Scientific American Supplement, No. 633, February 18, 1888 by Various
page 16 of 135 (11%)
page 16 of 135 (11%)
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AND STEEL.
BY GENERAL NICHOLAS KALAKOUTZKY. NO. I. _Determination of the Influence of Internal Stresses on the Strength of Materials._--We call internal stresses those which exist within the mass of any hollow cylinder or other body, when it appears to be in a state of repose, or not under the influence of external forces. When pressure is applied to a hollow cylinder, either externally or internally, the interior layers into which its walls may be conceived to be divided are subjected to a new series of stresses, the magnitude of which is independent of those already existing. These additional stresses combine with the former in such a manner that at every point of the thickness of the cylinder they have common resultants acting in various directions. Thus, if we call t the internal stress existing at a distance r_x from the axis of the cylinder, and in a direction tangential to its cross section, and T the additional stress due to pressure inside the cylinder acting at the same point and in the same direction, then the newly developed stress will be t + T. If R and r0 be the external and internal radii of the cylinder, and if we suppose the external pressure _nil_, then, if the pressure inside the bore be P0, the stress on the radius r_x is determined by the following expression deduced from the well-known fundamental formulæ of Lame:[1] r0² R² + (r_x)² |
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