MASS OF THE MOON.

Those elements which represent the moon's distance and motion are

accurately known, and may be taken from the Nautical Almanac, being all

embodied in the moon's parallax or semi-diameter, and in the declination

and right ascension; but for the most important element,--the moon's

mass, we in vain look to astronomy. In fact, it may be averred that the

importance attached to astronomical authority, concerning the mass of

the moon, has caused more trouble than any other question of the whole

theory, until we trusted implicitly to the theory itself to determine

it. The determination of three unknown elements, viz.: the moon's mass,

the inclination of the axis of the vortex, and the right ascension of

that axis, is a more difficult problem than at first sight appears,

owing to the nature of the phenomena, which affords the only clue for

its solution. There are six principal vortices ever in operation on the

surface of the earth, and their disturbing influence extends from 200 to

400 miles. To find the precise centre, by one observer confined to one

place, is difficult; and to separate them, so as to be fully assured

that you have the right one, is perhaps still more so. Happily this

tedious labor is accomplished, and we are able with confidence to give

the following important elements, as very close approximations to the

truth:

Mass of the moon 1/72.3

Obliquity of the axis of the vortex 15d to 32d variable.

Right ascension of ditto 250d to 290d variable.

It must be borne in mind that we are now discussing the main or central

vortex of the earth; but before applying them to the calculation, we

will explain the _modus operandi_, waiving for the present the

consideration of the law of density in the Terral vortex. It is evident

at first sight that if the periodic times of the parts of the vortex

contiguous to the moon, are equal to the moon's period approximately,

that the velocity of the ether is greater at the surface of the earth

than the velocity of that surface. Now, we have before argued that the

ether possesses inertia, it therefore would under such circumstances

exert some mechanical action. Consequently, the aerial envelope of our

globe, or its superior stratum, is impelled eastward by _convection_[4]

of the more rapidly rotating ether. And from the extreme tenuity of its

upper layers, is probably forced into immense waves, which will observe

to a certain degree, a general parallelism north and south.

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