The Lunar Farside: A Science and Exploration Imperative · 2019. 2. 5. · High-Level Trade Space...

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1 Lunar Science for Landed Missions Workshop,10-12 January 2018 The Lunar Farside : A Science and Exploration Imperative Lunar Science for Landed Mission Workshop NASA Ames Research Center, 10 - 12 January 2018 Jack Burns and Raul Monsalve University of Colorado Boulder Abhirup Datta Indian Institute of Technology, Indore A NASA-funded SSERVI Team

Transcript of The Lunar Farside: A Science and Exploration Imperative · 2019. 2. 5. · High-Level Trade Space...

Page 1: The Lunar Farside: A Science and Exploration Imperative · 2019. 2. 5. · High-Level Trade Space for Lunar Radio Telescopes Deployment Environment Power Location Communications Instruments

1Lunar Science for LandedMissionsWorkshop,10-12 January 2018

TheLunarFarside:AScience

andExplorationImperative

LunarScienceforLandedMissionWorkshopNASAAmesResearchCenter,10-12January2018

JackBurnsandRaulMonsalveUniversityofColoradoBoulder

AbhirupDattaIndianInstituteofTechnology,Indore

ANASA-fundedSSERVITeam

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WhytheLunarFarside?

• Awholenew,unexploredworldinEarth’sbackyard!Nearly4× landareaoftheUnitedStates.

• Opportunitytodemonstratehuman-roboticexplorationstrategiesneededtoexploretheMoon,asteroids,&Mars.

• Farside includestheSouthPole-Aitkenbasin– largest,deepest,&oldestimpactbasinintheinnersolarsystem.

• Farside alwaysfacesawayfromEarthandistheonlypristineradio-quietsitetopursueobservationsoftheearlyUniverse’sCosmicDawn.at?~10-80MHz.

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WhyEmplaceRadioTelescopesontheFarside?

• Earth’sIonosphere(e.g.,Vedantham etal.2014;Dattaetal.2016;Rogersetal.2015;Sokolowskietal.2015)

o Refraction,absorption,&emission.o Spatial&temporalvariationsrelatedtoforcingactionbysolarUV&X-rays

=>1/forflickernoiseactsasanothersystematicorbias.o Effectsscaleasν-2 sotheygetmuchworseapproaching10MHz.

• RadioFrequencyInterference(RFI)o RFIparticularlyproblematicforFMband(88-110MHz).o ReflectionofftheMoon,spacedebris,aircraft,&ionizedmeteortrailsare

anissueeverywhereonEarth(e.g.,Tingayetal.2013;Vedanthametal.2013).

o EveninLEO(108K)orlunarnearside(106 K),RFIbrightnessTB ishigh.NeedtosuppressRFIbyatleast-80dBtoobservecosmologicalsignal.

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AstrophysicsCommunitySurveysAdvocatefor

LowRadioFrequencyCosmologyontheFarside

Publications:o Burnsetal.2013,Adv. SpaceRes.,52,306.o Lazio,MacDowall,Burnsetal.,2011,Adv.Space

Res.,48,1942

•Astrophysics Decadal “New Worlds, NewHorizons”: “A great mystery now confrontsus: When and how did the first galaxies formout of cold clumps of hydrogen gas and startto shine—whenwas our Cosmic Dawn?”

•NASA Astrophysics Division Roadmap(2013): HowDoes our UniverseWork?•Small Mission: “Mapping the Universe’shydrogen clouds using 21-cm radio wavelengthsvia a lunar orbiter observing from the farside ofthe Moon”.•Visionary Era: “Cosmic Dawn Mapper (21-cmlunar surface radio telescope array) … Detailedmap of structure formation in the Dark Ages via21-cm observations”.

SurfaceTelerobotics Deployment

Astronaut-assisted Deployment

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High-LevelTradeSpaceforLunarRadioTelescopes

Environment PowerDeployment

CommunicationsLocation

Instruments

RFI

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InstrumentsHydrogenCosmologyGlobalSignalTelescope

CosmicDawnMapper

• 10-100MHz• Polarimeter• GroundPlane• Operation temperature=-250Cto+150C

• Power<200W• Datastorage(<1GBper24hr)• Datatransmission(<1GBperday)

• At10MHz,1° resolutionrequires~2kmbaselines

• Filledaperture:1element/3600sq.m• Circlelayout:1element/6meters

• 105 squaremeterscollectingarearequires>1000dipoles

• 1000dipoles*2pol*20MHzbandwidthà~40GB/s

• Power~2.5kW

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CanaLowFrequencyAntennabeSitedina

PolarCrater?

Receiver

Batteries

Antenna

Solarpanels CommunicationAntenna

1-m

HitbySunlight(Periodicallyorcontinuously)

NoSunlightEverCrateratLunarNorth/SouthPole

UndergroundforhigherandmorestabletemperaturesSideview

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RadioFrequencyInterference(RFI)withina

craterattheLunarPole

NO NPQR SR

U = ℎ2

X

1

NO

+1

NP

SimulatingRFIinapolarcrater,withtheedgeofthecraterasaknife-edge.Thetransmitter(TX)isonEarth,andthereceiver(RX)isinthecrater,atadistanceNP fromtheedge.TheRFIattenuationatRX iscomputedusing:

\ = 0, _`U < 0

\ = 6 +9U + 1.27Uf, _`0 < U < 2.4

\ = 13 +20 log U , _`U > 2.4

Attenuation

Problems:• Insufficient attenuation• Crater rimblockssky&corrupts

antennabeam.

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GlobalFarside RadioFrequencyInterference

Fromsimulation byDattaetal.(2018).Atlatitudeof-80° andfrequencyof1MHz,-80dBisachievedat≈45° fromthelunarlimb

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RFIConstraintsonTelescopeLocation

=>Northeasternquadrant ofSchrödingerimpactbasinissufficientlyquiet.

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• Data are required for the electricalconductivity & permittivity of the regolith,to model the response of low-frequencyantennas.

• On dayside, UV & X-rays positively-chargesurface with 1–5 V whereas nightside hasnegative surface potential with ≳-500 V.Charged dust grains are levitated (Fig. 1).

• Changes in surface potential by 10x occurduring solar energetic particle event

=> Need to stay grounded to plasma.• Elevated dust (Fig. 1) can cause visibilityproblems, especially for teleoperation.

• Strong electric fields occur in terminator &shadowed regions. Gradients causenegatively charged particles to accelerateaway from the surface (Fig. 2). Effect onelectronics mitigated by placing electronicsunderground (<1 m), & within Faradaycages.

Figure1. Top: ObservationsofelevateddustbySurveyor(Colwell2007).Bottom:Lunarsurfaceispositivechargedondayside&negativelychargedonnightside (Farrelletal.2007).

Figure2.Localizedelectricfieldeffects(Farrelletal.2007).

TheLunarEnvironment

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Longitude-averagetemperaturemodel(Source:LRODiviner)

Day

TheLunarEnvironmentSurfaceTemperature(K)

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Power,Communications,andtheDeep

SpaceGateway

PowerRequirement:0.2– 2.5kW• Assumingaboveaccountsforinstrumentandthermalcontrolelectronics.

• Battery+solarpanels(outsidecraterifnecessary).

• RTG(radioactive).• PowerbeamedfromDeepSpaceGateway.

Communications

• UseDeepSpaceGatewayascommunicationrelayforfirstgenerationinstruments.

DataDownlinkRequirement:<1GBper24hr to40GB/sec

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Summaryand Conclusions

• LunarFarside is theonlylocationintheinnersolarsystemquietenoughtoconductobservationsofCosmicDawndownto~10MHz.

• Possibleinstruments:SingleantennaforGlobal21-cmSignalandArrayofDipolestomeasurethespatialstructureintheearlyUniverse.

• Polar cratersdonotprovideenoughattenuationofRFIforsitingalowfrequencyradiotelescope.

• But,locations<80° latitudeand45° fromthelunarlimbonthefarside aresuitablesites.ThisincludesaNEquadrantofSchrödinger.

• Lunarenvironment:• Elevateddustandchangesinsurfacepotentialarepossibleissues.Needtostaygroundedtolocalplasma.Sitingelectronicsbelowgroundand/orinFaradaycagesareprobablyneeded.

• Day/nighttemperaturevariationsareanissue,butforelevations<70° temperaturesvaryfrom0℃ to-150℃.

• Power,communication,anddeploymentofaninitiallowradiofrequencyobservatorycanbefacilitatedbytheDeepSpaceGateway.