IPPW-10
description
Transcript of IPPW-10
IPPW-10
Royal Observatory of Belgium
18 June 2013
von Karman Institute for Fluid Dynamics
Mars atmosphere reconstructionusing FADS on ExoMars EDM
Bart Van HoveÖzgür Karatekin
Royal Observatory of BelgiumRinglaan 3, Brussel [email protected]
10th International PlanetaryProbe Workshop
San Jose, CA, US18 June 2013
Royal Observatory of Belgium
von Karman Institute for Fluid Dynamics
Why is reconstruction important?
Mars is the ultimate test facility:learn from one mission to design the next
Trajectory reconstruction
Vehicle response: deceleration, velocity, attitude
Atmosphere reconstruction
• What environment produces the vehicle response?• Constrain environment to validate ground predictions• Constrain Mars climate models
• ExoMars EDL Demonstrator Module (EDM) will land during the 2016 Mars dust season
Viking
MSL
Pathfinder
IPPW-1018 June 20132
Royal Observatory of Belgium
von Karman Institute for Fluid Dynamics
Reconstructing from conventional instrumentation
Inertial Measurement Unit = IMU
Positional measurements by accelerometers and gyroscopes
Estimate atmosphere from trajectory reconstruction:
Density from acceleration and drag coefficient
Pressure from hydrostatic equilibrium
Temperature from ideal gas law
Atmospheric reconstruction starts from density from drag equation:
acceleration aerodynamic drag coefficient true air speed
IPPW-1018 June 20133
Royal Observatory of Belgium
von Karman Institute for Fluid Dynamics
Reconstructing from heat shield instrumentation
Flush Air Data System = FADS
Installed on MSL and ExoMars EDM 2016:heat shield surface
pressure sensorsFlow field measurements include atmospheric motion
FADSsolver
IMU trajectory
FADS pressure signals
Surface pressure model
Relation to free stream
True air speed
Atmospheric density
Atmospheric winds
IPPW-1018 June 20134
Does not require aerodynamic drag model: could instead be validated
Royal Observatory of Belgium
von Karman Institute for Fluid Dynamics
Presentation overview
1. Toolkit development: EDL simulation and reconstruction tools
2. ExoMars EDM 2016: preliminary study reconstruction uncertainty
IPPW-1018 June 20135
Atmospheric reconstruction at high velocities, before parachute opening
Royal Observatory of Belgium
von Karman Institute for Fluid Dynamics
Toolkit development
Reconstruction tool + Monte Carlo
• Validated in Mars Phoenix case study(public IMU flight data set)
• Matches independent reconstructions
• Monte Carlo with time varying bias and noise errors
6-DOF entry simulator
• To produce flight data (IMU and FADS)
• No parachute phase, no guidance
• Validated in collaboration NASA Langley
IPPW-1018 June 20136
units [Desai et al. 2] This study
Time since entry (s) 227.8 227.8
Geocentric altitude (km) 13.3 13.55
Relative velocity (m/s) 387.6 391
Total angle of attack (deg) 4.73 4.82
Match reconstruction at parachute deployment
Royal Observatory of Belgium
von Karman Institute for Fluid Dynamics
ExoMars EDM 2016: preliminary reconstruction study
IPPW-1018 June 20137
• Solar longitude: 244.8 ° in dust season
• Unguided ballistic entry
Mars entry interface
Altitude: 120 km Longitude: 344.6 ° Latitude: 4.5 °Speed: 5.9 km/s Flight path: -12.7 ° Azimuth: 124 °
IMU & FADS instrumentation
Sampling frequencies:
• IMU 100 Hz
• FADS 10 Hz
Preliminary uncertainty estimatesExoMars EDM 2016 entry vehicle
Royal Observatory of Belgium
von Karman Institute for Fluid Dynamics
ExoMars EDM: 6-DOF simulation
IPPW-1018 June 20138
Simulated up to parachute opening at Mach 2
• MCD (Mars Climate Database) dust storm scenario predicted by LMD GCM [Forget et al.]
• Reproduces expected flight behavior
→ Let’s reconstruct from the synthetic flight data
Δt = 2 msESA aero v5.12
MCD 5.0 dust
Royal Observatory of Belgium
von Karman Institute for Fluid Dynamics
ExoMars EDM: impact of assumptions in IMU atmosphere reconstruction
IPPW-1018 June 20139
Typical error sources in IMU reconstruction
1. Start from “true” MCD density profile provided to 500 Hz simulation (dust storm scenario)
2. Reconstruct at 100 Hz like the ExoMars IMU3. Assume pure CO2 instead of actual gas mixture
4. Neglect winds since IMU can’t resolve those5. Incorrectly model the drag coefficient (+ 3-σ)
ConclusionNeglecting wind can be as detrimentalas mispredicting the drag coefficient!
𝜌∞ (h )=2𝑚 ·|�⃗�|
𝐶𝐷 · 𝐴𝑟𝑒𝑓 ·𝑉 ∞2
Royal Observatory of Belgium
von Karman Institute for Fluid Dynamics
Strong winds along EDM trajectory: especially during dust storms
IPPW-1018 June 201310
MCD 5.0 (Mars Climate Database) wind profiles
• EDM will fly along the equator
• Seen from the Mars surface:strong high altitude retrograde wind
• Seen from space: atmosphere lags behind rigid planet rotation
• Caused by migrating thermal tides due to solar heating
Relative velocity and atmospheric density from IMU data are uncorrected for winds
Could we improve density reconstruction by estimating winds from FADS?
Royal Observatory of Belgium
von Karman Institute for Fluid Dynamics
ExoMars EDM: FADS reconstruction methodology
IPPW-1018 June 2013
Rebuild oncoming flow from heat shield instrumentation
1. Surface pressure distribution modelstagnation pressure and flow angles
2. Shock wave pressure ratio
3. Derive density from dynamic pressureair speed from IMU (neglecting winds)or FADS (corrected with wind estimate)
𝒒∞=𝝆∞𝑽 ∞
𝟐
𝟐
?
angle of attack αside slip angle β
stagnationpressure
pt2
𝑽 ∞𝟐
correctedfor winds?
11
surface pressure
Royal Observatory of Belgium
von Karman Institute for Fluid Dynamics
ExoMars EDM: FADS reconstruction methodology
IPPW-1018 June 2013
Rebuild oncoming flow from heat shield instrumentation
angle of attack αside slip angle β
stagnationpressure
pt2
1. Surface pressure distribution model
• Modified Newtonian flow model:
• Non-linear least-squares solver
• Solve for and flow angles from
• Fix atmospheric pressure from IMU
(errors on have small impact since )
• True flow angles: sensitive to wind velocity
with
12
Royal Observatory of Belgium
von Karman Institute for Fluid Dynamics
ExoMars EDM: FADS reconstruction methodology
IPPW-1018 June 2013
Rebuild oncoming flow from heat shield instrumentation
angle of attack αside slip angle β
stagnationpressure
pt2
2. Shock wave pressure ratio
• Normal shock wave conservation equations
• VKI Mutation library: high temperature gas properties for 5-species CO2 [Magin et al. 2009]
• 1-D flow solver to build a database of
• High temperature effects are main approximation inanalytical cold gas relations – up to 5% difference!
𝒒∞
13
Royal Observatory of Belgium
von Karman Institute for Fluid Dynamics
ExoMars EDM: FADS reconstruction methodology
IPPW-1018 June 2013
Rebuild oncoming flow from heat shield instrumentation
𝒒∞=𝝆∞𝑽 ∞
𝟐
𝟐
3. Derive density from dynamic pressure
• Air speed from IMU (no winds) or corrected using FADS wind velocity estimates
• Wind estimate from true FADS flow angles
• Non-linear LSQ solver neglecting vertical wind
14
Royal Observatory of Belgium
von Karman Institute for Fluid Dynamics
Monte Carlo: FADS reconstruction vs. IMU
IPPW-1018 June 2013
Conclusion
Poor wind estimate increases uncertaintyBoth FADS and IMU over 5% uncertainty on
• IMU density estimate: large bias error (neglects winds)• FADS with IMU air speed: similar to IMU < 80 km• FADS with corrected air speed: wind estimate too noisy• Limited benefit from additional sensors
15
MCD 5.0 dust
Royal Observatory of Belgium
von Karman Institute for Fluid Dynamics
ExoMars EDM: horizontal wind estimate from FADS
IPPW-1018 June 2013
Along the entire entry trajectory the wind estimation error ≥ wind amplitude
16
Royal Observatory of Belgium
von Karman Institute for Fluid Dynamics
ExoMars EDM: uncertainties for different weather scenarios
IPPW-1018 June 201317
Dust storms strongly affect atmospheric profiles: detectable below 80 km
Royal Observatory of Belgium
von Karman Institute for Fluid Dynamics
Hypothetical FADS pressure sensors to resolve winds
IPPW-1018 June 201318
Imagine very accurate pressure sensors over the entire (high velocity) trajectory
Density bias error reduced: especially at high altitudes where winds are strongest
Royal Observatory of Belgium
von Karman Institute for Fluid Dynamics
Hypothetical FADS pressure sensors to resolve winds
IPPW-1018 June 201319
Royal Observatory of Belgium
von Karman Institute for Fluid Dynamics
Summary & Conclusions
• Approximate general FADS solver: modified Newtonian 1-D flow
• Winds can affect air speed and density estimate
• Currently difficult to resolve from FADS pressure measurements
• Additional low range pressure sensors
• Atmospheric reconstruction sufficiently accurate to detect dust storms
IPPW-1018 June 201320
Royal Observatory of Belgium
von Karman Institute for Fluid Dynamics
Future work
IPPW-1018 June 2013
• Coupled FADS-IMU reconstruction using Kalman filtering
• FADS reconstruction based on CFD
• Consider other Mars missions
• Consider Doppler analysis of radio communications
• Simulate parachute phase (multi-body model under development)
21
Royal Observatory of Belgium
von Karman Institute for Fluid Dynamics
Acknowledgements
François Forget – Université Paris
Jeffrey Herath / Juan Cruz / Daniel Litton – NASA Langley Research Center
Paul Withers – Boston University
IPPW-1018 June 2013
ESA Education IPPW student support
project support
22
Royal Observatory of Belgium
von Karman Institute for Fluid Dynamics
References
IPPW-1018 June 201323
Royal Observatory of Belgium
von Karman Institute for Fluid Dynamics
ExoMars EDM: is a dust storm detectable?
IPPW-1018 June 2013
Dust storm impact density profile very strongly: should be detectable above 20 km
24
Royal Observatory of Belgium
von Karman Institute for Fluid Dynamics
Impact of approximations on IMU temperature reconstruction
IPPW-1018 June 201325
Royal Observatory of Belgium
von Karman Institute for Fluid Dynamics
Aerodynamic drag uncertainty
IPPW-1018 June 201326
Royal Observatory of Belgium
von Karman Institute for Fluid Dynamics
FADS normal shock wave pressure ratio
IPPW-1018 June 2013
Discrepancy up to 7% with ideal (cold) gas approximation
27
Royal Observatory of Belgium
von Karman Institute for Fluid Dynamics
Toolkit development – 6-DOF entry simulator
Simulate entry to synthesize IMU and FADS flight data
• Impact of atmospheric conditions, wind velocities…• Planet, aerodynamics, gravity, vehicle models• No parachute phase or real-time flight control systems• Validated in collaboration with NASA Langley
IPPW-1018 June 201328
Royal Observatory of Belgium
von Karman Institute for Fluid Dynamics
Toolkit development – Reconstruction and Monte Carlo
IPPW-1018 June 2013
Integrate IMU data to reconstruct entry profiles
• Validated in our Mars Phoenix case study(only IMU available)
• Good match with independent reconstructions• Monte Carlo with time varying bias and noise
errors of various types and distributions
units [Desai et al. 2] This study
Time since entry (s) 227.8 227.8
Geocentric altitude (km) 13.3 13.55
Relative velocity (m/s) 387.6 391
Total angle of attack (deg) 4.73 4.82
Match reconstruction at parachute deployment
29