The option to generate orbits around
Jupiter is available only for
Advanced users.
Overview
For Jupiter, the SPENVIS
orbit generator can
be used to compute
general (elliptical) orbits around the planet and
flybys.
It takes into account the oblateness of Jupiter, the gravitational attraction of Sun and the four Galilean moons
and the solar radiation pressure.
The spacecraft trajectory is defined in terms of a mission, i.e. in
addition to defining the spacecraft orbital elements, the time period
the spacecraft is in orbit has to be specified as well. In the case of Jupiter,
by default, only one segment can be considered.
Once the mission has been defined, orbital parameters
have to be specified. Once this is done, a page with a summary table of
the mission segment is presented and the trajectory generation can be started.
Mission definition
A mission is defined by the time of the end of the mission (the start of the
mission is set to the starting point of the orbit for the segment). The
mission end can be specified by the total mission duration or by an end
date.
The start time of the mission segment is set to the start time of the
orbit defined for the segment.
The segment and mission lengths and epochs defined in this fashion are
used by the environment and effects models that run on a spacecraft
trajectory. Hence, these parameters need not be specified when running
the models in question. In particular, the
radiation sources and effects models
use the segment and mission lengths to scale orbit averaged fluxes to
segment and mission fluences, or to add dose contributions from trapped
particles to those from solar protons (which are defined for the total
mission length only).
Trajectory uploads
Advanced users
have also the option to
upload
a trajectory file.
Solar radiation pressure
The user has the option to input parameters for Solar radiation pressure.
The Solar radiation pressure parameter is defined as
0.451x10
-8 K A/M,
where:
- K is the material parameter:
K = 1 - gamma + rho
|
plate
|
K = 1 - gamma
|
sphere
|
K = 2
|
plate with perfect specular reflection
|
K = 1
|
sphere with perfect specular reflection or perfect absorption
|
K = 1.44
|
sphere with perfect diffuse reflection
|
rho and gamma are the reflectivity and transmittivity of
the satellite.
- A is the total reflective area (m2) of satellites
and plates; for spherical satellites it is the cross sectional area.
- M (kg) is the mass of the satellite.
Orbital parameters
A spececraft orbit is described by means of a number of
parameters, a start date
and a duration. The start date corresponds to the date and time of the first
point written on the
output file. The duration can be
specified as a number or orbits, or directly as a duration in days (non-integer
numbers of orbits or days are allowed). It is not
expedient to generate a trajectory file for the whole of a typical mission
duration, instead a duration should be selected that guarantees coverage of all
planetographic locations. For very high altitude trajectories, a short duration is
sufficient, as the models that can be run on a trajectory do not depend on spacecraft
location outside the magnetosphere.
It is recommended to produce
graphical representations
of the trajectory before proceeding with the environment models.
Two different orbit types are available:
and all parameters have to be entered. The segment title is used for annotating the report
and
output files.
General orbit parameters
Altitude
The orbit altitude can be specified
in three ways, by specifying the following sets of parameters:
- the altitude of the perijove and
apojove of the trajectory, respectively,
above the mean radius of Jupiter;
- the length of the semi-major axis and the eccentricity.
Note that for general (elliptical) orbits the semi-major axis
is positive and the eccentricity must be greater or equal (circular orbit)
to zero and less than one.
Inclination
The orbit inclination is the angle between the orbital plane and
the equatorial plane, measured at the ascending node in the direction of
orbital motion. The orbit is called
direct when the inclination is
smaller than 90° and
retrograde when the inclination is larger
than 90°.
Right ascension of the ascending node
The right ascension of the ascending node is the angle in the equatorial
plane between the line of nodes and the direction to the vernal equinox,
measured from the vernal equinox (the direction of the intersection of the
ecliptic and equatorial planes) towards the ascending node.
Alternatively, the longitude of perijove or apogee can be specified.
Argument of perijove
The argument of perijove is the angle measured in the orbital plane from
the ascending node to the perijove.
True anomaly
The true anomaly is the angle from the perijove direction to the satellite
direction.
Hyperbolic orbit parameters
The orbit altitude can be specified by providing the length of the semi-major
axis and the eccentricity. Note that for hyperbolic orbits the semi-major axis
has a negative value and the eccentricity must be greater than one.
The remaining orbital elements (inclination, right ascension of the ascending note,
argument of perijove and true anomaly) are defined in the same way as in the general
orbit case.
Advanced users
have the option to set the output resolution of the orbit generator.
Up to three time steps (s) can be set for three different regions defined
by a limiting altitude (km).
Mission summary
When the mission segment has been defined, the mission summary
page is presented. This page provides a table with the orbit type and
duration (or number of orbits) and
the start and end time for the mission segment.
This table can be
used for a final check of the mission definition. The orbit generator
will check the segment definitions for inconsistencies. If any discrepancies
are found, an error message will be displayed.
Pressing the
button will start the calculation and
bring up the "Results" page.
The button calls up the
model selection page for consecutive runs of
multiple models.
This feature is available for
advanced users
only.
Warning: using these buttons deletes all existing output from the
orbit generator and from any model that uses this output, in order to
ensure consistency in the outputs.