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Principal material directions definition

Compare the transformed orthotropic compliances in Equation (2.88) with the anisotropic compliances in terms of engineering constants in Equation (2.91). Obviously an apparenf shear-extension coupling coefficient results when an orthotropic lamina is stressed in non-principal material coordinates. Redesignate the coordinates 1 and 2 in Equation (2.90) as X and y because, by definition, an anisotropic material has no principal material directions. Then, substitute the redesignated Sy from Equation (2.91) in Equation (2.88) along with the orthotropic compliances in Equation (2.62). Finally, the apparent engineering constants for an orthotropic iamina that is stressed in non-principal x-y coordinates are... [Pg.80]

What has been accomplished in preceding sections on stiffness relationships serves as the basis for determination of the actual stress field what remains is the definition of the allowable stress field. The first step in such a definition is the establishment of allowable stresses or strengths in the principal material directions. Such information is basic to the study of strength of an orthotropic lamina. [Pg.88]

Molecular sieves, however, are crystalline and have, therefore, an internal structure of regularly spaced cavities with interconnecting pores of definite size. Details of the properties peculiar to the various materials are best obtained directly from the manufacturer. The following is a brief description of these principal adsorbents. [Pg.415]


See other pages where Principal material directions definition is mentioned: [Pg.89]    [Pg.88]    [Pg.451]    [Pg.87]    [Pg.62]    [Pg.91]    [Pg.861]    [Pg.74]    [Pg.8]    [Pg.49]    [Pg.362]    [Pg.188]    [Pg.393]    [Pg.236]    [Pg.241]    [Pg.480]    [Pg.161]    [Pg.21]    [Pg.174]    [Pg.167]    [Pg.115]    [Pg.165]    [Pg.382]   
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Materials, definition

Principal directions

Principal material directions

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