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SPIN STABILILIZATION 1. INTRODUCTION Z z x y Y X y Y Z z X x

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Presentation on theme: "SPIN STABILILIZATION 1. INTRODUCTION Z z x y Y X y Y Z z X x"— Presentation transcript:

1 SPIN STABILILIZATION 1. INTRODUCTION Z z x y Y X y Y Z z X x
Dynamics, Astrodynamics Orbital Dynamics, Attitude Dynamics Basic terminology Attitude X Y Z x y z

2 Spin stabilization H H X Y Z

3 Single Spinners Dual Spinners

4 x y z,p H  x y z x y z H, ,p H  Pure rotation Conning Nutation
2. The Euler’s Moment Equations Rigidy body dynamics: rotational motion in space Torque-free motion Reference systems: geometrical Angular momentum axis instantaneous rotation axis principal axes x y z,p H x y z x y z H, ,p H Pure rotation Conning Nutation

5 Torque-free motion dm x y z O

6 Spin stabilization with passive/active control

7 Major Axis Rule for Spin Stabilization
Stability of rotation about principal axes Consider the the perturbed the steady motion given by the Euler’s moment equation for torque-free motion: Differentating w.r.t. time and eliminating

8 Where Differentating w.r.t. time and eliminating
Both of these equations represent simple harmonic oscillator with general solution: Where If  is imaginary j will diverge andis unstable.  must be real for stability. This is satisfied when (Ix-Iy)(Ix-Iz) > 0 . Motion is stable when Ix>Iy e Ix>Iz or when Ix<Iy e Ix<Iz Conclusion: motion is stable about major or minor axis but motion about intermediate axis is unstable.

9 Internal Energy Dissipation Effects
All real spacecraft have, at least, some nonrigid properties. These include: elastic structural deflection and sloshing. Some lessons learned from the past: Explorer I (1958)

10 Energy dissipation Since for torque-free motion the angular momentum must be conserved motion about the major axis corresponds to the minimum energy state. Conclusion: a semirigid body is stable only when spinning about the major axis, bringing about the major axis rule for spin stabilization.

11 ATS-5 Satellite

12 Examples of Flexibility and/or Dissipation Effects
Year Satellite Control System Adverse Effect Probable Cause 1958 Explorer I Spin Stabilized Unstable Internal Energy dissipation 1952 Alouette Rapid Spin Decay Solar Torque on Thermally Deformed 1964 Explorer XX 1969 ATS-5 Spin Stabilized with active Nutation Control Dissipation

13 Momentum precession and spin thrusters locations
F R

14 SACI-1: Spin Stabilized with Geomagnetic Control
Nutation Damper Torque coil

15 SCD-1: Spin Stabilized Partially Filled Ring Nutation Damper Torque Coil

16 SACI-2 Spin stabilized with geomagnetic control Partially filled ring
Nutation Damper Spin plane coils Nutation damper

17 Mathematical model: Satellite With a Partially Filled Ring
Nutation Damper to Prevent Nutation Motion

18 Computer Simulation HT H Hx Hy Hz x y z

19

20 Conclusion Directional Stability: inertial pointing Gyroscopic properties of rotating bodies Major axis rule: rigid body are only idealizations Single and Dual Spinners Nutation Dampers: passive and active Spin stabilization combined with active control


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