Six numbers that describe the orbit (and where the satellite is on it), as an alternative to the Cartesian state vector. See also ENAE 441: Orbits and ENAE 441: State Information.
Orbital Motion So Far
- Summary of what the conservation laws give us:
- The orbit is in a plane (constant angular momentum)
- , semimajor axis: size
- , eccentricity: shape
- these are orbital elements
- true anomaly a function of time ???
- It is a conic section
- The orbit is in a plane (constant angular momentum)
- Next steps (start of “Orbital state and elements”):
- Go from the 2D orbit in space to
- 3D
- the orbit in time
- Orbital elements and the state vector: the state of a system
- Go from the 2D orbit in space to
Conserved Quantities
- Conserved quantities:
- Energy (1)
- Angular momentum (3)
- Eccentricity vector (3)
- These are constant, so the true anomaly can’t be extracted from them
- 7 conserved, yet ?
- for one of these, only two components are required
- Energy is redundant: it can be calculated from the angular momentum and eccentricity
- So the conserved quantities supply 5 elements; the sixth must be a time-dependent one
Orbit in Three Dimensions
- Embed the orbital plane in 3D space:
- three orbital elements from the plane (physics): , , and a time element
- three orbital elements from the 3D embedding (geometry): , ,
- Reference: the geocentric equatorial, Earth-centered inertial (ECI) frame
- toward the vernal equinox, toward the north pole
- “inertial” “non-rotating”, i.e., not rotating with the central body
- more in Coordinate Systems
- The orientation is a set of 3-1-3 Euler angles:
- , inclination: the angle from the equatorial to the orbital plane (from to )
- , right ascension of the ascending node (RAAN): angle between and the ascending node , which is the intersection of the orbital and equatorial planes on the side where the satellite goes from the southern to the northern hemisphere
- , argument of perigee: angle from the ascending node to the eccentricity vector
- Sketches (drawn after screen sharing failed): an inclined orbit seen edge-on, crossing the equator at angle ; and a view down the pole of an orbit circling the rotating Earth
Classical Element Set
- Special cases: (circular), (equatorial)
- here some angles are undefined: a “singular orbital element set” (fixes in Equinoctial Elements)
- Classical or Kepler orbital element set:
- [time dependent]: e.g. the true anomaly ; a time element, or position angle
- Description of the orbital state: the orbital state vector in Cartesian space
- Conversions both ways: Orbital Elements from State Vector and State Vector from Orbital Elements
Variants of Orbital Elements
- Handy variations of classical elements, e.g. , instead of ,
- Changing the time element / position angle (e.g. mean anomaly instead of )
- Nonsingular elements: circular elements, equinoctial
- Canonical elements
- Comparison of the element sets:
| Set | Position variable | Singularities | Nature |
|---|---|---|---|
| Classical | or | , , | Geometric |
| Equinoctial | Nonsingular | ||
| Modified Equinoctial | (true longitude) | None ( handled via factor) | Universal |
| Delaunay | (mean anomaly) | , , | Canonical |
| Poincaré | (mean longitude) | None | Canonical / Nonsingular |
Argument of Latitude
- For circular orbits there is no perigee, so measure the satellite’s position from the ascending node instead
- Argument of latitude : the angle from the ascending node to the satellite
- If the orbit is not circular:
- Sketch: line of nodes, perigee at from the node, satellite at from perigee; spans both