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//
// GENERATED FILE
//
use super::*;
use crate::SpiceContext;
use f2rust_std::*;
/// Unit Normalized Cross Product and Derivative
///
/// Compute the unit vector parallel to the cross product of
/// two 3-dimensional vectors and the derivative of this unit vector.
///
/// # Brief I/O
///
/// ```text
/// VARIABLE I/O DESCRIPTION
/// -------- --- --------------------------------------------------
/// S1 I Left hand state for cross product and derivative.
/// S2 I Right hand state for cross product and derivative.
/// SOUT O Unit vector and derivative of the cross product.
/// ```
///
/// # Detailed Input
///
/// ```text
/// S1 is any state vector. Typically, this might represent the
/// apparent state of a planet or the Sun, which defines the
/// orientation of axes of some coordinate system.
///
/// S2 is any state vector.
/// ```
///
/// # Detailed Output
///
/// ```text
/// SOUT is the unit vector parallel to the cross product of the
/// position components of S1 and S2 and the derivative of
/// the unit vector.
///
/// If the cross product of the position components is
/// the zero vector, then the position component of the
/// output will be the zero vector. The velocity component
/// of the output will simply be the derivative of the
/// cross product of the position components of S1 and S2.
/// ```
///
/// # Exceptions
///
/// ```text
/// Error free.
///
/// 1) If the position components of S1 and S2 cross together to
/// give a zero vector, the position component of the output
/// will be the zero vector. The velocity component of the
/// output will simply be the derivative of the cross product
/// of the position vectors.
///
/// 2) If S1 and S2 are large in magnitude (taken together,
/// their magnitude surpasses the limit allowed by the
/// computer) then it may be possible to generate a
/// floating point overflow from an intermediate
/// computation even though the actual cross product and
/// derivative may be well within the range of double
/// precision numbers.
/// ```
///
/// # Particulars
///
/// ```text
/// DUCRSS calculates the unit vector parallel to the cross product
/// of two vectors and the derivative of that unit vector.
/// ```
///
/// # Examples
///
/// ```text
/// The numerical results shown for this example 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) One can construct non-inertial coordinate frames from apparent
/// positions of objects or defined directions. However, if one
/// wants to convert states in this non-inertial frame to states
/// in an inertial reference frame, the derivatives of the axes of
/// the non-inertial frame are required.
///
/// Define a reference frame with the apparent direction of the
/// Sun as seen from Earth as the primary axis X. Use the Earth
/// pole vector to define with the primary axis the XY plane of
/// the frame, with the primary axis Y pointing in the direction
/// of the pole.
///
/// Use the meta-kernel shown below to load the required SPICE
/// kernels.
///
///
/// KPL/MK
///
/// File name: ducrss_ex1.tm
///
/// This meta-kernel is intended to support operation of SPICE
/// example programs. The kernels shown here should not be
/// assumed to contain adequate or correct versions of data
/// required by SPICE-based user applications.
///
/// In order for an application to use this meta-kernel, the
/// kernels referenced here must be present in the user's
/// current working directory.
///
/// The names and contents of the kernels referenced
/// by this meta-kernel are as follows:
///
/// File name Contents
/// --------- --------
/// de421.bsp Planetary ephemeris
/// pck00008.tpc Planet orientation and
/// radii
/// naif0009.tls Leapseconds
///
///
/// \begindata
///
/// KERNELS_TO_LOAD = ( 'de421.bsp',
/// 'pck00008.tpc',
/// 'naif0009.tls' )
///
/// \begintext
///
/// End of meta-kernel
///
///
/// Example code begins here.
///
///
/// PROGRAM DUCRSS_EX1
/// IMPLICIT NONE
///
/// C
/// C Local variables
/// C
/// DOUBLE PRECISION ET
/// DOUBLE PRECISION LT
/// DOUBLE PRECISION STATE ( 6 )
/// DOUBLE PRECISION TRANS ( 6, 6 )
/// DOUBLE PRECISION X_NEW ( 6 )
/// DOUBLE PRECISION Y_NEW ( 6 )
/// DOUBLE PRECISION Z ( 6 )
/// DOUBLE PRECISION Z_NEW ( 6 )
/// DOUBLE PRECISION ZINERT ( 6 )
///
/// INTEGER I
///
///
/// C
/// C Define the earth body-fixed pole vector (Z). The pole
/// C has no velocity in the Earth fixed frame IAU_EARTH.
/// C
/// DATA Z / 0.D0, 0.D0, 1.D0,
/// . 0.D0, 0.D0, 0.D0 /
///
/// C
/// C Load SPK, PCK, and LSK kernels, use a meta kernel for
/// C convenience.
/// C
/// CALL FURNSH ( 'ducrss_ex1.tm' )
///
/// C
/// C Calculate the state transformation between IAU_EARTH and
/// C J2000 at an arbitrary epoch.
/// C
/// CALL STR2ET ( 'Jan 1, 2009', ET )
/// CALL SXFORM ( 'IAU_EARTH', 'J2000', ET, TRANS )
///
/// C
/// C Transform the earth pole vector from the IAU_EARTH frame
/// C to J2000.
/// C
/// CALL MXVG ( TRANS, Z, 6, 6, ZINERT )
///
/// C
/// C Calculate the apparent state of the Sun from Earth at
/// C the epoch ET in the J2000 frame.
/// C
/// CALL SPKEZR ( 'Sun', ET, 'J2000', 'LT+S',
/// . 'Earth', STATE, LT )
///
/// C
/// C Define the z axis of the new frame as the cross product
/// C between the apparent direction of the Sun and the Earth
/// C pole. Z_NEW cross X_NEW defines the Y axis of the
/// C derived frame.
/// C
/// CALL DVHAT ( STATE, X_NEW )
/// CALL DUCRSS ( STATE, ZINERT, Z_NEW )
/// CALL DUCRSS ( Z_NEW, STATE, Y_NEW )
///
/// C
/// C Display the results.
/// C
/// WRITE(*,'(A)') 'New X-axis:'
/// WRITE(*,'(A,3F16.12)') ' position:', (X_NEW(I), I=1,3)
/// WRITE(*,'(A,3F16.12)') ' velocity:', (X_NEW(I), I=4,6)
/// WRITE(*,'(A)') 'New Y-axis:'
/// WRITE(*,'(A,3F16.12)') ' position:', (Y_NEW(I), I=1,3)
/// WRITE(*,'(A,3F16.12)') ' velocity:', (Y_NEW(I), I=4,6)
/// WRITE(*,'(A)') 'New Z-axis:'
/// WRITE(*,'(A,3F16.12)') ' position:', (Z_NEW(I), I=1,3)
/// WRITE(*,'(A,3F16.12)') ' velocity:', (Z_NEW(I), I=4,6)
///
///
/// END
///
///
/// When this program was executed on a Mac/Intel/gfortran/64-bit
/// platform, the output was:
///
///
/// New X-axis:
/// position: 0.183446637633 -0.901919663328 -0.391009273602
/// velocity: 0.000000202450 0.000000034660 0.000000015033
/// New Y-axis:
/// position: 0.078846540163 -0.382978080242 0.920386339077
/// velocity: 0.000000082384 0.000000032309 0.000000006387
/// New Z-axis:
/// position: -0.979862518033 -0.199671507623 0.000857203851
/// velocity: 0.000000044531 -0.000000218531 -0.000000000036
///
///
/// Note that these vectors define the transformation between the
/// new frame and J2000 at the given ET:
///
/// .- -.
/// | : |
/// | R : 0 |
/// M = | ......:......|
/// | : |
/// | dRdt : R |
/// | : |
/// `- -'
///
/// with
///
/// DATA R / X_NEW(1:3), Y_NEW(1:3), Z_NEW(1:3) /
///
/// DATA dRdt / X_NEW(4:6), Y_NEW(4:6), Z_NEW(4:6) /
/// ```
///
/// # Restrictions
///
/// ```text
/// 1) No checking of S1 or S2 is done to prevent floating point
/// overflow. The user is required to determine that the magnitude
/// of each component of the states is within an appropriate range
/// so as not to cause floating point overflow. In almost every
/// case there will be no problem and no checking actually needs
/// to be done.
/// ```
///
/// # Author and Institution
///
/// ```text
/// N.J. Bachman (JPL)
/// J. Diaz del Rio (ODC Space)
/// W.L. Taber (JPL)
/// ```
///
/// # Version
///
/// ```text
/// - SPICELIB Version 1.3.0, 06-JUL-2021 (JDR)
///
/// Added IMPLICIT NONE statement.
///
/// Edited the header to comply with NAIF standard. Removed
/// unnecessary $Revisions section.
///
/// Added complete code example.
///
/// - SPICELIB Version 1.2.0, 08-APR-2014 (NJB)
///
/// Now scales inputs to reduce chance of numeric
/// overflow.
///
/// - SPICELIB Version 1.1.1, 22-APR-2010 (NJB)
///
/// Header correction: assertions that the output
/// can overwrite the input have been removed.
///
/// - SPICELIB Version 1.1.0, 30-AUG-2005 (NJB)
///
/// Updated to remove non-standard use of duplicate arguments
/// in DVHAT call.
///
/// - SPICELIB Version 1.0.0, 15-JUN-1995 (WLT)
/// ```
pub fn ducrss(s1: &[f64; 6], s2: &[f64; 6], sout: &mut [f64; 6]) {
DUCRSS(s1, s2, sout);
}
//$Procedure DUCRSS ( Unit Normalized Cross Product and Derivative )
pub fn DUCRSS(S1: &[f64], S2: &[f64], SOUT: &mut [f64]) {
let S1 = DummyArray::new(S1, 1..=6);
let S2 = DummyArray::new(S2, 1..=6);
let mut SOUT = DummyArrayMut::new(SOUT, 1..=6);
let mut F1: f64 = 0.0;
let mut F2: f64 = 0.0;
let mut SCLS1 = StackArray::<f64, 6>::new(1..=6);
let mut SCLS2 = StackArray::<f64, 6>::new(1..=6);
let mut TMPSTA = StackArray::<f64, 6>::new(1..=6);
//
// Local variables
//
//
// Scale the components of the input states so the states have the
// same direction and angular rates, but their largest position
// components have absolute value equal to 1. Do not modify states
// that have all position components equal to zero.
//
F1 = intrinsics::DMAX1(&[f64::abs(S1[1]), f64::abs(S1[2]), f64::abs(S1[3])]);
F2 = intrinsics::DMAX1(&[f64::abs(S2[1]), f64::abs(S2[2]), f64::abs(S2[3])]);
if (F1 > 0.0) {
VSCLG((1.0 / F1), S1.as_slice(), 6, SCLS1.as_slice_mut());
} else {
MOVED(S1.as_slice(), 6, SCLS1.as_slice_mut());
}
if (F2 > 0.0) {
VSCLG((1.0 / F2), S2.as_slice(), 6, SCLS2.as_slice_mut());
} else {
MOVED(S2.as_slice(), 6, SCLS2.as_slice_mut());
}
//
// Not much to this. Just get the cross product and its derivative.
// Using that, get the associated unit vector and its derivative.
//
DVCRSS(SCLS1.as_slice(), SCLS2.as_slice(), TMPSTA.as_slice_mut());
DVHAT(TMPSTA.as_slice(), SOUT.as_slice_mut());
}