.. _examples-ancfcantilevertestdyn: ************************ ANCFcantileverTestDyn.py ************************ You can view and download this file on Github: `ANCFcantileverTestDyn.py `_ .. code-block:: python :linenos: #+++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ # This is an EXUDYN example # # Details: Test with ANCF cantilever beam; excitation with a coordinate constraint which is changed by preStepExecute function # # Author: Johannes Gerstmayr # Date: 2019-10-25 # # Copyright:This file is part of Exudyn. Exudyn is free software. You can redistribute it and/or modify it under the terms of the Exudyn license. See 'LICENSE.txt' for more details. # #+++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ import exudyn as exu from exudyn.itemInterface import * import numpy as np SC = exu.SystemContainer() mbs = SC.AddSystem() #background rect = [-10,-10,10,10] #xmin,ymin,xmax,ymax background = {'type':'Line', 'color':[0.1,0.1,0.8,1], 'data':[rect[0],rect[1],0, rect[2],rect[1],0, rect[2],rect[3],0, rect[0],rect[3],0, rect[0],rect[1],0]} #background oGround=mbs.AddObject(ObjectGround(referencePosition= [0,0,0], visualization=VObjectGround(graphicsData= [background]))) #+++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ #cable: L=2 # length of ANCF element in m E=2.07e11 # Young's modulus of ANCF element in N/m^2 rho=7800 # density of ANCF element in kg/m^3 b=0.1 # width of rectangular ANCF element in m h=0.1 # height of rectangular ANCF element in m A=b*h # cross sectional area of ANCF element in m^2 I=b*h**3/12 # second moment of area of ANCF element in m^4 f=3*E*I/L**2 # tip load applied to ANCF element in N print("load f="+str(f)) nGround = mbs.AddNode(NodePointGround(referenceCoordinates=[0,0,0])) #ground node for coordinate constraint mGround = mbs.AddMarker(MarkerNodeCoordinate(nodeNumber = nGround, coordinate=0)) #Ground node ==> no action mode = 1 if mode==0: #treat one element nc0 = mbs.AddNode(Point2DS1(referenceCoordinates=[0,0,1,0])) nc1 = mbs.AddNode(Point2DS1(referenceCoordinates=[L,0,1,0])) o0 = mbs.AddObject(Cable2D(physicsLength=L, physicsMassPerLength=rho*A, physicsBendingStiffness=E*I, physicsAxialStiffness=E*A, nodeNumbers=[nc0,nc1])) print(mbs.GetObject(o0)) mANCF0 = mbs.AddMarker(MarkerNodeCoordinate(nodeNumber = nc0, coordinate=0)) mANCF1 = mbs.AddMarker(MarkerNodeCoordinate(nodeNumber = nc0, coordinate=1)) mANCF2b = mbs.AddMarker(MarkerNodeCoordinate(nodeNumber = nc0, coordinate=3)) mbs.AddObject(CoordinateConstraint(markerNumbers=[mGround,mANCF0])) ccy=mbs.AddObject(CoordinateConstraint(markerNumbers=[mGround,mANCF1]),offset=1e-6) mbs.AddObject(CoordinateConstraint(markerNumbers=[mGround,mANCF2b])) mANCFnode = mbs.AddMarker(MarkerNodePosition(nodeNumber=nc1)) #force mbs.AddLoad(Force(markerNumber = mANCFnode, loadVector = [0, 0, 0])) else: #treat n elements nc0 = mbs.AddNode(Point2DS1(referenceCoordinates=[0,0,1,0])) nElements = 16 lElem = L / nElements for i in range(nElements): nLast = mbs.AddNode(Point2DS1(referenceCoordinates=[lElem*(i+1),0,1,0])) mbs.AddObject(Cable2D(physicsLength=lElem, physicsMassPerLength=rho*A, physicsBendingStiffness=E*I, physicsAxialStiffness=E*A, nodeNumbers=[int(nc0)+i,int(nc0)+i+1])) mANCF0 = mbs.AddMarker(MarkerNodeCoordinate(nodeNumber = nc0, coordinate=0)) mANCF1 = mbs.AddMarker(MarkerNodeCoordinate(nodeNumber = nc0, coordinate=1)) mANCF2 = mbs.AddMarker(MarkerNodeCoordinate(nodeNumber = nc0, coordinate=3)) mbs.AddObject(CoordinateConstraint(markerNumbers=[mGround,mANCF0])) ccy=mbs.AddObject(CoordinateConstraint(markerNumbers=[mGround,mANCF1])) mbs.AddObject(CoordinateConstraint(markerNumbers=[mGround,mANCF2])) #mANCFLast = mbs.AddMarker(MarkerNodePosition(nodeNumber=nLast)) #force #nl=mbs.AddLoad(Force(markerNumber = mANCFLast, loadVector = [0, -f*0.01, 0])) #will be changed in load steps mbs.Assemble() print(mbs) simulationSettings = exu.SimulationSettings() #takes currently set values or default values def UFexcitation(mbs, t): mbs.SetObjectParameter(ccy, 'offset', 0.1*np.sin(2*np.pi*20*t)) return True #True, means that everything is alright, False=stop simulation mbs.SetPreStepUserFunction(UFexcitation) fact = 20000 simulationSettings.timeIntegration.numberOfSteps = 1*fact simulationSettings.timeIntegration.endTime = 0.000025*fact simulationSettings.solutionSettings.writeSolutionToFile = True simulationSettings.solutionSettings.solutionWritePeriod = simulationSettings.timeIntegration.endTime/fact simulationSettings.displayComputationTime = True simulationSettings.timeIntegration.verboseMode = 1 simulationSettings.timeIntegration.newton.relativeTolerance = 1e-8*1000 #10000 simulationSettings.timeIntegration.newton.absoluteTolerance = 1e-10*100 simulationSettings.timeIntegration.newton.useModifiedNewton = True simulationSettings.timeIntegration.newton.maxModifiedNewtonIterations = 5 simulationSettings.timeIntegration.newton.numericalDifferentiation.minimumCoordinateSize = 1 simulationSettings.timeIntegration.newton.numericalDifferentiation.relativeEpsilon = 6.055454452393343e-06*0.1 #eps^(1/3) simulationSettings.timeIntegration.newton.modifiedNewtonContractivity = 1000 simulationSettings.timeIntegration.generalizedAlpha.useIndex2Constraints = False simulationSettings.timeIntegration.generalizedAlpha.useNewmark = False simulationSettings.timeIntegration.generalizedAlpha.spectralRadius = 0.6 simulationSettings.displayStatistics = True simulationSettings.displayComputationTime = True #SC.visualizationSettings.nodes.showNumbers = True SC.visualizationSettings.bodies.showNumbers = False #SC.visualizationSettings.connectors.showNumbers = True SC.visualizationSettings.nodes.defaultSize = 0.01 simulationSettings.solutionSettings.solutionInformation = "nonlinear beam oscillations" SC.renderer.Start() mbs.SolveDynamic(simulationSettings) SC.renderer.DoIdleTasks() SC.renderer.Stop() #safely close rendering window!