## Introduction to mechanics of deformable solids |

### From inside the book

Results 1-3 of 71

Page 35

The higher the viscosity, i.e., the higher the value of C, the slower the application

of load can be to satisfy this definition. A

recovery. An abrupt release of load to zero value causes all further deformation to

...

The higher the viscosity, i.e., the higher the value of C, the slower the application

of load can be to satisfy this definition. A

**linear**-**viscous**material exhibits norecovery. An abrupt release of load to zero value causes all further deformation to

...

Page 197

Correspondingly, aa is a constant (9.3:23, 18),

viscoelastic materials The solution for the homogeneous isotropic linear-elastic

thick-walled cylinder carries over directly to our homogeneous isotropic

Correspondingly, aa is a constant (9.3:23, 18),

**Linear**-**viscous**and linear-viscoelastic materials The solution for the homogeneous isotropic linear-elastic

thick-walled cylinder carries over directly to our homogeneous isotropic

**linear**-**viscous**...Page 433

... 55, 56

also under Symmetry) Approximation (see Idealizations of material) Area, first

moment of ...

... 55, 56

**linear**elastic, 323**linear**Kelvin, 327**linear**Maxwell, 326 nonlinear**viscous**, 328 Anisotropy, 69, 216, 222, 266, 286 Antisymmetry, 112, 171 (Seealso under Symmetry) Approximation (see Idealizations of material) Area, first

moment of ...

### What people are saying - Write a review

We haven't found any reviews in the usual places.

### Other editions - View all

### Common terms and phrases

applied assemblage axial force beam behavior centroid circumferential column compatibility components of stress conditions of deformation constant creep cross section cylinder deflection diameter direction displacement elastic-perfectly plastic elongation equations of equilibrium factor of safety free-body sketch fully plastic homogeneous idealization increase inelastic initial interior pressure isotropic Kelvin Kelvin material limit linear Maxwell linear-elastic response linear-viscoelastic linear-viscous load maximum Maxwell material modulus Mohr's circle neutral axis nonlinear normal stress outer perfectly plastic perpendicular plane plastic deformation plastic-limit Poisson's ratio principal stresses Prob problem pure bending radial radius ratio rectangular residual stress rotation shaft shear strain shear stress shell shown in Fig simple shear solution statically statically determinate steel stress and strain stress-strain curve stress-strain relations Suppose surface symmetry temperature tensile stress thick-walled sphere thickness time-dependent tion torque torsion uniform unloading versus viscous yield curve yield stress zero