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11009008

A 3d induction heating example

A 3d induction heating example

The main limitiations with this analysis type are 1) you can't have a
B-H curve in a harmonic analysis and 2)  BH curves are not temperature
dependent.  Given these limitations, the most accurate thing that can be
done is to define a series of effective constant permeabilities, and
assign elements different material set numbers based on their H value.  
Of course, this would be an iterative process.

!
!  3d Induction Heating Example created at ANSYS 6.0
!
/prep7
et,1,117
et,2,117,1                ! volt dof needed in eddy current region
et,11,200,7               ! quad with mid-side nodes for meshing
mp,murx,1,1
mp,murx,2,1000            ! approximate iron properties
mp,rsvx,2,.2e-6  
wprot,,90                 ! build model in xz plane for later use of
csys,1
                         ! build model in inches and scale to meters at
the end
rect,.5,1,,1
rect,.5,1,1,2
rect,.5,1,2,3
rect,1,1.2,,1
rect,1,1.2,1,2
rect,1,1.2,2,3
rect,1.2,2,,1
rect,1.2,2,1,2
rect,1.2,2,2,3
nummrg,kp
lsel,a,,,3,11,4
LESIZE,all,,,20,10,,,,1
lsel,all
lesize,1,,,20,.1,,,,1

lesize,25,,,10,5

lsel,s,,,27,35,4
lesize,all,,,10,.2
lsel,all

FLST,5,4,4,ORDE,4   
FITEM,5,6   
FITEM,5,8   
FITEM,5,18  
FITEM,5,30  
CM,_Y,LINE  
LSEL, , , ,P51X
CM,_Y1,LINE
CMSEL,,_Y   
!*  
LESIZE,_Y1, , ,20, , , , ,1
!*  
FLST,5,8,4,ORDE,8   
FITEM,5,2   
FITEM,5,4   
FITEM,5,10  
FITEM,5,12  
FITEM,5,14  
FITEM,5,22  
FITEM,5,26  
FITEM,5,34  
CM,_Y,LINE  
LSEL, , , ,P51X
CM,_Y1,LINE
CMSEL,,_Y   
!*  
LESIZE,_Y1, , ,10,5, , , ,1
!*  
FLST,5,4,4,ORDE,4   
FITEM,5,2   
FITEM,5,12  
FITEM,5,14  
FITEM,5,26  
CM,_Y,LINE  
LSEL, , , ,P51X
CM,_Y1,LINE
CMSEL,,_Y   
!*  
LESIZE,_Y1, , ,10,.2, , , ,1
!*  
FLST,5,4,4,ORDE,4   
FITEM,5,13  
FITEM,5,15  
FITEM,5,19  
FITEM,5,23  
CM,_Y,LINE  
LSEL, , , ,P51X
CM,_Y1,LINE
CMSEL,,_Y   
LESIZE,_Y1, , ,2, , , , ,1  

type,11
esha,2
amesh,all   

k,101,
k,102,,,1
type,1
esize,,2
vrotate,all,,,,,,101,102,15,1

aclear,1,9,1
etdele,11   
vsel,s,,,2  
eslv
emod,all,mat,2  
emod,all,type,2
alls
local,11,1
emod,all,esys,11      ! so current is applied tangentially

vlscale,all,,,1/39.36,1/39.36,1/39.36,,,1     ! scale to meters
FINISH  

!!! Create 10 magnetic solutions at 10 coil locations
/filn,emag/solu   
antype,harm
harf,,10000             ! excitation at 10 khz
nsel,s,ext
d,all,az,0              ! flux parallel at model edges
nsel,all
CoilLoc=1.15            ! parameter controlling coil location
*do,iii,1,10,1CoilLoc=CoilLoc+.05     ! move coil .05 meters each new solution
bfedel,all,js           ! delete previous curr density load
vsel,s,,,5  
eslv
nsel,s,loc,z,CoilLoc/39.36,(CoilLoc+.1)/39.36   
esln,r,1
bfe,all,js,2,1e8     ! Arbitrary current density input, 1e8
amps/meter**2alls
save
solve   
*enddo
fini

!!! Convert to thermal model and solve for the 10 heat generation cases
/filn,thermal/prep7  
et,1,0           ! make non steel elements null
et,2,70          ! 8 node thermal brick
mp,kxx,2,50  
mp,dens,2,7800
mp,c,2,4
FINISH  

antype,trans
ic,all,temp,70tval=0
*do,jjj,1,10,1ldread,hgen,jjj,1,,,emag,rst  
tval=tval+1      ! use 1 second between solutions, velocity = .05/1
Meters/sec.
time,tval
solve   
*enddo
fini

/exit

battlestar

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