CubeSat Design for Solar Sail Testing Applications
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Transcript CubeSat Design for Solar Sail Testing Applications
CubeSat Design for Solar Sail
Testing Applications
Phillip Hempel
Daniel Parcher
Paul Mears
Taffy Tingley
The University of Texas at Austin
October 11, 2001
Presentation Outline
Project
Goal
Budget
Management
Structure
Future Work
Satellite
Systems
Conclusion
Project Goal
Design a Test Platform for Solar
Sail Propulsion Technology
– Measure Thrust
– Measure Solar Sail Efficiency
Management Structure
Daniel Parcher
– Project Manager
– Tracking Systems Department Head
– Electronics Department Head
Phillip Hempel
– Mechanical Systems Department Head
Taffy Tingley
– Propulsion Systems Department Head
Paul Mears
– Orbital Trajectory Department Head
CubeSat Project Background
Sponsored by Stanford University
Utilizes picosatellite satellite
Designs that perform some
scientific task
Different CubeSat launches provide
different initial conditions
Constraints
CubeSat Prescribed Constraints
– 10cm Sided Cube
– 1 Kg Weight
– Timing System to Delay Power-On
– Space-Flown Materials
Adopted Constraints (for Simplicity and Reliability)
– No Attitude Control
– No Powered Systems (except required Timer)
– No Communications Systems
Presentation Outline
Project
Overview
Budget
Management
Structure
Future Work
Satellite
Systems
Conclusion
CubeSat Required Systems
Timer
– RDAS accelerometer/timer
– Voltage outputs to trigger
system events
Casing
– Aluminum
– Kill Switch
– Attached CC reflectors
Tracking / Communcations
No Satellite Communication
Tracking performed with corner cube reflectors
– determine position, rotation, acceleration
Corner cube reflectors to be supplied by
Banner Engineering Corp.
Mechanical Systems
Phillip Hempel
Satellite Components
Frame/ Corner Cube Reflectors
Kill Switch/ Timer
Sail
Inflation Capsule
Capillaries
Hardening Strips
Frame
10 cm Sided
Cube
Corner Cubes
Panels to be
Placed on Sides
Corner Cube Reflectors
Flat-Plate Reflectors
Attached to Frame
Released Prior to
Inflation
In the Plane of the
Solar Sail
Kill Switch/Timer
Kill Switch Triggered by Release
Begins Timer Sequence
Controls All Timing Sequences
Solar Sail Properties
Aluminized Mylar
Circular Shape
Area of 100 m^2
Example of Aluminized Mylar Structure
Capillaries
Tubes attached to the surface
of the solar sail
Capillaries will be placed
placed strategically for
structural rigidity
Tubes are inflated by nitrogen
from capsule
Total Length = 272 ft.
Diameter
= 0.5 in
Inflation Capsule
7.6 cm Long
3.8 cm Diameter
86 cm^3 Volume
60.5 psi
Placed in the Center
of the CubeSat
Hardening Strips
Thin tape-like strips
Strips will be placed strategically in
a spider web pattern on the sail
Strips harden with solar radiation
exposure
Total Strip Length = 308 ft.
Cut-Away CubeSat
Sequence of Events
P-Pod Release/ Deactivate Kill
Switch
Waiting Period
Side Panels Unlock
Inflation Begins
Inflation Ends/ Rigidization Occurs
Solar sail reaches final shape
Propulsion
Taffy Tingley
Solar Sail Material Selection
Encounter Satellite
Solar Blade Solar Sail
Solar Sail Material Selection
Cosmos I
Star of Tolerance
Satellite
Aluminized Mylar
High Strength to Weight Ratio
Tested
Cheap!
Double Reflective
ABAQUS
Finite Element Design
Monitor regions where high stress occurs
- Add tear strip or tension line to sail
Monitor rigidity
Model several perturbations and situations
Perform thermal analysis
Monitor effects of additional components
All in 3-D
Future Propulsion Work
Integrate deployment apparatus into FE model
Install Tear Strips into FE model
Perform Thermal Analysis
Orbit Simulation
Paul Mears
Solar Radiation Pressure
Electromagnetic
radiation flux
Photon energy
Momentum
exchange
produces force
per unit area
ΔV
Sail Thrust
Function of: T = f (A, S, e, q)
where
A = sail area
S = Power (scaled Watt)
e = reflectivity
q = angle of incidence
T (S A cosθ) (1 ε 2 2ε cos 2θ)
Sail Thrust Vector
Sail
-Fr
Fi
Sun
θ
FT
Fr
Thrust Acts in the direction
Normal to the Sail
Sail Normal makes an angle q
with the Sun Position Vector
Thrust is generated by
Incidental and Reflected Light
T T SN
θ a cos(SN u)
T Ti Tr
ŜN
4-Body Problem
Z
Y
X
SPV S
MPV M
r1
r2
ECEF Coordinate System (x, y, z)
(1) Earth (2) Sun (3) Moon
(4) Satellite (T) Thrust
r3
ˆ
SN , T
Forces on the Satellite
The gravitational
forces of all the
planets effect the
satellite, as well as
thrust
i
Fi
ri
3
ri
ri
i
F1 (Earth)
Z
Y
X
F3
F2 (Sun)
T (Thrust)
FBD: Satellite
i
FTotal T 3 ri i = 1, 2, 3
ri
(Moon)
Initial Conditions of Orbit
Injection will occur at perigee
Orbit will be highly elliptic with apogee at
42000km
Rp = 7178.14 km
Ra = 48619.23 km
Resulting Orbital
Elements
Vp = 10.19 km/s2
Va = 3.04 km/s2
e = 0.743
a = 55797.37 km
Orbit Propagation: Perturbing Forces
Earth Forces Only
Earth, Sun, Moon Forces
Orbit Propagation with Thrust
Earth, Sun, Moon Forces
All Gravitational Forces
plus Thrust
Future Work in Orbit Simulation
Rotating Thrust Vector
SN
Zˆ
α α0 α t
β β0 β t
α( t )
Xˆ
(t )
Yˆ
Presentation Outline
Project
Overview
Management
Structure
Satellite
Systems
Budget
Future Work
Conclusion
Budget
• Personnel
• Testing
• Materials
• Launch
• Total
- $15,633
- $ 2,000
- $ 5,000
- $50,000
- $72,653
Future Work
Hardware integration
– Part size and weight definition
and orientation within the
satellite
Deployment system timing
Finite element analysis
Orbital simulation
– Rotating thrust vector definition
– Orbital trajectories simulation
Conclusion
PaperSat is developing a picosatellite design for
CubeSat
Design will test solar sail propulsion technology
Design will not incorporate attitude control
Deployment system uses compressed gas
Solar sail will be reflective on both sides
Position, acceleration, and orientation will be
measured from ground stations
http://www.ae.utexas.edu/design/papersat/
Acknowledgements
Dr. Wallace Fowler
Dr. Cesar Ocampo
Dr. Eric Becker
Meredith Fitzpatrick
Previous CubeSat Design Groups
Questions?