The Pneumatic Despatch Tube System of the Batcheller Pneumatic Tube Co.: Also, Facts and General Information Relating to Pneumatic Despatch TubesBatcheller, Birney C. (Birney Clark)
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The Pneumatic Despatch Tube System of the Batcheller Pneumatic Tube Co.: Also, Facts and General Information Relating to Pneumatic Despatch Tubes
Batcheller, Birney C. (Birney Clark)
Pneumatic-tube transportation
=Law of Velocity.=—Next let us see what the velocity of the air is
in the tube. Suppose that we have some convenient means of measuring
the velocity of the air at any point, in feet per second or miles
per hour, with some form of anemometer. We will have our measurements
taken at the five points where we measured the pressure,—viz., at the
tank, one-quarter, one-half, three-quarters and one mile from the
tank. We will represent the velocities by a diagram similar to the
one used for pressures. At the tank we find the air entering the tube
with a velocity of 59.5 feet per second (40.6 miles per hour). We draw
the vertical line M N, to represent this. At the quarter mile point
the velocity is sixty-five feet per second (44.4 miles per hour) an
increase in the first quarter of a mile of 5.5 feet per second. We
construct the vertical line O P. At the half-mile point the velocity is
72.4 feet per second (49.4 miles per hour); at the three-quarter mile
point it is eighty-three feet per second (56.8 miles per hour); and at
the end of the tube, one mile from the tank, the air comes out of the
tube with a velocity of 100.4 feet per second (68.5 miles per hour),
about 1.7 times faster than it entered the tube at the tank. Drawing
all the vertical lines to represent these velocities, and drawing a
smooth curve line through the tops of our vertical lines, we have the
curve of velocities, N, P, R, T, V, for all points along the tube. It
is an increasing velocity and increases more rapidly as we approach the
end of the tube. This is shown more clearly by drawing the straight
dashed line N V.
If the fluid flowing in the tube were inelastic, like water, then the
curve of velocities would be a straight horizontal line, for the water
would not come out of the tube any faster than it went in. But we are
dealing with air, which is an elastic fluid, and, as we stated before,
it expands as the pressure is reduced and becomes larger in volume.
It is this expansion that increases its velocity as it flows along the
tube. It must go faster and faster to make room to expand. Since the
same actual quantity of air in pounds must come out of the tube each
minute as enters the tube at the other end in the same time, to prevent
an accumulation of air in the tube, and since it increases in volume as
it flows through the tube, it follows that its velocity must increase.
Public-domain text, read in full here on John Shaqi.
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