Permanent-Magnet Dipole for MiniBoone Original version from the 1987 User's Guide, Chapter 10.5 08-30-01 simple dipole 08-30-01 double pole bricks single side bricks 09-04-01 side bricks at bottom of gap 09-04-01 try 2" side bricks make pole smaller 09-04-01 make gap 0.8 inches high 09-07-01 put in ND-Iron form Hitachi ; Copyright 1998, by the University of California. ; Unauthorized commercial use is prohibited. ® kprob=0, ; Defines a POISSON or PANDIRA problem xreg = -10.0, -7.0, -1.0, 1.0, 7.0, xmax = 10.0, kreg = 0, 4, 17, 26, 39, kmax = 43, yreg = -10.0, -7.0, -0.4, 0.4, 7.0, ymax = 10.0, lreg = 0, 4, 20, 30, 46, lmax = 50, conv = 2.54, ; inches nbslo = 0, ; Dirchelt boundary condtion at bottom xmin=-10.0,xmax=10.0, ; Limits of X coordinates ymin=-10.0,ymax=10.0, ; Limits of Y coordinates kmin = 17 ,ktop = 26, ; limits on where to calculate fields for outpan lmin = 17 ,ltop = 26, ; limits on where to calculate fields for outpan ktype = 2, ; symmetry midplane for this nterm = 11, ; number of harmonics terms nptc = 1440, ; number of arc points rint = 0.35, ; radius to calculate harmonics angle = 360.0, ; angle to calculate harmonics mode=0 & ; Materials have variable permeability &po x=-10.0,y=-10.0 & ;entire universe &po x= 10.0,y=-10.0 & &po x= 10.0,y= 10.0 & &po x=-10.0,y= 10.0 & &po x=-10.0,y=-10.0 & ® mat=2 & ; top flux return &po x= -4.75, y= 3.50 & &po x= 4.75, y= 3.50 & &po x= 4.75, y= 4.50 & &po x= -4.75, y= 4.50 & &po x= -4.75, y= 3.50 & ® mat=2 & ; bottom flux return &po x= -4.75, y= -3.50 & &po x= 4.75, y= -3.50 & &po x= 4.75, y= -4.50 & &po x= -4.75, y= -4.50 & &po x= -4.75, y= -3.50 & ® mat=2 & ; RHS flux return &po x= 3.75, y= -3.50 & &po x= 4.75, y= -3.50 & &po x= 4.75, y= 3.50 & &po x= 3.75, y= 3.50 & &po x= 3.75, y= -3.50 & ® mat=2 & ; LHS flux return &po x= -3.75, y= -3.50 & &po x= -4.75, y= -3.50 & &po x= -4.75, y= 3.50 & &po x= -3.75, y= 3.50 & &po x= -3.75, y= -3.50 & ® mat=2 & ; top pole &po x=-3.25, y= 0.40 & &po x= 3.25, y= 0.40 & &po x= 3.25, y= 3.00 & &po x=-3.25, y= 3.00 & &po x=-3.25, y= 0.40 & ® mat=2 & ; bottom pole &po x=-3.25, y= -0.40 & &po x= 3.25, y= -0.40 & &po x= 3.25, y= -3.00 & &po x=-3.25, y= -3.00 & &po x=-3.25, y= -0.40 & ® mat=7,mshape=1,mtid=2 & ;Top Brick field pointing up &po x=-1.00,y= 3.00 & &po x= 1.00,y= 3.00 & &po x= 1.00,y= 3.50 & &po x=-1.00,y= 3.50 & &po x=-1.00,y= 3.00 & ® mat=7,mshape=1,mtid=2 & ;bottom Brick field pointing up &po x=-1.00,y= -3.00 & &po x= 1.00,y= -3.00 & &po x= 1.00,y= -3.50 & &po x=-1.00,y= -3.50 & &po x=-1.00,y= -3.00 & ® mat=8,mshape=1,mtid=4 & ; RHS Upper bricks &po x = 3.25, y = 0.50 & &po x = 3.75, y = 0.50 & &po x = 3.75, y = 2.50 & &po x = 3.25, y = 2.50 & &po x = 3.25, y = 0.50 & ® mat=9,mshape=1,mtid=6 & ; LHS Upper bricks &po x = -3.25, y = 0.50 & &po x = -3.75, y = 0.50 & &po x = -3.75, y = 2.50 & &po x = -3.25, y = 2.50 & &po x = -3.25, y = 0.50 & ® mat=9,mshape=1,mtid=4 & ; RHS Lower bricks &po x = 3.25, y = -0.50 & &po x = 3.75, y = -0.50 & &po x = 3.75, y = -2.50 & &po x = 3.25, y = -2.50 & &po x = 3.25, y = -0.50 & ® mat=8,mshape=1,mtid=6 & ; LHS Lower bricks &po x = -3.25, y = -0.50 & &po x = -3.75, y = -0.50 & &po x = -3.75, y = -2.50 & &po x = -3.25, y = -2.50 & &po x = -3.25, y = -0.50 & ;;;:::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::: &mt mtid=1,aeasy=90,gamper=1 ; Material ID, Easy axis direction, Gamma along hard axis hcept=-3500,bcept=3800. & ; H and B intercepts ;&mt mtid=2,aeasy= 90,gamper=1,hcept=-3115,bcept=3382. & ; Sr Ferrite comp ;&mt mtid=4,aeasy=180,gamper=1,hcept=-3115,bcept=3382. & ; Sr Ferrite comp ;&mt mtid=6,aeasy= 0,gamper=1,hcept=-3115,bcept=3382. & ; Sr Ferrite comp ;&mt mtid=8,aeasy=270,gamper=1,hcept=-3115,bcept=3382. & ; Sr Ferrite comp &mt mtid=2,aeasy= 90,gamper=1,hcept=-10940,bcept=11570. & ; ND Iron no comp &mt mtid=4,aeasy=180,gamper=1,hcept=-10940,bcept=11570. & ; ND Iron no comp &mt mtid=6,aeasy= 0,gamper=1,hcept=-10940,bcept=11570. & ; ND Iron no comp &mt mtid=8,aeasy=270,gamper=1,hcept=-10940,bcept=11570. & ; ND Iron no comp