and atmospheric pressure, and
range from 1.5 to more volumes of normal air,
compressed to an adequate pressure, for each
volume of water raised by this process. The
best efficiency is attained when the submer-
sion is three-fifths of the total length of the
eduction-pipe. Whatever the submergence
or lift may be, in order to secure the desired
continuous upward flaw of the contents of the
eduction-pipe without stoppage or downward
dropping of the same it is necessary that th?
air as introduced into the pipe should be in
quantity sufficient to form, immediately upon
its issue from the air-pipe bubbles which will
expand across to fill the educt’on-pipe from
side to side and make distinct piston-like lay-
ers, entirely separating the portions of the
water column between which they enter said
pipe. Where the bubbles are smaller than
this, they will pass up through the water, and,
while necessarily elongating the water col-
umn, will not exert the. positive elevating
power that my pipe-filling air layers, entirely
dividing the layers of water from each other, do.
The enlargement at the lower end of the
eduction-pipe I have found to be of advan-
tage, not only as compensating for the spa.ee
taken up by the air-pipe, but, where the mouth
of the latter is well below the upper end ot
the enlargement, as facilitating the formation
of bubbles sufficisntly large to make the de-
sired pipe-fitting piston-like layers, rapidly
and continuously following each other at very
short intervals in the flow up the eduction-
pipe. When the body of water first standing
in the eduction-pipe has been forced up out
of the latter by the compressed gaseous fluid
used, the fluid pressure is preferably dimin-
ished, as indicated hereinbefore. In practice
I so reduce the pressure to a point below the
weight of the column of liquid which, stand-
ing m the eduction-pipe above the point of
entrance of the gaseous fluid, has been re-
moved, as stated.
ft evident that the process above de-
scribed is applicable to a.11 other liquids be-
sides water—such as petroleum-oil, saline so-
lutions. brewers’ and tanners’ liquors, sewage
&c. and therefore I do not limit tfie inven-
tion to the elevating- of water. Neither do I
confin® the invention to compressed air alone
for the purpose of raising liquids by this pro-
cess, but claim any aeriform body, such as nat-
ural gas and steam when used in oily liquids
What I claim as my invention, and desire
to secure by Letters Patent, is—
. 1- ,4s ,a» improvement in the art of elevat-
ing liquid, the process which consists In sub-
rnerging- a. portion of an open-ended educ-
tion-pipe in a body of the liquid to be raised
and continuously introducing- into the liauid
hiiblVips^f lower Part of the pipe a series ot
bubbles of compressed gaseous fluid contain-
ing enough of the fluid to expand immedi-
across the pipe and fill the same from
side to side, forming pipe-fitting piston-like
layers at or just above the point of their en-
trance into the pipe, whereby the column of
rlsingr m the pipe after the forcing' out
of ,il9ul,d f,JLst stand>ng in the latter is
subdivided by the g-aseous fluid into small
portions before it reaches the level of the h'l-
U!d ouMde -of the p‘Pe> and a continuously
upward-flowing- series of well-defined alter-
°C gaseous fluid and short layers
I’1!1111? )s formed and forced up the pine
fied y aS and fOr the PurPOse specl-
. 2- As an improvement in the art of elevat-
ing liquid, the process which consists in sub-
£ody of the liquid to1 be raised
a portion ot an open-ended eduction-pine
having an enlarged chamber on its lower end
and continuously injecting into such enlarge-
ment well below its upper end gaseous fluid
under pressure to form bubbles in the nip“
above the enlargement large enoug-h to ex-
tend across from side to side of the pips ironer
and form pipe-fitting piston-like layers there-
in interposed between and entirely senarat
mg well-defined layers of liquid in the pipe
substantially as and for the purpose de-
scribed. F 1
3. As an improvement in the art of elevat-
ing water or other liquid, the process which
consists, in .submerging a portion of an opeti-
ended pipe in a body of the liquid to be raised
removing the upper portion of the column of
JJqyid within the pipe and injecting into the
îuJÂÎS at a Point well below the level of the
liquid in which the pipe is submerged gase-
ous fluid in quantity sufficient to form bub-
bles, which will expand immediately acros«
the pipe and fill the same from side to side
and under pressure less than the weight ot
a column of liquid in the pipe extending from
the point of entrance of the fluid to
the level of the body of liquid surrounding
the pipe, so that a continuous upward-mov-
ing series of alternate well-defined easeous
fluid and liquid layers will be formed in ånd
forced up the pipe, substantially asi and for
the purpose described. y a lor
Signed at New York, in the county of New
of°October, AatD °189ieW Y°rk> this 23d day
Witnesses: JULTUS G' POHLE-
CHAS. C. GILL.
ED. D. MILLER.
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