2.5 Data Tables - Implicit Analysis

2.5 Data Tables - Implicit Analysis (UP19980821 ) A data table is a series of constants that are interpreted when they are used. Data tables are always associated with a material number and are most often used to define nonlinear material data (stress-strain curves, creep constants, swelling constants, and magnetization curves). Other material properties are described in Section 2.4. For some element types, the data table is used for special element input data other than material properties. The form of the data table (referred to as the TB table) depends upon the data being defined. Where the form is peculiar to only one element type, the table is described with the element in Chapter 4. If the form applies to more than one element, it is described below and referenced in the element description. The following topics are described in this section:

Explicit dynamics materials are discussed in Section 2.6.

See Chapter 8 of the ANSYS Structural Analysis Guide for additional details.

2.5.1 Nonlinear Stress-Strain Materials

If Table 4.n-1 lists "plasticity" as a "Special Feature," then several options are available to describe the material behavior of that element. Six rate-independent plasticity options, one rate-dependent plasticity option, an elasticity option, and a user option are shown below. Select the material behavior option via menu path Main Menu>Preprocessor>Material Props> Data Tables>Define/Activate [TB,Lab].

Lab

Material Behavior Option

BKIN

Bilinear Kinematic Hardening (Rate-independent plasticity)

MKIN

Multilinear Kinematic Hardening (Rate-independent plasticity)

KINH

Multilinear Kinematic Hardening (Rate-independent plasticity)

MISO

Multilinear Isotropic Hardening (Rate-independent plasticity)

BISO

Bilinear Isotropic Hardening (Rate-independent plasticity)

ANISO

Anisotropic (Rate-independent plasticity)

DP

Drucker-Prager (Rate-independent plasticity)

ANAND

Anand's Model (Rate-dependent plasticity)

MELAS

Multilinear Elastic

USER

User-defined Nonlinear Stress-Strain Material Option

All options except DP, ANAND, and USER require a uniaxial stress-strain curve to be input. All options except ANISO and USER must have elastically isotropic (EX=EY=EZ) materials. Required values that aren't included in the data table are assumed to be zero. If the data table is not defined (or contains all zero values), the material is assumed to be linear. The material behavior options are briefly described below. See Chapter 4 of the ANSYS Theory Reference for more detail.

2.5.1.1 Bilinear Kinematic Hardening

This option (BKIN) assumes the total stress range is equal to twice the yield stress, so that the Bauschinger effect is included. BKIN may be used for materials that obey von Mises yield criteria (which includes most metals). The material behavior is described by a bilinear total stress-total strain curve starting at the origin and with positive stress and strain values. The initial slope of the curve is taken as the elastic modulus of the material. At the specified yield stress (C1), the curve continues along the second slope defined by the tangent modulus, C2 (having the same units as the elastic modulus). The tangent modulus cannot be less than zero nor greater than the elastic modulus.

Initialize the stress-strain table with TB,BKIN. For each stress-strain curve, define the temperature [TBTEMP], then define C1 and C2 [TBDATA]. You can define up to six temperature-dependent stress-strain curves (NTEMP=6 maximum on the TB command) in this manner. The constants C1 and C2 are:

Constant

Meaning

C1 Yield stress (Force/Area)

C2 Tangent modulus (Force/Area)

BKIN can be used with the TBOPT option. In this case, TBOPT takes two arguments. For TB,BKIN,,,,0, there is no stress relaxation with an increase in temperature. This option is not recommended for nonisothermal problems. For TB,BKIN,,,,1, Rice's hardening rule is applied (which does take stress relaxation with temperature increase into account). This is the default.

2.5.1.2 Multilinear Kinematic Hardening

There are two options, namely, TB,MKIN and TB,KINH, available to model metal plasticity behavior under cyclic loading. These two options use the Besseling model (see Section 4.1 of the ANSYS Theory Reference), also called the sublayer or overlay model. The material response is represented by multiple layers of perfectly plastic material; the total response is obtained by weighted average behavior of all the layers. Individual weights are derived from the uniaxial stress-strain curve. The uniaxial behavior is described by a piece-wise linear "total stress-total strain curve," starting at the origin, with positive stress and strain values. The slope of the first segment of the curve must correspond to the elastic modulus of the material and no segment slope should be larger. In the following, the option TB,MKIN is described first, followed by that of TB,KINH.

The curve defined with the MKIN option is continuous from the origin with a maximum of five total stress-total strain points. The slope of the first segment of the curve must correspond to the elastic modulus of the material and no segment slope should be larger.

The MKIN option has the following restrictions:

This option is used as follows:

Initialize the stress-strain table with TB,MKIN, followed by a special form of the TBTEMP command (TBTEMP,,STRAIN) to indicate that strains are defined next. The constants (C1-C5), entered on the next TBDATA command, are the five corresponding strain values (the origin strain is not input). The temperature of the first curve is then input with TBTEMP, followed by the TBDATA command with the constants C1-C5 representing the five stresses corresponding to the strains at that temperature. You can define up to five temperature-dependent stress-strain curves (NTEMP=5 max on the TB command) with the TBTEMP command.

MKIN can also be used in conjunction with the TBOPT option (TB,MKIN,,,,TBOPT). TBOPT has the following three valid arguments:

The KINH option removes some of the restrictions of the MKIN option, by allowing the user to define stress-strain curves with more numbers of points and/or for more numbers of temperatures. (TB, KINH is the same as TB, MKIN with TBOPT=2, but with less restrictions on the number of points per curve and the number of temperatures.) You can define up to 40 temperature-dependent stress-strain curves using the KINH option. If you define more than one stress-strain curve for temperature-dependent properties, then each curve should contain the same number of points (up to a maximum of 20 points in each curve). The assumption is that the corresponding points on the different stress-strain curves represent the temperature dependent yield behavior of a particular sublayer. The following example defines a three-layer KINH model for two temperatures.

TB,KINH,1,2,3
TBTEMP,20.0
TBPT,,0.001,1.0
TBPT,,0.1012,1.2
TBPT,,0.2013,1.3
TBTEMP,40.0
TBPT,,0.008,0.9
TBPT,,0.09088,1.0
TBPT,,0.12926,1.05
In the above example, the third point in the two stress-strain curves defines the temperature-dependent yield behavior of the third sublayer.

Note-The mechanical behavior of the TB,KINH option is the same as TB,MKIN with TBOPT=2.

2.5.1.3 Multilinear Isotropic Hardening

This option (MISO) uses the von Mises yield criteria coupled with an isotropic work hardening assumption and can be used for non-cyclic load histories or for those elements that do not support the multilinear kinematic hardening option (MKIN). This option may be preferred for large strain cycling where kinematic hardening could exaggerate the Bauchinger effect. The uniaxial behavior is described by a piece-wise linear total stress-total strain curve, starting at the origin, with positive stress and strain values. The curve is continuous from the origin through 100 (max) stress-strain points. The slope of the first segment of the curve must correspond to the elastic modulus of the material and no segment slope should be larger. No segment can have a slope less than zero.

You can specify up to 20 temperature-dependent stress-strain curves. Initialize the curves with TB,MISO. Input the temperature for the first curve [TBTEMP], followed by up to 100 stress-strain points (the origin stress-strain point is not input) [TBPT]. Define up to 20 temperature-dependent stress-strain curves (NTEMP=20 max on the TB command) in this manner. The constants (X,Y) entered on the TBPT command (2 per command) are:

Constant

Meaning

X Strain value (Dimensionless)

Y Corresponding stress value (Force/Area)

2.5.1.4 Bilinear Isotropic Hardening

This option (BISO) is similar to MISO except that a bilinear curve is used instead of a multilinear curve. The material behavior is described by a bilinear stress-strain curve starting at the origin with positive stress and strain values. The initial slope of the curve is taken as the elastic modulus of the material. At the specified yield stress (C1), the curve continues along the second slope defined by the tangent modulus C2 (having the same units as the elastic modulus). The tangent modulus cannot be less than zero nor greater than the elastic modulus.

Initialize the stress-strain table with TB,BISO. For each stress-strain curve, define the temperature [TBTEMP], then define C1 and C2 [TBDATA]. Define up to six temperature-dependent stress-strain curves (NTEMP=6 max on the TB command) in this manner. The constants C1 and C2 are:

Constant

Meaning

C1 Yield stress (Force/Area)

C2 Tangent modulus (Force/Area)

2.5.1.5 Anisotropic

This option (ANISO) allows for different stress-strain behavior in the material x, y, and z directions as well as different behavior in tension and compression. For anisotropic elastic materials, see Section 2.5.5. A modified von Mises yield criterion is used to determine yielding. The theory is an extension of Hill's formulation as noted in Section 3.1 of the ANSYS Theory Reference. This option is not recommended for cyclic or highly nonproportional load histories since work hardening is assumed. The principal axes of anisotropy coincide with the material (or element) coordinate system and are assumed not to change over the load history.

The material behavior is described by the uniaxial tensile and compressive stress-strain curves in three orthogonal directions and the shear stress-engineering shear strain curves in the corresponding directions. A bilinear response in each direction is assumed. The initial slope of the curve is taken as the elastic moduli of the material. At the specified yield stress, the curve continues along the second slope defined by the tangent modulus (having the same units as the elastic modulus). The tangent modulus cannot be less than zero or greater than the elastic modulus. Temperature dependent curves cannot be input. All values must be input as no defaults are defined. Input the magnitude of the yield stresses (without signs). No yield stress can have a zero value. The tensile x-direction is used as the reference curve for output quantities SEPL and EPEQ.

Initialize the stress-strain table with TB,ANISO. You can define up to 18 constants with TBDATA commands. The constants (C1-C18) entered on TBDATA commands (6 per command) are:

Constant

Meaning (all units are Force/Area)

C1-C3 Tensile yield stresses in the material x, y, and z directions

C4-C6 Corresponding tangent moduli

C7-C9 Compressive yield stresses in the material x, y, and z directions

C10-C12 Corresponding tangent moduli

C13-C15 Shear yield stresses in the material xy, yz, and xz directions

C16-C18 Corresponding tangent moduli

2.5.1.6 Drucker-Prager

This option (DP) is applicable to granular (frictional) material such as soils, rock, and concrete and uses the outer cone approximation to the Mohr-Coulomb law (see Section 3.1 of the ANSYS Theory Reference. The input consists of only three constants:

The amount of dilatancy (the increase in material volume due to yielding) can be controlled with the dilatancy angle. If the dilatancy angle is equal to the friction angle, the flow rule is associative. If the dilatancy angle is zero (or less than the friction angle), there is no (or less of an) increase in material volume when yielding and the flow rule is nonassociated. Temperature-dependent curves are not allowed.

Initialize the constant table with TB,DP. You can define up to three constants with TBDATA commands. The constants (C1-C3) entered on TBDATA are:

Constant

Meaning

C1 Cohesion value (Force/Area)

C2 Angle (in degrees) of internal friction

C3 dilatancy angle (in degrees)

2.5.1.7 Anand's Model

This option (ANAND) has input consisting of 9 constants. The Anand model is applicable to viscoplastic elements VISCO106, VISCO107, and VISCO108. See Section 4.2 of the ANSYS Theory Reference for details. Initialize the constant table with TB,ANAND. You can define up to nine constants (C1-C9) with TBDATA commands (6 per command):

Constant

Meaning

Material Property

Units

C1 so initial value of deformation resistance

stress

C2 Q/R Q = activation energy

R = universal gas constant

energy /volume

energy /(volume temp)

C3 A pre-exponential factor

1 / time

C4 xi multiplier of stress

dimensionless

C5 m strain rate sensitivity of stress

dimensionless

C6 ho hardening / softening constant

stress

C7 1 coefficient for deformation resistance saturation value

stress

C8 n strain rate sensitivity of saturation (deformation resistance) value

dimensionless

C9 a strain rate sensitivity of hardening or softening

dimensionless

1 The coefficient for deformation resistance saturation value is

2.5.1.8 Multilinear Elastic

This option (MELAS) is such that unloading occurs along the same path as loading. This behavior, unlike the other options, is conservative (path-independent). The plastic strain (pl) for this option should be interpreted as a "pseudo plastic strain" since it returns to zero when the material is unloaded (no hysteresis). See Section 4.4 of the ANSYS Theory Reference for details. The material behavior is described by a piece-wise linear stress-strain curve, starting at the origin, with positive stress and strain values. The curve is continuous from the origin through 100 (max) stress-strain points. Successive slopes can be greater than the preceding slope; however, no slope can be greater than the elastic modulus of the material. The slope of the first curve segment usually corresponds to the elastic modulus of the material, although the elastic modulus can be input as greater than the first slope to ensure that all slopes are less than or equal to the elastic modulus.

Specify up to 20 temperature-dependent stress-strain curves. Initialize the curves with TB,MELAS. The temperature for the first curve is input with TBTEMP, followed by TBPT commands for up to 100 stress-strain points (the origin stress-strain point is not input). You can define up to 20 temperature- dependent stress-strain curves (NTEMP=20 max on the TB command) in this manner. The constants (X,Y) entered on TBPT (2 per command) are:

Constant

Meaning

X Strain value (Dimensionless)

Y Corresponding stress value (Force/Area)

2.5.1.9 User

This option (USER) has input consisting of up to NPTS (specified on the TB command) user-defined constants. Initialize the constant table with TB,USER. The constants are defined with TBDATA commands (6 per command).

2.5.2 Mooney-Rivlin Hyperelastic Material Constants

The hyperelastic elements require various constants to define the Mooney-Rivlin function. This function is available in elements HYPER56, HYPER58, HYPER74, HYPER84, HYPER86, and HYPER158. (Note that for elements HYPER84 and HYPER86, only constants C1 and C2 are applicable. These two element types are generally less desirable for modeling incompressible hyperelastic materials than are the other elements.) Initialize the constant table with TB,MOONEY. Define the temperature with TBTEMP, and then define up to nine constants on subsequent TBDATA or *MOONEY commands. You can define up to six temperature-dependent sets of constants (NTEMP=6 max on the TB command) with TBTEMP commands (six per command):

Constant

Meaning

C1 1st strain energy constant (a10)

C2 2nd strain energy constant (a01)

C3 3rd strain energy constant (a20)

C4 4th strain energy constant (a11)

C5 5th strain energy constant (a02)

C6 6th strain energy constant (a30)

C7 7th strain energy constant (a21)

C8 8th strain energy constant (a12)

C9 9th strain energy constant (a03)

These constants have the units of strain energy per unit volume (Force/Area).

You can use the *MOONEY command to automatically determine two-term, five-term, or nine-term constants from physical test data.

2.5.3 Viscoelastic Material Constants

Elements VISCO88 and VISCO89 use a viscoelastic material model that is defined by entering the following data in the data table with TB commands. Data not input are assumed to be zero. You must enter the data table to perform the viscoelastic computation. A generalized Maxwell model is used to represent the material characteristics. See the ANSYS Theory Reference for an explanation of terms. Initialize the constant table with TB,EVISC. You can define up to 95 constants (C1-C95) with TBDATA commands (6 per command):

Constant - Meaning
1 - H/R (activation energy (H) divided by ideal gas constant (R)).
2 - Value of the constant x (0.0x1.0).
3 - No. of Maxwell elements (10 max) in volume decay function MV.
6-15 - Up to ten values of Cfi (coefficients of the Maxwell element
representing the volume decay function MV). Used to define the fictive temperature. ( Cfi = 1.0)
16-25 - Up to ten values of fi (constants associated with a discrete relaxation
spectrum). Used to define the fictive temperature. Each fi is also known as a relaxation time.
26-30 - Up to five values of Ci (coefficients of thermal expansion for the liquid state). ( = C1 + C2Tf + C3Tf2 + C4Tf3 + C5Tf4, where Tf = fictive temperature)
31-35 - Up to five values of Cgi (coefficients of thermal expansion for the glass state). (g = Cg1 + Cg2T + Cg3T2 + Cg4T3+ Cg5T4, where T = actual temperature)
36-45 - Up to ten values of Tfi (fictive temperature). Tf = CfiTfi
46 - GXY(0) (shear modulus at time = zero (the full shear modulus)).
47 - GXY() (shear modulus at time = infinity (the residual shear modulus after the full decay)). If no relaxation of the shear modulus,
use GXY() = GXY(0).
48 - K(0) (bulk modulus at time = zero).
49 - K() (bulk modulus at time = infinity). If no relaxation of the bulk
modulus, use K() = K(0).
50 - No. of Maxwell elements (10 max) used to approximate the shear
modulus (GXY(0) - GXY()) relaxation.
51-60 - Up to ten values of Csmi (coefficients for shear modulus relaxation
using Maxwell elements, Csmi = 1.0 if shear modulus relaxes).
61-70 - Up to ten values of smi (relaxation times for shear modulus relaxation using Maxwell elements).
71 - No. of Maxwell elements (10 max) used to approximate the bulk
modulus (K(0) - K()) relaxation.
76-85 - Up to ten values of Cbmi (coefficients for bulk modulus relaxation
using Maxwell elements, Cbmi = 1.0 if bulk modulus relaxes).
86-95 - Up to ten values of bmi (relaxation times for bulk modulus relaxation
using Maxwell elements).

2.5.4 Magnetic Materials

Elements with magnetic capability use the TB table to input points characterizing B-H curves. See Section 5.1 of the ANSYS Theory Reference for details. These curves are available in elements SOLID5, PLANE13, PLANE53, SOLID62, SOLID96, and SOLID98. Temperature-dependent curves cannot be input. Initialize the curves with TB,BH. Use TBPT commands to define up to 100 points (H,B). The constants (X,Y) entered on TBPT (2 per command) are:

Constant

Meaning

X Magnetic field intensity (H) (Magneto-motive force/length)

Y Corresponding magnetic flux density (B) (Flux/Area)

Specify the system of units (MKS, CGS, or user defined) with EMUNIT, which also determines the value of the permeability of free space. Free-space permeability is available in elements SOLID5, INFIN9, PLANE13, INFIN47, PLANE53, SOLID62, SOLID96, SOLID97, SOLID98, INFIN110, and INFIN111. This value is used with the relative permeability property values [MP] to establish absolute permeability values. The defaults (also obtained for Lab=MKS) are MKS units and free-space permeability of 4E-7 Henries/meter. If you specify the CGS system of units by Lab=CGS, free-space permeability is set to 1.0 (dimensionless). You can specify Lab=MUZRO to define any system of units, then input free-space permeability.

2.5.5 Anisotropic Elastic Materials

Anisotropic elastic capability is available with the SOLID64 structural element and the SOLID5, PLANE13, and SOLID98 coupled-field elements. For nonlinear anisotropic materials, see Section 2.5.1.5. Input the elastic coefficient matrix [D] either by specifying the stiffness constants (EX, EY, etc.) with MP commands, or by specifying the terms of the matrix with data table commands as described below. The matrix should be symmetric and positive definite (requiring all determinants to be positive).

The full 6 x 6 elastic coefficient matrix [D] relates terms ordered x,y,z,xy,yz,xz via 21 constants as shown below.

For 2-D problems, a 4 x 4 matrix relates terms ordered x,y,z,xy via 10 constants (D11, D21, D22, D31, D32, D33, D41, D42, D43, D44). Note, the order of the vector is expected as {x,y,z,xy,yz,xz}, whereas for some published materials the order is given as {x,y,z,yz,xz,xy}. This difference requires the "D" matrix terms to be converted to the expected format. The "D" matrix can be defined in either "stiffness" form (with units of Force/Area operating on the strain vector) or in "compliance" form (with units of the inverse of Force/Area operating on the stress vector), whichever is more convenient. Select a form using the appropriate element KEYOPT. Both forms use the same data table input as described below.

Enter the constants of the elastic coefficient matrix in the data table with the TB commands. Initialize the constant table with TB,ANEL. Define the temperature with TBTEMP, followed by up to 21 constants input with TBDATA commands. For the coupled-field elements, temperature- dependent matrix terms are not allowed. For the SOLID64 element, you can define up to six temperature-dependent sets of constants (NTEMP=6 max on the TB command) in this manner. Matrix terms are linearly interpolated between temperature points. The constants (C1-C21) entered on TBDATA (6 per command) are:

Constant

Meaning

C1-C6

Terms D11, D21, D31, D41, D51, D61

C7-C12

Terms D22, D32, D42, D52, D62, D33

C13-C18

Terms D43, D53, D63, D44, D54, D64

C19-C21

Terms D55, D65, D66

2.5.6 Piezoelectric Materials

Piezoelectric capability (not allowed in the ANSYS/Emag product) allows coupling between the structural and electric fields for the SOLID5, PLANE13, and SOLID98 coupled-field elements. Material properties required for the piezoelectric effects include the dielectric (permittivity) constants, the elastic coefficient matrix [c], and the piezoelectric matrix [e]. Input the dielectric constants on the MP command as the usual linear material properties (PERX, PERY, PERZ).

Input the elastic coefficient matrix [c] either by specifying the stiffness constants (EX, EY, etc.) with MP commands, or by specifying the terms of the matrix with TB commands as described in Section 2.5.4.

The full 6 x 3 piezoelectric matrix [e] relates terms x,y,z,xy,yz,xz to x,y,z via 18 constants as shown:

For 2-D problems, a 4 x 2 matrix relates terms ordered x,y,z,xy via 8 constants (e11, e12, e21, e22, e31, e32, e41, e42). The order of the vector is expected as {x,y,z,xy,yz,xz}, whereas for some published materials the order is given as {x,y,z,yz,xz,xy}. This difference requires the "e" matrix terms to be converted to the expected format.

Use the TB commands to enter the constants of the piezoelectric [e] matrix in the data table. Initialize the constant table with TB,PIEZ. You can define up to 18 constants (C1-C18) with TBDATA commands (6 per command):

Constant

Meaning

C1-C6 Terms e11, e12, e13, e21, e22, e23

C7-C12 Terms e31, e32, e33, e41, e42, e43

C13-C18 Terms e51, e52, e53, e61, e62, e63

2.5.7 Creep Equations

If Table 4.n-1 lists "creep" as a "Special Feature," then the element can model creep behavior. The creep strain rate, , can be a function of stress, strain, temperature, and neutron flux level. Tables 2.5-1 through 2.5-14 show a library of creep strain rate equations. Enter the constants shown in these equations into the data table as described below. These equations (expressed in incremental form) are characteristic of materials being used in creep design applications (see Section 4.3 of the ANSYS Theory Reference. You can incorporate other creep expressions into the program via user programmable features. See Guide to ANSYS User Programmable Features for more information.

Three different types of creep equations are available:

If you select more than one type of creep, the combined effects are used (except where indicated).

A linear stepping function is used to calculate the change in the creep strain within a time step (cr = ()(t)). The creep strain rate is evaluated at the condition corresponding to the beginning of the time interval and is assumed to remain constant over the time interval. Primary equivalent stresses and strains are used to evaluate the creep strain rate. For highly nonlinear creep strain vs. time curves, use a small time step. A creep time step optimization procedure is available for automatically increasing the time step whenever possible. A nonlinear stepping function (based on an exponential decay) is also available (C11=1) but should be used with caution since it can underestimate the total creep strain where primary stresses dominate. This function is available only for creep equations C6=0,1 and 2. Temperatures used in the creep equations should be based on an absolute scale [TOFFST].

Specify primary creep with constant C6. Tables 2.5-1 through 2.5-11 show the available equations. An equation is selected with the appropriate value of C6 (0 to 15). If C1 0, or if T + TOFFST 0, no primary creep is computed.

Specify secondary creep with constant C12. Tables 2.5-12 and 2.5-13 show the available equations. An equation is selected with the appropriate value of C12 (0 or 1). If C7 0, or if T + TOFFST 0, no secondary creep is computed. Also, primary creep equations C6=9,10,11,13,14, and 15 bypass any secondary creep equations since secondary effects are included in the primary part.

Specify irradiation induced creep with constant C66. Table 2.5-14 shows the single equation currently available; select it with C66=5. This equation can be used in conjunction with equations C6=0 to 11. The constants should be entered into the data table as indicated by their subscripts. If C55 0 and C61 0, or if T + TOFFST 0, no irradiation induced creep is computed.

Use the BF or BFE commands to enter temperature and fluence values. The input fluence (t) includes the integrated effect of time and time explicitly input is not used in the fluence calculation. Also, for the usual case of a constant flux (), the fluence should be linearly ramp changed.

Initialize the creep table with TB,CREEP. Temperature-dependent creep coefficients are not permitted (TBTEMP is not valid for creep). The constants entered on the TBDATA commands (6 per command) are:

Constant

Meaning

C1-CN

Constants C1, C2, C3, etc. (as defined in Tables 2.5-1 to 2.5-14) These are obtained by curve fitting test results for your material to the equation you choose. Exceptions are defined below.

Table 2.5-1 Primary Creep Equation for C6=0

where:

= equivalent strain (based on modified total strain)

= equivalent stress

T = temperature (absolute). TOFFST is internally added to all temperatures for convenience.

t = time at end of substep

e = natural logarithm base

Table 2.5-2 Primary Creep Equation for C6=1

Table 2.5-3 Primary Creep Equation for C6 =2

where:

Table 2.5-4 Primary Creep Equation for C6=9

Annealed 304 Stainless Steel:

Double Exponential Creep Equation (C4 = 0.0)
To use the following Double Exponential creep equation to calculate c, enter C4 = 0.0:

c = x (1-e-st) + t (1-e-rt) +

where:

x = 0 for C2

x = G + H for C2 < C3

C2 = 6000 psi (default), C3 = 25000 psi (default)

s, r, , G, and H are the functions of temperature and stress as described in the reference.

This double exponential equation is valid for Annealed 304 Stainless Steel over a temperature range from 800 to 1100°F. The equation, known as the Blackburn creep equation when C1 = 1, is described completely in the Nuclear Systems Material Handbook1. The first two terms describe the primary creep strain and the last term describes the secondary creep strain.

To use this equation, input a nonzero value for C1, C6 = 9.0, and C7 = 0.0. Temperatures should be in °R (or °F with TOFFST = 460.0). Conversion to °K for the built-in property tables is done internally. If the temperature is below the valid range, no creep is computed. Time should be in hours and stress in psi. The valid stress range is 6,000 - 25,000 psi.

Rational Polynomial Creep Equation with Metric Units (C4 = 1.0)
To use the following standard Rational Polynomial creep equation (with metric units) to calculate c, enter C4 = 1.0:

where:

c = limiting value of primary creep strain

p = primary creep time factor

= secondary (minimum) creep strain rate

This standard rational polynomial creep equation is valid for Annealed 304 SS over a temperature range from 427°C to 704°C. The equation is described completely in the Nuclear Systems Material Handbook1. The first term describes the primary creep strain. The last term describes the secondary creep strain. The average "lot constant" from Footnote 1 is used to calculate .

To use this equation, input C1 = 1.0, C4 = 1.0, C6 = 9.0, and C7 = 0.0. Temperature must be in °C and TOFFST must be 273 (because of the built-in property tables). If the temperature is below the valid range, no creep is computed. Also, time must be in hours and stress in Megapascals (MPa).

Various hardening rules governing the rate of change of creep strain during load reversal may be selected with the C5 value: 0.0 - time hardening, 1.0 - total creep strain hardening, 2.0 - primary creep strain hardening. These options are available only with the standard rational polynomial creep equation.

Rational Polynomial Creep Equation with English Units (C4 = 2.0)
To use the above standard Rational Polynomial creep equation (with English units), enter C4 = 2.0.

This standard rational polynomial equation is the same as described above except that temperature must be in °F, TOFFST must be 460, and stress must be in psi. The equivalent valid temperature range is 800 - 1300°F.

Table 2.5-5 Primary Creep Equation for C6=10

Annealed 316 Stainless Steel:

Double Exponential Creep Equation (C4 = 0.0)
To use the same form of the Double Exponential creep equation as described for Annealed 304 SS (C6 = 9.0, C4 = 0.0) in Table 2.5-4 to calculate c, enter C4 = 0.0.

This equation, also described in Ref. 1, differs from the Annealed 304 SS equation in that the built-in property tables are for Annealed 316 SS, the valid stress range is 4000 - 30,000 psi, C2 defaults to 4000 psi, C3 defaults to 30,000 psi, and the equation is called with C6 = 10.0 instead of C6 = 9.0.

Rational Polynomial Creep Equation with Metric Units (C4 = 1.0)
To use the same form of the standard Rational Polynomial creep equation with metric units as described for Annealed 304 SS (C6 = 9.0, C4 = 1.0) in Table 2.5-4, enter C4 = 1.0.

This standard rational polynomial equation, also described in Ref. 1, differs from the Annealed 304 SS equation in that the built-in property tables are for Annealed 316 SS, the valid temperature range is 482 - 704°C, and the equation is called with C6 = 10.0 instead of C6 = 9.0. The hardening rules for load reversal described for the C6 = 9.0 standard Rational Polynomial creep equation are also available. The average "lot constant" from Ref. 1 is used in the calculation of .

Rational Polynomial Creep Equation with English Units (C4 = 2.0)
To use the previous standard Rational Polynomial creep equation with English units, enter C4 = 2.0.

This standard rational polynomial equation is the same as described above except that the temperatures must be in °F, TOFFST must be 460, and the stress must be in psi (with a valid range from 0.0 to 24220 psi). The equivalent valid temperature range is 900 - 1300°F.

Table 2.5-6 Primary Creep Equation for C6=11

Annealed 2 1/4 Cr - 1 Mo Low Alloy Steel:

Modified Rational Polynomial Creep Equation (C4 = 0.0)
To use the following Modified Rational Polynomial creep equation to calculate c, enter C4 = 0.0:

A, B, and are functions of temperature and stress as described in the reference.

This modified rational polynomial equation is valid for Annealed 2 1/4 Cr -1 Mo Low Alloy steel over a temperature range of 700 - 1100 °F. The equation is described completely in the Nuclear Systems Material Handbook2. The first term describes the primary creep strain and the last term describes the secondary creep strain. No modification is made for plastic strains.

To use this equation, input C1 = 1.0, C6 = 11.0, and C7 = 0.0. Temperatures must be in °R (or °F with TOFFST = 460.0). Conversion to °K for the built-in property tables is done internally. If the temperature is below the valid range, no creep is computed. Time should be in hours and stress in psi. Valid stress range is 1000 - 65,000 psi.

Rational Polynomial Creep Equation with Metric Units (C4 = 1.0)
To use the following standard Rational Polynomial creep equation (with metric units) to calculate c, enter C4 = 1.0:

where:

c = limiting value of primary creep strain

p = primary creep time factor

= secondary (minimum) creep strain rate

This standard rational polynomial creep equation is valid for Annealed 2 1/4 Cr - 1 Mo Low Alloy Steel over a temperature range from 371°C to 593°C. The equation is described completely in the Nuclear Systems Material Handbook2. The first term describes the primary creep strain and the last term describes the secondary creep strain. No tertiary creep strain is calculated. Only Type I (and not Type II) creep is supported. No modification is made for plastic strains.

To use this equation, input C1 = 1.0, C4 = 1.0, C6 = 11.0, and C7 = 0.0. Temperatures must be in °C and TOFFST must be 273 (because of the built-in property tables). If the temperature is below the valid range, no creep is computed. Also, time must be in hours and stress in Megapascals (MPa). The hardening rules for load reversal described for the C6 = 9.0 standard Rational Polynomial creep equation are also available.

Rational Polynomial Creep Equation with English Units (C4 = 2.0)
To use the above standard Rational Polynomial creep equation with English units, enter C4 = 2.0.

This standard rational polynomial equation is the same as described above except that temperatures must be in °F, TOFFST must be 460, and stress must be in psi. The equivalent valid temperature range is 700 - 1100°F.

Table 2.5-7 Primary Creep Equations for C6=12

where

C1 =

Scaling constant

M,N,K =

Function of temperature (determined by linear interpolation within table) as follows:

C5

Number of temperature values to describe M, N, or K function
(2 minimum, 6 maximum)

C49

First absolute temperature value

C50

Second absolute temperature value

...

C48+C5

C5th absolute temperature value

C48+C5+1

First M value

...

C48+2C5

C5th M value

C48+2C5

C5th M value

...

C48+2C5

C5th M value

C48+2C5+1

First N value

...

C48+3C5

C5th N value

C48+3C5+1

First K value

...

This power function creep law having temperature dependent coefficients is similar to Equation C6 = 1.0 except with C1 = f1(T), C2 = f2(T), C3 = f3(T), and C4 = 0. Temperatures must not be input in decreasing order.

Table 2.5-8 Primary Creep Equation for C6=13

where:

acc = creep strain accumulated to this time (calculated by the program). Internally set to 1 x 10-5 at the first substep with nonzero time to prevent division by zero.

A = C1/T

B = C2/T + C3

C = C4/T + C5

This equation is often referred to as the Sterling Power Function creep equation. Constant C7 should be 0.0. Constant C1 should not be 0.0, unless no creep is to be calculated.

Table 2.5-9 Primary Creep Equation for C6=14

where:

c = cpt/(1+pt) +

ln c = -1.350 - 5620/T - 50.6 x 10-6 + 1.918 ln (/1000)

ln p = 31.0 - 67310/T + 330.6 x 10-6 - 1885.0 x 10-122

ln = 43.69 - 106400/T + 294.0 x 10-6 + 2.596 ln (/1000)

This creep law is valid for Annealed 316 SS over a temperature range from 800°F to 1300°F. The equation is similar to that given for C6 = 10.0 and is also described in Ref. 1.

To use equation, input C1 = 1.0 and C6 = 14.0. Temperatures should be in °R (or °F with TOFFST = 460). Time should be in hours. Constants are only valid for English units (pounds and inches). Valid temperature range: 800° - 1300°F. Maximum stress allowed for ec calculation: 45,000 psi; minimum stress: 0.0 psi. If T + TOFFST < 1160, no creep is computed.

Table 2.5-10 Primary Creep Equation for C6=15

General Material Rational Polynomial:

where:

= C2 (C2 must not be negative)

c = C7

p = C10

This rational polynomial creep equation is a generalized form of the standard rational polynomial equations given as C6 = 9.0, 10.0, and 11.0 (C4 = 1.0 and 2.0). This equation reduces to the standard equations for isothermal cases. The hardening rules for load reversal described for the C6 = 9.0 standard Rational Polynomial creep equation are also available.

Table 2.5-11 Primary Creep Equation for C6=100

A user-defined creep equation is used. See the Guide to ANSYS User Programmable Features for more information.

Table 2.5-12 Secondary Creep Equation for C12=0

where:

= equivalent stress

T = temperature (absolute). TOFFST is internally added to all temperatures for convenience.

t = time

e = natural logarithm base

Table 2.5-13 Secondary Creep Equation for C12=1

Table 2.5-14 Irradiation Induced Creep Equation for C66=5

where:

B = FG + C63

F =

G = 1 - e-t/C62a

= equivalent stress

T = temperature (absolute). TOFFST is internally added to all temperatures for convenience.

t = neutron fluence (input on BF or BFE command)

t = time

e = natural logarithm base

This irradiation induced creep equation is valid for 20% Cold Worked 316 SS over a temperature range from 700° to 1300°F. Constants 56, 57, 58 and 62 must be positive if the B term is included.

2.5.8 Swelling Equations

If Table 4.n-1 lists "swelling" as a "Special Feature," then the element can model swelling behavior. Swelling is a material enlargement due to neutron bombardment and other effects (see Section 4.8 of the ANSYS Theory Reference). The swelling strain rate may be a function of temperature, time, neutron flux level, and stress.

The fluence (which is the flux x time) is input on the BF or BFE command. A linear stepping function is used to calculate the change in the swelling strain within a load step:

where t is the fluence and the swelling strain rate equation is as defined in subroutine USERSW.

Because of the many empirical swelling equations available, the programming of the actual swelling equation is left to the user. In fact, the equation and the "fluence" input may be totally unrelated to nuclear swelling. See the Guide to ANSYS User Programmable Features for user programmable features.

For highly nonlinear swelling strain vs. fluence curves a small fluence step should be used. Note that since fluence (t), and not flux (), is input, a constant flux requires that a linearly changing fluence be input if time is changing. Temperatures used in the swelling equations should be based on an absolute scale [TOFFST]. Temperature and fluence values are entered with the BF or BFE command. Swelling calculations for the current substep are based upon the previous substep results.

Initialize the swelling table with TB,SWELL. The constants entered on the TBDATA commands (6 per command) are:

Constant

Meaning

C1-CN

Constants C1, C2, C3, etc. (as required by the user swelling equations). C72 must equal 10.