In science, the mechanical theory, according to 1824 views of French physicist Sadi Carnot, explains the operation of machines which have for a motor the force of men (manpower) or of animals (horsepower), a waterfall (waterpower), an air current (windpower), etc., but not those which receive their motion form heat. [1] In general, the "mechanical theory" is a term that refers to a geometric physics of, pre heat engine period, machines, those such as screw presses, pulleys, water wheels, wind mills, etc., defined by fundamental principles and limits of operation owing to the geometry of movement of the parts and the laws of force.
History
The works of French engineer Lazare Carnot embody the logic of the mechanical theory to a large extent. [2] In particular, Lazare Carnot’s 1778 “Memoir on the Theory of Machines”, written fresh out of engineering school, submitted to the French Academy of Sciences in Paris, in efforts to win their coveted prize contest to formulate a general mechanical theory, acts as a good point representative of the birth of the mechanical theory. Specifically, in an advertisement in the Gazette de France of 18 April 1777, the Academy specified that this machine theory or subject needed to be: [3]
“The theory of simple machines with regard to friction and the stiffness of cordage, [requiring] that the laws of friction and the examination of the effects resulting from stiffness in cordage be determined by new experiments conducted on a large scale; [requiring] further that these experiments be applicable to machines used in the Navy such as the pulley, the capstan, and the inclined plane.”
Mechanical theory of heat (1865) = mechanical theory (1778) + mechanical equivalent of heat (1798) + theory of heat (1837)