Treatise on Natural Philosophy, Volume 1, Part 2 |
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Page x
... - Composition and resolution of curvatures in a curved line - Laws of flexure and torsion - Warping of normal section by torsion 560-570 571-572 573-587 SECTIONS and flexure , infinitesimal - Rotations corresponding to flexure X CONTENTS .
... - Composition and resolution of curvatures in a curved line - Laws of flexure and torsion - Warping of normal section by torsion 560-570 571-572 573-587 SECTIONS and flexure , infinitesimal - Rotations corresponding to flexure X CONTENTS .
Page xii
... curvatures round perpendicular axes , and an anticlastic curvature round axis bisecting their right angles ; or a spherical curvature and two anticlastic curvatures ; or a spherical and one anti- clastic curvature - Work done in bending ...
... curvatures round perpendicular axes , and an anticlastic curvature round axis bisecting their right angles ; or a spherical curvature and two anticlastic curvatures ; or a spherical and one anti- clastic curvature - Work done in bending ...
Page xv
... curvature - Cases of curvilinear rect- angles for which torsion problem has been solved — Distor- tion zero at central angle of sector ( 4 ) , infinite at central angle of sector ( 6 ) ; zero at all the other angles - Problem of flexure ...
... curvature - Cases of curvilinear rect- angles for which torsion problem has been solved — Distor- tion zero at central angle of sector ( 4 ) , infinite at central angle of sector ( 6 ) ; zero at all the other angles - Problem of flexure ...
Page xxii
... curvature , horograph ( new ) . Some alteration . § 190j . Addition . § 198. Rewritten - degrees of freedom - geometrical slide ( new ) . § 200. Small alterations . § 201. Slight alteration . Appendix A. Laplace's equation in ...
... curvature , horograph ( new ) . Some alteration . § 190j . Addition . § 198. Rewritten - degrees of freedom - geometrical slide ( new ) . § 200. Small alterations . § 201. Slight alteration . Appendix A. Laplace's equation in ...
Page 23
... curvature of the surface but infinitely great in com- parison with PP ' . This disc will [ § 477 , ( b ) ] attract P and P with forces , each equal to 2πp and opposite to one another in the line PP ' . Whence the proposition . It is one ...
... curvature of the surface but infinitely great in com- parison with PP ' . This disc will [ § 477 , ( b ) ] attract P and P with forces , each equal to 2πp and opposite to one another in the line PP ' . Whence the proposition . It is one ...
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Common terms and phrases
amount angle angular velocity anticlastic applied forces attraction axes axis catenary centimetre centre of gravity centre of inertia centrobaric circular co-ordinates components condition confocal couple curvature curve cylinder denote density direction displacement distance distribution ds ds earth edge elastic solid ellipsoid elliptic equal equilibrium equipotential equipotential surfaces expression finite flexural rigidity fluid formulæ friction function given harmonic Hence homoeoid homogeneous infinitely small integral isotropic liquid mass matter modulus moment of inertia normal section osculating plane parallel particle plate position pressure prism problem radius rectangular resultant force rigid body rotation round shearing shell solid angle solid harmonic solution space sphere spherical harmonic spherical surface spheroid spiral strain stress substance suppose synclastic theorem tides tion torsion traction twist uniform unit of length whole wire Young's modulus zero
Popular passages
Page 9 - that every particle of matter in the universe attracts every other particle, with a force whose direction is that of the line joining the two, and whose magnitude is directly as the product of their masses, and inversely as the square of their distances from each other.
Page 9 - Newton generalized the law of attraction into a statement that every particle of matter in the universe attracts every other particle with a force which varies directly as the product of their masses and inversely as the square of the distance between them; and he thence deduced the law of attraction for spherical shells of constant density.
Page 478 - I infer that the general climate cannot be sensibly affected by conducted heat, at any time more than 10,000 years after the commencement of superficial solidification. No doubt, however, in particular places there might be an elevation of temperature by thermal springs, or by eruptions of melted lava, and everywhere vegetation would, for the first...
Page 460 - On the whole we may fairly conclude that, whilst there is some evidence of a tidal yielding of the earth's mass, that yielding is certainly small, and that the effective rigidity is at least as great as that of steel.
Page 479 - Do not the vast masses of basalt, the general appearances of mountain ranges, the violent distortions and fractures of strata, the great prevalence of metamorphic action (which must have taken place at depths of not many miles if so much), all agree in demonstrating that the rate of increase of temperature downwards must have been much more rapid, and in rendering it probable that volcanic energy, earthquake shocks, and every kind of so-called Plutonic action, have been, on the whole, more abundantly...
Page 216 - A body is called homogeneous when any two equal, similar parts of it, with corresponding lines parallel and turned towards the same parts, are undistinguishable from one another by any difference in quality.
Page 478 - Such is, on the whole, the most probable representation of the earth's present temperature, at depths of from 100 feet, where the annual variations cease to be sensible, to 100 miles ; below which the whole mass, or all, except a nucleus cool from the beginning, is (whether liquid or solid) probably at, or very nearly at, the proper melting temperature for the pressure at each depth.
Page 485 - It is thus shown that, although mechanical energy is indestructible, there is a universal tendency to its dissipation, which produces gradual augmentation and diffusion of heat, cessation of motion, and exhaustion of potential energy through the material universe.2 The result would inevitably be a state of universal rest and death, if the universe were finite and left to obey existing laws.
Page 471 - ... the substances, combining together, may be again separated electrolytically by thermo-electric currents, due to the heat generated by their combination, and thus the chemical action and its heat continued in an endless cycle, violates the principles of natural philosophy in exactly the same manner, and to the same degree, as to believe that a clock constructed with a self-winding movement may fulfil the expectations of its ingenious inventor by going for ever.
Page 492 - HEAT. The sun being, for reasons referred to above, assumed to be an incandescent liquid now losing heat, the question naturally occurs, How did this heat originate ? It is certain that it cannot have existed in the sun through an infinity of past...