Repatch (from linux) of OSX IRAF

1 files changed, 100 insertions, 0 deletions

diff --git a/math/deboor/difequ_io.f b/math/deboor/difequ_io.f
new file mode 100644
index 00000000..a8bc2709
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+++ b/math/deboor/difequ_io.f
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+      subroutine difequ ( mode, xx, v )
+c  from  * a practical guide to splines *  by c. de boor
+calls  ppvalu(interv)
+c  to be called by   c o l l o c ,  p u t i t
+c  information about the differential equation is dispensed from here
+c
+c******  i n p u t  ******
+c  mode  an integer indicating the task to be performed.
+c	 = 1   initialization
+c	 = 2   evaluate  de  at  xx
+c	 = 3   specify the next side condition
+c	 = 4   analyze the approximation
+c  xx a point at which information is wanted
+c
+c******  o u t p u t  ******
+c  v  depends on the  mode  . see comments below
+c
+c     parameter npiece=100,ncoef=2000
+      integer mode,   i,iside,itermx,k,kpm,l,m
+      real v(20),xx,   break,coef,eps,ep1,ep2,error,factor,rho,solutn
+     *		      ,s2ovep,un,x,xside
+      real ppvalu
+c     common /approx/ break(npiece),coef(ncoef),l,kpm
+      common /approx/ break(100),coef(2000),l,kpm
+      common /side/ m,iside,xside(10)
+      common /other/ itermx,k,rho(19)
+c
+c  this sample of  difequ  is for the example in chapter xv. it is a
+c  nonlinear second order two point boundary value problem.
+c
+					go to (10,20,30,40),mode
+c  initialize everything
+c  i.e. set the order  m  of the dif.equ., the nondecreasing sequence
+c  xside(i),i=1,...,m, of points at which side cond.s are given and
+c  anything else necessary.
+   10 m = 2
+      xside(1) = 0.
+      xside(2) = 1.
+c  *** print out heading
+      print 499
+  499 format(37h carrier,s nonlinear perturb. problem)
+      eps = .5e-2
+      print 610, eps
+  610 format(5h eps ,e20.10)
+c  *** set constants used in formula for solution below.
+      factor = (sqrt(2.) + sqrt(3.))**2
+      s2ovep = sqrt(2./eps)
+c  *** initial guess for newton iteration. un(x) = x*x - 1.
+      l = 1
+      break(1) = 0.
+      do 16 i=1,kpm
+   16	 coef(i) = 0.
+      coef(1) = -1.
+      coef(3) = 2.
+      itermx = 10
+					return
+c
+c  provide value of left side coeff.s and right side at  xx .
+c  specifically, at  xx  the dif.equ. reads
+c	 v(m+1)d**m + v(m)d**(m-1) + ... + v(1)d**0  =	v(m+2)
+c  in terms of the quantities v(i),i=1,...,m+2, to be computed here.
+   20 continue
+      v(3) = eps
+      v(2) = 0.
+      un = ppvalu(break,coef,l,kpm,xx,0)
+      v(1) = 2.*un
+      v(4) = un**2 + 1.
+					return
+c
+c  provide the	m  side conditions. these conditions are of the form
+c	 v(m+1)d**m + v(m)d**(m-1) + ... + v(1)d**0  =	v(m+2)
+c  in terms of the quantities v(i),i=1,...,m+2, to be specified here.
+c  note that v(m+1) = 0  for customary side conditions.
+   30 v(m+1) = 0.
+					go to (31,32,39),iside
+   31 v(2) = 1.
+      v(1) = 0.
+      v(4) = 0.
+					go to 38
+   32 v(2) = 0.
+      v(1) = 1.
+      v(4) = 0.
+   38 iside = iside + 1
+   39					return
+c
+c  calculate the error near the boundary layer at  1.
+   40 continue
+      print 640
+  640 format(44h x, g(x)  and  g(x)-f(x)  at selected points)
+      x = .75
+      do 41 i=1,9
+	 ep1 = exp(s2ovep*(1.-x))*factor
+	 ep2 = exp(s2ovep*(1.+x))*factor
+	 solutn = 12./(1.+ep1)**2*ep1 + 12./(1.+ep2)**2*ep2 - 1.
+	 error = solutn - ppvalu(break,coef,l,kpm,x,0)
+	 print 641,x,solutn,error
+  641	 format(3e20.10)
+   41	 x = x + .03125
+					return
+      end