DelMonte, Guidubaldo, Le mechaniche

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          <chap id="N14EBE">
            <pb pagenum="88" xlink:href="037/01/191.jpg"/>
            <p id="id.2.1.1023.0.0" type="main">
              <s id="id.2.1.1023.1.0">Ma ſe in O ſarà la poſſan­
                <lb/>
              za che moua il peſo A.
                <lb/>
              </s>
              <s id="id.2.1.1023.2.0">Dico lo ſpatio corſo dal­
                <lb/>
              la poſſanza di O eſſere
                <lb/>
              vna volta & vn terzo tan­
                <lb/>
              to quanto è lo ſpatio del
                <lb/>
              peſo A moſſo. </s>
            </p>
            <p id="id.2.1.1024.0.0" type="main">
              <s id="id.2.1.1024.1.0">
                <emph type="italics"/>
              Stando le coſe medeſime, ſia il centro
                <lb/>
              B moſſo in P; & C fin in Q;
                <lb/>
              & D in R; & E in S nel­
                <lb/>
              l'iſteſſo tempo: & ſiano per li cen­
                <lb/>
              tri condotte le linee ML
                <foreign lang="el">*s</foreign>
              ZFG
                <lb/>
              TV HK X
                <foreign lang="grc">Υ</foreign>
              egualmente diſtan
                <lb/>
              ti, & dall' orizonte, & fra ſe ſteſ­
                <lb/>
              ſe: ſimilmente, come nella prece­
                <lb/>
              dente ſi dimoſtrerà, le tre corde
                <lb/>
              XH SE
                <foreign lang="grc">Υ</foreign>
              K eſſere eguali alle
                <lb/>
              quattro TG VF ZL
                <foreign lang="el">*s</foreign>
              M. </s>
              <s id="N16DD5">&
                <lb/>
              percioche le tre XH SE
                <foreign lang="grc">Υ</foreign>
              K ſo­
                <lb/>
              no inſieme tre volte tanto quanto
                <lb/>
              lo ſpatio della poſſanza: ma le
                <lb/>
              quattro TG VF ZL
                <foreign lang="el">*s</foreign>
              M in­
                <lb/>
              ſieme ſono quattro volte
                <expan abbr="tãto">tanto</expan>
              quan
                <lb/>
              to lo ſpatio del peſo moſſo; ſarà lo
                <lb/>
              ſpatio della poſſanza verſo lo ſpa­
                <lb/>
              tio del peſo, come la terza parte
                <lb/>
              alla quarta parte. </s>
              <s id="id.2.1.1024.2.0">Ma la terza
                <lb/>
              parte verſo la quarta parte è come
                <lb/>
              tre terzi à tre quarti, cioè come il
                <lb/>
              tutto verſo tre quarti, che è come
                <lb/>
              quattro verſo tre. </s>
              <s id="id.2.1.1024.3.0">Lo ſpatio dun­
                <lb/>
              que della poſſanza allo ſpatio del
                <lb/>
              peſo moſſo hà proportione di vna
                <lb/>
              volta & vn terzo. </s>
              <s id="id.2.1.1024.4.0">che era damo­
                <lb/>
              ſtrarſi.
                <emph.end type="italics"/>
              </s>
            </p>
            <figure id="id.037.01.191.1.jpg" xlink:href="037/01/191/1.jpg" number="177"/>
            <p id="id.2.1.1026.0.0" type="main">
              <s id="id.2.1.1026.1.0">
                <emph type="italics"/>
              Ma ſe la corda in E ſarà inuolta d'in
                <lb/>
              torno vn'altra girella, laqual cor­
                <emph.end type="italics"/>
              </s>
            </p>
          </chap>
        </body>
      </text>
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