Force-Based Beam-Column Element: Difference between revisions
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{{CommandManualMenu}} | {{CommandManualMenu}} | ||
This command is used to construct a | This command is used to construct a forceBeamColumn element object, which is based on the iterative force-based formulation. | ||
A variety of numerical integration options can be used in the element state determination and encompass both distributed plasticity and plastic hinge integration. See [[image:IntegrationTypes.pdf]] for more details on the available numerical integration options. | |||
{| | {| | ||
| style="background:yellow; color:black; width:800px" | '''element forceBeamColumn $eleTag $iNode $jNode | | style="background:yellow; color:black; width:800px" | '''element forceBeamColumn $eleTag $iNode $jNode $transfTag "IntegrationType arg1 arg2 ..." <-mass $massDens> <-iter $maxIters $tol>''' | ||
|} | |||
{| | |||
| style="width:150px" | '''$eleTag''' || unique element object tag | |||
|- | |||
|'''$iNode $jNode''' || end nodes | |||
|- | |||
| '''$transfTag''' || identifier for previously-defined coordinate-transformation (CrdTransf) object | |||
|- | |||
| '''IntegrationType arg1 arg2 ...''' || specifies locations and weights of integration points and their associated section force-deformation models (see [[image:IntegrationTypes.pdf]]) | |||
|- | |||
| '''$massDens''' || element mass density (per unit length), from which a lumped-mass matrix is formed (optional, default=0.0) | |||
|- | |||
| '''$maxIters''' || maximum number of iterations to undertake to satisfy element compatibility (optional, default=10) | |||
|- | |||
| '''$tol''' ||tolerance for satisfaction of element compatibility (optional, default=10-12) | |||
|} | |} | ||
Original command that assumes Gauss-Lobatto integration with a copy of the same section force-deformation model at each integration point: | |||
{| | {| | ||
| style="background:yellow; color:black; width:800px" | '''element forceBeamColumn $eleTag $iNode $jNode $numIntgrPts | | style="background:yellow; color:black; width:800px" | '''element forceBeamColumn $eleTag $iNode $jNode $numIntgrPts $secTag $transfTag <-mass $massDens> <-iter $maxIters $tol> <-integration $intType>''' | ||
|} | |||
{| | |||
| style="width:150px" | '''$eleTag''' || unique element object tag | |||
|- | |||
| '''$numIntgrPts''' || number of Gauss-Lobatto integration points along the element. | |||
|- | |||
| '''$secTag''' || identifier for previously-defined section object | |||
|} | |} | ||
Alternative command (kept for backward compatability) | Alternative command (kept for backward compatability): | ||
{| | {| | ||
| style="background:yellow; color:black; width:800px" | '''element nonlinearBeamColumn $eleTag $iNode $jNode $numIntgrPts $secTag $transfTag <-mass $massDens> <-iter $maxIters $tol> <-integration $intType>''' | | style="background:yellow; color:black; width:800px" | '''element nonlinearBeamColumn $eleTag $iNode $jNode $numIntgrPts $secTag $transfTag <-mass $massDens> <-iter $maxIters $tol> <-integration $intType>''' | ||
|} | |||
{| | |||
| style="width:150px" | '''$eleTag''' || unique element object tag | |||
|- | |||
| '''$intType''' || numerical integration type, options are Lobatto, Legendre, Radau, NewtonCotes, Trapezoidal (optional, default= Lobatto) | |||
|} | |} | ||
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---- | ---- | ||
NOTE: | |||
The following three commands give the same element definition (with Gauss-Lobatto integration) despite some apparent permutations of the input arguments: | |||
# element forceBeamColumn $eleTag $iNode $jNode $transfTag Lobatto $secTag $numIntgrPts | |||
# element forceBeamColumn $eleTag $iNode $jNode $numIntgrPts $secTag $transfTag | |||
# element nonlinearBeamColumn $eleTag $iNode $jNode $numIntgrPts $secTag $transfTag | |||
NOTE: | NOTE: | ||
#The -iter switch enables the iterative form of the flexibility formulation. Note that the iterative form can improve the rate of global convergence at the expense of more local element computation. | #The -iter switch enables the iterative form of the flexibility formulation. Note that the iterative form can improve the rate of global convergence at the expense of more local element computation. | ||
#The valid response elements that an element of this type will respond to are: | #The valid response elements that an element of this type will respond to are: | ||
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## localForce | ## localForce | ||
## basicForce | ## basicForce | ||
## section $ | ## section $sectionNumber $arg1 $arg2 ... (note: $sectionNumer is integer 1 through $numIntegrPts) | ||
## basicDeformation | ## basicDeformation | ||
## plasticDeformation | ## plasticDeformation | ||
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EXAMPLE: | EXAMPLE: | ||
element forceBeamColumn 1 2 4 5 | element forceBeamColumn 1 2 4 9 Lobatto 8 5; # force beam column element added with tag 1 between nodes 2 and 4 that has Gauss-Lobatto 5 integration points, each using section 8, and the element uses geometric transformation 9 | ||
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Code | Code maintained by: [http://web.engr.oregonstate.edu/~mhscott Michael H. Scott, Oregon State University] |
Latest revision as of 01:31, 11 April 2016
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This command is used to construct a forceBeamColumn element object, which is based on the iterative force-based formulation. A variety of numerical integration options can be used in the element state determination and encompass both distributed plasticity and plastic hinge integration. See File:IntegrationTypes.pdf for more details on the available numerical integration options.
element forceBeamColumn $eleTag $iNode $jNode $transfTag "IntegrationType arg1 arg2 ..." <-mass $massDens> <-iter $maxIters $tol> |
$eleTag | unique element object tag |
$iNode $jNode | end nodes |
$transfTag | identifier for previously-defined coordinate-transformation (CrdTransf) object |
IntegrationType arg1 arg2 ... | specifies locations and weights of integration points and their associated section force-deformation models (see File:IntegrationTypes.pdf) |
$massDens | element mass density (per unit length), from which a lumped-mass matrix is formed (optional, default=0.0) |
$maxIters | maximum number of iterations to undertake to satisfy element compatibility (optional, default=10) |
$tol | tolerance for satisfaction of element compatibility (optional, default=10-12) |
Original command that assumes Gauss-Lobatto integration with a copy of the same section force-deformation model at each integration point:
element forceBeamColumn $eleTag $iNode $jNode $numIntgrPts $secTag $transfTag <-mass $massDens> <-iter $maxIters $tol> <-integration $intType> |
$eleTag | unique element object tag |
$numIntgrPts | number of Gauss-Lobatto integration points along the element. |
$secTag | identifier for previously-defined section object |
Alternative command (kept for backward compatability):
element nonlinearBeamColumn $eleTag $iNode $jNode $numIntgrPts $secTag $transfTag <-mass $massDens> <-iter $maxIters $tol> <-integration $intType> |
$eleTag | unique element object tag |
$intType | numerical integration type, options are Lobatto, Legendre, Radau, NewtonCotes, Trapezoidal (optional, default= Lobatto) |
NOTE:
The following three commands give the same element definition (with Gauss-Lobatto integration) despite some apparent permutations of the input arguments:
- element forceBeamColumn $eleTag $iNode $jNode $transfTag Lobatto $secTag $numIntgrPts
- element forceBeamColumn $eleTag $iNode $jNode $numIntgrPts $secTag $transfTag
- element nonlinearBeamColumn $eleTag $iNode $jNode $numIntgrPts $secTag $transfTag
NOTE:
- The -iter switch enables the iterative form of the flexibility formulation. Note that the iterative form can improve the rate of global convergence at the expense of more local element computation.
- The valid response elements that an element of this type will respond to are:
- force or globalForce
- localForce
- basicForce
- section $sectionNumber $arg1 $arg2 ... (note: $sectionNumer is integer 1 through $numIntegrPts)
- basicDeformation
- plasticDeformation
- inflectionPoint
- tangentDrift
- integrationPoints
- integrationWeights
- Here is a link to the source code to obtain information about the location and weight of the Gauss-Lobatto integration points [1]
EXAMPLE:
element forceBeamColumn 1 2 4 9 Lobatto 8 5; # force beam column element added with tag 1 between nodes 2 and 4 that has Gauss-Lobatto 5 integration points, each using section 8, and the element uses geometric transformation 9
FURTHER DOCUMENTATION ON INTEGRATION OPTIONS:
REFERENCES:
- Neuenhofer, Ansgar, FC Filippou. Geometrically Nonlinear Flexibility-Based Frame Finite Element. ASCE Journal of Structural Engineering, Vol. 124, No. 6, June, 1998. ISSN 0733-9445/98/0006-0704-0711. Paper 16537. pp. 704-711.
- Neuenhofer, Ansgar, FC Filippou. Evaluation of Nonlinear Frame Finite-Element Models. ASCE Journal of Structural Engineering, Vol. 123, No. 7, July, 1997. ISSN 0733-9445/97/0007-0958-0966. Paper No. 14157. pp. 958-966.
- Neuenhofer, Ansgar, FC Filippou. ERRATA -- Geometrically Nonlinear Flexibility-Based Frame Finite Element. ASCE Journal of Structural Engineering, Vol. 124, No. 6, June, 1998. ISSN 0733-9445/98/0006-0704-0711. Paper 16537. pp. 704-711.
- Taucer, Fabio F, E Spacone, FC Filippou. A Fiber Beam-Column Element for Seismic Response Analysis of Reinforced Concrete Structures. Report No. UCB/EERC-91/17. Earthquake Engineering Research Center, College of Engineering, University of California, Berkeley. December 1991.
- Spacone, Enrico, V Ciampi, FC Filippou. A Beam Element for Seismic Damage Analysis. Report No. UCB/EERC-92/07. Earthquake Engineering Research Center, College of Engineering, University of California, Berkeley. August 1992.
Code maintained by: Michael H. Scott, Oregon State University