## Introduction to Mechanics of Deformable Solids |

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Page 162

2 / SOLID BARS AND THICK - WALLED TUBES AS ASSEMBLAGES OF

concentric

analogous to the ...

2 / SOLID BARS AND THICK - WALLED TUBES AS ASSEMBLAGES OF

**THIN**-**WALLED**TUBES The extension of the previous results to any number ofconcentric

**thin**-**walled**tubes is straightforward . Again , the situation isanalogous to the ...

Page 175

1 / THICK - WALLED SPHERE The assembling of individually homogeneous

bars in tension and compression to form a beam was reasonably straightforward .

The assembling of homogeneous isotropic

...

1 / THICK - WALLED SPHERE The assembling of individually homogeneous

bars in tension and compression to form a beam was reasonably straightforward .

The assembling of homogeneous isotropic

**thin**-**walled**tubes in torsion to form a...

Page 186

Fixed spacing of two

the thick -

material . Try one which could be constructed with properly chosen metals and ...

Fixed spacing of two

**thin**shells Many choices seem possible for the simulation ofthe thick -

**walled**homogeneous sphere of isotropic elastic - perfectly plasticmaterial . Try one which could be constructed with properly chosen metals and ...

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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