Transformation of Strains
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Strain-Transformation equations are based on the geometry of the deformation of deformable bodies(including some small-angle approximations).
External strain , or normal strain, is defined as a ratio of a total elongation to an original length .
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Shear strain is defined as a change in angle between two originally perpendicular line segments that intersect at a point. When , angle the sheared line makes with its original orientation, equals 90 degrees, the shear strain is infinte.
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Normal and Shear Strain | |||||
The extensional strains and are determined by examining the change in length of short, mutually othogonal line segments and ; and the shear strains and are determined by the changes in right angles that originally exist between these lines. | |||||
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General Equations | |||||
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Principal Strains | |||||
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Maximum Shear Strains | |||||
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Mohr’s circle for two-dimensional Strain | |||||
Like the stress-transformation equations, the strain-transformation equations can be simplified bu introducing the double-angle trigonometric identities. This yields | |||||
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Therefore | |||||
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Equation of a circle in the plane with center at and radius R, with the angle being a parameter is | |||||
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