[Nek5000-users] Problems in getting eigenvalues using ARNOLDI
nek5000-users at lists.mcs.anl.gov
nek5000-users at lists.mcs.anl.gov
Wed Oct 3 01:24:57 CDT 2018
Hi Guillaume,
Thanks for your reply. My reply to your queries is as below:-
1) I am getting unstable pair of Eigen values with growth rate around 0.02.
2) Solver tolerance that I used are ;
7.00000 p020 NORDER
0.100000E-09 p021 DIVERGENCE
0.100000E-09. p022 HELMHOLTZ
0.00000 p023 NPSCAL
0.100000E-09 p024 TOLREL
0.100000E-04 p025 TOLABS
1.00000E-05. p113 : ARNOLDI: arpack tolerance
3) Boundary conditions are :
I am using sponge strength at inlet and outlet with following details in
.rea file
1.00000 p119 : SPONGE STRENGTH
25.0000 p120 : SPONGE TOTAL WIDTH
3.00000 p121 : SPONGE DROP WIDTH (INFLOW)
5.00000 p122 : SPONGE RISE WIDTH (OUTFLOW)
the sponge function and its cal is detailed in userf subroutine of .usr file
Also following is defined in .usr file
c-----------------------------------------------------------------------
subroutine userbc (ix,iy,iz,iside,eg)
include 'SIZE'
include 'NEKUSE' ! UX, UY, UZ, TEMP, X, Y
include 'PARALLEL' ! GLLEL
integer e,eg
c velocity
c e = GLLEL(eg)
UX = 0.0
UY = 0.0
UZ = 0.0
c t
TEMP=0.0
return
end
c-----------------------------------------------------------------------
subroutine useric (ix,iy,iz,ieg)
include 'SIZE'
include 'NEKUSE' ! UX, UY, UZ, TEMP, Z
integer idum
save idum
data idum / 0 /
real eps
if (idum.eq.0) idum = 99 + nid
eps = 0.1
c velocity
c random distribution
UX = eps*(ran1(idum)-0.50)
UY = eps*(ran1(idum)-0.50)
UZ = eps*(ran1(idum)-0.50)
c t
TEMP=0
return
end
40.0000 p109 : ARNOLDI: frequency of calling arn_solve
4.00000 p110 : ARNOLDI: maximal number of arnoldi cycles
90.0000 p111 : ARNOLDI: size of Krylov space
30.0000 p112 : ARNOLDI: number of eigenvectors
If I am increasing the Krylov subspace then will I get Eigen values at
lesser restart ?
Kindly help please as I am new to this. Thanks in advance.
Alok Mishra
Research Scholar
Computational Propulsion Lab
Aerospace Department IIT Kanpur
+91-8795844555
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