This law enables to model hydrodynamic behavior of an elastic-plastic material using
Johnson-Cook Yield criteria and any equation of state available with /EOS
card. It based on /MAT/LAW3 and adds strain rate and temperature
dependency. The advantage of material LAW04 regarding classical LAW02
(/MAT/JCOOK) is that you can choose any available EOS from
/EOS card.
The equation describing yield stress (scale value) is:
図 1 .
σ
y
=
(
A
+
B ε
p
n
)
(
1
+
C ln
ε
˙
ε
0
˙
)
(
1
−
T
*
m
)
Where,
T
*
=
T
-
T
r
T
m
e
l
t
-
T
r
MathType@MTEF@5@5@+=
feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn
hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr
4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9
vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x
fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamivamaaCa
aaleqabaGaamOkaaaakiaad2dadaWcaaqaaiaadsfacaWGTaGaamiv
amaaBaaaleaacaWGYbaabeaaaOqaaiaadsfadaWgaaWcbaGaamyBai
aadwgacaWGSbGaamiDaaqabaGccaWGTaGaamivamaaBaaaleaacaWG Ybaabeaaaaaaaa@439B@
The pressure and energy values are obtained by solving equation of state
P
(
μ
,
E
)
MathType@MTEF@5@5@+=
feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn
hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr
4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9
vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x
fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamiuamaabm
aabaGaeqiVd0MaaiilaiaadweaaiaawIcacaGLPaaaaaa@3B84@
related to the material (/EOS ).
Material parameters are the same as in LAW3.
The parameters are:
C
MathType@MTEF@5@5@+=
feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn
hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr
4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9
vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x
fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaam4qaaaa@36BE@
Strain rate coefficient
ε
˙
0
Reference strain rate
m
MathType@MTEF@5@5@+=
feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn
hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr
4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9
vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x
fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaam4qaaaa@36BE@
Temperature exponent
T melt
Melting temperature
T max
Maximum temperature
For
T
>
T
max
MathType@MTEF@5@5@+=
feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn
hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr
4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9
vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x
fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamivaiabg6
da+iaadsfadaWgaaWcbaGaciyBaiaacggacaGG4baabeaaaaa@3BB0@
, then
m
MathType@MTEF@5@5@+=
feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn
hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr
4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9
vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x
fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaam4qaaaa@36BE@
=1 is used.
ρ
0
C
p
Specific heat per unit volume
For an explanation about strain rate filtering, refer to Strain Rate Filtering .