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See:
Description
| Interface Summary | |
|---|---|
| BasicPropagator | This interface provides a way to propagate an orbit at any time. |
| BoundedPropagator | This interface is intended for ephemerides valid only during a time range. |
| Propagator | This interface provides a way to propagate an orbit at any time. |
| Class Summary | |
|---|---|
| AbstractPropagator | Common handling of Propagator methods for analytical-like propagators. |
| Ephemeris | This class is designed to accept and handle tabulated orbital entries. |
| SpacecraftState | This class is the representation of a complete state holding orbit, attitude and mass information at a given date. |
This package provides tools to propagate orbital states with different methods.
Propagation is the prediction of the evolution of an initial state.
The initial state and the propagated states are represented in OREKIT by a
SpacecraftState, which is a
simple container for all needed information at a specific date : mass,
kinematics,
attitude,
date,
frame. The state provides basic
interpolation features allowing to shift it slightly to close dates. For
more accurate and farthest dates, several full-featured propagators are
available to propagate the state.
KeplerianPropagator
implements the Propagator
interface, which ensures that we can obtain a propagated SpacecraftState
at any time once the instance is initialized with an initial state.
This extrapolation is not a problem with a simple
EquinoctialOrbit
representation: only the mean anomaly value changes.
Propagator interface.
NumericalPropagator
class realizes the interface between space mechanics and mathematical
resolutions. If its utilization seems difficult on first sight, it is in
fact quite clear and intuitive.
The mathematical problem to integrate is a seven dimension time derivative equations
system. The six first equations are given by the Gauss equations (expressed
in EquinoctialOrbit) and the
seventh is simply the flow rate and mass equation. This first order
system is computed by the
TimeDerivativesEquations class.
It will be instanced by the propagator and then be modified at each step
(a fixed t value) by all the needed
force models which
will add their contribution, the perturbing acceleration.
The integrators
provided by commons-math need the state vector at t0, the state vector first
time derivate at t0, and then calculates the next step state vector, and
ask for the next first time derivative, etc. until it reaches the final
asked date.
The NumericalPropagatorWithJacobians
is a specialized class which enables to compute jacobians with respect to orbital
parameters and force models parameters while propagating.
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