In Maxwell's 'Electricity and Magnetism,' a view is put forward, in accordance with which we may regard any irrotational motion in a perfect liquid, for which the velocity potential is a solid zonal harmonic, as due to the juxtaposition at the origin, and upon the axis of symmetry, of sinks and sources.
But, in a liquid, any irrotational motion which is symmetrical with respect to an axis gives a velocity potential which may be expressed as a sum of a series of solid zonal harmonics, their common axis being the axis of symmetry, and their origin arbitrary, provided it is excluded from...
%0 Journal Article
%1 citeulike:13428005
%A Sampson, R. A.
%D 1890
%I The Royal Society
%J Proceedings of the Royal Society of London
%K 76d07-stokes-and-related-oseen-etc-flows
%N 296-301
%P 46--53
%R 10.1098/rspl.1890.0064
%T On Stokes's Current Function
%U http://dx.doi.org/10.1098/rspl.1890.0064
%V 49
%X In Maxwell's 'Electricity and Magnetism,' a view is put forward, in accordance with which we may regard any irrotational motion in a perfect liquid, for which the velocity potential is a solid zonal harmonic, as due to the juxtaposition at the origin, and upon the axis of symmetry, of sinks and sources.
But, in a liquid, any irrotational motion which is symmetrical with respect to an axis gives a velocity potential which may be expressed as a sum of a series of solid zonal harmonics, their common axis being the axis of symmetry, and their origin arbitrary, provided it is excluded from...
@article{citeulike:13428005,
abstract = {{In Maxwell's 'Electricity and Magnetism,' a view is put forward, in accordance with which we may regard any irrotational motion in a perfect liquid, for which the velocity potential is a solid zonal harmonic, as due to the juxtaposition at the origin, and upon the axis of symmetry, of sinks and sources.
But, in a liquid, any irrotational motion which is symmetrical with respect to an axis gives a velocity potential which may be expressed as a sum of a series of solid zonal harmonics, their common axis being the axis of symmetry, and their origin arbitrary, provided it is excluded from...}},
added-at = {2017-06-29T07:13:07.000+0200},
author = {Sampson, R. A.},
biburl = {https://www.bibsonomy.org/bibtex/24893425650af5b4e60b6b7c6af83e21f/gdmcbain},
citeulike-article-id = {13428005},
citeulike-attachment-1 = {sampson_90_stokess_994040.pdf; /pdf/user/gdmcbain/article/13428005/994040/sampson_90_stokess_994040.pdf; f53b17116789550b743f139e8ee608e9e029734a},
citeulike-linkout-0 = {http://dx.doi.org/10.1098/rspl.1890.0064},
day = 01,
doi = {10.1098/rspl.1890.0064},
file = {sampson_90_stokess_994040.pdf},
interhash = {8cd8424b988d24c31a20a18fadeaef33},
intrahash = {4893425650af5b4e60b6b7c6af83e21f},
issn = {0370-1662},
journal = {Proceedings of the Royal Society of London},
keywords = {76d07-stokes-and-related-oseen-etc-flows},
month = jan,
number = {296-301},
pages = {46--53},
posted-at = {2014-11-14 00:08:42},
priority = {2},
publisher = {The Royal Society},
timestamp = {2017-06-29T07:13:07.000+0200},
title = {On {S}tokes's Current Function},
url = {http://dx.doi.org/10.1098/rspl.1890.0064},
volume = 49,
year = 1890
}