DelMonte, Guidubaldo, Le mechaniche

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    <archimedes>
      <text id="id.0.0.0.0.3">
        <body id="id.2.0.0.0.0">
          <chap id="N14EBE">
            <pb pagenum="82" xlink:href="037/01/179.jpg"/>
            <p id="id.2.1.959.0.0" type="main">
              <s id="id.2.1.959.1.0">Ma ſe in L ſarà la poſſanza, che moue il peſo. </s>
              <s id="id.2.1.959.2.0">Dico lo ſpatio
                <lb/>
              del peſo moſſo eſſere tre volte tanto, quanto lo ſpatio della
                <lb/>
              poſſanza moſſa. </s>
            </p>
            <p id="id.2.1.960.0.0" type="main">
              <s id="id.2.1.960.1.0">
                <emph type="italics"/>
              Mouaſi il centro della girella
                <lb/>
              K fin ad M, lo ſpatio
                <lb/>
              delquale mouimento è ve­
                <lb/>
              ramente eguale allo ſpatio
                <lb/>
              della poſſanza moſſa, co­
                <lb/>
              me è detto di ſopra: &
                <emph.end type="italics"/>
                <arrow.to.target n="note251"/>
                <lb/>
                <emph type="italics"/>
              quando K ſarà in M, B
                <lb/>
              ſarà in N, & NB ſa
                <lb/>
              rà eguale ad MK; &
                <lb/>
              mentre K è in M, fia il
                <lb/>
              peſo H, cioè il punto G
                <lb/>
              moſſo in O; & per MK
                <lb/>
              ſiano condotte le linee EF
                <lb/>
              PQ egualmente diſtanti
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              dall'orizonte; ſarà ciaſcu­
                <lb/>
              na delle EP BN FQ
                <lb/>
              eguale ad eſſa KM. </s>
              <s id="id.2.1.960.2.0">Et
                <lb/>
              percioche la coda BCD
                <lb/>
              EFG eguale è alla corda
                <lb/>
              NCDPQO; eſſendo
                <lb/>
              vna medeſima corda; &
                <lb/>
              la corda poſta intorno al
                <lb/>
              mezo cerchio ERF e­
                <lb/>
              guale è alla corda poſta in
                <lb/>
              torno al mezo cerchio
                <lb/>
              PSQ; tolte via dunque
                <lb/>
              le corde communi BC
                <lb/>
              DE, & FO, ſarà OG
                <lb/>
              eguale alle tre corde QF
                <lb/>
              NB PE preſe inſieme.
                <lb/>
              </s>
              <s id="id.2.1.960.3.0">ma QF NB PE in­
                <lb/>
              ſieme ſono tre volte tanto
                <lb/>
              quanto MK, cioè lo ſpa­
                <lb/>
              tio della poſſanza moſſa;
                <lb/>
              lo ſpatio dunque GO del
                <lb/>
              peſo H moſſo, è tre vol­
                <lb/>
              te tanto quanto è lo ſpa­
                <lb/>
              tio della poſſanza moſſa.
                <lb/>
              </s>
              <s id="id.2.1.960.4.0">che biſognaua moſtrare.
                <emph.end type="italics"/>
              </s>
            </p>
            <p id="id.2.1.961.0.0" type="margin">
              <s id="id.2.1.961.1.0">
                <margin.target id="note251"/>
                <emph type="italics"/>
              Nella precedente.
                <emph.end type="italics"/>
              </s>
            </p>
            <figure id="id.037.01.179.1.jpg" xlink:href="037/01/179/1.jpg" number="167"/>
          </chap>
        </body>
      </text>
    </archimedes>
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