The hydraulic gradient plays a very important part in the construction
of a long pipe-line or conduit. If any part of the pipe should rise
above the hydraulic gradient, the discharge would no longer be full
below that point. It is necessary, therefore, always to lay the pipe or
the closed conduit so that all parts of it shall be below the hydraulic
gradient. Caution is obviously necessary to lay a pipe carrying water
deep enough below the surface of the ground in cold climates to protect
the water against freezing. At the same time if the pipe-line is a long
one it must follow the surface of the ground approximately in order to
save expensive cutting. There will, therefore, generally be summits
in pipe-lines, and inasmuch as all potable water carries some air
dissolved in it, that air is liable to accumulate at the high points or
summits. If that accumulation goes on long enough, it will seriously
trench upon the carrying capacity of the pipe and decrease its flow. It
is therefore necessary to provide at summits what are called blow-off
cocks to let the air escape. At the low points of the pipe-line, on the
contrary, the solid matter, such as sand and dirt, carried by the water
is liable to accumulate, and it is customary to arrange blow-offs also
at such points, so as to enable some of the water to escape and carry
with it the sand and dirt.
[Illustration: IN LOOSE EARTH.]
[Illustration: IN ROCK.
Weston Aqueduct. Sections of Aqueduct and Embankment.]
[Illustration: SECTION OF EMBANKMENT.]
[Illustration: ON EMBANKMENT.
Weston Aqueduct. Sections of Aqueduct and Embankment. Gradient, 1 in
5000.]
=189. Flow of Water in Large Masonry Conduits.=—In order to apply
Chezy’s formula first to the flow of the masonry aqueducts of the New
York and Boston water-supplies, it is necessary to have the outlines of
those conduits so that the wetted perimeter and hence the mean radius
may be determined for any depth of water in them.
[Illustration: OUTLINES OF AQUADUCTS.
FIG. 3.]
The figure shows the desired cross-sections drawn carefully to scale.
Table XIV has been computed and arranged from data taken from various
official sources so as to show the depth, mean velocity, discharge per
second and per twenty-four hours, and the coefficient used in Chezy’s
formula, together with the coefficient of roughness _n_ in Kutter’s
formula for the conduits shown in the figure.
This table exhibits in a concise and clear manner the use of Chezy’s
formula in this class of hydraulic work.
TABLE XIV.
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