Title: Briefing to the Space Systems Academic Group
1Briefing to the Space Systems Academic Group
- Aerodynamic Orbital Transfer of the X-37 Orbital
Maneuvering Vehicle - LT John P. Pienkowski, USN
- 366 Curriculum Student
- Thesis Advisor
- Dr. Stephen Tony Whitmore
- Co-Advisor
- Dr. Michael G. Spencer
2Background
Brig Gen Anarde HQ AFSPC/XP
08/24/2001
Military Spaceplane (MSP) and Reusable Launch
Vehicle Study
3Purpose of Arnade Study
- Assess Reusable Launch Vehicles
- Operational Utility
- Science and Technology Maturity
- Assess X-33 and X-37 applicability
- Recommend position
- AF role in X-33 and X-37 programs
- Identify other options
- Establish glide slope for AF Reusable
- Launch Vehicle way ahead
4Arnade Council, Conclusions
Reusable vehicles offer potential warfighting
value Two Stage to Orbit -- the best
alternative Mix of Expendable and Reusable
Vehicles Suite of vehicles to cover the range
of ops and missions Substantial risks and
mitigations associated with continuing with the
X-33 and X-37 programs Programs fill only small
parts of flight profiles required to field
operational military space plane Do not pursue
X-33 program Approve further study of X-37 as we
develop RLV roadmap
5X-37, Concerns and Recommendations
Gaps in capability - Operations -
Technology - Performance Ops Concepts and
Requirements Definitions Immature Need to
Expand Orbital Operations Flexibility
6X-37, What is it?
Shuttle Deployment
- Prototype Re-Usable Orbital Maneuvering
- Vehicle (OMV)
- PROGRAM OBJECTIVE - Reduce cost of
- space transportation via flight demonstration
- to mature and validate advanced technology
- To and from LEO
- In-Space
- NASA/Boeing Cooperative Agreement
- X-40A flights demonstrated autonomous landing
EELV (Delta IV Launch)
7(No Transcript)
8X-37 Propulsion System
Rocketdyne AR2-3A Main Engine
Propellants 90 H2O2, JP-8 Oxidizer
Tank Usable mass 2454 lbm 90 H2O2 Fuel
Tank Usable mass 327 lbm JP-8 Propellant
Mass Fraction (propellant/dry mass) Pmf
0.3900 Nominal Thrust 3,300 lbf variable
throttle multiple restart capability Vacuum
Isp 240.8 sec Total Available ?V 2544.86
ft/sec
9X-37 Propulsion System (contd)
Total Available ?V 2544.86 ft/sec
Excessive for In-Plane maneuvering Requirements
Not enough available DV for significant plane
change capability
Need to Expand Orbital Operations Flexibility
10Cost Analysis
- Costly to change a spacecrafts inclination
- DV
- fuel consumption
- Space Shuttle can change inclination only by few
tenths of a degree - Must launch into desired orbit
- Heavier payloads, but a single orbit
- If X-37 can be demonstrated to have potential to
change up to 10 degrees orbital inclination - Achieve dual use of a single spacecraft for the
price of one launch - Expand Orbital Operations Flexibility
11Goal
- Assess Feasibility of using aerodynamic forces to
change the orbital inclination of a the X-37
Spacecraft, Preserving Fuel for In-Plane
maneuvers - Develop Optimized Strategies for Performing these
maneuvers
12Approach Develop real-time Piloted-Sim
that allows a wide variety of candidate maneuvers
and trajectories to be quickly assessed
Simulation serves as insight builder as to
which parameters are important to the problem
13 Develop batch simulation capable ofextended
Monte-Carlo analysis Batch and real-time
simulations used for cross-validation
Piloted simulation tool can be used for
generating feasible starting trajectories
forfollow-on optimization codes (i.e. DIDO,
POST)
Approach (continued)
14Maneuver Description
- At perigee, spacecraft descends into upper
atmosphere - Uses aerodynamic forces to alter flight path with
enough energy to maintain orbital velocity - Small boost from engine allows spacecraft to
regain altitude at new inclination
15Maneuver Description
16Maneuver Description
17Equations of Motion
18Equations of Motion (contd)
19Generalized Equations of Motion
J2 not included
20Equations of Motion (contd)
Lift/Drag Force
21Equations of Motion (contd)
X-37 Aero database
22Equations of Motion (contd)
Atmospheric Model 1976 US Standard extended to
600 km
23Equations of Motion (contd)
and of course about a zillion orbital
coordinate transformations
24Simulation Demonstrations Illustrate perigee
collapse concept Demonstrate the Need for
orbit Regulation
25Orbital Energy Regulation
Orbital Energy
Orbit decay
26Orbital Energy Regulation (contd)
Engine thrust used to return orbital energy
robbed by aerodynamic forces.
27Orbital Energy Regulation (contd)
Constrained Optimization Problem
28Orbital Energy Regulation (contd)
Constrained Optimization Problem
29Orbital Energy Regulation (contd)
Necessary Conditions for Optimization
30Orbital Energy Regulation (contd)
Necessary Conditions for Optimization
When all of the variational calculus is said
and done
Which is a dang! Simple control law
31Orbital Energy Regulation (contd)
and we can implement the control as an initial
value problem . Not! a boundary value problem!
Why?
po 0
Our final state is free .. And When t0, we are
near orbit apogee (just after de-orbit burn)
where the dissipative forces are REALLY CLOSE to
zero \the required initial throttle is zero, \
po is zero! we can integrate the co-state
equation forwards Instead of backwards! a
practical limit of many optimal control laws .
Yea, joy and clapping!
32Simulation Demonstrations Illustrate how
regulator avoids perigee collapse Show a
complete plane change cycle of greater
than 10?
33Whats Next?
- Perform complete Simulink/Labview Simulation
cross- - validation
- Fully evaluate Optimal Control Methods for Orbit
stabilization/re-boost - Implement J2 Perturbations
- Conduct parametric analysis to find optimum
flight path - Heating analysis during re-entry
- Assess vehicle Stability during maneuvers
- Vehicle Attitude Control Before Aero-forces
become dominant, entry - into aero maneuvers
34Simulink Model
35Labview Model
36Acknowledgements
- Thesis Advisor
- Dr. Stephen Tony Whitmore
- Co-Advisor
- Dr. Michael G. Spencer
- Matlab Help
- CDR Mark Couch, USN