/MAT/LAW112 (PAPER or XIA)

Block Format Keyword The Paperboard law models an orthotropic and dissymmetric elasto-plastic material from proposed by Xia, 2002.

The basic principle is to fully uncouple the behavior in the plane of the paper sheet and the behavior out of the plane. A yield stress is defined for each directions of loading, in tension and compression.

Format

(1) (2) (3) (4) (5) (6) (7) (8) (9) (10)
/MAT/LAW112/mat_ID/unit_ID or /MAT/PAPER/mat_ID/unit_ID or /MAT/XIA/mat_ID/unit_ID
mat_title
ρi
E1 E2 E3 Ires Itab Ismooth
ν21 G12 G23 G13
K E3C CC
ν1p ν2p ν4p ν5p
If Itab = 0, insert continuous yield stresses
(1) (2) (3) (4) (5) (6) (7) (8) (9) (10)
S01 A01 B01 C01
S02 A02 B02 C02
S03 A03 B03 C03
S04 A04 B04 C04
S05 A05 B05 C05
ASIG BSIG CSIG
TAU0 ATAU BTAU
If Itab = 1, insert tabulated yield stresses
(1) (2) (3) (4) (5) (6) (7) (8) (9) (10)
TAB_YLD1 MAT_Xscale1 MAT_Yscale1
TAB_YLD2 MAT_Xscale2 MAT_Yscale2
TAB_YLD3 MAT_Xscale3 MAT_Yscale3
TAB_YLD4 MAT_Xscale4 MAT_Yscale4
TAB_YLD5 MAT_Xscale5 MAT_Yscale5
TAB_YLDC MAT_XscaleC MAT_YscaleC
TAB_YLDS MAT_XscaleS MAT_YscaleS

Definition

Field Contents SI Unit Example
mat_ID Material identifier.

(Integer, maximum 10 digits)

unit_ID (Optional) Unit Identifier.

(Integer, maximum 10 digits)

mat_title Material title.

(Character, maximum 100 characters)

ρi Initial density.

(Real)

[kgm3]
Ei Young’s modulus in the ith orthotropic direction.

(Real)

[Pa]
νij Poisson's ratio related to the ith and jth orthotropic direction.

(Real)

Gij Shear modulus related to the ith and jth orthotropic direction.

(Real)

[Pa]
Ires Resolution method for plasticity.
= 0
Set to 2
= 1
NICE (Next Increment Correct Error) explicit method.
= 2 (Default)
Newton iterative method - cutting plane.

(Integer)

Itab Yield stresses computation.
= 0
Continuous yield stresses.
= 1
Tabulated yield stresses.

(Integer)

Ismooth Interpolation type (in case of tabulated yield function).
= 1 (Default)
Linear interpolation.
= 2
Logarithmic interpolation base 10.
=3
Logarithmic interpolation base n.

(Integer)

K In-plane yield surface exponent.

Default = 1.0 (Real)

E3C First elastic compression parameter.

Default = E3 (Real)

[Pa]
CC Second elastic compression parameter.

Default = 1.0 (Real)

ν1p Tensile plastic Poisson’s ratio in direction 1.

(Real)

ν2p Tensile plastic Poisson’s ratio in direction 2.

(Real)

ν4p Compressive plastic Poisson’s ratio in direction 1.

(Real)

ν5p Compressive plastic Poisson’s ratio in direction 2.

(Real)

S0i Initial yield stress in the ith direction of loading.
Each direction is associated to a given loading direction following the order:
i=1
Tension in orthotropic direction 1.
i=2
Tension in orthotropic direction 2.
i=3
In-plane shear.
i=4
Compression in orthotropic direction 1.
i=5
Compression in orthotropic direction 2.
i=C
Compression in out-of-plane direction 3.
i=S
Transverse shear direction.

Default = 1.0e20 (Real)

[Pa]
A0i First hardening parameter in the ith direction of loading.

(Real)

[Pa]
B0i Second hardening parameter in the ith direction of loading.

(Real)

C0i Third hardening parameter in the ith direction of loading.

(Real)

[Pa]
ASIG Initial out-of-plane yield stress in compression.

Default = 1.0e20 (Real)

[Pa]
BSIG First out-of-plane hardening parameter in compression.

(Real)

[Pa]
CSIG Second out-of-plane hardening parameter in compression.

(Real)

TAU0 Initial transverse shear yield stress.

Default = 1.0e20 (Real)

[Pa]
ATAU First transverse shear hardening parameter.

(Real)

[Pa]
BTAU Second transverse shear hardening parameter.

(Real)

TAB_YLDi Tabulated yield stress – plastic strain - strain rate function identifier in the ith direction of loading.

(Integer)

MAT_Xscalei X scale factor of the tabulated yield – plastic strain - strain rate function in the ith direction of loading.

Default = 1.0 (Real)

[Hz]
MAT_Yscalei Y scale factor of the tabulated yield – plastic strain - strain rate function in the ith direction of loading.

Default = 1.0 (Real)

[Pa]

Example (Paper)

Example (Tabulated)

Comments

  1. To describe the behavior of the paperboard material law, the following orthotropic direction is considered.


    Figure 1.
  2. The elastic behavior of this material law is orthotropic.

    The in-plane behavior should be fully uncoupled with the out-of-plane behavior, computed as:

    {σxx=C11εxx+C12εyyσyy=C21εxx+C22εyyσxy=G12γxy

    With C=11ν12ν21[E1ν12E2ν21E1E2]

    The transverse shear components are computed as:

    {σyz=G23εyzσzx=G21εzx

    The out-of-plane elastic behavior (for solids only) is treated as a uniaxial equivalent problem. However, the computation of the stress may differ between tension and compression. The elasticity becomes nonlinear for compressive loadings.

    σzz=E3εezzifεezz0σzz=E3C(1eCcεezz)ifεezz<0

  3. In the Xia 2002 formulation, the in-plane yield criterion, denoted as f , is defined as:
    f=6I=1χI(σ:NIσIY)2k1

    Where,

    χI={1ifσ:NI>00otherwise
    χI
    Switching parameters.
    σ
    Cauchy stress tensor.
    NI
    Normal direction of the yield planes.
    σIY
    Yield stresses.
    k
    Positive integer.
    Each direction is associated to a given loading direction following the order defined below:
    1
    Tension in orthotropic direction 1.
    2
    Tension in orthotropic direction 2.
    3
    Positive in-plane shear.
    4
    Compression in orthotropic direction 1.
    5
    Compression in orthotropic direction 2.
    6
    Negative in-plane shear (same input as positive in-plane shear σ6Y=σ3Y ).

    The normal direction vector to the yield planes are:

    N1=[11+ν21pν1p1+ν21p0000]N2=[ν2p1+ν22p11+ν22p0000]N3=[000100]N4=[11+ν24pν4p1+ν24p0000]N5=[ν5p1+ν25p11+ν25p0000]N6=[000100]

    Each direction I is then associated to a specific yield stress whose expression is:

    σIY=S0I+A0Itanh(B0Iεfp)+C0IεfpwithI[1,6]

    Where, εfp is the in-plane equivalent plastic strain (associated to the yield function f ).

    The out-of-plane yield function is denoted as g is defined as:

    g=σzzσCY with σCY=Aσ+Bσexp(Cσεgp)

    Where, εgp is the out-of-plane equivalent plastic strain (associated to the yield function g ).

    The transverse shear yield function is:

    h=σ2yz+σ2zxσSY1

    Where,
    σSY=τ0+[Aτmin(0,σzz)Bτ]εhp
    εhp
    Out-of-plane equivalent plastic strain (associated to the yield function h ).

    If the tabulated yield stress option is selected (Itab = 1), each yield stress is associated to a table (TAB_YLDi) to define the stress evolution with the plastic strain, at several plastic strain-rate. Two scale factors can be also defined in the X and Y direction for each table. In this case, the hardening parameters S0i , A0i , B0i , C0i , Aσ , Bσ , Cσ , τ0 , Aτ , and Bτ are ignored, and the yield stress becomes:

    σIY=ftab_YLDIY(εfp,˙εfp)I[1,6]σCY=ftab_YLDCY(εgp,˙εgp)σSY=ftab_YLDSY(εhp,˙εhp)

    For output field, an equivalent “global” plastic strain is computed as:

    εp=(εfp)2+(εgp)2+(εhp)2