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)
      • 𝑎, semimajor axis: size
      • 𝑒, eccentricity: shape
      • these are orbital elements
      • true anomaly 𝜃 a function of time ???
    • It is a conic section
  • 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

Conserved Quantities

  • Conserved quantities:
  • These are constant, so the true anomaly can’t be extracted from them
  • 7 conserved, yet 3+3+1=5 ?
    • 𝐡⟂𝐞 ⇒ 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): 𝑎, 𝑒, and a time element
    • three orbital elements from the 3D embedding (geometry): 𝑖, Ω, 𝜔
  • Reference: the geocentric equatorial, Earth-centered inertial (ECI) frame ̂𝐈,̂𝐉,̂𝐊
    • ̂𝐈 toward the vernal equinox, ̂𝐊 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:
    • 𝑖, inclination: the angle from the equatorial to the orbital plane (from ̂𝐊 to ̂𝐡=̂𝐖)
    • Ω, right ascension of the ascending node (RAAN): angle between ̂𝐈 and the ascending node ̂𝐧, which is the intersection of the orbital and equatorial planes on the side where the satellite goes from the southern to the northern hemisphere
    • 𝜔, argument of perigee: angle from the ascending node ̂𝐧 to the eccentricity vector ̂𝐞
  • Sketches (drawn after screen sharing failed): an inclined orbit seen edge-on, crossing the equator at angle 𝑖; and a view down the pole of an orbit circling the rotating Earth

Classical Element Set

  • Special cases: 𝑒=0 (circular), 𝑖=0 (equatorial)
    • here some angles are undefined: a “singular orbital element set” (fixes in Equinoctial Elements)
  • Classical or Kepler orbital element set:
    1. 𝑎
    2. 𝑒
    3. [time dependent]: e.g. the true anomaly 𝜃; a time element, or position angle
    4. 𝑖
    5. Ω
    6. 𝜔
  • Description of the orbital state: the orbital state vector in Cartesian space
    • 𝐫,̇𝐫→[𝐫̇𝐫]
  • Conversions both ways: Orbital Elements from State Vector and State Vector from Orbital Elements

Variants of Orbital Elements

  1. Handy variations of classical elements, e.g. 𝑟𝑝, 𝑟𝑎 instead of 𝑎, 𝑒
  2. Changing the time element / position angle (e.g. mean anomaly instead of 𝜃)
  3. Nonsingular elements: circular elements, equinoctial
  4. Canonical elements
  • Comparison of the element sets:
SetPosition variableSingularitiesNature
Classical𝑀 or 𝜃𝑒=0, 𝑖=0, 𝑖=180°Geometric
Equinoctial𝜆𝑖=180°Nonsingular
Modified Equinoctial𝐿 (true longitude)None (𝑖=180° handled via 𝐼 factor)Universal
Delaunay𝑙 (mean anomaly)𝑒=0, 𝑖=0, 𝑖=180°Canonical
Poincaré𝑙 (mean longitude)NoneCanonical / 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 𝑢: the angle from the ascending node to the satellite
  • If the orbit is not circular:
    • 𝑢=𝜔+𝜃
  • Sketch: line of nodes, perigee at 𝜔 from the node, satellite at 𝜃 from perigee; 𝑢 spans both