Borelli, Giovanni Alfonso, De motionibus naturalibus a gravitate pendentibus, 1670

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              quieſcat, ſiue circa eius axim
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              M conuertatur libra ſemper
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              in ſitu horizontali æquilibra­
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              ta perſiſtet. </s>
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              Cap. 3. flui­
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              dum in ſuo
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              toto quie­
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              ſcens pon­
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              derat.</s>
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              <s id="s.000365">Vt verò ratio huius effectus
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              percipiatur, recurrendum eſt
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              ad centri grauitatis definitio­
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              nem, ex qua habetur quòd corpus quodlibet ſuſpen­
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              ſum à centro grauitatis eius quomodocumque reuol­
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              uatur circa centrum, ſemper æquilibrari, & haberę
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              partes æqualium momentorum, vnde infertur, quòd
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              vniuerſa vis, qua corpus aliquod
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              deorsùm, ſci­
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              licet grauitas eius, exercetur in vnico illo puncto,
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              quod centrum grauitatis eius vocatur. </s>
              <s id="s.000366">Hinc deduci­
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              tur, quod ſi rota, ſiuè pila ſuſtineatur ex centro gra­
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              uitatis eius ſiuè quieſcat, ſiuè moueatur, numquam
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              centrum grauitatis ſitum commutabit, aliàs daretur
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              motus perpetuus, qui naturæ legibus repugnat. </s>
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              <s id="s.000367">Similitèr ſi concipiatur fiſtula vitrea inflexa ad
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              modum anuli, vt eſt EFGK, ſitque prædicta fiſtulą
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              plena aqua ſituata perpendiculari­
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              tèr ſuper planum ſubiectum RS à
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              quo fulciatur; habebit profectò
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                trum</expan>
              grauitatis in eius puncto in­
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              termedio N, dum quieſcit aqua iņ
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              prædicto anulo, at ſi reuoluatur vt
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              nimirùm pars EFG deſcendat, reliqua verò GKE
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              ſursùm
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              , non proindè centrum grauitatis
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                feretur</expan>
              ab N versùs O, ſcilicèt intra ſemicirculum̨ </s>
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