The English works of Thomas Hobbes of Malmesbury, Volume 01 (of 11)
Thomas Hobbes · en
three means, as 1 to 5, &c. But all the ordinate lines together in A I C
D are its moment; and all the ordinate lines in A I C B are its moment.
Wherefore the moments of the complements of the halves of deficient
figures in the table of art. 3 of chap. XVII, being compared, are as the
deficient figures themselves; and, therefore, the diameter of
equiponderation will divide the strait line A D in such proportion, that
the part next the vertex be to the other part, as the complete figure A
B C D is to the complement A I C D.
Coroll. The diameter of equiponderation of these halves may be found by
the table of art. 3 of chap. XVII, in this manner. Let there be
propounded any deficient figure, namely, the second three-sided figure
of two means. This figure is to the complete figure as 3⁄5 to 1, that is
3 to 5. Wherefore the complement to the same complete figure is as 2 to
5; and, therefore, the diameter of equiponderation of this complement
will cut the strait line drawn from the vertex parallel to the base, so
that the part next the vertex will be to the other part as 5 to 2. And,
in like manner, any other of the said three-sided figures being
propounded, if the numerator of its fraction found out in the table be
taken from the denominator, the strait line drawn from the vertex is to
be divided, so that the part next the vertex be to the other part, as
the denominator is to the remainder which that subtraction leaves.
[Sidenote: The centre of equiponderation of the half of any of the
deficient figures in the first row of the table of art. 3,
chapter xvii, may be found out by the numbers of the second
row.]
11. The centre of equiponderation of the half of any of those
crooked-lined figures, which are in the first row of the table of art. 3
of chap. XVII, is in that strait line which, being parallel to the axis,
divides the base according to the numbers of the fraction next below it
in the second row, so that the numerator be answerable to that part
which is towards the axis.