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//
// GENERATED FILE
//
use *;
use crateSpiceContext;
use *;
const MAXSRF: i32 = 100;
const INERTL: i32 = 1;
const PCK: i32 = ;
const CK: i32 = ;
const TK: i32 = ;
const DYN: i32 = ;
const SWTCH: i32 = ;
const ALL: i32 = -1;
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: & = b"CIRCLE";
const FTELLI: & = b"ELLIPSE";
const FTPOLY: & = b"POLYGON";
const FTRECT: & = b"RECTANGLE";
const ANNULR: & = b"ANNULAR";
const ANY: & = b"ANY";
const PARTL: & = b"PARTIAL";
const FULL: & = b"FULL";
const DSSHAP: & = b"DSK";
const EDSHAP: & = b"ELLIPSOID";
const PTSHAP: & = b"POINT";
const RYSHAP: & = b"RAY";
const SPSHAP: & = b"SPHERE";
const NOCTYP: i32 = 4;
const OCLLN: i32 = 7;
const SHPLEN: i32 = 9;
const MAXVRT: i32 = 10000;
const CIRFOV: & = b"CIRCLE";
const ELLFOV: & = b"ELLIPSE";
const POLFOV: & = b"POLYGON";
const RECFOV: & = b"RECTANGLE";
const NABCOR: i32 = 15;
const ABATSZ: i32 = 6;
const GEOIDX: i32 = 1;
const LTIDX: i32 = ;
const STLIDX: i32 = ;
const CNVIDX: i32 = ;
const XMTIDX: i32 = ;
const RELIDX: i32 = ;
const CORLEN: i32 = 5;
const CTRSIZ: i32 = 2;
const DSKSHP: i32 = 2;
const ELLSHP: i32 = 1;
const MTHLEN: i32 = 500;
const SUBLEN: i32 = 20;
const CVTLEN: i32 = 20;
const TANGNT: i32 = 1;
const GUIDED: i32 = 2;
const TMTLEN: i32 = 20;
const LMBCRV: i32 = 0;
const UMBRAL: i32 = 1;
const PNMBRL: i32 = 2;
const ACLLEN: i32 = 25;
const CTRCOR: i32 = 1;
const ELLCOR: i32 = 2;
const RNAME: & = b"SINCPT";
const MAXL: i32 = 36;
const FRNMLN: i32 = 32;
/// Surface intercept
///
/// Compute, for a given observer and a ray emanating from the
/// observer, the surface intercept of the ray on a target body at
/// a specified epoch, optionally corrected for light time and
/// stellar aberration.
///
/// The surface of the target body may be represented by a triaxial
/// ellipsoid or by topographic data provided by DSK files.
///
/// This routine supersedes SRFXPT.
///
/// # Required Reading
///
/// * [CK](crate::required_reading::ck)
/// * [DSK](crate::required_reading::dsk)
/// * [FRAMES](crate::required_reading::frames)
/// * [NAIF_IDS](crate::required_reading::naif_ids)
/// * [PCK](crate::required_reading::pck)
/// * [SCLK](crate::required_reading::sclk)
/// * [SPK](crate::required_reading::spk)
/// * [TIME](crate::required_reading::time)
///
/// # Brief I/O
///
/// ```text
/// VARIABLE I/O DESCRIPTION
/// -------- --- --------------------------------------------------
/// METHOD I Computation method.
/// TARGET I Name of target body.
/// ET I Epoch in ephemeris seconds past J2000 TDB.
/// FIXREF I Body-fixed, body-centered target body frame.
/// ABCORR I Aberration correction.
/// OBSRVR I Name of observing body.
/// DREF I Reference frame of ray's direction vector.
/// DVEC I Ray's direction vector.
/// SPOINT O Surface intercept point on the target body.
/// TRGEPC O Intercept epoch.
/// SRFVEC O Vector from observer to intercept point.
/// FOUND O Flag indicating whether intercept was found.
/// ```
///
/// # Detailed Input
///
/// ```text
/// METHOD is a short string providing parameters defining
/// the computation method to be used. In the syntax
/// descriptions below, items delimited by brackets
/// are optional.
///
/// METHOD may be assigned the following values:
///
/// 'ELLIPSOID'
///
/// The intercept computation uses a triaxial
/// ellipsoid to model the surface of the target
/// body. The ellipsoid's radii must be available
/// in the kernel pool.
///
///
/// 'DSK/UNPRIORITIZED[/SURFACES = <surface list>]'
///
/// The intercept computation uses topographic data
/// to model the surface of the target body. These
/// data must be provided by loaded DSK files.
///
/// The surface list specification is optional. The
/// syntax of the list is
///
/// <surface 1> [, <surface 2>...]
///
/// If present, it indicates that data only for the
/// listed surfaces are to be used; however, data
/// need not be available for all surfaces in the
/// list. If absent, loaded DSK data for any surface
/// associated with the target body are used.
///
/// The surface list may contain surface names or
/// surface ID codes. Names containing blanks must
/// be delimited by double quotes, for example
///
/// SURFACES = "Mars MEGDR 128 PIXEL/DEG"
///
/// If multiple surfaces are specified, their names
/// or IDs must be separated by commas.
///
/// See the $Particulars section below for details
/// concerning use of DSK data.
///
///
/// Neither case nor white space are significant in
/// METHOD, except within double-quoted strings. For
/// example, the string ' eLLipsoid ' is valid.
///
/// Within double-quoted strings, blank characters are
/// significant, but multiple consecutive blanks are
/// considered equivalent to a single blank. Case is
/// not significant. So
///
/// "Mars MEGDR 128 PIXEL/DEG"
///
/// is equivalent to
///
/// " mars megdr 128 pixel/deg "
///
/// but not to
///
/// "MARS MEGDR128PIXEL/DEG"
///
/// TARGET is the name of the target body. TARGET is
/// case-insensitive, and leading and trailing blanks in
/// TARGET are not significant. Optionally, you may
/// supply a string containing the integer ID code
/// for the object. For example both 'MOON' and '301'
/// are legitimate strings that indicate the Moon is the
/// target body.
///
/// When the target body's surface is represented by a
/// tri-axial ellipsoid, this routine assumes that a
/// kernel variable representing the ellipsoid's radii is
/// present in the kernel pool. Normally the kernel
/// variable would be defined by loading a PCK file.
///
/// ET is the epoch of participation of the observer,
/// expressed as ephemeris seconds past J2000 TDB: ET is
/// the epoch at which the observer's state is computed.
///
/// When aberration corrections are not used, ET is also
/// the epoch at which the state and orientation of the
/// target body are computed.
///
/// When aberration corrections are used, the position
/// and orientation of the target body are computed at
/// ET-LT or ET+LT, where LT is the one-way light time
/// between the intercept point and the observer, and the
/// sign applied to LT depends on the selected
/// correction. See the description of ABCORR below for
/// details.
///
/// FIXREF is the name of a body-fixed reference frame centered
/// on the target body. FIXREF may be any such frame
/// supported by the SPICE system, including built-in
/// frames (documented in the Frames Required Reading)
/// and frames defined by a loaded frame kernel (FK). The
/// string FIXREF is case-insensitive, and leading and
/// trailing blanks in FIXREF are not significant.
///
/// The output intercept point SPOINT and the observer-to-
/// intercept vector SRFVEC will be expressed relative to
/// this reference frame.
///
/// ABCORR indicates the aberration corrections to be applied
/// when computing the target's position and orientation.
///
/// For remote sensing applications, where the apparent
/// surface intercept point seen by the observer is
/// desired, normally the correction
///
/// 'CN+S'
///
/// should be used. This and the other supported options
/// are described below. ABCORR may be any of the
/// following:
///
/// 'NONE' Apply no correction. Return the
/// geometric surface intercept point on the
/// target body.
///
/// Let LT represent the one-way light time between the
/// observer and the surface intercept point (note: NOT
/// between the observer and the target body's center).
/// The following values of ABCORR apply to the
/// "reception" case in which photons depart from the
/// intercept point's location at the light-time
/// corrected epoch ET-LT and *arrive* at the observer's
/// location at ET:
///
/// 'LT' Correct for one-way light time (also
/// called "planetary aberration") using a
/// Newtonian formulation. This correction
/// yields the location of the surface
/// intercept point at the moment it
/// emitted photons arriving at the
/// observer at ET.
///
/// The light time correction uses an
/// iterative solution of the light time
/// equation. The solution invoked by the
/// 'LT' option uses one iteration.
///
/// Both the target position as seen by the
/// observer, and rotation of the target
/// body, are corrected for light time.
///
/// 'LT+S' Correct for one-way light time and
/// stellar aberration using a Newtonian
/// formulation. This option modifies the
/// surface intercept obtained with the
/// 'LT' option to account for the
/// observer's velocity relative to the
/// solar system barycenter. These
/// computations yield the apparent surface
/// intercept point.
///
/// 'CN' Converged Newtonian light time
/// correction. In solving the light time
/// equation, the 'CN' correction iterates
/// until the solution converges. Both the
/// position and rotation of the target
/// body are corrected for light time.
///
/// 'CN+S' Converged Newtonian light time and
/// stellar aberration corrections. This
/// option produces a solution that is at
/// least as accurate at that obtainable
/// with the 'LT+S' option. Whether the
/// 'CN+S' solution is substantially more
/// accurate depends on the geometry of the
/// participating objects and on the
/// accuracy of the input data. In all
/// cases this routine will execute more
/// slowly when a converged solution is
/// computed.
///
/// For reception-case applications
/// involving intercepts near the target
/// body limb, this option should be used.
///
/// The following values of ABCORR apply to the
/// "transmission" case in which photons *depart* from
/// the observer's location at ET and arrive at the
/// intercept point at the light-time corrected epoch
/// ET+LT:
///
/// 'XLT' "Transmission" case: correct for
/// one-way light time using a Newtonian
/// formulation. This correction yields the
/// intercept location at the moment it
/// receives photons emitted from the
/// observer's location at ET.
///
/// The light time correction uses an
/// iterative solution of the light time
/// equation. The solution invoked by the
/// 'XLT' option uses one iteration.
///
/// Both the target position as seen by the
/// observer, and rotation of the target
/// body, are corrected for light time.
///
/// 'XLT+S' "Transmission" case: correct for
/// one-way light time and stellar
/// aberration using a Newtonian
/// formulation. This option modifies the
/// intercept obtained with the 'XLT'
/// option to account for the observer's
/// velocity relative to the solar system
/// barycenter.
///
/// 'XCN' Converged Newtonian light time
/// correction. This is the same as 'XLT'
/// correction but with further iterations
/// to a converged Newtonian light time
/// solution.
///
/// 'XCN+S' "Transmission" case: converged
/// Newtonian light time and stellar
/// aberration corrections. This option
/// produces a solution that is at least as
/// accurate at that obtainable with the
/// 'XLT+S' option. Whether the 'XCN+S'
/// solution is substantially more accurate
/// depends on the geometry of the
/// participating objects and on the
/// accuracy of the input data. In all
/// cases this routine will execute more
/// slowly when a converged solution is
/// computed.
///
/// For transmission-case applications
/// involving intercepts near the target
/// body limb, this option should be used.
///
/// Case and embedded blanks are not significant in
/// ABCORR. For example, the string
///
/// 'Cn + s'
///
/// is valid.
///
/// OBSRVR is the name of the observing body. This is typically
/// a spacecraft, the earth, or a surface point on the
/// earth or on another extended object.
///
/// The observer must be outside the target body.
///
/// OBSRVR is case-insensitive, and leading and
/// trailing blanks in OBSRVR are not significant.
/// Optionally, you may supply a string containing the
/// integer ID code for the object. For example both
/// 'MOON' and '301' are legitimate strings that indicate
/// the Moon is the observer.
///
/// DREF is the name of the reference frame relative to which
/// the ray's direction vector is expressed. This may be
/// any frame supported by the SPICE system, including
/// built-in frames (documented in the Frames Required
/// Reading) and frames defined by a loaded frame kernel
/// (FK). The string DREF is case-insensitive, and
/// leading and trailing blanks in DREF are not
/// significant.
///
/// When DREF designates a non-inertial frame, the
/// orientation of the frame is evaluated at an epoch
/// dependent on the frame's center and, if the center is
/// not the observer, on the selected aberration
/// correction. See the description of the direction
/// vector DVEC for details.
///
/// DVEC is a ray direction vector emanating from the observer.
/// The intercept with the target body's surface of the ray
/// defined by the observer and DVEC is sought.
///
/// DVEC is specified relative to the reference frame
/// designated by DREF.
///
/// Non-inertial reference frames are treated as follows:
/// if the center of the frame is at the observer's
/// location, the frame is evaluated at ET. If the
/// frame's center is located elsewhere, then letting
/// LTCENT be the one-way light time between the observer
/// and the central body associated with the frame, the
/// orientation of the frame is evaluated at ET-LTCENT,
/// ET+LTCENT, or ET depending on whether the requested
/// aberration correction is, respectively, for received
/// radiation, transmitted radiation, or is omitted.
/// LTCENT is computed using the method indicated by
/// ABCORR.
/// ```
///
/// # Detailed Output
///
/// ```text
/// SPOINT is the surface intercept point on the target body of
/// the ray defined by the observer and the direction
/// vector. If the ray intersects the target body in
/// multiple points, the selected intersection point is
/// the one closest to the observer. The output argument
/// FOUND (see below) indicates whether an intercept was
/// found.
///
/// SPOINT is expressed in Cartesian coordinates,
/// relative to the target body-fixed frame designated by
/// FIXREF. The body-fixed target frame is evaluated at
/// the intercept epoch TRGEPC (see description below).
///
/// When light time correction is used, the duration of
/// light travel between SPOINT to the observer is
/// considered to be the one way light time. When both
/// light time and stellar aberration corrections are
/// used, SPOINT is compute such that, when the vector
/// from the observer to SPOINT is corrected for light
/// time and stellar aberration, the resulting vector
/// lies on the ray defined by the observer's location
/// and DVEC.
///
/// The components of SPOINT are given in units of km.
///
/// TRGEPC is the "intercept epoch." TRGEPC is defined as
/// follows: letting LT be the one-way light time between
/// the observer and the intercept point, TRGEPC is the
/// epoch ET-LT, ET+LT, or ET depending on whether the
/// requested aberration correction is, respectively, for
/// received radiation, transmitted radiation, or
/// omitted. LT is computed using the method indicated by
/// ABCORR.
///
/// TRGEPC is expressed as seconds past J2000 TDB.
///
/// SRFVEC is the vector from the observer's position at ET to
/// the aberration-corrected (or optionally, geometric)
/// position of SPOINT, where the aberration corrections
/// are specified by ABCORR. SRFVEC is expressed in the
/// target body-fixed reference frame designated by
/// FIXREF, evaluated at TRGEPC.
///
/// The components of SRFVEC are given in units of km.
///
/// One can use the SPICELIB function VNORM to obtain the
/// distance between the observer and SPOINT:
///
/// DIST = VNORM ( SRFVEC )
///
/// The observer's position OBSPOS, relative to the
/// target body's center, where the center's position is
/// corrected for aberration effects as indicated by
/// ABCORR, can be computed via the call:
///
/// CALL VSUB ( SPOINT, SRFVEC, OBSPOS )
///
/// To transform the vector SRFVEC from a reference frame
/// FIXREF at time TRGEPC to a time-dependent reference
/// frame REF at time ET, the routine PXFRM2 should be
/// called. Let XFORM be the 3x3 matrix representing the
/// rotation from the reference frame FIXREF at time
/// TRGEPC to the reference frame REF at time ET. Then
/// SRFVEC can be transformed to the result REFVEC as
/// follows:
///
/// CALL PXFRM2 ( FIXREF, REF, TRGEPC, ET, XFORM )
/// CALL MXV ( XFORM, SRFVEC, REFVEC )
///
/// The second example in the $Examples header section
/// below presents a complete program that demonstrates
/// this procedure.
///
/// FOUND is a logical flag indicating whether or not the ray
/// intersects the target. If an intersection exists
/// FOUND will be returned as .TRUE. If the ray misses
/// the target, FOUND will be returned as .FALSE.
/// ```
///
/// # Exceptions
///
/// ```text
/// 1) If the specified aberration correction is unrecognized, an
/// error is signaled by a routine in the call tree of this
/// routine.
///
/// 2) If either the target or observer input strings cannot be
/// converted to an integer ID code, the error
/// SPICE(IDCODENOTFOUND) is signaled.
///
/// 3) If OBSRVR and TARGET map to the same NAIF integer ID code,
/// the error SPICE(BODIESNOTDISTINCT) is signaled.
///
/// 4) If the input target body-fixed frame FIXREF is not
/// recognized, the error SPICE(NOFRAME) is signaled. A frame
/// name may fail to be recognized because a required frame
/// specification kernel has not been loaded; another cause is a
/// misspelling of the frame name.
///
/// 5) If the input frame FIXREF is not centered at the target body,
/// the error SPICE(INVALIDFRAME) is signaled.
///
/// 6) If the input argument METHOD cannot be parsed, an error
/// is signaled by either this routine or a routine in the
/// call tree of this routine.
///
/// 7) If the target and observer have distinct identities but are
/// at the same location (for example, the target is Mars and the
/// observer is the Mars barycenter), the error
/// SPICE(NOSEPARATION) is signaled.
///
/// 8) If insufficient ephemeris data have been loaded prior to
/// calling SINCPT, an error is signaled by a
/// routine in the call tree of this routine. Note that when
/// light time correction is used, sufficient ephemeris data must
/// be available to propagate the states of both observer and
/// target to the solar system barycenter.
///
/// 9) If the computation method specifies an ellipsoidal target
/// shape and triaxial radii of the target body have not been
/// loaded into the kernel pool prior to calling SINCPT, an error
/// is signaled by a routine in the call tree of this routine.
///
/// 10) The target must be an extended body: if any of the radii of
/// the target body are non-positive, an error is signaled by a
/// routine in the call tree of this routine.
///
/// 11) If PCK data specifying the target body-fixed frame orientation
/// have not been loaded prior to calling SINCPT, an error is
/// signaled by a routine in the call tree of this routine.
///
/// 12) If the reference frame designated by DREF is not recognized
/// by the SPICE frame subsystem, the error SPICE(NOFRAME)
/// is signaled.
///
/// 13) If the direction vector DVEC is the zero vector, the error
/// SPICE(ZEROVECTOR) is signaled.
///
/// 14) If METHOD specifies that the target surface is represented by
/// DSK data, and no DSK files are loaded for the specified
/// target, an error is signaled by a routine in the call tree
/// of this routine.
///
/// 15) If METHOD specifies that the target surface is represented
/// by DSK data, and DSK data are not available for a portion of
/// the target body's surface, an intercept might not be found.
/// This routine does not revert to using an ellipsoidal surface
/// in this case.
/// ```
///
/// # 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 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.
///
/// - PCK data: if the computation method is specified as
/// "Ellipsoid," triaxial radii for the target body must be
/// loaded into the kernel pool. Typically this is done by
/// loading a text PCK file via FURNSH.
///
/// - Further PCK data: rotation data for the target body must
/// be loaded. These may be provided in a text or binary PCK
/// file.
///
/// The following data may be required:
///
/// - DSK data: if METHOD indicates that DSK data are to be used,
/// DSK files containing topographic data for the target body
/// must be loaded. If a surface list is specified, data for
/// at least one of the listed surfaces must be loaded.
///
/// - Surface name-ID associations: if surface names are specified
/// in METHOD, the association of these names with their
/// corresponding surface ID codes must be established by
/// assignments of the kernel variables
///
/// NAIF_SURFACE_NAME
/// NAIF_SURFACE_CODE
/// NAIF_SURFACE_BODY
///
/// Normally these associations are made by loading a text
/// kernel containing the necessary assignments. An example
/// of such an assignment is
///
/// NAIF_SURFACE_NAME += 'Mars MEGDR 128 PIXEL/DEG'
/// NAIF_SURFACE_CODE += 1
/// NAIF_SURFACE_BODY += 499
///
/// - Frame data: if a frame definition is required to convert
/// the observer and target states to the body-fixed frame of
/// the target, that definition must be available in the kernel
/// pool. Similarly, the frame definition required to map
/// between the frame designated by DREF and the target
/// body-fixed frame must be available. Typically the
/// definitions of frames not already built-in to SPICE are
/// supplied by loading a frame kernel.
///
/// - CK data: if the frame to which DREF refers is fixed to a
/// spacecraft instrument or structure, at least one CK file
/// will be needed to permit transformation of vectors between
/// that frame and both the J2000 and the target body-fixed
/// frames.
///
/// - SCLK data: if a CK file is needed, an associated SCLK
/// kernel is required to enable conversion between encoded SCLK
/// (used to time-tag CK data) and barycentric dynamical time
/// (TDB).
///
/// In all cases, kernel data are normally loaded once per program
/// run, NOT every time this routine is called.
/// ```
///
/// # Particulars
///
/// ```text
/// Given a ray defined by a direction vector and the location of an
/// observer, SINCPT computes the surface intercept point of the ray
/// on a specified target body. SINCPT also determines the vector
/// from the observer to the surface intercept point. If the ray
/// intersects the target in multiple locations, the intercept
/// closest to the observer is selected.
///
/// When aberration corrections are used, this routine finds the
/// value of SPOINT such that, if SPOINT is regarded as an ephemeris
/// object, after the selected aberration corrections are applied to
/// the vector from the observer to SPOINT, the resulting vector is
/// parallel to the direction vector DVEC.
///
/// This routine computes light time corrections using light time
/// between the observer and the surface intercept point, as opposed
/// to the center of the target. Similarly, stellar aberration
/// corrections done by this routine are based on the direction of
/// the vector from the observer to the light-time corrected
/// intercept point, not to the target center. This technique avoids
/// errors due to the differential between aberration corrections
/// across the target body. Therefore it's valid to use aberration
/// corrections with this routine even when the observer is very
/// close to the intercept point, in particular when the
/// observer-intercept point distance is much less than the
/// observer-target center distance. It's also valid to use stellar
/// aberration corrections even when the intercept point is near or
/// on the limb (as may occur in occultation computations using a
/// point target).
///
/// When comparing surface intercept point computations with results
/// from sources other than SPICE, it's essential to make sure the
/// same geometric definitions are used.
///
///
/// Using DSK data
/// ==============
///
/// DSK loading and unloading
/// -------------------------
///
/// DSK files providing data used by this routine are loaded by
/// calling FURNSH and can be unloaded by calling UNLOAD or
/// KCLEAR. See the documentation of FURNSH for limits on numbers
/// of loaded DSK files.
///
/// For run-time efficiency, it's desirable to avoid frequent
/// loading and unloading of DSK files. When there is a reason to
/// use multiple versions of data for a given target body---for
/// example, if topographic data at varying resolutions are to be
/// used---the surface list can be used to select DSK data to be
/// used for a given computation. It is not necessary to unload
/// the data that are not to be used. This recommendation presumes
/// that DSKs containing different versions of surface data for a
/// given body have different surface ID codes.
///
///
/// DSK data priority
/// -----------------
///
/// A DSK coverage overlap occurs when two segments in loaded DSK
/// files cover part or all of the same domain---for example, a
/// given longitude-latitude rectangle---and when the time
/// intervals of the segments overlap as well.
///
/// When DSK data selection is prioritized, in case of a coverage
/// overlap, if the two competing segments are in different DSK
/// files, the segment in the DSK file loaded last takes
/// precedence. If the two segments are in the same file, the
/// segment located closer to the end of the file takes
/// precedence.
///
/// When DSK data selection is unprioritized, data from competing
/// segments are combined. For example, if two competing segments
/// both represent a surface as sets of triangular plates, the
/// union of those sets of plates is considered to represent the
/// surface.
///
/// Currently only unprioritized data selection is supported.
/// Because prioritized data selection may be the default behavior
/// in a later version of the routine, the UNPRIORITIZED keyword is
/// required in the METHOD argument.
///
///
/// Syntax of the METHOD input argument
/// -----------------------------------
///
/// The keywords and surface list in the METHOD argument
/// are called "clauses." The clauses may appear in any
/// order, for example
///
/// DSK/<surface list>/UNPRIORITIZED
/// DSK/UNPRIORITIZED/<surface list>
/// UNPRIORITIZED/<surface list>/DSK
///
/// The simplest form of the METHOD argument specifying use of
/// DSK data is one that lacks a surface list, for example:
///
/// 'DSK/UNPRIORITIZED'
///
/// For applications in which all loaded DSK data for the target
/// body are for a single surface, and there are no competing
/// segments, the above string suffices. This is expected to be
/// the usual case.
///
/// When, for the specified target body, there are loaded DSK
/// files providing data for multiple surfaces for that body, the
/// surfaces to be used by this routine for a given call must be
/// specified in a surface list, unless data from all of the
/// surfaces are to be used together.
///
/// The surface list consists of the string
///
/// SURFACES =
///
/// followed by a comma-separated list of one or more surface
/// identifiers. The identifiers may be names or integer codes in
/// string format. For example, suppose we have the surface
/// names and corresponding ID codes shown below:
///
/// Surface Name ID code
/// ------------ -------
/// 'Mars MEGDR 128 PIXEL/DEG' 1
/// 'Mars MEGDR 64 PIXEL/DEG' 2
/// 'Mars_MRO_HIRISE' 3
///
/// If data for all of the above surfaces are loaded, then
/// data for surface 1 can be specified by either
///
/// 'SURFACES = 1'
///
/// or
///
/// 'SURFACES = "Mars MEGDR 128 PIXEL/DEG"'
///
/// Double quotes are used to delimit the surface name because
/// it contains blank characters.
///
/// To use data for surfaces 2 and 3 together, any
/// of the following surface lists could be used:
///
/// 'SURFACES = 2, 3'
///
/// 'SURFACES = "Mars MEGDR 64 PIXEL/DEG", 3'
///
/// 'SURFACES = 2, Mars_MRO_HIRISE'
///
/// 'SURFACES = "Mars MEGDR 64 PIXEL/DEG", Mars_MRO_HIRISE'
///
/// An example of a METHOD argument that could be constructed
/// using one of the surface lists above is
///
/// 'DSK/UNPRIORITIZED/SURFACES = "Mars MEGDR 64 PIXEL/DEG", 3'
///
///
/// Round-off errors and mitigating algorithms
/// ------------------------------------------
///
/// When topographic data are used to represent the surface of a
/// target body, round-off errors can produce some results that
/// may seem surprising.
///
/// Note that, since the surface in question might have mountains,
/// valleys, and cliffs, the points of intersection found for
/// nearly identical sets of inputs may be quite far apart from
/// each other: for example, a ray that hits a mountain side in a
/// nearly tangent fashion may, on a different host computer, be
/// found to miss the mountain and hit a valley floor much farther
/// from the observer, or even miss the target altogether.
///
/// Round-off errors can affect segment selection: for example, a
/// ray that is expected to intersect the target body's surface
/// near the boundary between two segments might hit either
/// segment, or neither of them; the result may be
/// platform-dependent.
///
/// A similar situation exists when a surface is modeled by a set
/// of triangular plates, and the ray is expected to intersect the
/// surface near a plate boundary.
///
/// To avoid having the routine fail to find an intersection when
/// one clearly should exist, this routine uses two "greedy"
/// algorithms:
///
/// 1) If the ray passes sufficiently close to any of the
/// boundary surfaces of a segment (for example, surfaces of
/// maximum and minimum longitude or latitude), that segment
/// is tested for an intersection of the ray with the
/// surface represented by the segment's data.
///
/// This choice prevents all of the segments from being
/// missed when at least one should be hit, but it could, on
/// rare occasions, cause an intersection to be found in a
/// segment other than the one that would be found if higher
/// precision arithmetic were used.
///
/// 2) For type 2 segments, which represent surfaces as
/// sets of triangular plates, each plate is expanded very
/// slightly before a ray-plate intersection test is
/// performed. The default plate expansion factor is
///
/// 1 + 1.E-10
///
/// In other words, the sides of the plate are lengthened by
/// 1/10 of a micron per km. The expansion keeps the centroid
/// of the plate fixed.
///
/// Plate expansion prevents all plates from being missed
/// in cases where clearly at least one should be hit.
///
/// As with the greedy segment selection algorithm, plate
/// expansion can occasionally cause an intercept to be
/// found on a different plate than would be found if higher
/// precision arithmetic were used. It also can occasionally
/// cause an intersection to be found when the ray misses
/// the target by a very small distance.
///
///
/// Aberration corrections
/// ----------------------
///
/// For irregularly shaped target bodies, the distance between the
/// observer and the nearest surface intercept need not be a
/// continuous function of time; hence the one-way light time
/// between the intercept and the observer may be discontinuous as
/// well. In such cases, the computed light time, which is found
/// using an iterative algorithm, may converge slowly or not at
/// all. In all cases, the light time computation will terminate,
/// but the result may be less accurate than expected.
/// ```
///
/// # 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) The following program computes surface intercept points on Mars
/// for the boresight and FOV boundary vectors of the MGS MOC
/// narrow angle camera. The intercepts are computed for a single
/// observation epoch. Light time and stellar aberration
/// corrections are used. For simplicity, camera distortion is
/// ignored.
///
/// Intercepts are computed using both triaxial ellipsoid and
/// topographic surface models.
///
/// The topographic model is based on data from the MGS MOLA DEM
/// megr90n000cb, which has a resolution of 4 pixels/degree. A
/// triangular plate model was produced by computing a 720 x 1440
/// grid of interpolated heights from this DEM, then tessellating
/// the height grid. The plate model is stored in a type 2 segment
/// in the referenced DSK file.
///
/// Use the meta-kernel shown below to load the required SPICE
/// kernels.
///
///
/// KPL/MK
///
/// File: sincpt_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
/// --------- --------
/// de430.bsp Planetary ephemeris
/// mar097.bsp Mars satellite ephemeris
/// pck00010.tpc Planet orientation and
/// radii
/// naif0011.tls Leapseconds
/// mgs_moc_v20.ti MGS MOC instrument
/// parameters
/// mgs_sclkscet_00061.tsc MGS SCLK coefficients
/// mgs_sc_ext12.bc MGS s/c bus attitude
/// mgs_ext12_ipng_mgs95j.bsp MGS ephemeris
/// megr90n000cb_plate.bds Plate model based on
/// MEGDR DEM, resolution
/// 4 pixels/degree.
///
/// \begindata
///
/// KERNELS_TO_LOAD = ( 'de430.bsp',
/// 'mar097.bsp',
/// 'pck00010.tpc',
/// 'naif0011.tls',
/// 'mgs_moc_v20.ti',
/// 'mgs_sclkscet_00061.tsc',
/// 'mgs_sc_ext12.bc',
/// 'mgs_ext12_ipng_mgs95j.bsp',
/// 'megr90n000cb_plate.bds' )
/// \begintext
///
/// End of meta-kernel
///
///
/// Example code begins here.
///
///
/// PROGRAM SINCPT_EX1
/// IMPLICIT NONE
/// C
/// C SPICELIB functions
/// C
/// DOUBLE PRECISION VNORM
///
/// C
/// C Local parameters
/// C
/// CHARACTER*(*) META
/// PARAMETER ( META = 'sincpt_ex1.tm' )
///
/// INTEGER ABCLEN
/// PARAMETER ( ABCLEN = 20 )
///
/// INTEGER LNSIZE
/// PARAMETER ( LNSIZE = 78 )
///
/// INTEGER METLEN
/// PARAMETER ( METLEN = 40 )
///
/// INTEGER NAMLEN
/// PARAMETER ( NAMLEN = 32 )
///
/// INTEGER TIMLEN
/// PARAMETER ( TIMLEN = 50 )
///
/// INTEGER SHPLEN
/// PARAMETER ( SHPLEN = 80 )
///
/// INTEGER NCORNR
/// PARAMETER ( NCORNR = 4 )
///
/// INTEGER NMETH
/// PARAMETER ( NMETH = 2 )
///
/// C
/// C Local variables
/// C
/// CHARACTER*(ABCLEN) ABCORR
/// CHARACTER*(NAMLEN) CAMERA
/// CHARACTER*(NAMLEN) DREF
/// CHARACTER*(NAMLEN) FIXREF
/// CHARACTER*(METLEN) METHDS ( NMETH )
/// CHARACTER*(METLEN) METHOD
/// CHARACTER*(NAMLEN) OBSRVR
/// CHARACTER*(SHPLEN) SHAPE
/// CHARACTER*(NAMLEN) SRFTYP ( NMETH )
/// CHARACTER*(NAMLEN) TARGET
/// CHARACTER*(LNSIZE) TITLE
/// CHARACTER*(TIMLEN) UTC
///
/// DOUBLE PRECISION BOUNDS ( 3, NCORNR )
/// DOUBLE PRECISION BSIGHT ( 3 )
/// DOUBLE PRECISION DIST
/// DOUBLE PRECISION DPR
/// DOUBLE PRECISION DVEC ( 3 )
/// DOUBLE PRECISION ET
/// DOUBLE PRECISION LAT
/// DOUBLE PRECISION LON
/// DOUBLE PRECISION RADIUS
/// DOUBLE PRECISION SPOINT ( 3 )
/// DOUBLE PRECISION SRFVEC ( 3 )
/// DOUBLE PRECISION TRGEPC
///
/// INTEGER CAMID
/// INTEGER I
/// INTEGER J
/// INTEGER K
/// INTEGER N
///
/// LOGICAL FOUND
///
/// DATA ABCORR / 'CN+S' /
/// DATA CAMERA / 'MGS_MOC_NA' /
/// DATA FIXREF / 'IAU_MARS' /
/// DATA METHDS / 'ELLIPSOID',
/// . 'DSK/UNPRIORITIZED' /
/// DATA OBSRVR / 'MGS' /
/// DATA SRFTYP / 'Ellipsoid',
/// . 'MGS/MOLA topography, 4 pixel/deg' /
/// DATA TARGET / 'Mars' /
/// DATA UTC /
/// . '2003 OCT 13 06:00:00 UTC' /
///
/// C
/// C Load kernel files:
/// C
/// CALL FURNSH ( META )
///
/// C
/// C Convert the UTC request time to ET (seconds past
/// C J2000, TDB).
/// C
/// CALL STR2ET ( UTC, ET )
///
/// C
/// C Get the MGS MOC Narrow angle camera (MGS_MOC_NA)
/// C ID code. Then look up the field of view (FOV)
/// C parameters by calling GETFOV.
/// C
/// CALL BODN2C ( CAMERA, CAMID, FOUND )
///
/// IF ( .NOT. FOUND ) THEN
/// CALL SETMSG ( 'Could not find ID code for ' //
/// . 'instrument #.' )
/// CALL ERRCH ( '#', CAMERA )
/// CALL SIGERR ( 'SPICE(NOTRANSLATION)' )
/// END IF
///
/// C
/// C GETFOV will return the name of the camera-fixed frame
/// C in the string DREF, the camera boresight vector in
/// C the array BSIGHT, and the FOV corner vectors in the
/// C array BOUNDS.
/// C
/// CALL GETFOV ( CAMID, NCORNR, SHAPE, DREF,
/// . BSIGHT, N, BOUNDS )
///
///
/// WRITE (*,*) ' '
/// WRITE (*,*) 'Surface Intercept Locations for Camera'
/// WRITE (*,*) 'FOV Boundary and Boresight Vectors'
/// WRITE (*,*) ' '
/// WRITE (*,*) ' Instrument: ', CAMERA
/// WRITE (*,*) ' Epoch: ', UTC
/// WRITE (*,*) ' Aberration correction: ', ABCORR
///
/// C
/// C Now compute and display the surface intercepts for the
/// C boresight and all of the FOV boundary vectors.
/// C
/// DO I = 1, NCORNR+1
///
/// IF ( I .LE. NCORNR ) THEN
///
/// TITLE = 'Corner vector #'
/// CALL REPMI ( TITLE, '#', I, TITLE )
///
/// CALL VEQU ( BOUNDS(1,I), DVEC )
///
/// ELSE
///
/// TITLE = 'Boresight vector'
/// CALL VEQU ( BSIGHT, DVEC )
///
/// END IF
///
/// WRITE (*,*) ' '
/// WRITE (*,*) TITLE
///
/// TITLE = ' Vector in # frame = '
/// CALL REPMC ( TITLE, '#', DREF, TITLE )
///
/// WRITE (*,*) ' '
/// WRITE (*,*) TITLE
///
/// IF ( I .LE. NCORNR ) THEN
/// WRITE (*, '(1X,3F20.14)') ( BOUNDS(J,I), J=1,3 )
/// ELSE
/// WRITE (*, '(1X,3F20.14)') BSIGHT
/// END IF
///
/// WRITE (*,*) ' '
/// WRITE (*,*) ' Intercept:'
///
/// C
/// C Compute the surface intercept point using
/// C the specified aberration corrections. Loop
/// C over the set of computation methods.
/// C
/// DO K = 1, NMETH
///
/// METHOD = METHDS(K)
///
/// CALL SINCPT ( METHOD, TARGET, ET,
/// . FIXREF, ABCORR, OBSRVR,
/// . DREF, DVEC, SPOINT,
/// . TRGEPC, SRFVEC, FOUND )
///
/// IF ( FOUND ) THEN
/// C
/// C Compute range from observer to apparent
/// C intercept.
/// C
/// DIST = VNORM ( SRFVEC )
/// C
/// C Convert rectangular coordinates to
/// C planetocentric latitude and longitude.
/// C Convert radians to degrees.
/// C
/// CALL RECLAT ( SPOINT, RADIUS, LON, LAT )
///
/// LON = LON * DPR ()
/// LAT = LAT * DPR ()
/// C
/// C Display the results.
/// C
///
/// WRITE (*,*) ' '
/// CALL TOSTDO ( ' Surface representation: '
/// . // SRFTYP(K) )
/// WRITE (*,*) ' '
/// WRITE (*,*)
/// . ' Radius (km) = ', RADIUS
/// WRITE (*,*)
/// . ' Planetocentric Latitude (deg) = ', LAT
/// WRITE (*,*)
/// . ' Planetocentric Longitude (deg) = ', LON
/// WRITE (*,*)
/// . ' Range (km) = ', DIST
///
/// ELSE
///
/// CALL TOSTDO ( ' Surface representation: '
/// . // SRFTYP(K) )
/// WRITE (*,*) ' Intercept not found.'
/// WRITE (*,*) ' '
///
/// END IF
///
/// END DO
///
/// END DO
///
/// END
///
///
/// When this program was executed on a Mac/Intel/gfortran/64-bit
/// platform, the output was:
///
///
/// Surface Intercept Locations for Camera
/// FOV Boundary and Boresight Vectors
///
/// Instrument: MGS_MOC_NA
/// Epoch: 2003 OCT 13 06:00:00 UTC
/// Aberration correction: CN+S
///
/// Corner vector 1
///
/// Vector in MGS_MOC_NA frame =
/// 0.00000185713838 -0.00380156226592 0.99999277403434
///
/// Intercept:
///
/// Surface representation: Ellipsoid
///
/// Radius (km) = 3384.9411357607282
/// Planetocentric Latitude (deg) = -48.477482367206768
/// Planetocentric Longitude (deg) = -123.47407481971256
/// Range (km) = 388.98308225698986
///
/// Surface representation: MGS/MOLA topography, 4 pixel/deg
///
/// Radius (km) = 3387.6408267726060
/// Planetocentric Latitude (deg) = -48.492259559975267
/// Planetocentric Longitude (deg) = -123.47541193495911
/// Range (km) = 386.14510040407879
///
/// Corner vector 2
///
/// Vector in MGS_MOC_NA frame =
/// 0.00000185713838 0.00380156226592 0.99999277403434
///
/// Intercept:
///
/// Surface representation: Ellipsoid
///
/// Radius (km) = 3384.9396985743224
/// Planetocentric Latitude (deg) = -48.481636778911913
/// Planetocentric Longitude (deg) = -123.39881874871132
/// Range (km) = 388.97510005267708
///
/// Surface representation: MGS/MOLA topography, 4 pixel/deg
///
/// Radius (km) = 3387.6403704507966
/// Planetocentric Latitude (deg) = -48.496386688872484
/// Planetocentric Longitude (deg) = -123.40074354811055
/// Range (km) = 386.13616443321536
///
/// Corner vector 3
///
/// Vector in MGS_MOC_NA frame =
/// -0.00000185713838 0.00380156226592 0.99999277403434
///
/// Intercept:
///
/// Surface representation: Ellipsoid
///
/// Radius (km) = 3384.9396897286833
/// Planetocentric Latitude (deg) = -48.481662348858336
/// Planetocentric Longitude (deg) = -123.39882195503854
/// Range (km) = 388.97464113550637
///
/// Surface representation: MGS/MOLA topography, 4 pixel/deg
///
/// Radius (km) = 3387.6403603146168
/// Planetocentric Latitude (deg) = -48.496412042429789
/// Planetocentric Longitude (deg) = -123.40074672915324
/// Range (km) = 386.13571069851986
///
/// Corner vector 4
///
/// Vector in MGS_MOC_NA frame =
/// -0.00000185713838 -0.00380156226592 0.99999277403434
///
/// Intercept:
///
/// Surface representation: Ellipsoid
///
/// Radius (km) = 3384.9411269137695
/// Planetocentric Latitude (deg) = -48.477507940479093
/// Planetocentric Longitude (deg) = -123.47407797517749
/// Range (km) = 388.98262331952731
///
/// Surface representation: MGS/MOLA topography, 4 pixel/deg
///
/// Radius (km) = 3387.6408166344654
/// Planetocentric Latitude (deg) = -48.492284916898356
/// Planetocentric Longitude (deg) = -123.47541506563023
/// Range (km) = 386.14464664863726
///
/// Boresight vector
///
/// Vector in MGS_MOC_NA frame =
/// 0.00000000000000 0.00000000000000 1.00000000000000
///
/// Intercept:
///
/// Surface representation: Ellipsoid
///
/// [...]
///
///
/// Warning: incomplete output. Only 100 out of 112 lines have been
/// provided.
///
///
/// 2) Use SUBPNT to find the sub-spacecraft point on Mars for the
/// Mars Reconnaissance Orbiter spacecraft (MRO) at a specified
/// time, using the "near point: ellipsoid" computation method.
/// Use both LT+S and CN+S aberration corrections to illustrate
/// the differences.
///
/// Convert the spacecraft to sub-observer point vector obtained
/// from SUBPNT into the MRO_HIRISE_LOOK_DIRECTION reference frame
/// at the observation time. Perform a consistency check with this
/// vector: compare the Mars surface intercept of the ray
/// emanating from the spacecraft and pointed along this vector
/// with the sub-observer point.
///
/// Perform the sub-observer point and surface intercept
/// computations using both triaxial ellipsoid and topographic
/// surface models.
///
/// For this example, the topographic model is based on the MGS
/// MOLA DEM megr90n000eb, which has a resolution of 16
/// pixels/degree. Eight DSKs, each covering longitude and
/// latitude ranges of 90 degrees, were made from this data set.
/// For the region covered by a given DSK, a grid of approximately
/// 1500 x 1500 interpolated heights was produced, and this grid
/// was tessellated using approximately 4.5 million triangular
/// plates, giving a total plate count of about 36 million for the
/// entire DSK set.
///
/// All DSKs in the set use the surface ID code 499001, so there
/// is no need to specify the surface ID in the METHOD strings
/// passed to SINCPT and SUBPNT.
///
/// Use the meta-kernel shown below to load the required SPICE
/// kernels.
///
///
/// KPL/MK
///
/// File: sincpt_ex2.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
/// --------- --------
/// de430.bsp Planetary ephemeris
/// mar097.bsp Mars satellite ephemeris
/// pck00010.tpc Planet orientation and
/// radii
/// naif0011.tls Leapseconds
/// mro_psp4_ssd_mro95a.bsp MRO ephemeris
/// mro_v11.tf MRO frame specifications
/// mro_sclkscet_00022_65536.tsc MRO SCLK coefficients
/// parameters
/// mro_sc_psp_070925_071001.bc MRO attitude
/// megr90n000eb_*_plate.bds Plate model DSKs based
/// on MEGDR DEM, resolution
/// 16 pixels/degree.
///
/// \begindata
///
/// KERNELS_TO_LOAD = (
///
/// 'de430.bsp',
/// 'mar097.bsp',
/// 'pck00010.tpc',
/// 'naif0011.tls',
/// 'mro_psp4_ssd_mro95a.bsp',
/// 'mro_v11.tf',
/// 'mro_sclkscet_00022_65536.tsc',
/// 'mro_sc_psp_070925_071001.bc',
/// 'megr90n000eb_LL000E00N_UR090E90N_plate.bds'
/// 'megr90n000eb_LL000E90S_UR090E00S_plate.bds'
/// 'megr90n000eb_LL090E00N_UR180E90N_plate.bds'
/// 'megr90n000eb_LL090E90S_UR180E00S_plate.bds'
/// 'megr90n000eb_LL180E00N_UR270E90N_plate.bds'
/// 'megr90n000eb_LL180E90S_UR270E00S_plate.bds'
/// 'megr90n000eb_LL270E00N_UR360E90N_plate.bds'
/// 'megr90n000eb_LL270E90S_UR360E00S_plate.bds' )
///
/// \begintext
///
/// End of meta-kernel
///
///
/// Example code begins here.
///
///
/// PROGRAM SINCPT_EX2
/// IMPLICIT NONE
/// C
/// C SPICELIB functions
/// C
/// DOUBLE PRECISION DPR
/// DOUBLE PRECISION VDIST
/// DOUBLE PRECISION VNORM
///
/// C
/// C Local parameters
/// C
/// CHARACTER*(*) META
/// PARAMETER ( META = 'sincpt_ex2.tm' )
///
/// CHARACTER*(*) F1
/// PARAMETER ( F1 = '(A,F21.9)' )
///
/// CHARACTER*(*) F2
/// PARAMETER ( F2 = '(A)' )
///
/// INTEGER FRNMLN
/// PARAMETER ( FRNMLN = 32 )
///
/// INTEGER MTHLEN
/// PARAMETER ( MTHLEN = 50 )
///
/// INTEGER CORLEN
/// PARAMETER ( CORLEN = 5 )
///
/// INTEGER NCORR
/// PARAMETER ( NCORR = 2 )
///
/// INTEGER NMETH
/// PARAMETER ( NMETH = 2 )
///
/// C
/// C Local variables
/// C
/// CHARACTER*(CORLEN) ABCORR ( NCORR )
/// CHARACTER*(FRNMLN) FIXREF
/// CHARACTER*(FRNMLN) HIREF
/// CHARACTER*(MTHLEN) SINMTH ( NMETH )
/// CHARACTER*(MTHLEN) SUBMTH ( NMETH )
///
/// DOUBLE PRECISION ALT
/// DOUBLE PRECISION ET
/// DOUBLE PRECISION LAT
/// DOUBLE PRECISION LON
/// DOUBLE PRECISION MROVEC ( 3 )
/// DOUBLE PRECISION RADIUS
/// DOUBLE PRECISION SPOINT ( 3 )
/// DOUBLE PRECISION SRFVEC ( 3 )
/// DOUBLE PRECISION TRGEPC
/// DOUBLE PRECISION XFORM ( 3, 3 )
/// DOUBLE PRECISION XEPOCH
/// DOUBLE PRECISION XPOINT ( 3 )
/// DOUBLE PRECISION XVEC ( 3 )
///
/// INTEGER I
/// INTEGER J
///
/// LOGICAL FOUND
///
/// C
/// C Initial values
/// C
/// DATA ABCORR / 'LT+S', 'CN+S' /
/// DATA FIXREF / 'IAU_MARS' /
/// DATA SINMTH / 'Ellipsoid',
/// . 'DSK/Unprioritized' /
/// DATA SUBMTH / 'Ellipsoid/Near point',
/// . 'DSK/Unprioritized/Nadir' /
///
/// C
/// C Load kernel files via the meta-kernel.
/// C
/// CALL FURNSH ( META )
///
/// C
/// C Convert the TDB request time string to seconds past
/// C J2000, TDB.
/// C
/// CALL STR2ET ( '2007 SEP 30 00:00:00 TDB', ET )
///
/// C
/// C Compute the sub-spacecraft point using the
/// C "NEAR POINT: ELLIPSOID" definition.
/// C Compute the results using both LT+S and CN+S
/// C aberration corrections.
/// C
/// C Repeat the computation for each method.
/// C
/// C
/// DO I = 1, NMETH
///
/// WRITE(*,F2) ' '
/// WRITE(*,F2) 'Sub-observer point computation method = '
/// . // SUBMTH(I)
///
/// DO J = 1, NCORR
///
/// CALL SUBPNT ( SUBMTH(I),
/// . 'Mars', ET, FIXREF, ABCORR(J),
/// . 'MRO', SPOINT, TRGEPC, SRFVEC )
/// C
/// C Compute the observer's altitude above SPOINT.
/// C
/// ALT = VNORM ( SRFVEC )
/// C
/// C Express SRFVEC in the MRO_HIRISE_LOOK_DIRECTION
/// C reference frame at epoch ET. Since SRFVEC is
/// C expressed relative to the IAU_MARS frame at
/// C TRGEPC, we must call PXFRM2 to compute the position
/// C transformation matrix from IAU_MARS at TRGEPC to
/// C the MRO_HIRISE_LOOK_DIRECTION frame at time ET.
/// C
/// C To make code formatting a little easier, we'll
/// C store the long MRO reference frame name in a
/// C variable:
/// C
/// HIREF = 'MRO_HIRISE_LOOK_DIRECTION'
///
/// CALL PXFRM2 ( FIXREF, HIREF, TRGEPC, ET, XFORM )
/// CALL MXV ( XFORM, SRFVEC, MROVEC )
///
/// C
/// C Convert rectangular coordinates to planetocentric
/// C latitude and longitude. Convert radians to degrees.
/// C
/// CALL RECLAT ( SPOINT, RADIUS, LON, LAT )
///
/// LON = LON * DPR ()
/// LAT = LAT * DPR ()
/// C
/// C Write the results.
/// C
/// WRITE(*,F2) ' '
/// WRITE(*,F2) ' Aberration correction = '
/// . // ABCORR(J)
/// WRITE(*,F1) ' '
/// WRITE(*,F2) ' MRO-to-sub-observer vector in'
/// WRITE(*,F2) ' MRO HIRISE look direction frame'
/// WRITE(*,F1) ' X-component '
/// . // '(km) = ', MROVEC(1)
/// WRITE(*,F1) ' Y-component '
/// . // '(km) = ', MROVEC(2)
/// WRITE(*,F1) ' Z-component '
/// . // '(km) = ', MROVEC(3)
/// WRITE(*,F1) ' Sub-observer point radius '
/// . // '(km) = ', RADIUS
/// WRITE(*,F1) ' Planetocentric latitude '
/// . // '(deg) = ', LAT
/// WRITE(*,F1) ' Planetocentric longitude '
/// . // '(deg) = ', LON
/// WRITE(*,F1) ' Observer altitude '
/// . // '(km) = ', ALT
///
/// C
/// C Consistency check: find the surface intercept on
/// C Mars of the ray emanating from the spacecraft and
/// C having direction vector MROVEC in the MRO HIRISE
/// C reference frame at ET. Call the intercept point
/// C XPOINT. XPOINT should coincide with SPOINT, up to
/// C a small round-off error.
/// C
/// CALL SINCPT ( SINMTH(I), 'Mars', ET, FIXREF,
/// . ABCORR(J), 'MRO', HIREF, MROVEC,
/// . XPOINT, XEPOCH, XVEC, FOUND )
///
/// IF ( .NOT. FOUND ) THEN
/// WRITE (*,F1) 'Bug: no intercept'
/// ELSE
/// C
/// C Report the distance between XPOINT and SPOINT.
/// C
/// WRITE (*,* ) ' '
/// WRITE (*,F1) ' Intercept comparison '
/// . // 'error (km) = ',
/// . VDIST( XPOINT, SPOINT )
/// END IF
///
/// END DO
///
/// END DO
///
/// END
///
///
/// When this program was executed on a Mac/Intel/gfortran/64-bit
/// platform, the output was:
///
///
/// Sub-observer point computation method = Ellipsoid/Near point
///
/// Aberration correction = LT+S
///
/// MRO-to-sub-observer vector in
/// MRO HIRISE look direction frame
/// X-component (km) = 0.286933229
/// Y-component (km) = -0.260425939
/// Z-component (km) = 253.816326385
/// Sub-observer point radius (km) = 3388.299078378
/// Planetocentric latitude (deg) = -38.799836378
/// Planetocentric longitude (deg) = -114.995297227
/// Observer altitude (km) = 253.816622175
///
/// Intercept comparison error (km) = 0.000002144
///
/// Aberration correction = CN+S
///
/// MRO-to-sub-observer vector in
/// MRO HIRISE look direction frame
/// X-component (km) = 0.286933107
/// Y-component (km) = -0.260426683
/// Z-component (km) = 253.816315915
/// Sub-observer point radius (km) = 3388.299078376
/// Planetocentric latitude (deg) = -38.799836382
/// Planetocentric longitude (deg) = -114.995297449
/// Observer altitude (km) = 253.816611705
///
/// Intercept comparison error (km) = 0.000000001
///
/// Sub-observer point computation method = DSK/Unprioritized/Nadir
///
/// Aberration correction = LT+S
///
/// MRO-to-sub-observer vector in
/// MRO HIRISE look direction frame
/// X-component (km) = 0.282372596
/// Y-component (km) = -0.256289313
/// Z-component (km) = 249.784871247
/// Sub-observer point radius (km) = 3392.330239436
/// Planetocentric latitude (deg) = -38.800230156
/// Planetocentric longitude (deg) = -114.995297338
/// Observer altitude (km) = 249.785162334
///
/// Intercept comparison error (km) = 0.000002412
///
/// Aberration correction = CN+S
///
/// MRO-to-sub-observer vector in
/// MRO HIRISE look direction frame
/// X-component (km) = 0.282372464
/// Y-component (km) = -0.256290075
/// Z-component (km) = 249.784860121
/// Sub-observer point radius (km) = 3392.330239564
/// Planetocentric latitude (deg) = -38.800230162
/// Planetocentric longitude (deg) = -114.995297569
/// Observer altitude (km) = 249.785151209
///
/// Intercept comparison error (km) = 0.000000001
/// ```
///
/// # Restrictions
///
/// ```text
/// 1) A cautionary note: if aberration corrections are used, and
/// if DREF is the target body-fixed frame, the epoch at which
/// that frame is evaluated is offset from ET by the light time
/// between the observer and the *center* of the target body.
/// This light time normally will differ from the light time
/// between the observer and intercept point. Consequently the
/// orientation of the target body-fixed frame at TRGEPC will
/// not match that of the target body-fixed frame at the epoch
/// associated with DREF. As a result, various derived quantities
/// may not be as expected: for example, SRFVEC would not be
/// parallel to DVEC.
///
/// In many applications the errors arising from this frame
/// discrepancy may be insignificant; however a safe approach is
/// to always use as DREF a frame other than the target
/// body-fixed frame.
///
/// 2) This routine must not be used for cases where the observer
/// is inside the target body. This routine does not attempt to
/// detect this condition.
///
/// If the observer is a point on a target surface described
/// by DSK data, care must be taken to ensure the observer is
/// sufficiently far outside the target. The routine should
/// not be used for surfaces for which "outside" cannot be
/// defined.
/// ```
///
/// # Author and Institution
///
/// ```text
/// N.J. Bachman (JPL)
/// J. Diaz del Rio (ODC Space)
/// S.C. Krening (JPL)
/// B.V. Semenov (JPL)
/// E.D. Wright (JPL)
/// ```
///
/// # Version
///
/// ```text
/// - SPICELIB Version 3.1.0, 26-OCT-2021 (JDR) (NJB)
///
/// Bug fix: PRVCOR is no longer set to blank before
/// ABCORR is parsed.
///
/// ZZVALCOR is now used instead of ZZPRSCOR. This provides
/// better error handling.
///
/// Edits to $Examples section to comply with NAIF standard.
///
/// The header's $Detailed_Input and $Restrictions sections
/// were updated to state that the observer must be
/// outside the target body.
///
/// - SPICELIB Version 3.0.0, 04-APR-2017 (NJB)
///
/// 01-FEB-2016 (NJB)
///
/// Upgraded to support surfaces represented by DSKs.
///
/// Updated kernels are used in header example programs.
///
/// - SPICELIB Version 2.0.0, 31-MAR-2014 (NJB) (SCK) (BVS)
///
/// Bug fix: FIRST is now set to .FALSE. at the completion
/// of a successful initialization pass. This does not affect
/// the routine's outputs but improves efficiency.
///
/// Bug fix: redundant call to SPKSSB was removed. This does not
/// affect the routine's outputs but improves efficiency.
///
/// References to the new PXFRM2 routine were added, which changed
/// the Detailed Output section and the second example. Some header
/// comment corrections were made.
///
/// Upgrade: this routine now uses ZZVALCOR rather than
/// ZZPRSCOR, simplifying the implementation.
///
/// Upgrade: this routine now saves the input body names and
/// ZZBODTRN state counters and does name-ID conversions only if
/// the counters have changed.
///
/// Upgrade: this routine now saves the input frame names and POOL
/// state counters and does frame name-ID conversions only if the
/// counters have changed.
///
/// - SPICELIB Version 1.2.0, 07-APR-2010 (NJB)
///
/// Code style improvement: re-use of variables in
/// FRINFO calls has been eliminated. There is no impact
/// of the behavior of the routine.
///
/// - SPICELIB Version 1.1.0, 17-MAR-2009 (NJB) (EDW)
///
/// Bug fix: quick test for non-intersection is
/// no longer performed when observer-target distance
/// is less than target's maximum radius.
///
/// Typos in the Detailed Input section's description of DREF
/// were corrected.
///
/// In the header examples, meta-kernel names were updated to use
/// the suffix
///
/// ".tm"
///
/// Incorrect frame name FIXFRM was changed to FIXREF in
/// documentation.
///
/// Typo correction in $Required_Reading, changed FRAME
/// to FRAMES.
///
/// - SPICELIB Version 1.0.0, 02-MAR-2008 (NJB)
/// ```
///
/// # Revisions
///
/// ```text
/// - SPICELIB Version 3.0.0, 04-APR-2017 (NJB)
///
/// Upgraded to support surfaces represented by DSKs.
///
/// The routine was re-written so as to use a private
/// routine to implement the intersection algorithm.
/// That routine has been generalized so that it does
/// not depend on the target surface representation: it
/// uses callback routines to compute ray-surface intercepts
/// for a specified ray and time, the surface tangency point
/// for a given ray, and the radius of an outer bounding
/// sphere for the target.
/// ```
//$Procedure SINCPT ( Surface intercept )