A History of MechanicsRoutledge, 1955 - 671 стор. |
З цієї книги
Результати 1-3 із 63
Сторінка 396
... coordinates of the points of the system , and V is the function ( B ) = S2Tdt . V = S ' , Σm ( x'dx + y'dy + z'dz ) = S ′ 2Tdt . By considering the characteristic function V as a function of the initial and final coordinates and of the ...
... coordinates of the points of the system , and V is the function ( B ) = S2Tdt . V = S ' , Σm ( x'dx + y'dy + z'dz ) = S ′ 2Tdt . By considering the characteristic function V as a function of the initial and final coordinates and of the ...
Сторінка 442
... coordinates are functions of the coordinates which do not contain the initial values of the coordinates and components of velocity . 99 Kirchhoff writes the equations of motion d2x dt2 = X d2y dt2 d2z = Y = dt2 Ꮓ and considers the ...
... coordinates are functions of the coordinates which do not contain the initial values of the coordinates and components of velocity . 99 Kirchhoff writes the equations of motion d2x dt2 = X d2y dt2 d2z = Y = dt2 Ꮓ and considers the ...
Сторінка 504
... coordinates are directly measurable by means of an unit measuring - rod , and so that differences of time are direct- ly measurable by means of a standard clock . 99 Einstein remarks that every measurement is expressed by the ...
... coordinates are directly measurable by means of an unit measuring - rod , and so that differences of time are direct- ly measurable by means of a standard clock . 99 Einstein remarks that every measurement is expressed by the ...
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