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Nonlinear Static and Dynamic Analysis of Steel Structures with ...

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Chapter 2 Finite element modeling <strong>with</strong> ABAQUS/St<strong>and</strong>ard<br />

2.2 Structural elements<br />

There are six kinds <strong>of</strong> structural elements in Abaqus/St<strong>and</strong>ard; membrane, truss, beam,<br />

frame, elbow <strong>and</strong> shell elements. The most widely used are the beam-column <strong>and</strong> shell<br />

finite elements, which are discussed below.<br />

2.2.1 Beam elements<br />

Timoshenko beams (B21, B22, B31, B31OS, B32, B32OS, PIPE21, PIPE22, PIPE31,<br />

PIPE32, <strong>and</strong> their ―hybrid‖ equivalents) allow for transverse shear deformation. They can<br />

be used for thick (―stout‖) as well as slender beams. For beams made from uniform<br />

material, shear flexible beam theory can provide useful results for cross-sectional<br />

dimensions up to 1/8 <strong>of</strong> typical axial distances or the wavelength <strong>of</strong> the highest natural<br />

mode that contributes significantly to the response. Beyond this ratio the approximations<br />

that allow the member's behavior to be described solely as a function <strong>of</strong> axial position no<br />

longer provide adequate accuracy. It is assumed that the transverse shear behavior <strong>of</strong><br />

Timoshenko beams is linear elastic <strong>with</strong> a fixed modulus <strong>and</strong>, thus, independent <strong>of</strong> the<br />

response <strong>of</strong> the beam section to axial stretch <strong>and</strong> bending. The Timoshenko beams can be<br />

subjected to large axial strains. The axial strains due to torsion are assumed to be small. In<br />

combined axial-torsion loading, torsional shear strains are calculated accurately only when<br />

the axial strain is not large. The linear Timoshenko beam elements use a lumped mass<br />

formulation. The quadratic Timoshenko beam elements use a consistent mass formulation,<br />

except in dynamic procedures in which a lumped mass formulation <strong>with</strong> a 1/6, 2/3, 1/6<br />

distribution is used. The shear factor k (Cowper, 1966) is defined as:<br />

32<br />

Section type Shear factor, k<br />

Arbitrary 1.0<br />

Box 0.44<br />

Circular 0.89<br />

Elbow 0.85<br />

Generalized 1.0<br />

Hexagonal 0.53<br />

I (<strong>and</strong> T) 0.44<br />

L 1.0<br />

Meshed 1.0<br />

<strong>Nonlinear</strong> generalized 1.0<br />

Pipe 0.53<br />

Rectangular 0.85<br />

Trapezoidal 0.822<br />

Table 2.1: Shear factor k definition for Timoshenko beams

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