Scientific American Supplement, No. 275, April 9, 1881Various
Science
Scientific American Supplement, No. 275, April 9, 1881
Various
Science -- Periodicals
h being the difference of level between the two ends of the portion of
conduit of length, L, and the sign + or - being used according as the
conduit rises or falls. The specific weight, [delta], is constant, and the
quotients, p1/[delta] and p/[delta], represent the heights, z and z1, to
which the water could rise above the pipes, in vertical tubes branching
from it, at the beginning and end of the transit. The values assigned to
the coefficient b1 in France, are those determined by D'Arcy. For new
cast-iron pipes he gives b1 - 0.0002535 + 1/D 0.000000647; and recommends
that this value should be doubled, to allow for the rust and incrustation
which more or less form inside the pipes during use. The determination of
this coefficient has been made from experiments where the pressure has
not exceeded four atmospheres; within these limits the value of the
coefficient, as is generally admitted, is independent of the pressure. The
experiments made by M. Barret, on the pressure pipes of the accumulator at
the Marseilles docks, seem to indicate that the loss of pressure would be
greater for high pressures, everything else being equal. This pipe, having
a diameter of 0.127 m. (5 in.), was subjected to an initial pressure of 52
atmospheres. The author gives below the results obtained for a straight
length 320 m. (1050 ft) long; and has placed beside them the results which
D'Arcy's formula would give.
Loss of head, in meters or ft. respectively
per 100 meters or ft. run of pipes.
+-----------------^-------------------+
| |
Calculated loss.
+-----------^-----------+
| |
Velocity of flow Actual loss
per second. observed. Old pipes. New pipes.
Meters. Feet. Met. or Ft. Met. or Ft. Met. or Ft.
0.25 0.82 1.5 0.12 0.06
0.50 1.64 2.5 0.48 0.24
0.75 2.46 3.7 1.08 0.54
1.00 3.28 5.5 1.92 0.96
1.25 4.10 6.1 3.00 1.50
1.50 4.92 7.3 4.32 2.16
1.75 5.74 8.0 5.88 2.94
2.00 6.56 10.2 7.68 3.84
2.25 7.38 11.7 9.72 4.86
2.50 8.20 14.0 12.00 6.00
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