Elements of Natural Philosophy, Volume 1 |
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Page 75
... Plane- tarum et Cometarum corpora motus suos et progressivos et circulares , in spatiis minus resistentibus factos , conservant diutius . ' T M moon to be a uniform spherical body . DYNAMICAL LAWS AND PRINCIPLES . 75.
... Plane- tarum et Cometarum corpora motus suos et progressivos et circulares , in spatiis minus resistentibus factos , conservant diutius . ' T M moon to be a uniform spherical body . DYNAMICAL LAWS AND PRINCIPLES . 75.
Page 76
William Thomson Baron Kelvin, Peter Guthrie Tait. T M moon to be a uniform spherical body . The mutual action and reaction of gravitation between her mass and the earth's , will be equivalent to a single force in some line through her ...
William Thomson Baron Kelvin, Peter Guthrie Tait. T M moon to be a uniform spherical body . The mutual action and reaction of gravitation between her mass and the earth's , will be equivalent to a single force in some line through her ...
Page 79
... spherical body of uniform material resting on a horizontal plane . A right cylinder or cone , bounded by plane ends perpendicular to the axis , is also in neutral equilibrium on a horizontal plane . Practically , any mass of moderate ...
... spherical body of uniform material resting on a horizontal plane . A right cylinder or cone , bounded by plane ends perpendicular to the axis , is also in neutral equilibrium on a horizontal plane . Practically , any mass of moderate ...
Page 82
... spherical bodies whose centres before collision were moving in the same straight line . The force between them at each instant must be in this line , because of the symmetry of circumstances round it ; and by the third law it must be ...
... spherical bodies whose centres before collision were moving in the same straight line . The force between them at each instant must be in this line , because of the symmetry of circumstances round it ; and by the third law it must be ...
Page 125
... spherical surface . In fact if a be the distance between each pair of feet , l the length of screw corresponding to the difference of the two readings , R the radius of the spherical surface ; we have at once 2R 1 = a2 +1 , or , as l 31 ...
... spherical surface . In fact if a be the distance between each pair of feet , l the length of screw corresponding to the difference of the two readings , R the radius of the spherical surface ; we have at once 2R 1 = a2 +1 , or , as l 31 ...
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Common terms and phrases
acceleration action amount angular velocity anticlastic attraction axis called centimetre 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 ellipse ellipsoid elongation equal equations equilibrium external point 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 P₁ P₂ parallel parallelogram of forces particle path pendulum perpendicular plane perpendicular portion position potential pressure principal axes principle produce projection proportional quantity radius radius of gyration reckoned rectangular 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