Introduction to Mechanics of Deformable Solids |
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Page 138
or ē ith and Ý h + 7 = - 4h 2 The centroidal - axis requirement for linear - elastic
response to pure bending ( ū = 0 for N = 0 ) brings to mind a previous and
complementary result ( Sec . 2.3 ) . If an axial force is to produce no bending , but
just ...
or ē ith and Ý h + 7 = - 4h 2 The centroidal - axis requirement for linear - elastic
response to pure bending ( ū = 0 for N = 0 ) brings to mind a previous and
complementary result ( Sec . 2.3 ) . If an axial force is to produce no bending , but
just ...
Page 151
29 shows the much more difficult situation when the z axis , or axis of bending , is
not an axis of symmetry . For an elastic - perfectly plastic material , the elastic
stress distribution of triangular shape goes over gradually to the fully plastic ...
29 shows the much more difficult situation when the z axis , or axis of bending , is
not an axis of symmetry . For an elastic - perfectly plastic material , the elastic
stress distribution of triangular shape goes over gradually to the fully plastic ...
Page 368
Bending about an axis which is not an axis of symmetry , or an axis perpendicular
to a plane of symmetry , or in general a principal axis of the cross section may
give rise to a very complex response . The neutral axis is not parallel to the axis
of ...
Bending about an axis which is not an axis of symmetry , or an axis perpendicular
to a plane of symmetry , or in general a principal axis of the cross section may
give rise to a very complex response . The neutral axis is not parallel to the axis
of ...
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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