Salusbury, Thomas, Mathematical collections and translations (Tome I), 1667

List of thumbnails

< >
191
191
192
192
193
193
194
194
195
195
196
196
197
197
198
198
199
199
200
200
< >
page |< < of 701 > >|
    <archimedes>
      <text>
        <body>
          <chap>
            <pb xlink:href="040/01/279.jpg" pagenum="259"/>
            <p type="main">
              <s>SALV. </s>
              <s>I ſee that you underſtand the buſineſſe very well. </s>
              <s>I
                <lb/>
              lieve that you do likewiſe comprehend, that, in regard the ſtar B
                <lb/>
              is lower than C, the angle which is made by the rayes of the
                <lb/>
              ſight, which departing from the two places A and E, meet in C,
                <lb/>
              to wit, this angle A C E, is more narrow, or if we will ſay more
                <lb/>
              acute than the angle conſtituted in B, by the rayes A B and
                <lb/>
              E
                <emph type="italics"/>
              B.
                <emph.end type="italics"/>
              </s>
            </p>
            <p type="main">
              <s>SIMP. </s>
              <s>This I likewiſe underſtand very well.</s>
            </p>
            <p type="main">
              <s>SALV. </s>
              <s>And alſo, the Earth beine very little and almoſt
                <lb/>
              ſible, in reſpect of the Firmament
                <emph type="italics"/>
              (or Starry Sphere
                <emph.end type="italics"/>
              ;) and
                <lb/>
              ſequently the ſpace A E, paced on the Earth, being very ſmall in
                <lb/>
              compariſon of the immenſe length of the lines E G and E F,
                <lb/>
              ſing from the Earth unto the Firmament, you thereby collect that
                <lb/>
              the ſtar C might riſe and aſcend ſo much and ſo much above the
                <lb/>
              Earth, that the angle therein made by the rayes which depart
                <lb/>
              from the ſaid ſtationary points A and E, might become moſt
                <lb/>
              cute, and as it were abſolutely null and inſenſible.</s>
            </p>
            <p type="main">
              <s>SIMP. </s>
              <s>And this alſo is moſt manifeſt to ſenſe.</s>
            </p>
            <p type="main">
              <s>SALV. </s>
              <s>Now you know
                <emph type="italics"/>
              Simplicius
                <emph.end type="italics"/>
              that Aſtronomers and
                <lb/>
              thematicians have found infallible rules by way of Geometry and
                <lb/>
              Arithmetick, to be able by help of the quantity of theſe angles
                <lb/>
                <emph type="italics"/>
              B
                <emph.end type="italics"/>
              and C, and of their differences, with the additional knowledg
                <lb/>
              of the diſtance of the two places A and E, to find to a foot the
                <lb/>
              remoteneſſe of ſublime bodies; provided alwayes that the
                <lb/>
              ſaid diſtance, and angles be exactly taken.</s>
            </p>
            <p type="main">
              <s>SIMP. </s>
              <s>So that if the Rules dependent on
                <emph type="italics"/>
              Geometry
                <emph.end type="italics"/>
              and
                <emph type="italics"/>
                <lb/>
              nomy
                <emph.end type="italics"/>
              be true, all the fallacies and errours that might be met with
                <lb/>
              in attempting to inveſtigate thoſe altitudes of new Stars or
                <lb/>
              mets, or other things muſt of neceſſity depend on the diſtance A E,
                <lb/>
              and on the angles B and C, not well meaſured. </s>
              <s>And thus all thoſe
                <lb/>
              differences which are found in theſe twelve workings depend, not
                <lb/>
              on the deſects of the rules of the Calculations, but on the errours
                <lb/>
              committed in finding out thoſe angles, and thoſe diſtances, by means
                <lb/>
              of the Inſtrumental Obſervations.</s>
            </p>
            <p type="main">
              <s>SALV. True; and of this there is no doubt to be made. </s>
              <s>Now
                <lb/>
              it is neceſſary that you obſerve intenſely, how in removing the Star
                <lb/>
              from B to C, whereupon the angle alwayes grows more acute, the
                <lb/>
              ray E B G goeth farther and farther off from the ray A B D in
                <lb/>
              the part beneath the angle, as you may ſee in the line E C F,
                <lb/>
              whoſe inferiour part E C is more remote from the part A C, than
                <lb/>
              is the part E B, but it can never happen, that by any whatſoever
                <lb/>
              immenſe receſſion, the lines A D and E F ſhould totally ſever from
                <lb/>
              each other, they being finally to go and conjoyn in the Star: and
                <lb/>
              onely this may be ſaid, that they would ſeparate, and reduce
                <lb/>
              ſelves to parallels, if ſo be the receſſion ſhould be infinite, which </s>
            </p>
          </chap>
        </body>
      </text>
    </archimedes>