 ... (7). § 5. As a first and very simple illustration, suppose the atom to be spherical, of radius unity, with concentric interior spherical surfaces of equal density. This gives, for the direction of the resultant force on any particle of the ether,...  Proceedings of the Royal Society of Edinburgh - Page 202by Royal Society of Edinburgh - 1902Full view - About this book
 | William Thomson Baron Kelvin - 1904 - 848 pages
...parts and negative in other parts of the atom, in such quantities as to fulfil the condition //pla = 0 ........................... (7). § 5. As a first...of the atom, a line through the centre of the atom. We may now take A = 4wrsrfr. The further assumption of (7) may thus be expressed by (8); and this,... | |
 | William Thomson Baron Kelvin - 1904 - 734 pages
...parts and negative in other parts of the atom, in such quantities as to fulfil the condition J!P«-0 (7). § 5. As a first and very simple illustration,...of the atom, a line through the centre of the atom. We may now take A = 4nri-3dr. The further, assumption of (7) may thus be expressed by drr'a^Q (8);... | |
 | Royal Society of Edinburgh - 1902 - 594 pages
...parts and negative in other parts of the atom, in such quantities as to fulfil the condition JJjAa = 0 ....... (7). § 5. As a first and very simple illustration,...further assumption of (7) may now be expressed by /ldrrza = Q ....... (8); 0 and this, as we are now supposing the forces between every particle of the... | |
 | 1900 - 670 pages
...some parts and negative in other parts of the atom, in such quantities as to fulfil the condition § 5. As a first and very simple illustration, suppose...further assumption of (7) may now be expressed by (8); and this, as we are now supposing the forces between every particle of the atom and every particle... | |
 | Lord William Thomson Kelvin - 1904 - 732 pages
...parts and negative in other parts of the atom, in such quantities as to fulfil the condition //M« = 0 ........................... (7). § 5. As a first...of the atom, a line through the centre of the atom. We may now take A = 4>irr*dr. The further assumption of (7) may thus be expressed by 0 ........................... | |
 | 1900 - 664 pages
...parts and negative in other parts of the atom, in such quantities as to fulfil the condition f' ....... (7). § 5. As a first and very simple illustration,...equal density. This gives, for the direction of the resultnnt force on any particle of the ether, whether inside or outside the spherical boundary of the... | |
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