## Introduction to Mechanics of Deformable Solids |

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Page 15

3 / IDEALIZATIONS OF TIME - INDEPENDENT

majority of engineering applications of structural materials from metals to

concrete and ceramics to plastics and rubber , time independence of the stress -

strain ...

3 / IDEALIZATIONS OF TIME - INDEPENDENT

**BEHAVIOR**IN TENSION In themajority of engineering applications of structural materials from metals to

concrete and ceramics to plastics and rubber , time independence of the stress -

strain ...

Page 30

chapter 3 Time - dependent

AND RELAXATION Although time independence is a satisfactory approximation

to the

chapter 3 Time - dependent

**behavior**in tension and compression 3 . 1 / CREEPAND RELAXATION Although time independence is a satisfactory approximation

to the

**behavior**of structural materials in the majority of engineering applications ...Page 60

3 / IDEALIZATIONS OF MATERIAL

independent and the time - dependent

exhibit the same basic forms of response as the

compression .

3 / IDEALIZATIONS OF MATERIAL

**BEHAVIOR**IN SHEAR Both the time -independent and the time - dependent

**behavior**of material in simple shearexhibit the same basic forms of response as the

**behavior**in tension andcompression .

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### Common terms and phrases

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