Abstract
In a paper published by the author in the ‘Philosophical Transactions’ for 1884, “On the Motion of Fluid, part of which is moving rotationally and part irrotationally,” a certain case of motion, sj^mmetrical with regard to an axis, was noticed (see pp. 403-405). Taking the axis of symmetry as axis of
z
, and the distance of any point from it as
r
, and allowing for a difference of notation, it was shown that the surfaces
r
2
(
r
2
/
a
2
+ (
z
-Z)
2
/
c
2
- 1) = constant, where
a, c
are fixed constants, and Z any arbitrary function of the time, always contain the same particles of fluid in a possible case of motion
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