def __init__(self, length, radius, mass, endmass):
self.length = length
self.radius = radius
self.mass = mass
self.endmass = endmass
Jx = mass * radius**2 / 2
Jyz = mass*(3*radius**2 + length**2) / 12
self.A = Jyz + endmass*(length/2)**2
self.C = Jx
self.pivot = Hinge('pivot', [0,1,0])
self.offset = RigidConnection('offset', [0,0,-length/2])
self.axis = Hinge('axis', [0,0,1], rotmat_y(-np.pi/2))
self.body = UniformBeam('body', length, mass/length,
1, 1, 1, Jx=Jx/2) # /2 because added to both ends
self.endoffset = RigidConnection('endoffset', [0,0,length/2])
self.endbody = RigidBody('end', endmass)
self.pivot.add_leaf(self.offset)
self.offset.add_leaf(self.axis)
self.axis.add_leaf(self.body)
self.pivot.add_leaf(self.endoffset)
self.endoffset.add_leaf(self.endbody)
self.system = System(self.pivot)
# Prescribed DOF accelerations
self.system.prescribe(self.axis, acc=0.0) # constant rotational speed
self.system.prescribe(self.body, acc=0.0) # rigid beam
def __init__(self, length, radius, mass, endmass):
self.length = length
self.radius = radius
self.mass = mass
self.endmass = endmass
Jx = mass * radius**2 / 2
Jyz = mass * (3 * radius**2 + length**2) / 12
self.A = Jyz + endmass * (length / 2)**2
self.C = Jx
self.pivot = Hinge('pivot', [0, 1, 0])
self.offset = RigidConnection('offset', [0, 0, -length / 2])
self.axis = Hinge('axis', [0, 0, 1], rotmat_y(-np.pi / 2))
self.body = UniformBeam('body',
length,
mass / length,
1,
1,
1,
Jx=Jx / 2) # /2 because added to both ends
self.endoffset = RigidConnection('endoffset', [0, 0, length / 2])
self.endbody = RigidBody('end', endmass)
self.pivot.add_leaf(self.offset)
self.offset.add_leaf(self.axis)
self.axis.add_leaf(self.body)
self.pivot.add_leaf(self.endoffset)
self.endoffset.add_leaf(self.endbody)
self.system = System(self.pivot)
# Prescribed DOF accelerations
self.system.prescribe(self.axis, acc=0.0) # constant rotational speed
self.system.prescribe(self.body, acc=0.0) # rigid beam
def __init__(self, length, radius, mass, spin, endmass):
self.length = length
self.radius = radius
self.mass = mass
self.spin = spin
self.endmass = endmass
x = np.linspace(-length / 2, length / 2)
modes = linearisation.ModalRepresentation(
x=x,
shapes=np.zeros((len(x), 3, 0)),
rotations=np.zeros((len(x), 3, 0)),
density=np.ones_like(x) * mass / length,
mass_axis=np.zeros((len(x), 2)),
section_inertia=np.ones_like(x) * radius**2 / 4,
freqs=np.zeros((0, )),
)
self.bearing = Hinge('bearing', [0, 0, 1])
self.pivot = Hinge('pivot', [0, 1, 0])
self.axis = Hinge('axis', [0, 0, 1], rotmat_y(-np.pi / 2))
self.body = ModalElement('body', modes)
self.offset = RigidConnection('offset', [0, 0, length / 2])
self.endbody = RigidBody('end', endmass)
self.bearing.add_leaf(self.pivot)
self.pivot.add_leaf(self.axis)
self.axis.add_leaf(self.body)
self.pivot.add_leaf(self.offset)
self.offset.add_leaf(self.endbody)
self.system = System(self.bearing)
# Prescribed DOF accelerations
self.system.prescribe(self.axis, acc=0.0) # constant rotational speed
def __init__(self, length, radius, mass, spin, endmass):
self.length = length
self.radius = radius
self.mass = mass
self.spin = spin
self.endmass = endmass
x = np.linspace(-length/2, length/2)
modes = linearisation.ModalRepresentation(
x =x,
shapes =np.zeros((len(x),3,0)),
rotations =np.zeros((len(x),3,0)),
density =np.ones_like(x) * mass/length,
mass_axis =np.zeros((len(x),2)),
section_inertia=np.ones_like(x) * radius**2 / 4,
freqs =np.zeros((0,)),
)
self.bearing = Hinge('bearing', [0,0,1])
self.pivot = Hinge('pivot', [0,1,0])
self.axis = Hinge('axis', [0,0,1], rotmat_y(-np.pi/2))
self.body = ModalElement('body', modes)
self.offset = RigidConnection('offset', [0,0,length/2])
self.endbody = RigidBody('end', endmass)
self.bearing.add_leaf(self.pivot)
self.pivot.add_leaf(self.axis)
self.axis.add_leaf(self.body)
self.pivot.add_leaf(self.offset)
self.offset.add_leaf(self.endbody)
self.system = System(self.bearing)
# Prescribed DOF accelerations
self.system.prescribe(self.axis, acc=0.0) # constant rotational speed
def __init__(self, bladed_file, root_length=0, rigid=False):
# Modal element using data from Bladed model
print "Loading modes from '%s'..." % bladed_file
self.blade = Blade(bladed_file)
self.tower = Tower(bladed_file)
self.modes = self.blade.modal_rep()
#self.tmodes = self.tower.modal_rep()
Ry = rotmat_y(-pi/2)
Rhb1 = rotmat_x(0 * 2*pi/3)
Rhb2 = rotmat_x(1 * 2*pi/3)
Rhb3 = rotmat_x(2 * 2*pi/3)
self.base = FreeJoint('base')
self.towerlink = RigidConnection('tower', [0,0,self.tower.hubheight])
self.bearing = Hinge('bearing', [1,0,0])
root1 = RigidConnection('root1', root_length*np.dot(Rhb1,[0,0,1]), dot(Rhb1,Ry))
root2 = RigidConnection('root2', root_length*np.dot(Rhb2,[0,0,1]), dot(Rhb2,Ry))
root3 = RigidConnection('root3', root_length*np.dot(Rhb3,[0,0,1]), dot(Rhb3,Ry))
self.blade1 = ModalElement('blade1', self.modes)
self.blade2 = ModalElement('blade2', self.modes)
self.blade3 = ModalElement('blade3', self.modes)
self.base.add_leaf(self.towerlink)
self.towerlink.add_leaf(self.bearing)
self.bearing.add_leaf(root1)
self.bearing.add_leaf(root2)
self.bearing.add_leaf(root3)
root1.add_leaf(self.blade1)
root2.add_leaf(self.blade2)
root3.add_leaf(self.blade3)
self.system = System(self.base)
# Prescribed DOF accelerations - constant rotor speed
self.base_motion = None
self.base_motion_amp = 0
self.system.prescribe(self.bearing, vel=0)
self.system.prescribe(self.base, vel=0)
if rigid:
for b in (self.blade1, self.blade2, self.blade3):
self.system.prescribe(b, vel=0)
# setup integrator
self.integ = Integrator(self.system, ('pos','vel','acc'))
self.integ.add_output(dynamics.LoadOutput(self.base.iprox))
self.integ.add_output(dynamics.LoadOutput(self.towerlink.iprox))
self.integ.add_output(dynamics.LoadOutput(self.bearing.iprox))
for b in (self.blade1, self.blade2, self.blade3):
self.integ.add_output(dynamics.LoadOutput(b.iprox, local=True))
for b in (self.blade1, self.blade2, self.blade3):
self.integ.add_output(b.output_deflections())
for b in (self.blade1, self.blade2, self.blade3):
self.integ.add_output(b.output_positions())
for b in (self.blade1, self.blade2, self.blade3):
self.integ.add_output(dynamics.NodeOutput(b.iprox, local=True, deriv=2))
def __init__(self, mode_source_file, root_length=0):
# Modal element using data from Bladed model
print "Loading modes from '%s'..." % mode_source_file
self.modes = ModalRepresentation.from_Bladed(mode_source_file)
Ry = rotmat_y(-pi / 2)
Rhb1 = rotmat_x(0 * 2 * pi / 3)
Rhb2 = rotmat_x(1 * 2 * pi / 3)
Rhb3 = rotmat_x(2 * 2 * pi / 3)
self.bearing = Hinge('bearing', [1, 0, 0])
root1 = RigidConnection('root1', root_length * np.dot(Rhb1, [0, 0, 1]),
dot(Rhb1, Ry))
root2 = RigidConnection('root2', root_length * np.dot(Rhb2, [0, 0, 1]),
dot(Rhb2, Ry))
root3 = RigidConnection('root3', root_length * np.dot(Rhb3, [0, 0, 1]),
dot(Rhb3, Ry))
self.blade1 = ModalElement('blade1', self.modes)
self.blade2 = ModalElement('blade2', self.modes)
self.blade3 = ModalElement('blade3', self.modes)
self.bearing.add_leaf(root1)
self.bearing.add_leaf(root2)
self.bearing.add_leaf(root3)
root1.add_leaf(self.blade1)
root2.add_leaf(self.blade2)
root3.add_leaf(self.blade3)
self.system = System(self.bearing)
# Prescribed DOF accelerations - constant rotor speed
self.system.prescribe(self.bearing.istrain, vel=0.0, acc=0.0)
# setup integrator
self.integ = Integrator(self.system, ('pos', 'vel'))
self.integ.add_output(dynamics.LoadOutput(self.bearing.iprox))
for b in (self.blade1, self.blade2, self.blade3):
self.integ.add_output(dynamics.LoadOutput(b.iprox, local=True))
for b in (self.blade1, self.blade2, self.blade3):
self.integ.add_output(
dynamics.CustomOutput(lambda s: b.station_positions()[-1],
label="{} tip defl".format(b)))
for b in (self.blade1, self.blade2, self.blade3):
self.integ.add_output(
dynamics.CustomOutput(lambda s: dot(b.Rp,
b.station_positions()[-1]),
label="{} tip pos".format(b)))
def __init__(self, mode_source_file, root_length=0, wind_table=None):
# Modal element using data from Bladed model
print "Loading modes from '%s'..." % mode_source_file
self.blade = Blade(mode_source_file)
self.modes = self.blade.modal_rep()
if wind_table is not None:
loading = BladeLoading(self.blade, wind_table, None)
else:
loading = None
Ry = rotmat_y(-pi/2)
Rhb1 = rotmat_x(0 * 2*pi/3)
Rhb2 = rotmat_x(1 * 2*pi/3)
Rhb3 = rotmat_x(2 * 2*pi/3)
self.bearing = Hinge('bearing', [1,0,0])
root1 = RigidConnection('root1', root_length*np.dot(Rhb1,[0,0,1]), dot(Rhb1,Ry))
root2 = RigidConnection('root2', root_length*np.dot(Rhb2,[0,0,1]), dot(Rhb2,Ry))
root3 = RigidConnection('root3', root_length*np.dot(Rhb3,[0,0,1]), dot(Rhb3,Ry))
self.blade1 = ModalElement('blade1', self.modes, loading)
self.blade2 = ModalElement('blade2', self.modes)
self.blade3 = ModalElement('blade3', self.modes)
self.bearing.add_leaf(root1)
self.bearing.add_leaf(root2)
self.bearing.add_leaf(root3)
root1.add_leaf(self.blade1)
root2.add_leaf(self.blade2)
root3.add_leaf(self.blade3)
self.system = System(self.bearing)
# Prescribed DOF accelerations - constant rotor speed
self.system.prescribe(self.bearing, vel=0.0, acc=0.0)
# setup integrator
self.integ = Integrator(self.system, ('pos','vel'))
self.integ.add_output(dynamics.LoadOutput(self.bearing.iprox))
self.integ.add_output(dynamics.LoadOutput(self.blade1.iprox, local=True))
self.integ.add_output(self.blade1.output_deflections())
self.integ.add_output(self.blade1.output_positions())
def __init__(self, mode_source_file, root_length=0):
# Modal element using data from Bladed model
print "Loading modes from '%s'..." % mode_source_file
self.modes = ModalRepresentation.from_Bladed(mode_source_file)
Ry = rotmat_y(-pi/2)
Rhb1 = rotmat_x(0 * 2*pi/3)
Rhb2 = rotmat_x(1 * 2*pi/3)
Rhb3 = rotmat_x(2 * 2*pi/3)
self.bearing = Hinge('bearing', [1,0,0])
root1 = RigidConnection('root1', root_length*np.dot(Rhb1,[0,0,1]), dot(Rhb1,Ry))
root2 = RigidConnection('root2', root_length*np.dot(Rhb2,[0,0,1]), dot(Rhb2,Ry))
root3 = RigidConnection('root3', root_length*np.dot(Rhb3,[0,0,1]), dot(Rhb3,Ry))
self.blade1 = ModalElement('blade1', self.modes)
self.blade2 = ModalElement('blade2', self.modes)
self.blade3 = ModalElement('blade3', self.modes)
self.bearing.add_leaf(root1)
self.bearing.add_leaf(root2)
self.bearing.add_leaf(root3)
root1.add_leaf(self.blade1)
root2.add_leaf(self.blade2)
root3.add_leaf(self.blade3)
self.system = System(self.bearing)
# Prescribed DOF accelerations - constant rotor speed
self.system.prescribe(self.bearing.istrain, vel=0.0, acc=0.0)
# setup integrator
self.integ = Integrator(self.system, ('pos','vel'))
self.integ.add_output(dynamics.LoadOutput(self.bearing.iprox))
for b in (self.blade1, self.blade2, self.blade3):
self.integ.add_output(dynamics.LoadOutput(b.iprox, local=True))
for b in (self.blade1, self.blade2, self.blade3):
self.integ.add_output(dynamics.CustomOutput(
lambda s: b.station_positions()[-1], label="{} tip defl".format(b)))
for b in (self.blade1, self.blade2, self.blade3):
self.integ.add_output(dynamics.CustomOutput(
lambda s: dot(b.Rp, b.station_positions()[-1]), label="{} tip pos".format(b)))
def __init__(self, bladed_file, root_length=0):
# Load modes but use a simple flapped blade
print "Loading modes from '%s'..." % bladed_file
self.blade = Blade(bladed_file)
self.tower = Tower(bladed_file)
self.modes = self.blade.modal_rep()
# Calculate equivalent blade properties
I1 = self.modes.I0[0]
I2 = self.modes.J0[0,0]
print I1, I2
wflap = self.modes.freqs[0]
bmass = self.modes.mass
inertia = self.modes.inertia_tensor(np.zeros(len(self.modes.freqs)))
Xc = [I1 / bmass, 0, 0]
kflap = I2 * wflap**2
Ry = rotmat_y(-pi/2)
Rhb1 = rotmat_x(0 * 2*pi/3)
Rhb2 = rotmat_x(1 * 2*pi/3)
Rhb3 = rotmat_x(2 * 2*pi/3)
self.base = FreeJoint('base')
self.towerlink = RigidConnection('tower', [0,0,self.tower.hubheight])
self.bearing = Hinge('bearing', [1,0,0])
root1 = RigidConnection('root1', root_length*np.dot(Rhb1,[0,0,1]), dot(Rhb1,Ry))
root2 = RigidConnection('root2', root_length*np.dot(Rhb2,[0,0,1]), dot(Rhb2,Ry))
root3 = RigidConnection('root3', root_length*np.dot(Rhb3,[0,0,1]), dot(Rhb3,Ry))
self.flap1 = Hinge('flap1', [0,1,0])
self.flap2 = Hinge('flap2', [0,1,0])
self.flap3 = Hinge('flap3', [0,1,0])
self.blade1 = RigidBody('blade1', bmass, inertia, Xc)
self.blade2 = RigidBody('blade2', bmass, inertia, Xc)
self.blade3 = RigidBody('blade3', bmass, inertia, Xc)
self.flap1.stiffness = self.flap2.stiffness = self.flap3.stiffness = kflap
self.base.add_leaf(self.towerlink)
self.towerlink.add_leaf(self.bearing)
self.bearing.add_leaf(root1)
self.bearing.add_leaf(root2)
self.bearing.add_leaf(root3)
root1.add_leaf(self.flap1)
root2.add_leaf(self.flap2)
root3.add_leaf(self.flap3)
self.flap1.add_leaf(self.blade1)
self.flap2.add_leaf(self.blade2)
self.flap3.add_leaf(self.blade3)
self.system = System(self.base)
# Prescribed DOF accelerations - constant rotor speed
self.base_motion = None
self.base_motion_amp = 0
self.system.prescribe(self.bearing, vel=0)
self.system.prescribe(self.base, vel=0)
# setup integrator
self.integ = Integrator(self.system, ('pos','vel','acc'))
self.integ.add_output(dynamics.LoadOutput(self.base.iprox))
self.integ.add_output(dynamics.LoadOutput(self.towerlink.iprox))
self.integ.add_output(dynamics.LoadOutput(self.bearing.iprox, local=True))
self.integ.add_output(dynamics.LoadOutput(self.bearing.idist[0], local=True))
for b in (self.blade1, self.blade2, self.blade3):
self.integ.add_output(dynamics.LoadOutput(b.iprox, local=True))
for b in (self.blade1, self.blade2, self.blade3):
self.integ.add_output(dynamics.NodeOutput(b.iprox, local=True, deriv=2))
# Load Bladed data for comparison
import pybladed.data
brun = pybladed.data.BladedRun(bladed_path)
thrust = brun.get('rotating hub Fx')
bladed_defl = np.c_[brun.get('Nacelle fore-aft displacement'),
brun.get('Nacelle nod angle'), ]
#loading = PointLoading(blade, wind_table, None)
thrust_time = [0, 1, 2, 10]
thrust_force = [0, 0, 10e3, 10e3]
thrust = np.c_[thrust_force, np.zeros((4, 2))].T
loadfunc = scipy.interpolate.interp1d(thrust_time, thrust)
# Modal element
base = RigidConnection('base', rotation=rotmat_y(-np.pi / 2))
el = ModalElement('el', modes, distal=True, damping_freqs=[8.269, 10.248])
rna = RigidBody('rna',
24000,
np.diag([6400003, 6400003, 4266667]),
nodal_load=loadfunc)
base.add_leaf(el)
el.add_leaf(rna)
system = System(base)
integ = Integrator(system)
integ.add_output(el.output_deflections())
integ.add_output(el.output_rotations())
integ.add_output(dynamics.LoadOutput(rna.iprox))
linsys = LinearisedSystem(system)
dynamics.gravity = 0
bladedpath = '/bladed/gyro_effects/simpleblade_10rpm_10degs'
# Modal element using data from Bladed model
print "Loading modes from '%s'..." % bladedpath
modes = ModalRepresentation.from_Bladed(bladedpath + '.$pj')
rotorspeed = 10 * np.pi / 30 # 10 rpm
overhang = 1 # 1m
# Modal element
yaw = Hinge('yaw', [0, 0, 1])
overhang = RigidConnection('overhang', [-overhang, 0, 0])
bearing = Hinge('bearing', [1, 0, 0],
np.dot(rotmat_y(-np.pi / 2), rotmat_x(-np.pi / 2)))
el = ModalElement('el', modes)
yaw.add_leaf(overhang)
overhang.add_leaf(bearing)
bearing.add_leaf(el)
system = System(yaw)
# Prescribe rotation speed
system.prescribe(bearing.istrain, 0.0)
system.qd[bearing.istrain] = rotorspeed
# Prescribed yaw angle
acc_period = 0.1
yaw_time1 = 3.0
yaw_time2 = 6.0
dvyaw = 10 * np.pi / 180
def __init__(self, bladed_file, root_length=0, rigid=False):
# Modal element using data from Bladed model
print "Loading modes from '%s'..." % bladed_file
self.blade = Blade(bladed_file)
self.tower = Tower(bladed_file)
self.modes = self.blade.modal_rep()
Ry = rotmat_y(-pi / 2)
Rhb1 = rotmat_x(0 * 2 * pi / 3)
Rhb2 = rotmat_x(1 * 2 * pi / 3)
Rhb3 = rotmat_x(2 * 2 * pi / 3)
self.base = FreeJoint('base')
self.towerlink = RigidConnection('tower', [0, 0, self.tower.hubheight])
self.bearing = Hinge('bearing', [1, 0, 0])
root1 = RigidConnection('root1', root_length * np.dot(Rhb1, [0, 0, 1]),
dot(Rhb1, Ry))
root2 = RigidConnection('root2', root_length * np.dot(Rhb2, [0, 0, 1]),
dot(Rhb2, Ry))
root3 = RigidConnection('root3', root_length * np.dot(Rhb3, [0, 0, 1]),
dot(Rhb3, Ry))
self.blade1 = ModalElement('blade1', self.modes)
self.blade2 = ModalElement('blade2', self.modes)
self.blade3 = ModalElement('blade3', self.modes)
self.base.add_leaf(self.towerlink)
self.towerlink.add_leaf(self.bearing)
self.bearing.add_leaf(root1)
self.bearing.add_leaf(root2)
self.bearing.add_leaf(root3)
root1.add_leaf(self.blade1)
root2.add_leaf(self.blade2)
root3.add_leaf(self.blade3)
self.system = System(self.base)
# Prescribed DOF accelerations - constant rotor speed
self.base_motion = None
self.base_motion_amp = 0
self.system.prescribe(self.bearing, vel=0)
self.system.prescribe(self.base, vel=0)
if rigid:
for b in (self.blade1, self.blade2, self.blade3):
self.system.prescribe(b, vel=0)
# setup integrator
self.integ = Integrator(self.system, ('pos', 'vel', 'acc'))
self.integ.add_output(dynamics.LoadOutput(self.base.iprox))
self.integ.add_output(dynamics.LoadOutput(self.towerlink.iprox))
self.integ.add_output(
dynamics.LoadOutput(self.bearing.iprox, local=True))
self.integ.add_output(
dynamics.LoadOutput(self.bearing.idist[0], local=True))
for b in (self.blade1, self.blade2, self.blade3):
self.integ.add_output(dynamics.LoadOutput(b.iprox, local=True))
for b in (self.blade1, self.blade2, self.blade3):
self.integ.add_output(b.output_deflections())
for b in (self.blade1, self.blade2, self.blade3):
self.integ.add_output(b.output_positions())
for b in (self.blade1, self.blade2, self.blade3):
self.integ.add_output(
dynamics.NodeOutput(b.iprox, local=True, deriv=2))
def __init__(self, bladed_file, root_length=0):
# Load modes but use a simple flapped blade
print "Loading modes from '%s'..." % bladed_file
self.blade = Blade(bladed_file)
self.tower = Tower(bladed_file)
self.modes = self.blade.modal_rep()
# Calculate equivalent blade properties
I1 = self.modes.I0[0]
I2 = self.modes.J0[0, 0]
print I1, I2
wflap = self.modes.freqs[0]
bmass = self.modes.mass
inertia = self.modes.inertia_tensor(np.zeros(len(self.modes.freqs)))
Xc = [I1 / bmass, 0, 0]
kflap = I2 * wflap**2
Ry = rotmat_y(-pi / 2)
Rhb1 = rotmat_x(0 * 2 * pi / 3)
Rhb2 = rotmat_x(1 * 2 * pi / 3)
Rhb3 = rotmat_x(2 * 2 * pi / 3)
self.base = FreeJoint('base')
self.towerlink = RigidConnection('tower', [0, 0, self.tower.hubheight])
self.bearing = Hinge('bearing', [1, 0, 0])
root1 = RigidConnection('root1', root_length * np.dot(Rhb1, [0, 0, 1]),
dot(Rhb1, Ry))
root2 = RigidConnection('root2', root_length * np.dot(Rhb2, [0, 0, 1]),
dot(Rhb2, Ry))
root3 = RigidConnection('root3', root_length * np.dot(Rhb3, [0, 0, 1]),
dot(Rhb3, Ry))
self.flap1 = Hinge('flap1', [0, 1, 0])
self.flap2 = Hinge('flap2', [0, 1, 0])
self.flap3 = Hinge('flap3', [0, 1, 0])
self.blade1 = RigidBody('blade1', bmass, inertia, Xc)
self.blade2 = RigidBody('blade2', bmass, inertia, Xc)
self.blade3 = RigidBody('blade3', bmass, inertia, Xc)
self.flap1.stiffness = self.flap2.stiffness = self.flap3.stiffness = kflap
self.base.add_leaf(self.towerlink)
self.towerlink.add_leaf(self.bearing)
self.bearing.add_leaf(root1)
self.bearing.add_leaf(root2)
self.bearing.add_leaf(root3)
root1.add_leaf(self.flap1)
root2.add_leaf(self.flap2)
root3.add_leaf(self.flap3)
self.flap1.add_leaf(self.blade1)
self.flap2.add_leaf(self.blade2)
self.flap3.add_leaf(self.blade3)
self.system = System(self.base)
# Prescribed DOF accelerations - constant rotor speed
self.base_motion = None
self.base_motion_amp = 0
self.system.prescribe(self.bearing, vel=0)
self.system.prescribe(self.base, vel=0)
# setup integrator
self.integ = Integrator(self.system, ('pos', 'vel', 'acc'))
self.integ.add_output(dynamics.LoadOutput(self.base.iprox))
self.integ.add_output(dynamics.LoadOutput(self.towerlink.iprox))
self.integ.add_output(
dynamics.LoadOutput(self.bearing.iprox, local=True))
self.integ.add_output(
dynamics.LoadOutput(self.bearing.idist[0], local=True))
for b in (self.blade1, self.blade2, self.blade3):
self.integ.add_output(dynamics.LoadOutput(b.iprox, local=True))
for b in (self.blade1, self.blade2, self.blade3):
self.integ.add_output(
dynamics.NodeOutput(b.iprox, local=True, deriv=2))
dynamics.gravity = 0
bladedpath = '/bladed/gyro_effects/simpleblade_10rpm_10degs'
# Modal element using data from Bladed model
print "Loading modes from '%s'..." % bladedpath
modes = ModalRepresentation.from_Bladed(bladedpath+'.$pj')
rotorspeed = 10 * np.pi/30 # 10 rpm
overhang = 1 # 1m
# Modal element
yaw = Hinge('yaw', [0,0,1])
overhang = RigidConnection('overhang', [-overhang,0,0])
bearing = Hinge('bearing', [1,0,0],np.dot(rotmat_y(-np.pi/2), rotmat_x(-np.pi/2)))
el = ModalElement('el', modes)
yaw.add_leaf(overhang)
overhang.add_leaf(bearing)
bearing.add_leaf(el)
system = System(yaw)
# Prescribe rotation speed
system.prescribe(bearing.istrain, 0.0)
system.qd[bearing.istrain] = rotorspeed
# Prescribed yaw angle
acc_period = 0.1
yaw_time1 = 3.0
yaw_time2 = 6.0
dvyaw = 10 * np.pi/180
import numpy as np
from numpy import pi, zeros, diag
from dynamics import (FreeJoint, Hinge, rotmat_x, rotmat_y,
EulerBeam, RigidConnection, System, solve_system, NQD)
import matplotlib.pylab as plt
import dynvis
tower_height = 90.0
overhang = 0.8
r_root = 0.5
blade_length = 60.0
EIy = 1000e6
EIz = 1000e6
Ry = rotmat_y(-pi/2)
Rhb1 = rotmat_x(0 * 2*pi/3)
Rhb2 = rotmat_x(1 * 2*pi/3)
Rhb3 = rotmat_x(2 * 2*pi/3)
fstiff = 1e6 * diag([1, 1, 5, 1000, 1000, 100])
foundation = FreeJoint('foundation', fstiff, post_transform=rotmat_y(-pi/2))
tower = EulerBeam('tower', tower_height, 3000, 100e6, 300e6, 300e6, 200e6)
nacelle = RigidConnection('nacelle', [0,0,overhang], rotmat_y(100*pi/180))
bearing = Hinge('bearing', [1,0,0])
hb1 = RigidConnection('hb1', np.dot(Rhb1,[0,0,1]), np.dot(Rhb1,Ry))
hb2 = RigidConnection('hb2', np.dot(Rhb2,[0,0,1]), np.dot(Rhb2,Ry))
hb3 = RigidConnection('hb3', np.dot(Rhb3,[0,0,1]), np.dot(Rhb3,Ry))
b1 = EulerBeam('b1',blade_length, 250, 1000e6, EIy, EIz, 200e6)
b2 = EulerBeam('b2',blade_length, 250, 1000e6, EIy, EIz, 200e6)
b3 = EulerBeam('b3',blade_length, 250, 1000e6, EIy, EIz, 200e6)
import pybladed.data
brun = pybladed.data.BladedRun(bladed_path)
thrust = brun.get('rotating hub Fx')
bladed_defl = np.c_[
brun.get('Nacelle fore-aft displacement'),
brun.get('Nacelle nod angle'),
]
#loading = PointLoading(blade, wind_table, None)
thrust_time = [0, 1, 2, 10 ]
thrust_force = [0, 0, 10e3, 10e3]
thrust = np.c_[ thrust_force, np.zeros((4,2)) ].T
loadfunc = scipy.interpolate.interp1d(thrust_time, thrust)
# Modal element
base = RigidConnection('base', rotation=rotmat_y(-np.pi/2))
el = ModalElement('el', modes, distal=True, damping_freqs=[8.269, 10.248])
rna = RigidBody('rna', 24000, np.diag([6400003, 6400003, 4266667]), nodal_load=loadfunc)
base.add_leaf(el)
el.add_leaf(rna)
system = System(base)
integ = Integrator(system)
integ.add_output(el.output_deflections())
integ.add_output(el.output_rotations())
integ.add_output(dynamics.LoadOutput(rna.iprox))
linsys = LinearisedSystem(system)
def ani_xy(s,t,y):
return dynvis.anim(s, t, y, (0,1), (-5,45), (-5,5), velocities=False)
# Load Bladed data for comparison
import pybladed.data
brun = pybladed.data.BladedRun(bladed_path)
thrust = brun.get("rotating hub Fx")
bladed_defl = np.c_[brun.get("Nacelle fore-aft displacement"), brun.get("Nacelle nod angle")]
# loading = PointLoading(blade, wind_table, None)
thrust_time = [0, 1, 2, 10]
thrust_force = [0, 0, 10e3, 10e3]
thrust = np.c_[thrust_force, np.zeros((4, 2))].T
loadfunc = scipy.interpolate.interp1d(thrust_time, thrust)
# Modal element
base = RigidConnection("base", rotation=rotmat_y(-np.pi / 2))
el = DistalModalElement("el", modes, distal=True, damping_freqs=modes2.freqs)
# el = ModalElement('el', modes, distal=True, damping_freqs=modes2.freqs)
rna = RigidBody("rna", 24000, np.diag([6400003, 6400003, 4266667]), nodal_load=loadfunc)
base.add_leaf(el)
el.add_leaf(rna)
system = System(base)
system.prescribe(el, vel=0, part=[0, 3])
integ = Integrator(system)
integ.add_output(el.output_deflections())
integ.add_output(el.output_rotations())
integ.add_output(dynamics.LoadOutput(rna.iprox))
linsys = LinearisedSystem(system)