A History of MechanicsRoutledge & Paul, 1957 - 671 стор. |
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Результати 1-3 із 42
Сторінка 336
... differentials that are not 66 exact differences " -these are the constraints that are now called non - holonomic ... differential are equated to zero , which will give as many particular equations as there are differentials ; and if ...
... differentials that are not 66 exact differences " -these are the constraints that are now called non - holonomic ... differential are equated to zero , which will give as many particular equations as there are differentials ; and if ...
Сторінка 609
... differential equations - by a continuous field of phenomena in configuration space , governed by one partial differential equation which arises from a variation principle . This variation principle , or this partial differential ...
... differential equations - by a continuous field of phenomena in configuration space , governed by one partial differential equation which arises from a variation principle . This variation principle , or this partial differential ...
Сторінка 637
... differentials appeared , with Clairaut , in hydrostatics and partial differential equations , with Euler and d'Alembert , in hydrodynamics . By the time of Lagrange the mathematical tools were highly perfected and became an essential ...
... differentials appeared , with Clairaut , in hydrostatics and partial differential equations , with Euler and d'Alembert , in hydrodynamics . By the time of Lagrange the mathematical tools were highly perfected and became an essential ...
Зміст
Nicholas Copernicus 14721543 His system of the world | 5 |
The priority of Herman and Euler in the matter of dAlemberts | 6 |
Transformation of Maxwells equations including convection | 11 |
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able acceleration according action appears applied assumed become body called carried cause centre of gravity Century classical complete concept concerned condition connection considered constant continuous corresponding Descartes determined direction distance dynamics Earth effect energy equal equations equilibrium Euler example existence experiment expressed fact fall field fluid function Galileo given hand Huyghens hypothesis ideas impact impetus inclined increases Lagrange length lever light living forces mass matter means measure mechanics motion moving natural necessary observation obtained original particle physical plane position possible principle problem produced proportional Proposition quantity quantum quantum mechanics reference relation relative remains remarked represented resistance respect rest result sense shows simple solution space special relativity starts statics supposed surface taken theory travelled true velocity wave weight World writes