Galilei, Galileo, De Motu Antiquiora

Table of figures

< >
[Figure 41]
[Figure 42]
[Figure 43]
[Figure 44]
[Figure 45]
[Figure 46]
[Figure 47]
[Figure 48]
[Figure 49]
[Figure 50]
[Figure 51]
[Figure 52]
[Figure 53]
[Figure 54]
[Figure 55]
[Figure 56]
[Figure 57]
[Figure 58]
< >
page |< < of 383 > >|
    <archimedes>
      <text>
        <body>
          <chap>
            <subchap1>
              <subchap2>
                <p>
                  <s id="id.1.1.8.12.03">
                    <pb ed="manuscript" n="74r"/>
                  sursum, et tantae molis aquae; quanta est moles ligni, gravitas est 6, feretur iam lignum celeritate ut 2: quod si, rursus, idem lignum feratur sursum in medio aqua graviori, ita ut tantae molis huius secundi medii, quanta est moles ligni, gravitas sit 10, iam lignum in hoc feretur sursum celeritate ut </s>
                  <s id="id.1.1.8.12.04">In altero autem ferebatur celeritate ut 2: ergo istae duae celeritates erunt inter se sicut et 2; non autem ut gravitates aut crassities mediorum, ut volebat Aristoteles, quae sunt inter se ut 10 et </s>
                  <s id="id.1.1.8.12.05">Patet igitur, universaliter, celeritates inter se motuum sursum, esse, sicut excessus gravitatis unius medii super gravitatem
                    <lb ed="Favaro" n="30"/>
                  mobilis se habet ad excessum gravitatis alterius medii super gravitatem eiusdem </s>
                  <s id="id.1.1.8.12.06">Quare, si statim voluerimus cognoscere celeritates eiusdem mobilis in duobus mediis, accipiamus ex utroque medio duas moles aequales moli mobilis, et gravitas mobilis ex utriusque medii gravitate subtrahatur; et remanentes numeri erunt inter se sicut </s>
                </p>
              </subchap2>
            </subchap1>
          </chap>
        </body>
      </text>
    </archimedes>