Load (physics)

Definition and stakes

Frederick William Lanchester,  Aerodynamics, constituting the first volume of a complete work on aerial flight… (1906)

“ Therefore, adopting a method of expression common in mathematical work (but not so frequently employed in direct physical demonstration) , we may say that if we take as hypothesis a small finite load, so that the actual motions of the fluid be small finite quantities, the expenditure of energy in sustaining the load will be zero, neglecting small quantities of the second order. ”
Source: Wikisource

Portrait of Robert S. Ball Robert S. Ball,  Experimental Mechanics

“ When the power arm is longer than the load arm, the load is greater than the power; but when the power arm is shorter than the load arm, the power is greater than the load.
We may regard the strain on the balance as a power which supports the weight, just as we regard the weight to be a power producing the strain on the balance. We see, then, that for the lever of the first order to be efficient as a mechanical power it is necessary that the power arm be longer than the load arm.
”
Source: Gutenberg

Portrait of Robert S. Ball Robert S. Ball,  Experimental Mechanics

“ We can ascertain the loss by computing the percentage of applied [Pg 159] energy which is utilized. Let us suppose a weight of 100 lbs. has to be raised one foot: for this purpose a force of 100 ÷ 5·54 = 18·1 lbs. must be applied. This is evident from the definition of the mechanical efficiency; but since the load has to be raised one foot, it is clear from the meaning of the velocity ratio that the power must move over 5'·94: hence the number of units of work to be applied is to be measured by the product of 5·94 and 18·1, that is, by 107·5 ”
Source: Gutenberg

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