Hydraulic Tables; The Elements Of Gagings And The Friction Of Water Flowing In Pipes, Aqueducts, Sewers, Etc., As Determined By The Hazen And Williams Formula And The Flow Of Water Over The Sharp-Edged And Irregular Weirs, And The Quantity Discharged
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Hydraulic Tables; The Elements Of Gagings And The Friction Of Water Flowing In Pipes, Aqueducts, Sewers, Etc., As Determined By The Hazen And Williams Formula And The Flow Of Water Over The Sharp-Edged And Irregular Weirs, And The Quantity Discharged - Gardner Stewart Williams
INTRODUCTION.
THE following tables show the flow of water in pipes and other passages, as computed by the Hazen-Williams hydraulic slide-rule, based upon the formula
The most commonly used formula for determining the velocity of flow of water in pipes and channels is the Chezy formula, namely
where v is the velocity in feet per second, s is the hydraulic slope, and r the hydraulic radius in feet. c is a factor the value of which is an approximation to a constant, but depends upon the roughness of the pipe and upon the hydraulic radius and slope. The variations in the value of c are considerable, and make the general use of the formula difficult.
Kutter’s formula was devised to compute the value of c in the Chezy formula. The value of c so computed depends upon an assumed coefficient of roughness, upon the slope, and upon the hydraulic radius. With the same degree of roughness the value of c increases with the hydraulic slope and with the hydraulic radius. This is because the exponents used for these terms in the formula are below the true values. If the exponents were increased to correspond more nearly with the facts, the variations in the value of c would become less. If exponents could be selected agreeing perfectly with the facts, the value of c would depend upon the roughness only, and for any given degree of roughness c would then be a constant. It is not possible to reach this actually, because the values of the exponents vary with different surfaces, and also their values may not be exactly the same for large diameters and for small ones, nor for steep slopes and for flat ones. Exponents can be selected, however, representing approximately average conditions, so that the value of c for a given condition of surface will vary so little as to be practically constant. Several such exponential
formulas have been suggested. These formulas are among the most satisfactory yet devised, but their use has been limited by the difficulty in making computations by them. This difficulty was eliminated by the use of a slide-rule constructed for that