Scientific American Supplement, No. 799, April 25, 1891 by Various
page 63 of 124 (50%)
page 63 of 124 (50%)
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in which A equals the area of blade in square feet, V and v velocities
of current and wheel periphery respectively, in feet per second. Thus, for example, a wheel 10 feet in diameter with blades 6 feet long and 1 foot in width, running in a stream of 5 feet per second--assuming the wheel to be giving as much power as will reduce its velocity to one half that of the stream--the figures will be 6' × 5' 2 ------- × 2.5 = 0.468 400 [TEX: \frac{6' \times 5'}{400} \times 2.5^2 = 0.468] horse power of the wheel. The total power of the stream due to the area of the blade equals the Square of the velocity of the stream ------------------------------------ × Twice gravity (64.33) volume of water in cubic feet per second × 62.5 (weight of 1 C') = the value or gross effect in pounds falling 1 foot per second. This sum divided by 550 = horse power. Thus, as per last example, 2 5 ------ × 30 × 62.5 64.33 ---------------------- = 1.32 the horse power of the current |
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