Galilei, Galileo, Les méchaniques, 1634

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    <archimedes>
      <text>
        <body>
          <chap>
            <pb pagenum="7" xlink:href="047/01/027.jpg"/>
            <p type="head">
              <s id="s.000092">
                <emph type="center"/>
                <emph type="italics"/>
              Premiere definition.
                <emph.end type="italics"/>
                <emph.end type="center"/>
              </s>
            </p>
            <p type="main">
              <s id="s.000093">La
                <emph type="italics"/>
              peſanteur
                <emph.end type="italics"/>
              d'vn corps eſt l'inclina­
                <lb/>
              tion naturelle qu'il a pour ſe mouuoir,
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              & ſe porter en bas vers le centre de la
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              terre. </s>
              <s id="s.000094">Cette peſanteur ſe rencontre
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              dans les corps peſans à raiſon de la
                <expan abbr="quã-tité">quan­
                  <lb/>
                tité</expan>
              des parties materielles, dont ils
                <expan abbr="sõt">sont</expan>
                <lb/>
              compoſez; de ſorte qu'ils ſont dautant
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              plus peſans qu'ils ont vne plus grande
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              quantité deſdites parties ſouz vn meſ­
                <lb/>
              me volume. </s>
            </p>
            <p type="head">
              <s id="s.000095">
                <emph type="center"/>
                <emph type="italics"/>
              Deuxieſme definition.
                <emph.end type="italics"/>
                <emph.end type="center"/>
              </s>
            </p>
            <p type="main">
              <s id="s.000096">Le
                <emph type="italics"/>
              moment
                <emph.end type="italics"/>
              eſt l'inclination du meſ­
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              me corps, lors qu'elle n'eſt pas ſeule­
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              ment conſiderée dans ledit corps, mais
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              conioinctement auec la ſituation qu'il
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              a ſur le bras d'vn leuier, ou d'vne balan­
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              ce; & cette ſituation fait qu'il contre­
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              peſe ſouuent à vn plus grands poids, à
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              raiſon de ſa plus
                <expan abbr="grãde">grande</expan>
              diſtance d'auec
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              le centre de la balance. </s>
              <s id="s.000097">Car cet éloi­
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              gnement eſtant ioint à la propre peſan­
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              teur du corps peſant, luy
                <expan abbr="dõne">donne</expan>
              vne plus
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              forte inclination à deſcendre: de ſorte </s>
            </p>
          </chap>
        </body>
      </text>
    </archimedes>