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subdyn.py
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subdyn.py
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"""
Tools for SubDyn
- Setup a FEM model, compute Guyan and CB modes
- Get a dataframe with properties
- More todo
"""
import numpy as np
import pandas as pd
import matplotlib.pyplot as plt
import copy
import re
# Local
from pyFAST.io.fast_input_file import FASTInputFile
from pyFAST.tools.tictoc import Timer
idGuyanDamp_None = 0
idGuyanDamp_Rayleigh = 1
idGuyanDamp_66 = 2
class SubDyn:
def __init__(self, sdFilename_or_data=None):
"""
Initialize a SubDyn object either with:
- sdFilename: a subdyn input file name
- sdData: an instance of FASTInputFile
"""
self._graph=None
self.File=None
# Read SubDyn file
if sdFilename_or_data is not None:
if hasattr(sdFilename_or_data,'startswith'): # if string
self.File = FASTInputFile(sdFilename_or_data)
else:
self.File = sdFilename_or_data
self.M_tip=None
# Internal
self._graph=None
self._mgraph=None # Member graph
self._FEM=None
def __repr__(self):
s='<{} object>:\n'.format(type(self).__name__)
s+='|properties:\n'
s+='|- File: (input file data)\n'
s+='|* graph: (Nodes/Elements/Members)\n'
s+='|* pointsMJ, pointsMN, pointsMNout\n'
s+='|methods:\n'
s+='|- memberPostPro\n'
s+='|- setTopMass\n'
s+='|- beamDataFrame, beamFEM, beamModes\n'
s+='|- toYAMSData\n'
return s
# --------------------------------------------------------------------------------}
# --- Functions for general FEM model (jacket, flexible floaters)
# --------------------------------------------------------------------------------{
def init(self, TP=(0,0,0), gravity = 9.81):
"""
Initialize SubDyn FEM model
TP: position of transition point
gravity: position of transition point
"""
import welib.FEM.fem_beam as femb
import welib.FEM.fem_model as femm
BC = 'clamped-free' # TODO Boundary condition: free-free or clamped-free
element = 'frame3d' # Type of element used in FEM
FEMMod = self.File['FEMMod']
if FEMMod==1:
mainElementType='frame3d'
elif FEMMod==2:
mainElementType='frame3dlin'
elif FEMMod==3:
mainElementType='timoshenko'
else:
raise NotImplementedError()
# Get graph
graph = self.graph
#print('>>> graph\n',graph)
#graph.toJSON('_GRAPH.json')
# Convert to FEM model
with Timer('From graph'):
FEM = femm.FEMModel.from_graph(self.graph, mainElementType=mainElementType, refPoint=TP, gravity=gravity)
#model.toJSON('_MODEL.json')
with Timer('Assembly'):
FEM.assembly()
with Timer('Internal constraints'):
FEM.applyInternalConstraints()
FEM.partition()
with Timer('BC'):
FEM.applyFixedBC()
with Timer('EIG'):
Q, freq = FEM.eig(normQ='byMax')
with Timer('CB'):
FEM.CraigBampton(nModesCB = self.File['Nmodes'])
with Timer('Modes'):
FEM.setModes(nModesFEM=30, nModesCB=self.File['Nmodes'])
# FEM.nodesDisp(Q)
# --- SubDyn partition/notations
FEM.MBB = FEM.MM_CB[np.ix_(FEM.DOF_Leader_CB , FEM.DOF_Leader_CB)]
FEM.KBB = FEM.KK_CB[np.ix_(FEM.DOF_Leader_CB , FEM.DOF_Leader_CB)]
FEM.MBM = FEM.MM_CB[np.ix_(FEM.DOF_Leader_CB , FEM.DOF_Follower_CB)]
FEM.KMM = FEM.KK_CB[np.ix_(FEM.DOF_Follower_CB, FEM.DOF_Follower_CB)]
zeta =self.File['JDampings']/100
if not hasattr(zeta,'__len__'):
zeta = [zeta]*FEM.nModesCB
FEM.CMM = 2*np.array(zeta) * FEM.f_CB * 2 * np.pi
# --- Matrices wrt TP point
TI=FEM.T_refPoint
MBBt = TI.T.dot(FEM.MBB).dot(TI)
KBBt = TI.T.dot(FEM.KBB).dot(TI)
MBBt[np.abs(MBBt)<1e-4] =0
KBBt[np.abs(KBBt)<1e-4] =0
FEM.MBBt = MBBt
FEM.KBBt = KBBt
# --- Set Damping
dampMod = self.File['GuyanDampMod']
alpha_Rayleigh, beta_Rayleigh = None, None
# 6x6 Guyan Damping matrix
CC_CB_G = None
if dampMod == idGuyanDamp_None:
FEM.CBBt = np.zeros((6,6))
elif dampMod == idGuyanDamp_Rayleigh:
# Rayleigh Damping
alpha_Rayleigh, beta_Rayleigh = self.File['RayleighDamp']
FEM.CBBt = alpha_Rayleigh * FEM.MBBt + beta_Rayleigh * FEM.KBBt
elif dampMod == idGuyanDamp_66:
FEM.CBBt = self.File['GuyanDampMatrix']
else:
raise Exception()
# --- Compute rigid body equivalent
FEM.rigidBodyEquivalent()
self._FEM = FEM
return FEM
def setTopMass(self):
# TODO
# Add an optional top mass and ineria
if TopMass:
# NOTE: you can use welib.yams.windturbine to compute RNA mass and inertia
Mtop = 50000 # Top mass [kg]
M_tip= rigidBodyMassMatrixAtP(m=Mtop, J_G=None, Ref2COG=None)
else:
M_tip=None
def getGraph(self, nDiv=1):
# See welib.weio.fast_input_file_graph.py to see how SubDyn files are converted to graph
# See welib.fem.graph.py for Graph interface
_graph = self.File.toGraph().divideElements(nDiv,
excludeDataKey='Type', excludeDataList=['Cable','Rigid'], method='insert',
keysNotToCopy=['IBC','RBC','addedMassMatrix'] # Very important
)
if len(_graph.Members)==0:
raise Exception('Problem in graph subdivisions, no members found.')
# Sanitization
#idBC_Fixed = 0 # Fixed BC
#idBC_Internal = 10 # Free/Internal BC
#idBC_Leader = 20 # Leader DOF
MapIBC={0:0, 1:20} # 1 in the input file is leader
MapRBC={0:10, 1:0} # 1 in the input file is fixed
for n in _graph.Nodes:
#print(n)
if 'IBC' in n.data.keys():
IBC = n.data['IBC'].copy()
n.data['IBC'] = [MapIBC[i] for i in IBC[:6]]
if 'RBC' in n.data.keys():
RBC = n.data['RBC'].copy()
n.data['RBC'] = [MapRBC[i] for i in RBC[:6]]
if any(RBC[:6])==0:
print('RBC ',RBC)
print('n.data[RBC]',n.data['RBC'] )
print('n ',n )
raise NotImplementedError('SSI')
return _graph
@property
def graph(self):
if self._graph is None:
self._graph = self.getGraph(nDiv = self.File['NDiv'])
return copy.deepcopy(self._graph)
@property
def pointsMJ(self):
""" return a dataframe with the coordinates of all members and joints
The index corresponds to the SubDyn outputs "M_J_XXX"
"""
Joints=[]
labels =[]
graph = self.graph
for ie,M in enumerate(graph.Members): # loop on members
Nodes = M.getNodes(graph)
for iN,N in enumerate([Nodes[0], Nodes[-1]]):
s='M{}J{}'.format(ie+1, iN+1)
Joints.append([N.x,N.y,N.z])
labels.append(s)
df =pd.DataFrame(data=np.asarray(Joints), index=labels, columns=['x','y','z'])
return df
@property
def pointsMN(self):
""" return a dataframe with the coordinates of all members and nodes
The index would correspond to the SubDyn outputs "M_N_XXX *prior* to the user selection"
"""
Nodes=[]
labels =[]
graph = self.graph
for im,M in enumerate(graph.Members): # loop on members
nodes = M.getNodes(graph)
for iN,N in enumerate(nodes): # Loop on member nodes
s='M{}N{}'.format(im+1, iN+1)
Nodes.append([N.x,N.y,N.z])
labels.append(s)
df =pd.DataFrame(data=np.asarray(Nodes), index=labels, columns=['x','y','z'])
return df
@property
def pointsMNout(self):
""" return a dataframe with the coordinates of members and nodes requested by user
The index corresponds to the SubDyn outputs "M_N_XXX selected by the user"
"""
Nodes=[]
labels =[]
graph = self.graph
for im, out in enumerate(self.File['MemberOuts']):
mID = out[0] # Member ID
iNodes = np.array(out[2:])-1 # Node positions within member (-1 for python indexing)
nodes = graph.getMemberNodes(mID)
nodes = np.array(nodes)[iNodes]
for iN,N in enumerate(nodes): # Loop on selected nodes
s='M{}N{}'.format(im+1, iN+1)
Nodes.append([N.x,N.y,N.z])
labels.append(s)
df =pd.DataFrame(data=np.asarray(Nodes), index=labels, columns=['x','y','z'])
return df
def memberPostPro(self, dfAvg):
"""
Convert a dataframe of SubDyn/OpenFAST outputs (time-averaged)
with columns such as: M_N_* and M_J_*
into a dataframe that is organized by main channel name and nodal coordinates.
The scripts taken into account with member ID and node the user requested as outputs channels.
Discretization (nDIV) is also taken into account.
For instance:
dfAvg with columns = ['M1N1MKye_[N*m]', 'M1N2MKye_[N*m]', 'M1N1TDxss_[m]']
returns:
MNout with columns ['x', 'y', 'z', 'MKye_[Nm]', 'TDxss_[m]']
and index ['M1N1', 'M1N2']
with x,y,z the undisplaced nodal positions (accounting for discretization)
INPUTS:
- dfAvg: a dataframe of time-averaged SubDyn/OpenFAST outputs, for instance obtained as:
df = FASTInputFile(filename).toDataFrame()
dfAvg = postpro.averageDF(df, avgMethod=avgMethod ,avgParam=avgParam)
OUTPUTS
- MNout: dataframe of members outputs (requested by the user)
- MJout: dataframe of joints outputs
"""
import welib.fast.postpro as postpro # Import done here to avoid circular dependency
# --- Get Points where output are requested
MJ = self.pointsMJ
MNo= self.pointsMNout
MJ.columns = ['x_[m]','y_[m]', 'z_[m]']
MNo.columns = ['x_[m]','y_[m]', 'z_[m]']
# --- Requested Member Outputs
Map={}
Map['^'+r'M(\d*)N(\d*)TDxss_\[m\]'] = 'TDxss_[m]'
Map['^'+r'M(\d*)N(\d*)TDyss_\[m\]'] = 'TDyss_[m]'
Map['^'+r'M(\d*)N(\d*)TDzss_\[m\]'] = 'TDzss_[m]'
Map['^'+r'M(\d*)N(\d*)RDxe_\[rad\]'] = 'RDxe_[deg]' # NOTE rescale needed
Map['^'+r'M(\d*)N(\d*)RDye_\[rad\]'] = 'RDye_[deg]' # NOTE rescale needed
Map['^'+r'M(\d*)N(\d*)RDze_\[rad\]'] = 'RDze_[deg]' # NOTE rescale needed
Map['^'+r'M(\d*)N(\d*)FKxe_\[N\]'] = 'FKxe_[N]'
Map['^'+r'M(\d*)N(\d*)FKye_\[N\]'] = 'FKye_[N]'
Map['^'+r'M(\d*)N(\d*)FKze_\[N\]'] = 'FKze_[N]'
Map['^'+r'M(\d*)N(\d*)MKxe_\[N\*m\]'] = 'MKxe_[Nm]'
Map['^'+r'M(\d*)N(\d*)MKye_\[N\*m\]'] = 'MKye_[Nm]'
Map['^'+r'M(\d*)N(\d*)MKze_\[N\*m\]'] = 'MKze_[Nm]'
ColsInfo, _ = postpro.find_matching_columns(dfAvg.columns, Map)
nCols = len(ColsInfo)
if nCols>0:
newCols=[c['name'] for c in ColsInfo ]
ValuesM = pd.DataFrame(index=MNo.index, columns=newCols)
for ic,c in enumerate(ColsInfo):
Idx, cols, colname = c['Idx'], c['cols'], c['name']
labels = [re.match(r'(^M\d*N\d*)', s)[0] for s in cols]
ValuesM.loc[labels,colname] = dfAvg[cols].values.flatten()
if 'deg' in colname and 'rad' in cols[0]:
ValuesM[colname] *= 180/np.pi
# We remove lines that are all NaN
Values = ValuesM.dropna(axis = 0, how = 'all')
MNo2 = MNo.loc[Values.index]
MNout = pd.concat((MNo2, Values), axis=1)
else:
MNout = None
# --- Joint Outputs
Map={}
Map['^'+r'M(\d*)J(\d*)FKxe_\[N\]'] ='FKxe_[N]'
Map['^'+r'M(\d*)J(\d*)FKye_\[N\]'] ='FKye_[N]'
Map['^'+r'M(\d*)J(\d*)FKze_\[N\]'] ='FKze_[N]'
Map['^'+r'M(\d*)J(\d*)MKxe_\[N\*m\]']='MKxe_[Nm]'
Map['^'+r'M(\d*)J(\d*)MKye_\[N\*m\]']='MKye_[Nm]'
Map['^'+r'M(\d*)J(\d*)MKze_\[N\*m\]']='MKze_[Nm]'
Map['^'+r'M(\d*)J(\d*)FMxe_\[N\]'] ='FMxe_[N]'
Map['^'+r'M(\d*)J(\d*)FMye_\[N\]'] ='FMye_[N]'
Map['^'+r'M(\d*)J(\d*)FMze_\[N\]'] ='FMze_[N]'
Map['^'+r'M(\d*)J(\d*)MMxe_\[N\*m\]']='MMxe_[Nm]'
Map['^'+r'M(\d*)J(\d*)MMye_\[N\*m\]']='MMye_[Nm]'
Map['^'+r'M(\d*)J(\d*)MMze_\[N\*m\]']='MMze_[Nm]'
ColsInfo, _ = postpro.find_matching_columns(dfAvg.columns, Map)
nCols = len(ColsInfo)
if nCols>0:
newCols=[c['name'] for c in ColsInfo ]
ValuesJ = pd.DataFrame(index=MJ.index, columns=newCols)
for ic,c in enumerate(ColsInfo):
Idx, cols, colname = c['Idx'], c['cols'], c['name']
labels = [re.match(r'(^M\d*J\d*)', s)[0] for s in cols]
ValuesJ.loc[labels,colname] = dfAvg[cols].values.flatten()
# We remove lines that are all NaN
Values = ValuesJ.dropna(axis = 0, how = 'all')
MJ2 = MJ.loc[Values.index]
MJout = pd.concat((MJ2, Values), axis=1)
else:
MJout = None
return MNout, MJout
# --------------------------------------------------------------------------------}
# --- Functions for beam-like structure (Spar, Monopile)
# --------------------------------------------------------------------------------{
def beamDataFrame(self, equispacing=False):
""" """
# --- Parameters
UseSubDynModel=True
TopMass = False
# Convert to "welib.fem.Graph" class to easily handle the model (overkill for a monopile)
locgraph = self.graph.sortNodesBy('z')
# Add nodal properties from propsets (NOTE: Not done anymore by SubDyn because a same node can have different diameters...)
for e in locgraph.Elements:
locgraph.setElementNodalProp(e, propset=e.propset, propIDs=e.propIDs)
df = locgraph.nodalDataFrame()
if equispacing:
from welib.tools.pandalib import pd_interp1
# Interpolate dataframe to equispaced values
xOld = df['z'] # NOTE: FEM uses "x" as main axis
nSpan = len(xOld)
x = np.linspace(np.min(xOld),np.max(xOld), nSpan)
df = pd_interp1(x, 'z', df)
x = df['z'] # NOTE: FEM uses "x" as main axis
D = df['D'] # Diameter [m]
t = df['t'] # thickness [m]
# Derive section properties for a hollow cylinder based on diameter and thickness
A = np.pi*( (D/2)**2 - (D/2-t)**2) # Area for annulus [m^2]
I = np.pi/64*(D**4-(D-2*t)**4) # Second moment of area for annulus (m^4)
Kt = I # Torsion constant, same as I for annulus [m^4]
Ip = 2*I # Polar second moment of area [m^4]
df['A'] = A
df['I'] = I
df['Kt'] = Kt
df['Ip'] = Ip
df['m'] = df['rho'].values*A
return df
def beamFEM(self, df=None):
""" return FEM model for beam-like structures, like Spar/Monopile"""
import welib.FEM.fem_beam as femb
BC = 'clamped-free' # TODO Boundary condition: free-free or clamped-free
element = 'frame3d' # Type of element used in FEM
if df is None:
df = self.beamDataFrame()
x = df['z'] # NOTE: FEM uses "x" as main axis
E = df['E'] # Young modules [N/m^2]
G = df['G'] # Shear modules [N/m^2]
rho = df['rho'] # material density [kg/m^3]
Ip = df['Ip']
I = df['I']
A = df['A']
Kt = df['Kt']
# --- Compute FEM model and mode shapes
with Timer('Setting up FEM model'):
FEM=femb.cbeam(x,m=rho*A,EIx=E*Ip,EIy=E*I,EIz=E*I,EA=E*A,A=A,E=E,G=G,Kt=Kt,
element=element, BC=BC, M_tip=self.M_tip)
return FEM
def beamModes(self, nCB=8, FEM = None):
""" Returns mode shapes for beam-like structures, like Spar/Monopile """
import welib.FEM.fem_beam as femb
element = 'frame3d' # Type of element used in FEM
if FEM is None:
FEM = self.beamFEM()
# --- Perform Craig-Bampton reduction, fixing the top node of the beam
with Timer('FEM eigenvalue analysis'):
Q_G,_Q_CB, df_G, df_CB, Modes_G, Modes_CB, CB = femb.CB_topNode(FEM, nCB=nCB, element=element, main_axis='x')
# df_CB.to_csv('_CB.csv',index=False)
# df_G.to_csv('_Guyan.csv',index=False)
return Q_G,_Q_CB, df_G, df_CB, Modes_G, Modes_CB, CB
def beamModesPlot(self):
""" """
# TODO
nModesPlot=8
# --- Show frequencies to screen
print('Mode Frequency Label ')
for i in np.arange(8):
print('{:4d} {:10.3f} {:s}'.format(i+1,FEM['freq'][i],FEM['modeNames'][i]))
# --- Plot mode components for first few modes
print(x.shape)
#Q=FEM['Q'] ; modeNames = FEM['modeNames']
#Q=Q_CB ;modeNames = names_CB
Modes=Modes_CB
nModesPlot=min(len(Modes),nModesPlot)
fig,axes = plt.subplots(1, nModesPlot, sharey=False, figsize=(12.4,2.5))
fig.subplots_adjust(left=0.04, right=0.98, top=0.91, bottom=0.11, hspace=0.40, wspace=0.30)
for i in np.arange(nModesPlot):
key= list(Modes.keys())[i]
axes[i].plot(x, Modes[key]['comp'][:,0] ,'-' , label='ux')
axes[i].plot(x, Modes[key]['comp'][:,1] ,'-' , label='uy')
axes[i].plot(x, Modes[key]['comp'][:,2] ,'-' , label='uz')
axes[i].plot(x, Modes[key]['comp'][:,3] ,':' , label='vx')
axes[i].plot(x, Modes[key]['comp'][:,4] ,':' , label='vy')
axes[i].plot(x, Modes[key]['comp'][:,5] ,':' , label='vz')
axes[i].set_xlabel('')
axes[i].set_ylabel('')
axes[i].set_title(Modes[key]['label'])
if i==0:
axes[i].legend()
# --------------------------------------------------------------------------------}
# --- IO/Converters
# --------------------------------------------------------------------------------{
def toYAML(self, filename):
if self._FEM is None:
raise Exception('Call `initFEM()` before calling `toYAML`')
subdyntoYAMLSum(self._FEM, filename, more = self.File['OutAll'])
def toYAMSData(self, shapes=[0,4], main_axis='z'):
"""
Convert to Data needed to setup a Beam Model in YAMS (see bodies.py in yams)
"""
from welib.mesh.gradient import gradient_regular
# --- Perform Craig-Bampton reduction, fixing the top node of the beam
# Get beam data frame
df = self.beamDataFrame(equispacing=True)
if np.any(df['y']!=0):
raise NotImplementedError('FASTBeamBody for substructure only support monopile, structure not fully vertical in file: {}'.format(self.File.filename))
if np.any(df['x']!=0):
raise NotImplementedError('FASTBeamBody for substructure only support monopile, structure not fully vertical in file: {}'.format(self.File.filename))
FEM = self.beamFEM(df)
Q_G,_Q_CB, df_G, df_CB, Modes_G, Modes_CB, CB = self.beamModes(nCB=0, FEM=FEM)
x = df['z'].values
nSpan = len(x)
# TODO TODO finda way to use these matrices instead of the ones computed with flexibility
#print('CB MM\n',CB['MM'])
#print('CB KK\n',CB['KK'])
# --- Setup shape functions
if main_axis=='x':
raise NotImplementedError('')
else:
pass
# we need to swap the CB modes
nShapes=len(shapes)
PhiU = np.zeros((nShapes,3,nSpan)) # Shape
PhiV = np.zeros((nShapes,3,nSpan)) # Shape
PhiK = np.zeros((nShapes,3,nSpan)) # Shape
dx=np.unique(np.around(np.diff(x),4))
if len(dx)>1:
print(x)
print(dx)
raise NotImplementedError()
for iShape, idShape in enumerate(shapes):
if idShape==0:
# shape 0 "ux" (uz in FEM)
PhiU[iShape][0,:] = df_G['G3_uz'].values
PhiV[iShape][0,:] =-df_G['G3_ty'].values
PhiK[iShape][0,:] = gradient_regular(PhiV[iShape][0,:],dx=dx[0],order=4)
elif idShape==1:
# shape 1, "uy"
PhiU[iShape][1,:] = df_G['G2_uy'].values
PhiV[iShape][1,:] = df_G['G2_tz'].values
PhiK[iShape][1,:] = gradient_regular(PhiV[iShape][1,:],dx=dx[0],order=4)
elif idShape==4:
# shape 4, "vy" (vz in FEM)
PhiU[iShape][0,:] = df_G['G6_uy'].values
PhiV[iShape][0,:] = df_G['G6_tz'].values
PhiK[iShape][0,:] = gradient_regular(PhiV[iShape][0,:],dx=dx[0],order=4)
else:
raise NotImplementedError()
# --- Dictionary structure for YAMS
p=dict()
p['s_span']=x-np.min(x)
p['s_P0']=np.zeros((3,nSpan))
if main_axis=='z':
p['s_P0'][2,:]=x-np.min(x)
p['r_O'] = (df['x'].values[0], df['y'].values[0], df['z'].values[0])
p['R_b2g'] = np.eye(3)
p['m'] = df['m'].values
p['EI'] = np.zeros((3,nSpan))
if main_axis=='z':
p['EI'][0,:]=df['E'].values*df['I'].values
p['EI'][1,:]=df['E'].values*df['I'].values
p['jxxG'] = df['rho']*df['Ip'] # TODO verify
p['s_min'] = p['s_span'][0]
p['s_max'] = p['s_span'][-1]
p['PhiU'] = PhiU
p['PhiV'] = PhiV
p['PhiK'] = PhiK
# --- Damping
damp_zeta = None
RayleighCoeff = None
DampMat = None
if self.File['GuyanDampMod']==1:
# Rayleigh Damping
RayleighCoeff=self.File['RayleighDamp']
#if RayleighCoeff[0]==0:
# damp_zeta=omega*RayleighCoeff[1]/2.
elif self.File['GuyanDampMod']==2:
# Full matrix
DampMat = self.File['GuyanDampMatrix']
DampMat=DampMat[np.ix_(shapes,shapes)]
return p, damp_zeta, RayleighCoeff, DampMat
# --------------------------------------------------------------------------------}
# --- Export of summary file and Misc FEM variables used by SubDyn
# --------------------------------------------------------------------------------{
def yaml_array(var, M, Fmt='{:15.6e}', comment=''):
M = np.atleast_2d(M)
if len(comment)>0:
s='{}: # {} x {} {}\n'.format(var, M.shape[0], M.shape[1], comment)
else:
s='{}: # {} x {}\n'.format(var, M.shape[0], M.shape[1])
if M.shape[0]==1:
if M.shape[1]==0:
s+= ' - [ ]\n'
else:
for l in M:
s+= ' - [' + ','.join([Fmt.format(le) for le in l]) + ',]\n'
else:
for l in M:
s+= ' - [' + ','.join([Fmt.format(le) for le in l]) + ']\n'
s = s.replace('e+','E+').replace('e-','E-')
return s
def subdynPartitionVars(model):
from welib.FEM.fem_elements import idDOF_Leader, idDOF_Fixed, idDOF_Internal
# --- Count nodes per types
nNodes = len(model.Nodes)
nNodes_I = len(model.interfaceNodes)
nNodes_C = len(model.reactionNodes)
nNodes_L = len(model.internalNodes)
# --- Partition Nodes: Nodes_L = IAll - NodesR
Nodes_I = [n.ID for n in model.interfaceNodes]
Nodes_C = [n.ID for n in model.reactionNodes]
Nodes_R = Nodes_I + Nodes_C
Nodes_L = [n.ID for n in model.Nodes if n.ID not in Nodes_R]
# --- Count DOFs - NOTE: we count node by node
nDOF___ = sum([len(n.data['DOFs_c']) for n in model.Nodes])
# Interface DOFs
nDOFI__ = sum([len(n.data['DOFs_c']) for n in model.interfaceNodes])
nDOFI_B = sum([sum(np.array(n.data['IBC'])==idDOF_Leader) for n in model.interfaceNodes])
nDOFI_F = sum([sum(np.array(n.data['IBC'])==idDOF_Fixed ) for n in model.interfaceNodes])
if nDOFI__!=nDOFI_B+nDOFI_F: raise Exception('Wrong distribution of interface DOFs')
# DOFs of reaction nodes
nDOFC__ = sum([len(n.data['DOFs_c']) for n in model.reactionNodes])
nDOFC_B = sum([sum(np.array(n.data['RBC'])==idDOF_Leader) for n in model.reactionNodes])
nDOFC_F = sum([sum(np.array(n.data['RBC'])==idDOF_Fixed) for n in model.reactionNodes])
nDOFC_L = sum([sum(np.array(n.data['RBC'])==idDOF_Internal) for n in model.reactionNodes])
if nDOFC__!=nDOFC_B+nDOFC_F+nDOFC_L: raise Exception('Wrong distribution of reaction DOFs')
# DOFs of reaction + interface nodes
nDOFR__ = nDOFI__ + nDOFC__ # Total number, used to be called "nDOFR"
# DOFs of internal nodes
nDOFL_L = sum([len(n.data['DOFs_c']) for n in model.internalNodes])
if nDOFL_L!=nDOF___-nDOFR__: raise Exception('Wrong distribution of internal DOF')
# Total number of DOFs in each category:
nDOF__B = nDOFC_B + nDOFI_B
nDOF__F = nDOFC_F + nDOFI_F
nDOF__L = nDOFC_L + nDOFL_L
# --- Distibutes the I, L, C nodal DOFs into B, F, L sub-categories
# NOTE: order is importatn for compatibility with SubDyn
IDI__ = []
IDI_B = []
IDI_F = []
for n in model.interfaceNodes:
IDI__ += n.data['DOFs_c'] # NOTE: respects order
IDI_B += [dof for i,dof in enumerate(n.data['DOFs_c']) if n.data['IBC'][i]==idDOF_Leader]
IDI_F += [dof for i,dof in enumerate(n.data['DOFs_c']) if n.data['IBC'][i]==idDOF_Fixed ]
IDI__ = IDI_B+IDI_F
IDC__ = []
IDC_B = []
IDC_L = []
IDC_F = []
for n in model.reactionNodes:
IDC__ += n.data['DOFs_c'] # NOTE: respects order
IDC_B += [dof for i,dof in enumerate(n.data['DOFs_c']) if n.data['RBC'][i]==idDOF_Leader ]
IDC_L += [dof for i,dof in enumerate(n.data['DOFs_c']) if n.data['RBC'][i]==idDOF_Internal]
IDC_F += [dof for i,dof in enumerate(n.data['DOFs_c']) if n.data['RBC'][i]==idDOF_Fixed ]
IDR__=IDC__+IDI__
IDL_L = []
for n in model.internalNodes:
IDL_L += n.data['DOFs_c']
# Storing variables similar to SubDyn
SD_Vars={}
SD_Vars['nDOF___']=nDOF___;
SD_Vars['nDOFI__']=nDOFI__; SD_Vars['nDOFI_B']=nDOFI_B; SD_Vars['nDOFI_F']=nDOFI_F;
SD_Vars['nDOFC__']=nDOFC__; SD_Vars['nDOFC_B']=nDOFC_B; SD_Vars['nDOFC_F']=nDOFC_F; SD_Vars['nDOFC_L']=nDOFC_L;
SD_Vars['nDOFR__']=nDOFR__; SD_Vars['nDOFL_L']=nDOFL_L;
SD_Vars['nDOF__B']=nDOF__B; SD_Vars['nDOF__F']=nDOF__F; SD_Vars['nDOF__L']=nDOF__L;
SD_Vars['IDC__']=IDC__;
SD_Vars['IDC_B']=IDC_B;
SD_Vars['IDC_F']=IDC_F;
SD_Vars['IDC_L']=IDC_L;
SD_Vars['IDI__']=IDI__;
SD_Vars['IDR__']=IDR__;
SD_Vars['IDI_B']=IDI_B;
SD_Vars['IDI_F']=IDI_F;
SD_Vars['IDL_L']=IDL_L;
SD_Vars['ID__B']=model.DOFc_Leader
SD_Vars['ID__F']=model.DOFc_Fixed
SD_Vars['ID__L']=model.DOFc_Follower
return SD_Vars
def subdyntoYAMLSum(model, filename, more=False):
"""
Write a YAML summary file, similar to SubDyn
"""
# --- Helper functions
def nodeID(nodeID):
if hasattr(nodeID,'__len__'):
return [model.Nodes.index(model.getNode(n))+1 for n in nodeID]
else:
return model.Nodes.index(model.getNode(nodeID))+1
def elemID(elemID):
#e=model.getElement(elemID)
for ie,e in enumerate(model.Elements):
if e.ID==elemID:
return ie+1
def elemType(elemType):
from welib.FEM.fem_elements import idMemberBeam, idMemberCable, idMemberRigid
return {'SubDynBeam3d':idMemberBeam, 'SubDynFrame3d':idMemberBeam, 'Beam':idMemberBeam, 'Frame3d':idMemberBeam,
'SubDynTimoshenko3d':idMemberBeam,
'SubDynCable3d':idMemberCable, 'Cable':idMemberCable,
'Rigid':idMemberRigid,
'SubDynRigid3d':idMemberRigid}[elemType]
def propID(propID, propset):
prop = model.NodePropertySets[propset]
for ip, p in enumerate(prop):
if p.ID == propID:
return ip+1
SD_Vars = subdynPartitionVars(model)
# --- Helper functions
s=''
s += '#____________________________________________________________________________________________________\n'
s += '# RIGID BODY EQUIVALENT DATA\n'
s += '#____________________________________________________________________________________________________\n'
s0 = 'Mass: {:15.6e} # Total Mass\n'.format(model.M_O[0,0])
s += s0.replace('e+','E+').replace('e-','E-')
s0 = 'CM_point: [{:15.6e},{:15.6e},{:15.6e},] # Center of mass coordinates (Xcm,Ycm,Zcm)\n'.format(model.center_of_mass[0],model.center_of_mass[1],model.center_of_mass[2])
s += s0.replace('e+','E+').replace('e-','E-')
s0 = 'TP_point: [{:15.6e},{:15.6e},{:15.6e},] # Transition piece reference point\n'.format(model.refPoint[0],model.refPoint[1],model.refPoint[2])
s += s0.replace('e+','E+').replace('e-','E-')
s += yaml_array('MRB', model.M_O, comment = 'Rigid Body Equivalent Mass Matrix w.r.t. (0,0,0).')
s += yaml_array('M_P' , model.M_ref,comment = 'Rigid Body Equivalent Mass Matrix w.r.t. TP Ref point')
s += yaml_array('M_G' , model.M_G, comment = 'Rigid Body Equivalent Mass Matrix w.r.t. CM (Xcm,Ycm,Zcm).')
s += '#____________________________________________________________________________________________________\n'
s += '# GUYAN MATRICES at the TP reference point\n'
s += '#____________________________________________________________________________________________________\n'
s += yaml_array('KBBt' , model.KBBt, comment = '')
s += yaml_array('MBBt' , model.MBBt, comment = '')
s += yaml_array('CBBt' , model.CBBt, comment = '(user Guyan Damping + potential joint damping from CB-reduction)')
s += '#____________________________________________________________________________________________________\n'
s += '# SYSTEM FREQUENCIES\n'
s += '#____________________________________________________________________________________________________\n'
s += '#Eigenfrequencies [Hz] for full system, with reaction constraints (+ Soil K/M + SoilDyn K0) \n'
s += yaml_array('Full_frequencies', model.freq)
s += '#Frequencies of Guyan modes [Hz]\n'
s += yaml_array('GY_frequencies', model.f_G)
s += '#Frequencies of Craig-Bampton modes [Hz]\n'
s += yaml_array('CB_frequencies', model.f_CB)
s += '#____________________________________________________________________________________________________\n'
s += '# Internal FEM representation\n'
s += '#____________________________________________________________________________________________________\n'
s += 'nNodes_I: {:7d} # Number of Nodes: "interface" (I)\n'.format(len(model.interfaceNodes))
s += 'nNodes_C: {:7d} # Number of Nodes: "reactions" (C)\n'.format(len(model.reactionNodes))
s += 'nNodes_L: {:7d} # Number of Nodes: "internal" (L)\n'.format(len(model.internalNodes))
s += 'nNodes : {:7d} # Number of Nodes: total (I+C+L)\n'.format(len(model.Nodes))
if more:
s += 'nDOFI__ : {:7d} # Number of DOFs: "interface" (I__)\n'.format(len(SD_Vars['IDI__']))
s += 'nDOFI_B : {:7d} # Number of DOFs: "interface" retained (I_B)\n'.format(len(SD_Vars['IDI_B']))
s += 'nDOFI_F : {:7d} # Number of DOFs: "interface" fixed (I_F)\n'.format(len(SD_Vars['IDI_F']))
s += 'nDOFC__ : {:7d} # Number of DOFs: "reactions" (C__)\n'.format(len(SD_Vars['IDC__']))
s += 'nDOFC_B : {:7d} # Number of DOFs: "reactions" retained (C_B)\n'.format(len(SD_Vars['IDC_B']))
s += 'nDOFC_L : {:7d} # Number of DOFs: "reactions" internal (C_L)\n'.format(len(SD_Vars['IDC_L']))
s += 'nDOFC_F : {:7d} # Number of DOFs: "reactions" fixed (C_F)\n'.format(len(SD_Vars['IDC_F']))
s += 'nDOFR__ : {:7d} # Number of DOFs: "intf+react" (__R)\n'.format(len(SD_Vars['IDR__']))
s += 'nDOFL_L : {:7d} # Number of DOFs: "internal" internal (L_L)\n'.format(len(SD_Vars['IDL_L']))
s += 'nDOF__B : {:7d} # Number of DOFs: retained (__B)\n'.format(SD_Vars['nDOF__B'])
s += 'nDOF__L : {:7d} # Number of DOFs: internal (__L)\n'.format(SD_Vars['nDOF__L'])
s += 'nDOF__F : {:7d} # Number of DOFs: fixed (__F)\n'.format(SD_Vars['nDOF__F'])
s += 'nDOF_red: {:7d} # Number of DOFs: total\n' .format(SD_Vars['nDOF___'])
s += yaml_array('Nodes_I', nodeID([n.ID for n in model.interfaceNodes]), Fmt='{:7d}', comment='"interface" nodes"');
s += yaml_array('Nodes_C', nodeID([n.ID for n in model.reactionNodes ]), Fmt='{:7d}', comment='"reaction" nodes"');
s += yaml_array('Nodes_L', nodeID([n.ID for n in model.internalNodes ]), Fmt='{:7d}', comment='"internal" nodes"');
if more:
s += yaml_array('DOF_I__', np.array(SD_Vars['IDI__'])+1, Fmt='{:7d}', comment = '"interface" DOFs"')
s += yaml_array('DOF_I_B', np.array(SD_Vars['IDI_B'])+1, Fmt='{:7d}', comment = '"interface" retained DOFs')
s += yaml_array('DOF_I_F', np.array(SD_Vars['IDI_F'])+1, Fmt='{:7d}', comment = '"interface" fixed DOFs')
s += yaml_array('DOF_C__', np.array(SD_Vars['IDC__'])+1, Fmt='{:7d}', comment = '"reaction" DOFs"')
s += yaml_array('DOF_C_B', np.array(SD_Vars['IDC_B'])+1, Fmt='{:7d}', comment = '"reaction" retained DOFs')
s += yaml_array('DOF_C_L', np.array(SD_Vars['IDC_L'])+1, Fmt='{:7d}', comment = '"reaction" internal DOFs')
s += yaml_array('DOF_C_F', np.array(SD_Vars['IDC_F'])+1, Fmt='{:7d}', comment = '"reaction" fixed DOFs')
s += yaml_array('DOF_L_L', np.array(SD_Vars['IDL_L'])+1, Fmt='{:7d}', comment = '"internal" internal DOFs')
s += yaml_array('DOF_R_' , np.array(SD_Vars['IDR__'])+1, Fmt='{:7d}', comment = '"interface&reaction" DOFs')
s += yaml_array('DOF___B', np.array(model.DOFc_Leader )+1, Fmt='{:7d}', comment='all retained DOFs');
s += yaml_array('DOF___F', np.array(model.DOFc_Fixed )+1, Fmt='{:7d}', comment='all fixed DOFs');
s += yaml_array('DOF___L', np.array(model.DOFc_Follower)+1, Fmt='{:7d}', comment='all internal DOFs');
s += '\n'
s += '#Index map from DOF to nodes\n'
s += '# Node No., DOF/Node, NodalDOF\n'
s += 'DOF2Nodes: # {} x 3 (nDOFRed x 3, for each constrained DOF, col1: node index, col2: number of DOF, col3: DOF starting from 1)\n'.format(model.nDOFc)
DOFc2Nodes = model.DOFc2Nodes
for l in DOFc2Nodes:
s +=' - [{:7d},{:7d},{:7d}] # {}\n'.format(l[1]+1, l[2], l[3], l[0]+1 )
s += '# Node_[#] X_[m] Y_[m] Z_[m] JType_[-] JDirX_[-] JDirY_[-] JDirZ_[-] JStff_[Nm/rad]\n'
s += 'Nodes: # {} x 9\n'.format(len(model.Nodes))
for n in model.Nodes:
s += ' - [{:7d}.,{:15.3f},{:15.3f},{:15.3f},{:14d}., 0.000000E+00, 0.000000E+00, 0.000000E+00, 0.000000E+00]\n'.format(nodeID(n.ID), n.x, n.y, n.z, int(n.data['Type']) )
s += '# Elem_[#] Node_1 Node_2 Prop_1 Prop_2 Type Length_[m] Area_[m^2] Dens._[kg/m^3] E_[N/m2] G_[N/m2] shear_[-] Ixx_[m^4] Iyy_[m^4] Jzz_[m^4] T0_[N]\n'
s += 'Elements: # {} x 16\n'.format(len(model.Elements))
for e in model.Elements:
I = e.inertias
s0=' - [{:7d}.,{:7d}.,{:7d}.,{:7d}.,{:7d}.,{:7d}.,{:15.3f},{:15.3f},{:15.3f},{:15.6e},{:15.6e},{:15.6e},{:15.6e},{:15.6e},{:15.6e},{:15.6e}]\n'.format(
elemID(e.ID), nodeID(e.nodeIDs[0]), nodeID(e.nodeIDs[1]), propID(e.propIDs[0], e.propset), propID(e.propIDs[1], e.propset), elemType(e.data['Type']),
e.length, e.area, e.rho, e.E, e.G, e.kappa, I[0], I[1], I[2], e.T0)
s += s0.replace('e+','E+').replace('e-','E-')
s += '#____________________________________________________________________________________________________\n'
s += '#User inputs\n'
s += '\n'
s += '#Number of properties (NProps):{:6d}\n'.format(len(model.NodePropertySets['Beam']))
s += '#Prop No YoungE ShearG MatDens XsecD XsecT\n'
for ip,p in enumerate(model.NodePropertySets['Beam']):
s0='#{:8d}{:15.6e}{:15.6e}{:15.6e}{:15.6e}{:15.6e}\n'.format(p.ID, p['E'],p['G'],p['rho'],p['D'],p['t'])
s += s0.replace('e+','E+').replace('e-','E-')
s +='\n'
s += '#No. of Reaction DOFs:{:6d}\n'.format(len(SD_Vars['IDC__']) )
s += '#React. DOF_ID BC\n'
s += '\n'.join(['#{:10d}{:10s}'.format(idof+1,' Fixed' ) for idof in SD_Vars['IDC_F']])
s += '\n'.join(['#{:10d}{:10s}'.format(idof+1,' Free' ) for idof in SD_Vars['IDC_L']])
s += '\n'.join(['#{:10d}{:10s}'.format(idof+1,' Leader') for idof in SD_Vars['IDC_B']])
s += '\n\n'
s += '#No. of Interface DOFs:{:6d}\n'.format(len(SD_Vars['IDI__']))
s += '#Interf. DOF_ID BC\n'
s += '\n'.join(['#{:10d}{:10s}'.format(idof+1,' Fixed' ) for idof in SD_Vars['IDI_F']])
s += '\n'.join(['#{:10d}{:10s}'.format(idof+1,' Leader') for idof in SD_Vars['IDI_B']])
s += '\n\n'
CM = []
from welib.yams.utils import identifyRigidBodyMM
for n in model.Nodes:
if 'addedMassMatrix' in n.data:
mass, J_G, ref2COG = identifyRigidBodyMM(n.data['addedMassMatrix'])
CM.append( (n.ID, mass, J_G, ref2COG) )
s += '#Number of concentrated masses (NCMass):{:6d}\n'.format(len(CM))
s += '#JointCMas Mass JXX JYY JZZ JXY JXZ JYZ MCGX MCGY MCGZ\n'
for cm in CM:
s0 = '# {:9.0f}.{:15.6e}{:15.6e}{:15.6e}{:15.6e}{:15.6e}{:15.6e}{:15.6e}{:15.6e}{:15.6e}{:15.6e}\n'.format( nodeID(cm[0]), cm[1], cm[2][0,0], cm[2][1,1], cm[2][2,2], cm[2][0,1], cm[2][0,2], cm[2][1,2],cm[3][0],cm[3][1],cm[3][2] )
s += s0.replace('e+','E+').replace('e-','E-')
s += '\n'
#s += '#Number of members 18\n'
#s += '#Number of nodes per member: 2\n'
#s += '#Member I Joint1_ID Joint2_ID Prop_I Prop_J Mass Length Node IDs...\n'
#s += '# 77 61 60 11 11 1.045888E+04 2.700000E+00 19 18\n'
#s += '#____________________________________________________________________________________________________\n'
#s += '#Direction Cosine Matrices for all Members: GLOBAL-2-LOCAL. No. of 3x3 matrices= 18\n'
#s += '#Member I DC(1,1) DC(1,2) DC(1,3) DC(2,1) DC(2,2) DC(2,3) DC(3,1) DC(3,2) DC(3,3)\n'
#s += '# 77 1.000E+00 0.000E+00 0.000E+00 0.000E+00 -1.000E+00 0.000E+00 0.000E+00 0.000E+00 -1.000E+00\n'
s += '#____________________________________________________________________________________________________\n'
s += '#FEM Eigenvectors ({} x {}) [m or rad], full system with reaction constraints (+ Soil K/M + SoilDyn K0)\n'.format(*model.Q.shape)
s += yaml_array('Full_Modes', model.Q)
s += '#____________________________________________________________________________________________________\n'
s += '#CB Matrices (PhiM,PhiR) (reaction constraints applied)\n'
s += yaml_array('PhiM', model.Phi_CB[:,:model.nModesCB] ,comment='(CB modes)')
s += yaml_array('PhiR', model.Phi_G, comment='(Guyan modes)')
s += '\n'
if more:
s += '#____________________________________________________________________________________________________\n'
s += '# ADDITIONAL DEBUGGING INFORMATION\n'
s += '#____________________________________________________________________________________________________\n'
s += ''
e = model.Elements[0]
rho=e.rho
A = e.area
L = e.length
t= rho*A*L
s0 = '{:15.6e}{:15.6e}{:15.6e}{:15.6e}{:15.6e}{:15.6e}{:15.6e}{:15.6e}{:15.6e}{:15.6e}{:15.6e}\n'.format(model.gravity,e.area, e.length, e.inertias[0], e.inertias[1], e.inertias[2], e.kappa, e.E, e.G, e.rho, t)
s0 = s0.replace('e+','E+').replace('e-','E-')
s += s0
s += yaml_array('KeLocal' +str(), model.Elements[0].Ke(local=True))
for ie,e in enumerate(model.Elements):
s += yaml_array('DC' +str(ie+1), e.DCM.transpose())
s += yaml_array('Ke' +str(ie+1), e.Ke())
s += yaml_array('Me' +str(ie+1), e.Me())
s += yaml_array('FGe'+str(ie+1), e.Fe_g(model.gravity))
s += yaml_array('FCe'+str(ie+1), e.Fe_o())
s += yaml_array('KeLocal' +str(ie+1), e.Ke(local=True))
s += yaml_array('MeLocal' +str(ie+1), e.Me(local=True))
s += yaml_array('FGeLocal'+str(ie+1), e.Fe_g(model.gravity, local=True))
s += yaml_array('FCeLocal'+str(ie+1), e.Fe_o(local=True))
s += '#____________________________________________________________________________________________________\n'
e = model.Elements[0]
s += yaml_array('Ke', e.Ke(local=True), comment='First element stiffness matrix'); # TODO not in local
s += yaml_array('Me', e.Me(local=True), comment='First element mass matrix');
s += yaml_array('FGe', e.Fe_g(model.gravity,local=True), comment='First element gravity vector');
s += yaml_array('FCe', e.Fe_o(local=True), comment='First element cable pretension');
s += '#____________________________________________________________________________________________________\n'
s += '#FULL FEM K and M matrices. TOTAL FEM TDOFs: {}\n'.format(model.nDOF); # NOTE: wrong in SubDyn, should be nDOFc
s += yaml_array('K', model.KK, comment='Stiffness matrix');
s += yaml_array('M', model.MM, comment='Mass matrix');
s += '#____________________________________________________________________________________________________\n'
s += '#Gravity and cable loads applied at each node of the system (before DOF elimination with T matrix)\n'
s += yaml_array('FG', model.FF_init, comment=' ');
s += '#____________________________________________________________________________________________________\n'
s += '#Additional CB Matrices (MBB,MBM,KBB) (constraint applied)\n'
s += yaml_array('MBB' , model.MBB, comment='');
s += yaml_array('MBM' , model.MBM[:,:model.nModesCB], comment='');
s += yaml_array('CMMdiag', model.CMM, comment='(2 Zeta OmegaM)');
s += yaml_array('KBB' , model.KBB, comment='');
s += yaml_array('KMM' , np.diag(model.KMM), comment='(diagonal components, OmegaL^2)');
s += yaml_array('KMMdiag', np.diag(model.KMM)[:model.nModesCB], comment='(diagonal components, OmegaL^2)');
s += yaml_array('PhiL' , model.Phi_CB, comment='');
s += 'PhiLOm2-1: # 18 x 18 \n'
s += 'KLL^-1: # 18 x 18 \n'
s += '#____________________________________________________________________________________________________\n'
s += yaml_array('T_red', model.T_c, Fmt = '{:9.2e}', comment='(Constraint elimination matrix)');
s += 'AA: # 16 x 16 (State matrix dXdx)\n'
s += 'BB: # 16 x 48 (State matrix dXdu)\n'
s += 'CC: # 6 x 16 (State matrix dYdx)\n'
s += 'DD: # 6 x 48 (State matrix dYdu)\n'
s += '#____________________________________________________________________________________________________\n'
s += yaml_array('TI', model.T_refPoint, Fmt = '{:9.2e}',comment='(TP refpoint Transformation Matrix TI)');
if filename is not None:
with open(filename, 'w') as f:
f.write(s)