The Mechanics of Pumping Machinery a Text book for Technical Schools And a Guid
The Mechanics of Pumping Machinery a Text book for Technical Schools And a Guid
Julius Weisbach
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2 COS a Introducing in this equation the above value a= 102 34', at which the suction valve is entirely out of action, we get V = Fr(l+ 0-217 + 2-190) = 3'407Fr; that is, about 1/7 times as great as the cylinder volume 2Fr. Of course this increased discharge is accompanied by a corre- spondingly greater expenditure of work. The numerical values found for a and V in the preceding investigations are in reality modified by the influence of the frictional resistances of the water in the pipes, whic...h were neglected in the above discussion, as was also the hydraulic resistance due to the imparting of a velocity to the water originally at rest, and entering the suction pipe while the aforesaid upward motion through the delivery valve is taking place. In consequence of these resistances the motion of the water is not uniformly retarded, as was assumed. Neverthe- less, the above discussion explains the peculiar result, often observed in practice, that sometimes the actual discharge of a pump is greater than the theoretical discharge.
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