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VAFCRP1D

Viscous J2 Steel Model

The VAFCRP1D model is the uniaxial version of the VAFCRP model.

Reference

  1. 10.1017/S0368393100118759
  2. 10.1179/096034007X207589
  3. 10.1016/0749-6419(89)90015-6
  4. 10.1002/nme.1620360807

Theory

The VAFCRP model is a von Mises J2 yield criterion based model and uses an associative plasticity flow. The yield function is defined as

F=|σβ|k.

So the plastic flow is

ε˙p=γFσ=γn,

where n=η|η|=σβ|σβ|=sign (σβ).

V

The Voce (1955) type isotropic hardening equation is used.

k=σy+ks(1emp)+klp,

where σy is the initial elastic limit (yielding stress), ks is the saturated stress, kl is the linear hardening modulus, m is a constant that controls the speed of hardening, dp=|dεp|=γ is the rate of accumulated plastic strain p.

AF

The Armstrong-Frederick (1966) kinematic hardening rule is used. The rate form of back stress βi is

dβi=ai dεpbiβ dp,

where ai and bi are material constants.

CR

A multiplicative formulation (Chaboche and Rousselier, 1983) is used for the total back stress.

β=βi.

P

The Peric (1993) type definition is used for viscosity.

γΔt=γ˙=1μ((|η|k)1ϵ1),

where μ and ϵ are two material constants that controls viscosity. Note either (μ or (ϵ can be set to zero to disable rate-dependent response, in that case this model is identical to the Armstrong-Frederick model.

Syntax

Text Only
material VAFCRP1D (1) (2) (3) (4) (5) (6) (7) (8) [(9) (10)...] [11]
# (1) int, unique material tag
# (2) double, elastic modulus
# (3) double, yield stress
# (4) double, saturated stress
# (5) double, linear hardening modulus
# (6) double, m
# (7) double, mu
# (8) double, epsilon
# (9) double, a
# (10) double, b
# [11] double, density, default: 0.0