Salusbury, Thomas
,
Mathematical collections and translations (Tome I)
,
1667
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that the two augmentations of the Lengths and of the Gravities
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being put together, the Moment compounded of both is in double
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proportion to ei
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ther of them. </
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>We
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conclude there
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fore, That the Mo
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ments of the For
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ces of Priſmes and
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Cylinders of equal
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thickneſſe, but of
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unequal length, are
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to one another in
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duplicate proporti
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on to that of their
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Lengths; that is,
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are as the Squares of
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their Lengths.</
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>We will ſhew, in
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the ſecond place,
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according to what proportion the Reſiſtance of Fraction in Priſmes
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and Cylinders encreaſeth, when they continue of the ſame length,
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and encreaſe in thickneſs. </
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<
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>And here I ſay, that</
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>PROPOSITION IV.</
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In Priſmes and Cylinders of equal length, but unequal
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thickneſs, the Reſiſtance againſt Fraction encreaſeth
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in a proportion iriple to the Diameters of their
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Thickneſſes, that is, of their Baſes.
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<
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>Let the two Cylinders be theſe A and
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B, [as in
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Fig. </
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>5.]
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whoſe equal lengths are D G, and F H, the unequal
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B
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aſes
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the Circles, whoſe Diameters are C D, and E F. </
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>I ſay,
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that the Reſiſtance of the Cylinder
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B
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is to the Reſiſtance of the
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Cylinder A againſt Fraction, in a proportion triple to that which
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the Diameter F E hath to the Diameter D C. </
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<
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>For if we conſider
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the abſolute and ſimple Reſiſtance that reſides in the
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B
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aſes, that
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is, in the Circles E F, and D C to breaking, offering them vio
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lence by pulling them end-waies, without all doubt, the Reſiſtance
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of the Cylinder
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B,
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is ſo much greater than that of the Cylinder A,
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by how much the Circle E F is greater than C D; for the Fibres,
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Filaments, or tenacious parts, which hold together the Parts of the
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Solid, are ſo many the more.
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B
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ut if we conſider, that in offering </
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