geometricallyExactBeamTest.py
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1#+++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
2# This is an EXUDYN example
3#
4# Details: Test models for GeometricallyExactBeam (2-node shear deformable beam,
5# Lie group formulation for work of elastic forces);
6# test models: cantilever beam with tip force and torque
7#
8# Author: Johannes Gerstmayr
9# Date: 2023-04-05
10#
11# 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.
12#
13#+++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
14
15import exudyn as exu
16from exudyn.utilities import * #includes itemInterface and rigidBodyUtilities
17from math import sin, cos
18import exudyn.graphics as graphics
19
20import numpy as np
21
22testIsActive = exu.sys.get('testIsActive', False)
23
24SC = exu.SystemContainer()
25mbs = SC.AddSystem()
26
27compute2D = False
28compute3D = True
29
30#test examples
31#2011 MUBO, Nachbagauer Pechstein Irschik Gerstmayr (2D)
32#2013 CND, Nachbagauer Gruber Gerstmayr (static, 3D); "Structural and Continuum Mechanics Approaches for a 3D Shear Deformable ANCF Beam Finite Element: Application to Static and Linearized Dynamic Examples"
33### not yet: 2013 CND, Nachbagauer Gerstmayr (dynamic, 3D)
34cases = ['CantileverLinear2011', 'Cantilever2011', 'GeneralBending2013', 'PrincetonBeamF2', 'PrincetonBeamF3', 'Eigenmodes2013']
35nElementsList = [1,2,4,8,16,32,64,128,256,512,1024]
36# nElementsList = [8,32, 128]
37nElements = 8
38
39betaList = [0,15,30,45,60,75,90]
40betaDegree = 45
41
42caseList = [0,1,2,3,4] #case 0 not working for Geometrically exact beam
43#case=2
44
45testIsActive = True
46verbose = 1*0
47
48useEP = True #for geometrically exact beam node
49if useEP:
50 NodeClass = NodeRigidBodyEP
51 initialRotationsGE = eulerParameters0
52else: #does not work for static case, as static solver currently (2023-04) cannot solve for Lie group nodes
53 NodeClass = NodeRigidBodyRotVecLG
54 initialRotationsGE = [0,0,0]
55
56
57bodyFixedLoad = False
58testErrorSum = 0
59case=4
60
61printCase = True
62#for nElements in nElementsList:
63#for betaDegree in betaList:
64for case in caseList:
65#if True:
66 if printCase:
67 printCase=False
68 exu.Print('case=', case, cases[case])
69 mbs.Reset()
70
71 computeEigenmodes = False
72 csFact = 1
73 sectionData = exu.BeamSection()
74 fTip = 0
75 MxTip = 0
76 MyTip = 0
77
78 ks1=1 #shear correction, torsion
79 ks2=1 #shear correction, bending
80 ks3=1 #shear correction, bending
81 ff=1 #drawing factor
82
83 if case == 0 or case == 1:
84 caseName = cases[case]
85
86 L = 2 #length of beam
87 w = 0.1 #width of beam
88 h = 0.5 #height Y
89
90 fTip = 5e5*h**3
91 if case == 1:
92 fTip *= 1000
93
94 Em = 2.07e11
95 rho = 1e2
96
97 A=h*w
98 nu = 0.3 # Poisson ratio
99 ks2= 10*(1+nu)/(12+11*nu)
100 ks3=ks2
101
102 elif case == 2:
103 L = 2 #length of beam
104 h = 0.2 #height Y
105 w = 0.4 #width Z of beam
106 Em = 2.07e11
107 rho = 1e2
108
109 A=h*w
110
111 nu = 0.3 # Poisson ratio
112 ks1= 0.5768 #torsion correction factor if J=Jyy+Jzz
113 ks2= 0.8331
114 ks3= 0.7961
115
116 MxTip = 0.5e6
117 MyTip = 2e6
118
119 csFact = 10
120 elif case == 3 or case == 4: #Princeton beam example
121 L = 0.508 #length of beam
122 h = 12.3777e-3 #height Y; 12.3777e-3 with Obrezkov's paper
123 w = 3.2024e-3 #width Z of beam
124 Em = 71.7e9
125 ks1=0.198
126 nu = 0.31
127
128 ks2=1
129 ks3=1
130 # ks2=0.9
131 # ks3=0.9
132
133
134 rho = 1e2 #unused
135 A=h*w
136
137 MxTip = 0
138 MyTip = 0
139 if case == 3:
140 fTip = 8.896 #F2
141 elif case == 4:
142 fTip = 13.345 #F3
143 #if kk==0: exu.Print('load=', fTip)
144
145 beta = betaDegree/180*pi #beta=0 => negative y-axis
146 bodyFixedLoad = False
147
148 csFact = 10
149
150 Gm = Em/(2*(1+nu)) # Shear modulus
151
152 # Cross-section properties
153 Iyy = h*w**3/12 # Second moment of area of the beam cross-section
154 Izz = w*h**3/12 # Second moment of area of the beam cross-section
155 J = (Iyy+Izz) # approximation; Polar moment of area of the beam cross-section
156
157 sectionData.stiffnessMatrix = np.diag([Em*A, Gm*A*ks2, Gm*A*ks3, Gm*J*ks1, Em*Iyy, Em*Izz])
158
159
160 rhoA = rho*A
161
162 if False:
163 #linear solution:
164 uzTip = fTip*L**3/(3*Em*Iyy)
165 exu.Print('uz linear=',uzTip)
166 uyTip = fTip*L**3/(3*Em*Izz)
167 exu.Print('uy linear=',uyTip)
168
169 sectionData.inertia= rho*J*np.eye(3)
170 sectionData.massPerLength = rhoA
171
172 sectionGeometry = exu.BeamSectionGeometry()
173
174 #points, in positive rotation sense viewing in x-direction, points in [Y,Z]-plane
175 #points do not need to be closed!
176 lp = exu.Vector2DList()
177 if True:
178 lp.Append([h*ff,-w*ff])
179 lp.Append([h*ff,w*ff])
180 lp.Append([-h*ff,w*ff])
181 lp.Append([-h*ff,-w*ff])
182
183 sectionGeometry.polygonalPoints = lp
184 #exu.Print('HERE\n',sectionGeometry.polygonalPoints)
185 nGround = mbs.AddNode(NodePointGround(referenceCoordinates=[0,0,0])) #ground node for coordinate constraint
186 mnGround = mbs.AddMarker(MarkerNodeCoordinate(nodeNumber=nGround, coordinate=0))
187
188
189 eY=[0,1,0]
190 eZ=[0,0,1]
191 lElem = L/nElements
192 useGeometricallyExact = True
193 if compute3D:
194 if useGeometricallyExact:
195 n0 = mbs.AddNode(NodeClass(referenceCoordinates=[0,0,0]+initialRotationsGE))
196 else:
197 initialRotations = eY+eZ
198 n0 = mbs.AddNode(NodePointSlope23(referenceCoordinates=[0,0,0]+initialRotations))
199 nInit = n0
200 for k in range(nElements):
201 if useGeometricallyExact:
202 n1 = mbs.AddNode(NodeClass(referenceCoordinates=[lElem*(k+1),0,0]+initialRotationsGE))
203
204 oBeam = mbs.AddObject(ObjectBeamGeometricallyExact(nodeNumbers=[n0,n1], length = lElem,
205 sectionData = sectionData,
206 visualization=VBeam3D(sectionGeometry=sectionGeometry)))
207 else:
208 n1 = mbs.AddNode(NodePointSlope23(referenceCoordinates=[lElem*(k+1),0,0]+initialRotations))
209 oBeam = mbs.AddObject(ObjectANCFBeam(nodeNumbers=[n0,n1], length = lElem,
210 #testBeamRectangularSize = [h,w],
211 sectionData = sectionData,
212 crossSectionPenaltyFactor = [csFact,csFact,csFact],
213 visualization=VANCFBeam(sectionGeometry=sectionGeometry)))
214 n0 = n1
215
216
217 mTip = mbs.AddMarker(MarkerNodeRigid(nodeNumber = n1))
218 if fTip != 0:
219 if case < 3:
220 mbs.AddLoad(Force(markerNumber=mTip, loadVector = [0,fTip,0], bodyFixed = bodyFixedLoad))
221 elif case >= 3:
222 mbs.AddLoad(Force(markerNumber=mTip, loadVector = [0,-fTip*cos(beta),fTip*sin(beta)], bodyFixed = bodyFixedLoad))
223
224 if MxTip != 0 or MyTip != 0:
225 mbs.AddLoad(Torque(markerNumber=mTip, loadVector = [MxTip, MyTip,0]))#, bodyFixed = True ))
226
227 if useGeometricallyExact:
228 nm0 = mbs.AddMarker(MarkerNodeRigid(nodeNumber=nInit))
229 nmGround = mbs.AddMarker(MarkerNodeRigid(nodeNumber=nGround))
230 mbs.AddObject(GenericJoint(markerNumbers=[nmGround, nm0]))
231 else:
232 for i in range(9):
233 #if i != 4 and i != 8: #exclude constraining the slope lengths
234 if True:
235 nm0 = mbs.AddMarker(MarkerNodeCoordinate(nodeNumber=nInit, coordinate=i))
236 mbs.AddObject(CoordinateConstraint(markerNumbers=[mnGround, nm0]))
237
238
239 # exu.Print(mbs)
240 mbs.Assemble()
241
242 tEnd = 100 #end time of simulation
243 stepSize = 0.5*0.01*0.1 #step size; leads to 1000 steps
244
245 simulationSettings = exu.SimulationSettings()
246 simulationSettings.solution.file.writePeriod = 2e-2 #output interval general
247 simulationSettings.solution.sensors.writePeriod = 1e-1 #output interval of sensors
248 simulationSettings.timeIntegration.numberOfSteps = int(tEnd/stepSize) #must be integer
249 simulationSettings.timeIntegration.endTime = tEnd
250 #simulationSettings.solution.file.information = "This is the info\nNew line\n and another new line \n"
251 simulationSettings.timeIntegration.generalizedAlpha.spectralRadius = 0.5
252 #simulationSettings.timeIntegration.realtime.active=True
253 #simulationSettings.timeIntegration.realtime.factor=0.1
254
255 simulationSettings.timeIntegration.verboseMode = verbose
256 simulationSettings.staticSolver.verboseMode = verbose
257
258 simulationSettings.timeIntegration.newton.useModifiedNewton = True
259 #simulationSettings.timeIntegration.newton.numericalDifferentiation.minimumCoordinateSize = 1e0
260
261 #simulationSettings.timeIntegration.newton.numericalDifferentiation.relativeEpsilon = 1e-4
262 simulationSettings.timeIntegration.newton.relativeTolerance = 1e-6
263
264 # simulationSettings.show.computationTime = True
265 simulationSettings.linearSolver.solverType = exu.LinearSolverType.EigenSparse
266
267 simulationSettings.staticSolver.numberOfLoadSteps = 5
268 simulationSettings.staticSolver.adaptiveStep = True
269 #simulationSettings.staticSolver.stabilizerODE2term = 100
270
271 if useGeometricallyExact:
272 # simulationSettings.staticSolver.newton.numericalDifferentiation.forODE2 = True
273 # simulationSettings.staticSolver.newton.numericalDifferentiation.relativeEpsilon = 1e-5
274 if case == 0:
275 simulationSettings.staticSolver.newton.relativeTolerance = 1e-4
276 simulationSettings.staticSolver.newton.absoluteTolerance = 1e-5
277 simulationSettings.staticSolver.numberOfLoadSteps = 1 #otherwise makes problems
278
279 if nElements > 32 and case==0: #change tolerance, because otherwise no convergence
280 simulationSettings.staticSolver.newton.relativeTolerance = 1e-6
281 if case == 1: #tolerance changed from 1e-8 to 5e-10 to achieve values of paper (1024 has difference at last digit in paper)
282 simulationSettings.staticSolver.newton.relativeTolerance = 0.5e-9
283
284
285
286 #add some drawing parameters for this example
287 SC.visualizationSettings.nodes.drawNodesAsPoint=False
288 SC.visualizationSettings.nodes.defaultSize=0.01
289
290 SC.visualizationSettings.bodies.beams.axialTiling = 50
291 SC.visualizationSettings.view0.scene.drawWorldBasis = True
292 SC.visualizationSettings.view0.scene.worldBasisSize = 0.1
293 SC.visualizationSettings.openGL.multiSampling = 4
294
295
296 # [M, K, D] = exu.solver.ComputeLinearizedSystem(mbs, simulationSettings, useSparseSolver=True)
297 # exu.Print('M=',M.round(1))
298
299 if not testIsActive:
300 SC.renderer.Start()
301 SC.renderer.DoIdleTasks()
302
303 mbs.SolveStatic(simulationSettings)
304 # mbs.SolveDynamic(simulationSettings)
305 #mbs.SolveDynamic(simulationSettings, solverType = exu.DynamicSolverType.RK44)
306
307 #check jacobian
308 if False:
309 #%%+++++++++++++++++++++++++++++++++++
310 solver=mbs.sys['staticSolver']
311 solver.InitializeSolver(mbs, simulationSettings)
312 solver.ComputeJacobianODE2RHS(mbs)
313 J=solver.GetSystemJacobian()
314 exu.Print((1e-6*J[:14,:7]).round(3))
315 exu.Print((1e-6*J[:14,7:14]).round(3))
316
317 #%%+++++++++++++++++++++++++++++++++++
318 if not testIsActive:
319 SC.renderer.DoIdleTasks()
320 SC.renderer.Stop() #safely close rendering window!
321
322 ##evaluate final (=current) output values
323 uTip = mbs.GetNodeOutput(n1, exu.OutputVariableType.Displacement)
324
325 errorFact = 1
326 if case != 1:
327 errorFact *= 100
328
329 testErrorSum += np.linalg.norm(uTip)
330
331
332
333 if case < 2:
334 pTip = mbs.GetNodeOutput(n1, exu.OutputVariableType.Position)
335 exu.Print('ne=',nElements, ', ux=',L-pTip[0], ', uy=',pTip[1])
336 elif case == 2:
337 rotTip = mbs.GetNodeOutput(n1, exu.OutputVariableType.Rotation)
338 exu.Print('ne=',nElements, ', u=',list(uTip))
339 # exu.Print('ne=',nElements, ', rot=',rotTip)
340 elif case == 3 or case == 4:
341 exu.Print('ne=', nElements, ', beta=', round(beta*180/pi,1), ', u=',uTip.round(7))
342
343
344exu.Print('Solution of geometricallyExactBeamTest=', testErrorSum)
345exu.sys['testResult'] = testErrorSum
346
347
348#+++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
349#all results are taken from ANCFBeam (shear deformable 2-node 3D beam):
350#+++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
351
352# case= 0/CantileverLinear2011
353#NachbagauerPechsteinIrschikGerstmayrMUBO2011 (2D):
354# ne=1, 9.12273046e–8, 6.16666566e–4, 0.000193
355# ne=2, 1.61293091e–7, 7.61594059e–4, 4.831e–5
356# ne=4, 1.81763233e–7, 7.97825954e–4, 1.208e–5
357# ne=256, 1.88847418e–7, 8.09900305e–4, 2.945e–9
358#Exudyn: ksFact=1
359# ne= 1 , ux= 9.122730637578513e-08 , uy= 0.0006166665660910789
360# ne= 2 , ux= 1.612930911054633e-07 , uy= 0.0007615940599560586
361# ne= 4 , ux= 1.8176323512975046e-07 , uy= 0.0007978259537503566
362# ne= 8 , ux= 1.8706537496804287e-07 , uy= 0.0008068839288072378
363# ne= 16 , ux= 1.8840244964124508e-07 , uy= 0.0008091484226773518
364# ne= 32 , ux= 1.887374359021976e-07 , uy= 0.0008097145461515286
365# ne= 64 , ux= 1.888212299849812e-07 , uy= 0.0008098560770202866
366# ne= 128 , ux= 1.8884218011550047e-07 , uy= 0.000809891459736643
367# ne= 256 , ux= 1.8884741770364144e-07 , uy= 0.0008099003054122335
368
369
370# case= 1/Cantilever2011
371#NachbagauerPechsteinIrschikGerstmayrMUBO2011 (2D):
372# ne=1, 0.07140274, 0.54225823, 0.168310
373# ne=2, 0.12379212, 0.65687111, 0.053697
374# ne=4, 0.14346767, 0.69593561, 0.014633
375# ne=1024, 0.15097103, 0.71056837, 2.280e–7
376
377#Exudyn: ksFact=1
378# ne= 1 , ux= 0.07140273975041422 , uy= 0.5422582285449739
379# ne= 2 , ux= 0.12379212054619537 , uy= 0.6568711099777776
380# ne= 4 , ux= 0.14346766617229956 , uy= 0.695935613449867
381# ne= 8 , ux= 0.14904162148449163 , uy= 0.7068152604035266
382# ne= 16 , ux= 0.15048521526298897 , uy= 0.709623891842095
383# ne= 32 , ux= 0.15084943688011565 , uy= 0.7103320154655514
384# ne= 64 , ux= 0.15094070328691145 , uy= 0.7105094267817303
385# ne= 128 , ux= 0.15096353326024237 , uy= 0.7105538037895819
386# ne= 256 , ux= 0.15096924149743085 , uy= 0.7105648993600513
387# ne= 512 , ux= 0.15097066651939461 , uy= 0.7105676689547459
388# ne= 1024 , ux= 0.15097102364723924 , uy= 0.7105683631862169
389
390# case = 2:
391#2013 CND, Nachbagauer Gruber Gerstmayr (static, 3D); "Structural and Continuum Mechanics Approaches for a 3D Shear Deformable ANCF Beam Finite Element: Application to Static and Linearized Dynamic Examples"
392#Table 4:
393# SMF
394# 8, 1.0943e-4, 1.8638e-4, 1.8117e-2
395# 32, 1.0943e-4, 1.8625e-4, 1.8117e-2
396# ANSYS
397# 40, 1.0939e-4, 1.8646e-4, 1.8117e-2
398#Exudyn, ksFact=10:
399# ne= 8 , u= [-0.00010900977088157404, -0.0001902100873246334, -0.01811732779800177]
400# ne= 32 , u= [-0.00010941122286522997, -0.00018667435478355072, -0.01811739809277171]
401# ne= 128 , u= [-0.00010943631319815239, -0.000186451835025629, -0.018117402461210096]
402#==> in 2013 paper, element performed slightly better, especially in ux and uy terms
403
404# case = 3:
405#Princeton beam with ANSYS (Leonid Obrezkov / Aki Mikkola / Marko Matikainen et al.,
406# Performance review of locking alleviation methods for continuum ANCF beam elements,
407# Nonlinear Dynamics, Vol. 109, pp. 31–546, May 2022
408# beta=[0 15 30 45 60 75 90];
409if (case==3 or case == 4) and False:
410 # F2=8.896
411 # % ANSYS beam (10-199 el)
412 ANSYSF2y=np.array([1.071417630E-002, 1.061328706E-002, 1.011169630E-002, 8.837226265E-003, 6.604665004E-003, 3.538889001E-003, 0])
413 ANSYSF2z=np.array([0, 4.208232124E-002, 7.939482948E-002, 0.108987937, 0.129887616, 0.142194370, 0.146245978])
414 exu.Print('refsol ANSYS F2=8.896:\n',ANSYSF2y.round(6), '\n', ANSYSF2z.round(6))
415 # % ANSYS solid (el) (4x12x500) - finer mesh doesn't have much influence see in Size effect file
416 # ANSYS_solid_y=[1.069752828E-002 1.057180106E-002 9.938278402E-003 8.686786771E-003 6.500006282E-003 3.481999513E-003 0];
417 # ANSYS_solid_z=[0 4.101165651E-002 7.696749069E-002 0.105976311 0.127251299 0.139594740 0.143848652];
418
419 # F3=13.345
420 # % ANSYS beam (10-199 el)
421 ANSYSF3y=np.array([1.606423724E-002, 1.645825752E-002, 1.665873206E-002, 1.518618440E-002, 1.157837500E-002, 6.248967384E-003, 0])
422 ANSYSF3z=np.array([0, 6.435812858E-002, 0.117735994, 0.156467239, 0.181861627, 0.196097131, 0.200677707])
423 # % ANSYS solid (el) (4x12x500) - finer mesh see in Size effect file
424 #ANSYS_solid_y=[1.603700622E-002 1.637026068E-002 1.640440775E-002 1.485055210E-002 1.127173264E-002 6.062461977E-003 0])
425 #ANSYS_solid_z=[0 6.270699533E-002 0.113752002 0.153554457 0.179978534 0.192972233 0.197669499])
426 exu.Print('refsol ANSYS F3=13.345:\n',ANSYSF3y.round(6), '\n', ANSYSF3z.round(6))
427#Exudyn results for Princeton beam:
428#not exactly the same, but around the previous values with HOTINT
429#using 16 elements, csFact=10 (no influence)
430# F2=8.896
431# case= 3, PrincetonBeam
432# ne= 16 , beta= 0.0 , u= [-0.0001352 -0.0107023 0. ]
433# ne= 16 , beta= 15.0 , u= [-0.0022414 -0.0106295 0.0421374]
434# ne= 16 , beta= 30.0 , u= [-0.0076567 -0.0101861 0.0794434]
435# ne= 16 , beta= 45.0 , u= [-0.0143664 -0.0089529 0.1089703]
436# ne= 16 , beta= 60.0 , u= [-0.0204225 -0.0067182 0.1297877]
437# ne= 16 , beta= 75.0 , u= [-0.0245093 -0.0036079 0.1420319]
438# ne= 16 , beta= 90.0 , u= [-0.0259403 -0. 0.1460608]
439
440# F3=13.345
441# case= 4, PrincetonBeam
442# ne= 16 , beta= 0.0 , u= [-0.0003039 -0.0160454 0. ]
443# ne= 16 , beta= 15.0 , u= [-0.005319 -0.0165469 0.064622 ]
444# ne= 16 , beta= 30.0 , u= [-0.0171901 -0.0169316 0.1179818]
445# ne= 16 , beta= 45.0 , u= [-0.0303357 -0.0155488 0.1565214]
446# ne= 16 , beta= 60.0 , u= [-0.0411035 -0.0118996 0.1817173]
447# ne= 16 , beta= 75.0 , u= [-0.0479101 -0.0064334 0.1958343]
448# ne= 16 , beta= 90.0 , u= [-0.0502184 -0. 0.2003738]