## Analysis and Behavior of StructuresOffering students a presentation of classical structural analysis, this text emphasizes the limitations required in creating mathematical models for analysis, including these used in computer programs. Students are encouraged to use hand methods of analysis to develop a feel for the behaviour of structures. |

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Page 196

When constant shear is present with moment, the deformed

longer plane, but the normal strains still vary linearly through the depth. When

variable shear acts with moment, the normal strains no longer vary linearly with ...

When constant shear is present with moment, the deformed

**cross section**is nolonger plane, but the normal strains still vary linearly through the depth. When

variable shear acts with moment, the normal strains no longer vary linearly with ...

Page 199

The mathematical model does not include displacements of points in the

about the x axis. As a consequence, the theory cannot recognize lateral, torsional

...

The mathematical model does not include displacements of points in the

**cross****section**or along the member in the z direction or rotation of the**cross section**about the x axis. As a consequence, the theory cannot recognize lateral, torsional

...

Page 350

9.5a a rectangular

neutral axis, or axis of zero strain located a distance y from the bottom of the

variation is ...

9.5a a rectangular

**cross section**of height, h, and width, b, is shown with theneutral axis, or axis of zero strain located a distance y from the bottom of the

**cross section**. Taking the origin of the coordinate system at this point, the strainvariation is ...

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### Common terms and phrases

action analysis applied loads assumptions axial loads axis of symmetry behavior calculation centroidal chord column complementary virtual concentrated load conjugate beam constant cross section curvature diagram defined deformation system direct integration distributed load end moments equation of condition equations of equilibrium equilibrium equations Example Figure final moment diagram force in member forces and moments free body geometrically stable horizontal indeterminate influence line integration joint kips left end linear linear elastic loading diagram loads acting magnitude mathematical model maximum member forces ment method nonlinear materials numerical integration panel points portal frame positive reaction components rigid bodies rotation shown in Fig sign convention simply supported beam slope slope-deflection spreadsheet static determinacy statically determinate structures Step strains stress stress-strain relation struc structure of Fig summing moments superposition symmetric structure tion uniform load unit load unknown vertical deflection vertical displacement virtual force system virtual work principle zero