grace mission: architecture of the flight segment€¦ · 6 grace mission the seminal sst gravity...

27
1 GRACE Mission GRACE Mission: Architecture of the Flight Segment Ab Davis 27 June 2002

Upload: others

Post on 16-May-2020

6 views

Category:

Documents


1 download

TRANSCRIPT

Page 1: GRACE Mission: Architecture of the Flight Segment€¦ · 6 GRACE Mission The Seminal SST Gravity Mission Milo Wolff, MIT-SAO - JGR, Vol.,74, No. 22, Oct. 1969 • Two geometrically

1

GRACE Mission

GRACE Mission: Architecture of the Flight

Segment

Ab Davis27 June 2002

Page 2: GRACE Mission: Architecture of the Flight Segment€¦ · 6 GRACE Mission The Seminal SST Gravity Mission Milo Wolff, MIT-SAO - JGR, Vol.,74, No. 22, Oct. 1969 • Two geometrically

2

GRACE MissionPrinciples

Focus• "Do one thing. Do it well."

• "Chose an objective that is worth pursuing"

Balance • "Technology without economics is not engineering"

Risk Containment• "Don't stretch the limits of hardware performance"

Page 3: GRACE Mission: Architecture of the Flight Segment€¦ · 6 GRACE Mission The Seminal SST Gravity Mission Milo Wolff, MIT-SAO - JGR, Vol.,74, No. 22, Oct. 1969 • Two geometrically

3

GRACE MissionBalance

• Minimizing Total Cost• Total Cost = ∑(C1+C2+C3 . . . . . . . . . .+Ck)• For a given level of performance, Total Cost is minimum if

• ∂ Perf/∂C1=∂ ��Perf/∂C2=∂ Perf/∂C3…….=∂ Perf/∂Ck

• Cost functions are very non-linear and not well known• Pushing technology is very costly• Doing things for the first time is very costly

• Line Item Cost = (Fixed Cost) + n x (Unit Cost)• GRACE Satellite Subcontract

• Fixed cost = $11 M• Unit cost = $12 M / satellite• Better thermal control = $0.06 M total

• Build identical units. • Lower total Cost and fewer spares

Page 4: GRACE Mission: Architecture of the Flight Segment€¦ · 6 GRACE Mission The Seminal SST Gravity Mission Milo Wolff, MIT-SAO - JGR, Vol.,74, No. 22, Oct. 1969 • Two geometrically

4

GRACE MissionFocus

Heritage Gravity Missions all carried a Magnetometer• NASA's Gravity Research Mission (GRM) proposal - died 1985• ESA's Aristoteles proposal - died 1990 when NASA pulled out • NASA-GSFC's GAMES proposal died 1994• GFZ-Potsdam's CHAMP launched 2000

Heritage Gravity Missions Emphasized Spatial Resolution• GRM proposed to fly at an altitude of 156 to 170 km• Aristoteles proposed to fly at an altitude of 200 km

Page 5: GRACE Mission: Architecture of the Flight Segment€¦ · 6 GRACE Mission The Seminal SST Gravity Mission Milo Wolff, MIT-SAO - JGR, Vol.,74, No. 22, Oct. 1969 • Two geometrically

5

GRACE MissionCompeting Objectives

• Orbit Design• Magnetic field missions prefer an inclination of 85 degrees• Gravity mission prefer an inclination of:

• First choice - near 90 degrees• Second choice - sun-synchronous orbit at 97 degrees

• Structural Stability• Magnetometers want to be located on a long boom

• 1 nano-Tesla• A satellite for a Gravity Mission needs to be very stable

• 1 µm @ 2x per orbit, or 5E-12 m/s2 - .0002 to .04 Hz• Root Cause of the Problem: Organizational

• Funding for gravity missions came NASA’s Geo-potential Fields Program Office

Page 6: GRACE Mission: Architecture of the Flight Segment€¦ · 6 GRACE Mission The Seminal SST Gravity Mission Milo Wolff, MIT-SAO - JGR, Vol.,74, No. 22, Oct. 1969 • Two geometrically

6

GRACE MissionThe Seminal SST Gravity Mission

Milo Wolff, MIT-SAO - JGR, Vol.,74, No. 22, Oct. 1969• Two geometrically identical satellites • Equipped to measure relative velocity

∆U = Vmean orbital x ∆valong track

• 200-km separation - Altitude ≥ separation• USO + Transponded RF signal, or Laser doppler system

• Doppler (i.e. ∆valong track) sampled every 10 seconds

• Store and forward data to the ground

• Non-gravitational forces controlled by careful design and accounted for by modeling

Page 7: GRACE Mission: Architecture of the Flight Segment€¦ · 6 GRACE Mission The Seminal SST Gravity Mission Milo Wolff, MIT-SAO - JGR, Vol.,74, No. 22, Oct. 1969 • Two geometrically

7

GRACE MissionGRACE - How it Works

Microwave LinkTracking Phase - Range change24 & 32-GHz - Ionosphere Dual One-way - Clocks

GPS Relative ClocksLocation

Accelerometers -Non-Gravitational Forces

Star Cameras measure attitude

Mission Ops predicts the orbits for each GRACE

Each GRACE points at thepredicted location of the other GRACE

Page 8: GRACE Mission: Architecture of the Flight Segment€¦ · 6 GRACE Mission The Seminal SST Gravity Mission Milo Wolff, MIT-SAO - JGR, Vol.,74, No. 22, Oct. 1969 • Two geometrically

8

GRACE MissionGravity Research Mission -1985

Star CameraAssembly

ThrusterAssembly

Vector Magnetometer

Leading Satellite Only

Satellite-to-Satellite Doppler Antennas

Transmit

Receive

ThrusterAssembly

Fuel Tanks10.8 M

4.4 M

Solar Array

Unfriendly Features• 1200 kg of Hydrazine Fuel• Flexible Boom & Solar Arrays• Multipath on the SST RF link

Challenges• No feasible operational safe mode• Continuous Drag Compensation• Time synchronization

Dual One-Way Ranging Concept Developed at APL!

Page 9: GRACE Mission: Architecture of the Flight Segment€¦ · 6 GRACE Mission The Seminal SST Gravity Mission Milo Wolff, MIT-SAO - JGR, Vol.,74, No. 22, Oct. 1969 • Two geometrically

9

GRACE MissionOrbit Life & Mission Safety

0.01

0.1

1

10

100

150 200 250 300 350 400 450 500 550 600Altitude, km

Orbit Life,

months

GRM had 12:1 variation of Mass / Area

125250500100020004000

kg / m2

12 hrs

Average Solar�Conditions

5 yrsGRACE

Page 10: GRACE Mission: Architecture of the Flight Segment€¦ · 6 GRACE Mission The Seminal SST Gravity Mission Milo Wolff, MIT-SAO - JGR, Vol.,74, No. 22, Oct. 1969 • Two geometrically

10

GRACE MissionGA�MES - 1992

Instrumentation Concept • SubSatellite Retro Reflectors

• Size of a Soda Can • Aerodynamically stabilized• 2 units released sequentially

• Laser Ranging System • Pulsed at 2-GHz rate• 100 µ/s range rate

Challenges• Acquisition & tracking by the laser

ranging telescope• Sub-satellite aerodynamic stability

Unfriendly Features• Hydrazine Propulsion System• Flexible 6-M boom• Flexible Solar Arrays• Uncontrolled Non-gravitational

forces - aerodynamic

Page 11: GRACE Mission: Architecture of the Flight Segment€¦ · 6 GRACE Mission The Seminal SST Gravity Mission Milo Wolff, MIT-SAO - JGR, Vol.,74, No. 22, Oct. 1969 • Two geometrically

11

GRACE MissionCompetition vs. SST (Before GRACE)

0.001

0.01

0.1

1

10

100

1000

10000

0 60 120 180 240 300 360Degree

SSI @�500 km

300 km��SGG ��200 km�

SST @ 500 km, 400 km, & 300 kmKuala's�Pwr Law

Source: NRC,1997, Satellite Gravity and the Geosphere, Jean Dickey, etal.

EGM-96Geoid Height Error,�mm

Page 12: GRACE Mission: Architecture of the Flight Segment€¦ · 6 GRACE Mission The Seminal SST Gravity Mission Milo Wolff, MIT-SAO - JGR, Vol.,74, No. 22, Oct. 1969 • Two geometrically

12

GRACE MissionListen for Simple Truths

• Minimum Science Mission Objective - A moving target• Oceanography base

• 1994 Geoid with 5-cm accuracy cummulative to degree 50 • 1996 Geoid with 0.5-cm accuracy to degree 50

• Victor Zlotnicki casually commented "I wouldn't compromise the accuracy of a single low-degree term in order to improve the accuracy of the high-degree terms."• Our response was to develop performance specifications for

J2 - usually ignored by predecessors• Labrecque pushed the idea of using gravity to measure

time-varying geophysical parameters - Richard Gross, B. Chao etal., - "low-degree and order terms were significant"

• Brooks Thomas applied signal filter theory to the problem and showed how to improve SST performance @ all scales

Page 13: GRACE Mission: Architecture of the Flight Segment€¦ · 6 GRACE Mission The Seminal SST Gravity Mission Milo Wolff, MIT-SAO - JGR, Vol.,74, No. 22, Oct. 1969 • Two geometrically

13

GRACE MissionFocus on the Long Wavelength

10 -3

10 -1

10 1

10 3

10 5

100100010000Half Wavelength on the Earth's Surface ( km )

EGM96

Kaula's Mean Ocean

Ocean (Annual)Hydrology (Annual)

GRACE 300 km

GRACE 450 km

Power Law

Improved Knowledge

Source: UT-CSR 1998

deg 100deg 66

Page 14: GRACE Mission: Architecture of the Flight Segment€¦ · 6 GRACE Mission The Seminal SST Gravity Mission Milo Wolff, MIT-SAO - JGR, Vol.,74, No. 22, Oct. 1969 • Two geometrically

14

GRACE MissionAbandoned Orbit Design

• Baseline Co-planar Orbit has one drawback• The partial derivative of the m=n terms of the spherical

harmonics are ~zero for the baseline co-planar, polar, orbit

• Option for improvement• Offset the LAN's of the twin satellites• 40-km offset: Marginal improvement

• Drag & control penalty similar to the baseline• 200-km offset: Significant improvement

• Drag penalty is high• Exceeded out-of plane ACC performance• The plane change would be costly

200 km

Approaching the Descending Node

Leaving theAscending Node200 km

Page 15: GRACE Mission: Architecture of the Flight Segment€¦ · 6 GRACE Mission The Seminal SST Gravity Mission Milo Wolff, MIT-SAO - JGR, Vol.,74, No. 22, Oct. 1969 • Two geometrically

15

GRACE MissionImpact of the Advanced Digital Filtering

Center of Mass Control• ≤500 microns not good enough• ≤100 microns needed• Cost: $2,000,000 for on-orbit

adjustment • Cost $50,000 for tank valving

Accelerometer Performance• 10E-9 ms-2Hz-1/2 no longer good

enough• 10E-10 needed• Cost: $ 0.0 (available)

Digital Filtering the data by 335 • Incremental Cost: Worth it!

Higher Data Rate for ACC & K-Band data• Brooks wanted 50 Hz • Compromised at 10 Hz• Cost: $0.0

Attitude Control Pointing• ≤ 1 mr not good enough• ≤ 0.5 mr needed• Cost uncertain

Control on the PSD of the noise from attitude control • 20-mN thrusters too strong• 10-mN thrusters needed• Cost: $ 0.0 (available)

Page 16: GRACE Mission: Architecture of the Flight Segment€¦ · 6 GRACE Mission The Seminal SST Gravity Mission Milo Wolff, MIT-SAO - JGR, Vol.,74, No. 22, Oct. 1969 • Two geometrically

16

GRACE MissionLimiting Error Sources

Accelerometer

USO sans GPS

USO with GPS

Microwave

[Spectral Noise Density] 1/2

Microns

sec2 Hz1/2

0.001

0.05-Hz cut-off for low-pass digital filter

10 -7

10 -5

0.1

0.0001 0.001 0.01 0.1

Gravity-Signal Band, degree Š 100

Source: J.B. Thomas

Frequency, HzSOURCE: J.B. Thomas

Page 17: GRACE Mission: Architecture of the Flight Segment€¦ · 6 GRACE Mission The Seminal SST Gravity Mission Milo Wolff, MIT-SAO - JGR, Vol.,74, No. 22, Oct. 1969 • Two geometrically

17

GRACE MissionLimiting Errors Mapped to Geoid

1

10

100

0 10 20 30 40 50Spherical Harmonic Degree

Orbits: polar, coplanar, H = 300 km, R = 200 km Fit: 6.5-day up to degree 50, order 50

System-noise error for µwaveranging at λ= 1 cm with¦S

R = 1 µm/¦Hz for R = 200 kmG

eoid

Err

or p

er D

egre

e, M

icro

ns

= 10Accelerometer error, based onS a

-20 (1 + 0.005 / f ), f in Hz,per accelerometer, in m s Hz2 -4 -1

USO error with 0.5-MHz offsetτfor = 1, 10, 100, 1000 s

and (τ )*10 13 = 2, 2, 3, 5y

σ

The key to the long wavelength terms is the Accelerometer

The satellites must be mechanically quiet• Avoid Parasitic Harmonic

Oscillators• No rotating machinery • Limit Thrusting

• Heaters mounted on Low conductivity material - limit Lenz-Law effects

• Well staked cables

Page 18: GRACE Mission: Architecture of the Flight Segment€¦ · 6 GRACE Mission The Seminal SST Gravity Mission Milo Wolff, MIT-SAO - JGR, Vol.,74, No. 22, Oct. 1969 • Two geometrically

18

GRACE MissionFrench Electrostatic Accelerometer

70-gram Proof Mass• 1x 4x 4-cm Titanium block• Not cagedElectrostatic Suspension• 10-volt bias • 150-micron gap• 12-micron free motionPerformance • Noise 10-10 m/s2 Hz-1/2

• Full Scale 5x10-5 m/s2

Architectural Implication• No requirement for continuous

drag compensation!Source: ONERA

YAW

ROLLPITCH

Page 19: GRACE Mission: Architecture of the Flight Segment€¦ · 6 GRACE Mission The Seminal SST Gravity Mission Milo Wolff, MIT-SAO - JGR, Vol.,74, No. 22, Oct. 1969 • Two geometrically

19

GRACE MissionNon-Gravitational Effects

1 µm

10 µm

100 µm

1 mm

1 cm

10 cm 1.E-10

m/s^

21.E

-09 m

/s^2

1.E-08

m/s^

21.E

-07 m

/s^2

1 µgram 1 gram 1 kg

Mass

Non-Gravitational Forces• Solar pressure = 50E-09 m/s2• Drag @ 500 km = 1E-07 m/s2• Drag @ 300 km = 5E-06 m/s2Parasitic Harmonic Oscillators• @ frequency 0.1 Hz, 1-gram

parasitic oscillator with amplitude of 1mm results in a satellite acceleration of 1E-09 m/s2

Rotating Machines• Reaction wheel run at 600 to

3000 rpm• This is 10 to 50 Hz• Interferes with ACC control loops

they have a resonance at ~30 Hz

Page 20: GRACE Mission: Architecture of the Flight Segment€¦ · 6 GRACE Mission The Seminal SST Gravity Mission Milo Wolff, MIT-SAO - JGR, Vol.,74, No. 22, Oct. 1969 • Two geometrically

20

GRACE MissionControlling Torques

Front View

Microwave Horn

Side View

S-Band Antenna Winglets

Center of Mass

Astrium, GmbH

Thrusters (4 places)

Page 21: GRACE Mission: Architecture of the Flight Segment€¦ · 6 GRACE Mission The Seminal SST Gravity Mission Milo Wolff, MIT-SAO - JGR, Vol.,74, No. 22, Oct. 1969 • Two geometrically

21

GRACE MissionK-Band Ranging

XYZ

X Y

Z

24- and 32-GHzUnmodulated CarrierFrequencies separated by 670 kHz @ 32 GHz

Transmit and ReceiveSingle Corrugated HornLinear Polarization45°to Z-Axis

GRACE Satellites are twins

Transmit

Receive

Page 22: GRACE Mission: Architecture of the Flight Segment€¦ · 6 GRACE Mission The Seminal SST Gravity Mission Milo Wolff, MIT-SAO - JGR, Vol.,74, No. 22, Oct. 1969 • Two geometrically

22

GRACE MissionDual One-Way Ranging

~Cos ω t 2

USO-2

Mixer

~Power Amp Antennas

LNACos ω t 1

USO-1

+

timePhas

etime

Phas

e

timePhas

e

∂f/f = 10-13

SOURCE: C.E. Dunn

Page 23: GRACE Mission: Architecture of the Flight Segment€¦ · 6 GRACE Mission The Seminal SST Gravity Mission Milo Wolff, MIT-SAO - JGR, Vol.,74, No. 22, Oct. 1969 • Two geometrically

23

GRACE MissionThe Laser Interferometer Option

Advantages• The Transmit and Receive

frequency are the same• Potential to Improve

Ranging performance for the longest wave length terms

Microwave Offsets• Lowered the offset between

K-Band frequencies to under 1 MHz

• Spitzmesser showed it could be done

Challenges in 1996• Frequency stability 1E-12

was not demonstrated• SIM was working on a

cavity stabilization approach objective 1E-11

• Needed arc-second level pointing to make fringes• An optical concept with

less stringent pointing rqt had poor SNR

Abandoned after a 6 week preliminary design effort

Page 24: GRACE Mission: Architecture of the Flight Segment€¦ · 6 GRACE Mission The Seminal SST Gravity Mission Milo Wolff, MIT-SAO - JGR, Vol.,74, No. 22, Oct. 1969 • Two geometrically

24

GRACE MissionRisk Containment

Level of Integration into the I�PU• GPS• K-band Tone Tracking• Timing Signals• Star Camera Image Processing

Star Camera Configuration

Redundancy

Page 25: GRACE Mission: Architecture of the Flight Segment€¦ · 6 GRACE Mission The Seminal SST Gravity Mission Milo Wolff, MIT-SAO - JGR, Vol.,74, No. 22, Oct. 1969 • Two geometrically

25

GRACE MissionLevel of IPU Integration

K-band ToneTracking

• Essential integration to achieve 100 psec timesynchronization

Timing Signals1-Hz OBDH

• Synchronize telemetry and command with theinstrumentation

Timing Signals10-Hz ACC1-MHz ACC

• Required to synchronize the10-Hz ACC data with the10-Hz K-Band ranging data. Simplifies the digitalfiltering of the data by the Science Data System

Star CameraImageProcessing

• Intel 486 micro-processor from DTU Ğ expected similarproblems to the 603e used in the BlackJack

• Utility of K-band data depends on star camera data• Unit cost of Processors > $250,000 (needed at least 4)

Page 26: GRACE Mission: Architecture of the Flight Segment€¦ · 6 GRACE Mission The Seminal SST Gravity Mission Milo Wolff, MIT-SAO - JGR, Vol.,74, No. 22, Oct. 1969 • Two geometrically

26

GRACE MissionStar Camera Configuration

• Two Star Cameras 45 degrees to Zenith - Camera pointed away form the Sun is "Prime" and used by AOCS.• Simultaneous Sun and Moon blinding in both occurs monthly• Simply letting the satellite float with control actuators OFF

works for 5- to 8-minute moon intrusions in the "prime camera"

• Every 160 days, the sun shifts from one side of the satellite tothe other. Prime camera must be switched at this point.

• If one camera fails, the IMU provides an inertial reference during those periods when the Sun interferes with the only camera.

• If the both the IMU and a camera fail on one Satellite, then leading satellite must switch places with the trailer

• Three- & Four-camera options abandoned -• Packaging close to the ACC was too difficult

Page 27: GRACE Mission: Architecture of the Flight Segment€¦ · 6 GRACE Mission The Seminal SST Gravity Mission Milo Wolff, MIT-SAO - JGR, Vol.,74, No. 22, Oct. 1969 • Two geometrically

27

GRACE MissionCold Gas Sub-System

Twelve 10-mN Thrusters �Two 40-mN Thrusters

Regulators

Two Tanks

Solenoid Valve

Twin HP Latch Valves

LP Latch Valve

Center of Mass Stability • CHAMP manifolds the two tanks

together and has one high pressure regulator & 2 low pressure latch valves

• 1°K ∆T between Tanks moves the CoM 80 µm

GRACE Dual-String Architecture • No mass exchange between tanks

from ∆T• Redundant regulators• Compensates for tuck-open thruster• X-axis CoM is controlled by single

string operation of orbit control maneuvers