Property definitions#

Beam property module (pyfe3d.beamprop)#

class pyfe3d.beamprop.BeamProp#

General class to represent beam properties.

About shear correction factors, usually one should only apply the shear correction factor to the shear modulus G. It is, however, possible to have more complex scenarios where the different cross section parameters Ay, Az, J have different corrections applied due to geometric properties. It is the user’s responsability to apply these correction factors properly to achieve a general representation of the beam element behaviour by means of this property class. No shear correction factors or geometric correction factors are applied internally during the calculation of the structural matrices.

Notes

For beams with homogeneous material along the cross section some of the quantities above can be calculated as follows, assuming that rho is the material density:

intrho = A*rho intrhoy2 = Izz*rho intrhoz2 = Iyy*rho intrhoyz = Iyz*rho

Attributes:
A,float

Area of the cross section

E,float

Young modulus

G,float

Shear modulus

Iyy,float

Second moment of area about the y axis \(\int_y \int_z z^2 dy dz\)

Izz,float

Second moment of area about the z axis \(\int_y \int_z y^2 dy dz\)

Iyz,float

Product moment of area \(\int_y \int_z y z dy dz\)

J,float

Torsion stiffness or torsion constant, see https://en.wikipedia.org/wiki/Torsion_constant.

Ay,float

Integral \(\int_y \int_z y dy dz\)

Az,float

Integral \(\int_y \int_z z dy dz\)

intrho,float

Integral \(\int_{y_e} \int_{z_e} \rho(y, z) dy dz\), where \(\rho\) Is the density

intrhoy,float

Integral \(\int_y \int_z y \rho(y, z) dy dz\)

intrhoz,float

Integral \(\int_y \int_z z \rho(y, z) dy dz\)

intrhoy2,float

Integral \(\int_y \int_z y^2 \rho(y, z) dy dz\)

intrhoz2,float

Integral \(\int_y \int_z z^2 \rho(y, z) dy dz\)

intrhoyz,float

Integral \(\int_y \int_z y z \rho(y, z) dy dz\)

A#

A: ‘double’

Ay#

Ay: ‘double’

Az#

Az: ‘double’

E#

E: ‘double’

G#

G: ‘double’

Iyy#

Iyy: ‘double’

Iyz#

Iyz: ‘double’

Izz#

Izz: ‘double’

J#

J: ‘double’

intrho#

intrho: ‘double’

intrhoy#

intrhoy: ‘double’

intrhoy2#

intrhoy2: ‘double’

intrhoyz#

intrhoyz: ‘double’

intrhoz#

intrhoz: ‘double’

intrhoz2#

intrhoz2: ‘double’

Shell property module (pyfe3d.shellprop)#

Highly based on the composites. module.

class pyfe3d.shellprop.GradABDE#

Container to store the gradients of the ABDE matrices with respect to the lamination parameters

Attributes:
gradAij, gradBij, gradDij, gradEijtuple of 2D np.array objects

The shapes of these gradient matrices are:

gradAij: (6, 5) gradBij: (6, 5) gradDij: (6, 5) gradEij: (3, 3)

They contain the gradients of each laminate stiffness with respect to the thickness and respective lamination parameters. The rows and columns correspond to:

Methods

calc_LP_grad(self, double thickness, ...)

Gradients of the shell stiffnesses with respect to the thickness and lamination parameters

calc_LP_grad(self, double thickness, MatLamina mat, LaminationParameters lp) void#

Gradients of the shell stiffnesses with respect to the thickness and lamination parameters

Parameters:
thicknessfloat

The total thickness of the laminate

matMatLamina object

Material object

lpLaminationParameters object

The container class with all lamination parameters already defined

Returns:
None

The attributes of the object are updated.

gradAij#

gradAij: ‘double[:, ::1]’

gradBij#

gradBij: ‘double[:, ::1]’

gradDij#

gradDij: ‘double[:, ::1]’

gradEij#

gradEij: ‘double[:, ::1]’

class pyfe3d.shellprop.Lamina#
Attributes:
plyidint

plyid: ‘int’

matlaminaMatLamina object

matlamina: pyfe3d.shellprop.MatLamina

hfloat

h: ‘double’

thetadegfloat

thetadeg: ‘double’

Methods

get_constitutive_matrix(self)

Return the constitutive matrix

get_transf_matrix_displ_to_laminate(self)

Return displacement transformation matrix from lamina to laminate

get_transf_matrix_stress_to_lamina(self)

Return stress transformation matrix from laminate to lamina

get_transf_matrix_stress_to_laminate(self)

Return stress transformation matrix from lamina to laminate

rebuild(self)

Update constitutive matrices

cos2t#

cos2t: ‘double’

cos4t#

cos4t: ‘double’

cost#

cost: ‘double’

get_constitutive_matrix(self) double[:, ::1]#

Return the constitutive matrix

get_transf_matrix_displ_to_laminate(self) double[:, ::1]#

Return displacement transformation matrix from lamina to laminate

get_transf_matrix_stress_to_lamina(self) double[:, ::1]#

Return stress transformation matrix from laminate to lamina

get_transf_matrix_stress_to_laminate(self) double[:, ::1]#

Return stress transformation matrix from lamina to laminate

h#

h: ‘double’

matlamina#

matlamina: pyfe3d.shellprop.MatLamina

plyid#

plyid: ‘int’

q11L#

q11L: ‘double’

q12L#

q12L: ‘double’

q16L#

q16L: ‘double’

q22L#

q22L: ‘double’

q26L#

q26L: ‘double’

q44L#

q44L: ‘double’

q45L#

q45L: ‘double’

q55L#

q55L: ‘double’

q66L#

q66L: ‘double’

rebuild(self) void#

Update constitutive matrices

Reference:

Reddy, J. N., Mechanics of Laminated Composite Plates and Shells - Theory and Analysys. Second Edition. CRC PRESS, 2004.

sin2t#

sin2t: ‘double’

sin4t#

sin4t: ‘double’

sint#

sint: ‘double’

thetadeg#

thetadeg: ‘double’

class pyfe3d.shellprop.LaminationParameters#

Lamination parameters

Attributes:
xiA1, xiA2, xiA3, xiA4float

Lamination parameters \(\xi_{Ai}\) (in-plane)

xiB1, xiB2, xiB3, xiB4float

Lamination parameters \(\xi_{Bi}\) (in-plane coupling with bending)

xiD1, xiD2, xiD3, xiD4float

Lamination parameters \(\xi_{Di}\) (bending)

xiE1, xiE2float

Lamination parameters \(\xi_{Ei}\) (transverse shear)

xiA1#

xiA1: ‘double’

xiA2#

xiA2: ‘double’

xiA3#

xiA3: ‘double’

xiA4#

xiA4: ‘double’

xiB1#

xiB1: ‘double’

xiB2#

xiB2: ‘double’

xiB3#

xiB3: ‘double’

xiB4#

xiB4: ‘double’

xiD1#

xiD1: ‘double’

xiD2#

xiD2: ‘double’

xiD3#

xiD3: ‘double’

xiD4#

xiD4: ‘double’

xiE1#

xiE1: ‘double’

xiE2#

xiE2: ‘double’

xiE3#

xiE3: ‘double’

xiE4#

xiE4: ‘double’

class pyfe3d.shellprop.MatLamina#

Orthotropic material lamina

Notes

For isotropic materials when the user defines \(\nu\) and \(E\), \(G\) will be recaculated based on equation: \(G = E/(2 \times (1+\nu))\); in a lower priority if the user defines \(\nu\) and \(G\), \(E\) will be recaculated based on equation: \(E = 2 \times (1+\nu) \times G\).

Attributes:
e1float

e1: ‘double’

e2float

e2: ‘double’

g12float

g12: ‘double’

g13float

g13: ‘double’

g23float

g23: ‘double’

nu12

nu12: ‘double’

nu13

nu13: ‘double’

nu23

nu23: ‘double’

nu21

nu21: ‘double’

nu31

nu31: ‘double’

nu32

nu32: ‘double’

rho

rho: ‘double’

a1

a1: ‘double’

a2

a2: ‘double’

a3

a3: ‘double’

tref

tref: ‘double’

st1,st2

allowable tensile stresses for directions 1 and 2

sc1,sc2

allowable compressive stresses for directions 1 and 2

ss12

ss12: ‘double’

q11

q11: ‘double’

q12

q12: ‘double’

q13

q13: ‘double’

q21

q21: ‘double’

q22

q22: ‘double’

q23

q23: ‘double’

q31

q31: ‘double’

q32

q32: ‘double’

q33

q33: ‘double’

q44

q44: ‘double’

q55

q55: ‘double’

q66

q66: ‘double’

ci

lamina stiffness constants

ui

lamina material invariants

Methods

get_constitutive_matrix(self)

Return the constitutive matrix

get_invariant_matrix(self)

Return the invariant matrix

rebuild(self)

Update constitutive and invariant terms

trace_normalize_plane_stress(self)

Trace-normalize the lamina properties for plane stress

a1#

a1: ‘double’

a2#

a2: ‘double’

a3#

a3: ‘double’

c11#

c11: ‘double’

c12#

c12: ‘double’

c13#

c13: ‘double’

c22#

c22: ‘double’

c23#

c23: ‘double’

c33#

c33: ‘double’

c44#

c44: ‘double’

c55#

c55: ‘double’

c66#

c66: ‘double’

e1#

e1: ‘double’

e2#

e2: ‘double’

e3#

e3: ‘double’

g12#

g12: ‘double’

g13#

g13: ‘double’

g23#

g23: ‘double’

get_constitutive_matrix(self) double[:, ::1]#

Return the constitutive matrix

get_invariant_matrix(self) double[:, ::1]#

Return the invariant matrix

nu12#

nu12: ‘double’

nu13#

nu13: ‘double’

nu21#

nu21: ‘double’

nu23#

nu23: ‘double’

nu31#

nu31: ‘double’

nu32#

nu32: ‘double’

q11#

q11: ‘double’

q12#

q12: ‘double’

q13#

q13: ‘double’

q21#

q21: ‘double’

q22#

q22: ‘double’

q23#

q23: ‘double’

q31#

q31: ‘double’

q32#

q32: ‘double’

q33#

q33: ‘double’

q44#

q44: ‘double’

q55#

q55: ‘double’

q66#

q66: ‘double’

rebuild(self) void#

Update constitutive and invariant terms

Reference:

Reddy, J. N., Mechanics of laminated composite plates and shells. Theory and analysis. Second Edition. CRC Press, 2004.

rho#

rho: ‘double’

sc1#

sc1: ‘double’

sc2#

sc2: ‘double’

ss12#

ss12: ‘double’

st1#

st1: ‘double’

st2#

st2: ‘double’

trace_normalize_plane_stress(self) void#

Trace-normalize the lamina properties for plane stress

Modify the original MatLamina object with a trace-normalization performed after calculating the trace according to Eq. 1 of reference:

Melo, J. D. D., Bi, J., and Tsai, S. W., 2017, “A Novel Invariant-Based Design Approach to Carbon Fiber Reinforced Laminates,” Compos. Struct., 159, pp. 44–52.

The trace calculated as \(tr = Q_{11} + Q_{22} + 2Q_{66}\). The universal in-plane stress stiffness components \(Q_{11},Q_{12},Q_{22},Q_{44},Q_{55},Q_{66}\) are divided by \(tr\), and the invariants \(U_1,U_2,U_3,U_4,U_5,U_6,U_7\) are calculated with the normalized stiffnesses, such they also become trace-normalized invariants. These can be accessed using the u1,u2,u3,u4,u5,u6,u7 attributes.

tref#

tref: ‘double’

u1#

u1: ‘double’

u2#

u2: ‘double’

u3#

u3: ‘double’

u4#

u4: ‘double’

u5#

u5: ‘double’

u6#

u6: ‘double’

u7#

u7: ‘double’

class pyfe3d.shellprop.ShellProp#
Attributes:
plieslist

plies: list

stacklist

stack: list

hfloat

h: ‘double’

offsetfloat

offset: ‘double’

e1, e2float

Equivalent laminate moduli in directions 1 and 2

g12float

g12: ‘double’

nu12, nu21float

Equivalent laminate Poisson ratios in the 12 and 21 directions

scf_k13, scf_k23float

Shear correction factor in the 13 and 23 directions

intrhofloat

intrho: ‘double’

intrhozfloat

intrhoz: ‘double’

intrhoz2float

intrhoz2: ‘double’

Methods

calc_constitutive_matrix(self)

Calculate the laminate constitutive terms

calc_equivalent_properties(self)

Calculate the equivalent laminate properties

calc_lamination_parameters(self)

Calculate the lamination parameters.

calc_scf(self)

Update shear correction factors of the ShellProp object

force_balanced(self)

Force a balanced laminate

force_orthotropic(self)

Force an orthotropic laminate

force_symmetric(self)

Force a symmetric laminate

A11#

A11: ‘double’

A12#

A12: ‘double’

A16#

A16: ‘double’

A22#

A22: ‘double’

A26#

A26: ‘double’

A66#

A66: ‘double’

B11#

B11: ‘double’

B12#

B12: ‘double’

B16#

B16: ‘double’

B22#

B22: ‘double’

B26#

B26: ‘double’

B66#

B66: ‘double’

D11#

D11: ‘double’

D12#

D12: ‘double’

D16#

D16: ‘double’

D22#

D22: ‘double’

D26#

D26: ‘double’

D66#

D66: ‘double’

E44#

E44: ‘double’

E45#

E45: ‘double’

E55#

E55: ‘double’

calc_constitutive_matrix(self) void#

Calculate the laminate constitutive terms

This is the commonly called ABD matrix with shape=(6, 6) when the classical laminated plate theory is used, or the ABDE matrix when the first-order shear deformation theory is used, containing the transverse shear terms.

calc_equivalent_properties(self) void#

Calculate the equivalent laminate properties

The following attributes are updated:

e1, e2, g12, `u12, nu21

calc_lamination_parameters(self) LaminationParameters#

Calculate the lamination parameters.

The following attributes are calculated:

xiA, xiB, xiD, xiE

calc_scf(self) void#

Update shear correction factors of the ShellProp object

Reference:

Vlachoutsis, S. “Shear correction factors for plates and shells”, Int. Journal for Numerical Methods in Engineering, Vol. 33, 1537-1552, 1992.

http://onlinelibrary.wiley.com/doi/10.1002/nme.1620330712/full

Using “one shear correction factor” (see reference), assuming:

  • constant G13, G23, E1, E2, nu12, nu21 within each ply

  • g1 calculated using z at the middle of each ply

  • zn1 = ShellProp offset attribute

Returns:
k13, k23tuple

Shear correction factors. Also updates attributes: scf_k13 and scf_k23.

e1#

e1: ‘double’

e2#

e2: ‘double’

force_balanced(self) void#

Force a balanced laminate

The attributes \(A_{16}\), \(A_{26}\), \(B_{16}\), \(B_{26}\) are set to zero to force a balanced laminate.

force_orthotropic(self) void#

Force an orthotropic laminate

The attributes \(A_{16}\), \(A_{26}\), \(B_{16}\), \(B_{26}\), \(D_{16}\), \(D_{26}\) are set to zero to force an orthotropic laminate.

force_symmetric(self) void#

Force a symmetric laminate

The \(B_{ij}\) terms of the constitutive matrix are set to zero.

g12#

g12: ‘double’

h#

h: ‘double’

intrho#

intrho: ‘double’

intrhoz#

intrhoz: ‘double’

intrhoz2#

intrhoz2: ‘double’

nu12#

nu12: ‘double’

nu21#

nu21: ‘double’

offset#

offset: ‘double’

plies#

plies: list

scf_k13#

scf_k13: ‘double’

scf_k23#

scf_k23: ‘double’

stack#

stack: list

pyfe3d.shellprop.force_balanced_LP(LaminationParameters lp) LaminationParameters#

Force balanced lamination parameters

The lamination parameters \(\xi_{A2}\) and \(\xi_{A4}\) are set to null to force a balanced laminate.

pyfe3d.shellprop.force_orthotropic_LP(LaminationParameters lp) LaminationParameters#

Force orthotropic lamination parameters

The lamination parameters \(\xi_{A2}\), \(\xi_{A4}\), \(\xi_{B2}\), \(\xi_{B4}\), \(\xi_{D2}\) and \(\xi_{D4}\) are set to null to force an orthotropic laminate. The \(\xi_{D2}\) and \(\xi_{D4}\) are related to the bend-twist coupling and become often very small for balanced laminates with a large amount of plies.

pyfe3d.shellprop.force_symmetric_LP(LaminationParameters lp) LaminationParameters#

Force symmetric lamination parameters

The lamination parameters \(\xi_{Bi}\) are set to null to force a symmetric laminate.

pyfe3d.shellprop.shellprop_from_LaminationParameters(double thickness, MatLamina mat, LaminationParameters lp) ShellProp#

Return a ShellProp object based in the thickness, material and lamination parameters

Parameters:
thicknessfloat

The total thickness of the laminate

matMatLamina object

Material object

lpLaminationParameters object

The container class with all lamination parameters already defined

Returns:
lamShellProp

laminate with the ABD and ABDE matrices already calculated

pyfe3d.shellprop.shellprop_from_lamination_parameters(double thickness, MatLamina matlamina, double xiA1, double xiA2, double xiA3, double xiA4, double xiB1, double xiB2, double xiB3, double xiB4, double xiD1, double xiD2, double xiD3, double xiD4, double xiE1=0, double xiE2=0) ShellProp#

Return a ShellProp object based in the thickness, material and lamination parameters

Note that \(\xi_{E1}\) and \(\xi_{E2}\) are optional and usually equal to zero, becoming important only when the transverse shear modulus is different in the two directions, i.e. when \(G_{13} \ne G{23}\).

Parameters:
thicknessfloat

The total thickness of the plate

matlaminaMatLamina object

Material object

xiAj, xiBj, xiDj, xiEjfloat

The 14 lamination parameters according to the first-order shear deformation theory: \(\xi_{A1} \cdots \xi_{A4}\), \(\xi_{B1} \cdots \xi_{B4}\), \(\xi_{D1} \cdots \xi_{D4}\), \(\xi_{E1}\) and \(\xi_{E2}\)

Returns:
lamShellProp

Shell property with the ABD and ABDE matrices already calculated

Shell property utils module (pyfe3d.shellprop_utils)#

Highly based on the composites. module.

pyfe3d.shellprop_utils.isotropic_plate(thickness, E, nu, offset=0.0, calc_scf=True, rho=0.0)#

Read data for an isotropic plate

ShellProp object is returned based on the inputs given.

Parameters:
thicknessfloat

Plate thickness.

Efloat

Young modulus.

nufloat, optional

Poisson’s ratio.

rhofloat, optional

Material density

offsetfloat, optional

Offset along the normal axis about the mid-surface, which influences the extension-bending coupling (B matrix).

calc_scfbool, optional

If True, use ShellProp.calc_scf() to compute shear correction factors, otherwise the default value of 5/6 is used.

pyfe3d.shellprop_utils.laminated_plate(stack, plyt=None, laminaprop=None, rho=0.0, plyts=None, laminaprops=None, rhos=None, offset=0.0, calc_scf=True)#

Read a laminate stacking sequence data.

ShellProp object is returned based on the inputs given.

Parameters:
stacklist

Angles of the stacking sequence in degrees.

plytfloat, optional

When all plies have the same thickness, plyt can be supplied.

laminaproptuple, optional

When all plies have the same material properties, laminaprop can be supplied.

rhofloat, optional

Uniform material density to be used for all plies.

plytslist, optional

A list of floats with the thickness of each ply.

laminapropslist, optional

A list of tuples with a laminaprop for each ply.

rhoslist, optional

A list of floats with the material density of each ply.

offsetfloat, optional

Offset along the normal axis about the mid-surface, which influences the laminate properties.

calc_scfbool, optional

If True, use ShellProp.calc_scf() to compute shear correction factors, otherwise the default value of 5/6 is used

Notes

plyt or plyts must be supplied laminaprop or laminaprops must be supplied

For orthotropic plies, the laminaprop should be:

laminaprop = (E11, E22, nu12, G12, G13, G23)

For isotropic plies, the laminaprop should be:

laminaprop = (E, nu)
pyfe3d.shellprop_utils.read_laminaprop(laminaprop, rho=0)#

Returns a MatLamina object based on an input laminaprop tuple

Parameters:
laminaproplist or tuple

For the most general case of tri-axial stress, use a tuple containing the folliwing entries:

laminaprop = (e1, e2, nu12, g12, g13, g23, e3, nu13, nu23)

For isotropic materials aiming calculations with tri-axial stresses, use:

g = e/(2*(1+nu))
laminaprop = (e, e, nu, g, g, g, e, nu, nu)

For othotropic materials with in-plane stresses the user can only supply:

laminaprop = (e1, e2, nu12, g12, g13, g23)

For isotropic materials with in-plane stresses the user can only supply:

laminaprop = (e, nu) # new

symbol

value

e1

Young Module in direction 1

e2

Young Module in direction 2

nu12

12 Poisson’s ratio

g12

12 Shear Modulus

g13

13 Shear Modulus

g23

13 Shear Modulus

e3

Young Module in direction 3

nu13

13 Poisson’s ratio

nu23

23 Poisson’s ratio

rhofloat, optional

Material density

Returns:
matlamMatLamina

A MatLamina object.