Introduction to Mechanics of Deformable Solids |
From inside the book
Results 1-3 of 90
Page 4
1 Pure Bending of Plane Assemblages of Bars in Tension and Compression 111
Linear - elastic behavior 114 Elastic - perfectly plastic idealization 115 Linear -
work - hardening idealization 117 Linear Maxwell idealization 118 Nonlinear ...
1 Pure Bending of Plane Assemblages of Bars in Tension and Compression 111
Linear - elastic behavior 114 Elastic - perfectly plastic idealization 115 Linear -
work - hardening idealization 117 Linear Maxwell idealization 118 Nonlinear ...
Page 18
This geometric calculation is valid , but the linear - elastic idealization is no
longer applicable once appreciable plastic deformation occurs . Answers to
problems in practice and in class , which presume elastic behavior , must always
be ...
This geometric calculation is valid , but the linear - elastic idealization is no
longer applicable once appreciable plastic deformation occurs . Answers to
problems in practice and in class , which presume elastic behavior , must always
be ...
Page 102
Pi + P2 = Rc Pi + P2 = RY 002A2 Elastic solution PER PER Pi + P , = R | 004 , Pi '
+ P = 0 Line of residual states PiRLi PERL2 AETA EZ ( Elastic compatibility ) (
Equilibrium ) Fig . 6 . 5 Elastic - perfectly plastic tubes of Fig . 6 . 4 . Diagram
drawn ...
Pi + P2 = Rc Pi + P2 = RY 002A2 Elastic solution PER PER Pi + P , = R | 004 , Pi '
+ P = 0 Line of residual states PiRLi PERL2 AETA EZ ( Elastic compatibility ) (
Equilibrium ) Fig . 6 . 5 Elastic - perfectly plastic tubes of Fig . 6 . 4 . Diagram
drawn ...
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
acts actual addition angle answer applied assemblage axial axis beam behavior bending carry circle circular column combined compatibility components compression compressive stress Consider constant creep cross section curve deflection deformation determined diameter dimensions direction displacement effect elastic equal equation example Figure Find force given gives homogeneous idealization increase independent 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 response result rotation shear stress shell shown shows simple sketch solution steel strain stress-strain relations structural Suppose surface symmetry temperature tensile tension thickness thin-walled tube twisting uniform unloading versus viscous yield zero