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
be diminished faster than the ratio of the 2.5th power of the distances.
But whichever view we adopt, the diameter would again increase in the
same ratio on leaving the sun, if we make allowance for increase of
temperature, as well as for diminution of density, for the ordinary
distance of a comet's visibility. We, however, regard the change of
diameter, as due to both these nodes of action, as best agreeing with
the indications afforded by their tails.
From the preceding remarks, it results that the density of the particles
producing the nebulous envelope of a comet, renders the variations of
diameter only approximate to the law of the radial stream; a comet's own
electric energy, or the intensity of the escaping ether, may also modify
this expression, and many other causes may be suggested. That the radial
stream is the cause, in the way we have pointed out, is proved by the
positions of the major axis of the short-period comet, making frequently
nearly a right angle with the radius vector of the orbit in 1828. A soap
bubble gently blown aside, without detaching it from the pipe, will
afford a good illustration of the mode, and a confirmation of the cause.
The angles measured by Struve, reckoned from the radius vector,
prolonged towards the sun, are subjoined:
November 7 99°.7 | December 7 154°.0
November 30 145 .3 | December 14 149 .4
At this last date, the comet was getting pretty close to the sun. When
the angle was greater, as on November 7th, the comet appeared to make
almost a right angle with the radius vector; and in this position of the
earth and comet, the longer axis of the elliptical comet was directed to
the axis of the vortex, as may be verified by experiment. At the later
dates, the comet was more rapidly descending, and, at the same time, the
axis of the comet was getting more directed towards the earth; so that
the angle increased between this axis and the radius vector, and
consequently became more coincident with it. We have now to consider the
luminous appendage of a comet, commonly called a tail.
Public-domain text, read in full here on John Shaqi.
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