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

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            <p type="main">
              <s id="s.001204">
                <pb pagenum="234" xlink:href="010/01/242.jpg"/>
                <arrow.to.target n="marg312"/>
                <lb/>
              pla potentia P, ſed a duplici
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                <figure id="id.010.01.242.1.jpg" xlink:href="010/01/242/1.jpg" number="94"/>
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              potentia, tanquam à forcipe,
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              vel prælo, nempè à P, & ab
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              huic æquali reſiſtentia paui­
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              menti RS. </s>
              <s id="s.001205">Igitur æquè com­
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              primetur anulus, vel veſica
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              aerea ſolo innixa à ſingulari
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              potentia P, ac ſi à duabus contrarijs potentijs P, &
                <lb/>
              E, vel G conſtringeretur. </s>
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            <p type="margin">
              <s id="s.001206">
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              Cap. 5. de ae
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              ris grauitate
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              æquilibrio,
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              ſtructura, &
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              vi elateria
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              eius.</s>
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            <p type="main">
              <s id="s.001207">
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              COROLLARIVM.
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                <emph.end type="center"/>
              </s>
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            <p type="main">
              <s id="s.001208">HInc patet, quòd ſi duæ potentiæ æquales ſimul
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              coniunctæ comprimant eumdem ſupremum̨
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              anuli terminum pauimento innixi, tunc momentum̨
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              fiue energia, qua anulus contunditur ſtringiturquę
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              duplex eſt eius, qua ab ijſdem potentijs oppoſitos
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              terminos ſtringentibus comprimitur. </s>
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            <p type="main">
              <s id="s.001209">Quia quotieſcum que duæ potentiæ inter ſe æqua­
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              les P & G premunt ſupremum terminum B anuli BC,
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              tunc ſolum ſtabile RS in E, cui innititur idem præſtat,
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              & tanta energia operatur, ac ſi in E adeſſet potentią
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              æqualis ambabus contrarijs potentijs G & P: quare
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              vis, qua ſtringitur anulus æqualis eſt duplo potentia­
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              rum G, & P. è contrà quando anulus ſtringitur ab ijſ­
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              dem potentijs G, & P ſubdiuiſis, ſcilicèt à potentią
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              P in ſitu B, atque à potentia G in oppoſito eius ter­
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              mino C vt in præcedenti figura videre eſt, tunc vis,
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              qua ſtringitur anulus, æqualis eſt præcisè duabus po­
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              tentijs oppoſitis G, & P, igitur quando anulus ſolo </s>
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          </chap>
        </body>
      </text>
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