by the Axis at c and! C • ani d<Z A r ’ interce P te<1 
Canals of the Fluid gravitating A J tW0 Tubes or 
nicatingatC. I fay that ^. tovvar ^ s ’ and comma- 
Principles of Gravity the t0 ^ onf ‘ Mairan’s 
■•"s ^oidici 
: Is to the Gravity at tf:: As A wr Gra ™r at< * 
it will follow (from the Nature of the^IlTnfe/t! X , V* 
Gravity at A : will be m th* n • ^ Ul P le ) that the 
to dd and therefore the Fo S’S* ^ 7 A A ^ : 
lumns of Fluid A C and d C rend !■’ ] wblch t,le Co- 
their Malles drawn into the C ’ WlJ1 be as 
that is, as A C x A odJ r 5 drmn S “wards C, 
Principles of Hydroftaticks ;► j, X A' . ^ ow b f tk e 
in the Cam I A hTl? evldent th « the Fluid 
m rue^anat A C, will caule the Fluid in rl,„ r- 
to run out at d as Ion? as AC y m" Canal d C 
dCxdO: And if the Canal cA° ^7 than 
to the Surface of the F u id fn A C liT <I uite 
whilft the Surface of the F " j 7 .' Vl11 fink » «, 
which Cafe as * C = C / the IW a fa ■ u P t0 ^ in 
“nCf t ww e b A 
ssa a krjf' V s ^ 
rc^iK's^oi-'rSi 11 ^ = 
ufe of Sir Ifaac Newton's Principles in this R 7 f m . ake 
we fliall alfo Ihew, that an „S r i ;afomn & 
,he 
d--:As V cd: ^AU 7 
* Fig. II. 
NB. Afe/v 
