A History of MechanicsRoutledge, 1955 - 671 стор. |
З цієї книги
Результати 1-3 із 51
Сторінка 329
... writes the condition for the equilibrium of a system , in continuous motion under the influence of the forces p , in ... write SMW2 SMV2 + SMU2 + 2 SMVU cos ( V , U ) = where W is the velocity before the impact and law ( 1 ) is applied ...
... writes the condition for the equilibrium of a system , in continuous motion under the influence of the forces p , in ... write SMW2 SMV2 + SMU2 + 2 SMVU cos ( V , U ) = where W is the velocity before the impact and law ( 1 ) is applied ...
Сторінка 579
... writes 1 xy - yx = ih 2π [ x , y ] . 2 ih 2л In the synthetic statement which he was to give later of quantum mechanics , Dirac omits the intermediaries ; he starts from the canon- ical equations of classical dynamics dq , dt = ән др ...
... writes 1 xy - yx = ih 2π [ x , y ] . 2 ih 2л In the synthetic statement which he was to give later of quantum mechanics , Dirac omits the intermediaries ; he starts from the canon- ical equations of classical dynamics dq , dt = ән др ...
Сторінка 585
... write for all k . W = hvik The second of the quantum equations of motion would be retrieved in the same way . As the partial differential equation ( 1 ) is nothing else than ... writes- " If , in a specific DEVELOPMENT OF THE PRINCIPLES 585.
... write for all k . W = hvik The second of the quantum equations of motion would be retrieved in the same way . As the partial differential equation ( 1 ) is nothing else than ... writes- " If , in a specific DEVELOPMENT OF THE PRINCIPLES 585.
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