Planned Path Curvature: Spacecraft Braking as Trajectory Reorientation in USP Field Theory
This paper develops a conservative engineering-style USP Field Theory interpretation of spacecraft braking. Spacecraft braking is often imagined as direct opposition to motion: thrust backward, reduce speed, and stop. This document reframes deep-space braking as a problem of trajectory curvature. At high velocity, a sharp turn requires extreme centripetal acceleration, given by: ac = v² / R Therefore, high-speed spacecraft cannot safely redirect their path late or abruptly unless very large accelerations, thermal loads, and structural stresses are accepted. A more efficient strategy is to begin curvature early, shaping the trajectory over a long distance. In USP Field Theory language, this process is interpreted as corridor re-entry. The spacecraft gradually changes its interaction geometry so that its velocity vector is redirected into a capture-compatible, lower-energy, or mission-compatible trajectory corridor. The paper clearly separates three roles: Trajectory curvature — changing the direction of the velocity vector over distance. Internal angular-momentum control — using flywheels, reaction wheels, or control-moment gyroscopes to orient and stabilize the spacecraft. External coupling — exchanging momentum or energy with an outside channel. A key guardrail is emphasized: internal flywheels or gyroscopes cannot reduce the spacecraft’s total translational momentum in isolation. They can reorient the vehicle, stabilize attitude, align sails or tethers, and manage control geometry, but real braking requires an external momentum or energy exchange channel. Possible external channels include: chemical or electric propulsion exhaust photon pressure from a sail or laser sail magnetic or plasma interaction electrodynamic tether coupling atmospheric drag and aerobraking gravity-assist trajectory shaping plasma braking or charged-particle interaction The document introduces a corridor-length momentum framework using: J = m Δv tint = m Δv / Fext ℓcorr ≈ v tint This shows why weak external forces can still produce useful braking if the interaction corridor is long enough and the maneuver begins early enough. The paper includes photon-sail and plasma-brake numerical examples, energy accounting, propellant comparison, guidance-control architecture, risk and failure modes, structural-load considerations, and a pseudocode-style planning logic. The central message is: A weak force can brake a spacecraft if the corridor is long enough. This does not create free energy or reactionless motion. It simply distributes the required momentum exchange over a longer distance and time, reducing peak acceleration and structural loading.
Authors
- Sadegh Sepehri
Publication Details
- Journal
- Zenodo (CERN European Organization for Nuclear Research)
- Published
- 2026-05-16
- DOI
- https://doi.org/10.5281/zenodo.20236516
- Primary Topic
- Spacecraft Dynamics and Control
- Type
- preprint