# -------------------------------------------------------------------------------------------------- # Example 1. cantilever 2D # EQ ground motion with gravity # all units are in kip, inch, second # elasticBeamColumn ELEMENT # Silvia Mazzoni & Frank McKenna, 2006 # # ^Y # | # 2 __ # | | # | | # | | # (1) 36' # | | # | | # | | # =1= ---- -------->X # # SET UP ---------------------------------------------------------------------------- wipe; # clear opensees model model basic -ndm 2 -ndf 3; # 2 dimensions, 3 dof per node file mkdir Data; # create data directory # define GEOMETRY ------------------------------------------------------------- # nodal coordinates: node 1 0 0; # node#, X Y node 2 0 432 # Single point constraints -- Boundary Conditions fix 1 1 1 1; # node DX DY RZ # nodal masses: mass 2 5.18 1.e-9 0.; # node#, Mx My Mz, Mass=Weight/g. # Define ELEMENTS ------------------------------------------------------------- # define geometric transformation: performs a linear geometric transformation of beam stiffness and resisting force from the basic system to the global-coordinate system geomTransf Linear 1; # associate a tag to transformation # connectivity: (make A very large, 10e6 times its actual value) element elasticBeamColumn 1 1 2 3600000000 4227 1080000 1; # element elasticBeamColumn $eleTag $iNode $jNode $A $E $Iz $transfTag # Define RECORDERS ------------------------------------------------------------- recorder Node -file Data/DFree.out -time -node 2 -dof 1 2 3 disp; # displacements of free nodes recorder Node -file Data/DBase.out -time -node 1 -dof 1 2 3 disp; # displacements of support nodes recorder Node -file Data/RBase.out -time -node 1 -dof 1 2 3 reaction; # support reaction recorder Drift -file Data/Drift.out -time -iNode 1 -jNode 2 -dof 1 -perpDirn 2 ; # lateral drift recorder Element -file Data/FCol.out -time -ele 1 globalForce; # element forces -- column recorder Element -file Data/DCol.out -time -ele 1 deformations; # element deformations -- column # define GRAVITY ------------------------------------------------------------- pattern Plain 1 Linear { load 2 0. -2000. 0.; # node#, FX FY MZ -- superstructure-weight } constraints Plain; # how it handles boundary conditions numberer Plain; # renumber dof's to minimize band-width (optimization), if you want to system BandGeneral; # how to store and solve the system of equations in the analysis test NormDispIncr 1.0e-8 6 ; # determine if convergence has been achieved at the end of an iteration step algorithm Newton; # use Newton's solution algorithm: updates tangent stiffness at every iteration integrator LoadControl 0.1; # determine the next time step for an analysis, # apply gravity in 10 steps analysis Static # define type of analysis static or transient analyze 10; # perform gravity analysis loadConst -time 0.0; # hold gravity constant and restart time # DYNAMIC ground-motion analysis ------------------------------------------------------------- # create load pattern set accelSeries "Series -dt 0.01 -filePath BM68elc.acc -factor 1"; # define acceleration vector from file (dt=0.01 is associated with the input file gm) pattern UniformExcitation 2 1 -accel $accelSeries; # define where and how (pattern tag, dof) acceleration is applied rayleigh 0. 0. 0. [expr 2*0.02/pow([eigen 1],0.5)]; # set damping based on first eigen mode # create the analysis wipeAnalysis; # clear previously-define analysis parameters constraints Plain; # how it handles boundary conditions numberer Plain; # renumber dof's to minimize band-width (optimization), if you want to system BandGeneral; # how to store and solve the system of equations in the analysis test NormDispIncr 1.0e-8 10; # determine if convergence has been achieved at the end of an iteration step algorithm Newton; # use Newton's solution algorithm: updates tangent stiffness at every iteration integrator Newmark 0.5 0.25 ; # determine the next time step for an analysis analysis Transient; # define type of analysis: time-dependent analyze 1000 0.02; # apply 1000 0.02-sec time steps in analysis puts "Done!"