Salusbury, Thomas, Mathematical collections and translations (Tome I), 1667

Table of figures

< >
[Figure 141]
[Figure 142]
[Figure 143]
[Figure 144]
[Figure 145]
[Figure 146]
[Figure 147]
[Figure 148]
[Figure 149]
[Figure 150]
[Figure 151]
[Figure 152]
[Figure 153]
[Figure 154]
[Figure 155]
[Figure 156]
[Figure 157]
[Figure 158]
[Figure 159]
[Figure 160]
[Figure 161]
[Figure 162]
[Figure 163]
[Figure 164]
[Figure 165]
[Figure 166]
[Figure 167]
[Figure 168]
[Figure 169]
[Figure 170]
< >
page |< < of 701 > >|
1an Horizontal Line, and parallel to C D. And if the Amplitude C D
be equal to the whole Altitude D A, B I ſhall be equal to B A and B D.
And if the Time of the Fall along A B, and the Moment of Velocity
acquired in B along the Deſcent A B ex quiete in A be ſuppoſed to be
meaſured by the ſaid A B, then D C (that is twice B I) ſhall be the
Space which ſhall be paſſed by the Impetus A B turned along the Hori­
zontal Line in the ſame Time: But in the ſame Time falling along B D
out of Reſt in B, it ſhall paſs the Altitude B D: Therefore the Movea­
ble falling out of Reſt in A along A B,
being converted with the Impetus A B
150[Figure 150]
along the Horizontal Parallel ſhall
paſs a Space equal to D C.
And the
Fall along B D ſupervening, it paſſeth
the Altitude B D, and deſcribes the
Parabola B C; whoſe Impetus in the
Term C is compounded of the Equable
Tranſverſal whoſe Moment is as A B,
and of another Moment acquired in the
Fall B D in the Term D or C; which
Moments are Equal.
If therefore we
ſuppoſe A B to be the Meaſure of one of them, as ſuppoſe of the Equa­
ble Tranſverſal; and B I, which is equal to B D, to be the Meaſure of
the Impetus acquired in D or C; then the Subtenſe I A ſhall be the
quantity of the Moment compound of them both: Therefore it ſhall be
the quantity or Meaſure of the whole Moment which the Project deſcend­
ing along the Parabola B C ſhall acquire of Impetus in C. This pre­
miſed, take in the Parabola any point E, in which we are to determine
of the Impetus of the Project. Draw the Horizontal Parallel E F,
and let B G be a Mean-proportional between B D and B F.
And foraſ­
much as A B or B D is ſuppoſed to be the Meaſure of the Time, and of
the Moment of the Velocity in the Fall B D ex quiete in B: B G ſhall
be the Time, or the Meaſure of the Time, and of the Impetus in F, coming
out of B.
If therefore B O be ſuppoſed equal to B G, the Diagonal
drawn from A to O ſhall be the quantity of the Impetus in E; for
A B hath been ſuppoſed the determinator of the Time, and of the Impe­
tus in B, which turned along the Horizontal Parallel doth alwaies
continue the ſame: And B O determineth the Impetus in F or in E
along the Deſcent ex quiete in B in the Altitude B F: But theſe two
A B and B O are potentia equal to the Power A O. Therefore that is
manifeſt which was ſought.
SAGR. The Contemplation of the Compoſition of theſe diffe­
rent Impetus's, and of the quantity of that Impetus which reſults
from this mixture, is ſo new to me, that it leaveth my mind in no
ſmall confuſion.
I do not ſpeak of the mixtion of two Motions

Text layer

  • Dictionary
  • Places

Text normalization

  • Original
  • Regularized
  • Normalized

Search


  • Exact
  • All forms
  • Fulltext index
  • Morphological index