Archimedes, Natation of bodies, 1662

Table of figures

< >
[Figure 21]
[Figure 22]
[Figure 23]
[Figure 24]
[Figure 25]
[Figure 26]
[Figure 27]
[Figure 28]
[Figure 29]
[Figure 30]
[Figure 31]
[Figure 32]
[Figure 33]
[Figure 34]
[Figure 35]
[Figure 36]
[Figure 37]
[Figure 38]
[Figure 39]
[Figure 40]
[Figure 41]
[Figure 42]
[Figure 43]
[Figure 44]
[Figure 45]
[Figure 46]
[Figure 47]
[Figure 48]
[Figure 49]
[Figure 50]
< >
page |< < of 68 > >|
    <archimedes>
      <text>
        <body>
          <chap>
            <pb xlink:href="073/01/024.jpg" pagenum="353"/>
            <p type="head">
              <s>ARCHIMEDES,
                <lb/>
              HIS TRACT
                <lb/>
                <emph type="italics"/>
              DE
                <lb/>
              INSIDENTIBUS HUMIDO,
                <emph.end type="italics"/>
                <lb/>
              OR,
                <lb/>
              Of the NATATION of BODIES Upon, or
                <lb/>
              Submerſion In the WATER, or other LIQUIDS.</s>
            </p>
            <p type="head">
              <s>
                <emph type="italics"/>
              BOOK
                <emph.end type="italics"/>
              II.</s>
            </p>
            <p type="head">
              <s>PROP. I. THEOR. I.</s>
            </p>
            <p type="main">
              <s>
                <emph type="italics"/>
              If any Magnitude lighter than the Liquid be demitted
                <lb/>
              into the ſaid Liquid, it ſhall have the ſame proporti­
                <lb/>
              on in Gravity to a Liquid of equal Maſſe, that the
                <lb/>
              part of the Magnitude demerged hath unto the
                <lb/>
              whole Magnitude.
                <emph.end type="italics"/>
              </s>
            </p>
            <p type="main">
              <s>For let any Solid Magnitude, as for in­
                <lb/>
              ſtance F A, lighter than the Liquid, be de­
                <lb/>
              merged in the Liquid, which let be F A:
                <lb/>
              And let the part thereof immerged be A,
                <lb/>
              and the part above the Liquid F, It is to
                <lb/>
              be demonſtrated that the Magnitude F A
                <lb/>
              hath the ſame proportion in Gravity to a
                <lb/>
              Liquid of Equall Maſſe that A hath to F
                <lb/>
              A. </s>
              <s>Take any Liquid Magnitude, as ſup­
                <lb/>
              poſe N I, of equall Maſſe with F A; and let F be equall to N, and
                <lb/>
              A to I: and let the Gravity of the whole Magnitude F A be B, and
                <lb/>
              let that of the Magnitude N I be O,
                <lb/>
              and let that of I be R. </s>
              <s>Now the
                <lb/>
                <figure id="id.073.01.024.1.jpg" xlink:href="073/01/024/1.jpg" number="19"/>
                <lb/>
              Magnitude F A hath the ſame pro­
                <lb/>
              portion unto N I that the Gravity B
                <lb/>
              hath to the Gravity O R: But for
                <lb/>
              aſmuch as the Magnitude F A demit­
                <lb/>
              ted into the Liquid is lighter than
                <lb/>
              the ſaid Liquid, it is manifeſt that a Maſſe of the Liquid, I, equall
                <lb/>
              to the part of the Magnitude demerged, A, hath equall Gravity
                <lb/>
                <arrow.to.target n="marg1163"/>
                <lb/>
              with the whole Magnitnde, F A: For this was
                <emph type="italics"/>
              (a)
                <emph.end type="italics"/>
              above demon­
                <lb/>
              ſtrated: But B is the Gravity of the Magnitude F A, and R of I: </s>
            </p>
          </chap>
        </body>
      </text>
    </archimedes>