
After go1.16, go will use module mode by default, even when the repository is checked out under GOPATH or in a one-off directory. Add go.mod, go.sum to keep this repo buildable without opting out of the module mode. > go mod init github.com/mmcgrana/gobyexample > go mod tidy > go mod vendor In module mode, the 'vendor' directory is special and its contents will be actively maintained by the go command. pygments aren't the dependency the go will know about, so it will delete the contents from vendor directory. Move it to `third_party` directory now. And, vendor the blackfriday package. Note: the tutorial contents are not affected by the change in go1.16 because all the examples in this tutorial ask users to run the go command with the explicit list of files to be compiled (e.g. `go run hello-world.go` or `go build command-line-arguments.go`). When the source list is provided, the go command does not have to compute the build list and whether it's running in GOPATH mode or module mode becomes irrelevant.
341 lines
11 KiB
Fortran
341 lines
11 KiB
Fortran
SUBROUTINE AHCON (SIZE,N,M,A,B,OLEVR,OLEVI,CLEVR,CLEVI, TRUNCATED
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& SCR1,SCR2,IPVT,JPVT,CON,WORK,ISEED,IERR) !Test inline comment
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C
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C FUNCTION:
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CF
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CF Determines whether the pair (A,B) is controllable and flags
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CF the eigenvalues corresponding to uncontrollable modes.
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CF this ad-hoc controllability calculation uses a random matrix F
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CF and computes whether eigenvalues move from A to the controlled
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CF system A+B*F.
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CF
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C USAGE:
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CU
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CU CALL AHCON (SIZE,N,M,A,B,OLEVR,OLEVI,CLEVR,CLEVI,SCR1,SCR2,IPVT,
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CU JPVT,CON,WORK,ISEED,IERR)
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CU
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CU since AHCON generates different random F matrices for each
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CU call, as long as iseed is not re-initialized by the main
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CU program, and since this code has the potential to be fooled
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CU by extremely ill-conditioned problems, the cautious user
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CU may wish to call it multiple times and rely, perhaps, on
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CU a 2-of-3 vote. We believe, but have not proved, that any
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CU errors this routine may produce are conservative--i.e., that
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CU it may flag a controllable mode as uncontrollable, but
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CU not vice-versa.
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CU
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C INPUTS:
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CI
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CI SIZE integer - first dimension of all 2-d arrays.
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CI
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CI N integer - number of states.
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CI
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CI M integer - number of inputs.
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CI
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CI A double precision - SIZE by N array containing the
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CI N by N system dynamics matrix A.
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CI
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CI B double precision - SIZE by M array containing the
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CI N by M system input matrix B.
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CI
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CI ISEED initial seed for random number generator; if ISEED=0,
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CI then AHCON will set ISEED to a legal value.
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CI
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C OUTPUTS:
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CO
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CO OLEVR double precision - N dimensional vector containing the
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CO real parts of the eigenvalues of A.
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CO
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CO OLEVI double precision - N dimensional vector containing the
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CO imaginary parts of the eigenvalues of A.
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CO
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CO CLEVR double precision - N dimensional vector work space
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CO containing the real parts of the eigenvalues of A+B*F,
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CO where F is the random matrix.
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CO
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CO CLEVI double precision - N dimensional vector work space
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CO containing the imaginary parts of the eigenvalues of
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CO A+B*F, where F is the random matrix.
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CO
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CO SCR1 double precision - N dimensional vector containing the
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CO magnitudes of the corresponding eigenvalues of A.
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CO
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CO SCR2 double precision - N dimensional vector containing the
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CO damping factors of the corresponding eigenvalues of A.
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CO
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CO IPVT integer - N dimensional vector; contains the row pivots
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CO used in finding the nearest neighbor eigenvalues between
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CO those of A and of A+B*F. The IPVT(1)th eigenvalue of
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CO A and the JPVT(1)th eigenvalue of A+B*F are the closest
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CO pair.
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CO
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CO JPVT integer - N dimensional vector; contains the column
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CO pivots used in finding the nearest neighbor eigenvalues;
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CO see IPVT.
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CO
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CO CON logical - N dimensional vector; flagging the uncontrollable
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CO modes of the system. CON(I)=.TRUE. implies the
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CO eigenvalue of A given by DCMPLX(OLEVR(IPVT(I)),OLEVI(IPVT(i)))
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CO corresponds to a controllable mode; CON(I)=.FALSE.
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CO implies an uncontrollable mode for that eigenvalue.
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CO
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CO WORK double precision - SIZE by N dimensional array containing
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CO an N by N matrix. WORK(I,J) is the distance between
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CO the open loop eigenvalue given by DCMPLX(OLEVR(I),OLEVI(I))
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CO and the closed loop eigenvalue of A+B*F given by
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CO DCMPLX(CLEVR(J),CLEVI(J)).
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CO
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CO IERR integer - IERR=0 indicates normal return; a non-zero
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CO value indicates trouble in the eigenvalue calculation.
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CO see the EISPACK and EIGEN documentation for details.
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CO
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C ALGORITHM:
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CA
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CA Calculate eigenvalues of A and of A+B*F for a randomly
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CA generated F, and see which ones change. Use a full pivot
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CA search through a matrix of euclidean distance measures
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CA between each pair of eigenvalues from (A,A+BF) to
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CA determine the closest pairs.
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CA
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C MACHINE DEPENDENCIES:
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CM
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CM NONE
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CM
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C HISTORY:
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CH
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CH written by: Birdwell & Laub
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CH date: May 18, 1985
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CH current version: 1.0
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CH modifications: made machine independent and modified for
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CH f77:bb:8-86.
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CH changed cmplx -> dcmplx: 7/27/88 jdb
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CH
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C ROUTINES CALLED:
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CC
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CC EIGEN,RAND
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CC
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C COMMON MEMORY USED:
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CM
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CM none
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CM
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C----------------------------------------------------------------------
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C written for: The CASCADE Project
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C Oak Ridge National Laboratory
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C U.S. Department of Energy
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C contract number DE-AC05-840R21400
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C subcontract number 37B-7685 S13
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C organization: The University of Tennessee
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C----------------------------------------------------------------------
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C THIS SOFTWARE IS IN THE PUBLIC DOMAIN
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C NO RESTRICTIONS ON ITS USE ARE IMPLIED
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C----------------------------------------------------------------------
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C
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C--global variables:
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C
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INTEGER SIZE
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INTEGER N
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INTEGER M
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INTEGER IPVT(1)
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INTEGER JPVT(1)
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INTEGER IERR
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C
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DOUBLE PRECISION A(SIZE,N)
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DOUBLE PRECISION B(SIZE,M)
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DOUBLE PRECISION WORK(SIZE,N)
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DOUBLE PRECISION CLEVR(N)
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DOUBLE PRECISION CLEVI(N)
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DOUBLE PRECISION OLEVR(N)
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DOUBLE PRECISION OLEVI(N)
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DOUBLE PRECISION SCR1(N)
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DOUBLE PRECISION SCR2(N)
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C
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LOGICAL CON(N)
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C
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C--local variables:
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C
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INTEGER ISEED
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INTEGER ITEMP
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INTEGER K1
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INTEGER K2
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INTEGER I
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INTEGER J
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INTEGER K
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INTEGER IMAX
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INTEGER JMAX
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C
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DOUBLE PRECISION VALUE
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DOUBLE PRECISION EPS
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DOUBLE PRECISION EPS1
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DOUBLE PRECISION TEMP
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DOUBLE PRECISION CURR
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DOUBLE PRECISION ANORM
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DOUBLE PRECISION BNORM
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DOUBLE PRECISION COLNRM
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DOUBLE PRECISION RNDMNO
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C
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DOUBLE COMPLEX DCMPLX
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C
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C--compute machine epsilon
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C
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EPS = 1.D0
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100 CONTINUE
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EPS = EPS / 2.D0
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EPS1 = 1.D0 + EPS
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IF (EPS1 .NE. 1.D0) GO TO 100
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EPS = EPS * 2.D0
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C
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C--compute the l-1 norm of a
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C
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ANORM = 0.0D0
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DO 120 J = 1, N
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COLNRM = 0.D0
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DO 110 I = 1, N
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COLNRM = COLNRM + ABS(A(I,J))
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110 CONTINUE
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IF (COLNRM .GT. ANORM) ANORM = COLNRM
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120 CONTINUE
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C
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C--compute the l-1 norm of b
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C
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BNORM = 0.0D0
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DO 140 J = 1, M
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COLNRM = 0.D0
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DO 130 I = 1, N
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COLNRM = COLNRM + ABS(B(I,J))
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130 CONTINUE
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IF (COLNRM .GT. BNORM) BNORM = COLNRM
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140 CONTINUE
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C
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C--compute a + b * f
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C
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DO 160 J = 1, N
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DO 150 I = 1, N
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WORK(I,J) = A(I,J)
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150 CONTINUE
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160 CONTINUE
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C
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C--the elements of f are random with uniform distribution
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C--from -anorm/bnorm to +anorm/bnorm
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C--note that f is not explicitly stored as a matrix
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C--pathalogical floating point notes: the if (bnorm .gt. 0.d0)
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C--test should actually be if (bnorm .gt. dsmall), where dsmall
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C--is the smallest representable number whose reciprocal does
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C--not generate an overflow or loss of precision.
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C
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IF (ISEED .EQ. 0) ISEED = 86345823
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IF (ANORM .EQ. 0.D0) ANORM = 1.D0
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IF (BNORM .GT. 0.D0) THEN
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TEMP = 2.D0 * ANORM / BNORM
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ELSE
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TEMP = 2.D0
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END IF
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DO 190 K = 1, M
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DO 180 J = 1, N
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CALL RAND(ISEED,ISEED,RNDMNO)
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VALUE = (RNDMNO - 0.5D0) * TEMP
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DO 170 I = 1, N
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WORK(I,J) = WORK(I,J) + B(I,K)*VALUE
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170 CONTINUE
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180 CONTINUE
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190 CONTINUE
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C
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C--compute the eigenvalues of a + b*f, and several other things
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C
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CALL EIGEN (0,SIZE,N,WORK,CLEVR,CLEVI,WORK,SCR1,SCR2,IERR)
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IF (IERR .NE. 0) RETURN
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C
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C--copy a so it is not destroyed
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C
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DO 210 J = 1, N
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DO 200 I = 1, N
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WORK(I,J) = A(I,J)
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200 CONTINUE
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210 CONTINUE
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C
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C--compute the eigenvalues of a, and several other things
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C
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CALL EIGEN (0,SIZE,N,WORK,OLEVR,OLEVI,WORK,SCR1,SCR2,IERR)
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IF (IERR .NE. 0) RETURN
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C
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C--form the matrix of distances between eigenvalues of a and
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C--EIGENVALUES OF A+B*F
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C
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DO 230 J = 1, N
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DO 220 I = 1, N
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WORK(I,J) =
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& ABS(DCMPLX(OLEVR(I),OLEVI(I))-DCMPLX(CLEVR(J),CLEVI(J)))
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220 CONTINUE
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230 CONTINUE
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C
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C--initialize row and column pivots
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C
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DO 240 I = 1, N
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IPVT(I) = I
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JPVT(I) = I
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240 CONTINUE
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C
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C--a little bit messy to avoid swapping columns and
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C--rows of work
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C
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DO 270 I = 1, N-1
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C
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C--find the minimum element of each lower right square
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C--submatrix of work, for submatrices of size n x n
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C--through 2 x 2
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C
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CURR = WORK(IPVT(I),JPVT(I))
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IMAX = I
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JMAX = I
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TEMP = CURR
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C
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C--find the minimum element
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C
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DO 260 K1 = I, N
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DO 250 K2 = I, N
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IF (WORK(IPVT(K1),JPVT(K2)) .LT. TEMP) THEN
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TEMP = WORK(IPVT(K1),JPVT(K2))
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IMAX = K1
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JMAX = K2
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END IF
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250 CONTINUE
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260 CONTINUE
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C
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C--update row and column pivots for indirect addressing of work
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C
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ITEMP = IPVT(I)
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IPVT(I) = IPVT(IMAX)
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IPVT(IMAX) = ITEMP
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C
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ITEMP = JPVT(I)
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JPVT(I) = JPVT(JMAX)
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JPVT(JMAX) = ITEMP
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C
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C--do next submatrix
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C
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270 CONTINUE
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C
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C--this threshold for determining when an eigenvalue has
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C--not moved, and is therefore uncontrollable, is critical,
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C--and may require future changes with more experience.
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C
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EPS1 = SQRT(EPS)
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C
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C--for each eigenvalue pair, decide if it is controllable
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C
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DO 280 I = 1, N
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C
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C--note that we are working with the "pivoted" work matrix
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C--and are looking at its diagonal elements
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C
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IF (WORK(IPVT(I),JPVT(I))/ANORM .LE. EPS1) THEN
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CON(I) = .FALSE.
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ELSE
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CON(I) = .TRUE.
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END IF
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280 CONTINUE
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C
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C--finally!
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C
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RETURN
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END
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