Corrected definition of vector n and d per deformation system; n is the system plane normal and d the corresponding direction
This commit is contained in:
parent
fe2f3e4d36
commit
d3343ef795
|
@ -657,14 +657,14 @@ function lattice_initializeStructure(struct,CoverA)
|
|||
if (lattice_fcc_Nstructure == 1_pInt) then
|
||||
processMe = .true.
|
||||
do i = 1,myNslip
|
||||
sn(:,i) = lattice_fcc_systemSlip(1:3,i)/dsqrt(math_mul3x3(lattice_fcc_systemSlip(1:3,i),lattice_fcc_systemSlip(1:3,i)))
|
||||
sd(:,i) = lattice_fcc_systemSlip(4:6,i)/dsqrt(math_mul3x3(lattice_fcc_systemSlip(4:6,i),lattice_fcc_systemSlip(4:6,i)))
|
||||
st(:,i) = math_vectorproduct(sn(:,i),sd(:,i))
|
||||
sd(:,i) = lattice_fcc_systemSlip(1:3,i)/dsqrt(math_mul3x3(lattice_fcc_systemSlip(1:3,i),lattice_fcc_systemSlip(1:3,i)))
|
||||
sn(:,i) = lattice_fcc_systemSlip(4:6,i)/dsqrt(math_mul3x3(lattice_fcc_systemSlip(4:6,i),lattice_fcc_systemSlip(4:6,i)))
|
||||
st(:,i) = math_vectorproduct(sd(:,i),sn(:,i))
|
||||
enddo
|
||||
do i = 1,myNtwin
|
||||
tn(:,i) = lattice_fcc_systemTwin(1:3,i)/dsqrt(math_mul3x3(lattice_fcc_systemTwin(1:3,i),lattice_fcc_systemTwin(1:3,i)))
|
||||
td(:,i) = lattice_fcc_systemTwin(4:6,i)/dsqrt(math_mul3x3(lattice_fcc_systemTwin(4:6,i),lattice_fcc_systemTwin(4:6,i)))
|
||||
tt(:,i) = math_vectorproduct(tn(:,i),td(:,i))
|
||||
td(:,i) = lattice_fcc_systemTwin(1:3,i)/dsqrt(math_mul3x3(lattice_fcc_systemTwin(1:3,i),lattice_fcc_systemTwin(1:3,i)))
|
||||
tn(:,i) = lattice_fcc_systemTwin(4:6,i)/dsqrt(math_mul3x3(lattice_fcc_systemTwin(4:6,i),lattice_fcc_systemTwin(4:6,i)))
|
||||
tt(:,i) = math_vectorproduct(td(:,i),tn(:,i))
|
||||
ts(i) = lattice_fcc_shearTwin(i)
|
||||
enddo
|
||||
interactionSlipSlip => lattice_fcc_interactionSlipSlip
|
||||
|
@ -681,14 +681,14 @@ function lattice_initializeStructure(struct,CoverA)
|
|||
if (lattice_bcc_Nstructure == 1_pInt) then
|
||||
processMe = .true.
|
||||
do i = 1,myNslip
|
||||
sn(:,i) = lattice_bcc_systemSlip(1:3,i)/dsqrt(math_mul3x3(lattice_bcc_systemSlip(1:3,i),lattice_bcc_systemSlip(1:3,i)))
|
||||
sd(:,i) = lattice_bcc_systemSlip(4:6,i)/dsqrt(math_mul3x3(lattice_bcc_systemSlip(4:6,i),lattice_bcc_systemSlip(4:6,i)))
|
||||
st(:,i) = math_vectorproduct(sn(:,i),sd(:,i))
|
||||
sd(:,i) = lattice_bcc_systemSlip(1:3,i)/dsqrt(math_mul3x3(lattice_bcc_systemSlip(1:3,i),lattice_bcc_systemSlip(1:3,i)))
|
||||
sn(:,i) = lattice_bcc_systemSlip(4:6,i)/dsqrt(math_mul3x3(lattice_bcc_systemSlip(4:6,i),lattice_bcc_systemSlip(4:6,i)))
|
||||
st(:,i) = math_vectorproduct(sd(:,i),sn(:,i))
|
||||
enddo
|
||||
do i = 1,myNtwin
|
||||
tn(:,i) = lattice_bcc_systemTwin(1:3,i)/dsqrt(math_mul3x3(lattice_bcc_systemTwin(1:3,i),lattice_bcc_systemTwin(1:3,i)))
|
||||
td(:,i) = lattice_bcc_systemTwin(4:6,i)/dsqrt(math_mul3x3(lattice_bcc_systemTwin(4:6,i),lattice_bcc_systemTwin(4:6,i)))
|
||||
tt(:,i) = math_vectorproduct(tn(:,i),td(:,i))
|
||||
td(:,i) = lattice_bcc_systemTwin(1:3,i)/dsqrt(math_mul3x3(lattice_bcc_systemTwin(1:3,i),lattice_bcc_systemTwin(1:3,i)))
|
||||
tn(:,i) = lattice_bcc_systemTwin(4:6,i)/dsqrt(math_mul3x3(lattice_bcc_systemTwin(4:6,i),lattice_bcc_systemTwin(4:6,i)))
|
||||
tt(:,i) = math_vectorproduct(td(:,i),tn(:,i))
|
||||
ts(i) = lattice_bcc_shearTwin(i)
|
||||
enddo
|
||||
interactionSlipSlip => lattice_bcc_interactionSlipSlip
|
||||
|
@ -706,28 +706,28 @@ function lattice_initializeStructure(struct,CoverA)
|
|||
processMe = .true.
|
||||
! converting from 4 axes coordinate system (a1=a2=a3=c) to ortho-hexgonal system (a, b, c)
|
||||
do i = 1,myNslip
|
||||
hex_n(1) = lattice_hex_systemSlip(1,i) ! plane (hkil)->(h (h+2k)/sqrt(3) l/(c/a))
|
||||
hex_n(2) = (lattice_hex_systemSlip(1,i)+2.0_pReal*lattice_hex_systemSlip(2,i))/dsqrt(3.0_pReal)
|
||||
hex_n(3) = lattice_hex_systemSlip(4,i)/CoverA
|
||||
hex_d(1) = lattice_hex_systemSlip(5,i)*1.5_pReal ! direction [uvtw]->[3u/2 (u+2v)*sqrt(3)/2 w*(c/a)]
|
||||
hex_d(2) = (lattice_hex_systemSlip(5,i)+2.0_pReal*lattice_hex_systemSlip(6,i))*(0.5_pReal*dsqrt(3.0_pReal))
|
||||
hex_d(3) = lattice_hex_systemSlip(8,i)*CoverA
|
||||
hex_d(1) = lattice_hex_systemSlip(1,i) ! direction [uvtw]->[3u/2 (u+2v)*sqrt(3)/2 w*(c/a)]
|
||||
hex_d(2) = (lattice_hex_systemSlip(1,i)+2.0_pReal*lattice_hex_systemSlip(2,i))/dsqrt(3.0_pReal)
|
||||
hex_d(3) = lattice_hex_systemSlip(4,i)/CoverA
|
||||
hex_n(1) = lattice_hex_systemSlip(5,i)*1.5_pReal ! plane (hkil)->(h (h+2k)/sqrt(3) l/(c/a))
|
||||
hex_n(2) = (lattice_hex_systemSlip(5,i)+2.0_pReal*lattice_hex_systemSlip(6,i))*(0.5_pReal*dsqrt(3.0_pReal))
|
||||
hex_n(3) = lattice_hex_systemSlip(8,i)*CoverA
|
||||
|
||||
sn(:,i) = hex_n/dsqrt(math_mul3x3(hex_n,hex_n))
|
||||
sd(:,i) = hex_d/dsqrt(math_mul3x3(hex_d,hex_d))
|
||||
st(:,i) = math_vectorproduct(sn(:,i),sd(:,i))
|
||||
sn(:,i) = hex_n/dsqrt(math_mul3x3(hex_n,hex_n))
|
||||
st(:,i) = math_vectorproduct(sd(:,i),sn(:,i))
|
||||
enddo
|
||||
do i = 1,myNtwin
|
||||
hex_n(1) = lattice_hex_systemTwin(1,i)
|
||||
hex_n(2) = (lattice_hex_systemTwin(1,i)+2.0_pReal*lattice_hex_systemTwin(2,i))/dsqrt(3.0_pReal)
|
||||
hex_n(3) = lattice_hex_systemTwin(4,i)/CoverA
|
||||
hex_d(1) = lattice_hex_systemTwin(5,i)*1.5_pReal
|
||||
hex_d(2) = (lattice_hex_systemTwin(5,i)+2.0_pReal*lattice_hex_systemTwin(6,i))*(0.5_pReal*dsqrt(3.0_pReal))
|
||||
hex_d(3) = lattice_hex_systemTwin(8,i)*CoverA
|
||||
hex_d(1) = lattice_hex_systemTwin(1,i)
|
||||
hex_d(2) = (lattice_hex_systemTwin(1,i)+2.0_pReal*lattice_hex_systemTwin(2,i))/dsqrt(3.0_pReal)
|
||||
hex_d(3) = lattice_hex_systemTwin(4,i)/CoverA
|
||||
hex_n(1) = lattice_hex_systemTwin(5,i)*1.5_pReal
|
||||
hex_n(2) = (lattice_hex_systemTwin(5,i)+2.0_pReal*lattice_hex_systemTwin(6,i))*(0.5_pReal*dsqrt(3.0_pReal))
|
||||
hex_n(3) = lattice_hex_systemTwin(8,i)*CoverA
|
||||
|
||||
tn(:,i) = hex_n/dsqrt(math_mul3x3(hex_n,hex_n))
|
||||
td(:,i) = hex_d/dsqrt(math_mul3x3(hex_d,hex_d))
|
||||
tt(:,i) = math_vectorproduct(tn(:,i),td(:,i))
|
||||
tn(:,i) = hex_n/dsqrt(math_mul3x3(hex_n,hex_n))
|
||||
tt(:,i) = math_vectorproduct(td(:,i),tn(:,i))
|
||||
ts(i) = lattice_hex_shearTwin(i)
|
||||
enddo
|
||||
interactionSlipSlip => lattice_hex_interactionSlipSlip
|
||||
|
|
Loading…
Reference in New Issue