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Sensitivity Analysis of Separation Time Along Weak Stability Boundary Transfers

Isabel Nolton, Kento Tomita, Yuri Shimane, Koki Ho

Abstract

This study analyzes the sensitivity of the dynamics around Weak Stability Boundary Transfers (WSBT) in the elliptical restricted three-body problem. With WSBTs increasing popularity for cislunar transfers, understanding its inherently chaotic dynamics becomes pivotal for guiding and navigating cooperative spacecrafts as well as detecting non-cooperative objects. We introduce the notion of separation time to gauge the deviation of a point near a nominal WSBT from the trajectory's vicinity. Employing the Cauchy-Green tensor to identify stretching directions in position and velocity, the separation time, along with the Finite-Time Lyapunov Exponent are studied within a ball of state uncertainty scaled to typical orbit determination performances.

Sensitivity Analysis of Separation Time Along Weak Stability Boundary Transfers

Abstract

This study analyzes the sensitivity of the dynamics around Weak Stability Boundary Transfers (WSBT) in the elliptical restricted three-body problem. With WSBTs increasing popularity for cislunar transfers, understanding its inherently chaotic dynamics becomes pivotal for guiding and navigating cooperative spacecrafts as well as detecting non-cooperative objects. We introduce the notion of separation time to gauge the deviation of a point near a nominal WSBT from the trajectory's vicinity. Employing the Cauchy-Green tensor to identify stretching directions in position and velocity, the separation time, along with the Finite-Time Lyapunov Exponent are studied within a ball of state uncertainty scaled to typical orbit determination performances.
Paper Structure (14 sections, 11 equations, 13 figures)

This paper contains 14 sections, 11 equations, 13 figures.

Figures (13)

  • Figure 1: Illustration of separation time. The blue nominal trajectory originates from some point (usually the center) of the grid; the red neighbor trajectory stems from one of the gridded state, and its evolution in time is tracked. When the Euclidean distance of the position or velocity vector exceeds a threshold, the time stamp is recorded as the separation time for this neighbor trajectory.
  • Figure 2: WSBT (a) shown in Earth-Moon rotatin-pulsating frame, with integer labels corresponding to time indices corresponding to locations where FTLE grid is constructed.
  • Figure 3: WSBT (b) shown in Earth-Moon rotating-pulsating frame, with integer labels corresponding to time indices corresponding to locations where FTLE grid is constructed.
  • Figure 4: WSBT (a): Separation Time vs. Time Index (unstable grid, OD-ball=(10 km, 10 cm/s))
  • Figure 5: Contour FTLE and Separation Time Plots for WSBT (a) with unstable grid
  • ...and 8 more figures