rsspice 0.1.0

Pure Rust port of the SPICE Toolkit for space geometry
Documentation
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//
// GENERATED FILE
//

use super::*;
use crate::SpiceContext;
use f2rust_std::*;

const CNVTOL: f64 = 0.000001;
const NWMAX: i32 = 15;
const NWDIST: i32 = 5;
const NWSEP: i32 = 5;
const NWRR: i32 = 5;
const NWUDS: i32 = 5;
const NWPA: i32 = 5;
const NWILUM: i32 = 5;
const ADDWIN: f64 = 0.5;
const FRMNLN: i32 = 32;
const FOVTLN: i32 = 40;
const FTCIRC: &[u8] = b"CIRCLE";
const FTELLI: &[u8] = b"ELLIPSE";
const FTPOLY: &[u8] = b"POLYGON";
const FTRECT: &[u8] = b"RECTANGLE";
const ANNULR: &[u8] = b"ANNULAR";
const ANY: &[u8] = b"ANY";
const PARTL: &[u8] = b"PARTIAL";
const FULL: &[u8] = b"FULL";
const DSSHAP: &[u8] = b"DSK";
const EDSHAP: &[u8] = b"ELLIPSOID";
const PTSHAP: &[u8] = b"POINT";
const RYSHAP: &[u8] = b"RAY";
const SPSHAP: &[u8] = b"SPHERE";
const NOCTYP: i32 = 4;
const OCLLN: i32 = 7;
const SHPLEN: i32 = 9;
const MAXVRT: i32 = 10000;
const CIRFOV: &[u8] = b"CIRCLE";
const ELLFOV: &[u8] = b"ELLIPSE";
const POLFOV: &[u8] = b"POLYGON";
const RECFOV: &[u8] = b"RECTANGLE";
const ZZGET: i32 = -1;
const ZZPUT: i32 = -2;
const ZZRESET: i32 = -3;
const ZZNOP: i32 = 3;
const GEN: i32 = 1;
const GF_REF: i32 = 2;
const GF_TOL: i32 = 3;
const GF_DT: i32 = 4;
const NID: i32 = 4;
const LBCELL: i32 = -5;
const LNSIZE: i32 = 80;
const QNPARS: i32 = 3;
const NOBAIL: bool = false;
const NORPT: bool = false;

/// GF, distance search
///
/// Determine time intervals over which a specified constraint on
/// observer-target distance is met.
///
/// # Required Reading
///
/// * [GF](crate::required_reading::gf)
/// * [NAIF_IDS](crate::required_reading::naif_ids)
/// * [SPK](crate::required_reading::spk)
/// * [TIME](crate::required_reading::time)
/// * [WINDOWS](crate::required_reading::windows)
///
/// # Brief I/O
///
/// ```text
///  VARIABLE  I/O  DESCRIPTION
///  --------  ---  --------------------------------------------------
///  LBCELL     P   SPICE Cell lower bound.
///  CNVTOL     P   Convergence tolerance.
///  NWDIST     P   Number of workspace windows for distance search.
///  TARGET     I   Name of the target body.
///  ABCORR     I   Aberration correction flag.
///  OBSRVR     I   Name of the observing body.
///  RELATE     I   Relational operator.
///  REFVAL     I   Reference value.
///  ADJUST     I   Adjustment value for absolute extrema searches.
///  STEP       I   Step size used for locating extrema and roots.
///  CNFINE     I   SPICE window to which the search is confined.
///  MW         I   Workspace window size.
///  NW         I   Workspace window count.
///  WORK       O   Array of workspace windows.
///  RESULT    I-O  SPICE window containing results.
/// ```
///
/// # Detailed Input
///
/// ```text
///  TARGET   is the name of a target body. Optionally, you may supply
///           the integer ID code for the object as an integer string.
///           For example both 'MOON' and '301' are legitimate strings
///           that indicate the Moon is the target body.
///
///           The target and observer define a position vector which
///           points from the observer to the target; the length of
///           this vector is the "distance" that serves as the subject
///           of the search performed by this routine.
///
///           Case and leading or trailing blanks are not significant
///           in the string TARGET.
///
///  ABCORR   indicates the aberration corrections to be applied to the
///           observer-target position vector to account for one-way
///           light time and stellar aberration.
///
///           Any aberration correction accepted by the SPICE routine
///           SPKEZR is accepted here. See the header of SPKEZR for a
///           detailed description of the aberration correction
///           options. For convenience, the options are listed below:
///
///              'NONE'     Apply no correction.
///
///              'LT'       "Reception" case: correct for
///                         one-way light time using a Newtonian
///                         formulation.
///
///              'LT+S'     "Reception" case: correct for
///                         one-way light time and stellar
///                         aberration using a Newtonian
///                         formulation.
///
///              'CN'       "Reception" case: converged
///                         Newtonian light time correction.
///
///              'CN+S'     "Reception" case: converged
///                         Newtonian light time and stellar
///                         aberration corrections.
///
///              'XLT'      "Transmission" case: correct for
///                         one-way light time using a Newtonian
///                         formulation.
///
///              'XLT+S'    "Transmission" case: correct for
///                         one-way light time and stellar
///                         aberration using a Newtonian
///                         formulation.
///
///              'XCN'      "Transmission" case: converged
///                         Newtonian light time correction.
///
///              'XCN+S'    "Transmission" case: converged
///                         Newtonian light time and stellar
///                         aberration corrections.
///
///           Case and leading or trailing blanks are not significant
///           in the string ABCORR.
///
///  OBSRVR   is the name of an observing body. Optionally, you may
///           supply the ID code of the object as an integer string.
///           For example, both 'EARTH' and '399' are legitimate
///           strings to supply to indicate the observer is Earth.
///
///           Case and leading or trailing blanks are not significant
///           in the string OBSRVR.
///
///  RELATE   is a relational operator used to define a constraint on
///           the observer-target distance. The result window found by
///           this routine indicates the time intervals where the
///           constraint is satisfied.
///
///           Supported values of RELATE and corresponding meanings are
///           shown below:
///
///              '>'        Distance is greater than the reference
///                         value REFVAL.
///
///              '='        Distance is equal to the reference
///                         value REFVAL.
///
///              '<'        Distance is less than the reference
///                         value REFVAL.
///
///              'ABSMAX'   Distance is at an absolute maximum.
///
///              'ABSMIN'   Distance is at an absolute  minimum.
///
///              'LOCMAX'   Distance is at a local maximum.
///
///              'LOCMIN'   Distance is at a local minimum.
///
///           The caller may indicate that the region of interest is
///           the set of time intervals where the distance is within a
///           specified offset relative to an absolute extremum. The
///           argument ADJUST (described below) is used to specify this
///           offset.
///
///           Local extrema are considered to exist only in the
///           interiors of the intervals comprising the confinement
///           window:  a local extremum cannot exist at a boundary
///           point of the confinement window.
///
///           Case and leading or trailing blanks are not significant
///           in the string RELATE.
///
///  REFVAL   is the reference value used together with the argument
///           RELATE to define an equality or inequality to be
///           satisfied by the distance between the specified target
///           and observer. See the discussion of RELATE above for
///           further information.
///
///           The units of REFVAL are km.
///
///  ADJUST   is a parameter used to modify searches for absolute
///           extrema: when RELATE is set to 'ABSMAX' or 'ABSMIN' and
///           ADJUST is set to a positive value, GFDIST will find times
///           when the observer-target distance is within ADJUST km of
///           the specified extreme value.
///
///           If ADJUST is non-zero and a search for an absolute
///           minimum AMIN is performed, the result window contains
///           time intervals when the observer-target distance has
///           values between AMIN and AMIN + ADJUST.
///
///           If the search is for an absolute maximum AMAX, the
///           corresponding range is  between AMAX - ADJUST and AMAX.
///
///           ADJUST is not used for searches for local extrema,
///           equality or inequality conditions.
///
///  STEP     is the step size to be used in the search. STEP must be
///           shorter than any maximal time interval on which the
///           specified distance function is monotone increasing or
///           decreasing. That is, if the confinement window is
///           partitioned into alternating intervals on which the
///           distance function is either monotone increasing or
///           decreasing, STEP must be shorter than any of these
///           intervals.
///
///           However, STEP must not be *too* short, or the search will
///           take an unreasonable amount of time.
///
///           The choice of STEP affects the completeness but not the
///           precision of solutions found by this routine; the
///           precision is controlled by the convergence tolerance. See
///           the discussion of the parameter CNVTOL for details.
///
///           STEP has units of TDB seconds.
///
///  CNFINE   is a SPICE window that confines the time period over
///           which the specified search is conducted. CNFINE may
///           consist of a single interval or a collection of
///           intervals.
///
///           The endpoints of the time intervals comprising CNFINE are
///           interpreted as seconds past J2000 TDB.
///
///           See the $Examples section below for a code example that
///           shows how to create a confinement window.
///
///           CNFINE must be initialized by the caller via the SPICELIB
///           routine SSIZED.
///
///           In some cases the observer's state may be computed at
///           times outside of CNFINE by as much as 2 seconds. See
///           $Particulars for details.
///
///  MW       is a parameter specifying the length of the SPICE windows
///           in the workspace array WORK (see description below) used
///           by this routine.
///
///           MW should be set to a number at least twice as large as
///           the maximum number of intervals required by any workspace
///           window. In many cases, it's not necessary to compute an
///           accurate estimate of how many intervals are needed;
///           rather, the user can pick a size considerably larger than
///           what's really required.
///
///           However, since excessively large arrays can prevent
///           applications from compiling, linking, or running
///           properly, sometimes MW must be set according to the
///           actual workspace requirement. A rule of thumb for the
///           number of intervals NINTVLS needed is
///
///              NINTVLS  =  2*N  +  ( M / STEP )
///
///           where
///
///              N     is the number of intervals in the confinement
///                    window
///
///              M     is the measure of the confinement window, in
///                    units of seconds
///
///              STEP  is the search step size in seconds
///
///           MW should then be set to
///
///              2 * NINTVLS
///
///  NW       is a parameter specifying the number of SPICE windows in
///           the workspace array WORK (see description below) used by
///           this routine. NW should be set to the parameter NWDIST;
///           this parameter is declared in the include file gf.inc.
///           (The reason this dimension is an input argument is that
///           this allows run-time error checking to be performed.)
///
///  RESULT   is a double precision SPICE window which will contain
///           the search results. RESULT must be declared and
///           initialized with sufficient size to capture the full
///           set of time intervals within the search region on which
///           the specified condition is satisfied.
///
///           RESULT must be initialized by the caller via the
///           SPICELIB routine SSIZED.
///
///           If RESULT is non-empty on input, its contents will be
///           discarded before GFDIST conducts its search.
/// ```
///
/// # Detailed Output
///
/// ```text
///  WORK     is an array used to store workspace windows.
///
///           This array should be declared by the caller as shown:
///
///              INCLUDE 'gf.inc'
///                 ...
///
///              DOUBLE PRECISION    WORK ( LBCELL : MW, NWDIST )
///
///           where MW is a constant declared by the caller and NWDIST
///           is a constant defined in the SPICELIB INCLUDE file
///           gf.inc. See the discussion of MW above.
///
///           WORK need not be initialized by the caller.
///
///           WORK is modified by this routine. The caller should
///           re-initialize this array before attempting to use it for
///           any other purpose.
///
///  RESULT   is the SPICE window of intervals, contained within the
///           confinement window CNFINE, on which the specified
///           distance constraint is satisfied.
///
///           The endpoints of the time intervals comprising RESULT
///           are interpreted as seconds past J2000 TDB.
///
///           If the search is for local extrema, or for absolute
///           extrema with ADJUST set to zero, then normally each
///           interval of RESULT will be a singleton: the left and
///           right endpoints of each interval will be identical.
///
///           If no times within the confinement window satisfy the
///           search criteria, RESULT will be returned with a
///           cardinality of zero.
/// ```
///
/// # Parameters
///
/// ```text
///  LBCELL   is the lower bound for SPICE Cell arrays.
///
///  CNVTOL   is the convergence tolerance used for finding
///           endpoints of the intervals comprising the result
///           window. CNVTOL is also used for finding intermediate
///           results; in particular, CNVTOL is used for finding the
///           windows on which the specified distance is increasing
///           or decreasing. CNVTOL is used to determine when binary
///           searches for roots should terminate: when a root is
///           bracketed within an interval of length CNVTOL; the
///           root is considered to have been found.
///
///           The accuracy, as opposed to precision, of roots found
///           by this routine depends on the accuracy of the input
///           data. In most cases, the accuracy of solutions will be
///           inferior to their precision.
///
///  NWDIST   is the number of workspace windows required by
///           this routine.
///
///  See INCLUDE file gf.inc for declarations and descriptions of
///  parameters used throughout the GF system.
/// ```
///
/// # Exceptions
///
/// ```text
///  1)  In order for this routine to produce correct results,
///      the step size must be appropriate for the problem at hand.
///      Step sizes that are too large may cause this routine to miss
///      roots; step sizes that are too small may cause this routine
///      to run unacceptably slowly and in some cases, find spurious
///      roots.
///
///      This routine does not diagnose invalid step sizes, except that
///      if the step size is non-positive, an error is signaled by a
///      routine in the call tree of this routine.
///
///  2)  Due to numerical errors, in particular,
///
///         - Truncation error in time values
///         - Finite tolerance value
///         - Errors in computed geometric quantities
///
///      it is *normal* for the condition of interest to not always be
///      satisfied near the endpoints of the intervals comprising the
///      result window.
///
///      The result window may need to be contracted slightly by the
///      caller to achieve desired results. The SPICE window routine
///      WNCOND can be used to contract the result window.
///
///  3)  If an error (typically cell overflow) occurs while performing
///      window arithmetic, the error is signaled by a routine
///      in the call tree of this routine.
///
///  4)  If the relational operator RELATE is not recognized, an
///      error is signaled by a routine in the call tree of this
///      routine.
///
///  5)  If the aberration correction specifier contains an
///      unrecognized value, an error is signaled by a routine in the
///      call tree of this routine.
///
///  6)  If ADJUST is negative, an error is signaled by a routine in
///      the call tree of this routine.
///
///  7)  If either of the input body names do not map to NAIF ID
///      codes, an error is signaled by a routine in the call tree of
///      this routine.
///
///  8)  If required ephemerides or other kernel data are not
///      available, an error is signaled by a routine in the call tree
///      of this routine.
///
///  9)  If the window size MW is less than 2, the error
///      SPICE(INVALIDDIMENSION) is signaled.
///
///  10) If the window count NW is less than NWDIST, the error
///      SPICE(INVALIDDIMENSION) is signaled.
///
///  11) If the result window has size less than 2, the error
///      SPICE(INVALIDDIMENSION) is signaled.
///
///  12) If the output SPICE window RESULT has insufficient capacity
///      to contain the number of intervals on which the specified
///      distance condition is met, an error is signaled
///      by a routine in the call tree of this routine.
/// ```
///
/// # Files
///
/// ```text
///  Appropriate kernels must be loaded by the calling program before
///  this routine is called.
///
///  The following data are required:
///
///  -  SPK data: ephemeris data for target and observer for the
///     time period defined by the confinement window must be
///     loaded. If aberration corrections are used, the states of
///     target and observer relative to the solar system barycenter
///     must be calculable from the available ephemeris data.
///     Typically ephemeris data are made available by loading one
///     or more SPK files via FURNSH.
///
///  -  If non-inertial reference frames are used, then PCK
///     files, frame kernels, C-kernels, and SCLK kernels may be
///     needed.
///
///  -  In some cases the observer's state may be computed at times
///     outside of CNFINE by as much as 2 seconds; data required to
///     compute this state must be provided by loaded kernels. See
///     $Particulars for details.
///
///  Kernel data are normally loaded once per program run, NOT every
///  time this routine is called.
/// ```
///
/// # Particulars
///
/// ```text
///  This routine determines a set of one or more time intervals
///  within the confinement window when the distance between the
///  specified target and observer satisfies a caller-specified
///  constraint. The resulting set of intervals is returned as a SPICE
///  window.
///
///  Below we discuss in greater detail aspects of this routine's
///  solution process that are relevant to correct and efficient
///  use of this routine in user applications.
///
///
///  The Search Process
///  ==================
///
///  Regardless of the type of constraint selected by the caller, this
///  routine starts the search for solutions by determining the time
///  periods, within the confinement window, over which the
///  distance function is monotone increasing and monotone
///  decreasing. Each of these time periods is represented by a SPICE
///  window. Having found these windows, all of the range rate
///  function's local extrema within the confinement window are known.
///  Absolute extrema then can be found very easily.
///
///  Within any interval of these "monotone" windows, there will be at
///  most one solution of any equality constraint. Since the boundary
///  of the solution set for any inequality constraint is contained in
///  the union of
///
///  -  the set of points where an equality constraint is met
///
///  -  the boundary points of the confinement window
///
///  the solutions of both equality and inequality constraints can be
///  found easily once the monotone windows have been found.
///
///
///  Step Size
///  =========
///
///  The monotone windows (described above) are found via a two-step
///  search process. Each interval of the confinement window is
///  searched as follows: first, the input step size is the time
///  separation at which the sign of the rate of change of distance
///  ("range rate") is sampled. Starting at the left endpoint of the
///  interval, samples will be taken at each step. If a change of sign
///  is found, a root has been bracketed; at that point, the time at
///  which the range rate is zero can be found by a refinement
///  process, for example, via binary search.
///
///  Note that the optimal choice of step size depends on the lengths
///  of the intervals over which the distance function is monotone:
///  the step size should be shorter than the shortest of these
///  intervals (within the confinement window).
///
///  The optimal step size is *not* necessarily related to the lengths
///  of the intervals comprising the result window. For example, if
///  the shortest monotone interval has length 10 days, and if the
///  shortest result window interval has length 5 minutes, a step size
///  of 9.9 days is still adequate to find all of the intervals in the
///  result window. In situations like this, the technique of using
///  monotone windows yields a dramatic efficiency improvement over a
///  state-based search that simply tests at each step whether the
///  specified constraint is satisfied. The latter type of search can
///  miss solution intervals if the step size is longer than the
///  shortest solution interval.
///
///  Having some knowledge of the relative geometry of the target and
///  observer can be a valuable aid in picking a reasonable step size.
///  In general, the user can compensate for lack of such knowledge by
///  picking a very short step size; the cost is increased computation
///  time.
///
///  Note that the step size is not related to the precision with which
///  the endpoints of the intervals of the result window are computed.
///  That precision level is controlled by the convergence tolerance.
///
///
///  Convergence Tolerance
///  =====================
///
///  As described above, the root-finding process used by this routine
///  involves first bracketing roots and then using a search process
///  to locate them. "Roots" include times when extrema are attained
///  and times when the distance function is equal to a reference
///  value or adjusted extremum. All endpoints of the intervals
///  comprising the result window are either endpoints of intervals of
///  the confinement window or roots.
///
///  Once a root has been bracketed, a refinement process is used to
///  narrow down the time interval within which the root must lie.
///  This refinement process terminates when the location of the root
///  has been determined to within an error margin called the
///  "convergence tolerance." The default convergence tolerance
///  used by this routine is set by the parameter CNVTOL (defined
///  in gf.inc).
///
///  The value of CNVTOL is set to a "tight" value so that the
///  tolerance doesn't become the limiting factor in the accuracy of
///  solutions found by this routine. In general the accuracy of input
///  data will be the limiting factor.
///
///  The user may change the convergence tolerance from the default
///  CNVTOL value by calling the routine GFSTOL, e.g.
///
///     CALL GFSTOL( tolerance value )
///
///  Call GFSTOL prior to calling this routine. All subsequent
///  searches will use the updated tolerance value.
///
///  Setting the tolerance tighter than CNVTOL is unlikely to be
///  useful, since the results are unlikely to be more accurate.
///  Making the tolerance looser will speed up searches somewhat,
///  since a few convergence steps will be omitted. However, in most
///  cases, the step size is likely to have a much greater effect
///  on processing time than would the convergence tolerance.
///
///
///  The Confinement Window
///  ======================
///
///  The simplest use of the confinement window is to specify a time
///  interval within which a solution is sought. However, the
///  confinement window can, in some cases, be used to make searches
///  more efficient. Sometimes it's possible to do an efficient search
///  to reduce the size of the time period over which a relatively
///  slow search of interest must be performed. See the "CASCADE"
///  example program in gf.req for a demonstration.
///
///  Certain types of searches require the state of the observer,
///  relative to the solar system barycenter, to be computed at times
///  slightly outside the confinement window CNFINE. The time window
///  that is actually used is the result of "expanding" CNFINE by a
///  specified amount "T": each time interval of CNFINE is expanded by
///  shifting the interval's left endpoint to the left and the right
///  endpoint to the right by T seconds. Any overlapping intervals are
///  merged. (The input argument CNFINE is not modified.)
///
///  The window expansions listed below are additive: if both
///  conditions apply, the window expansion amount is the sum of the
///  individual amounts.
///
///  -  If a search uses an equality constraint, the time window
///     over which the state of the observer is computed is expanded
///     by 1 second at both ends of all of the time intervals
///     comprising the window over which the search is conducted.
///
///  -  If a search uses stellar aberration corrections, the time
///     window over which the state of the observer is computed is
///     expanded as described above.
///
///  When light time corrections are used, expansion of the search
///  window also affects the set of times at which the light time-
///  corrected state of the target is computed.
///
///  In addition to the possible 2 second expansion of the search
///  window that occurs when both an equality constraint and stellar
///  aberration corrections are used, round-off error should be taken
///  into account when the need for data availability is analyzed.
/// ```
///
/// # Examples
///
/// ```text
///  The numerical results shown for these examples may differ across
///  platforms. The results depend on the SPICE kernels used as
///  input, the compiler and supporting libraries, and the machine
///  specific arithmetic implementation.
///
///
///  1) Find times during the first three months of the year 2007 when
///     the geometric Earth-Moon distance is greater than 400000 km.
///     Display the start and stop times of the time intervals over
///     which this constraint is met, along with the Earth-Moon
///     distance at each interval endpoint.
///
///     We expect the Earth-Moon distance to be an oscillatory
///     function with extrema roughly two weeks apart. Using
///     a step size of one day guarantees that the GF system
///     won't fail to find any distance extrema. (Recall that a
///     search for distance extrema is an intermediate step
///     in the GF search process.)
///
///     Use the meta-kernel shown below to load the required SPICE
///     kernels.
///
///
///        KPL/MK
///
///        File name: gfdist_ex1.tm
///
///        This meta-kernel is intended to support operation of SPICE
///        example programs. The kernels shown here should not be
///        assumed to contain adequate or correct versions of data
///        required by SPICE-based user applications.
///
///        In order for an application to use this meta-kernel, the
///        kernels referenced here must be present in the user's
///        current working directory.
///
///        The names and contents of the kernels referenced
///        by this meta-kernel are as follows:
///
///           File name                     Contents
///           ---------                     --------
///           de421.bsp                     Planetary ephemeris
///           pck00008.tpc                  Planet orientation and
///                                         radii
///           naif0009.tls                  Leapseconds
///
///
///        \begindata
///
///           KERNELS_TO_LOAD = ( 'de421.bsp',
///                               'pck00008.tpc',
///                               'naif0009.tls'  )
///
///        \begintext
///
///        End of meta-kernel
///
///
///     Example code begins here.
///
///
///           PROGRAM GFDIST_EX1
///           IMPLICIT NONE
///
///     C
///     C     Include GF parameter declarations:
///     C
///           INCLUDE 'gf.inc'
///
///     C
///     C     SPICELIB functions
///     C
///           DOUBLE PRECISION      SPD
///           DOUBLE PRECISION      VNORM
///           INTEGER               WNCARD
///
///     C
///     C     Local parameters
///     C
///           INTEGER               LBCELL
///           PARAMETER           ( LBCELL = -5 )
///
///     C
///     C     Use the parameter MAXWIN for both
///     C     the result window size and the workspace
///     C     size.
///     C
///           INTEGER               MAXWIN
///           PARAMETER           ( MAXWIN = 20000 )
///
///     C
///     C     Length of output time string:
///     C
///           INTEGER               TIMLEN
///           PARAMETER           ( TIMLEN = 26 )
///
///     C
///     C     Local variables
///     C
///           CHARACTER*(TIMLEN)    TIMSTR
///
///           DOUBLE PRECISION      ADJUST
///           DOUBLE PRECISION      CNFINE ( LBCELL : 2 )
///           DOUBLE PRECISION      DIST
///           DOUBLE PRECISION      ET0
///           DOUBLE PRECISION      ET1
///           DOUBLE PRECISION      FINISH
///           DOUBLE PRECISION      LT
///           DOUBLE PRECISION      POS    ( 3 )
///           DOUBLE PRECISION      REFVAL
///           DOUBLE PRECISION      RESULT ( LBCELL : MAXWIN )
///           DOUBLE PRECISION      START
///           DOUBLE PRECISION      STEP
///           DOUBLE PRECISION      WORK   ( LBCELL : MAXWIN, NWDIST )
///
///           INTEGER               I
///
///     C
///     C     Saved variables
///     C
///     C     The confinement, workspace and result windows CNFINE,
///     C     WORK and RESULT are saved because this practice helps to
///     C     prevent stack overflow.
///     C
///           SAVE                  CNFINE
///           SAVE                  RESULT
///           SAVE                  WORK
///
///     C
///     C     Load kernels.
///     C
///           CALL FURNSH ( 'gfdist_ex1.tm' )
///
///     C
///     C     Initialize windows.
///     C
///           CALL SSIZED ( MAXWIN, RESULT )
///           CALL SSIZED ( 2,      CNFINE )
///
///     C
///     C     Store the time bounds of our search interval in
///     C     the confinement window.
///     C
///           CALL STR2ET ( '2007 JAN 1', ET0 )
///           CALL STR2ET ( '2007 APR 1', ET1 )
///
///           CALL WNINSD ( ET0, ET1, CNFINE )
///
///     C
///     C     Search using a step size of 1 day (in units of
///     C     seconds). The reference value is 450000 km.
///     C     We're not using the adjustment feature, so
///     C     we set ADJUST to zero.
///     C
///           STEP   = SPD()
///           REFVAL = 4.D5
///           ADJUST = 0.D0
///
///     C
///     C     Perform the search. The set of times when the
///     C     constraint is met will be stored in the SPICE
///     C     window RESULT.
///     C
///           CALL GFDIST ( 'MOON', 'NONE', 'EARTH', '>',
///          .              REFVAL, ADJUST, STEP,    CNFINE,
///          .              MAXWIN, NWDIST, WORK,    RESULT )
///
///     C
///     C     Display the results.
///     C
///           IF ( WNCARD(RESULT) .EQ. 0 ) THEN
///
///              WRITE (*, '(A)') 'Result window is empty.'
///
///           ELSE
///
///              DO I = 1, WNCARD(RESULT)
///
///     C
///     C           Fetch the endpoints of the Ith interval
///     C           of the result window.
///     C
///                 CALL WNFETD ( RESULT, I, START, FINISH )
///
///     C
///     C           Check the distance at the start and stop times.
///     C
///                 CALL SPKPOS ( 'MOON',  START, 'J2000', 'NONE',
///          .                    'EARTH', POS,   LT            )
///                 DIST = VNORM(POS)
///
///                 CALL TIMOUT ( START, 'YYYY-MON-DD HR:MN:SC.###',
///          .                    TIMSTR                            )
///
///                 WRITE (*, '(A,F14.7)' ) 'Start time, distance = '//
///          .                              TIMSTR, DIST
///
///                 CALL SPKPOS ( 'MOON',  FINISH, 'J2000', 'NONE',
///          .                    'EARTH', POS,     LT            )
///                 DIST = VNORM(POS)
///
///                 CALL TIMOUT ( FINISH, 'YYYY-MON-DD HR:MN:SC.###',
///          .                    TIMSTR                            )
///
///                 WRITE (*, '(A,F14.7)' ) 'Stop time,  distance = '//
///          .                              TIMSTR, DIST
///              END DO
///
///           END IF
///           END
///
///
///     When this program was executed on a Mac/Intel/gfortran/64-bit
///     platform, the output was:
///
///
///     Start time, distance = 2007-JAN-08 00:10:02.439  400000.0000000
///     Stop time,  distance = 2007-JAN-13 06:36:42.770  400000.0000000
///     Start time, distance = 2007-FEB-04 07:01:30.094  400000.0000000
///     Stop time,  distance = 2007-FEB-10 09:29:56.659  400000.0000000
///     Start time, distance = 2007-MAR-03 00:19:19.998  400000.0000000
///     Stop time,  distance = 2007-MAR-10 14:03:33.312  400000.0000000
///     Start time, distance = 2007-MAR-29 22:52:52.961  400000.0000000
///     Stop time,  distance = 2007-APR-01 00:00:00.000  404531.9552322
///
///
///     Note that the distance at the final solutions interval's stop
///     time is not close to the reference value of 400000 km. This is
///     because the interval's stop time was determined by the stop
///     time of the confinement window.
///
///
///  2) Extend the first example to demonstrate use of all supported
///     relational operators. Find times when
///
///        Earth-Moon distance is = 400000 km
///        Earth-Moon distance is < 400000 km
///        Earth-Moon distance is > 400000 km
///        Earth-Moon distance is at a local minimum
///        Earth-Moon distance is at the absolute minimum
///        Earth-Moon distance is > the absolute minimum + 100 km
///        Earth-Moon distance is at a local maximum
///        Earth-Moon distance is at the absolute maximum
///        Earth-Moon distance is > the absolute maximum - 100 km
///
///     To shorten the search time and output, use the
///     shorter search interval
///
///        2007 JAN 15 00:00:00 UTC  to
///        2007 MAR 15 00:00:00 UTC
///
///     As before, use geometric (uncorrected) positions, so
///     set the aberration correction flag to 'NONE'.
///
///     Use the meta-kernel from the first example.
///
///
///     Example code begins here.
///
///
///           PROGRAM GFDIST_EX2
///           IMPLICIT NONE
///
///     C
///     C     Include GF parameter declarations:
///     C
///           INCLUDE 'gf.inc'
///
///     C
///     C     SPICELIB functions
///     C
///           DOUBLE PRECISION      SPD
///           DOUBLE PRECISION      VNORM
///           INTEGER               WNCARD
///
///     C
///     C     Local parameters
///     C
///           INTEGER               LBCELL
///           PARAMETER           ( LBCELL = -5 )
///
///     C
///     C     Use the parameter MAXWIN for both
///     C     the result window size and the workspace
///     C     size.
///     C
///           INTEGER               MAXWIN
///           PARAMETER           ( MAXWIN = 20000 )
///
///     C
///     C     Length of output time string:
///     C
///           INTEGER               TIMLEN
///           PARAMETER           ( TIMLEN = 26 )
///
///     C
///     C     Number of relational operators:
///     C
///           INTEGER               NRELOP
///           PARAMETER           ( NRELOP = 9 )
///
///     C
///     C     Operator name length:
///     C
///           INTEGER               OPNMLN
///           PARAMETER           ( OPNMLN = 6 )
///
///     C
///     C     Output line length:
///     C
///           INTEGER               LNSIZE
///           PARAMETER           ( LNSIZE = 80 )
///
///     C
///     C     Output format
///     C
///           CHARACTER*(*)         FMT1
///           PARAMETER           ( FMT1 = '(A,F12.5)' )
///
///     C
///     C     Local variables
///     C
///           CHARACTER*(OPNMLN)    RELATE ( NRELOP )
///           CHARACTER*(LNSIZE)    TEMPLT ( NRELOP )
///           CHARACTER*(TIMLEN)    TIMSTR
///           CHARACTER*(LNSIZE)    TITLE
///
///           DOUBLE PRECISION      ADJUST ( NRELOP )
///           DOUBLE PRECISION      CNFINE ( LBCELL : 2 )
///           DOUBLE PRECISION      DIST
///           DOUBLE PRECISION      ET0
///           DOUBLE PRECISION      ET1
///           DOUBLE PRECISION      FINSH
///           DOUBLE PRECISION      LT
///           DOUBLE PRECISION      POS    ( 3 )
///           DOUBLE PRECISION      REFVAL
///           DOUBLE PRECISION      RESULT ( LBCELL : MAXWIN )
///           DOUBLE PRECISION      START
///           DOUBLE PRECISION      STEP
///           DOUBLE PRECISION      WORK   ( LBCELL : MAXWIN, NWDIST )
///
///           INTEGER               I
///           INTEGER               J
///
///     C
///     C     Saved variables
///     C
///           SAVE                  ADJUST
///           SAVE                  RELATE
///           SAVE                  TEMPLT
///
///     C
///     C     The confinement, workspace and result windows CNFINE,
///     C     WORK and RESULT are saved because this practice helps to
///     C     prevent stack overflow.
///     C
///           SAVE                  CNFINE
///           SAVE                  RESULT
///           SAVE                  WORK
///
///     C
///     C     Initial values
///     C
///           DATA                  ADJUST / 0.D0,
///          .                               0.D0,
///          .                               0.D0,
///          .                               0.D0,
///          .                               0.D0,
///          .                               100.D0,
///          .                               0.D0,
///          .                               0.D0,
///          .                               100.D0 /
///
///           DATA                  RELATE / '=',
///          .                               '<',
///          .                               '>',
///          .                               'LOCMIN',
///          .                               'ABSMIN',
///          .                               'ABSMIN',
///          .                               'LOCMAX',
///          .                               'ABSMAX',
///          .                               'ABSMAX'  /
///
///           DATA                  TEMPLT /
///          .   'Condition: distance = # km',
///          .   'Condition: distance < # km',
///          .   'Condition: distance > # km',
///          .   'Condition: distance is a local minimum',
///          .   'Condition: distance is the absolute minimum',
///          .   'Condition: distance < the absolute minimum + * km',
///          .   'Condition: distance is a local maximum',
///          .   'Condition: distance is the absolute maximum',
///          .   'Condition: distance > the absolute maximum - * km' /
///
///     C
///     C     Load kernels.
///     C
///           CALL FURNSH ( 'gfdist_ex1.tm' )
///
///     C
///     C     Initialize windows.
///     C
///           CALL SSIZED ( MAXWIN, RESULT )
///           CALL SSIZED ( 2,      CNFINE )
///
///     C
///     C     Store the time bounds of our search interval in
///     C     the confinement window.
///     C
///           CALL STR2ET ( '2007 JAN 15', ET0 )
///           CALL STR2ET ( '2007 MAR 15', ET1 )
///
///           CALL WNINSD ( ET0, ET1, CNFINE )
///
///     C
///     C     Search using a step size of 1 day (in units of
///     C     seconds). Use a reference value of 400000 km.
///     C
///           STEP   = SPD()
///           REFVAL = 4.D5
///
///           DO I = 1, NRELOP
///
///              CALL GFDIST ( 'MOON', 'NONE',    'EARTH', RELATE(I),
///          .                 REFVAL, ADJUST(I), STEP,    CNFINE,
///          .                 MAXWIN, NWDIST,    WORK,    RESULT    )
///
///     C
///     C        Display the results.
///     C
///              WRITE (*,*) ' '
///
///     C
///     C        Substitute the reference and adjustment values,
///     C        where applicable, into the title string:
///     C
///              CALL REPMD ( TEMPLT(I), '#', REFVAL,    6, TITLE )
///              CALL REPMD ( TITLE,     '*', ADJUST(I), 6, TITLE )
///
///              WRITE (*, '(A)' ) TITLE
///
///              IF ( WNCARD(RESULT) .EQ. 0 ) THEN
///                 WRITE (*, '(A)' ) ' Result window is empty.'
///              ELSE
///                 WRITE (*, '(A)' ) ' Result window:'
///
///                 DO J = 1, WNCARD(RESULT)
///
///     C
///     C              Fetch the endpoints of the Jth interval
///     C              of the result window.
///     C
///                    CALL WNFETD ( RESULT, J, START, FINSH )
///
///     C
///     C              Check the distance at the start and stop times.
///     C
///                    CALL SPKPOS ( 'MOON',  START, 'J2000', 'NONE',
///          .                       'EARTH', POS,   LT              )
///                    DIST = VNORM(POS)
///
///                    CALL TIMOUT ( START, 'YYYY-MON-DD HR:MN:SC.###',
///          .                       TIMSTR                           )
///
///                    WRITE (*, FMT1 ) '  Start time, distance = '
///          .         //               TIMSTR, DIST
///
///                    CALL SPKPOS ( 'MOON',  FINSH, 'J2000', 'NONE',
///          .                       'EARTH', POS,     LT            )
///                    DIST = VNORM(POS)
///
///                    CALL TIMOUT ( FINSH, 'YYYY-MON-DD HR:MN:SC.###',
///          .                       TIMSTR                           )
///
///                    WRITE (*, FMT1 ) '  Stop time,  distance = '
///          .         //               TIMSTR, DIST
///                 END DO
///
///              END IF
///
///           END DO
///
///           WRITE (*,*) ' '
///
///           END
///
///
///     When this program was executed on a Mac/Intel/gfortran/64-bit
///     platform, the output was:
///
///
///     Condition: distance = 4.00000E+05 km
///      Result window:
///       Start time, distance = 2007-FEB-04 07:01:30.094  400000.00000
///       Stop time,  distance = 2007-FEB-04 07:01:30.094  400000.00000
///       Start time, distance = 2007-FEB-10 09:29:56.659  400000.00000
///       Stop time,  distance = 2007-FEB-10 09:29:56.659  400000.00000
///       Start time, distance = 2007-MAR-03 00:19:19.998  400000.00000
///       Stop time,  distance = 2007-MAR-03 00:19:19.998  400000.00000
///       Start time, distance = 2007-MAR-10 14:03:33.312  400000.00000
///       Stop time,  distance = 2007-MAR-10 14:03:33.312  400000.00000
///
///     Condition: distance < 4.00000E+05 km
///      Result window:
///       Start time, distance = 2007-JAN-15 00:00:00.000  393018.60991
///       Stop time,  distance = 2007-FEB-04 07:01:30.094  400000.00000
///       Start time, distance = 2007-FEB-10 09:29:56.659  400000.00000
///       Stop time,  distance = 2007-MAR-03 00:19:19.998  400000.00000
///       Start time, distance = 2007-MAR-10 14:03:33.312  400000.00000
///       Stop time,  distance = 2007-MAR-15 00:00:00.000  376255.45393
///
///     Condition: distance > 4.00000E+05 km
///      Result window:
///       Start time, distance = 2007-FEB-04 07:01:30.094  400000.00000
///       Stop time,  distance = 2007-FEB-10 09:29:56.659  400000.00000
///       Start time, distance = 2007-MAR-03 00:19:19.998  400000.00000
///       Stop time,  distance = 2007-MAR-10 14:03:33.312  400000.00000
///
///     Condition: distance is a local minimum
///      Result window:
///       Start time, distance = 2007-JAN-22 12:30:49.458  366925.80411
///       Stop time,  distance = 2007-JAN-22 12:30:49.458  366925.80411
///       Start time, distance = 2007-FEB-19 09:36:29.968  361435.64681
///       Stop time,  distance = 2007-FEB-19 09:36:29.968  361435.64681
///
///     Condition: distance is the absolute minimum
///      Result window:
///       Start time, distance = 2007-FEB-19 09:36:29.968  361435.64681
///       Stop time,  distance = 2007-FEB-19 09:36:29.968  361435.64681
///
///     Condition: distance < the absolute minimum + 1.00000E+02 km
///      Result window:
///       Start time, distance = 2007-FEB-19 01:09:52.706  361535.64681
///       Stop time,  distance = 2007-FEB-19 18:07:45.136  361535.64681
///
///     Condition: distance is a local maximum
///      Result window:
///       Start time, distance = 2007-FEB-07 12:38:29.870  404992.42429
///       Stop time,  distance = 2007-FEB-07 12:38:29.870  404992.42429
///       Start time, distance = 2007-MAR-07 03:37:02.122  405853.45213
///       Stop time,  distance = 2007-MAR-07 03:37:02.122  405853.45213
///
///     Condition: distance is the absolute maximum
///      Result window:
///       Start time, distance = 2007-MAR-07 03:37:02.122  405853.45213
///       Stop time,  distance = 2007-MAR-07 03:37:02.122  405853.45213
///
///     Condition: distance > the absolute maximum - 1.00000E+02 km
///      Result window:
///       Start time, distance = 2007-MAR-06 15:56:00.957  405753.45213
///       Stop time,  distance = 2007-MAR-07 15:00:38.674  405753.45213
/// ```
///
/// # Restrictions
///
/// ```text
///  1)  The kernel files to be used by this routine must be loaded
///      (normally via the SPICELIB routine FURNSH) before this routine
///      is called.
/// ```
///
/// # Author and Institution
///
/// ```text
///  N.J. Bachman       (JPL)
///  J. Diaz del Rio    (ODC Space)
///  E.D. Wright        (JPL)
/// ```
///
/// # Version
///
/// ```text
/// -    SPICELIB Version 1.1.1, 27-OCT-2021 (JDR) (NJB)
///
///         Edited the header to comply with NAIF standard.
///
///         Edited second example code and modified the output resolution
///         for the distances in that example to fit in the $Examples
///         section without modifications. Renamed example's meta-kernel.
///         Added SAVE statements for CNFINE, WORK and RESULT variables in
///         code examples.
///
///         Updated description of WORK and RESULT arguments in $Brief_I/O,
///         $Detailed_Input and $Detailed_Output.
///
///         Updated header to describe use of expanded confinement window.
///
/// -    SPICELIB Version 1.1.0, 05-SEP-2012 (EDW)
///
///         Edit to comments to correct search description.
///
///         Implemented use of ZZHOLDD to allow user to alter convergence
///         tolerance.
///
///         Removed the STEP > 0 error check. The GFSSTP call includes
///         the check.
///
/// -    SPICELIB Version 1.0.0, 15-APR-2009 (NJB) (EDW)
/// ```
pub fn gfdist(
    ctx: &mut SpiceContext,
    target: &str,
    abcorr: &str,
    obsrvr: &str,
    relate: &str,
    refval: f64,
    adjust: f64,
    step: f64,
    cnfine: &[f64],
    mw: i32,
    nw: i32,
    work: &mut [f64],
    result: &mut [f64],
) -> crate::Result<()> {
    GFDIST(
        target.as_bytes(),
        abcorr.as_bytes(),
        obsrvr.as_bytes(),
        relate.as_bytes(),
        refval,
        adjust,
        step,
        cnfine,
        mw,
        nw,
        work,
        result,
        ctx.raw_context(),
    )?;
    ctx.handle_errors()?;
    Ok(())
}

//$Procedure GFDIST ( GF, distance search )
pub fn GFDIST(
    TARGET: &[u8],
    ABCORR: &[u8],
    OBSRVR: &[u8],
    RELATE: &[u8],
    REFVAL: f64,
    ADJUST: f64,
    STEP: f64,
    CNFINE: &[f64],
    MW: i32,
    NW: i32,
    WORK: &mut [f64],
    RESULT: &mut [f64],
    ctx: &mut Context,
) -> f2rust_std::Result<()> {
    let CNFINE = DummyArray::new(CNFINE, LBCELL..);
    let mut WORK = DummyArrayMut2D::new(WORK, LBCELL..=MW, 1..=NW);
    let mut RESULT = DummyArrayMut::new(RESULT, LBCELL..);
    let mut TOL: f64 = 0.0;
    let mut OK: bool = false;
    let mut QCPARS = ActualCharArray::new(LNSIZE, 1..=QNPARS);
    let mut QPNAMS = ActualCharArray::new(LNSIZE, 1..=QNPARS);
    let QDPARS = StackArray::<f64, 3>::new(1..=QNPARS);
    let QIPARS = StackArray::<i32, 3>::new(1..=QNPARS);
    let QLPARS = StackArray::<bool, 3>::new(1..=QNPARS);

    //
    // SPICELIB functions
    //

    //
    // External functions
    //

    //
    // Interrupt indicator function:
    //

    //
    // Routines to set step size, refine transition times
    // and report work.
    //

    //
    // Local parameters
    //

    //
    // Local variables
    //

    //
    // Quantity definition parameter arrays:
    //

    //
    // Standard SPICE error handling.
    //
    if RETURN(ctx) {
        return Ok(());
    }

    CHKIN(b"GFDIST", ctx)?;

    //
    // Check the workspace window dimensions.
    //
    if (MW < 2) {
        SETMSG(
            b"Workspace window size was #; size must be at least 2.",
            ctx,
        );
        ERRINT(b"#", MW, ctx);
        SIGERR(b"SPICE(INVALIDDIMENSION)", ctx)?;
        CHKOUT(b"GFDIST", ctx)?;
        return Ok(());
    }

    if (NW < NWDIST) {
        SETMSG(
            b"Workspace window count was #; count must be at least #.",
            ctx,
        );
        ERRINT(b"#", NW, ctx);
        ERRINT(b"#", NWDIST, ctx);
        SIGERR(b"SPICE(INVALIDDIMENSION)", ctx)?;
        CHKOUT(b"GFDIST", ctx)?;
        return Ok(());
    }

    //
    // Check the result window size.
    //
    if (SIZED(RESULT.as_slice(), ctx)? < 2) {
        SETMSG(b"Result window size was #; size must be at least 2.", ctx);
        ERRINT(b"#", SIZED(RESULT.as_slice(), ctx)?, ctx);
        SIGERR(b"SPICE(INVALIDDIMENSION)", ctx)?;
        CHKOUT(b"GFDIST", ctx)?;
        return Ok(());
    }

    //
    // Set up a call to GFEVNT, which will handle the search.
    //
    fstr::assign(QPNAMS.get_mut(1), b"TARGET");
    fstr::assign(QCPARS.get_mut(1), TARGET);

    fstr::assign(QPNAMS.get_mut(2), b"OBSERVER");
    fstr::assign(QCPARS.get_mut(2), OBSRVR);

    fstr::assign(QPNAMS.get_mut(3), b"ABCORR");
    fstr::assign(QCPARS.get_mut(3), ABCORR);

    //
    // Check and set the step size.
    //
    GFSSTP(STEP, ctx)?;

    //
    // Retrieve the convergence tolerance, if set.
    //
    ZZHOLDD(ZZGET, GF_TOL, &mut OK, &mut TOL, ctx)?;

    //
    // Use the default value CNVTOL if no stored tolerance value.
    //
    if !OK {
        TOL = CNVTOL;
    }

    //
    // Initialize the RESULT window.
    //
    SCARDD(0, RESULT.as_slice_mut(), ctx)?;

    //
    // Look for solutions.
    //
    // Progress report and bail-out options are set to .FALSE.
    //
    GFEVNT(
        GFSTEP,
        GFREFN,
        b"DISTANCE",
        QNPARS,
        QPNAMS.as_arg(),
        QCPARS.as_arg(),
        QDPARS.as_slice(),
        QIPARS.as_slice(),
        QLPARS.as_slice(),
        RELATE,
        REFVAL,
        TOL,
        ADJUST,
        CNFINE.as_slice(),
        NORPT,
        GFREPI,
        GFREPU,
        GFREPF,
        MW,
        NWDIST,
        WORK.as_slice_mut(),
        NOBAIL,
        GFBAIL,
        RESULT.as_slice_mut(),
        ctx,
    )?;

    CHKOUT(b"GFDIST", ctx)?;
    Ok(())
}