Elements of the Theory of the Newtonian Potential Function |
Contents
| 1 | |
| 7 | |
| 13 | |
| 15 | |
| 24 | |
| 29 | |
| 30 | |
| 39 | |
| 246 | |
| 251 | |
| 259 | |
| 262 | |
| 273 | |
| 278 | |
| 291 | |
| 298 | |
| 66 | |
| 71 | |
| 75 | |
| 76 | |
| 83 | |
| 145 | |
| 157 | |
| 160 | |
| 164 | |
| 171 | |
| 175 | |
| 218 | |
| 222 | |
| 241 | |
| 299 | |
| 301 | |
| 304 | |
| 312 | |
| 326 | |
| 332 | |
| 337 | |
| 357 | |
| 378 | |
| 396 | |
| 416 | |
| 479 | |
| 486 | |
| 489 | |
Other editions - View all
Common terms and phrases
A₁ angle attracting mass attraction due axis C₁ carries a steady cavity centimetres centre charge circuit closed surface condenser conductor constant coördinate axes curl curve cylinder D₂ derivatives dielectric direction distance distribution electricity electromotive force element ellipsoid energy equal equipotential surfaces everywhere exterior normal finite Gauss's Theorem given Green's Theorem homogeneous induction infinite infinity intensity L₁ lamellar Laplace's Equation limit line integral lines of force M₁ medium negative normal component P₁ parallel particle perpendicular Poisson's Equation polarization positive potential function due Prove quantity r₁ radius ratio repelling matter resistance respectively resultant force S₁ self-inductance shell Show solenoidal space sphere spherical surface steady current straight line surface density surface integral tion tube of force unit V₁ V₂ vanishes at infinity vector wire xy plane zero
Popular passages
Page 91 - An Essay on the application of Mathematical Analysis to the Theories of Electricity and Magnetism...
Page 1 - Every particle in the universe attracts every other particle with a force that is directly proportional to the product of the masses of the two particles and inversely proportional to the square of the distance between them.
Page 116 - Q is a point so chosen on the normal at P of the surface of constant v which passes through P, that VQ — vp is positive.
Page 1 - Every body in the universe attracts every other body with a force which is directly proportional to the product of their masses and inversely proportional to the. square of the distance between them.
Page 28 - Show that the attraction at the focus of a segment of a paraboloid of revolution bounded by a plane perpendicular to the axis at a distance b from the vertex is of the form 4irpa log (1 + b/a~).
Page 277 - K and E are the complete elliptic integrals of the first and second kinds with modulus k ; so that the quantity in PA brackets is a function of the ratio p^r simply.