Implemented frames and coordinates
Numerous frames are implemented in SPICE through built-in options and those we have defined in custom_frames_v01.tf
. We describe each implemented frame and its associate coordinate system here. More detail on the frames and where they have appeared in past studies can be found in the supplemental text of the PlanetMag publication (DOI TBD).
All frames use the body center of mass for the origin. Any axis direction not listed can be inferred by that needed to complete a right-handed coordinate system. All frames in PlanetMag and all those available in SPICE are right-handed. All frames implemented in PlanetMag use Cartesian basis vectors.
IAU frames
Defined in reports of the IAU Working Group on Cartographic Coordinates and Rotational Elements.
\(\hat{z}\) is along the angular momentum vector
\(\hat{x}\) is approximately toward the planet, with the \(xz\) plane containing a specific surface feature identified by the IAU
Available in SPICE as
IAU_BODY
for any body for which ephemeris data has been loaded into the kernel pool
System III frames
These frames rotate with the planet according to the period inferred from regular oscillations in the magnetic field, or physical behavior tied to the field such as synchrotron emission.
\(\hat{z}\) is along the planet’s angular momentum vector
\(\hat{x}\) is in an arbitrarily defined direction at an arbitrary moment, because the giant planets generally lack stable surface features
Identical to
IAU_JUPITER
andIAU_SATURN
for those planetsImplemented as
ULS
andNLS
for the Uranus Longitude System and Neptune Longitude System, respectively
SPRH frames
This is a designation sometimes used in NASA Planetary Data System (PDS) archives for data aligned to spherical coordinate basis vectors. The frame is identical to System III coordinates for those bodies for which data are expressed in this format. However, because spherical coordinate axes are not aligned to Cartesian axes, the data must be converted for comparison to SPICE frames.
Planet–Sun–Orbit frames
\(\hat{x}\) is toward the Sun
\(\hat{y}\) is along the component normal to \(\hat{x}\) of the velocity vector of the Sun as seen from the body
Implemented as
JSO
,KSO
,USO
,NSO
for Jupiter, Saturn, Uranus, and Neptune respectively
Planet–Sun–Magnetic frames
\(\hat{x}\) is toward the Sun
\(\hat{y}\) is along \(\hat{\mathbf{M}}\times\hat{x}\), where \(\mathbf{M}\) is the magnetic dipole moment vector. Requires a choice of magnetic field model in order to infer the dipole moment direction.
For use in particular models that require this frame. The selected multipole models are:
JSM
: O4 (Acuna and Ness, 1976) https://doi.org/10.1029/JA081i016p02917KSM
: Cassini 11 (Dougherty et al., 2018) https://doi.org/10.1126/science.aat5434USM
: OTD (Ness et al., 1986) https://doi.org/10.1126/science.233.4759.85NSM
: O8 (Connerney et al., 1992) https://doi.org/10.1016/0273-1177(92)90394-D
Planet–Dipole–Solar–Zenith frames
\(\hat{z}\) is toward the Sun
\(\hat{y}\) is along \(\hat{\mathbf{M}}\times\hat{z}\), where \(\mathbf{M}\) is the same dipole moment vector as used in Planet–Sun–Magnetic frames
Implemented as
JDSZ
,KDSZ
,UDSZ
,NDSZ
for Jupiter, Saturn, Uranus, and Neptune respectively
Solar–Magnetic–Planet frames
\(\hat{z}\) is along \(\hat{\mathbf{M}}\) as defined in Planet–Sun–Magnetic frames
\(\phi=0\) at the sub-solar point, i.e. the \(x\) axis is along the direction perpendicular to \(\hat{z}\) along the noon local time longitude line
The \(xy\) plane defines the magnetic equatorial plane
Implemented as
SMJ
,SMK
,SMU
,SMN
for Jupiter, Saturn, Uranus, and Neptune respectively