 | Elijah Galloway - Steam-engines - 1829 - 890 pages
...velocity in feet, per second, by 4.01, and the square of the quotient by the diameter of iht circle; the quotient is the centrifugal force when the weight of the body is 1. Hence the quotient, multiplied by the weight of the body, is the centrifugal force. /.j«".-;./-. Required... | |
 | Luke Hebert - Industrial arts - 1835 - 816 pages
...velocity in feet per second by 4.01, and the square of the quotient by the diameter of the circle; the quotient is the centrifugal force when the weight of the body is 1. Hence the quotient, multiplied by the weight of the body, is the centrifugal force required. — Ex.... | |
 | Luke Hebert - Industrial arts - 1836 - 814 pages
...velocity in feet per second by 4.01, and the square of the quotient by the diameter of the circle ; the quotient is the centrifugal force when the weight of the body is 1. Hence the quotient, multiplied by the weight of the body, is the centrifugal force required. — Ex.... | |
 | Charles Haynes Haswell - Engineering - 1844 - 298 pages
...minute by the diameter of the circle in feet, and divide the product by the constant number 5870 ; the quotient is the centrifugal force when the weight of the body is 1. Then, as in the previous rule, this quotient, multiplied by the weight of the body, is the centrifugal... | |
 | J. M. Scribner - Mechanical engineering - 1849 - 286 pages
...minute by the diameter of the circle in feet, and divide the product by the constant number 5870 ; the quotient is the centrifugal force when the weight of the body is 1. Hence, as in the 1st rule, the quotient multiplied by the weight of the body, is the centrifugal force.... | |
 | Charles Haynes Haswell - Engineering - 1851 - 346 pages
...minute by the diameter of the circle in feet, and divide the product by the constant number 5870 ; the quotient is the centrifugal force when the weight of the body is 1. Then, as in the previous rule, this quotient, multiplied by the weight of the body, is the centrifugal... | |
 | John Arthur Phillips, John Darlington - Metallurgy - 1857 - 350 pages
...velocity in feet per second by 4 • 01, and the square of the quotient by the diameter of the circle : the quotient is the centrifugal force when the weight of the body is one. Hence, the quotient multiplied by the weight of the body is the centrifugal force. jEx. — Eequired... | |
 | John Bourne (C. E.) - Steam engineering - 1868 - 602 pages
...height in feet due to the velocity. Divide this quadruple height by the diameter of the circle, and the quotient is the centrifugal force when the weight of the body is 1 ; consequently, multiplying it by the weight of the body, gives the actual centrifugal force in pounds... | |
 | John Bourne - Steam-engines - 1873 - 510 pages
...height in feet due to the velocity. Divide this quadrupled height ly the diameter of the circle, and the quotient is the centrifugal force when the weight of the body is 1 ; consequently, multiplying it ly the weight of the lady gives the actual centrifugal force in pounds... | |
 | Herbert Ashton Megraw - Cyanide process - 1910 - 112 pages
...of revolutions per minute by the diameter of the circle in feet and divide the product by 5217. This is the centrifugal force when the weight of the body is 1. This figure multiplied by the weight of the body is the centrifugal force required. The weight of 1... | |
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... the quotient is the centrifugal force when the weight of the body is 1. 