Elements of Natural Philosophy, Part 1 |
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Page 5
... relative motions of all parts of other systems of pulleys and cords as long as all the free parts of the cords are parallel . Of course , if a pulley be fixed , the motion of a point of one end of the cord to or from it involves an ...
... relative motions of all parts of other systems of pulleys and cords as long as all the free parts of the cords are parallel . Of course , if a pulley be fixed , the motion of a point of one end of the cord to or from it involves an ...
Page 17
... Relative merely . We can calculate from astronomical data for any instant the direction in which , and the velocity with which , we are moving on account of the earth's diurnal rotation . We may compound this with the ( equally ...
... Relative merely . We can calculate from astronomical data for any instant the direction in which , and the velocity with which , we are moving on account of the earth's diurnal rotation . We may compound this with the ( equally ...
Page 18
... relative motion among the stars that we can observe ; and , in all probability , sun and stars are moving on ( it ... relative motions with regard to any one of them ; and how , having given the relative motions of all but one with ...
... relative motion among the stars that we can observe ; and , in all probability , sun and stars are moving on ( it ... relative motions with regard to any one of them ; and how , having given the relative motions of all but one with ...
Page 19
... relative path depends only upon the length and G ' A G direction of the line joining the two points at any instant , it is obvious that these will be the same for A with regard to B , as for B with regard to A , saving only the ...
... relative path depends only upon the length and G ' A G direction of the line joining the two points at any instant , it is obvious that these will be the same for A with regard to B , as for B with regard to A , saving only the ...
Page 22
... relative circles . On CQ and CQ describe a parallelogram SQCQ ; and through S draw SR perpendicular to B'A ' produced . We have P'R CP ( being projections of the equal and parallel lines Q'S , CQ , on CR ) . Hence CR = CP + CP ' ; and ...
... relative circles . On CQ and CQ describe a parallelogram SQCQ ; and through S draw SR perpendicular to B'A ' produced . We have P'R CP ( being projections of the equal and parallel lines Q'S , CQ , on CR ) . Hence CR = CP + CP ' ; and ...
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Common terms and phrases
acceleration action amount angular velocity anticlastic applied attraction axes axis called Cambridge centre of gravity centre of inertia circle circular co-ordinates component configuration consider constant corresponding cosine couple curvature curve cylinder Demy 8vo denote density described diagram displacement distance edition elastic ellipse ellipsoid elongation equal equations equilibrium external point fixed point fluid forces acting friction geometrical given force Hence hodograph inclined infinitely small instant inversely kinetic energy length magnitude mass matter measured moment of inertia momentum moving normal P₁ P₂ parallel parallelogram particle path pendulum perpendicular portion position pressure principal axes principle produce projection proportional quantity radius radius of gyration reckoned resultant right angles rigid body rotation round shear shell simple harmonic motion solid solid angle space spherical surface spiral square straight line strain suppose tangent torsion uniform unit University of Cambridge vertical whole wire
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