Fabri, Honoré
,
Tractatus physicus de motu locali
,
1646
Text
Text Image
Image
XML
Thumbnail overview
Document information
None
Concordance
Figures
Thumbnails
Page concordance
<
1 - 30
31 - 60
61 - 90
91 - 120
121 - 150
151 - 180
181 - 210
211 - 240
241 - 270
271 - 300
301 - 330
331 - 360
361 - 390
391 - 420
421 - 450
451 - 480
481 - 491
>
Scan
Original
81
82
83
84
85
86
87
88
89
90
91
92
93
94
95
96
97
98
99
100
101
102
103
104
105
106
107
108
109
110
<
1 - 30
31 - 60
61 - 90
91 - 120
121 - 150
151 - 180
181 - 210
211 - 240
241 - 270
271 - 300
301 - 330
331 - 360
361 - 390
391 - 420
421 - 450
451 - 480
481 - 491
>
page
|<
<
of 491
>
>|
<
archimedes
>
<
text
>
<
body
>
<
chap
id
="
N1137F
">
<
pb
pagenum
="
51
"
xlink:href
="
026/01/083.jpg
"/>
<
p
id
="
N144CB
"
type
="
main
">
<
s
id
="
N144CD
">
<
emph
type
="
center
"/>
<
emph
type
="
italics
"/>
Scholium.
<
emph.end
type
="
italics
"/>
<
emph.end
type
="
center
"/>
</
s
>
</
p
>
<
p
id
="
N144D9
"
type
="
main
">
<
s
id
="
N144DB
">Obſeruabis propagationem impetus, vel alterius qualitatis eſſe tan
<
lb
/>
tùm continuatam eiuſdem productionem, quæ incipit ab ea parte, cui
<
lb
/>
potentia eſt immediatè applicata, & propagatur, ſeu diffunditur per
<
lb
/>
omnes alias donec ad vltimam perueniat eo modo, quo iam definio. </
s
>
</
p
>
<
p
id
="
N144E4
"
type
="
main
">
<
s
id
="
N144E6
">
<
emph
type
="
center
"/>
<
emph
type
="
italics
"/>
Theorema
<
emph.end
type
="
italics
"/>
92.
<
emph.end
type
="
center
"/>
</
s
>
</
p
>
<
p
id
="
N144F2
"
type
="
main
">
<
s
id
="
N144F4
">
<
emph
type
="
italics
"/>
Illa progatio non fit per motum localem, ita vt pars impetus producta in
<
lb
/>
prima parte ſubiecti tranſeat ad ſecundam,
<
emph.end
type
="
italics
"/>
patet; quia cum impetus ſit ac
<
lb
/>
cidens per Th. 8. de ſubiecto in ſubiectum tranſire non poteſt per deff. </
s
>
<
s
id
="
N14501
">
<
lb
/>
accidentis; de qua in Metaphyſicâ; </
s
>
<
s
id
="
N14505
">nec eſt quod aliqui dicant ſe
<
expan
abbr
="
nõ
">non</
expan
>
poſſe
<
lb
/>
concipere, quomodo id fiat ſine motu locali; </
s
>
<
s
id
="
N1450F
">cum ipſis etiam oculis
<
lb
/>
quaſi cernatur; </
s
>
<
s
id
="
N14515
">cum enim percutis corpus oblongum AE, & cadit ictus
<
lb
/>
in extremitatem A, corpus ipſum totum ſimul moues; igitur pars impe
<
lb
/>
tus, quæ recipitur in A, non migrat in E, ſed hæc producitur in A, &
<
lb
/>
alia in B, alia in C, atque ita deinceps. </
s
>
</
p
>
<
p
id
="
N1451F
"
type
="
main
">
<
s
id
="
N14521
">
<
emph
type
="
center
"/>
<
emph
type
="
italics
"/>
Scholium.
<
emph.end
type
="
italics
"/>
<
emph.end
type
="
center
"/>
</
s
>
</
p
>
<
p
id
="
N1452D
"
type
="
main
">
<
s
id
="
N1452F
">Obſeruabis ex hac propagatione impetus per analogiam rectè om
<
lb
/>
ninò explicari propagationem luminis, & aliarum qualitatum, de qui
<
lb
/>
bus ſuo loco. </
s
>
</
p
>
<
p
id
="
N14536
"
type
="
main
">
<
s
id
="
N14538
">
<
emph
type
="
center
"/>
<
emph
type
="
italics
"/>
Theorema
<
emph.end
type
="
italics
"/>
92.
<
emph.end
type
="
center
"/>
</
s
>
</
p
>
<
p
id
="
N14544
"
type
="
main
">
<
s
id
="
N14546
">
<
emph
type
="
italics
"/>
In propagatione impetus prima pars
<
emph.end
type
="
italics
"/>
A v. g.
<
emph
type
="
italics
"/>
non producit partem
<
emph.end
type
="
italics
"/>
B,
<
emph
type
="
italics
"/>
&
<
lb
/>
hæc
<
emph.end
type
="
italics
"/>
C; </
s
>
<
s
id
="
N1455F
">
<
emph
type
="
italics
"/>
hæc verò
<
emph.end
type
="
italics
"/>
D,
<
emph
type
="
italics
"/>
atque ita deinceps
<
emph.end
type
="
italics
"/>
; Probatur. </
s
>
<
s
id
="
N1456F
">Primò, quia ſi hoc eſſet,
<
lb
/>
omne corpus poſſet moueri à qualibet potentia; nam modò poſſet pro
<
lb
/>
duci vnum punctum impetus, hoc etiam aliud produceret, & hoc aliud,
<
lb
/>
atque ita deinceps. </
s
>
<
s
id
="
N14579
">Secundò, Minimum granum ſuperpoſitum rupi, to
<
lb
/>
tam ipſam rupem mouere poſſet. </
s
>
<
s
id
="
N1457E
">Tertio, Quia vel in omnibus, vel in
<
lb
/>
nulla parte impetus producitur per Th.33. Quartò, quia impetus mobi
<
lb
/>
lis projecti intenderetur; nam impetus vnius partis impetum alterius
<
lb
/>
intenderet. </
s
>
<
s
id
="
N14588
">Quintò, quia impetus partis B, tàm ageret in A, trahendo,
<
lb
/>
quàm in C pellendo; cum impetus vtroque modo propagetur. </
s
>
<
s
id
="
N1458E
">Sextò, ſi
<
lb
/>
applicaretur potentia in C, non video, cur impetus partis C, ageret po
<
lb
/>
tius versùs E, quàm versùs A? alioquin eadem pars impetus plures pro
<
lb
/>
ducere poſſet; igitur impetus potentiæ motricis ſufficiens erit cauſa ad
<
lb
/>
producendum totum alium. </
s
>
<
s
id
="
N1459A
">Septimò, tractionis impetus explicari non
<
lb
/>
poteſt, ſi impetus vnius partis producat in alia impetum; alioquin dare
<
lb
/>
tur mutua actio infinities repetita, vt conſideranti patebit. </
s
>
<
s
id
="
N145A2
">Octauò, ſi
<
lb
/>
impetus vnius partis producit in alia; </
s
>
<
s
id
="
N145A8
">ſint duo globi contigui; igitur il
<
lb
/>
le, qui impellit alium, reflecti poſſet, quod nunquam accidit quando
<
lb
/>
ſunt contigui. </
s
>
</
p
>
<
p
id
="
N145B0
"
type
="
main
">
<
s
id
="
N145B2
">Obſeruabis illud quidem verum eſſe in motu recto, ſecus in circulari; </
s
>
<
s
id
="
N145B6
">
<
lb
/>
nam cum cylindrus circa alteram extremitatem vibratus deorſum cadit;
<
lb
/>
partes, quæ propiùs ad extremitatem immobilem accedunt iuuant mo
<
lb
/>
tum aliarum, quæ longiùs ab eadem recedunt. </
s
>
</
p
>
</
chap
>
</
body
>
</
text
>
</
archimedes
>