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# Title: Leibniz-Handschriften zur Varia Physica LH 37, 4
# Folio 166v, page id 00068606:0336
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Seocorpus ci curtat in devene
Eledua corperae incaventit
ut
l 
sit
corum non s con at
aequalia quiescentrata  t
exunt Sicorpus t
diversis velocitatibus in diversa corporir
ipsis velocitatibus proportionalia. Et sarcita quad quarenus hoc pleai sili impingat
exunt detrimenta velocitatis in corpore incurrente
resiiA contingit  cum mobile movetur ia
 unitormi
asi elementis decrementa.
medio fluido sibe simili
relocitatis ipsis velocitatibus proportionalia
erunt in aequalibus
obyrietens
(quisimalet et primo quidem
ee
 pleno incursu (hoc est nornaliter
sit enim corpus A incvrrems in quiescens B inleo1B et centraliter)
centrum gravitatis
utqi post concursum Equibiunt et B)
 C2C.
perget lolito verocitate 2C3C.
  aquali ipsi 1C2C, et quia A pervendet
n3A  et positie A et A eunte velocitate
A3A ac B velocilata 2B3B post concursum
dabet esse 3A3(3 aiqualis ipsi 1A1B, ut eadem
scrvetur caleritas arespectiva) itaque differentia
inter ipsius A velocitatem priorem 1A2A, et posteriorem
A3A sic innagabitur AEA L 2ABA1B Se stantia coporum
A 3A plus 2A2B distantia coniorum, sumta
in
dividitur per, C in ratom in duas pariss AcC et BBB.C
ABqum. R. BH A3A aequ. 2AC+ C3C
in ratione B ad A, apprimamus hanc rationem numeris
nm erit A1C aequol.
e 1C 2 C aeqe 1AIB - 1AIC = 2B2C aequ. 2C3C. Ed Et
ACtECIC. CA
A3 aequ.  2A2C + 2C3C - 3A3C et 3A3C aequ. iA. C. Eyd. 43A =  A A
Ergo fit 2A3A aequ. 2A2C L 1A. B - . A, C - 2B2C = 1A.C
jam A2A aequ. 1A, 3 - 2A2B. ergo fit
1A2A - Z A3 A aequ. BCA, B = 2AB C_CI = 2A+ (- . B2C
c
= EA2C = 1AIB + .A, C+ 2B2C + 1A1C
id est demtis utrobui aequalibus sit
qua quantitus est
ad AB, ut (seu
1t
+quaequantitas est
aqu vis 1A1Cm bis 2A2Csed si corporis quiescentio
detrimentum veloci
B magnitudo sit inconsiderabilis, etium
em
ecerit plio
ram statim ipsius
tis A aequale magnitiaio dicabilem a qua
ratio iptius A
leo espellitur qu Lipisam M
id es. ratio
2A2C ad 1AIC, inconsiderabilis adeoque pro
indius 2A2Ba
quantitate bis. A, C minus bs 2A2C sufficit
quaentitas bis AIC, eti est ergo detr
est autem AIC proportionalis ipsi
A 1B, hoc
st (ob 2A2B inconsiderab ilem) ipsi 1A 2A velocitati
ipsius A.jam iccetredia cpepu corne si uedium
fluidum uniforme, ex aec aqualibus quiestentibus
particulis perpetuo continget
 solido diuo
litius 
ebii
 uol
uju
distat
um
A, aequalem ipsi. B
 sed. AIC = 2AEC est
proportionalis ipsi 1A1B
2A2B, id est isi rA2A
vetorit
isius de
excipientis ad corforuu
amborum summum) e
1A. B = 2A2:3, est 1A2A
velocitas incurrentis. Ha–
bemus ergo detrineutum
prop velocitatis ipsi veloci
tati proportionale.
uns ad latus est non consi
xcitotus directos est magnam partem hiido et
tamen motus
fn
muta
que tecte
eA H2B
vicinarum jam fulsarum,
varenus
q A comradais
at in
c.1B 3A 3C