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
With respect to the direction of the tail, astronomers have been forced
to abandon the antiquated notion, that the tail always pointed directly
from the sun; yet they still pertinaciously cling to the idea, that
although this is not always the case, the tail only deviates from this
direction _in the plane of the orbit_. As this is a most important
question, it is necessary formally to protest against such a conclusion.
If the earth should happen to be in the plane of the comet's orbit and
the tail appears in that plane, it must of course be in that plane
_really_; but if the earth is not in the plane of the comet's orbit, the
tail is not _necessarily_ in the same plane, whatever its apparent
direction may indicate. It is true there is a tendency of every particle
of the tail, moving under the restraining influence of the sun's
attraction, to continue in the plane of the orbit; and in certain
positions there is no oblique action arising from the force of the
radial stream to cause it to deviate from that plane; yet in other
positions of the comet, the action of the radial stream may be oblique,
forcing it out of that plane, and still such a direction might be
assigned to it as to make it conform. In the comet of 1843, P. Smythe
observed a forked tail 25° long on March 3d, and from the end of the
forked tail, and from its _north_ side, a streamer diverged at an angle
of 6° or 7° to the _north_. As this was contrary to the _direction_ of
the curvature, if the tail had been curved, it could only arise from a
portion being driven off by the radial stream, or bent towards the plane
of the ecliptic. The curvature observed by others at a later date, was
concave to the south. Towards the middle and close of March, the tail
became straight, and with the above exception, might be considered to
move in the plane of the orbit.
Public-domain text, read in full here on John Shaqi.
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