DelMonte, Guidubaldo, Le mechaniche

Table of figures

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              in Z; ma
                <foreign lang="el">*s</foreign>
              Z è eguale ad FG, eſſendo eguale ad X
                <foreign lang="grc">Υ</foreign>
              : dunque
                <foreign lang="el">*s</foreign>
              Z ſarà due
                <lb/>
              volte tanto, quanto OH. </s>
              <s id="id.2.1.882.3.0">Per laqual coſa mentre le poſſanze ſaranno in G
                <foreign lang="grc">Υ</foreign>
              , i
                <lb/>
              peſi AV ſaranno in OZ. </s>
              <s id="id.2.1.882.4.0">Hor nell'iſteſſo tempo ſaranno le poſſanze in G
                <foreign lang="grc">Υ</foreign>
              ,
                <lb/>
              peroche le vetocità de mouimenti ſono eguali: onde la forza di F mouerà il pe­
                <lb/>
              ſo A nel medeſimo tempo per la metà di quello ſpatio, per loquale il peſo V ſa
                <emph.end type="italics"/>
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                <figure id="id.037.01.164.1.jpg" xlink:href="037/01/164/1.jpg" number="154"/>
                <lb/>
                <emph type="italics"/>
              rà moſſo dalla poſſanza di X: & li peſi ſono eguali, adunque la poſſanza moue­
                <lb/>
              rà il peſo iſl eſſo in tempo eguale per la metà dello ſpatio, con la corda, & la taglia
                <lb/>
              legata in queſto modo al peſo, che ſenza taglia; purche le velocità della poſſanza
                <lb/>
              de'mouimenti ſiano eguali, che era da moſtrarſi.
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