VAFCRP1D
Viscous J2 Steel Model
The VAFCRP1D
model is the uniaxial version of the VAFCRP
model.
References
- 10.1017/S0368393100118759
- 10.1179/096034007X207589
- 10.1016/0749-6419(89)90015-6
- 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
So the plastic flow is
where \(n=\dfrac{\eta}{\Big|\eta\Big|}=\dfrac{\sigma-\beta}{\Big|\sigma-\beta\Big|}=\mathrm{sign}~\left( \sigma-\beta\right)\).
V
The Voce (1955) type isotropic hardening equation is used.
where \(\sigma_y\) is the initial elastic limit (yielding stress), \(k_s\) is the saturated stress, \(k_l\) is the linear hardening modulus, \(m\) is a constant that controls the speed of hardening, \(\mathrm{d}p=\Big|\mathrm{d}\varepsilon^p\Big|=\gamma\) is the rate of accumulated plastic strain \(p\).
AF
The Armstrong-Frederick (1966) kinematic hardening rule is used. The rate form of back stress \(\beta^i\) is
where \(a^i\) and \(b^i\) are material constants.
CR
A multiplicative formulation (Chaboche and Rousselier, 1983) is used for the total back stress.
P
The Peric (1993) type definition is used for viscosity.
where \(\mu\) and \(\epsilon\) are two material constants that controls viscosity. Note either (\(\mu\) or (\(\epsilon\) can be set to zero to disable rate-dependent response, in that case this model is identical to the Armstrong-Frederick model.