A History of MechanicsRoutledge, 1955 - 671 стор. |
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Сторінка 27
... measure of the lengths DH and HK since it is a common measure of their halves . But A is to B as DC is to CE , so that A is to B as LH is to HK . Let A be as many times greater than Z as LH is greater than N. The length LH will be to ...
... measure of the lengths DH and HK since it is a common measure of their halves . But A is to B as DC is to CE , so that A is to B as LH is to HK . Let A be as many times greater than Z as LH is greater than N. The length LH will be to ...
Сторінка 236
... measure . This common measure is the time ; at least I can take the time or the times to be equal . . . . " Now given this , in the effects of a body which has twice as much velocity , I only find an effect which is double and not ...
... measure . This common measure is the time ; at least I can take the time or the times to be equal . . . . " Now given this , in the effects of a body which has twice as much velocity , I only find an effect which is double and not ...
Сторінка 628
... Measure P1 . After the measurement the state of the system I reduces to an eigenstate of the quantity P1 . The state of the system II is also specified . b ) Measure q1 instead of measuring P1 . After this measurement the state of the ...
... Measure P1 . After the measurement the state of the system I reduces to an eigenstate of the quantity P1 . The state of the system II is also specified . b ) Measure q1 instead of measuring P1 . After this measurement the state of 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