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State Vectors, STM & Covariance

This page covers the state representation used by satkit's numerical propagator, the state transition matrix, and how to propagate covariance and impulsive maneuvers.

State Vector

The propagator integrates a 6-dimensional state \(\vec{s} = (\vec{p}, \vec{v})\) — position and velocity in the GCRF (inertial) frame, in SI units. The free function satkit.propagate() operates directly on these 6-vectors.

For most workflows the higher-level satstate class is more ergonomic — it bundles state with time, optional covariance, optional maneuvers, and a propagate() method that handles everything automatically.

State Transition Matrix

The state transition matrix \(\Phi\) describes the partial derivative of propagated state with respect to initial state:

\[ \Phi(t; t_0)~=~\frac{\partial(\vec{p}(t),\vec{v}(t))}{\partial(\vec{p}_0,\vec{v}_0)} \]

This 6×6 matrix is computed by augmenting the ODE integration with the partial derivatives of each force term (Montenbruck & Gill Ch. 7). It is the central object for:

  • Covariance propagation\(\sigma^2_{p,v} = \Phi\,\sigma^2_{p_0,v_0}\,\Phi^T\)
  • State estimation — linearization for least-squares fits and Kalman filters
  • Sensitivity analysis — "how does the orbit at time \(t\) change if I nudge the initial state?"

Pass output_phi=True to satkit.propagate() to compute it. (rodas4 and gauss_jackson8 integrators do not support STM propagation — use one of the rkv* family.)

The satstate Class

Compare:

Feature propagate() satstate.propagate()
Position + velocity Yes Yes
Covariance propagation Manual (output_phi + matrix math) Automatic via STM
Impulsive maneuvers Not supported Automatic segmentation
Continuous thrust Via satproperties Via satproperties

Basic Usage

import satkit as sk
import numpy as np

r = sk.consts.earth_radius + 500e3
v = np.sqrt(sk.consts.mu_earth / r)
sat = sk.satstate(sk.time(2024, 1, 1), np.array([r, 0, 0]), np.array([0, v, 0]))

# Propagate forward 6 hours
new_state = sat.propagate(sat.time + sk.duration.from_hours(6))
print(new_state.pos)  # position at t + 6h

Covariance Propagation

Attach position and/or velocity uncertainty and it will be propagated automatically via the STM. The set_pos_uncertainty and set_vel_uncertainty methods accept 1-sigma components along any supported satellite-local or inertial frame:

# 1-sigma position uncertainty in LVLH (frame is required — no default)
sat.set_pos_uncertainty(np.array([100.0, 200.0, 50.0]), frame=sk.frame.LVLH)

# Or in RTN — the convention used in CCSDS OEM messages (RSW and RIC
# are Python-level aliases for the same frame)
sat.set_pos_uncertainty(np.array([10.0, 200.0, 30.0]), frame=sk.frame.RTN)

# Or directly in GCRF
sat.set_pos_uncertainty(np.array([150.0, 150.0, 150.0]), frame=sk.frame.GCRF)

# Set velocity uncertainty the same way — the position block is preserved
sat.set_vel_uncertainty(np.array([0.1, 0.2, 0.05]), frame=sk.frame.LVLH)

# Or set the full 6x6 covariance matrix directly (in GCRF)
sat.cov = my_6x6_matrix

# Propagate -- covariance propagates automatically
new_state = sat.propagate(sat.time + sk.duration.from_hours(6))
print(new_state.cov)  # 6x6 covariance at the new time

Supported uncertainty frames are GCRF, LVLH, RIC (= RSW = RTN), and NTW. See the Maneuver Coordinate Frames guide for a side-by-side comparison and guidance on which to use.

Impulsive Maneuvers

Add delta-v events at scheduled times. The propagator automatically segments at each maneuver time and applies the burn:

t_burn = sat.time + sk.duration.from_hours(1)

# Option 1: ergonomic constructors (recommended for the common cases).
# These pick the right coordinate frame for you.
sat.add_prograde(t_burn, 10.0)     # +10 m/s along velocity (NTW +T)
sat.add_retrograde(t_burn, 5.0)    # -5 m/s along velocity
sat.add_radial(t_burn, 2.0)        # +2 m/s radial-out (NTW +N)
sat.add_normal(t_burn, 1.0)        # +1 m/s cross-track (NTW +W)

# Option 2: explicit delta-v vector in a chosen frame.
sat.add_maneuver(t_burn, [0, 10, 0], frame=sk.frame.NTW)  # tangent = along velocity
sat.add_maneuver(t_burn, [0, 10, 0], frame=sk.frame.RTN)  # tangential ≠ velocity on eccentric orbits
sat.add_maneuver(t_burn, [0, 0, 5], frame=sk.frame.GCRF)  # 5 m/s in inertial +Z

# Propagate past the burn -- delta-v is applied at t_burn
new_state = sat.propagate(sat.time + sk.duration.from_hours(3))

Multiple maneuvers can be added and will be applied in chronological order. Backward propagation reverses the maneuvers automatically.

Supported maneuver frames are frame.GCRF, frame.RTN (a.k.a. RSW, RIC), frame.NTW, and frame.LVLH. For circular orbits the three non-inertial frames are equivalent; for eccentric orbits they differ by the flight-path angle in ways that matter for precision maneuver planning. See the Maneuver Coordinate Frames guide for a detailed comparison and recommendations on which frame to use.

See Also