c c . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . c . . c . copyright (c) 1998 by UCAR . c . . c . University Corporation for Atmospheric Research . c . . c . all rights reserved . c . . c . . c . SPHEREPACK . c . . c . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . c c c c ... file islapgc.f c c this file includes documentation and code for c subroutine islapgc i c c ... files which must be loaded with islapgc.f c c sphcom.f, hrfft.f, shagc.f, shsgc.f c c subroutine islapgc(nlat,nlon,isym,nt,xlmbda,sf,ids,jds,a,b, c +mdab,ndab,wshsgc,lshsgc,work,lwork,pertrb,ierror) c c islapgc inverts the laplace or helmholz operator on a Gaussian c grid using o(n**2) storage. given the c spherical harmonic coefficients a(m,n) and b(m,n) of the right c hand side slap(i,j), islapgc computes a solution sf(i,j) to c the following helmhotz equation : c c 2 2 c [d(sf(i,j))/dlambda /sint + d(sint*d(sf(i,j))/dtheta)/dtheta]/sint c c - xlmbda * sf(i,j) = slap(i,j) c c where sf(i,j) is computed at the Gaussian colatitude point theta(i) c (see nlat as an input argument) and longitude c c lambda(j) = (j-1)*2*pi/nlon c c for i=1,...,nlat and j=1,...,nlon. c c c input parameters c c nlat the number of points in the gaussian colatitude grid on the c full sphere. these lie in the interval (0,pi) and are computed c in radians in theta(1) <...< theta(nlat) by subroutine gaqd. c if nlat is odd the equator will be included as the grid point c theta((nlat+1)/2). if nlat is even the equator will be c excluded as a grid point and will lie half way between c theta(nlat/2) and theta(nlat/2+1). nlat must be at least 3. c note: on the half sphere, the number of grid points in the c colatitudinal direction is nlat/2 if nlat is even or c (nlat+1)/2 if nlat is odd. c c nlon the number of distinct longitude points. nlon determines c the grid increment in longitude as 2*pi/nlon. for example c nlon = 72 for a five degree grid. nlon must be greater c than zero. the axisymmetric case corresponds to nlon=1. c the efficiency of the computation is improved when nlon c is a product of small prime numbers. c c isym this parameter should have the same value input to subroutine c shagc to compute the coefficients a and b for the scalar field c slap. isym is set as follows: c c = 0 no symmetries exist in slap about the equator. scalar c synthesis is used to compute sf on the entire sphere. c i.e., in the array sf(i,j) for i=1,...,nlat and c j=1,...,nlon. c c = 1 sf and slap are antisymmetric about the equator. the c synthesis used to compute sf is performed on the c northern hemisphere only. if nlat is odd, sf(i,j) is c computed for i=1,...,(nlat+1)/2 and j=1,...,nlon. if c nlat is even, sf(i,j) is computed for i=1,...,nlat/2 c and j=1,...,nlon. c c c = 2 sf and slap are symmetric about the equator. the c synthesis used to compute sf is performed on the c northern hemisphere only. if nlat is odd, sf(i,j) is c computed for i=1,...,(nlat+1)/2 and j=1,...,nlon. if c nlat is even, sf(i,j) is computed for i=1,...,nlat/2 c and j=1,...,nlon. c c c nt the number of solutions. in the program that calls islapgc c the arrays sf,a, and b can be three dimensional in which c case multiple solutions are computed. the third index c is the solution index with values k=1,...,nt. c for a single solution set nt=1. the description of the c remaining parameters is simplified by assuming that nt=1 c and sf,a,b are two dimensional. c c xlmbda a one dimensional array with nt elements. if xlmbda is c is identically zero islapgc solves poisson's equation. c if xlmbda > 0.0 islapgc solves the helmholtz equation. c if xlmbda < 0.0 the nonfatal error flag ierror=-1 is c returned. negative xlambda could result in a division c by zero. c c ids the first dimension of the array sf as it appears in the c program that calls islapgc. if isym = 0 then ids must be at c least nlat. if isym > 0 and nlat is even then ids must be c at least nlat/2. if isym > 0 and nlat is odd then ids must c be at least (nlat+1)/2. c c jds the second dimension of the array sf as it appears in the c program that calls islapgc. jds must be at least nlon. c c c a,b two or three dimensional arrays (see input parameter nt) c that contain scalar spherical harmonic coefficients c of the scalar field slap. a,b must be computed by shagc c prior to calling islapgc. c c c mdab the first dimension of the arrays a and b as it appears c in the program that calls islapgc. mdab must be at c least min0(nlat,(nlon+2)/2) if nlon is even or at least c min0(nlat,(nlon+1)/2) if nlon is odd. c c ndab the second dimension of the arrays a and b as it appears c in the program that calls islapgc. ndbc must be at least c least nlat. c c mdab,ndab should have the same values input to shagc to c compute the coefficients a and b. c c wshsgc an array which must be initialized by subroutine shsgci c once initialized, wshsgc can be used repeatedly by islapgc c as long as nlon and nlat remain unchanged. wshsgc must c not be altered between calls of islapgc. c c c lshsgc the dimension of the array wshsgc as it appears in the c program that calls islapgc. let c c l1 = min0(nlat,(nlon+2)/2) if nlon is even or c l1 = min0(nlat,(nlon+1)/2) if nlon is odd c c and c c l2 = nlat/2 if nlat is even or c l2 = (nlat+1)/2 if nlat is odd c c then lshsgc must be at least c c nlat*(2*l2+3*l1-2)+3*l1*(1-l1)/2+nlon+15 c c work a work array that does not have to be saved. c c lwork the dimension of the array work as it appears in the c program that calls islapgc. define c c l2 = nlat/2 if nlat is even or c l2 = (nlat+1)/2 if nlat is odd c l1 = min0(nlat,(nlon+2)/2) if nlon is even or c l1 = min0(nlat,(nlon+1)/2) if nlon is odd c c if isym = 0 let c c lwkmin = nlat*(2*nt*nlon+max0(6*l2,nlon)+2*nt*l1+1). c c if isym > 0 let c c lwkmin = l2*(2*nt*nlon+max0(6*nlat,nlon))+nlat*(2*nt*l1+1) c c c then lwork must be greater than or equal to lwkmin (see ierror=10) c c ************************************************************** c c output parameters c c c sf a two or three dimensional arrays (see input parameter nt) that c inverts the scalar laplacian in slap. sf(i,j) is given at c the colatitude c c theta(i) = (i-1)*pi/(nlat-1) c c and longitude c c lambda(j) = (j-1)*2*pi/nlon c c for i=1,...,nlat and j=1,...,nlon. c c pertrb a one dimensional array with nt elements (see input c parameter nt). in the discription that follows we assume c that nt=1. if xlmbda > 0.0 then pertrb=0.0 is always c returned because the helmholtz operator is invertible. c if xlmbda = 0.0 then a solution exists only if a(1,1) c is zero. islapgc sets a(1,1) to zero. the resulting c solution sf(i,j) solves poisson's equation with c pertrb = a(1,1)/(2.*sqrt(2.)) subtracted from the c right side slap(i,j). c c ierror a parameter which flags errors in input parameters as follows: c c = 0 no errors detected c c = 1 error in the specification of nlat c c = 2 error in the specification of nlon c c = 3 error in the specification of ityp c c = 4 error in the specification of nt c c = 5 error in the specification of ids c c = 6 error in the specification of jds c c = 7 error in the specification of mdbc c c = 8 error in the specification of ndbc c c = 9 error in the specification of lshsgc c c = 10 error in the specification of lwork c c c ********************************************************************** c c end of documentation for islapgc c c ********************************************************************** c