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# Title: Leibniz-Handschriften zur Mechanik: Dynamika LH 37, 5
# Folio 135r, page id 00068534:0265
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+ fig L
Haec cum scriberem
nondum inteligebam
quid esset cenetem
Gravitatis
Si sit corpus Cylindricum, (quale est cylim
der, Rectangulum solidum, aliaque corpora,
quae fiunt ex ductu basis in altitudinem:)
abc. suspensum ex centro b. ita 
ratione cognita .... 
chium ab. sit majus, bc. minus; invenire
pondus d, quo appenso ex puncto C. bra-
cium bc. sit in aequilibrio cum brachio
ab.
Id quidem tam facile est, ut compendionas
artes quaerere non sit operae pretium.
Esto bc librae unius, ba trium, lentrum
gravitatis ab H. in medio e.  et centrum gra-
vitatis bc. in medio f. ergo si ab vel
aa bb. Suspensum intelligeretur ex e tan.
tundem ponde gravitarent, quantum nunc
cum centrum b. immedia attingunt. Porro
be. est triplum bf. Ergo si bb cc ex f.
valet unam libram, aa bb. ex e.  (curus ti-
stantia a centro b. triplo major est) valebit
libras novem, Ergo 8 librae ex centabf.
appendendae essent, ut bc. aequivaleat ipsi ab.
Sed cum ex duplo bf. nempe ex b c. suspendendae
sint, sufficiunt librae 4. Erit ergo pondus
 d librarum 4. quod erut ineniendum.
Eodem modo facile est per regressum dato pondere
d. et cylindrico ac. invenire punctum suspen.
sionis b. ut fiat brachiorum aequilibrium.
Sed iida Methodus, (qua corpus suppo-
nitur suspendi ex suo centro gravitatis)
non est Universalis, quod exemplo ostendo.
Esto in fig. 2. Triangulum aequilaterum EFG.
in fixum apice E mbrachio ab. quod conti–
nuatum incideret ncentrum Tria gravitatis A.
Trianguli supponatur latus Trianguli aequi-
lateri esse 3. crit altitud  93
seu R9. 27. s
cta in 3. , eu 4
moducto
143
diato
erit Area triangli 24.  ren eq. 4 d
Eda
tet be. exf.
+attudo F dh, R1 -