Newton, Isaac, Philosophia naturalis principia mathematica, 1713

List of thumbnails

< >
341
341
342
342
343
343
344
344
345
345
346
346
347
347
348
348
349
349
350
350
< >
page |< < of 524 > >|
    <archimedes>
      <text>
        <body>
          <chap>
            <subchap1>
              <subchap2>
                <p type="main">
                  <s>
                    <pb xlink:href="039/01/344.jpg" pagenum="316"/>
                    <lb/>
                    <arrow.to.target n="note292"/>
                    <emph type="center"/>
                  PROPOSITIO XXXVIII. THEOREMA XXX.
                    <emph.end type="center"/>
                    <lb/>
                  </s>
                </p>
                <p type="margin">
                  <s>
                    <margin.target id="note292"/>
                  DE MOTU
                    <lb/>
                  CORPORUM</s>
                </p>
                <p type="main">
                  <s>
                    <emph type="italics"/>
                  Globi, in Fluido compreſſo infinito & non elaſtico uniformiter progre­
                    <lb/>
                  dientis, reſiſtentia eſt ad vim qua totus ejus motus, quo tempore
                    <lb/>
                  octo tertias partes diametri ſuæ deſcribit, vel tolli poſſit vel
                    <lb/>
                  generari, ut denſitas Fluidi ad denſitatem Globi quamproxime.
                    <emph.end type="italics"/>
                    <lb/>
                  </s>
                </p>
                <p type="main">
                  <s>Nam Globus eſt ad Cylindrum circumſcriptum ut duo ad tria;
                    <lb/>
                  & propterea Vis illa, quæ tollere poſſit motum omnem Cylindri
                    <lb/>
                  interea dum Cylindrus deſcribat longitudinem quatuor diametro­
                    <lb/>
                  rum, Globi motum omnem tollet interea dum Globus deſcribat
                    <lb/>
                  duas tertias partes hujus longitudinis, id eſt, octo tertias partes
                    <lb/>
                  diametri propriæ. Reſiſtentia autem Cylindri eſt ad hanc Vim
                    <lb/>
                  quamproxime ut denſitas Fluidi ad denſitatem Cylindri vel Globi,
                    <lb/>
                  per Prop.XXXVII; & Reſiſtentia Globi æqualis eſt Reſiſtentiæ Cy­
                    <lb/>
                  lindri, per Lem. V, VI, VII.
                    <emph type="italics"/>
                  Q.E.D.
                    <emph.end type="italics"/>
                    <lb/>
                  </s>
                </p>
                <p type="main">
                  <s>
                    <emph type="italics"/>
                  Corol.
                    <emph.end type="italics"/>
                  1. Globorum, in Mediis compreſſis infinitis, reſiſtentiæ ſunt
                    <lb/>
                  in ratione quæ componitur ex duplicata ratione velocitatis, & du­
                    <lb/>
                  plicata ratione diametri, & duplicata ratione denſitatis Mediorum.
                    <lb/>
                  </s>
                </p>
                <p type="main">
                  <s>
                    <emph type="italics"/>
                  Corol.
                    <emph.end type="italics"/>
                  2 Velocitas maxima quacum Globus, vi ponderis ſui com­
                    <lb/>
                  parativi, in fluido reſiſtente poteſt deſcendere, ea eſt quam acqui­
                    <lb/>
                  rere poteſt Globus idem, eodem pondere, abſque reſiſtentia caden­
                    <lb/>
                  do & caſu ſuo deſcribendo ſpatium quod ſit ad quatuor tertias
                    <lb/>
                  partes diametri ſuæ ut denſitas Globi ad denſitatem Fluidi. </s>
                  <s>Nam
                    <lb/>
                  Globus tempore caſus ſui, cum velocitate cadendo acquiſita, de­
                    <lb/>
                  ſcribet ſpatium quod erit ad octo tertias diametri ſuæ, ut denſitas
                    <lb/>
                  Globi ad denſitatem Fluidi; & vis ponderis motum hunc generans,
                    <lb/>
                  erit ad vim quæ motum eundem generare poſſit quo tempore Glo­
                    <lb/>
                  bus octo tertias diametri ſuæ eadem velocitate deſcribit, ut denſitas
                    <lb/>
                  Fluidi ad denſitatem Globi: ideoque per hanc Propoſitionem, vis
                    <lb/>
                  ponderis æqualis erit vi Reſiſtentiæ, & propterea Globum accele­
                    <lb/>
                  rare non poteſt.
                    <lb/>
                  </s>
                </p>
                <p type="main">
                  <s>
                    <emph type="italics"/>
                  Corol.
                    <emph.end type="italics"/>
                  3. Data & denſitate Globi & velocitate ejus ſub initio
                    <lb/>
                  motus, ut & denſitate fluidi compreſſi quieſcentis in qua Globus
                    <lb/>
                  movetur; datur ad omne tempus & velocitas Globi & ejus reſi­
                    <lb/>
                  ftentia & ſpatium ab eo deſcriptum, per Corol. 7. Prop. XXXV. </s>
                </p>
              </subchap2>
            </subchap1>
          </chap>
        </body>
      </text>
    </archimedes>