Steel01 Material: Difference between revisions

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| style="background:yellow; color:black; width:800px" | '''uniaxialMaterial Steel01 $matTag $Fy $E0 $b <$a1 $a2 $a3 $a4>'''
| style="background:lightgreen; color:black; width:800px" | '''uniaxialMaterial Steel01 $matTag $Fy $E0 $b <$a1 $a2 $a3 $a4>'''
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[[Image:Steel01HystereticC.jpg]]
[[Image:Steel01HystereticC.jpg]]
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NOTES:
* If strain-hardening ratio is zero and you do not expect softening of your system use BandSPD solver.


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Latest revision as of 00:46, 1 June 2013




This command is used to construct a uniaxial bilinear steel material object with kinematic hardening and optional isotropic hardening described by a non-linear evolution equation (REF: Fedeas).

uniaxialMaterial Steel01 $matTag $Fy $E0 $b <$a1 $a2 $a3 $a4>

$matTag integer tag identifying material
$Fy yield strength
$E0 initial elastic tangent
$b strain-hardening ratio (ratio between post-yield tangent and initial elastic tangent)
$a1 isotropic hardening parameter, increase of compression yield envelope as proportion of yield strength after a plastic strain of $a2*($Fy/E0). (optional)
$a2 isotropic hardening parameter (see explanation under $a1). (optional).
$a3 isotropic hardening parameter, increase of tension yield envelope as proportion of yield strength after a plastic strain of $a4*($Fy/E0). (optional)
$a4 isotropic hardening parameter (see explanation under $a3). (optional)


Steel01 Material -- Hysteretic Behavior of Model w/o Isotropic Hardening

Steel01 Material -- Hysteretic Behavior of Model with Isotropic Hardening in Compression

Steel01 Material -- Hysteretic Behavior of Model with Isotropic Hardening in Tension


NOTES:

  • If strain-hardening ratio is zero and you do not expect softening of your system use BandSPD solver.



Code Developed by: Filip Filippou, UC Berkeley

Images Developed by: Silvia Mazzoni