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

Table of figures

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            <p type="main">
              <s>
                <pb xlink:href="040/01/917.jpg" pagenum="224"/>
              Quantities, that is to ſay, of Spaces, of Times, and of
                <emph type="italics"/>
              Impetus's,
                <emph.end type="italics"/>
              let
                <lb/>
              it be required to determine in the aſſigned Space, and at the height
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              A C, how much the Time of the Fall of the Moveable from A to
                <lb/>
              C is to be, and what the
                <emph type="italics"/>
              Impetus
                <emph.end type="italics"/>
              is that ſhall be found to have been
                <lb/>
              acquired in the ſaid Term C, in relation to the Time and to the
                <lb/>
                <emph type="italics"/>
              Impetus
                <emph.end type="italics"/>
              meaſured by A B. </s>
              <s>Both theſe queſtions ſhall be reſolved
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              taking A D the Mean-proportional betwixt the two Lines A C
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              and A B; affirming the Time of the Fall along the whole Space
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              A C to be as the Time A D is in relation to A B, aſſigned in the
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              beginning for the Quantity of the Time in the Fall A B. </s>
              <s>And like­
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              wiſe we will ſay that the
                <emph type="italics"/>
              Impetus,
                <emph.end type="italics"/>
              or degree of Velocity that the
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              Cadent Moveable ſhall obtain in the Term C, in relation to the
                <lb/>
                <emph type="italics"/>
              Impetus
                <emph.end type="italics"/>
              that it had in B, is as the ſame Line A D is in relation to
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              A B, being that the Velocity encreaſeth with the ſame proportion
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              as the Time doth: Which Concluſion although it was aſſumed as
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              a
                <emph type="italics"/>
              Poſtulatum,
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              yet the Author was pleaſed to explain the Applicati­
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              on thereof above in the third Propoſition.</s>
            </p>
            <p type="main">
              <s>This point being well underſtood and proved, we come to the
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              Conſideration of the
                <emph type="italics"/>
              Impetus
                <emph.end type="italics"/>
              derived from two compound Moti­
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              ons: whereof let one be compounded of the Horizontal and alwaies
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              Equable, and of the Perpendicular unto the Horizon, and it alſo
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              Equable: but let the other be compounded of the Horizontal like­
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              wiſe alwaies Equable, and of the Perpendicular Naturally-Accele­
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              rate. </s>
              <s>If both ſhall be Equable, it hath been ſeen already that the
                <lb/>
                <emph type="italics"/>
              Impetus
                <emph.end type="italics"/>
              emerging from the compoſition of both is
                <emph type="italics"/>
              potentia
                <emph.end type="italics"/>
              equal to
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              both, as for more plainneſs we will thus Exemplifie. </s>
              <s>Let the Move­
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              able deſcending along the Perpendicular A B be ſuppoſed to have,
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              for example, three degrees of Equable
                <emph type="italics"/>
              Impetus,
                <emph.end type="italics"/>
              but being tranſ­
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              ported along A B towards C, let the ſaid Velocity and
                <emph type="italics"/>
              Impetus
                <emph.end type="italics"/>
              be
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              ſuppoſed four degrees, ſo that in the ſame Time that falling it would
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              paſs along the Perpendicular,
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              v. </s>
              <s>gr.
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              three yards,
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                <figure id="id.040.01.917.1.jpg" xlink:href="040/01/917/1.jpg" number="152"/>
                <lb/>
              it would in the Horizontal paſs four, but in
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              that compounded of both the Velocities it
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              cometh in the ſame Timefrom the point A un­
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              to the Term C, deſcending all the way along the Diagonal Line
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              A C, which is not ſeven yards long, as that ſhould be which is com­
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              pounded of the two Lines A B, 3, and B C, 4, but is 5; which 5 is
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                <emph type="italics"/>
              potentia
                <emph.end type="italics"/>
              equal to the two others, 3 and 4: For having found the
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              Squares of 3 and 4, which are 9 and 16, and joyning theſe together,
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              they make 25 for the Square of A C, which is equal to the two
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              Squares of A B and B C: whereupon A C ſhall be as much as is the
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              Side, or, if you will, Root of the Square 25, which is 5. For a conſtant
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              and certain Rule therefore, when it is required to aſſign the
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              Quantity of the
                <emph type="italics"/>
              Impetus
                <emph.end type="italics"/>
              reſulting from two
                <emph type="italics"/>
              Impetus's
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              given, the
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              one Horizontal, and the other Perpendicular, and both Equable, </s>
            </p>
          </chap>
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