## Introduction to Mechanics of Deformable Solids |

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Page 6

3 Pure Bending of Any Doubly Symmetric Arrangement of Bars 124 Linear -

elastic

3 Pure Bending of Any Doubly Symmetric Arrangement of Bars 124 Linear -

elastic

**response**127 Linear - viscous**response**129 Linear - viscoelastic**response**149 Elastic - perfectly plastic**response**130 Nonlinear - viscous**response**131 7 .Page 129

7 , any changes in moment which constitute unloading or which involve no plastic

action would produce the same

variation must be considered and ( 7 . 3 : 18 ) takes over as the appropriate form ,

with ...

7 , any changes in moment which constitute unloading or which involve no plastic

action would produce the same

**response**. If E varies from bar to bar , thevariation must be considered and ( 7 . 3 : 18 ) takes over as the appropriate form ,

with ...

Page 130

Suppose that the

the two loadings are applied simultaneously or with any time lag between them ,

the

Suppose that the

**response**to this loading has been calculated or observed . ... Ifthe two loadings are applied simultaneously or with any time lag between them ,

the

**response**of the system is simply the sum of the two**responses**calculated or ...### What people are saying - Write a review

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acting actual addition angle answer applied approximation assemblage axial force axis beam behavior bending circle circular column combined compatibility components compression compressive stress Consider constant creep cross section curve deflection deformation determined direction displacement effect elastic equal equation equations of equilibrium example Find force given gives homogeneous idealization increase initial interior isotropic length limit linear linear-elastic load material maximum Maxwell modulus moment nonlinear normal obtained plane plastic positive pressure principal Prob problem produced pure radius range ratio relation replaced requires response result rotation shear stress shell shown shows simple sketch solution solved statically steel strain stress-strain relations structural substitution Suppose surface symmetry temperature tensile tension tion tube twisting uniform virtual viscous yield zero