Galilei, Galileo - The systems of the world

Galilei, Galileo, The systems of the world, 1661

None
Concordance
Figures
Thumbnails

Page concordance

Scan	Original
21
22
23
24
25
26
27
28
29
30
31
32
33
34
35
36
37
38
39
40
41
42
43
44
45
46
47
48
49
50

perpendicular ſhould be taken near to the end C, and in the in
clination, far from it.

SALV. You ſee then, that the Propoſition which ſaith, that
the motion by the perpendicular is more ſwift than by the incli
nation, holds not true univerſally, but onely of the motions,
which begin from the extremity, namely from the point of reſt:
without which reſtriction, the Propoſition would be ſo deficient,
that its very direct contrary might be true; namely, that the mo
tion in the inclining plane is ſwifter than in the perpendicular:
for it is certain, that in the ſaid inclination, we may take a ſpace
paſt by the moveable in leſs time, than the like ſpace paſt in the
perpendicular. Now becauſe the motion in the inclination is in
ſome places more, in ſome leſs, than in the perpendicular; there
fore in ſome places of the inclination, the time of motion of the
moveable, ſhall have a greater proportion to the time of the motion
of the moveable, by ſome places of the perpendicular, than the
ſpace paſſed, to the ſpace paſſed: and in other places, the pro
portion of the time to the time, ſhall be leſs than that of the
ſpace to the ſpace. As for example: two moveables departing
from their quieſcence, namely, from the point C, one by the per
pendicular C B, [in Fig. 4.] and the other by the inclination C A,
in the time that, in the perpendicular, the moveable ſhall have
paſt all C B, the other ſhall have paſt C T leſſer. And therefore
the time by C T, to the time by C B (which is equal) ſhall have
a greater proportion than the line C T to C B, being that the
ſame to the leſs, hath a greater proportion than to the greater.
And on the contrary, if in C A, prolonged as much as is requi
ſite, one ſhould take a part equal to C B, but paſt in a ſhorter
time; the time in the inclination ſhall have a leſs proportion to
the time in the perpendicular, than the ſpace to the ſpace. If
therefore in the inclination and perpendicular, we may ſuppoſe
ſuch ſpaces and velocities, that the proportion between the ſaid
ſpaces be greater and leſs than the proportion of the times; we
may eaſily grant, that there are alſo ſpaces, by which the times
of the motions retain the ſame proportion as the ſpaces.

SAGR. I am already freed from my greateſt doubt, and con
ceive that to be not onely poſſible, but neceſſary, which I but
now thought a contradiction: but nevertheleſs I underſtand not
as yet, that this whereof we now are ſpeaking, is one of theſe
poſſible or neceſſary caſes; ſo as that it ſhould be true, that the
time of deſcent by C A, to the time of the fall by C B, hath the
ſame proportion that the line C A hath to C B; whence it may
without contradiction be affirmed, that the velocity by the incli
nation C A, and by the perpendicular C B, are equal.

SALV. Content your ſelf for this time, that I have removed

Text layer

Text normalization

Search