The Mathematical Principles of Natural Philosophy, Volume 1Isaac Newton's The Mathematical Principles of Natural Philosophy translated by Andrew Motte and published in two volumes in 1729 remains the first and only translation of Newton's Philosophia naturalis principia mathematica, which was first published in London in 1687. As the most famous work in the history of the physical sciences there is little need to summarize the contents.J. Norman, 2006. 
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Recensione dell'utente  donbuch1  LibraryThingThis classic series represents the Western canon not without academic controversy. The latest volumes of the Great Books include some women writers, but they are still definitely underrepresented ... Leggi recensione completa
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Recensione dell'utente  rylltraka  LibraryThingThe texts themselves are priceless, but the translations in this volume are seriously dated and often obscure the meaning of the Greek  especially worthy of disdain are the Aristophanes translations ... Leggi recensione completa
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The Mathematical Principles of Natural Philosophy, Volume 2 Sir Isaac Newton Visualizzazione completa  1729 
The Mathematical Principles of Natural Philosophy, Volume 3 Sir Isaac Newton,William Davis Visualizzazione completa  1803 
The Mathematical Principles of Natural Philosophy: In Three Volumes, Volume 3 Isaac Newton Visualizzazione completa  1803 
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ABFD accelerative forces altitude angle VCP apsides attracting body axis bisected body revolving centre of force centre of gravity centripetal force circle common centre conic section corpuscle curve line curvilinear cycloid decrease descend described diameter diminished distance draw drawn duplicate ratio Earth ellipsis evanescent fame ratio fame thing figure focus given by position given points given ratio globe greater Hence hyperbola immoveable infinitum inversely latus rectum Lemma let fall meeting motion move nodes orbit ordinate parabola parallel parallelogram particles perpendicular plane principal axe principal vertex Problem prop Proposition quadratures quantity radius ratio compounded rectangle rectilinear right lines given Scholium scribe similar triangles sine space sphærical sphere square subducted subduplicate ratio superficies suppose syzygies tangent thence Theorem thofe touch trajectory trapezium triangles upper apsis velocity Wherefore whofe whole
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Pagina 9  Absolute, true, and mathematical time, of itself, and from its own nature, flows equably without relation to anything external, and by another name is called duration: relative, apparent, and common time, is some sensible and external (whether accurate or unequable) measure of duration by the means of motion, which is commonly used instead of true time; such as an hour, a day, a month, a year.
Pagina 66  From the same demonstration it likewise follows that the arc which a body, uniformly revolving in a circle by means of a given centripetal force, describes in any time is a mean proportional between the diameter of the circle and the space which the same body falling by the same given force would descend through in the same given time.
Pagina 36  ... of a hammer) is (as far as I can perceive) certain and determined, and makes the bodies to return one from the other with a relative velocity, which is in a given ratio to that relative velocity with which they met.
Pagina 19  The change of motion is proportional to the motive force impressed; and is made in the direction of the right line in which that force is impressed.
Pagina 41  QUANTITIES, AND THE RATIOS OF QUANTITIES, WHICH IN ANY FINITE TIME CONVERGE CONTINUALLY TO EQUALITY, AND BEFORE THE END OF THAT TIME APPROACH NEARER THE ONE TO THE OTHER THAN BY ANY GIVEN DIFFERENCE, BECOME ULTIMATELY EQUAL.
Pagina 20  If a body impinge upon another, and by its force change the motion of the other, that body also (because of the equality of the mutual pressure) will undergo an equal change, in its own motion, towards the contrary part.
Pagina 15  The effects which distinguish absolute from relative motion are the forces of receding from the axis of circular motion. For there are no such forces in a circular motion purely relative, but in a true and absolute circular motion they are greater or less, according to the quantity of the motion.
Pagina 3  This force consists in the action only, and remains no longer in the body when the action is over. For a body maintains every new state it acquires, by its inertia only. But impressed forces are of different origins, as from percussion, from pressure, from centripetal force.