Outlines of a mechanical theory of storms : $b containing the true law of lunar influence, with practical instructions to the navigator, to enable him approximately to calculate the coming changes of the wind and weather, for any given day, and for any part of the oceanBassnett, Thomas
Science
Outlines of a mechanical theory of storms : $b containing the true law of lunar influence, with practical instructions to the navigator, to enable him approximately to calculate the coming changes of the wind and weather, for any given day, and for any part of the ocean
Bassnett, Thomas
Weather
In the following figure, the arrows represent the ethereal current of
the terral vortex; the linear circle, the earth; C the centre of gravity
of the earth and moon, and, consequently, the central vortex or axis of
the vortex of the earth, I represents the position of the inner vortex,
and O that of the outer vortex. These two last are eddies, caused by the
obstacle presented by the earth in being _pushed_ out from the centre by
the moon, and are called lateral vortices. There are, therefore, two
lateral vortices, and one central, in both hemispheres, and by this
simple arrangement is the earth watered, and the atmospheric circulation
produced.
[Illustration: Fig. 3]
ILLUSTRATION OF THEIR ACTION.
If we place a globe in a vessel of water, so that the vertex shall only
just be covered, and place the globe eccentrically in the vessel so that
the centre of the vessel may not be too far from the outside of the
globe, and then impart an equable but slow motion to the water, in the
manner of a vortex; by viewing the reflected light of the sky from the
surface of the water above the globe, we shall be able to trace a
succession of dimples, originating at I and O, and passing off with the
current, and dying away. The direction of the fluid in these little
eddies, will be the same as the direction of the current in the main
vortex. If we displace the globe, so as to remove it far from the centre
of the vessel, and impart the same motion, the vortex I will be found at
E, and the direction of the current will be contrary to the direction
of the fluid in the vessel. In the case of the earth and moon, the
displacement can never change the position of the inner vortex much. It
will always be to the right hand of the central vortex in north
latitudes, and in consequence of the ether striking our globe in such a
position, the current that is deflected from its true path, by the
protuberance of the earth forcing it inside, is prevented by the
circular current of the parts nearer the axis of the vortex, from
passing off; so that a vortex is formed, and is more violent, _ceteris
paribus_, than the vortex at O.
ORDER OF OCCURRENCE.
Whether this mode of action has been correctly inferred, matters little;
the lateral vortices follow the law of such a position. The inner vortex
always precedes the central from five to eight days, when ascending in
this latitude, and comes to the meridian after the moon. The outer
vortex, on the contrary, follows the central in its monthly round, and
comes to the meridian before the moon. It will be readily understood
that if the axes of these lateral vortices be produced through the
earth, they will pass through similar vortices in the opposite
hemisphere; but as the greatest latitude of the one, corresponds to the
least latitude of the other, the same calculation will not answer for
both. The same remark applies to the central vortex also.
Public-domain text, read in full here on John Shaqi.
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