poymr - space.nss.org€¦ · the sps syskms definition study was initiatt.-d in de..-ember 1976....
TRANSCRIPT
D 180-20689-1
Contract NAS9-I S 196 DRL NumberT-1346 DRD Number MA-664T Line Item 3
Solar PoYMr Satellite SYSTEM DEFINITION STUDY
Part I Volume I
Executive Summary
Jur.e 28, 1977
Submitted to The National Aeronautics and Space Administration
Lyndon B. Johnson Space Center In Partial Fulfillment of the Requirements
of Contract NAS 9-15196
Boeing Aerospace Company Missiles And Space Group Space Division P.O. Box 3999 Seattle, Washington
Approved By:
G.R. Woodcock Study Manager
FOREWORD
The SPS syskms definition study was initiatt.-d in De..-ember 1976. Part I was '-"001plded on May I.
1977. Part I includc:d a principal analysis effort to "'valuate SPS energy "'-onv,:rsion options and spa"'-e
l"OllSln.action locations. A transportalion add-on task provided for further anc.'vsis of transportation
options. operaf ions. and coses.
The study was mana,ed by the Lyndon B. Johnson Space Center (JSC) of the National Aeronautk'S
and Space Administr.ation (NASA). The Contr.acting Offit.-er·s Representative KOR) was Oarice
Covington of JSC. JSC study management l'-'am members included:
Lou Livingston System Engineering Dick Kennedy Power Distribution
and Analysis Bob Ried Strudure and Thennal
Lyle Jenkins Space Construclion Analysis
Jim Jones Design F r"-d Stebbins Structural Analysis
Sam Nassiff Construction Base Bob Bond Man-Machine lnterfa"'-e
Buddy Heineman Mass Properties Bob GundefS'-'n Man-Machine Interface
Dickey Arndt Mkrowave System Analysis Hu Davis T rJnsportation Systems
R.H. Diet1 Microwave Tr.ansmitter Harold Benson Cost Analysis
and Rectenna Stu Nachtwey Mkrowave Biologkal
Lou Lc.-opold Microwave GcnerJtors Effeds
Jack Seyl Pha~ Control Andrei Konradi Space Radiation
Bill Dusenbury f nergy Conve~ion Environment
Jim Cioni PhotO\·oltaic Systems Al\·a Hardy Radiation Shidding
Bill Simon Thermal Cyde Systems Don Kessler Collision Probability
The Boeing study manag"'r was Gordon Woodcock. Boeing technical leaders were-:
Vince Caluori Photovoltaic SPS's
Dan Gregory Thermal Engine SPS's
Eldon Davis Con~tn11.:tion and Orbit-to-
Orbit Transportation
Hal DiRamio Earth-to-Orbit
Transportation
Or. JO\: Gauger co~t
Boll Conrad Mas~ Propertii:s
Rod Darrow Operation:!>
Bill Emsley Flight Control
ii
Jack Gewin Powi:r Distribution
llon Grim [k..:tric Propulsion
Henry Hillbrath Propulsion
Dr. Ted Kramer Thennal Analysis and
Optics
Keith Miller Human Factors and
Construction Operations
Jai:k Olson Confi!?uration Design
Dr. lknry Oman Photovoltaics
John Perry Structures
ORIGINAL PAGE Ill O! POOR QUALITY
The Part I Report includes a total of five volumes:
Vol. I
Vol. II
Vol.Ill
Vol. IV
Vol. V
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D 180-:?0689-4
DI 80-:?0689-S
Ext.-cu1ivc Summary
System Requirements ind Energy Conversion Options
Constrodion. Tm1Sportation. and Cost Analyses
SPS Tr.msportation Syskm Requirements
SPS Trctnsportation: Repn.-scntative System Descriptions
Requ"-sts for informat•on should be d~ded to Gordon R. Woodcock of the Boeing Aerospace
Company in ~attle or Clarke Covington of the future Progr.uns Division of the Johnson Spat.-c
C enter in Houston.
iii
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SOLAR POWER SATE LUTE SYSTEM DEFINITION STIJDY PART I TECHNICAL REPORT
1.0 EXECUTIVE SUMMARY
I .I THE SPS CONCEPT
Soliir power sateUites represent a proposed means of tapping baseload electric utility power from
the sun on a large scale. Th~ advantages of the space environment for generation of electric power
can thereby be ••brouaht down to Earth ... These advantages include essentially l"Ontinuous sunlight.
the ability to l"Onstruct very large solar l"Ollectors with minimum resource investment. and the abil
ity to always aim the collectors at the sun. Studies presently in progress sponsored by ERDA and
NASA. of which this SPS Systems Definition Study is one element. are defining the systems. devd
opment approal-hes, and risks and costs for this ,·enture and evaluating the probable benefits of the
system against these risks and \."OSts.
SYSTEM CONCEP·;
An SPS system for utility electric power would include a number of satellites in geosynchronous
orbit. ead1 with one or two associated power receiving stations on the ground. Receiving stations
can be located near load centers (weather is not a significant factor>: each will provide IOOO mega·
watts or more of basdoad electrical output. A satellite system is pictorialized in Figure 1-1. Power
is tr.msferred from the satellites to the ground stations by high-precision electromagnetic beams.
The tran-.missions would presumably use the industrial microwave band at :!.45 GHz: an alternative
industrial allo1.:ation available at 5.8 GHz l·ould be used but has received comparatively litrle
attention.
A complete SPS system is depicted in Figure 1-2. In addition to the satellites and their ground sys
tems it will include:
• A space transportation system capable of delivery of the SPS's to geosynchronous orbit and
capahlc of supporting all required space operations needed to establish and maintain the SPS
system.
• One or more constrm:tion bases. located either in geosynduonous orbit or low Earth orbit.
capable of constructing the satellites. Satellite hardware delivered to the construction hases
will be prefabricated to the extent practicable.
• Mainknance and ... cn·ice bascll capable of supporting the maintenan1.:e operationi. required to
kl.'ql th1.· SPS's operating.
ORIGINAL PAGE JS OF POOR QUAI.ll'»
Power Satellite
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El..ECTIUCAL OUTPUT: 10.000,000 kW {2.5 TIMES GRAND COULEE DAMJ
figure t-t. The SPS Concept
PH1'.J'tOVOt TAIC SP$
Figure l ·2. Major Program Elements
TH£flMAL ENGH\1£ 1WS
ORiGL~AL lS Of<' Pl·~ Ht LJt /\ l rrv
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• One or more Earth-based space transportation ports (launch sites) capable of supporting space
transportation operations.
• One or more spa'--e-based transportation operations support bases, capable of supporting spal·e
transportation operations. This function could conceivably be combined with that of either a
'-"Onstruction base or a maintenance base.
• Earth-based manufacturing facihties capable of producing the hardware and consumables nec
essary to transport. l"Onstruct and maintain the SPS system.
• An Earth-based logisti<:~ system capable of delivering the hardware ancJ consumabks to the
space transportation parts.
1.2 STUDY OBJECTIVES
The objectives of Part I of the study. as specified by the NASA statement of work. were as follows:
(I) Issues-To derive spedfic. comprehensive supporting data necessary for NASA evaluation of
the following two major SPS system issues:
a. What is the overall most effective means of accomplishing solar energy-to-electrical energy
conversion on an SPS in geosynchronous orbit?
b. At what location (or locations) in space l·ould the various phases of SPS construction and
assembly be done?
( 21 Transportation-To increase the scope and depth of understanding of the space transportation
systems necessary to support an SPS program.
a. Provide a set of transportation system requirements and reference transportation system
elements descriptions appropriate to the conduct of an SPS program as represented by
JSC Scenario "B".
o. Identify and define analyses and tests nel·essary ro advance the confidl'nce levd in pro
jected SPS transportation systems performance and cost sufficient to recommend initia
tion of an SPS technology advancement program.
3
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1.3 STIJDY APPROACH AND PLAN
The SPS System Definitions study is being conducted in tw'> parts as indkated in Figure 1-3. It
began with two reference "Ystems: the photovoltak syskm from what is popularly known as the
JSC tireen book CJSC 11568,: and the Brayton thermal system from prior study work by Boeing.
We have also in this phase considered the other options shown: high tedrnology gallium arsenide.
thin films. and Rankine and thermionic thermal options. Part I provided evaluation data that would
allow selection of one or two energy conversion options and evaluate LEO and GEO space construc
tion locations. In Part II we will analy 1.c the mh:rowavc power transmission system and develop an
integrated system definition. The objective of Part II is to reduce the ~ystem mass and 1.·ost uncer
tainties as much as possible.
The program under study is basically an operational or commcrdal SPS program. Ground rules arc
summarized in Table 1-1. It starts with the first full capabilit/ I 0.000 mcgawan satdlite and g~s
through a program of many satellites. In a few instances where the cost of money was important wt.•
have used a 7!1~~ discount rate as recommended by Econ in earlkr studies. We are assuming a 30
year system life for purposes of financial horizon analysis. even though there is no particular lifo
limit on the SPS's. There are a few cases where creep rupture analysis was required. A safety factor
of I Yi on 30 year creep-rupture-Hf e material thickness was used. The reft>rcm."e data for transporta
tion came from the Heavy-Lift Launch Vehicle study and Future Space Transportation Systems
Analysis study data base (contrads NAS 8-3~169 and NAS 9-143~3. res~ctivcly). That data base
was updated as part of this study.
Table 1-1. SPS Program Ground Rules
• IOC date: end of 1995
• 11 ~ SPS program
• I 0-gigawatt SPS size
• 7.5' ~ discount rak ( 1977 constant dollars)
• 30-year satellite life
• Transportation system reference data to be tahn from HLLV
and FSTSA data base and JSC-11568
• Operational system design and performan~:e projcdions bast.'d
on 1987 te1.·hnology baseline
The program s1.·enario U'il'd for SPS in-.1.1lldtion rak was JS( s(enario B. shown in Figure 1-4. Th1.•
fir-.t .. akllite was 1.·ompkted in 1995 and produl."lion rate increases gradually to 7 pcr ycar at tht.' l'lld
of the program. For purro~1.·s of predktmg tran~portation l'O'>t. wt: have takt.•n J ~nap,hot of the
mid-point of the program at the rail' of four SPS\ per year.
4
Point of Departure
Reference Systems :
Silicon photov91taic from JSC study
Brayton thermal from Boeing study
Options
Gallium arsenide and thin-film photovoltaics
Rankine and thermionic thermal engines
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Part I December 1976 to May 1977
&esig : y reference
designs to next level of detail.
Analyze: Construction and transportation systems and operations. CharactPrize: Options and delta off reference designs Compare: Performance, practicality. operations, environt:lental factors, cost, and technical risk.
Select: Q.;0r two energy conversion options and low versus geosynchronous orbit construction.
Part II May 1977to December 1977
Analyze: Microwave power transmission syst'!m.
Design: Integrated SPS systems-energy conversion, power transmission, construction, transportation, and overall operations.
Develop: . • Integrated system
conceptual definition. • System mass estimates • System cost estimates • System de.velopment plan5 • Technology advancement
requirements
Figure 1-3. Solar Power SateOite Systems Study Overview
NUMBER OF SYSTEMS COMPLETED
CUMULATIVE TOTAL
NUMBER OF SYSTEMS COMPLETED
CUMULATIVE TOTAL
• Corresponds to JSC scenario B
0 .. 2
1
1
4
3~
0 1 1
0 2 3
4 5 5
34 39 44
1
4
5
g 0 N
IO .. 0 N
1
5
6
49 55
1 2 2
6 8 10
6 6 6
61 67 73
Figure 1-4. Baseline Operational Program Scenario
5
8 N
2 2 3 3 3
12 14 17 20 23
6 6 6 7 7
79 85 91 98 105
0 -~ 3
26
7
112
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During Part I no power transmission system analysis was done. The data shown in Table I-~ came
from the JSC .. green book." This information was used for purposes of sizing satellites to dl·liwry
I0,000 megawatts of ground output ro rhe receiver antenna system.
Table 1-2. Reference MPTS/MCRS Nominal Efficiencies*
Antenna power distribution .98
DC-RF conversion .87
Phase control ** Waveguides cJ.:!R) .98
Mel·hankal alignment .98
Atmosphere .98
Energy collel·tion .88
RF-DC l'Onversion .90
Power interface .99
Overall .6.:!9
* From JSC 11568. fig. IV-A-I-I. .. SPS Effo:iendes"
** Included in energy coJlection
The Part I analysis effort was grouped into four higher-level task types as shown in Figure 1-5.
These analyses were based on the point-of-departure configuratiom. Results of the analyses were
integrated as indh:ated in the figure. Additional tradeoffs and analyses dfort after the midterm led
to the evaluation data summarized in the summary sc:ction of this report.
The silii:on single crystal photovoltaic SPS system and the Brayton thermal engine system referenn~
designs wert" used to 1.:arry out analyses such as performance. structures. and powt•r distribution.
The constn11..:tion and transportation analysc:s consider~d both geosynchronous orbit and low earth
orbit as construction locations. The analyses resulted in the configuration ~volutions shown in Fig
un.• l-6. These analyses led to concepts for fai.:ilitization of construction. influencing the satellite
design, e~pecially in the thermal engines where a configuration change from compound curvature
concentrators occurred. In both cases modular SPS designs at approximately 1.000 megawatts of
onhoard husbar power per module were developed.
The thermioni.: syskm was re.:ommended for 1.li~rnntinuanl'l' about halfway through the Part I
efforr.
1.4 DOCUMENT STRUCTURE
Tim, l'Xt'l·utiVl' 'unHnJry dc~nihl'~ thl· re~ults of the Part I '-·valuations of enl·rg~ l'onwrsio:i and l'On
strw.:tion l<Kation options. Voh1ml'S If through V prm idl' dda1lcd rl'porting of the Part I efforr.
6
ORIENTATION
CONFIGURATION ANALYSES
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PART 1 MIDTERM
PART1 FINAL
EVALUATION DATA PRODUCTS
ISSUEN0.1 ENERGY CONVERSION METHOD
•PERFORM· ANCE
•PERFORM· AND DEGRADA· TION
ISSUE NO 2 CONSTRUC· TION LOCATION
• O\I qALL DESIGN REOUIRE· MEI-HS
IOPTION&ORIENTEDI ITRAOESORIENTEDI •SIZE •MASS
• PERf-ORM· ANCE• DCGRADA· TION
SILICON PHOTOVOLTAIC GEO CONSTRUCTION
BRAYTON THERMAL ENGINE-LEO CONSTRUCTION
4MODULES
ORIGINAL PAGD:. IS OF POOR QUALtrf
•TRANSPOR· TATION
•CONSTRUC· TION
•MAINTAIN· ABILITY
• ENVIRONMEl'fT •MATERIALS
•SYSTEM COMPLEXITY
• TECHNOt.OGY ADVANCE· MENT REOUIRE· MENTS
eCOST DIFFERENTIAL FACTORS
e TR,NSPORTA TIOl'f ROTS& COMPLEX ITV
• CONSTRUCTION • LAUNCH SITE
DIFFFHENTIALS e SYSTEM
STARTUP •OPERATIONS •COLLISION
•COST DIFFERENTIAL FACTORS
Figure 1-S. Synopsis of Part 1 Study Logic
STRUCTURES, CELL CHARACTERISTICS, PERFORMANCE, Iii POWER DISTRIBUTION
GEO COl'l:STRUCTION 6 TRANSPORTATION
LEO CONSTRUCTION 6 lRANSPORTATION
PERFORMANCE, SUB~YSTEMS, STRUCTURES, f'OWER DISTRIBUTION
THERMIONICS DROPPEDEXCESSIVEL V MASSIVE
SILICON
a •CR•1 • • • CR•2
~~· • MAINTENANCE ~ IGEOt OPTIONS
/7) • GALLIUM ARSENIDE
~ ILEOt ntlN FILM
18MODULES
BRAYTON
• METALLIC TURBINE
e SIC TURB1NE
RANKINE
e POTASSIUM • STEAM
Figure 1-6. Part 1 Analyses and Configuration Evolution 7
ORIGINAL PAGB JS or POOR QUALl'IT .
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l.S ENERGY CONVERSION EVALUATION
The statement of work spedfied the evaluation factors listed in Table 1-3 for energy l·onwrsion.
The cost differential factors are presented at the end of this summary because they combine re!-iults
of b1..1lh evaluation efforts.
Table t-3. Energy Conversion Evaluation Factors
Evaluation Factor
a) SPS Performance
h) Performance Degradation
c) SPS Size
di SPS Mass
e) System Complexity
fl Maintainability
g) C'onstmction Requirements
h) Transportation Requirements
i l Technology Advancement Requirements
j I System Cost Differential Factors
k) Environmental Effects Differential Fal·tors
ll Materials Differential Factors
SPS Performance-The first factor is performance c efficiency). When this study began it wa'.'>
bdieved that thae was quite a diffrrence hetwt•en thennal t:"ngine and photovoltaic performanl"t.'.
There is mm:h less than we had thought. Effidency generally follows the technology advances and
advanced ~ystcms t1..nd to he more efficient. except for the thermionics option. Efficiency is not an
important discriminator unles., very low. Effickncy re!-iults are summarited in Figure 1-7.
Perfonnance Degradation-Degradation effects were found in ali of the systems. The silicon photo
voltaic degrades more than thermal engine systems. with gallium arsenide in between.
On the left hand -.ide of Figure 1-8 " the magnitude of the degradation effect and on the right lwnd
it 1s normalized to indicalt' what pen:entage of SPS mass h affoded. for example. thin film rdlel··
tors are the Jegrad<ition mode for them1<1I engines hut rt.>pre ... ent only a small fradion of satd ... e
nwso;. In .tll l·a-.l''> maintaining th~ ~atdlite output .,cems lo he promi-.ing. We comp1..·nsatcd for tkgra·
dation in our rc1.:ommendcd SPS\. Pcrformanct• degradation is rdleded in size. mass. and l"<ht and
therefor~ l·arries litth.· weight a~ :111 independent evaluation fal..'tor.
SPS Size-Figure l-9 ;..; ;1 -.i1c ..:omr:~o1.,on of the prin..:ipal sysktn.... The small~st sy.,tem io; the
gallium ar.,t.'nidt.' amwalahk follow~d by thl.! Brayton. Tht• -;ili..:on ... y~tcms show that t·on..:entration
8
ID .
1&
10
&
0
1
.15
.25
0 0
--
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EFFICIENCY FOLl.OWS TECHNOLOGY ADVANCE EXCEPT FOR THERMIONICS
-
..---
--
~
-
-
-
SILICON REF CR2
SILICON ARRAY ADDITION cu
SILICON ANNEAL· ING
GALLIUM ARSENIDE ANNEAL· ING
THIN FILM
BRAYTON BRAYTON RANKINE ADVANCED THERM· 1422K 1660K 16SOK BRAYTON IONIC
CR1 .EOL CR1
Figure I· 7. Energy Convenion Comparison SPS Performance
RECOMMENDED SPS OPl IONS COMPENSATE DEGRADATION BY ANNEALING, MAINTCNAloCE. OR INITIAL OVlRSIZE
DEGRADATION EFFECTS PREDICTED MAGNITUDE
10 20 TIMt. ON ORBIT, YEARS
GALLIUM ARSENIDE CELLS
SILICON CELLS
30
.15
0
NORMALIZ.OD DEGRADATION
~ ~ -THERMAL
I '-----------J-GA A~ . SILICON
0 10 20 Tlft4E ON ORlllT, ~EARS
Figure 1·8. Ene19y Convenion Comparilon Performance Depadation
9
ORIGINAL PAGE IS OF POOR QUALITY
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ralio I kads to a sipificanl redudion in size. The tJ1in fdm size esrimate is a guess bc~au~ of the
unc.-ertainty in the dala base. Size does nor sttm &o lk:- a slron1 diSl."rimir.alor: m~h more imporlanl
is mass.
SPS Mass-Mass c."Omp .. ;ison fort~ systems is shown ;n a igure 1-IO. Note rhal annealin(! is a mu~h
~ner syslem from the mas." s1andpoinl lhan arr.ay addilion. The annealing melhoJ employ"
eleclron-beam or laser healing. A t'1ennal pulse di~-tty inlo lhe solar ~di r.ai~ the tempcr.ature
momen!aril)· .and anneals out rhe deg.Old;ation. Heat j,!cner.a1ed in rhe \."'ell diff US&."S only sli"1tly in10
the subslrale. Rough es1im1t1es indicate that 'lie need aboo• a half dozen annealing ma~hines. 1wo
meters squaR by thr« ureters long. This nun:~r of u1ad1ines oper.uing c."Ontinually durin~ satdlite
operation will keep lhe performanc.-e iAp. These madlines \."OUld be oper.ated remotely by oper.tlors
via RF links. Annealing is like painting the Golden Gale Bridge: as~ as it is finished. ii ·n~•SI
Sl3rt dpin.
The lighlest system of all is plli•1m arsenide. We have found lhat there is a c."Onsidcr.tble va.riation in
Brayton system mass as a funclion of ledmology. The steam Rankine sys1em was ex"·essively mas
sive and c."Ould nol be ploned on the dlan. Thennionics • .:onversion was also quile massive.
SySlem Compleury-There are two ways to measure "-omple"ily: one way is 10 eslimale lhc: num
ber of uniqu~ parls or subas..;emblies. The thermal engine system h..s abou1 five ti:nes as many
u,ique paras as lhe (lho1ovol1ak. Total parts is lh(' olher measure. If one 1.."0unts indi,idual solar
cells. photornltaks have about 1.000 limes as many 1otal pans. lnlegration \."Ompkxit)· of 1he sys
!c:m is delc:nnined primarily by the number of unique parls. Syslem romplexitites are \."Omp:1red in
Figure 1-11.
Main1ainabili1y Faclors-For both types of ene~ l·onversion we found mainlenance problems. and
in borh ba~s \. ~ found )()h.aions. The results after applying the solurions are summarized in Table
1-1. Roughly 5 tt• I 0 manhours per hour for annealing are needed wilh lhe pholo\'Ollaic syslem and
~ligiltl} r111m· than 10 mh;h with lhe thermal syslem for mel·hanical repair and repla•:e. h i:> l·on
l·ei,ahle 1hat rho~ manhours might be spenl on lhe ground if '.\'e can dewlop suitable automakJ
'~\fems lhJI 1.-an he man-Jirech:u from a remole dislanl·'-'· It does not nec.·essarily mean thal lhe
Sfi~ "s haw to ~ manned. It j, likdy that these maintenance requirements will be overshadowed hy
th;·I for lh.: miaowa\e transmirter.
10
118
125
I I •
•
I-
-,_
-
GAU.W ....... ·~ C.""'
0
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llml 111ml
Fagure 1-9. Eaeqy Coavenion Comparisoa SPS Size
-,..._ - -,..._
- -..-
-
-
llLICON SILllCOll llUCION GM.Lii# ANNEAL· MllNIOE
mm ftUI
llllAY"ON lllAY10N AOVMCID flOTA'S- TttlflMIONIC lllf Allflill\' tGl!X t&A IRA\'TON SIUM lllCllADINGI AOOITICllll .... ANllUlllWG llWdUNI Cll2 all an Cllt
Cllt
figure 1-IO. Energy Conversion Comparison SPS Mass
JI
• Ill ::; • ~ Ill
! ! a: ~ Ill
8 z :>
1
1
1
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I THERMAL ENGINE kAS ABOUT 6 T•ES AS MANY I _ UNIOUE~ARTSASPHOTOVOLTAIC _
® THERMAL ENGINE
10
TOTAL PARTS
PHOTOVOLTAIC
1
Figure 1-11. Energy Corwenion Compariwn System Complexity
12
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Table 1-4. Energy Conversion Comparison Maintainability Factors
Photovoltaic
Problem
Sensitivity of Solar Cell
Strings to Cell Failures
Solution
Parc1lleling and Diode
Shunting
Result
Equivalent maintenance
load roughly 5 to 10 MH/H
for annealing or arrc1y
addition
Thermal Engim.·
Problem
Reliability of NaK System
Solution
Technology Advancement Progrc1m
or redesign to eliminate NaK
~ Equivalent maintenance
lo.id roughly 10 Mff/H
for med1anical repair anJ replace
Construction Requirements-A constructability rating is shown in Figure 1-1 '.! that involves a num
ber of factors as devdoi<d by the construction analysis task. The LEO/GEO comparison is shown
as w .:II as the thermal engine and photovoltaic comparison. This is a weighted Sl."Ore l'.'Omparison.
The numbers in parenthesis are weighting factors; a long bar is good. A long bar means a smaller
facdity. less complexity. and a smaller crew size. It is a "goodness" rating and not a measure of the
physil:al size or numbers of people. Tht>re is not a dramatic difference between th..- sysrems bur
some preferenl'.'e for the simpler ph'ltovoltaic, as expected because the system is less med1anically
complex.
One of the reasons that the conl'.'entrc1tion ratio = I photovoltail'.' satdlite is preferred is rhat it is
simpler to construct. It avoids having to install rhe large tlat V-ridge reflectors: that is a signitkanr
advantage.
Transportation Requirements-In transpoHarion requircmenrs. there was nor a great deal of difkr
ence in the mass between the systems but the photovoltaic systems packaged to roughly 20 times
the density of the thermal engine systems. Some diffaully was experienl'.'ed in packaging the latter.
We finally gor down to a Jen~ity compatible with the laund1 vchide capability: further improve
mentc; appear possible. Most of the demcnts of the photovoltaic system can fold into a dense pack
al,!c. For the thermal system unless plumbing is produced in spal'.'e or prefilled. ther..- an: limits on
aaainablc packaging density.
Values ~hown m Figure 1-13 are an average but we ad1ieveJ that average in a(tual pa1.·kaging for
ea\:'h type. The size ~hown in the figure represents a volunw large enough to \:'Ontain the entire SPS
as pa\:'kagcJ for laundi.
13
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CJ> HIGH SCORE IS BEST
- 131
128 112
,.. 171
e NUMBERS INC t DENOTE WEIGHTING FACTOR
- NUMBER OF MACHINES 111
-MINOR FACILITY SIZE C1J
- MAatlNE COMPLEXITY C2t
-CREW SIZE 131
(j 180 97
- FACILITY COMPLEXITY 141 .. IC
I ..
- MAJOR FACILITY SIZE 141
lilO
-ASSEMBLY COMPLEXITY 151
LEO GEO
l'HOTOVOt. TAIC SATELLITE CCA•2t
LEO GEO
THERMAL ENGINE SATELLITE
LEO GEO
PHOTOVOLTAIC SATELLITE CCA•1t
figure 1-12. Preliminary Relative ConsbUctability Rating
PHOTOVOLTAIC
52000m3 PERSPS DENSITY• 1300 kg/m2
a1 lblftl
t3Smj ,. -1 .... ~
53m
. .l ----
MOST IMPORTANT DIFFERENCE IS PACKAGING DENSITY
L--98m -
THERMAL ENGINE
CBRAYTONJ
1.1x1o6m3 PERSPS DENSITY • 72 kglm3
•4.S lblftl
Figure 1-13. Energy Conversion Comparison T ransportalion Requirements
14
147m
D 180-20689-1
Technology Advancement Requirements-Technology advancement requirements listed in Table 1-5
are the most important ones. The Brayton lhennal qde requires the leasl tt>chnology advance. The
silicon photovoltaic system is the next least. Continuou:. photovoltaic "-ell and blankd production is
mu'h more impo.tant than obtaining maximum possible efficiency. 14';f solar cells made by con·
tinuous production proc..""esses would make the silicon !.YSl ·m attractiw. 18',; cdls made by today\
processes would not yield an economically attractive system.
The other systems require more tedmology advance: Brayton and silicon are the least risky.
Environmental Effects Differential factors-Env•ronmenlal effects di:ferences are summarized as
follows:
• No significant environmental effects associated with energy conversion were found.
• The principal factor is launch vehicle emissions. which are proportional to SPS mass.
• A launch pad fire with gallium arsenide ta~nic• appears kss of a toxicity problem than the
hydrochloric acid effluent from shuttle SRB's.
Arsenic was specifically investigated. Launch accident cloud analyses indicate that concentratiO!b
get below allowable levels quickly. Further. this is not a routine condition. but an exceptional
condition.
Materials Differential Factors-Materials factors are displayed on a very compressed logarithmic
scale in Figure 1-14. We have picked five materials that are used in sufficient quantity in SPS sys
tems to present polential concerns. The figure shows how many SPS's can be built per year with
today's production rates and finally. how many SPS\ total could be built with the total known
reserves. Reserves are quantities available by today's recowry process at today·s costs. Silicon is
produced in large quaa.tities for mdallurgical reasons. The reserves arc on the order of half the cmst
of the earth. so there is no supply problem.
Presently the U.S. production of columbium is essentially zero. But the world production is suffi
cient to build several SPS's per year. The reSc:rves in the United States are not large, but world
rc:serves are adequale. Aluminum is no problem. Gallium was the only material indicating a polen
tial problem. The assumptions are very important for gallium. We show ~.000 tons of gallium per
SPS and no process improvement. There are known potentials for process improvements up to
about a factor of 4. Gallium today is produced as a byproduct of aluminum production. The yield
is about one-fourth of what it coul<l be. Akoa. for example. has stated that if more gallium is
needed from ahaninum. it could be obtained with more inveo;tment in reco\'ery l!quipm~nt. Gallium
production rate may he more of a problem than total reserv~s.
IS
1o8
1o5
i 1o4
1000 ... z ... -' 100 c > 5 10 0 ...
1
.1
.01
.001
D 180-20689-1
Table 1 ·S. Eneqy Convenion: Technology AdYancemeat Requirements
SIUCON
CONTINUOUS CELLIBLANKET MODUCTION fROCESS
-ANNEALING
PHOlOVOLTAIC THERMAL CYCLE
GALLIUM THIN-FILM BRAYTON RANKINE ARSENIDE
THIN-FILM THIN..flLM RELIABLE HIGHTEllP· GALLIUM ARSENIDE TECHNOLOGY FLUID ERATUrtE APPLICATION - CONTAINMENT 11£1' 1.L VAPOR PROCESS PRODl.'CT ION TECHNOLOGY
- PROCESSES -CONTINUOUS RtLIABLE CELL/BLANKET FLUID PROOUCllON CONTAINMENT PROCUS
-ANNEALING
CONCLUSION BRAYTON AND SILla>N LEAST RISK
GALLIUM WAS ONL V IDENTIFIED MATERIALS AVAILABILITY PROBLEM. VALUES SHOWN ASSUME 2000 TONS GALLIUM PER SPS AND r~ PRODUCTION PROCESS IMPROVEMENT
COLUMBl!JM SILICON (BRAYTON) ALUMINUM GALLIUM
SPSIYR SPS TOTAL SPSIVR SPS TOTAL SPS/VR SPS TOTAL SPSIVR1
SPS TOT Al
1D ,w WORLD!;
U.S. Cl. ~ Ow Uo t-ic Oc Z..1 en> Wcz: >"' ffi> :s a:m
WORLD I
WORLD
lu.s.
I WORLD
U.S.
WORLD
U.S. PRCD. IS -o
.s. ES. AVE
.. 0
U.S. PROO. NOT AVAIL.
WORLD
•GRAPHITE FIBER PRODUCERS ARE TOOLING UP FOR THOUSANDS OF TONS PER VEAR
I I I I I I WORLD I I
THERMIONICS
THERMIONIC DIODE TECHNOLOGY
GRAPHITP
SPSIVR SPS TOT AL
ID w 15 I a.
:& 18w , ... ~ I ~:5
WORLDI ~ ~ PAOO >w NOT I ffi >
U.S. AVAIL. ~ !; I a: ID
I
Figure 1-14. Energy Conversion Comparison Materials Differential Facton
16
OJUGINAL PAGE 18 or POOR QUALITI
D 180-20689--1
Graphite today (graphite fibers of an Aerospac."\! quality. not total gr.tphite ). is a small production
item. But the producers are presently tooling up for very high production ratc:s: graphite tih<r is
becoming a commercial product.
Energy Conversion Evaluation Summary-Four ene~y conversion options were found that make
SPS look promising. Any one of them would work: they are not remarkably different in owrall
potential. Thennal engines are more complicated but require less technology ad\'ancc. The rt:oto
voltaic."S require continuous production cell process development more than they need anything else.
As will be shown in the cost summary. there is not much difftarence in production cost projections
for the Silicon and Br.tyton systems Gallium arsenide looks slightly cheaper. but there is a huge
uncertainty in the data.
We propose to concentrate on the silicon concentr.ation ratio = I with annealing capability and
Brayton sysh~ms. We propose gallium-arsenide a~ an advanced technology option. showing one way
that the SPS system could ~row to achieve potentially lower costs with technology improvement.
There are certain things in the potassium Rankine system that need further evaluat:on. especially
machinery mass properties.
A problem was experienced with thin films in that the data base was just not sufficient to drdw
definitive conclusions. Finally. we recommend rejecting two systems, specifically thermionics and
skam Rankine. The recommendations stated apply to the Part II study and not necessarily to an
SPS progr.am. They relate to the fact that the study objectives are. in part. to minimize uncertainties
in mass and cost.
Construction Location Evaluation-The statement of work specified the evaluation factors listed in
Table 1-6 for construdion location. The construction locations to be evaluated are low Earth orbit
CLEO) and geosynchronous orbit (GEO). A significant proportion of the evaluation relates to selec
tion of orbit-to-orbit transportation. because with LEO construction the satdlite (or satellite mod
ules) must be moved with low thrust to prevent structural failure. The power output from the mod
ules can be used to opernte an electric propulsion system for the transfer. With GEO construction
the satellite hardware is not cc1pable of self-powered transfer: conventional means must be used. For
the purposes of this study reusable L02/LH 2 orbit transfer vehicles were baselined. In summar)·.
LEO constmction impli.:s self-powered electric rocket transfer: GEO construction impli.:s chemicJl
vehicle transfor of HLLV-sized payloads to the GEO construction bas~.
17
D 180-20689-1
Table 1-6. Construction Location Evaluation Factors
l:.valuation Factor
a) Transportation Requirements
b) Construction Requirements
c) SPS Overall Design Req.iirements
d) SPS Performan'-~ and Degradation Potential
e) Launch Site Difforential Effects
0 System Startup Requirements
g > Operations Considerations
h > ( ollision Considerations
i) System Cost Differential factors
H Clrbital Transfer (omplexity Factors
Transportation Requirements-The principal difference in tr~ nsportation rel1uirements bdween LEO
and GEO construction location is the difference in total delivery to low Earth orbit. shown in Fig
ure 1-15 in tenns of numbers of HLLV launches. The difference results primarily from the
differences in propellant ret1uircd for the transfer due to the great diffe:-ence in propulsion spedfo.:
impulse. typkally 5000 sec for ekctric rockets versus 470 seconds for LO-,/LH-, chemical rockds.
Construction Requirements-(onstruction n!t1uirements in low Earth orbit involve sever.ti nuisance
factors. As noted in Figure 1-16 atmosphere drag results in an aver.tge propellant consumption (to
keep the construction facility orbit trimmed) of about 800 kilograms per day. The construction
approaches that we have developed do not appear sensitive to light/dark cycling on crew producli\;
ity. For gravity gradient effects. the only practical thing to do is to select a stable attitude and con
struct in that attitude. Ont' simply car, .10t afford to expend enough propellant to hold a non-stable
attitude.
Thermal t:fti!cts may have some influence on construction. but with low,o\."ffo.:ient-of~xpansion
graphite epoxy. Hhe baseline structure l that does not appear to be a strong consideration. There an:
similar thermal dfrcts in geosynduonous orbit. although less frequent.
In geosynchronous orbit. radiation environment may be an issue if massiw shielding is required.
With the Apollo/Skylab cn:w radiation exposure standards. construction bases can provide most of
the shielding required without mass penalties. Thl' solar tlare contribution can b\.' avoided with a
"storm cellar.'" If it is ncccssar} to go to a lower level radiation standard. and add shielding. there is
not mud1 differen~e in the amount of shielding rl.'quircJ. but there is quite a Jiffercn(I.' in thi: trans
portation cost I a one-time CO!>t for each facility 1.
18
32
28
24
20
LAUNCHES PER DAV 16
12
8
4
2
D 180-20689· 1
CHEM OTV r-\_ GEO CONST '\.
t AVG
4 6
SATELLITES PER VEAR
.. MAX
8
• JSC SCENARIO B •BALL/BALL Hl..LV
P/L•4od< KG
Figure 1-1 S. Construction Location Evaluation
SPS810
• DRAG-AVERAGE PROPELLANT CONSUMPTION (Oz - Hz> 700 TO 800 Kg /DAY TO KEEP ORBIT TRIMMED
• LIGHT/DARK - NOT A MAJOR PROBLEM WITH MECHANIZED CONSTRUCTION
•GRAVITY GRADIENT-CONST!1UCT IN STABLE ATTITUDE
~
•RADIATION ENVIRONMENT IS ISSUE IF MASSIVE SHIELDING REQUIRED
• CONSTRUCTION BASE LIKELY TO PROVIDE &TO 15glcm2
APOLLO/ SKYLAB GEO
_....-(SHADED REGION IS SOLAR PROTON CONTRIBUTION)
INDUSTRIAL -~
1--~~~.._~~~--~.a.-~
' 10 100 SHIELDING, g/an2 AL
Figure I· 16. Construction Location Evaluation Construction Requirements
19 ()IUGINAL PAGE 1S or rooR QUIJj'rl
D 180-20689-1
SPS Design Requirements-A number of design requirements on the satdlite were found for LEO
construction. First is modularization, Cwhich may be a blessing in disguise). The satdlitc must be
modular, because otherwise it is not controllable during the orbit tr.msfer. The photovoltaic system
must have the capability to operate the proportion of the array used for electric propulsion at
reJuceJ voltage: and must incorporate additional power distribution provisions. Further requin:d i~
the capability to accept propuls;on installations and then provide for their removal at GEO. All of
these were reflected as satellite impact costs as part of the LEO/GEO construction cost differential
factors. In most cases. the costs were trivial. but thesl' additional design re{1uirements represent
additional <lesig.l c:>mplexities.
SPS Performance and Degradation Potential-An SPS module being transported from LEO to GlO
must pass through the Van Allen trapped radiation belts. If the transfer is accomplished by a high
thrust system in a total time of roughly six hours the radiation dose received is minimal. even with
the scantie~t of shielding. Electric propelled transfers (low thrust). however. arl! likl!ly to re{1uirl! 2
months to a year. and substantial doses will be receivl!d. (The electric-powered trip time can be var
ied over a wide range by selection of power level and specitk impulse. Radiation dl!gradation is a
significant factor in trip time selection.)
Significant radiation dl!gradation phenomena were identified for solar cells and for plastic film
retlectors. Representative solar cdl degradation data are shown in Figurl! 1-17 and plastic film
reflector estimates are shown in Figure 1-18. Additional potential degradation concerns include
plastic matrix compositl! structural materials: no data werl! found on radiation degradation cf these
materials.
As a design practice. the idl!ntifil!d modl!s of degradation were compensakd by oversizing or. in the
case of solar cells. in certain cases by annealing. Consequently. radiation degradation effrcts were
reflected in cost tradl!s for LEO wrsus GEO ..:onstruction.
Launch Site Differential Effects-The principal effect on launch site operations was due to the
aforementioned difference in launch rates. This diffrrence was also retleded in costs of providing
facilities capable.: of supporting the requisite launch rates. with estimated values of 10.6 billion for
LEO construction and 15.8 billion for GEO constmction. These facilitks would be incrementally
procured over a period of years as the launch rate increased along with the rate of ~PS capacity
addition.
System Startup Requirements-Certain startup factors Wl!re identified that are unique to the LLO
con~truction option:
20
~ t Ill _, ... Ill s s s a • _,
i ... 0
i u s r
D 180-20689-1
0.9
38Y£ARS
0.7
PORTION OF SILICON
INITIAL POWER
0.6 AVAILABLE
0.6
OA
0.3
0 60 100 150 200 2SO 300 350 400 .e&O
THICKNESS OF CELL COVER, pm
Figure 1-17. Photovoltaic Array Radiation Degradation Characteristics
100
eo
ID
40 • • •
20
e THUS All FACETS Will 3E INSTALLED AT LEO e GEO-ASSEMBLED SPS IS LESS THAN 1% LIGHTER
TRANSFER EFFECTS IALL FACETS OUTI --._____
DEGRADATION CURVE FOR AlUMINIZED KAPTON CFROM PROJECT ABLEI
...E:!!... • 1.0505 69.3'.
CONCEN I RA TOR MASS IS 8.706% OF SPS
l5Jl5%) X c• .7011%1 • 0.44% of SPS
45DAY1•8 YRI 900AY 1•18 YRI
180 DAY 1=28 YRI
1 1800AY TRANSFER +38YEARS
72.l'Jli
19.3"
0---~~~---~~-'------------~.....1~--~---~-----------~--------...._--..___._ 0.01 0.1 1.0 10 100
YEARS EQUIVALENT GEOSYNCHRONOUS ORBIT EXPOSURE
Figure 1-18. f.elf Power Transfer Has Utde Oversizing Impact
:!I ()lUGINAL PA:; or pOOR QU
D 180-20689-1
(I) The SPS moduks must have chemical propulsion attitude control capability with suftident
control authority to establish a sun-pointing orientation to activate th•: power generation sys
tem. Th!s capability is al~o required to successfully ..:xecute the orbit transfer, in view of fre
quent passage through the Earth's shadow.
(2) Orbit transl er simulations by the FSTSA study indicated that a typical 180-day transfer would
experience 800 to 1000 occultations by the Earth's shadow. In GEO service the satellite will
experience about 80 occultations per year.
(3) Satellih: modules arriving at GEO must be joined together. \I hcreas '.f constructed at GEO the
satellite may be of a rnon1Jlithic dc!>ign. or :f modular can be construded with moduks joilll·d.
One concept for module joining is illustrated in Figure 1-19. This concept b db~.-u~sl.'d in morl.'
detail in the body of the report.
Operations Considerations-No strong disaiminators in or::rations were found. LEO '-·onstn11.:tion
has more distinct kinds of operations. notably chemical and electric orbit transfer operations (chem
ical for crew rotation and resupply at GEO) and SPS module assembly operations at GEO. The
number of orbit transfor vehicles in flight at one time all requring control is ab0ut double for LEO
construction. 13 :! vs 16 at an SPS addition rate of 4 per year) but the number of HLL V operations
is less, as discussed above.
Collision Considerations-LEO construction operations result in an increased risk of collisions. The
situation for the photovoltaic SPS is summarw:d in Figure 1-:!0. The collision analysis is described
in ti.e body of the report.
System Cost Differential Factors-The~e dre discussed in conjunction with energy comersion co~t
differentials. LEO construction consistently shows Iowa overall cost as a result of rt!duced cost for
Earth-to-orbit transportation.
Orbit Transfer Complexity-The sdf-powen:d operations associated with LEO construchon arc
more compkx as r~gards propulsion systems. flight control. guidance and navigation. and software.
Orbit transfer systems arc discussed in some dl.'pth in the body of the report.
Figure I-~ I summaritcs the construction loi.:ation evaluation. A hullet shows the preferred option
for each evaluation factor. Th·.:re an~ b bullets for GEO and 3 for LEO which indicates GEO con
struction. However. the co~.t of LEO construi.:tion has consistently been found to be cheaper than
GlO. Either option is workable. LEO is cheaper, but more i.:emplex. In a '-·ommercial environment
i.:osts will eventually dn\'c the decision. Much mon: interesting is the question. not where satellite
number I 0 or 50 will bl.' built but where will the first one he built. The condusions of <.-. .. r anJlysi!>
may not appl} to thi~ ':ucstion. Thi.' rci.:ommcndation!> in the Figure arc aimed .1t rt!Jucing Sl'lhiti\·
ity of the continuing analy~i~ to thl.' LEO v~ c;Eu is.,ue.
22
0180-20{>89- l
SPHJI NEW MODULE ARRIVAL
-
e CLOSE TO WITHIN 1000.2000 M WITH PROPULSION
INITIAL DOCKING Iii ALIGNMENT
MOVEABLE~ DOCKING \ CRANES
No. t
/;-
l>OCK1NG MODULES
OOCKlhG I RECEPTACLES ' ...
e MODULES HAVE DIFFERENT e 111nTUDE eALTITUOE
e MA5S"'8Mk~
FINAL POSIT!( ~ING
CONTROlS ATTITUDE ANO CLJSING SPEED
MODULE No.2
r;JLLSINTO POSITION
Figure 1-19. Satellite Module Docking at GEO
... 711
;; Ill ~ :> 0
~i II!~ ...
" .. zU o< 1:: og !! 0 ~ ... 8i
2ID
15
10
6
REGIONIKMI
TIMEIN REGION IDAYS
CONSTRUCTIQN
500
ORIGINAL PAGB I! OF POOR QUALl'l'Y
500
TO
1000
1C.I
·:·:·::·:·:: - GROWTH ::·:·:·:·:·:· OBJECT
......
1000 TO
2000
22.2
MODEL (YEAR 20001
-CJRRENT OBJECT MODEL IYEAR 1975)
2:llOO TO
3000
11.0
3000
TO 5000
22.3
~
5000 TO
10000
29.9
figure t-20. Number of Collisions
• 3X 3M OBJECTS • NOOBJECTClEAN\JP e NO AVOIDANCE DURING TRANSFER e 100%ARRAY DEPLOYED AT GEO e ~OF ARRAY DEPLOYED
DURING CONST. & TRANSFER
0 ......
10000
TO
2!000
34.2
0
20000 TO
35788
39.8
GEO
oPS
10,950
D 180-20689-1
For a dewelopment program. these kinds of questions arc important:
• When must manned GEO operations be-gin'!
• What are relative transportation costs with dewlopmental Earth launch system (q; .. shuttk
derived HLLV)'!
• Can the: dcwlopmental SPS confaguntion (such as 1-GW module) be tr.ansfem:d to GEO with
transmitter inSlalkd or stowed'!
• Can the developmental SPS configuration survive the transfer radiation environment?
• What is the program funding vs time compari- n~
Program funding vcrst1S time is always an important factor in deftlopment decisions. For LEO con
struction. ekctric propulsion must be developed. while for GEO. more in,-esunent may be needed in
~ ~tion~ and in earlier manned GEO operations.
Cost Diffeteatial Factors-This discussion begins with energy payback considerations. Solar cells arc
very energy intensive. Pr.:senkd in figure 1-22 are energy costs in kilowatt hours per kilogr.am of
"'"dk. The e.•crgy payback for solar cells as a function of this energy cost is also shown on two
5alcs These seal~ show SPS and ground applications. Pricing the energy at 40 mills per kilowatt
hour. the actual cost of 4he energy is shown on the outside scale.
The main reason toda) 's \.'l:lls are so intensiw ts that yields are very poor. Most of the silicon. in
which a great deal of energy is invested. ends up as waste (saw filings and grindings•. Continuous
proccSSt"s can probably reach a yield ran~ of 60'K to 800( makino= the payback very attradive.
Eni.:rg)· c~t is a basic factor in the cost of solar cells. like materials cost in building hardware. If the
energy cost is below l ~/watt one might be reasonably confident that "'-ells in the 1~/watt r.ange,
made by a continuous production process. would be possible.
Why is energy cost important? The reason is that energy payback tim~ is economically significant.
Typical economics equations uSc:d. for example. by Caputo and Truscello in the JPL report. predict
the cost of energy from an energy system. One can dose the loop in these equations b) setti:'lg the
capital cost of the eneri,'}· in\·esteJ in the system equal to the capital cost of cnern that the system
produces. In other words one does not borrow from a cht>ap energy system to create an expcnsi-..-e
energy system. Wirn typical economic factors. ene~y payback less than about 8 years is essential.
Othen1;ise. enc:rgy cost will spiral upward ever more rapidly. as inJicated in Figure 1-~3. With con·
tinuous pro<ludion proceSSt":. for solar cells cor with thennal engines•. SPS payback (for the total
s)·)tem • is I 1; to 3 yeah where this curve is not very stei.:p. With its short lyba1:k. SPS should have:
economic ad"anta~es when the: system tedmology is m.iture.
24
MEHRREO CONITRUC-
EVALUATIOll FACIOR TION LOCATION
LEO GEO
el 'l'RAlllPORTATION • RIGUIRPllMS .. a.nucTIOll lllO
B£QUIREllEll1'S sn.ECTIOll
cl IPIOVIAAU. • -llEGUIRBIBlfS
• IPIPEllFORMAllC£ MD • 0£GRADATION l'OTEllT1AL
tlUl.:Hlfll DlfffRUmAl EFRCIS •
• SYSTEMST...-... • REOUIRDEIJ1'S
fl Ol'ERATIC*S • COllSIDERATICMG
NCOLLISIOll COllSIDERATIOICS •
I SYSTEM COST • DIFFERENTIAL FA.."JOAS
J OR&ITAL TRMSFER CDm'UJUTY FACTORS •
D 180-20689-1
D&:ISlCJllORIVER
UO REQUIRES LESS FLIGHlS AlllO LESS CNt-ORaT PROPELLANT TRANSFER
•uo DRAG 6 l>Altlt P£RIOOS VS. GEO RAOIATIOel 6 OISTAM:f
UORlOUIRU~lATIOll
6 OTHER SPECIAUZATION
DEGRADATION DUE 10 VAiii ALLEN RADIATIOllCM BE ~TED
ffWER lAUlllCHES fOR LEO
LEO STARnJPMORf COMPLEX
UO HAS llORE DISTINCT KllmS OF Of'£RA TIONS
A80UT 15 COLUSIOlllSISPS FOR LEO VS 1 FOR GEO
UO AllOUT 2" CHEAPER OV£RAU. TRANSPORTATION
ELECTRIC PROl'UlSIOll llEOt llORE COMl'l.EX
HIGHLIGHTS
• EllNER LEO OR GEO CONSTRUCTION IS A VIABt.E OPflON
• LEO IS LOW£R COST BUT-E a...EX FLIGHT CONTROL; PAOl'UUION
e •A COl&WRCIAL ElllVIAOMIENT COST Will DRIVE THE OECISIOll
e llllTIAl DtCISIONS Dfl'ENDEllT Olll DEVEll)PMENT PflOGRAll
• lmCUAR ANSl'ftR-eont llDDES PROBA8l Y HAVE THEIR PlACE
• SELECI' llOOl!I~ SPS FOR a>NSTRUCTIOfl BASE ANALYSIS
F1g111e 1-21. Consaruction Locaaioa Evaluation Summary
' D
a: z ~
i Ir 0 a
~ c ?: K > I 6
I • > z f • 4
2
• Sll.ANE PROCESS
• ENERGY OOST l.04IKWlf
• SPACE CELLS• 111' BLANKET EFFICIENCY 6 GS WTS EFFICIENCY. 30 K1ftfMl-OAY
"' • GROUND CELLS• 141' BLANKET ~ ~
EFFICIENCY 6 9°" POW£R .. u COLLECTION EFFICIENCY. 5 l(WHIM2.oAy .. • 0 0 • " c %
?: 2 :c K " u i ~ > c > .. 0 POTPmAL c .. FOR z t CIONTllllUOUS
' ..
PROCESS
TYPICAL TODAY
• 0 •o .2 A
YIELD KG SOLAR CELLS PEA KG SEMICONDUCTt'A GRADE SILICON
Fiple 1-22. Energy Costs and Payback for Silicon Solar CeDs
25
ORIGJNAL PAGI • or POOR QUALITY
1.8
DI 80-20689-1
Cost differential factors reflect cost impacts of all the evaluation factors. Thi! data shown in Figure
1-24 are for a 112-SPS program. for our preferred SPS designs. The number I unit SPS will be a sig
nificantly higher cost than the program average. Also. note that there are some things t'tat were not
'-'"OSted in Part I. Our ROM estimate of the range for the uncosted items is shown.
We did the costing in two ways. first was in a mature industry fashion. a projection of things in a
commercial environment with high quantities of mass production. The second method was aero
spa~ cost prediction techniques, using our parametric cost model. For satellite production. the
mature industry projection and the higher aerospa"-e prediction are shown. Transportation costs
used only the aerospace methods. The results were mature industry system costs trending LI less
than S2.000 a kilowatt for the I 12-SPS. No significant differences were sc:en between the silkon
photovoltaic and Brayton thermal engine. Typkal LEO versus GEO differences are also shown.
Shown in Figure 1-25 are two alternate systems costs to provide an idea of cost r-.mges. The silicon
array addition system is more massive than the annealable system and suffers a significant satellik
imract if constructed in LEO. The gallium arsenide system costs are a rough-order-of-magnitude
projection because of the relatively great technology extrapolation. Because it is low in mass . .,·ery
low potential costs are projected for the future. We did not know how t" .:stimate an uncertainty.
Also in the gallium a~nide case. the U:.0-(;l:.0 diUerence 1s less. because the satdlite is low in mass
and the transportation cost contribution is less significant.
Transportation Evaluation Summary--The results of the transportation add-on t?'ik are summariz.:d
in Figure 1-26.
Two Earth launch options w.:re analyzed: ( 2) A ballist,.:. two-stage sea reco.,·ery \'dtide with a
retractable payload shroud that was 1 O<Y1c recoverabk. ( ~) A two-stage wing-wing whide that was
also )()()';( recoverable. No significant diffaences Wt!r.: found in cost pt!r flight or pl!rformance. For
the ballistic system tt.~ main technical concern is sea recowl). It appears feasible. but there is not
much data base. For the! winged system. the lowest achievable payload density is considerably
higher. There are conc.:ms about launch and recovery siting because the booster is a down range!
lander and a suitable place to launch must haw a down range ,·ecovery site. The wing-wing vc!hicle
also has a somewhat higher DDT &E cost.
Orbit transfer options included a space-based :md a ground-based OTV. and self-power. Self-power
le~ns transportation costs about 25'1. The space based OTV showed 15' (better performance than
the ground based OTV. Thi: space-based orbit transkr vehicle requires on-orbit propdlant transfer
but based on work Joni." by General Dynanucs. it appears possible to transfer the propellant without
rotating the staging ha~. It may be sufficient maely to rotak th.: propellant by using electric
pumps to withdraw the propdlant and inject it into the OTV tanks in such a \\ay that a rotation is
set up within the tanks.
26
, ..
•
••
SAME CELLS USED IN SPACE
2
TYPICAL RANGE FOR TOTALSPS
•
D 180-20689-1
6 8
ENERGY PAYBACK TIME. YR
• CAPITAL COST IN ADDITION TO ENERGY • S1CIOOIKWe
• CAPITAL COST OF ENERGY 911V£STED • CAPITAL a>ST OF ENERGY PAOOUCED
• SOLAACELLOATA FOR CURRENT CELL PAOOUCTIO!ll natNOLOGY
18
TYPICAL SILICON SOI.AR CELLS USED ON GROUND
12 14
F"....,e 1-23. Energy Payback Tune Is Signif"acant!
MATURE SYSTEM COSTS TRENDING TO LESS THAN $2000/KWe
SILICON CR1/ANNEALABLE
LEO
r--, I I I I I I I I
GEO ..--, I I : I I I I I
l'RAVTON 1650K
LEO
r-, I I I I I I I a I I
GEO
r--1 AEROSPACE 1 : COSTING : 1 DELTAON I I SATELLITE I I PRODUCTION
SATELLITE PRODUCTION (MATURE INDUSTRY)
CRE\Y ROTATION & RESUPPLY
FREIGHT TRANSPORT
NOT COSTED IN PART I
• CONSTRUCTION BASE AMORTIZATION
• CREW SALARIES
•OPERATIONS& SUPPORT COSTS OTHER THA'4 TRANSPORTATION
• GROUND RECEIVING STATION CUSED JSC VALUE FOR MPrSI
ROM RANGE IS $300-$500 KWe
Figure 1-24. Cost Differential Facton Recommended Reference Systems (112 SPS Program)
27 ORIGINAL PAGE IS or POOR QUAUIY
I !
i 100D
SATELLITE IMPACT
D 180-20689-1
SILICON ARRAY ADDITION
LEO
r-, I I I I I I
GEO
r - 1 AEROSPACE I !COSTING I 1DELTACN
1SATELLITE 1 PRODUCTION
GALLIUM ARSENIDE :R•1 ANNEALABLE
LEO
1
GEO
I 1 I I I I I
I
SATELLITE PRODUCTION CROM PROJECTIOl'.ll
NOTCOSTEDINPARTI
• CONSTRUCTION BASE AMORTIZATION
• CREW SALARIES •OPERATIONS& SUPl'ORT
COSTS OTHER THAN TRANS?>ORT A TION
• GROUND RECEIVING ST A TION IUSED JSC VALUE FOR MPTSI
CREW ROTATION & RESUPPLY
FREIGHT TRANSPORT
Figure l-2S. Cost Differential Factors (112 SPS Program)
FREIGHT LAUNCH OPTIONS ORBIT TRANSFER OPTIONS
' ! I
.L
• PERFORMANCE AND CDSTP£R FLIGHT ABOUT EOUAL. <S'IO/LB
e BALLISTIC CONCERN: SEA RECOVERY"
e WING/WING CONCERNS: • PAYLOAD BAY DENSITY • LAUNCH & REC.OVEllY SITING • HIGHER DDT&E COST
CHEMICAL
SPACE GROUND BASED BASED
ELECTRIC
SELF POWER
e SELF.f'OWER REDUCES NET TRANSPORTATION COST ABOUT 25"'°
e SPACE-8ASED CHEMICAL OTV ABOUT 15'4 BEnER PERFORMANCE
e SELF.VOWER CONCLRNS
• RADIATION DEGRADATION • COMPLEXITY •COLLISION
• SPACE·BASED OTV cor~CERN. PROPELLANT TRANSFER
Figure 1-26. Transportation Evaluation Summary
28