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# Title: Leibniz-Handschriften zur Varia Physica LH 37, 4
# Folio 170r, page id 00068606:0343
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VXZ spatium aeris gnte altera,
tionem, quod vocetur E. jam is voceturt
CT vel RQ vocetur L. habemus
B aequal. D plus A5 plus bis L e 
porgo
porro OR vocemus M, fit A aequal.  plus RS
plus L  plus E. ce similiter i casu aeris
seu bisL aequeal A bis A minus bis gR minus visAs
minus bis E. Erguesit  seu B minus D minusRs Ergo sit bhius D aequal
ergo sit D aequal B plus OR p RS minus bs A D plus bis E aequal. D minus bis A
minus bis E. Spatium egitur aer posse plus pRS. Similiter igitur
igitur post alterationem aerissp
translato  Hydrargyro ex PqRX Y in
FGASC, et vondo altitudinem Hydrargyri FG
quam nunc aer sustinet vocando M. a et aeris spatium CVXZ
spatium quod nunc soccupat vocando N, fit
M plus bis N aequal. D plus bis E B minus bis A
peus DRs, itaque M plus bis N aequal P phis bis E
jau
vicaloris aeris in 2Y
A  Hydrargyro ex DqR57 transtato in FGAsC
patet esse c t c. TC aequal 2G, rursus
TC aequal. PF. Ergo GF minus D P aequal. bis TC
eslere . GFmen 4 differ. si id est dus l seu vulmina
id est differentia inter duo sfetia velumina Me
Hdrargyri sustentati in diversis aeris secundum
calorem statibus seu inter GF et QP, est aequalis dp ipsi C7, dupla
differentiae inter volumina aeris ejusdem calore
differentis diversi CT, idemque concluditur si minuto
calore Hydrapgyrum ex PQRY in GH  RSX translatum ponamus
ad aequilibrium Dnsr magis accossisse ponamus, (a quo
ia
tamen semper longe abest,  sufficit V initium
pilae esse ex adverso iptius H puncti medii inter P et Z..)
nam op - H8 aequal. bis CK. et vero minuto calore nydram stu accedit
se ab Hydrurgyro acdit ad aequilibrium DRSV, quanquam id nunquam attingit, et
quanquam ge semper ab eo absit (itaque cum D sit
punctum medium inter P et a. quorum distantia deter.
minata est, potest pila v in V incipere ex
adverso ipsios nunero sumen aeris ante alte-
rationem docemus A, post alterationem B es ZXVC e ZK viemus NB, et alt tu dinem se
volumen  Hydrargyri aue
apte alterationem vocemus D
differentia inter ee aequalis auplae differentiae inter
A Et B. Sede vertus cFKXZ (id est A) pus CF e plus
sed rursus A seu TV. X Z plas CT, plus
porro volumen totius instrumenti OK S VXZ vocemus L
et votumen totius Hydrargori vocemus M patet fore
adenere edena ab aere ante alterationem susten A(hoc est VX Z) plus CF, plus M (seu CSRF) plus
uta
et sitest ptus   minus et per pus e mout
aequal. L. V
detur tam ac
+Tubi 
ats.  pe super aequilibrium gR5T
suspensa fuera
e
hurc; spaisis
adentis in
ex Y pesabcruit.  caloriem
ZXI
paer (ex ZVV F se ex pandensas
n ZXVC) translato in FGRSC
(ita ut _ pars Hydrargyr
jam suspensa sit super aequilibrium
GRSC) patet esse TC aequal
S
et tursus F C aequal. PF
generaliter sine discrimine caloris auct.
H voc mu M erio differentia inter Let
y
valus
uplae dfferentiae teA et B. Datu jam L et M ex
dantre qu differentia autem inter A et B
nemper
TC vet T_ (quae est C vel + K) vocemus _Pet
erit differentia inter LeM aequacis duptae N. Dantu
uteem
ispectione Tubi aquabiliter
crassi, cujus sunt partes s datur et A, seu capacitas ipsim
et Op sit N spatii L
pacita) ado pilae
14. eni
cujus quia ng
partis instrumenti in aequalite
19. ratio ad tubum aeque
alitu
huc
sum vel partes et
tum
Essitati
amissa
tas potuit ante quam
explovati Pati erg et B sea A +s vel A a A