The arabic numbers refer to sections. The numbers 1. and 11. preceding them indicate the volume (parts of the original first volume) in which they will be found. The capital letters refer to the Appendixes. In the case of the Appendixes A, A, B, references are given to the pages of 1.; the other Appendixes are at the ends of their respective volumes.
Attraction of a spherical surface with den- sity varying inversely as the cube of the distance from a given point, II. 474-476
of a sphere whose density varies inversely as the fifth power of the distance from a point, 11. 518
of a sphere composed of concentric shells of uniform density, 11. 480, 491 (d)
of a uniform circular disc on a par- ticle in its axis, I. 477, 517
of a cylinder on a particle in its axis, II. 477
of a right cone on a particle at its vertex, 11. 477
of a uniform circular arc, II. 481 of a straight line, 11. 481
of a uniform hemisphere on a particle at its edge, 11. 478
of matter arranged in infinite paralle planes of uniform density, 11. 491 (ƒ)
of coaxal cylinders of uniform density to infinite lengths, I. 491 (e) of a homogeneous ellipsoid, II. 494 (j) -(0); 11. 519-532
of a shell bounded by similar con- centric and similarly situated ellip- soids, 11. 519-521, 523
of an infinite homogeneous elliptic cylinder, 11. 494 (p) (q)
of a heterogeneous ellipsoid, n. 527 of a particle on a distant body, 1. 540, 541
inverse problem of, 11. 494 (a)--(ƒ)
Compressibility, defined, 11. 680; 1. (C) l. Conservative system, defined, 1. 271 Constraint, of a point with two or one degrees of free lom, 1. 196
of a rigid body with various degrees of freedom, I. 197, 199
of a rigid body, five degrees of, 1. 198 of a rigid body, one degree of, most general form of, 1. 200; mechanical illustration of, 1. 201; analytical expression of, 1. 201
Gauss's principle of least, 1. 293 kinetic, cases of motion governed by, 1. 319
Continuity, integral equation of, 1. 192
differential equation of, 1. 193, 194 Co-ordinates, Rodrigues, 1. 95
generalized, of a point, 1. 202, 203 generalized, of a system. 1. 204 generalized, kinetic energy expressed in, 1. 313
generalized, equations of motion in, 1. 318
ignoration of, 1. 319
generalized orthogonal transforma- tion of, 1. 337 note
D'Alembert's principle, 1. 264
Density, line, surface and volume, 11. 460 of the Earth, 11. 774, 831
Determinant, expression for the square of, 1. p. 166 4, (k)
minors of a, 1. 343 (b)
relations between the minors of an
evanescent, 1. 343 (b)
square root of skew symmetric, 1. 345 (ix)
Diagonal scale, 1. 419
Direction, integral change of, in a surface, I. 135
Displacement, in one plane, equivalent to a rotation, 1. 79, 80, 83; or a trans- lation, 1. 81
in one plane, examples of, 1. 84,
of a non-rigid solid with one point fixed, general analytical investiga- tion of, 1. 181, 190 (e), (f), (i) tangential, defined, 1. 186; of dis- placed and undisplaced curve com- pared, 1. 187-189; of a closed curve, due to rotation, 1. 190; of a closed curve due to strain, 1. 190 (a)—(d) Dissipativity, 1. 345 (ii)
Earth, The, as a time-keeper, 11. 830 figure of, as determined by geodesy, 11. 797
rigidity of, 11. 832-848
distribution of land on, 11. 848
secular cooling of, 11. (D)
Edge of regression, 1. 148
Elastic curve, 11. 611, 612
Elastic body, perfectly, defined, 11. 672
Elasticity, of volume, 11. 680
of figure, 11. 680
Elastic solid, equations of equilibrium of, II. 697, 698; 11. (C)
integration of equations of equi- librium of infinite, 11. 730 displacements of, by stress applied to an infinitely small part, 11. 731 displacements of, by stress applied over the boundary, 11. 732-734 displacement of, when the strain is plane, 11. 739
Green's theory of, 11. (C) (4), (h) sphere, deformation of, by rotation, II. 837, 838
spherical shell, equilibrium of, under
surface tractions, n. 735-737 Ellipticity of strata of equal density within the earth resulting from Laplace's law, II. 824, 824'
Energy, kinetic, defined, 1. 213
kinetic, rate of change of, 1. 214; analytical expression for, 1.280 potential, defined and explained, 1. 241, 273, 274
conservation of, 1. 269-278 apparent loss of, 1. 275-277 equation of, 1. 293, 318
kinetic and potential, expressed as functions of the time in the case of small motions, 1. 337
potential, exhaustion of, 11.547-549 Eolotropy, 11. 676–678 Epicycloid, 1. 49, 94
Equilibrant, of a system of forces, 11.558 Equilibrium, neutral, stable and unstable, examples of, 1. 291
of a particle, 11. 455, 456 of three forces, II. 564.
of forces proportional and perpen- dicular to the sides of a polygon at their middle points, or the faces of a polyhedron at their centres of inertia, 11. 559 (e)
of a free rigid body, 11. 551-553 of a constrained rigid body, II. 554— 557
of a body moveable about an axis, II. 567
of a body resting on a fixed surface, II. 568
of a body capable of a single screw motion, 11. 556
simple examples of, 11. 572
of a floating body, stability of, 11. 763 -768
of a rotating gravitational fluil ellip- soid of equilibrium, 11. 770-773, 775-777, 778'
of a rotating gravitational fluid ellip- soid with three unequal axes, 11. 778
Equilibrium of a rotating fluid mass gene. rally, 11. 778'
of a rotating heterogeneous liquid spheroid, enclosing a rigid spherical nucleus and subjected to disturb- ance, 11. 822-824
of rotating spheroid of two incom- pressible non-mixing fluids, 11. 831 energy criterion for, 1. 289, 290, 292 slightly disturbed, application of the Lagrange equation to, 1. 337
general solution of any case of slightly disturbed, 1. 343 (ƒ)—(p) Equipotential surfaces, defined, 11. 491 (g) of homogeneous harmonic spheroids, II. 789, 790
for approximately spherical mass due
to gravitation and rotation con- jointly, II. 794
of rotating fluid covering a spherical nucleus, 11. 800-802
of fluid covering a fixed spherical nucleus, and disturbed by the attrac- tion of a distant body, II. 803 Ergometer, 1. 436, 437 Error, law of, 1. 391
probable, 1. 392, 393 Errors, theory of, 1. 387-394 Evolute, 1. 17-19
Experiment, remarks on, 1. 373–382
Flexure, of a bar, 11. 711-713 of a plate, I. 719-729
of a plate bounded by an infinite plane edge, 11. 728
Fluid, perfect, defined, 1. 320; 11. 742 cases of motion in a perfect, 1. 320- 325
equations of equilibrium of a perfect, II. 753
equilibrium of, in a closed vessel, 11. 754, 755
equilibrium of, under non-conserva- tive forces, 11. 757-759
equilibrium of, possibility of, under given forces, II. 755, 756
density of, in terms of potential of applied forces, 11. 760
impulsive generation of motion in an incompressible, 1. 312, 317 Fluxions, 1. 24, 203 Foci, kinetic, 1. 357-364 Force, measure of, 1. 220, 413
specification of, 1. 218 accelerative effect of, 1. 219 measurement of, 1. 258 unit of, 1. 221
Gauss's absolute unit of, 1. 223 British absolute unit of, 1. 225 ideal units of, 1. 223
Force, comparison of absolute and gravi- tational measures of, 1. 226 effective component of, 1. 228 moment of, 1. 232
time-integral of, 1. 297
line of, defined and illustrated, 11. 489, 490
Forces, composition of, 1. 255
parallel, composition of, 11. 561, 563 parallelogram and polygon of, 1. 256 system of, reduced to two, 11. 560 system of, reduced to a force and a couple, 11. 559 (c)
Freedom, degrees of, 1. 195–201; (see Constraint)
Friction, laws of, between solids, 11. 450
laws of fluid, 1. 340
Function, simple harmonic, 1. 54
complex harmonic, 1. 75, 76; repre- sentation of the results of experi ment by means of a, 1. 338' plane harmonic, 11. 739 displacement, 1. 190 (k) spherical harmonic, 1. p. 171 B. (see Spherical harmonics)
Laplace's, I. p. 208 B. (e') (see Sphe- rical harmonics)
Hamilton's characteristic, 1. 331; complete solution derived from a knowledge of, 1. 331 cyclic, 11. 755, note
Harmonic motions, mechanical composi tion of, in one line, 1. 62
graphical representation of, 1. 62, 69, 72, 74
composition of, in different lines, 1. 63-73
Harmonic, spheroid, defined, 11. 779 nodal cone, defined, 11. 779; proper- ties of, 11. 780
spherical (see Spherical harmonics) Heat, specific, defined, 11. (E) 1 note Hodograph, definition of, 1. 37
elementary properties of, 1. 37
for the undisturbed motion of a planet is a circle, 1. 38
physical applications of, 1. 39 Homogeneousness, defined, u. 675 Hooke's joint, 1. 109
Horograph, defined, 1. 136
exercises on, 1. 137
Horse-power, 1. 268 Hypocycloid, 1. 91, 94 Hypotheses, use of, 1. 383-386
Laplace's law of density of the earth's strata, 11. 824; applied to determine the constant of precession, 11. 827, 828; compressibility involved in, II. 829 Laplace's differential equation for the potential, etc., with Poisson's ex- tension, II. 491 (b) (c)
expressed in generalized co-ordinates by physical considerations, 1. A ̧ p. 160 (a)-(e)
expressed in generalized co-ordinates by algebraical transformation, 1. p. 166 A。 (j)—(m)
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