Castelli, Benedetto, Of the mensuration of running waters, 1661

List of thumbnails

< >
11
11
12
12
13
13
14
14
15
15
16
16
17
17
18
18
19
19
20
20
< >
page |< < of 137 > >|
    <archimedes>
      <text>
        <body>
          <chap>
            <p type="main">
              <s>
                <pb xlink:href="068/01/084.jpg" pagenum="70"/>
              him be never ſo great a Wit, can never promiſe to frame a con­
                <lb/>
              ceit of the quantity of the Body of Water, without the third
                <lb/>
              Dimenſion of length: and hereupon I return to affirm, that the
                <lb/>
              vulgar Rule of meaſuring Running water is vain and erroneous.
                <lb/>
              </s>
              <s>This point being agreed on, I come to the ſecond, which is, Whe­
                <lb/>
              ther the third Dimenſion of length may be meaſured. </s>
              <s>And I ſay,
                <lb/>
              that if one would know the whole length of the water of a
                <lb/>
              Fountain or River, thereby to come to know the quantity of all
                <lb/>
              the Water, it would prove an impoſſible enterprize, nay the
                <lb/>
              knowing of it would not be uſeful. </s>
              <s>But if one would know how
                <lb/>
              much water a Fountain, or a River carrieth in a determinate time
                <lb/>
              of an hour, of a day, or of a moneth, &c. </s>
              <s>I ſay, that it is a very
                <lb/>
              poſſible and profitable enquiry, by reaſon of the innumerable
                <lb/>
              benefits that may be derived thence, it much importing to know
                <lb/>
              how much Water a Chanel carrieth in a time given; and I have
                <lb/>
              demonſtrated the ſame above in the beginning of this Book; and
                <lb/>
              of this we ſtand in need in the buſineſſe of the Lake, that ſo we
                <lb/>
              may be able to determine how much ſhall be the height of the
                <lb/>
                <emph type="italics"/>
              Brent,
                <emph.end type="italics"/>
              when it is ſpread all over the Lake: For the three dimen­
                <lb/>
              ſions of a Body being given, the Body is known; and the quan­
                <lb/>
              tity of a Body being given, if you have but two dimenſions, the
                <lb/>
              third ſhall be known. </s>
              <s>And thus diving farther and farther into
                <lb/>
              this Conſideration, I found that the Velocity of the courſe of the
                <lb/>
              water may be an hundred times greater or leſſer in one part of
                <lb/>
              its Chanel than in another. </s>
              <s>And therefore although there ſhould
                <lb/>
              be two mouths of Waters equal in bigneſſe; yet nevertheleſs it
                <lb/>
              might come to paſſe, that one might diſcharge an hundred or a
                <lb/>
              thouſand times more water than another: and this would be, if
                <lb/>
              the water in one of the mouths ſhould run with an hundred or a
                <lb/>
              thouſand times greater velocity, than the other; for that it
                <lb/>
              would be the ſame as to ſay, that the ſwifter was an hundred or
                <lb/>
              a thouſand times longer, than the ſlower: and in this manner I
                <lb/>
              diſcovered that to keep account of the velocity, was the keeping
                <lb/>
              account of the Length.</s>
            </p>
            <p type="main">
              <s>And therefore it is manifeſt, that when two Mouths diſcharge
                <lb/>
              the ſame quantity of Wa r in an equal velocity, it is neceſſary
                <lb/>
              that the leſs ſwift Mouth be ſo much bigger than the more ſwift;
                <lb/>
              as the more ſwift exceedeth in velocity the leſs ſwift; as for
                <lb/>
              example.</s>
            </p>
            <p type="main">
              <s>In caſe two Rivers ſhould carry equal quantity of water in
                <lb/>
              equal times, but that one of them ſhould be four times more
                <lb/>
              ſwift than the other, the more ſlow ſhould of neceſſity be four
                <lb/>
              times more large. </s>
              <s>And becauſe the ſame River in any part
                <lb/>
              thereof alwaies diſchargeth the ſame quantity of Water in equal
                <lb/>
              times (as is demonſtrated in the firſt Propoſition of the firſt </s>
            </p>
          </chap>
        </body>
      </text>
    </archimedes>