Elements of Natural Philosophy, Deel 1University Press, 1872 - 279 pagina's |
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Pagina 2
... position to another it must evidently describe a continuous line , which may be curved or straight , or even made up of portions of curved and straight lines meeting each other at any angles . If the motion be that of a material ...
... position to another it must evidently describe a continuous line , which may be curved or straight , or even made up of portions of curved and straight lines meeting each other at any angles . If the motion be that of a material ...
Pagina 2
... position to another it must evidently describe a continuous line , which may be curved or straight , or even made up of portions of curved and straight lines meeting each other at any angles . If the motion be that of a material ...
... position to another it must evidently describe a continuous line , which may be curved or straight , or even made up of portions of curved and straight lines meeting each other at any angles . If the motion be that of a material ...
Pagina 3
... positions of it contain the second side of the polygon above men- tioned , it is evident that the osculating plane passes from one position : to the next by revolving about the tangent to the curve . 13. Thus , as we proceed along such ...
... positions of it contain the second side of the polygon above men- tioned , it is evident that the osculating plane passes from one position : to the next by revolving about the tangent to the curve . 13. Thus , as we proceed along such ...
Pagina 6
... position , is called its Velocity . It is greater or less as the space passed over in a given time is greater or less : and it may be uniform , i.e. the same at every instant ; or it may be variable . Uniform velocity is measured by the ...
... position , is called its Velocity . It is greater or less as the space passed over in a given time is greater or less : and it may be uniform , i.e. the same at every instant ; or it may be variable . Uniform velocity is measured by the ...
Pagina 10
... point we have given the whole velocity and its direction , or simply the components of the velocity in three rectangular directions , at any time , or , as is most commonly • the case , for any position ; the determination JO PRELIMINARY .
... point we have given the whole velocity and its direction , or simply the components of the velocity in three rectangular directions , at any time , or , as is most commonly • the case , for any position ; the determination JO PRELIMINARY .
Overige edities - Alles bekijken
Elements of Natural Philosophy, Deel 1 William Thomson Baron Kelvin,Peter Guthrie Tait Volledige weergave - 1885 |
Elements of Natural Philosophy, Volume 1 William Thomson Baron Kelvin,Peter Guthrie Tait Volledige weergave - 1873 |
Elements of Natural Philosophy, Volume 1 William Thomson Baron Kelvin,Peter Guthrie Tait Volledige weergave - 1873 |
Veelvoorkomende woorden en zinsdelen
acceleration action amount angular velocity anticlastic attraction axis called Cambridge centre of gravity centre of inertia circle circular co-ordinates component configuration consider constant cosine couple curvature curve cylinder denote density described diagram displacement distance ellipsoid elongation equal equations equilibrium external finite fixed point flexure fluid forces acting friction geometrical given force Hence hodograph horizontal infinitely small instant inversely kinetic energy length magnitude mass matter measured moment of inertia momentum moving normal section Octavo P. G. TAIT P₁ P₂ parallel particle path pendulum perpendicular plane perpendicular portion position potential pressure principal axes principle produce projection proportional quantity radius radius of gyration reckoned rectangular resultant right angles rigid body rotation round shear shell sides simple harmonic motion solid angle space spherical surface spiral square straight line strain stress suppose tangent theorem theory tion torsion uniform unit vertical whole wire
Populaire passages
Pagina 5 - Mathematical and Physical Papers. By Sir W. THOMSON, LL.D., DCL, FRS, Professor of Natural Philosophy, in the University of Glasgow. Collected from different Scientific Periodicals from May, 1841, to the present time.
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Pagina 65 - Every body continues in its state of rest or of uniform motion in a straight line, except in so far as it is compelled by force to change that state.