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Sizing of "Mother Ship and Catcher" Missions for LEO Small Debris and for GEO Large Object Capture John B Bacon, Ph.D. NASA Johnson Space Center Abstract: Most LEO debris lies in a limited number of inclination "bands" associated with specific useful orbits. Objects in such narrow inclination bands have all possible Right Ascensions of Ascending Node (RAANs), creating a different orbit plane for nearly every piece of debris. However, a low-orbiting satellite will always phase in RAAN faster than debris objects in higher orbits at the same inclination, potentially solving the problem. Such a low-orbiting base can serve as a "mother ship" that can tend and then send small, disposable common individual catcher/deboost devices--one for each debris object--as the facility drifts into the same RAAN as each higher object. The dV necessary to catch highly-eccentric orbit debris in the center of the band alternatively allows the capture of less-eccentric debris in a wider inclination range around the center. It is demonstrated that most LEO hazardous debris can be removed from orbit in three years, using a single LEO launch of one mother ship--with its onboard magazine of free- flying low-tech catchers--into each of ten identified bands, with second or potentially third launches into only the three highest-inclination bands. The nearly 1000 objects near the geostationary orbit present special challenges in mass, maneuverability, and ultimate disposal options, leading to a dramatically different architecture and technology suite than the LEO solution. It is shown that the entire population of near-GEO derelict objects can be gathered and tethered together within a 3 year period for future scrap-yard operations using achievable technologies and only two earth launches. https://ntrs.nasa.gov/search.jsp?R=20090041616 2018-08-22T00:52:10+00:00Z

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Sizing of "Mother Ship and Catcher" Missions for LEO Small Debris and for GEOLarge Object CaptureJohn B Bacon, Ph.D.NASA Johnson Space Center

Abstract:Most LEO debris lies in a limited number of inclination "bands" associated with specificuseful orbits. Objects in such narrow inclination bands have all possible RightAscensions of Ascending Node (RAANs), creating a different orbit plane for nearlyevery piece of debris. However, a low-orbiting satellite will always phase in RAANfaster than debris objects in higher orbits at the same inclination, potentially solving theproblem. Such a low-orbiting base can serve as a "mother ship" that can tend and thensend small, disposable common individual catcher/deboost devices--one for each debrisobject--as the facility drifts into the same RAAN as each higher object. The dVnecessary to catch highly-eccentric orbit debris in the center of the band alternativelyallows the capture of less-eccentric debris in a wider inclination range around the center.It is demonstrated that most LEO hazardous debris can be removed from orbit in threeyears, using a single LEO launch of one mother ship--with its onboard magazine of free-flying low-tech catchers--into each of ten identified bands, with second or potentiallythird launches into only the three highest-inclination bands.

The nearly 1000 objects near the geostationary orbit present special challenges in mass,maneuverability, and ultimate disposal options, leading to a dramatically differentarchitecture and technology suite than the LEO solution. It is shown that the entirepopulation of near-GEO derelict objects can be gathered and tethered together within a 3year period for future scrap-yard operations using achievable technologies and only twoearth launches.

https://ntrs.nasa.gov/search.jsp?R=20090041616 2018-08-22T00:52:10+00:00Z

Sizing of"Mother Ship and Catcher" Missions

LEO Small DebrisGEO Large Object Capture

John B. Bacon Ph.D.NASA JSC/OM3

2101 NASA ParkwayHouston, TX 77058

(281) 244-7086

Release Approvals

• The contents of this presentation are in thepublic domain and maybe used freely withappropriate citation.

• The satellite catalog data contained hereinhas been approved for public release by:

GHQ AFSPC/XOCS150 VANDENBERG ST. STE 1105PETERSON AFB, CO 80914-4220

• The analyses contained herein have beenapproved for public release by NASAIJSC

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Outfine.Alr

• Characteristics of LEO Debris Inclination Bands• Relative drift of orbital planes• Rendezvous or Intercept?• Reachable width of the debris band• Post-capture flight plan and functions• Mother-ship functions• Special Case: GEO sizing

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Perigees of Objects in Band Centers Perigees of Objects Not Within 2 deg of Band Centers

0 10 20 30 40 50 60 70 80 90 100

Inclination (deg)

600

500

400

Y

CJ300

bA^L

a200

100

0

The Big Picture of LEO Debris BandsPerigee (e700 km) vs. Inclination

700

600

• Bands are evident in scatte500

plot of perigee vs. Y 400

inclination 300a

• 10 bands hold the major 200

100

fra tion of debris objects 0 04 Remainder is also banded

20 40 60 80 100 120 140 160

Inclination (deg)

.. •♦ •♦ ♦ Eqq

<^

• ^• •• q

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♦ ^ s

C • ♦ ^.

♦ ♦ •^•^ ♦ ♦^tip

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700

600

500

400mmP

CL

300

200

100

0

♦ USA

q CIS

PRC

ESA

Other•Ind is

•Japan

Sources by Launch Nation;

Sources of Objects in Debris Bands

0 10 20 30 40 50 60 70 80 90 100

Inclination (deg)

[email protected] 244-7086

and- Lac Ana tion;Eccentricit

=oo4 1O°

Y.

o ^s0004Q ^o^^o

^

- - - _- - A IFogee 5 and Pel l igees in E3 p^ bris B ids-

Low inclination bands are— d minat^^^g y^trsc— 0. US

High inclination bands are— ominated-by--low eccentrics# ,

orbits

-0000 001"

s

r _

700

600g

^S ♦ o500 --♦ USA

400 -- o CIS^ 8 ^ 1 PRG

^^ ^^ 0 1 ., ESA300 - q► <` other

p ^- ^Jap ariO

200

n100 -

TT It TT irO7° 0 25° 1 287 62.5° 1 65° 74° 82°

9098°

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Sizing the Catcher• Cost of catcher HW/Firmware is a mission cost

driver♦ Cost of propellant is negligible as long as resulting mass budget

does not challenge required performance of HW/firmware.^ Cheap and dumb HW is preferable to light and expensive, up to a point.^ Prefer catcher net cost <$1000 USD each. (=$13.2M for catchers for all LEO tracked debris)

• Prefer one mother ship per inclination band♦ second largest cost driver is the launcher.♦ (Launcher capability)/(number of objects in band) is thus a major

sizing determinant.• How many can we catch?

♦ Rocket equation for 3000 m/sec:Mf/Mo=EXP(-3000/g*ISP) 22% for 200 ISP monopropellant_ -as sume monopropellant for design simpGcity/weight

A 10 kg initial mass catcher can have 2.2 kg of infrastructure & payload at capture in this scenario

A comprehensive satellite can be packaged in this sort of mass.

♦ After optimizing prop loading per object, 13200 objects can be caught* from 10"mother ships" at this dry catcher mass.

cL- *Immediate propulsive de-orbit is possible for many (but not all) objects.*Drag enhancement to accelerate natural decay is a solution for large debris objects

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0 20 40 60 80 100 120

n

w

Inclination

Fast Intercept or Slow Catch?Precession Rates in Deg/Day

• High eccentricity dominates the long-duration population♦ Small inclination differences within the band add quickly to required dV

• RAAN and Mean Anomaly precess at a fixed ratio for any inclinationtw

W

S^2, JZ = -2.06474 * 10 14 a -^^^ ^l - e^^ cos(i)[deg/ day

6J2 = +1.03237 * 10 14 a -' /2 (l - e2 Y

2 [4 - 5 sin e (1)][deg/ day]** from Larson and Wertz, Space Mission Analysis and Design (9992) p141

,Y= Cannot simultaneously solve the mother ship solution for hundreds of target objectsd Particularly near 63.43 deg where mean anomaly is stationary

Therefore, must circularize the mother ship orbit, and launch catcher into co-elliptic elliptic orbit forbest use of dV budget and minimum time-of-missionGenerally, better for mass budget and mission duration to launch mother ship to as low as possiblecircular orbit, and make up dV difference with catchers.

• Delta-Vs associated with intercept from low-circular are many km/sec• Safe capture is crucial: sizing/strengths of capture system and precise high-

speed targeting dominate the mass budget and complexity/risk in "intercept"scenarios

• To simplify and lighten the catcher and to avoid export control issues, a lowrelative velocity is necessary (==Slow Catch)♦ May as well rendezvous♦ Small prop reserve budget provides ballistic margin for timing, repeat attempts, and

often for immediate debris [email protected] 244-7086

Loglo(RCS m2) for 7 0 Band Objects2

1.5

1

0.5

V 0

-0.5

O 1

-1.5

-2

-2.5

3

Object Count

Radar Cross Section Average (M2)

y

98765

4

3

2

1

0

Size Distribution in Bands(Radar Cross Section is surrogate for size:L oglo(RCS) plotted)

Log1O(RCS m2) for 980 Band Objects2

1

V 0eH 'tl- n O M lD M N V9 00 rl ^ n O CO k.0 M N Ill 00 . - , n

M tD O M lD M M lD M M lD M M ID M N lD M N l0 M NN Izr r- M -1 M lD 00 O M Ln r- O N -It r- M -1 -'t l0 00 -1O N N N N M M M M M '^Y V ^ Ir LA

J _ _

-2 -

-3 -

Object Count

Size distribution moves from larger tosmaller as inclination increases

Band7 Band band Band Band Band Band Band Band Band

25 28.5 39.5 51.6 62.5 65 74 82 98

Debris Band

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Relative Drift Rate to Circular at Perigee

—*-Relative Drift

Phasing Rate

—2.06474 1014 a -'/2 cos(il 1— e 2 2[deg/ day] 0 \Io J

S2 relative = —2.06474 * 10 14 cos ( i ll '^ a1 -' /2 1 — e 1 2 2 - a

n

_7/2 1 — e 0

2 -2l

* from Larson and Wertz, Space Mission Analysis and Design (9992) p141

• At any higher orbit a 1 >ao (especially with higher eccentricity)an object's absolute phase rate compared to a lowercircularized-orbit object (ao) will be asymptotically 1closer to zero, and differential drift rate

0.8

approaches D7x 0.6

o 0.50.40.30.20.1

0

0 1 2 3 4 5 6 7 8

Apogee/Perigee

• Because of differential drift, the orbit planes of the debris object and of the lower mothership slowly move through periodic alignment

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10.9

W 0.8

L 0.70.60.5a,0.40.30.20.1

00 1 2 3 4 5 6 7 8

Apogee/Perigee

Differentia/ Phasing Rate

• Slow phase rates & small altitude differences at high inclinations may demandadditional missions to rotated orbit planes to shorten program duration

• Particularly useful move considering quantities of high-inclination objects

Relative Drift Rate to Circular at PerigeeBand Center w Years to Lap

360 Deg

-2.0 4-M 0.4

2 -187 3.21 0.5

2 -1.8 2.9 0.5

3 -1.6 2.0 0.61

51. -1.2E 0.9E 0.7

6 -0.97 0.11 1.0

-0.8 -0.11 1.1

74 0. -0.6 178 -0.2 -0.9 3.4

9 0.2 -0.9 3.4

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High d V A flo ws Wider Bands(lower out-of-plane objects reachable, as well as

higher in-plane objects)

dV vs Inclination from Nearest-Band LEO Orbit3000

X q

q

zsooEl

c

c1^t

q

tK

<X1 c0

2000

0 q

^e +

0 ^^ c q qC^ 0

£ 1500y^

a <\ C C - C^

<\E]X

<i c0 X

Elc

1000c

<^

500

X [Ell +d

q Q

0

0 USA

q a5_^ PRC

X ESA

X Other

Olndia

+Japan

0 20 40 60 80 100

Incination (deg)

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6000

5000

4000

t

00sm 3000v

OOC0U

2000

1000

20

10

t Band7

-4W-Band 25

-%—.band 28.5

-)FBand 39.5

-NO--Band 51.6

--W-Band 62.5

Band 65— Band 74

—Band 82

-$--Band 98

100

90

80

70

v

E60

0a

m

T^

500vatu

40

0a

30

tBand7

(Band 25

band 28.5

--E-Band 39.5

­00-Band 51.6

Band 62.5

Band 65

—Band 74

-)K- : Band 82

--*--Band 98

Band Populations & Capture dV

Number of Reachable Objects vs. dV Percentof objects captured vs. dV

0 0 ' -

0 500 1000 1500 2000 2500 3000 3500 4000

0 500 1000 1500 2000 2500 3000 3500 4000

dV M/sec from 400km circular dV m/sec from 400km circular

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Prop Budget for Common Catchers• Can implement variable tank sizes for common engine and payload• Typical sizing mix for common 2.2 kg payload shows that a common total

10Kg catcher works in launcher mass budget for SIX inclination bands.• High debris quantities at other inclinations need variable prop loads, smaller

catcher payload, or more mother-ship missions• 250 & 28.50 band pair may be clearable with a single launch.

2-Bucket Prop and Catcher Masses (k p ) for dV from 400 km Circular

QTY>

0-1000

misec

1000-

1500

misec

1500-

2000

misec

2000-

2500

misec

2500-

3000

misec

3000-

3500

misec

Total Prop

2.2kg

payloads

T<2

Total

catchers

Total

Catcher &

Prop

Bandl 0 21 5 601 238 172 It WAI 1OAQ

r 2957 598

3120 631

81b 166

AN

3556

3752

1081

Band 25 1 7

48

20

161

311

4461

8

33

19

78

16

129

23

61

44

98

391

1651

126

87

161

69

771

281

92

15

57

18

1531

band 28.1 2

Band 39.! 3

Band 51.f 41 2869 860 3729

Band 62.! 51

Band 65 1 6

1 3186 645 3830

10189 3082 13271

Band 74 7 72 333 120 3 47 5630 51611 10791

Band 82 8 993 29 553 175 38 11181 4657 15838

Band 98 9 2456 532 561 1921 35 20488 11805 32293

6-Bucket Prop and Catcher Masses (kq) for dV from 400 km Circular

Prop

0-1000

misec

1000-

1500

misec

1500-

2000

misec

2000-

2500

misec

2500-

3000

misec

3000-

3500

misec

Total Prop

2.2kg

payloads

T<6

Total

catchers

Total

Catcher &

Prop

Band7 0 5 19 339 1888 1870 4122 1049 5172

Band 25 1 18 31 130 1000 1000 2180 565 2746

band 28.5 3 121 128 345 690 163 1451 541 1992

Band 39.51 4 501 74 2491 127 98 602 244 847

Band 51.6 6 40 303 554 547 620 2071 708 2780

Band 62.5 7 78 62 221 611 196 1175 409 1584

Band 65 9 1125 502 933 2230 1664 6462 2596 1 9058

Band 74 10 182 1296 679 24 511 2701 1280 13981

Band 82 12 2504 113 3128 1389 4131 75591 3951 11510

Band 98 131 6194 20701 3173 1523 3811 133541 832 21681

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bris objects not Reachable in Initial Band Selection

60 80 100 120 140 160

Inclination (deg)

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700

600 t

j

500

400s

mg 300

200

100

0

0

Before and After

Perigee (<700 km) vs. Inclination700

i► f '.s

600 M♦ ♦ ♦

soo•

400

T-T td300

• z •

200 'M

100

0

0 20 40 60 81

Band near 17 deg inclination is tempting next target

Summary in LEO,

• Low inclinations have: • High inclinations have:♦ high eccentricity, ♦ low eccentricity,♦ low counts ♦ high counts♦ Larger radar cross section ♦ Smaller radar cross section♦ Rapid differential phasing ♦ Slow phasing

• Single mission with single • Probable need for multiplemagazine of high dV missions to same bandcatchers should work for • Potential need for multiplemost objects prop load variants on one

• Drag-assisted de-orbit is missionprobable removal • Propulsive de-orbit ismechanism for half of practical for most capturedcaptured objects objects

• Propulsive de-orbit ispossible for remainder

Typical Catcher Reference Concept:Kevlar® snag web

Retroreflector/solar cells/net containmentAvionics with MEMS thruster/antenna shell

Kapton® Drag Sail (post capture)Tank with main thruster below

TypicalMass

Item CommentTracking sensor 90 BW lipstick camera with caseIntegrated circuitry: send-receive,transponder, attitude control, system control,video processing 133 IMass of an I- hone 3G with battery)

Ref mission: 90% open-mesh Kevlar 149185 0.1 mm-strand snag netting, 4m diameter

Capture mechanism webCinching mechanism 50 Kevlar thread ands innerLaser/Radar retroreflector 20 Mostly art of structureLocal short-duration power source 133 11-Phone batter againSmal 60

Pt integrate as structure

Sizing ref mission: 0.02mm Kapton (1.4Drag enhancement 400 /cm3) 6m diameter film sailof ude control 16 IMEMS Solid state enginesMain thruster 290 EADS/Astrium 1 N Thruster massStructure 100 Carbon fiber nanosat bus

Max titanium tank for 7.8kg monopropellantTankage 100 dV-dependent) (=0.256m dia sphere)

Margin-dependent grams of excess massavailable to reach 2200 grams: Could bemore available prop with excess in main

- - tank- Each 100 grams of monoprop yields19.64 m/sec dV capability for a combined

Post-capture Propellant capability 439 Okg catcher/ca tured object

- - - - - - - - 2200 otal [email protected] 281244- 7086

Useful Features;Mother Ship-5,000-90,000kg

• 3-axis gyro-stable control• Magazines of (varying) dV catchers• Debris shields (to protect the many "eggs still in the nest")• (strong) Laser to illuminate target• Solar power• Doppler Radar (to track catcher)• Accurate on-board ephemerides for self and targets• Very high ballistic number (for long duration low orbit)• Potentially an electric spinner/lateral launcher

♦ to launch catchers symmetrically out-of plane♦ Greatly expands inclination width of band for no additional prop

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^y

SEC/AL CASENe/ict Object Capture

GEOS TA TIONA R Y Case

• Predominantly large (spent) objects♦ 1000-2000kg, or often much more♦ Specialized catchers are more useful for recovery

option

t Common altitude (35786 km)

♦ De-orbit not practical

• Common orbit inclination (0)• Derelict objects using valuable space• Retired objects within only afew m/sec of

GEO♦ Use orbit period rather than plane precession to

accomplish phasing/[email protected] 281244-7086

a

h v

Ar a

1'4

°y

WOTAN and Valkyries

• WOTAN==special variant of the Mother Ship• Valkyries==special Catcher variants

• Both optimized for large objects near GEO• Designed for rendezvous, stabilization, collection, and manipulation of

large uncooperative objects

• 4 Useful missions in one:- Clean explosion hazards and derelicts from Clarke orbit region- Demonstrate space mining/asteroid capture techniques- Consolidate and transfer upwards a highly-valuable resource depot,

already very high in the gravity well— (62% of Earth-escape dV)

- Develop worldwide cooperative space mission— Military/Proprietary nature of many target objects requires special security attention

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Valkyries

• Mythical riders who carried dead from battlefield to a usefulafterlife

• MUCH more massive and capable "catchers" than used in LEO

• Grapple-able free-flyers- with interchangeable arms and robust effectors specialized to

snare/despin/retain each class of object- Likely lon/Plasma Engine for fuel budget constraint- Implies High Power/weight requirement:

— Probably receive beamed power from WOTAN and/or ground

- Refuelable at WOTAN berthing station- Video link for tele-robotic control during rendezvous and capture- Approximately large-trash-can sized.- 10-20 of them aboard.

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WOTAN

• Overlord of the Valkyries and of all others below• _Worldwide Orbit _Transfer of Assets _Nexus*

— *nexus (nkss) n_ pl_ nexus or nex•us•es1.A means of connection, a link or tie: "this nexus between New York's .. _ real-estate investors and its _ _ _ politicians" (Wall StreetJournal)_2.A connected series or group_3. The core or center. "The real nexus of the money culture [was] Wall Street" (Bill Barol).

— The American HeritageS Dictionary of the English Language, Fourth Edition

• Drifting 1 m/sec above GEO- 24 km above functioning satellites- Retrograde drift once around planet every 3 years

• Berthing/Refueling and communications relay base for Valkyries.

• Tele-robotic transfer and attachment of recovered satellites, clipped to a sturdyspooled tether (-5 km for 5m/object, -1000 objects)

• KEVLARO' 149 3mm-diameter stranded cable weighs 53 kg, with 133 tonnes tensile strength.

• Large power capability for high ISP arc jet propulsion• Beamed up or self-generated (solar or nuclear).• Valkyries supply the plasma engines on ride upwards• Convert power to energy beam towards free-flying Valkyries in harvest mode

• Strong shielding for spiral transit up to GEO+

• Gyro stabilization

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Mission Scenario;PremHarvest

• 20,000+kg WOTAN Mother-ship with Valkyries to near-equatorial LEO (includes 8000 kg prop)

• 20,000+kg ""dumb".' propellant tank to coplanar orbit• Valkyrie dispatched to capture and retrieve prop tank• Robotic mechanical- and fluid-attachment of prop tank to

WOTAN• Slow spiral transfer to GEO with 3000+sec ISP solar-

powered arc-jet- Valkyries supply the engines- Valkyries (and catchers) dispatched to debris targets of

opportunity during journey.- -8000 kg propellant used @ 3000 ISP for LEO-GEO transfer- -20,000kg prop available at GEO for recapture ops

— also @ 3000 ISP

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Mission Scenafio;Harvest

• Valkyrie outfitted with object-specific capture effectorand fueled at berthing station on WOTAN

• Valkyrie dispatched to tele-robotically capture, de-spin,and retrieve GEO object

• WOTAN tele-robotic capture of free-flying Valkyrie withattached retrieved object

• Tele-robotic attachment of tethering clips to retrievedobject

• Tele-robotic object transfer to WOTAN with subsequentobject attachment to tether

• Robotic berthing of Valkyrie to refueling/sustenance port• (TBR: Beginning of scrap-rendering depot operations)

• Especially jumpering of retrieved power systems to commonsupplemental power bus

• Probably wait until post-departure from Clarke orbit region for anydisassembly/consolidation ops.

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Near-GEO Objects938 published objects♦ Large RCS♦ estimated average mass 1000 kg each

Half within 400 m/sec ofGeostationary♦ - All of the dV is related to inclination

change.

dV from GEO vs. Launch Date

Log10(RadarCross Section) near GEO3

2.52

ryC 1.5G

U 0.5c7 0°J -0.5

-1-1.5

-2,i M Ln r, m .i M Ln r, m M Ln r, m M Ln r, m .i M Ln

W N lD ci In m M I, N l0 O -ZT W M I, I i In m IZI, W N-1 -1 N N N M M ZT IZT Ln Ln Ln t0 l0 I, n r W W m

Object Count

Counts of Near-GEO Objects vs dV

1200

Q 1000

£ 800OU 600EOL. 400

4-

200

0

15-Sep-65 25-May-79 31-Jan-93 10-Oct-06

Launch Date

ern

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Mass Budget;

• 20,000kg prop at 3000 ISP provides maximum 6*10 8 kg*m/sec• At - 1000kg/object, -400 m/sec average delta V, and -1000 objects,

this is enough d V to capture most objects, with a -150-kg Valkyrie

• -10 Valkyries =1500 kg (results in -20-day retrieval cycle perobject, 1 object/day for 3 years)

• WOTAN =20,000kg LEO insertion- 8, 000kg Prop to spiral up- 1.500 kg for 10 Valkyries= 10, 500 kg for WOTAN

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Mission Scenafio;Pdst-Harvest

• Valkyries dispatched back to LEO to capture andretrieve prop tanks (with power)

• Valkyries bring staged prop and increasing power farmto GEO+ rendezvous with WOTAN

• Robotic attachment of fresh prop tank to WOTAN• Used tanks to the tether

• Slow spiral Earth departure and Lunar or Mars transferwith 3000+sec ISP solar-powered arc-jet

• Depot/scrap recovery operations begin.

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Conclusion

• ^13200 objects in LEO can be removed in 3 yearswith approximately 12 heavy-lift launchers♦ Most of the cost is expected to be in the operations,

launchers, and integration of the "mother ships"♦ Mass produced mono-prop low-ISP "catchers" (2.2kg

dry, 10 kg wet) are the cheap part.($26M @ $2000 USD Each)

• All debris near GEO can be removed in a 3-yearmission using 2 heavy-lift launches♦ Scrap yard would weigh 3x mass of ISS and can be

easily propelled further out to alleviate raw materialsneeds in future exploration.

♦ Reusable 150 kg ion-drive "Valkyrie' catchers are thekey

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Backup

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Net sizAV AW

ing

• Kevlae 149:♦ 1.47 g/cm3♦ Assume 4 m diameter web, of 0.1 mm fiber

90% open mesh0, 23N per fiber tensile strength (3 GPa tensile

strength)4 Vol= 7r*(200cm) 2 *(0.01 cm) *(0.1 solid fraction)

= 785 cm3

♦ 186 GPa tensile Modulus♦ 2% elongation

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