A History of MechanicsRoutledge, 1955 - 671 стор. |
З цієї книги
Результати 1-3 із 35
Сторінка 542
... integral can be formed . The symbol Jk = { Prdqk , indicates that the variable q ranges over the whole domain of its ... integral S of Jacobi's partial differential equation . Let this solution be S = S ( q1 , 92 , qn , W , α1 , α2 ...
... integral can be formed . The symbol Jk = { Prdqk , indicates that the variable q ranges over the whole domain of its ... integral S of Jacobi's partial differential equation . Let this solution be S = S ( q1 , 92 , qn , W , α1 , α2 ...
Сторінка 569
... integral along the tra- jectory is equal to the total variation of the phase of this wave along the trajectory , taking 2л as the unit . 66 To write that the integral in question is a whole multiple of h amounts to the same as to write ...
... integral along the tra- jectory is equal to the total variation of the phase of this wave along the trajectory , taking 2л as the unit . 66 To write that the integral in question is a whole multiple of h amounts to the same as to write ...
Сторінка 619
... integral of the system , conservative or not , that is characterised by the hamilton- ian H , is written direcly as ( 3 ) ДА 2πί + де h [ AH — HA ] = 0 . This is obtained by analogy with the corresponding condition in ordinary mechanics ...
... integral of the system , conservative or not , that is characterised by the hamilton- ian H , is written direcly as ( 3 ) ДА 2πί + де h [ AH — HA ] = 0 . This is obtained by analogy with the corresponding condition in ordinary mechanics ...
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