A History of MechanicsRoutledge & Paul, 1957 - 671 стор. |
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Сторінка 336
... equations.2 Lagrange expressed the constraints of the system by equations of the type L = 0 M = 0 N = 0 ... where L , M , N are finite functions of the coordinates of the points of the system . Differentiating these conditions ...
... equations.2 Lagrange expressed the constraints of the system by equations of the type L = 0 M = 0 N = 0 ... where L , M , N are finite functions of the coordinates of the points of the system . Differentiating these conditions ...
Сторінка 397
... equations must be satisfied identically by V. Hamilton verifies that , by differentiating equations ( C ) and taking account of ( F ) , there are retrieved the ordinary equations of motion m1x1 = au дх1 etc .... If the rectangular ...
... equations must be satisfied identically by V. Hamilton verifies that , by differentiating equations ( C ) and taking account of ( F ) , there are retrieved the ordinary equations of motion m1x1 = au дх1 etc .... If the rectangular ...
Сторінка 468
... equations ( E ' ) only imper- fectly achieved the end that he had set himself , and which Einstein was to accomplish - in fact there remains , in the equations ( E ' ) , a vu term which Lorentz did not succeed in removing . c2 The equations ...
... equations ( E ' ) only imper- fectly achieved the end that he had set himself , and which Einstein was to accomplish - in fact there remains , in the equations ( E ' ) , a vu term which Lorentz did not succeed in removing . c2 The equations ...
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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Загальні терміни та фрази
acceleration Albert of Saxony Archimedes Aristotle assumed axis Bernoulli Blasius of Parma Carnot centre of gravity classical mechanics concept conservation considered coordinates d'Alembert Daniel Bernoulli deduced Descartes differential direction displacement distance Duhem dynamics Earth Einstein elastic electron energy equal equations equilibrium Euler experiment fall Fermat fluid function Galileo generalised given heavy body Huyghens hypothesis impact impetus inclined plane inertia instant Jean Bernoulli Kepler Lagrange least action Leibniz length Leonardo lever living forces Louis de Broglie mass Maupertuis means moving body natural necessary Newton observation obtained Oresme oscillation particle pendulum physical problem projectile proportional Proposition quantity of motion quantum mechanics ratio relation relative resistance rest Roberval rotation solution space sphere statics supposed surface theory trajectory travelled treatise uniformly variables velocity vertical wave weight XIIIth Century ди ду дх