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//
// GENERATED FILE
//
use *;
use crateSpiceContext;
use *;
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 NEVFLG: i32 = 3;
const EVLFLN: i32 = 25;
const EVLOBS: i32 = 1;
const EVLTRG: i32 = 2;
const EVLCTR: i32 = 3;
const MAXL: i32 = 36;
const FRNMLN: i32 = 32;
/// SPK, constant velocity observer state
///
/// Return the state of a specified target relative to an "observer,"
/// where the observer has constant velocity in a specified reference
/// frame. The observer's state is provided by the calling program
/// rather than by loaded SPK files.
///
/// # Required Reading
///
/// * [FRAMES](crate::required_reading::frames)
/// * [PCK](crate::required_reading::pck)
/// * [SPK](crate::required_reading::spk)
/// * [TIME](crate::required_reading::time)
///
/// # Brief I/O
///
/// ```text
/// VARIABLE I/O DESCRIPTION
/// -------- --- --------------------------------------------------
/// TARGET I Name of target ephemeris object.
/// ET I Observation epoch.
/// OUTREF I Reference frame of output state.
/// REFLOC I Output reference frame evaluation locus.
/// ABCORR I Aberration correction.
/// OBSSTA I Observer state relative to center of motion.
/// OBSEPC I Epoch of observer state.
/// OBSCTR I Center of motion of observer.
/// OBSREF I Frame of observer state.
/// STATE O State of target with respect to observer.
/// LT O One way light time between target and
/// observer.
/// ```
///
/// # Detailed Input
///
/// ```text
/// TARGET is the name of a target 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 target
/// is Earth.
///
/// Case and leading and trailing blanks are not
/// significant in the string TARGET.
///
///
/// ET is the ephemeris time at which the state of the
/// target relative to the observer is to be computed. ET
/// is expressed as seconds past J2000 TDB. ET refers to
/// time at the observer's location.
///
/// ET is independent of the observer epoch OBSEPC.
///
///
/// OUTREF is the name of the reference frame with respect to
/// which the output state is expressed.
///
/// When OUTREF is time-dependent (non-inertial), its
/// orientation relative to the J2000 frame is evaluated
/// in the manner commanded by the input argument REFLOC
/// (see description below).
///
/// Case and leading and trailing blanks are not
/// significant in the string OUTREF.
///
///
/// REFLOC is a string indicating the output reference frame
/// evaluation locus: this is the location associated
/// with the epoch at which this routine is to evaluate
/// the orientation, relative to the J2000 frame, of the
/// output frame OUTREF. The values and meanings of
/// REFLOC are:
///
/// 'OBSERVER' Evaluate OUTREF at the observer's
/// epoch ET.
///
/// Normally the locus 'OBSERVER' should
/// be selected when OUTREF is centered
/// at the observer.
///
///
/// 'TARGET' Evaluate OUTREF at the target epoch;
/// letting LT be the one-way light time
/// between the target and observer, the
/// target epoch is
///
/// ET-LT if reception aberration
/// corrections are used
///
/// ET+LT if transmission aberration
/// corrections are used
///
/// ET if no aberration corrections
/// are used
///
/// Normally the locus 'TARGET' should
/// be selected when OUTREF is centered
/// at the target object.
///
///
/// 'CENTER' Evaluate the frame OUTREF at the epoch
/// associated its center. This epoch,
/// which we'll call ETCTR, is determined
/// as follows:
///
/// Let LTCTR be the one-way light time
/// between the observer and the center
/// of OUTREF. Then ETCTR is
///
/// ET-LTCTR if reception
/// aberration corrections
/// are used
///
/// ET+LTCTR if transmission
/// aberration corrections
/// are used
///
/// ET if no aberration
/// corrections are used
///
///
/// The locus 'CENTER' should be selected
/// when the user intends to obtain
/// results compatible with those produced
/// by SPKEZR.
///
/// When OUTREF is inertial, all choices of REFLOC
/// yield the same results.
///
/// Case and leading and trailing blanks are not
/// significant in the string REFLOC.
///
///
/// ABCORR indicates the aberration corrections to be applied to
/// the observer-target state to account for one-way
/// light time and stellar aberration.
///
/// ABCORR may be any of the following:
///
/// 'NONE' Apply no correction. Return the
/// geometric state of the target
/// relative to the observer.
///
/// The following values of ABCORR apply to the
/// "reception" case in which photons depart from the
/// target'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 state of the target 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.
///
/// 'LT+S' Correct for one-way light time and
/// stellar aberration using a Newtonian
/// formulation. This option modifies the
/// state obtained with the 'LT' option to
/// account for the observer's velocity
/// relative to the solar system
/// barycenter. The result is the apparent
/// state of the target---the position and
/// velocity of the target as seen by the
/// observer.
///
/// 'CN' Converged Newtonian light time
/// correction. In solving the light time
/// equation, the 'CN' correction iterates
/// until the solution converges.
///
/// 'CN+S' Converged Newtonian light time
/// and stellar aberration corrections.
///
///
/// 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
/// target's location 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
/// state of the target at the moment it
/// receives photons emitted from the
/// observer's location at ET.
///
/// 'XLT+S' "Transmission" case: correct for
/// one-way light time and stellar
/// aberration using a Newtonian
/// formulation This option modifies the
/// state obtained with the 'XLT' option to
/// account for the observer's velocity
/// relative to the solar system
/// barycenter. The position component of
/// the computed target state indicates the
/// direction that photons emitted from the
/// observer's location must be "aimed" to
/// hit the target.
///
/// 'XCN' "Transmission" case: converged
/// Newtonian light time correction.
///
/// 'XCN+S' "Transmission" case: converged
/// Newtonian light time and stellar
/// aberration corrections.
///
///
/// Neither special nor general relativistic effects are
/// accounted for in the aberration corrections applied
/// by this routine.
///
/// Case and leading and trailing blanks are not
/// significant in the string ABCORR.
///
///
/// OBSSTA is the geometric state of an observer moving at
/// constant velocity relative to its center of motion
/// OBSCTR, expressed in the reference frame OBSREF, at
/// the epoch OBSEPC.
///
/// OBSSTA is a six-dimensional vector representing
/// position and velocity in cartesian coordinates: the
/// first three components represent the position of an
/// observer relative to its center of motion; the last
/// three components represent the velocity of the
/// observer.
///
/// Units are always km and km/sec.
///
///
/// OBSEPC is the epoch, expressed as seconds past J2000 TDB, at
/// which the observer state OBSSTA is applicable. For
/// other epochs, the position of the observer relative
/// to its center of motion is linearly extrapolated
/// using the velocity component of OBSSTA.
///
/// OBSEPC is independent of the epoch ET at which the
/// state of the target relative to the observer is to be
/// computed.
///
/// OBSCTR is the name of the center of motion of OBSSTA. The
/// ephemeris of OBSCTR is provided by loaded SPK files.
///
/// 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 center of motion.
///
/// Case and leading and trailing blanks are not
/// significant in the string OBSCTR.
///
///
/// OBSREF is the name of the reference frame relative to which
/// the input state OBSSTA is expressed. The observer has
/// constant velocity relative to its center of motion
/// in this reference frame.
///
/// Case and leading and trailing blanks are not
/// significant in the string OBSREF.
/// ```
///
/// # Detailed Output
///
/// ```text
/// STATE is a Cartesian state vector representing the position
/// and velocity of the target relative to the specified
/// observer. STATE is corrected for the specified
/// aberrations and is expressed with respect to the
/// reference frame specified by OUTREF. The first three
/// components of STATE represent the x-, y- and
/// z-components of the target's position; the last three
/// components form the corresponding velocity vector.
///
/// The position component of STATE points from the
/// observer's location at ET to the aberration-corrected
/// location of the target. Note that the sense of the
/// position vector is independent of the direction of
/// radiation travel implied by the aberration
/// correction.
///
/// The velocity component of STATE is the derivative
/// with respect to time of the position component of
/// STATE.
///
/// Units are always km and km/sec.
///
/// When STATE is expressed in a time-dependent
/// (non-inertial) output frame, the orientation of that
/// frame relative to the J2000 frame is evaluated in the
/// manner indicated by the input argument REFLOC (see
/// description above).
///
///
/// LT is the one-way light time between the observer and
/// target in seconds. If the target state is corrected
/// for aberrations, then LT is the one-way light time
/// between the observer and the light time corrected
/// target location.
/// ```
///
/// # Exceptions
///
/// ```text
/// 1) If either the name of the center of motion or the target
/// cannot be translated to its NAIF ID code, the error
/// SPICE(IDCODENOTFOUND) is signaled.
///
/// 2) If the reference frame OUTREF is unrecognized, the error
/// SPICE(UNKNOWNFRAME) is signaled.
///
/// 3) If the reference frame OBSREF is unrecognized, an error is
/// signaled by a routine in the call tree of this routine.
///
/// 4) If the frame evaluation locus REFLOC is not recognized,
/// the error SPICE(NOTSUPPORTED) is signaled.
///
/// 5) If the loaded kernels provide insufficient data to compute
/// the requested state vector, an error is signaled
/// by a routine in the call tree of this routine.
///
/// 6) If an error occurs while reading an SPK or other kernel file,
/// the error is signaled by a routine in the call tree of
/// this routine.
///
/// 7) If the aberration correction ABCORR is not recognized, 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 the observer center and target
/// must be loaded. If aberration corrections are used, the
/// states of observer center and target 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 using FURNSH.
///
/// The following data may be required:
///
/// - PCK data: if the target frame is a PCK frame, rotation data
/// for the target frame must be loaded. These may be provided
/// in a text or binary PCK file.
///
/// - Frame data: if a frame definition not built into SPICE is
/// required, for example to convert the observer-target state
/// to the output frame, that definition must be available in
/// the kernel pool. Typically frame definitions are supplied
/// by loading a frame kernel using FURNSH.
///
/// - Additional kernels: if any frame used in this routine's
/// state computation is a CK frame, then at least one CK and
/// corresponding SCLK kernel is required. If dynamic frames
/// are used, additional SPK, PCK, CK, or SCLK kernels may be
/// required.
///
/// In all cases, kernel data are normally loaded once per program
/// run, NOT every time this routine is called.
/// ```
///
/// # Particulars
///
/// ```text
/// This routine computes observer-target states for observers whose
/// trajectories are not provided by SPK files.
///
/// Observers supported by this routine must have constant velocity
/// with respect to a specified center of motion, expressed in a
/// caller-specified reference frame. The state of the center of
/// motion relative to the target must be computable using
/// loaded SPK data.
///
/// For applications in which the observer has zero velocity
/// relative to its center of motion, the SPICELIB routine
///
/// SPKCPO { SPK, constant position observer }
///
/// can be used. SPKCPO has a simpler interface than that of SPKCVO.
///
/// This routine is suitable for computing states of target ephemeris
/// objects, as seen from landmarks on the surface of an extended
/// object, in cases where no SPK data are available for those
/// landmarks.
///
/// This routine's treatment of the output reference frame differs
/// from that of the principal SPK API routines
///
/// SPKEZR
/// SPKEZ
/// SPKPOS
/// SPKEZP
///
/// which require both observer and target ephemerides to be provided
/// by loaded SPK files:
///
/// The SPK API routines listed above evaluate the orientation of
/// the output reference frame (with respect to the J2000 frame)
/// at an epoch corrected for one-way light time between the
/// observer and the center of the output frame. When the center
/// of the output frame is not the target (for example, when the
/// target is on the surface of Mars and the output frame is
/// centered at Mars' center), the epoch of evaluation may not
/// closely match the light-time corrected epoch associated with
/// the target itself. A similar problem may occur when the
/// observer is a surface point on an extended body and the
/// output frame is centered at the body center: the listed
/// routines will correct the orientation of the output frame for
/// one-way light time between the frame center and the observer.
///
/// This routine allows the caller to dictate how the orientation
/// of the output reference frame is to be evaluated. The caller
/// passes to this routine an input string called the output
/// frame's evaluation "locus." This string specifies the location
/// associated with the output frame's evaluation epoch. The three
/// possible values of the locus are
///
/// 'TARGET'
/// 'OBSERVER'
/// 'CENTER'
///
/// The choice of locus has an effect when aberration corrections
/// are used and the output frame is non-inertial.
///
/// When the locus is 'TARGET' and light time corrections are
/// used, the orientation of the output frame is evaluated at the
/// epoch obtained by correcting the observation epoch ET for
/// one-way light time LT. The evaluation epoch will be either
/// ET-LT or ET+LT for reception or transmission corrections
/// respectively.
///
/// For remote sensing applications where the target is a surface
/// point on an extended object, and the orientation of that
/// object should be evaluated at the emission time, the locus
/// 'TARGET' should be used.
///
/// When the output frame's orientation should be evaluated at
/// the observation epoch ET, which is the case when the
/// output frame is centered at the observer, the locus
/// 'OBSERVER' should be used.
///
/// The locus option 'CENTER' is provided for compatibility
/// with existing SPK state computation APIs such as SPKEZR.
///
/// Note that the output frame evaluation locus does not affect
/// the computation of light time between the target and
/// observer.
///
///
/// The SPK routines that compute observer-target states for
/// combinations of objects having ephemerides provided by the SPK
/// system and objects having constant position or constant velocity
/// are
///
/// SPKCPO {SPK, Constant position observer}
/// SPKCPT {SPK, Constant position target}
/// SPKCVO {SPK, Constant velocity observer}
/// SPKCVT {SPK, Constant velocity target}
/// ```
///
/// # 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) Compute apparent solar azimuth and elevation as seen from a
/// specified surface point on the earth.
///
/// Task Description
/// ================
///
/// In this example we'll use the location of the DSN station
/// DSS-14 as our surface point.
///
/// We'll perform the solar azimuth and elevation computation two
/// ways:
///
/// - Using a station frame kernel to provide the
/// specification of a topocentric reference frame
/// centered at DSS-14.
///
/// - Computing inline the transformation from the earth-fixed,
/// earth-centered frame ITRF93 to a topocentric frame
/// centered at DSS-14.
///
/// Note that results of the two computations will differ
/// slightly. This is due to differences in the orientations
/// of the topocentric frames. There are two sources of the
/// differences:
///
/// 1) The station position is time-dependent due to tectonic
/// plate motion, and epochs of the station positions used
/// to specify the axes of the topocentric frame are
/// different in the two cases. This gives rise to different
/// orientations of the frame's axes relative to the frame
/// ITRF93.
///
/// 2) The two computations use different earth radii; this
/// results in computation of different geodetic latitudes
/// of the station. This difference also affects the
/// topocentric frame orientation relative to ITRF93.
///
///
/// Kernels
/// =======
///
/// Use the meta-kernel shown below to load the required SPICE
/// kernels.
///
///
/// KPL/MK
///
/// File name: spkcvo_ex1.tm
///
/// This is the meta-kernel file for the header code example for
/// the subroutine SPKCVO. These kernel files can be found on
/// the NAIF website.
///
/// 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
/// pck00010.tpc Planet orientation and
/// radii
/// naif0010.tls Leapseconds
/// earth_720101_070426.bpc Earth historical
/// binary PCK
/// earthstns_itrf93_050714.bsp DSN station SPK
/// earth_topo_050714.tf DSN station FK
/// 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
///
/// \begindata
///
/// KERNELS_TO_LOAD = ( 'de421.bsp',
/// 'pck00010.tpc',
/// 'naif0010.tls',
/// 'earth_720101_070426.bpc',
/// 'earthstns_itrf93_050714.bsp',
/// 'earth_topo_050714.tf',
/// 'mgs_moc_v20.ti',
/// 'mgs_sclkscet_00061.tsc',
/// 'mgs_sc_ext12.bc',
/// 'mgs_ext12_ipng_mgs95j.bsp' )
///
/// \begintext
///
/// End of meta-kernel.
///
///
/// Example code begins here.
///
///
/// C
/// C This program uses SPKCVO to compute solar azimuth
/// C and elevation at a given surface point on the earth:
/// C the DSN station DSS-14.
/// C
///
/// PROGRAM SPKCVO_EX1
/// IMPLICIT NONE
/// C
/// C SPICELIB functions
/// C
/// DOUBLE PRECISION DPR
/// DOUBLE PRECISION VDIST
///
/// C
/// C Local parameters
/// C
/// CHARACTER*(*) FMT0
/// PARAMETER ( FMT0 = '(A,3F20.8)' )
///
/// CHARACTER*(*) FMT1
/// PARAMETER ( FMT1 = '(1X,A, F20.8)' )
///
/// CHARACTER*(*) META
/// PARAMETER ( META = 'spkcvo_ex1.tm' )
///
/// CHARACTER*(*) TIMFMT
/// PARAMETER ( TIMFMT =
/// . 'YYYY MON DD HR:MN:SC.###### UTC' )
///
/// CHARACTER*(*) TIMFM2
/// PARAMETER ( TIMFM2 =
/// . 'YYYY MON DD HR:MN:SC.###### TDB ::TDB' )
///
/// INTEGER BDNMLN
/// PARAMETER ( BDNMLN = 36 )
///
/// INTEGER CORLEN
/// PARAMETER ( CORLEN = 10 )
///
/// INTEGER EVLLEN
/// PARAMETER ( EVLLEN = 25 )
///
/// INTEGER FRNMLN
/// PARAMETER ( FRNMLN = 32 )
///
/// INTEGER TIMLEN
/// PARAMETER ( TIMLEN = 40 )
///
/// C
/// C Local variables
/// C
/// CHARACTER*(CORLEN) ABCORR
/// CHARACTER*(TIMLEN) EMITIM
/// CHARACTER*(TIMLEN) EPCSTR
/// CHARACTER*(EVLLEN) REFLOC
/// CHARACTER*(BDNMLN) OBSCTR
/// CHARACTER*(FRNMLN) OBSREF
/// CHARACTER*(TIMLEN) OBSTIM
/// CHARACTER*(FRNMLN) OUTREF
/// CHARACTER*(BDNMLN) TARGET
///
/// DOUBLE PRECISION AZ
/// DOUBLE PRECISION EL
/// DOUBLE PRECISION ET
/// DOUBLE PRECISION F
/// DOUBLE PRECISION LAT
/// DOUBLE PRECISION LON
/// DOUBLE PRECISION LT0
/// DOUBLE PRECISION LT1
/// DOUBLE PRECISION NORMAL ( 3 )
/// DOUBLE PRECISION OBSALT
/// DOUBLE PRECISION OBSEPC
/// DOUBLE PRECISION OBSLAT
/// DOUBLE PRECISION OBSLON
/// DOUBLE PRECISION OBSSTA ( 6 )
/// DOUBLE PRECISION R
/// DOUBLE PRECISION RADII ( 3 )
/// DOUBLE PRECISION RE
/// DOUBLE PRECISION RP
/// DOUBLE PRECISION STATE0 ( 6 )
/// DOUBLE PRECISION STATE1 ( 6 )
/// DOUBLE PRECISION TOPVEC ( 3 )
/// DOUBLE PRECISION XFORM ( 3, 3 )
/// DOUBLE PRECISION Z ( 3 )
///
/// INTEGER I
/// INTEGER N
///
/// C
/// C Initial values
/// C
/// DATA Z / 0.D0, 0.D0, 1.D0 /
///
///
/// C
/// C Load SPICE kernels.
/// C
/// CALL FURNSH ( META )
///
/// C
/// C Convert the observation time to seconds past J2000 TDB.
/// C
/// OBSTIM = '2003 OCT 13 06:00:00.000000 UTC'
///
/// CALL STR2ET ( OBSTIM, ET )
///
/// C
/// C Set the target, observer center, observer frame, and
/// C observer state relative to its center.
/// C
/// TARGET = 'SUN'
/// OBSCTR = 'EARTH'
/// OBSREF = 'ITRF93'
///
/// C
/// C Set the state of DSS-14 relative to the earth's
/// C center at the J2000 epoch, expressed in the
/// C ITRF93 reference frame. Values come from the
/// C earth station SPK specified in the meta-kernel.
/// C
/// C The velocity is non-zero due to tectonic
/// C plate motion.
/// C
/// OBSEPC = 0.D0
///
/// OBSSTA(1) = -2353.6213656676991D0
/// OBSSTA(2) = -4641.3414911499403D0
/// OBSSTA(3) = 3677.0523293197439D0
/// OBSSTA(4) = -0.00000000000057086D0
/// OBSSTA(5) = 0.00000000000020549D0
/// OBSSTA(6) = -0.00000000000012171D0
///
/// C
/// C Find the apparent state of the sun relative
/// C to the station in the DSS-14_TOPO reference frame.
/// C Evaluate the output frame's orientation, that is the
/// C orientation of the DSS-14_TOPO frame relative to the
/// C J2000 frame, at the observation epoch. This
/// C correction is obtained by setting REFLOC to
/// C 'OBSERVER'.
/// C
/// OUTREF = 'DSS-14_TOPO'
/// ABCORR = 'CN+S'
///
/// REFLOC = 'OBSERVER'
///
/// C
/// C Compute the observer-target state.
/// C
/// CALL SPKCVO ( TARGET, ET, OUTREF, REFLOC,
/// . ABCORR, OBSSTA, OBSEPC, OBSCTR,
/// . OBSREF, STATE0, LT0 )
///
/// C
/// C Compute planetocentric coordinates of the
/// C observer-target position in the local
/// C topocentric reference frame DSS-14_TOPO.
/// C
/// CALL RECLAT ( STATE0, R, LON, LAT )
///
/// C
/// C Compute solar azimuth. The latitude we've
/// C already computed is the elevation. Express
/// C both angles in degrees.
/// C
/// EL = LAT * DPR()
/// AZ = - LON * DPR()
///
/// IF ( AZ .LT. 0.D0 ) THEN
/// AZ = AZ + 360.D0
/// END IF
///
/// C
/// C Display the computed state, light time, and
/// C angles.
/// C
/// CALL TIMOUT ( ET-LT0, TIMFMT, EMITIM )
/// CALL TIMOUT ( OBSEPC, TIMFM2, EPCSTR )
///
/// WRITE (*,*) ' '
/// WRITE (*,*) 'Frame evaluation locus: ', REFLOC
/// WRITE (*,*) ' '
/// WRITE (*,*) 'Target: ', TARGET
/// WRITE (*,*) 'Observation time: ', OBSTIM
/// WRITE (*,*) 'Observer center: ', OBSCTR
/// WRITE (*,*) 'Observer-center state time: ', EPCSTR
/// WRITE (*,*) 'Observer frame: ', OBSREF
/// WRITE (*,*) 'Emission time: ', EMITIM
/// WRITE (*,*) 'Output reference frame: ', OUTREF
/// WRITE (*,*) 'Aberration correction: ', ABCORR
/// WRITE (*,*) ' '
/// WRITE (*,*) 'Observer-target position (km): '
/// WRITE (*,FMT0) ' ', ( STATE0(I), I = 1, 3 )
/// WRITE (*,*) 'Observer-target velocity (km/s): '
/// WRITE (*,FMT0) ' ', ( STATE0(I), I = 4, 6 )
/// WRITE (*,FMT1) 'Light time (s): ', LT0
/// WRITE (*,*) ' '
/// WRITE (*,FMT1) 'Solar azimuth (deg): ', AZ
/// WRITE (*,FMT1) 'Solar elevation (deg): ', EL
/// WRITE (*,*) ' '
///
/// C
/// C For an arbitrary surface point, we might not
/// C have a frame kernel available. In this case
/// C we can look up the state in the observer frame
/// C using SPKCVO and then convert the state to
/// C the local topocentric frame. We'll first
/// C create the transformation matrix for converting
/// C vectors in the observer frame to the topocentric
/// C frame.
/// C
/// C First step: find the geodetic (planetodetic)
/// C coordinates of the observer. We need the
/// C equatorial radius and flattening coefficient
/// C of the reference ellipsoid.
/// C
/// CALL BODVRD ( 'EARTH', 'RADII', 3, N, RADII )
///
/// RE = RADII(1)
/// RP = RADII(3)
///
/// F = ( RE - RP ) / RE
///
/// CALL RECGEO ( OBSSTA, RE, F, OBSLON, OBSLAT, OBSALT )
///
/// C
/// C Find the outward surface normal on the reference
/// C ellipsoid at the observer's longitude and latitude.
/// C
/// CALL LATREC ( 1.D0, OBSLON, OBSLAT, NORMAL )
///
/// C
/// C The topocentric frame has its +Z axis aligned
/// C with NORMAL and its +X axis pointed north.
/// C The north direction is aligned with the component
/// C of the ITRF93 +Z axis orthogonal to the topocentric
/// C +Z axis.
/// C
/// CALL TWOVEC ( NORMAL, 3, Z, 1, XFORM )
///
/// OUTREF = 'ITRF93'
/// ABCORR = 'CN+S'
///
/// REFLOC = 'OBSERVER'
///
/// C
/// C Compute the observer-target state.
/// C
/// CALL SPKCVO ( TARGET, ET, OUTREF, REFLOC,
/// . ABCORR, OBSSTA, OBSEPC, OBSCTR,
/// . OBSREF, STATE1, LT1 )
///
/// C
/// C Convert the position to the topocentric frame.
/// C
/// CALL MXV ( XFORM, STATE1, TOPVEC )
///
/// C
/// C Compute azimuth and elevation.
/// C
/// CALL RECLAT ( TOPVEC, R, LON, LAT )
///
/// EL = LAT * DPR()
/// AZ = - LON * DPR()
///
/// IF ( AZ .LT. 0.D0 ) THEN
/// AZ = AZ + 360.D0
/// END IF
///
/// WRITE (*,*) ' '
/// WRITE (*,*) ' '
/// WRITE (*,*) 'AZ/EL computed without frame kernel: '
/// WRITE (*,*) ' '
/// WRITE (*,FMT1) 'Distance between last two '
/// .// 'positions (km): ',
/// . VDIST ( STATE0, TOPVEC )
/// WRITE (*,*) ' '
/// WRITE (*,FMT1) 'Solar azimuth (deg): ', AZ
/// WRITE (*,FMT1) 'Solar elevation (deg): ', EL
/// WRITE (*,*) ' '
///
/// END
///
///
/// When this program was executed on a Mac/Intel/gfortran/64-bit
/// platform, the output was:
///
///
/// Frame evaluation locus: OBSERVER
///
/// Target: SUN
/// Observation time: 2003 OCT 13 06:00:00.000000 UTC
/// Observer center: EARTH
/// Observer-center state time: 2000 JAN 01 12:00:00.000000 TDB
/// Observer frame: ITRF93
/// Emission time: 2003 OCT 13 05:51:42.068322 UTC
/// Output reference frame: DSS-14_TOPO
/// Aberration correction: CN+S
///
/// Observer-target position (km):
/// 62512272.82076502 58967494.42506485 -122059095.46751761
/// Observer-target velocity (km/s):
/// 2475.97326517 -9870.26706232 -3499.90809969
/// Light time (s): 497.93167797
///
/// Solar azimuth (deg): 316.67141599
/// Solar elevation (deg): -54.85253168
///
///
///
/// AZ/EL computed without frame kernel:
///
/// Distance between last two positions (km): 3.07056969
///
/// Solar azimuth (deg): 316.67141786
/// Solar elevation (deg): -54.85253216
///
///
/// 2) Demonstrate applications of the output frame evaluation locus.
///
/// The following program is not necessarily realistic: for
/// brevity, it combines several unrelated computations.
///
/// Task Description
/// ================
///
/// Find the state of the Mars Global Surveyor spacecraft, as seen
/// from a given surface point on earth, corrected for light time
/// and stellar aberration, expressed in the earth fixed reference
/// frame ITRF93. The surface point is the position of the DSN
/// station DSS-14.
///
/// Contrast the states computed by setting the output frame
/// evaluation locus to 'OBSERVER' and to 'CENTER'. Show that the
/// latter choice produces results very close to those that
/// can be obtained using SPKEZR.
///
/// Also compute the central meridian longitude on Mars of DSS-14.
/// This computation performs aberration corrections for the center
/// of Mars.
///
/// Note that in general, the routine SUBPNT should be used for
/// sub-observer point computations when high-accuracy aberration
/// corrections are desired.
///
/// The observation epoch is 2003 OCT 13 06:00:00 UTC.
///
///
/// Kernels
/// =======
///
/// Use the meta-kernel of example 1 above.
///
///
/// Example code begins here.
///
///
/// C
/// C This program demonstrates the use of SPKCVO.
/// C Computations are performed using all three possible
/// C values of the output frame evaluation locus REFLOC:
/// C
/// C 'OBSERVER'
/// C 'CENTER'
/// C 'TARGET'
/// C
/// C Several unrelated computations are performed in
/// C this program. In particular, computation of the
/// C central meridian longitude on Mars is included
/// C simply to demonstrate use of the 'TARGET' option.
/// C
///
/// PROGRAM SPKCVO_EX2
/// IMPLICIT NONE
/// C
/// C SPICELIB functions
/// C
/// DOUBLE PRECISION DPR
/// DOUBLE PRECISION VDIST
///
/// C
/// C Local parameters
/// C
/// CHARACTER*(*) FMT0
/// PARAMETER ( FMT0 = '(A,3F20.8)' )
///
/// CHARACTER*(*) FMT1
/// PARAMETER ( FMT1 = '(1X,A, F20.8)' )
///
/// CHARACTER*(*) META
/// PARAMETER ( META = 'spkcvo_ex1.tm' )
///
/// CHARACTER*(*) TIMFMT
/// PARAMETER ( TIMFMT =
/// . 'YYYY MON DD HR:MN:SC.###### UTC' )
///
/// CHARACTER*(*) TIMFM2
/// PARAMETER ( TIMFM2 =
/// . 'YYYY MON DD HR:MN:SC.###### TDB ::TDB' )
///
///
/// INTEGER BDNMLN
/// PARAMETER ( BDNMLN = 36 )
///
/// INTEGER CORLEN
/// PARAMETER ( CORLEN = 10 )
///
/// INTEGER LOCLEN
/// PARAMETER ( LOCLEN = 25 )
///
/// INTEGER FRNMLN
/// PARAMETER ( FRNMLN = 32 )
///
/// INTEGER TIMLEN
/// PARAMETER ( TIMLEN = 40 )
///
/// C
/// C Local variables
/// C
/// CHARACTER*(CORLEN) ABCORR
/// CHARACTER*(TIMLEN) EMITIM
/// CHARACTER*(TIMLEN) EPCSTR
/// CHARACTER*(LOCLEN) REFLOC
/// CHARACTER*(BDNMLN) OBSRVR
/// CHARACTER*(TIMLEN) OBSTIM
/// CHARACTER*(FRNMLN) OUTREF
/// CHARACTER*(BDNMLN) TARGET
/// CHARACTER*(BDNMLN) OBSCTR
/// CHARACTER*(FRNMLN) OBSREF
///
/// DOUBLE PRECISION ET
/// DOUBLE PRECISION LAT
/// DOUBLE PRECISION LON
/// DOUBLE PRECISION LT0
/// DOUBLE PRECISION LT1
/// DOUBLE PRECISION LT2
/// DOUBLE PRECISION LT3
/// DOUBLE PRECISION R
/// DOUBLE PRECISION STATE0 ( 6 )
/// DOUBLE PRECISION STATE1 ( 6 )
/// DOUBLE PRECISION STATE2 ( 6 )
/// DOUBLE PRECISION STATE3 ( 6 )
/// DOUBLE PRECISION OBSEPC
/// DOUBLE PRECISION OBSSTA ( 6 )
/// DOUBLE PRECISION OBSVEC ( 3 )
///
/// INTEGER I
///
/// C
/// C Load SPICE kernels.
/// C
/// CALL FURNSH ( META )
///
/// C
/// C Convert the observation time to seconds past J2000 TDB.
/// C
/// OBSTIM = '2003 OCT 13 06:00:00.000000 UTC'
///
/// CALL STR2ET ( OBSTIM, ET )
///
/// C
/// C Set the target, observer center, observer frame, and
/// C observer state relative to its center.
/// C
/// TARGET = 'MGS'
/// OBSCTR = 'EARTH'
/// OBSREF = 'ITRF93'
///
/// C
/// C Set the state of DSS-14 relative to the earth's
/// C center at the J2000 epoch, expressed in the
/// C ITRF93 reference frame. Values come from the
/// C earth station SPK specified in the meta-kernel.
/// C
/// C The velocity is non-zero due to tectonic
/// C plate motion.
/// C
/// OBSEPC = 0.D0
///
/// OBSSTA(1) = -2353.6213656676991D0
/// OBSSTA(2) = -4641.3414911499403D0
/// OBSSTA(3) = 3677.0523293197439D0
/// OBSSTA(4) = -0.00000000000057086D0
/// OBSSTA(5) = 0.00000000000020549D0
/// OBSSTA(6) = -0.00000000000012171D0
///
/// C
/// C Find the apparent state of the spacecraft relative
/// C to the station in the ITRF93 reference frame.
/// C Evaluate the earth's orientation, that is the
/// C orientation of the ITRF93 frame relative to the
/// C J2000 frame, at the observation epoch. This
/// C correction is obtained by setting REFLOC to
/// C 'OBSERVER'.
/// C
/// OUTREF = 'ITRF93'
/// ABCORR = 'CN+S'
///
/// REFLOC = 'OBSERVER'
///
/// C
/// C Compute the observer-target state.
/// C
/// CALL SPKCVO ( TARGET, ET, OUTREF, REFLOC,
/// . ABCORR, OBSSTA, OBSEPC, OBSCTR,
/// . OBSREF, STATE0, LT0 )
///
/// C
/// C Display the computed state and light time.
/// C
/// CALL TIMOUT ( ET-LT0, TIMFMT, EMITIM )
/// CALL TIMOUT ( OBSEPC, TIMFM2, EPCSTR )
///
/// WRITE (*,*) ' '
/// WRITE (*,*) 'Frame evaluation locus: ', REFLOC
/// WRITE (*,*) ' '
/// WRITE (*,*) 'Target: ', TARGET
/// WRITE (*,*) 'Observation time: ', OBSTIM
/// WRITE (*,*) 'Observer center: ', OBSCTR
/// WRITE (*,*) 'Observer-center state time: ', EPCSTR
/// WRITE (*,*) 'Observer frame: ', OBSREF
/// WRITE (*,*) 'Emission time: ', EMITIM
/// WRITE (*,*) 'Output reference frame: ', OUTREF
/// WRITE (*,*) 'Aberration correction: ', ABCORR
/// WRITE (*,*) ' '
/// WRITE (*,*) 'Observer-target position (km): '
/// WRITE (*,FMT0) ' ', ( STATE0(I), I = 1, 3 )
/// WRITE (*,*) 'Observer-target velocity (km/s): '
/// WRITE (*,FMT0) ' ', ( STATE0(I), I = 4, 6 )
/// WRITE (*,FMT1) 'Light time (s): ', LT0
/// WRITE (*,*) ' '
///
/// C
/// C Repeat the computation, this time evaluating the
/// C earth's orientation at the epoch obtained by
/// C subtracting from the observation time the one way
/// C light time from the earth's center.
/// C
/// C This is equivalent to looking up the observer-target
/// C state using SPKEZR.
/// C
/// REFLOC = 'CENTER'
///
/// CALL SPKCVO ( TARGET, ET, OUTREF, REFLOC,
/// . ABCORR, OBSSTA, OBSEPC, OBSCTR,
/// . OBSREF, STATE1, LT1 )
///
/// C
/// C Display the computed state and light time.
/// C
/// CALL TIMOUT ( ET-LT1, TIMFMT, EMITIM )
///
/// WRITE (*,*) ' '
/// WRITE (*,*) 'Frame evaluation locus: ', REFLOC
/// WRITE (*,*) ' '
/// WRITE (*,*) 'Target: ', TARGET
/// WRITE (*,*) 'Observation time: ', OBSTIM
/// WRITE (*,*) 'Observer center: ', OBSCTR
/// WRITE (*,*) 'Observer-center state time: ', EPCSTR
/// WRITE (*,*) 'Observer frame: ', OBSREF
/// WRITE (*,*) 'Emission time: ', EMITIM
/// WRITE (*,*) 'Output reference frame: ', OUTREF
/// WRITE (*,*) 'Aberration correction: ', ABCORR
/// WRITE (*,*) ' '
/// WRITE (*,*) 'Observer-target position (km): '
/// WRITE (*,FMT0) ' ', ( STATE1(I), I = 1, 3 )
/// WRITE (*,*) 'Observer-target velocity (km/s): '
/// WRITE (*,FMT0) ' ', ( STATE1(I), I = 4, 6 )
/// WRITE (*,FMT1) 'Light time (s): ', LT1
/// WRITE (*,*) ' '
///
/// WRITE (*,FMT1) 'Distance between above positions '
/// .// '(km): ', VDIST( STATE0, STATE1 )
/// WRITE (*,FMT1) 'Velocity difference magnitude '
/// .// ' (km/s): ',
/// . VDIST( STATE0(4), STATE1(4) )
///
/// C
/// C Check: compare the state computed directly above
/// C to one produced by SPKEZR.
/// C
/// OBSRVR = 'DSS-14'
///
/// CALL SPKEZR ( TARGET, ET, OUTREF, ABCORR,
/// . OBSRVR, STATE2, LT2 )
///
/// WRITE (*,*) ' '
/// WRITE (*,*) ' '
/// WRITE (*,*) 'State computed using SPKEZR: '
/// WRITE (*,*) ' '
/// WRITE (*,*) 'Target: ', TARGET
/// WRITE (*,*) 'Observation time: ', OBSTIM
/// WRITE (*,*) 'Output reference frame: ', OUTREF
/// WRITE (*,*) 'Aberration correction: ', ABCORR
/// WRITE (*,*) 'Observer: ', OBSRVR
/// WRITE (*,*) ' '
/// WRITE (*,*) 'Observer-target position (km): '
/// WRITE (*,FMT0) ' ', ( STATE2(I), I = 1, 3 )
/// WRITE (*,*) 'Observer-target velocity (km/s): '
/// WRITE (*,FMT0) ' ', ( STATE2(I), I = 4, 6 )
/// WRITE (*,FMT1) 'Light time (s): ', LT2
/// WRITE (*,*) ' '
///
/// WRITE (*,FMT1) 'Distance between last two '
/// .// 'positions (km): ',
/// . VDIST ( STATE1, STATE2 )
/// WRITE (*,FMT1) 'Velocity difference magnitude '
/// .// ' (km/s): ',
/// . VDIST( STATE1(4), STATE2(4) )
///
/// C
/// C Finally, compute an observer-target state in
/// C a frame centered at the target. This state
/// C can be used to compute the central meridian longitude.
/// C The reference frame is the Mars-fixed frame IAU_MARS.
/// C
/// TARGET = 'MARS'
/// OUTREF = 'IAU_MARS'
///
/// REFLOC = 'TARGET'
///
/// CALL SPKCVO ( TARGET, ET, OUTREF, REFLOC,
/// . ABCORR, OBSSTA, OBSEPC, OBSCTR,
/// . OBSREF, STATE3, LT3 )
///
/// C
/// C Central meridian longitude is the longitude of the
/// C observer relative to the target center, so we must
/// C negate the position portion of the state we just
/// C computed.
/// C
/// CALL VMINUS ( STATE3, OBSVEC )
///
/// CALL RECLAT ( OBSVEC, R, LON, LAT )
///
/// WRITE (*,*) ' '
/// WRITE (*,*) ' '
/// WRITE (*,*) 'Frame evaluation locus: ', REFLOC
/// WRITE (*,*) ' '
/// WRITE (*,*) 'Target: ', TARGET
/// WRITE (*,*) 'Observation time: ', OBSTIM
/// WRITE (*,*) 'Observer center: ', OBSCTR
/// WRITE (*,*) 'Observer-center state time: ', EPCSTR
/// WRITE (*,*) 'Observer frame: ', OBSREF
/// WRITE (*,*) 'Emission time: ', EMITIM
/// WRITE (*,*) 'Output reference frame: ', OUTREF
/// WRITE (*,*) 'Aberration correction: ', ABCORR
/// WRITE (*,*) ' '
/// WRITE (*,*) 'Observer-target position (km): '
/// WRITE (*,FMT0) ' ', ( STATE3(I), I = 1, 3 )
/// WRITE (*,*) 'Observer-target velocity (km/s): '
/// WRITE (*,FMT0) ' ', ( STATE3(I), I = 4, 6 )
/// WRITE (*,FMT1) 'Light time (s): ', LT3
/// WRITE (*,*) ' '
/// WRITE (*,*) 'Central meridian '
/// WRITE (*,FMT1) 'longitude (deg): ', LON*DPR()
/// WRITE (*,*) ' '
/// END
///
///
/// When this program was executed on a Mac/Intel/gfortran/64-bit
/// platform, the output was:
///
///
/// Frame evaluation locus: OBSERVER
///
/// Target: MGS
/// Observation time: 2003 OCT 13 06:00:00.000000 UTC
/// Observer center: EARTH
/// Observer-center state time: 2000 JAN 01 12:00:00.000000 TDB
/// Observer frame: ITRF93
/// Emission time: 2003 OCT 13 05:55:44.201144 UTC
/// Output reference frame: ITRF93
/// Aberration correction: CN+S
///
/// Observer-target position (km):
/// -53720675.37940782 -51381249.05338467 -18838416.34716543
/// Observer-target velocity (km/s):
/// -3751.69274754 3911.73417167 -2.17503628
/// Light time (s): 255.79885530
///
///
/// Frame evaluation locus: CENTER
///
/// Target: MGS
/// Observation time: 2003 OCT 13 06:00:00.000000 UTC
/// Observer center: EARTH
/// Observer-center state time: 2000 JAN 01 12:00:00.000000 TDB
/// Observer frame: ITRF93
/// Emission time: 2003 OCT 13 05:55:44.201144 UTC
/// Output reference frame: ITRF93
/// Aberration correction: CN+S
///
/// Observer-target position (km):
/// -53720595.74378239 -51381332.31467460 -18838416.34737090
/// Observer-target velocity (km/s):
/// -3751.69880992 3911.72835653 -2.17503628
/// Light time (s): 255.79885530
///
/// Distance between above positions (km): 115.21404098
/// Velocity difference magnitude (km/s): 0.00840050
///
///
/// State computed using SPKEZR:
///
/// Target: MGS
/// Observation time: 2003 OCT 13 06:00:00.000000 UTC
/// Output reference frame: ITRF93
/// Aberration correction: CN+S
/// Observer: DSS-14
///
/// Observer-target position (km):
/// -53720595.74378239 -51381332.31467460 -18838416.34737090
/// Observer-target velocity (km/s):
/// -3751.69880992 3911.72835653 -2.17503628
/// Light time (s): 255.79885530
///
/// Distance between last two positions (km): 0.00000000
/// Velocity difference magnitude (km/s): 0.00000000
///
///
/// Frame evaluation locus: TARGET
///
/// Target: MARS
/// Observation time: 2003 OCT 13 06:00:00.000000 UTC
/// Observer center: EARTH
/// Observer-center state time: 2000 JAN 01 12:00:00.000000 TDB
/// Observer frame: ITRF93
/// Emission time: 2003 OCT 13 05:55:44.201144 UTC
/// Output reference frame: IAU_MARS
/// Aberration correction: CN+S
///
/// Observer-target position (km):
/// -71445232.12767358 2312773.74168720 27766441.52046534
/// Observer-target velocity (km/s):
/// 155.65895286 5061.78618477 5.09447029
/// Light time (s): 255.79702283
///
/// Central meridian
/// longitude (deg): -1.85409037
/// ```
///
/// # Restrictions
///
/// ```text
/// 1) This routine may not be suitable for work with stars or other
/// objects having large distances from the observer, due to loss
/// of precision in position vectors.
/// ```
///
/// # Author and Institution
///
/// ```text
/// N.J. Bachman (JPL)
/// J. Diaz del Rio (ODC Space)
/// S.C. Krening (JPL)
/// B.V. Semenov (JPL)
/// ```
///
/// # Version
///
/// ```text
/// - SPICELIB Version 1.0.1, 25-MAY-2021 (JDR)
///
/// Edited the header to comply with NAIF standard.
///
/// Modified code examples output format for the solutions to fit
/// within the $Examples section without modifications.
///
/// - SPICELIB Version 1.0.0, 31-MAR-2014 (NJB) (SCK) (BVS)
/// ```
//$Procedure SPKCVO ( SPK, constant velocity observer state )