A History of MechanicsRoutledge, 1955 - 671 стор. |
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Сторінка 468
... Lorentz , should be called the Voigt - Lorentz transformation . This all the more so as the conservation of the wave equation is one of the most remarkable of properties and is , moreover , directly related to the invariance of the ...
... Lorentz , should be called the Voigt - Lorentz transformation . This all the more so as the conservation of the wave equation is one of the most remarkable of properties and is , moreover , directly related to the invariance of the ...
Сторінка 489
René Dugas. Poincaré declared that Lorentz's hypothesis is " the only one com- patible with the impossibility of making absolute motion evident . " We must therefore " fall back on the theory of Lorentz , but if we wish to retain it and ...
René Dugas. Poincaré declared that Lorentz's hypothesis is " the only one com- patible with the impossibility of making absolute motion evident . " We must therefore " fall back on the theory of Lorentz , but if we wish to retain it and ...
Сторінка 647
... Lorentz's transformations form a continuous group , which he calls Lorentz's group , and from this he deduces that a certain parameter , introduced by Lorentz in the beginning of his analysis , is necessarily reduced to the unit . For ...
... Lorentz's transformations form a continuous group , which he calls Lorentz's group , and from this he deduces that a certain parameter , introduced by Lorentz in the beginning of his analysis , is necessarily reduced to the unit . For ...
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