Mission Concept Study Robin Stebbins Study Scientist Ninth LISA Symposium Paris 22 May 2012 Outline Goals Elements of the study Context of the study Responses to the RequestForInformation RFI ID: 794786
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Slide1
NASA’s Gravitational-Wave Mission Concept Study
Robin Stebbins, Study ScientistNinth LISA SymposiumParis, 22 May 2012
Slide2OutlineGoalsElements of the studyContext of the study
Responses to the Request-For-Information (RFI)Science performance analysisAssessment of architecturesRiskCost2This document contains no ITAR-controlled information and is suitable for public release.
Slide3Goals of the StudyDevelop mission concepts that will accomplish some or all of the LISA science objectives at lower cost points
.Explore how mission architecture choices impact science, cost and risk.Big QuestionsAre there concepts at $300M, $600M or $1B?What is the lowest cost GW mission?Is there a game-changing technology that hasn't been adequately considered?3This document contains no ITAR-controlled information and is suitable for public release.
Slide4Elements of the StudyRequest for Information (RFI) – due Nov. 10
th.Core Team – ~25 GSFC, JPL & university scientists and engineers critically reviewing RFI responsesScience task force – ~15 volunteer scientists evaluating science performance of conceptsCommunity Science Team (CST) – 10 scientists, Rai Weiss, Ned Wright co-chairsPublic workshop – December 20-21st Concurrent engineering studies by JPL’s Team-X in March and AprilFinal Report to NASA Headquarters – July 6thPresentation to the Committee on Astronomy and Astrophysics (CAA) of the National Research Council (NRC)This document contains no ITAR-controlled information and is suitable for public release. 4
Slide5Context of the Study – A Brief History of LISA
1974 - A dinner conversation: Weiss, Bender, Misner and Pound1985 – LAGOS Concept (Faller, Bender, Hall, Hils and Vincent)1993 – LISAG - ESA M3 study: six S/C LISA & Sagittarius1997 - JPL Team-X Study: 3 S/C LISA 2001-2015 - LISA Pathfinder and ST-7 DRS2001 – NASA/ESA project began2003 – TRIP Review2005 – GSFC AETD Review2007 – NRC BEPAC Review2009 – Astro2010 Review2011 – NASA/ESA partnership ended2011 – Next Generation Gravitational-Wave Observatory (NGO) started2012 – ESA L1 downselect5
This document contains no ITAR-controlled information and is suitable for public release.
Slide6Context of the Study – Activities in Europe
LISA PathfinderDemonstration of space-based GW technology, in late stages of I&T2014 launchTechnology developmentInertial sensor electronics, charge controlOptical systemLaser systemPointing and point-ahead mechanismsNGOHighly developed concept with extensive science case and technical detail6This document contains no ITAR-controlled information and is suitable for public release.
Slide7Context of the Study in the U.S.Next major mission in Astrophysics starts after 2018.
The Astrophysics Division anticipates that a “probe-class” mission could be started ~2017.The Division will not commit to a ‘large’ mission until after Astro2020. ‘Commit’ means the Confirmation Review at the end of Phase B.A partnership with ESA seems highly likely. That would require:Rebuilding a partnershipReliably coordinating two agencies’ programs7
Slide8RFI Responses
8
Slide9RFI Responses17 responses total12 for mission concepts, several with options
3 for instrument concepts2 for technologiesFour natural groupsNo-drag-free concepts (2)Geocentric orbits (4)LISA-like (5)Other (2)9
Slide10What constitutes “LISA-like?”Drag-free controlFree-falling test mass
Precision stationkeepingContinuous laser rangingHeliocentric orbitsConstellation in stable equilateral triangleNo orbital maintenanceMillion-kilometer long armsLaser frequency noise subtraction (TDI)Emulate Michelson’s white-light fringe condition through post-processing10
Slide11No-Drag-Free Concepts
11
Slide12No-Drag-Free ConceptsRely on either very long arms (50X LISA) or geometry (100X reduction) to compensate for using the spacecraft as the test mass.
Disturbances are solar radiation pressure variability, solar wind, interplanetary magnetic fieldMeasure, model and correct for spurious forces (102 - 104 X)Displacement noise from motions of the spacecraft CG, owing to, say, thermoelastic effectsConcerns about measuring solar wind and modeling/testing other disturbance (e.g., Pioneer effect)12
Slide13Geocentric Concepts
13
Slide14Geocentric ConceptsNoise concerns
Thermal environment: moving sub-Sun point, eclipsesSun in the telescopeVarying Earth albedoGeosynchronous may have interesting modulation properties. (McWilliams’ talk Thursday afternoon)LAGRANGE/Conklin described by Buchman Tuesday afternoon.A big cost question: can you do this for a factor of 4 less by employing nanosat technology, lower reliability standards, standard bus, a different way of doing business, … a different business model?14
Slide15LISA-like Concepts
15
Slide16LISA-like ConceptsHow far can the LISA architecture be descoped
?No technical or performance issuesScience performance falls off much faster than cost Found the bottom!See Jeff Livas’s talk Tuesday afternoon in LISA-NGO Technology session.16
Slide17Other Concepts
17
Slide18Other ConceptsThe superconductor idea doesn’t work.
Atom InterferometryAtoms clouds as test massesAtom interferometer as a phasemeterSee John Baker’s talk Thursday afternoon in Other Experiments and Alternative Design sessionInSpRLMost aggressive design conceptInvoked ‘superclocks’ and resonanceSeems to require a few orders of magnitude improvement in several key performance parametersLacks enough definition to evaluateYu concept doesn’t promise to be cheaper.Digital Interferometry is interesting.18
Slide19Science Performance
Analysis19
Slide20Science Performance
20Volume of the Universe exploredDetection numbers for source populations (Massive BHs, EMRIs, Galactic Binaries)Discovery spaceParameter resolutionAll work done by Neil Cornish and the Science Task Force. See Cornish talk, Friday morning.
Slide21Sensitivity Curves – All 15 Concepts
21
Slide22Massive Black Hole Horizons
22
Slide23Massive Black Hole Horizons – No-Drag-Free
23
Slide24Massive Black Hole Horizons – Geocentric
24
Slide25Massive Black Hole Horizons – Geosynchronous
25
Slide26Massive Black Hole Horizons – LISA-Like
26
Slide27Detection Rates – Large Seed Models (/yr)
27
Slide28Detection Rates – Small Seed Models (/yr)
28
Slide29EMRI Horizons
29
Slide30EMRI Detections
3010 M⊙ compact object, eccentricity 0.5 at 2 yrs to plunge, spin 0.5 central BH, SNR=15
Slide31WD-WD Detection Numbers
31
Slide32Parameter Estimation – LISA-like Concepts
32Similar detection numbers, but each descope x 3-10 loss in resolution
Slide33Architecture Choices
33
Slide34Architecture Choices – Mission DesignHeliocentric – fixed, drift-away, in-line, L2/leading/trailing, 1 AU
Geocentric – OMEGA, geosync, L3/L4/L5, LEOCompare delta-v, constellation stability, propellant, thermal, modulation of science signal, comm34
Slide35Architecture Choices – Inertial ReferenceProof mass – cubical, parallelepiped or spherical free-
falling, or torsion pendulumSpacecraft center-of-gravity (aka no-drag-free) with modeled correctionsAtom interferometry - atoms as proof masses, atoms as secondary inertial referencePayload as separated spacecraft35
Slide36Architecture Choices – Measurement StrategiesLaser interferometry with laser heterodyne phase comparison – free-space or digital
interferometryLaser interferometry with atom interferometer phase comparisonLaser and clock frequency noise correction – 3 spacecraft & TDI, or very much better phase reference (AI)36
Slide37Implementation Strategies
37
Slide38Implementation Strategies
38ParameterSGO MidLAGRANGEOMEGAMass Margin53%
53%
53%
Payload mass (kg), power (W) CBE
216.5 kg, 233 W
99.7 kg, 99.3 W
Option 1:
64.3 kg, 80W;
Option 2:
55 kg, 54W
Mass rack-up
Science-craft type 1
Science-craft type 2
Propulsion Module type 1 + Prop
Propulsion module type 2 + Prop
LV Adapter
Launch Mass Wet
717
kg (3)
661 + 139 (3)
?
4553 kg
531
kg (2)
586 kg (1)
224 + 174 (2)
591 + 114 (1)
32 kg
3182 kg
147
kg (6)
374 + 465.5 (1)
28 kg
2347 kg
Launch Vehicle
Atlas V 551;
6075
kg
Atlas V 511;
3285
kg
Falcon 9 Block
2;
2490 kg
Slide39Risk
39SGO-Mid/HighLAGRANGEOMEGAThese are a combination of Team-X and Core Team risks.Risk rises rapidly with modest (<10%) cost reductions.This assessment is not complete.
Slide40CostTeam-X is very conservative.
Cost estimates range from $1.2B to 2.1B.Per science year costsSGO-hi $450M/yr SGO-mid/Lagrange ~$800-900/yrOmega ~$1,300M/yrImportant cost driversNon-recurring costs (NRE) and recurring costs (RE) are important.Design validationSerial vs parallel construction of multiple units (~$150M/yr)40
Slide41SummaryThe CST prefers SGO-Mid (3 arms, LISA-like, 1 Mkm
, drift-away).Big QuestionsWe found no concepts at $300M, $600M or $1B.The lowest cost GW mission is ~$1.4B (±0.2).We found no game-changing technology that hasn't been adequately considered.Heliocentric is a better choice than geocentric.Three dual-string spacecraft appear to be more robust than six single-string spacecraft.No-drag-free achieves only modest savings while incurring substantial risk. [Cost model is uncertain.]Three arms has lower risk and mediating cost factors relative to two arms.41
Slide42Backup Slides
42
Slide43FeedstockWhitepapers (17x~15 pages = 235)
Workshop Presentations (~20 x 30 charts = 600)Core Team Work (~200 pages)Team-X inputPresentations (4 x ~60 charts = 240)Master Equipment ListsFunctional Interface DiagramsCAD filesOrbit analysesTeam-X outputViewgraphs (~3 x 280 = 840)Team-X reports (~3 x 10-20 = 45)CST Work (~50 pages)Total: north of 2230 pages43
Slide44Mission Design Review 1/2
44 FeatureSGO-MidLagrangeOmega 1. Trajectory Phase DV
[174, 153, 200]
m/s
Stack ~ 120 m/s to L2
[SC1,
3
]: [460, 300
]
[206, 328, 450] + 4 m/s
vs.
3
210 m/s if 3 PMs
Significance: Prop module size(s), Total mass, Launch
vehicle
2. Trajectory
Phase
D
t
17 months
27 months
12 months (
vs. ~ 7
)
Significance: Cost/complexity of trajectory phase operations (FDF & Ops)
3. Lunar Flybys Used
No
Yes
No
Significance: Cost/complexity/risk of trajectory phase operations (FDF & Ops)
4. Mission Phase
D
t
2 yr / extendable
2 yr /
not
extendable
1 yr / extendable
Significance: Cost of science operations, Amount of science, Constellation
Stability
5.
Const. Stability
D
L/L,
Da
,
Dn
, (
Dg
||
,
Dg
+
)
±0.007, ±0.6
, ±1.5
Mhz
,
±(0.008, 1.0)
m
rad
±0.1, ±0.12
, ±94
Mhz
,
±(0.8, 0.32)
m
rad
±0.025, ±2.2
, ±60
Mhz
,
±(0.17, 0.15)
m
rad
Significance: Cost of additional mechanisms and electronics
6.
Mission Phase
D
V
No
Yes (SC2)
No
Significance: Cost/sophistication of
mN
-thruster system (~ 10 m/s/yr)
Slide45Mission Design Review 2/2
45 FeatureSGO-MidLagrangeOmega 7. Distance to Earth /
HGA, ISC
req
?
24 to 55
10
6
km /
HGA
[21, 1.5,
21
]
10
6
km
HGA/LGA,
ISC/LGA
0.6
10
6
km
LGA
Significance: Cost/complexity of communications;
ISC = inter-spacecraft comm.
8.
GeoEcliptic
Orbit
No
No
Yes
Significance: (a) Sun direction variation
(thermal stability)
(b) Sun in telescope aperture (thermal, optical interference)
(c) Earth eclipses (thermal, science interruptions)
Feature
SGO-Mid
Lagrange
Omega
9.
Launch Vehicle C3
+0.27 (km/s)
2
-0.3 (km/s)
2
-0.05 (km/s)
2
Significance: Launch vehicle selection
10.
Single Prop Option
No
(
?
)
Yes (but not necessary)
Yes (but not necessary)
Significance: Input to possible trade for single prop module cost savings (?)
11.
“FDF” Ops Cost
$ 18
M
$ 27
M
$ 23
M
(?
if 3 PMs
)
Cost Drivers: Trajectory and mission phase durations, trajectory complexity