Elements of Natural Philosophy, Part 1 |
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Page 1
... Observation and experiment have afforded us the means of translating , as it were , from Kinematics into Dynamics , and vice versa . This is merely mentioned now in order to show the necessity for , and the value of , the preliminary ...
... Observation and experiment have afforded us the means of translating , as it were , from Kinematics into Dynamics , and vice versa . This is merely mentioned now in order to show the necessity for , and the value of , the preliminary ...
Page 6
... observe here , that since , by our formula , we have generally $ v = t and since nothing has been said as to the magnitudes of s and t , we may take these as small as we choose . Thus we get the same result whether we derive v from the ...
... observe here , that since , by our formula , we have generally $ v = t and since nothing has been said as to the magnitudes of s and t , we may take these as small as we choose . Thus we get the same result whether we derive v from the ...
Page 17
... observe ; and , in all probability , sun and stars are moving on ( it may be with incon- ceivable rapidity ) relatively to other bodies in space . We must there- fore consider how , from the actual motions of a set of bodies , we may ...
... observe ; and , in all probability , sun and stars are moving on ( it may be with incon- ceivable rapidity ) relatively to other bodies in space . We must there- fore consider how , from the actual motions of a set of bodies , we may ...
Page 52
... observation or experiment . How such experience is to be conducted will form the subject of a subsequent chapter . 172. We cannot do better , at all events in commencing , than follow Newton somewhat closely . Indeed the introduction to ...
... observation or experiment . How such experience is to be conducted will form the subject of a subsequent chapter . 172. We cannot do better , at all events in commencing , than follow Newton somewhat closely . Indeed the introduction to ...
Page 56
... observation is made . Thus , let W be the mass of a body in pounds ; g the velocity it would acquire in falling for a second under the influence of its weight , or the earth's attraction diminished by centrifugal force ; and Pits weight ...
... observation is made . Thus , let W be the mass of a body in pounds ; g the velocity it would acquire in falling for a second under the influence of its weight , or the earth's attraction diminished by centrifugal force ; and Pits weight ...
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Common terms and phrases
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
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Page 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.