Introduction to Mechanics of Deformable Solids |
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Page 5
1 General Discussion of Stress 218 11 . 2 Principal Stresses in Two Dimensions (
Plane Stress ) 224 Principal values given 224 Stress components 0z , Oy , Try =
Tyz = 1 given 229 11 . 3 Problems of Two - dimensional States of Stress 234 11 ...
1 General Discussion of Stress 218 11 . 2 Principal Stresses in Two Dimensions (
Plane Stress ) 224 Principal values given 224 Stress components 0z , Oy , Try =
Tyz = 1 given 229 11 . 3 Problems of Two - dimensional States of Stress 234 11 ...
Page 30
Creep , the change in dimension with time at a given load , and relaxation , the
loss of stress with time at a given deformation , are two of the manifestations of
time effects . They often govern the useful life of turbines , engines and other ...
Creep , the change in dimension with time at a given load , and relaxation , the
loss of stress with time at a given deformation , are two of the manifestations of
time effects . They often govern the useful life of turbines , engines and other ...
Page 229
Similarly , results for the inclined plane i are given by a line from the pole at 30°
counterclockwise from the line to 1 . Figure 11 . 12 shows the planes of maximum
shear stress and the magnitudes and directions of the shear stress and the ...
Similarly , results for the inclined plane i are given by a line from the pole at 30°
counterclockwise from the line to 1 . Figure 11 . 12 shows the planes of maximum
shear stress and the magnitudes and directions of the shear stress and the ...
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actual addition angle answer applied assemblage axes axial axis beam behavior bending circle circular column combined compatibility components compression compressive stress Consider constant creep cross section curve cylinder deflection deformation determined diameter direction displacement effect elastic equal equation equilibrium example Figure Find force given gives homogeneous idealization increase initial interior isotropic length limit linear linear-elastic load material maximum Maxwell modulus moment needed nonlinear normal obtained outer plane plastic positive pressure principal Prob problem produced pure radius range ratio relation replaced requires residual response result rotation shaft shear stress shell shown shows simple sketch solid solution steel strain stress-strain relations structural Suppose surface symmetry temperature tensile tension thickness thin-walled torsion tube twisting uniform unloading versus viscous yield zero