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Constraints on Electrical Power System Design From IPS Operation

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1. SS Table 3 1 EPS Sizing and available MB Power for IPS Operation NSSK manoeuvres IPS operation for NSSK tasks is possible without impacts on EPS provided that the following conditions are met IPS operated only outside eclipse seasons at SS the EOL batteries DOD during IPS operation must be 75 max e the batteries must be fully recharged before a second IPS firing occurs IPS operated also during eclipse seasons e at SS and at VE the EOL batteries DOD during IPS operation must be 75 max e at SS the batteries must be fully recharged before a second IPS firing occurs e at VE the batteries must be fully recharged before an eclipse occurs and last but not least the overall batteries stress must be within the operating limits of the battery cells 4 IMPACTS OF NSSK IPS OPERATION The impacts of NSSK IPS operation on EPS have been evaluated for the RITA configurations provided in Table 2 6 1 E W accomodation has been analysed for RITA 10 15 and 18 systems only after considerations on available MB power versus number of operating thrusters at the same time and operating time constraints as well All parameters relevant to NSSK IPS operation and power requirements have been computed for the four IEPC 97 184 1125 satellites classes and based on IPS operating cycle as described in 2 2 1 2 2 2 and 2 2 3 RITA s PSCU Power Supply and Control Unit electronics for Anti Earth and E W thrusters allocation req
2. carried out between the supply of the IPS power demand at beginning of life either via the solar generator or via the spacecraft batteries The increased number of battery charge discharge cycles is also considered versus battery expected lifetime battery charge rates and battery charge regulator configuration Main bus protection and thermal dissipation constraints are also discussed The results of the above trade off is then summarised in defining the optimum configuration of an EPS sized to supply a GEO satellite equipped with an IPS with the minimum overall mass The specific design constraints are also highlighted Key Words Electric Propulsion IPS Ion Propulsion RITA EPS NSSK GEO satellites 1 INTRODUCTION Ion thrusters require electric energy to operate When compared with the chemical systems or other electric propulsion systems like the arcject and SPT Stationary Plasma Thruster RITAs being characterised by a high specific impulse Isp allow significant propellant mass saving Typical RITA advantages vs arcject and SPT electric propulsions are shown in Figure 1 1 where the launch mass saving and the spacecraft S C platform capability improvements are reported in applications where IPS is used for NSSK tasks in GEO satellites Additional S C dry mass capability increase is expected to be gained replacing the apogee motor with ion thrusters of some hundreds of mN thrust level coupled with a different GEO transf
3. IEPC 97 184 1122 _ CONSTRAINTS ON ELECTRICAL POWER SYSTEM DESIGN FROM IPS OPERATION L Croci P Galantini A Trivulzio FIAR S p A Space Division a Finmeccanica company Via Montefeltro 8 20126 MILANO 1 tel 439 2 35790 1 fax 39 2 33400981 E mail fiarskco iol it H Bassner Daimler Benz Aerospace AG Space Infrastructure Postfach 801168 81663 MUNICH Germany tel 449 89 60723126 fax 49 89 60725070 ABSTRACT Ion Propulsion Systems IPS like the Radiofrequency Ion Thrusters Assembly RITA from DASA are now at the threshold of application on commercial satellites and appear to be a very attractive alternative to the chemical propulsion systems to perform the North South Station Keeping NSSK manoeuvres of geostationary GEO satellites as well as to perform orbit raising manouvres RITA IPSs are available in several configurations from 15 to 200 mN thrust levels and are characterised by a large throttling capabilities to adjust the thrust level to meet the optimum combination of operating time and Electrical Power System EPS load during the different mission phases Starting from the operational characteristics in terms of electric power demand daily switching cycle and operating time of the different RITAs the influence of the relevant requirements over the electrical power system EPS characteristics is evaluated with particular consideration for the energy source sizing A trade off is
4. age i e 100 V fuses are the favourite choice for all RITAs 9 EPS THERMAL ASPECTS IPS implementation requires additional S C heat rejection capability due to e dissipated power due to IPS e additional dissipated power in the EPS In fact the MRU has to provide the additional power required by the IPS via SA and batteries when IPS is used for NSSK tasks Figure 9 1 shows the power dissipated by the RITA and the additional power to be dissipated by the MRU as consequence of RITA operation To reduce the MRU thermal constraints when RITA 18 or RITA 26 are implemented the thrust level can be reduced increasing the IPS operating time Thermal Control Requirements IPS Dissipated EPS deta Power Dissipated PWR m eee z 3 ES 3 8 SPT 100 RITA 10 25 a RITA 10 1 RITA 10 15 a RITA 15 a ITA 10 25 b 2 a for Anti Earth b for EW arrangement Figure 9 1 Additional S C Thermal Rejection Requirements For orbit raising tasks IPS is always operated via SA and therefore no additional constraints on MRU apply during this mission phase 10 ESD CONSTRAINTS Electromagnetic interactions between plasma and satellite structure occurs if charged ions are emitted IEPC 97 184 1128 No additional precautions have to be taken with RITAs since very few charged ions are emitted by the thruster as measured and the flight test data from the EURECA experiment 11 RITA ADVANTAGES To compare RITA versus oth
5. al Eagle Picher Industries IEPC 97 184 1129 4 B Thiard G Beaufils H Declerq SPT Electrical Module Development 2nd European Spacecraft Propulsion Conference 1997 ESTEC Noordwijk The Netherlands 5 M P Burgasov et al The Results Of Complex Work Concerning The Problem Of Electric Rocket Thrusters Integration With Spacecraft And Its Subsystems 2nd European Spacecraft Propulsion Conference 1997 ESTEC Noordwijik The Netherlands 6 J F Roussel J Bemard Numerical Simulation Of Induced Environment Sputtering And Contamination Of Satellite Due To Electric Propulsion 2nd European Spacecraft Propulsion Conference 1997 ESTEC Noordwijik The Netherlands
6. bsystems of the spacecraft to analyse impacts and constraints On the EPS these constraints are function of several parameters like satellite mass Mission time IPS thrust level and related power consumption thruster allocation and AOCS strategy needed to operate also during eclipse periods etc 2 IPS OPERATIONAL CHARACTERISTICS IPS can be used on GEO satellites to perform efficiently several tasks e autonomous and smooth NSSK manoeuvres with consequent improved antenna pointing accuracy less frequent ranging operations and easier collocation of satellites e efficient and fast satellite repositioning in orbit e End of Life EOL de orbiting orbit raising and final orbit circularisation with hybrid propulsion chemical plus IPS or full ion propulsion e East West Station Keeping EWSK manoeuvres The first major application of IPS on GEO spacecraft s is the replacement of chemical propulsion for NSSK tasks NSSK manoeuvres are performed to compensate the required thrust velocity increment 47 m s year around the orbit s nodes that occur at 90 and 270 positions of the orbit Today the NSSK manoeuvres are executed about every 70 days and manually controlled from the ground staff With IPS the NSSK manoeuvres are to be executed once or two times per day and can be done autonomously by the spacecraft itself 2 1 Satellite Performances GEO satellites are growing in mass installed electrical power and mission lif
7. constant period of 12 hours or every 36 hours 2 2 2 East W ion for NSSK In the E W configuration the thrusters are to be operated in pair No radial component have to be compensated and only one firing per day can be done North or South thrusters but duration has to be doubled with respect to two operations per day Therefore the NSSK manoeuvre is executed once a day but with a constant period of 24 hours or twice a day with a constant period of 12 hours The canting angle versus the N S axis can be decreased to 35 2 2 3 Allocation for NSSK and Orbit Raising Two possibility exists e separate and different thrusters for the two tasks or e single thruster for combined tasks In the Anti Earth approach mounting the thrusters on gimbals with large pointing capability makes possible to change the thrusters position to perform orbit raising or NSSK manoeuvres For orbit raising two or four thrusters have to be operated depending on the power available inclination with respect to the flight direction could be 10 The payload is off during this phase and all power is availabe to feed the IPS For NSSK manoeuvres the thrusters will be brought into a position where the thrust vector pass through the CoG of the satellite One thruster is operated at a time at reduced thrust level if there are limitation on available power for IPS operation The increased thrust available by operating two thrusters at the same time can be
8. e RITA power electronics generates a smooth MB voltage transient due to RITA on off switching No particular measures due to ESD phenomena have to be considered for RITA systems The critical aspect of IPS implementation is represented by the additional S C thermal rejection capability requested and in particular the requirement for the MRU to provide contemporary power from SA and batteries In case the IPS is implemented to reduce launch mass this aspect has to be investigated with the available S C thermal rejection margins at Winter Solstice In case IPS is implemented to allow embarkment of more complex payload without increasing the launch mass the available S C capability increase is used partially to increase the payload performances and the rest to increase electric power availability and thermal rejection capability In any case to perform NSSK tasks the selection of long life gridded ion thrusters like the RITA 10 systems reduces the additional power to be dissipated by the MRU References 1 H Bassner K Bohnhoff A Trivulzio Commercialized Ion Propulsion For North South Station Keeping Of Communication Satellites 25th TEPC 1997 Cleveland Ohio 2 S Arcisto M Gambarara A Garutti A Trivulzio A Truffi H Bassner H M ller Power Supply And Control Unit PSCU For Radio Frequency Ion Thrusters RIT 2nd European Spacecraft Propulsion Conference 1997 ESTEC Noordwjik The Netherlands 3 NiH User Manu
9. er ion propulsion concepts a design exercise similar to the one described before has been performed considering an IPS realised with SPT 100 thrusters whose main performances are summarised in Table 11 1 Sos Parameter Value j C ee 1 80 mN nominal corrected for beam divergence Table 11 1 SPT 100 IPS Main Performances Comparing the results the RITA systems provides the following advantages in spite of the lower thrust to power consumption ratio with respect to SPT technology no penalizations on EPS sizing is caused by RITA e the low beam divergence allows both Anti Earth and E W thrusters allocations with canting angle as low as 35 for RITA but not for SPT 100 RITA 10 requires only one half of the heat rejection capability increase compared to SPT 100 RITA 15 is similar to SPT 100 e RITA does not generate ESD problems very few charged ions are emitted and therefore no particular filters to decouple RITA s PSCU and thruster are required On the contrary due to the special ionisation process and to the open extraction area SPT emits ions with different exhaust velocities and filters have to be inserted to avoid conducted susceptibility problems Ref 4 5 The filter losses have not been considered in the SPT required power consumption indicated here above e RITA s soft start up reduces power loads variations With SPT the MB load variation at switch on is even amplified because 50 more power
10. er orbit e g supersynchronous transfer orbits Sateilite Mass at Launch sc on an or TOSA No SET TEs 5 years mission time S C Dry Mass Capability EP mass exctuded 4 050 kg at launch 2500 kg BOL 15 years mission time Arcject SPT 100 RITA 10 EP Technology for NS8K Figure 1 1 Typical Advantages of RITA IPS 60 ardeat SPT 100 RITA 10 EP Tesh tor NESK To meet commercial market requirements four RITA versions are available with thrust levels from 15 to 200 mN Ref 1 0 40 8 100 120 140 160 180 200 Thrust Level mN RITA 10 RITA 15 RITA 18 RITA 26 IPS MB Power Ne ee Figure 1 2 RITA Ion Propulsion Systems One of the most interesting capability of the RITAs is the throttling performance associated to high specific Copyright 1997 by the Electric Rocket Propulsion Society All rights reserved impulse with this capability the thrust level can be adjusted to meet the optimum combination of operating time and EPS load constraints during the different mission phases Figure 1 2 provides the thrust level capability and related overall Main Bus MB power consumption of the planned RITA systems Even if primarily designed for commercial GEO satellites RITA IPSs can find application also in scientific earth observation and planetary missions However IPS implementation is not a simple straightforward approach and requires accurate trade off on the different su
11. etime as well Table 2 1 provides the four satellite categories that have been considered representing the largest GEO satellites market expected in the future 2 430 3 6 Overall minimum MB Power P L power SM power Batteries Charge power Table 2 1 GEO Satellite Main Performances a IEPC 97 184 1123 The launch masses reported assume chemical propulsion for apogee injection into GEO orbit from geostationary transfer orbit GTO A Fully regulated EPS i e Main Bus MB voltage kept constant in both sunlight and eclipse conditions has been considered 2 2 RITA Thrusters Allocation The ion thrusters for NSSK tasks can be allocated in the Anti Earth configuration or in the more simple and efficient E W configuration Ref 1 The Anti Earth allocation is easily adaptable to existing S C s platforms while the E W allocation is recommended for the platforms conceived for IPS operation since the beginning 2 2 1 Anti E odation for NSSK In the Anti Earth configuration the thrusters are to be mounted on gimbals for alignment towards the spacecraft s CoG Centre of Gravity canting angle depends on satellite geometry 45 towards N S axis is a standard A North thrust firing at 90 has to be followed by a South thruster firing at 270 in order to cancel the effects of the radial component of the thrust eccentricity impact Therefore the NSSK manoeuvre has to be executed twice a day with a
12. he following constraints have to be taken into account in selecting the EPS architecture e all SA power bas to be delivered to the MB gt sequential batteries charge strategy should be avoided e Main Regulation Unit MRU dissipation increases during sunlight operation e high power loads switch on off response No batteries charge via dedicated SA sections architecture has to be selected being SA power dedicated to battery charge to be used also for IPS operation Sequential batteries charge strategy in case of BCR failure imposes a complicated batteries management and therefore has to be avoided Consequently redundancy of BCR functions have to be implemented This approach is already common on several EPS if not about 2 kg EPS mass increase has to be taken into account Anyhow in case of emergency conditions the IPS can be switched off and sequential batteries charge can be performed During sunlight conditions some power has to be provided by the batteries for IPS operation during NSSK manoeuvres Therefore the MRU must be able to operate when power is provided by both S R and BDR functions with consequent increased unit dissipation For better EPS and IPS optimisation a single bus EPS is highly recommended 5 BATTERY STRESS RITA operation places additional stress and increased cycles on the batteries This demand which is repetitive over the life of the mission imposes peak power requirements which will necessitate batter
13. iciency 93 L1 losses between S R and SA 3 L2 losses between BCR BDR and batteries 2 K factor battery charge rate efficiency coefficient 1 05 Figure 3 1 EPS Block Diagram The EOL SA power at Summer Solstice SS represents the minimum SA available power but the worst case for EPS sizing is represented by the Spring Vernal Equinox VE conditions when the SA must provide the power also to recharge the batteries Therefore the EPS has been first sized at VE with the following constraints energy in eclipses provided by two batteries e 75 nominal Batteries Depth of Discharge DOD parallel batteries charge charge rate C 15 e possibility to sequential batteries charge charge rate C 10 e SA fitted with Si cells e no additional MB power load considered for IPS operation The EPS main performances and the available MB power for IPS operation are provided in Table 3 1 and 3 2 _ ___sSatellite Cat i Cat 2 Cala Gat ac W 285 570 760 1 140 Total MB pwr W 8 000 Wh 12 710 ati 4 EOL SA pwr W VE 3 188 6 377 8 502 SS 3 108 6 216 8 288 12 433 BOL SA pwr W VE 3 916 7 832 10 442 15 664 SS 3 817 7 635 10 179 15 269 fo Xo N EOL MB pwr for IPS operation W VE 285 570 760 1 140 SS 210 419 559 838 BOL MB pwr for IPS operation W E 970 1 939 2 585 3 878 876 1 754 2 337 3 507
14. ing manoeuvres can be considered to save additional mass If thrusters are dedicated to this task they can be mounted in fixed position and aligned versus the flight direction or can be placed on gimbals to be used for both orbit raising and NSSK tasks To avoid disturbances to the spacecraft the thrusters have to be operated in pair s The high thrust level stability the fine thrust level adjustment capability and the large throttling range associated to a high specific impulse make RITAs a suitable candidate for this tasks The S C s payload is normally off in this phase of the mission thermal control has to be active to keep the equipmet within minimum temperature range and the IPS must be operated during sunlight conditions only and switched off as soon as the satellite is entering into eclipse being the batteries utilised for thermal control purpose only during this phase Assuming that the required MB power is available up to four thusters can be contemporary operated achieving up to a nominal thrust of 320 mN for RITA 18 and 800 mN for RITA 26 system 70 100 V MB voltages are recommended for this application The throttling capability of RITAs allow thrust level reduction increasing the time required to performed the task in case EPS constraints impose less IPS power consumption In case of one thruster failure at beginning of mission only two thrusters are stil available to perform the task 4 4 EPS Architecture Impacts T
15. is required by SPT for some millisenconds with respect to normal power e the RITA large throttling capability associated to high specific impulse allows optimum combination of power consumption and operating time ratio e The RITA low beam divergence has negligible impacts on SA degradation Recent data on SPT 100 thrusters indicates serious problem if 45 canting angle is used due to direct impingement of the plume on the SA in certain orbital conditions Ref 5 6 If confirmed a large canting angle has to be implemented with reduced benefits from the high thrust level e RITA long thruster lifetime gt 20 000 hours expected 12 SUMMARY Today GEO commercial spacecraft can be equipped with RITA IPS operating also during the eclipse seasons without impacts in terms of EPS energy source sizing thanks to the increased available on board electrical power with respect to previous spacecraft sgenerations and due to availability of NiH batteries A combined assembly for NSSK manoeuvres and orbit raising tasks is possible accomodating the thrusters on gimbals with high regulation angle adjusting the thrust level according to the satellite mission phase if MB power constraints exists Use of fuses for MB protection from short circuits is possible in most of the cases even if more sophisticated and costly EF or SSPC devices offers best performances in terms of protection and MB transients The soft start up implemented in th
16. lue is much higher and can be in the order of 8 10 kW RITAs have been designed to avoid large power load variations In fact a soft start up is implemented and moreover it is possible to mitigate the MB load variations using the throttling capability function All these operating modes are executed automatically by the PSCU of the thruster upon receipt of the on off command or can be commnaded from ground 8 MB PROTECTION To protect the MB from short circuits two alternatives exists e fuses e EF Electronic Fuses or SSPC Solid State Power Controllers Fuse protection is very popular being very cheap but high margin from nominal to actual value have to be taken and a MB voltage drop of some tens of ms have to be accepted before a fuse blow Considering the in rush current and the required derating rules of the different devices fuses can be used efficiently for loads up to 15 A nominal With a 50 V MB the nominal IPS MB current is in the range of 11 6 to 16 A for the RITA 10 versions 31 A for RITA 15 and 50 A for the RITA 18 Therefore fuses can be considered only for the RITA 10 version while EF or SSPC are mandatory for RITA 15 and RITA 18 unless specific design architectures are implemented in the IPS electronics Ref 2 EF or SSPC complexity are almost proportional to the rated current and therefore power dissipation and cost of a 32 A device is near twice the value of a 16 A device In case of higher MB volt
17. n particular the nodes for NSSK manoeuvres are six hours after or before eclipses In the past IPS operation during eclipse seasons 1 2 hours for 84 days a year was avoided due to the maximum allowable battery stress and the large EPS oversize required to feed the IPS The ever increase of today GEO satellite performances and the replacement of NiCd batteries with NiH type has resulted in e increased available on board power e increased allowable batteries stress and therefore new trade offs have to be performed to quantify the impacts on EPS sizing if IPS has to be operated also during eclipses IEPC 97 184 1124 2 6 RITA Selection Vs Spacecraft Performances Based on the spacecraft s performances identified in Table 2 1 the best application of the different RITA versions is provided in Table 2 6 1 However final selection has to be based on Customer trade off since optimum solution from a technical point of view could be commercially less attractive when benefits from commonalities among the production are taken into consideration or last but not least lifetime demonstration required time is evaluated Ref 1 Table 2 6 1 RITA Applications Vs Spacecraft Performances Cat 2 Cat 3 Cat 4 3 EPS SIZING WITHOUT IPS Figure 3 1 shows a simplified block diagram of a fully regulated EPS The following efficiencies losses have been considered S R efficiency 97 BCR efficiency 90 BDR eff
18. perating temperatures have to be followed 6 SOLAR ARRAY DEGRADATION The embarkment of IPS can produce additional power constraints on the SA due to e additional SA degradation due to the ion beam e additional SA degradation during transfer orbit manoeuvres due to the longer duration with respect to chemical propulsion RITAs as all gridded thrusters are characterised by a low beam divergency gt 90 of the energy concentrated into 12 beam width Considering a minimum canting angle of 35 respect to N S axis the evaluated additional solar array degradation is expected to be less than 1 for a 15 year mission As concerns SA degradation due to longer permanence into low medium orbits if orbit raising and final allocation manoeuvres are performed by IPS the relevant amount is function of the selected transfer orbit and thrust level available to perform the orbit raising Use of GaAs solar cells which are more tolerant to radiations reduce the impacts 7 MB TRANSIENTS RESPONSE IPS on off switching generates a very large load variation to the MB this variation can cause the MB to go outside specified variation range if not properly addressed in the design of the EPS or in the IPS implementation In case of NSSK tasks the power load variation can be in the order of 1 5 3 kW depending on the nominal thrust level and number of thrusters to be switched at the same time In case of use of IPS for orbit raising the va
19. rusters Allocations All RITAs can be operated also during eclipses without any SA EOL power increase with exception of Category l spacecraft were a 115 W SA increase is required A typical batteries charge profile during eclipses is shown in Figure 4 2 1 100 OT NOWMORDASK ANCHOR AIOK NGS Sree weer HH aN N Dally Anti Earth Arrangement IPS Nodes at Time 6 and 18 hours Figure 4 2 1 Typical EOL battery cycles during eclipse seasons Anti Earth Configuration E W Thrusters Allocations RITA 10 15 and 18 only A slightly increase in the EOL SA power at VE is required as per Table 4 2 1 to operate the system also during eclipses A typical batteries charge profile during eclipses for E W thrusters allocation is shown in Figure 4 2 2 IEPC 97 184 1126 82 0 0 1 Required additional EOL SA power can be reduced adjusting thrust level if requested power is not available Table 4 2 1 Additional EOL SA Power Required with E W Thrusters Allocation for RITA Operation Also During Eclipses 3 Cat 2 616 82 LENA 1500 kg BOL 15 Years Mission IPS Operated Also During Eclipses 313 days year RITA 10 25 mN Node 1 RITA 10 25 mN Node 2 o amp gt F a 8 a TT TTTTTT Daily Cycle h Figure 4 2 2 Typical EOL battery cycles during eclipse seasons E W Configuration 4 3 RITA Operated for Orbit Raising Tasks IPS application for orbit rais
20. uire slightly different architectures to minimise overall mass and number of boxes still meeting failure tolerance requirements Ref 1 2 As an example the parameters for IPS operated only outside eclipse seasons and computed for a 2000 kg BOL satellite mass equipped with RITA 10 25 mN are provided in Table 4 1 here below RITA 10 25 mN 2000 kg BOL 15 years mission IPS operated only outside eclipse seasons RITA Operated Only Outside Eclipses 4 1 RITA Operated Only Outside Eclipses From a SA sizing point of view all RITA configurations evaluated can be handled by the EPS without any additional requirement in terms of electrical power or energy to be provided if RITA is operated only outside eclipses i e for 241 days year The batteries DOD at EOL is within the 13 to 33 range A C 15 batteries charge rate provides more than 10 margin to achieve full batteries charge before another manoeuvre has to be executed A typical batteries charge profile is shown in Figure 4 1 1 2000 kg BOL 15 Years Mission C 15 Battery Charge Rate IPS Operated Only Outside Eclipses 241 days year o 8 8 amp B EOL Battery DOD During Eclipses 8 OMAHA ISOM SASENS TE SrSesgungy rere ee Dail cle h EW Arrangement Nodes at Time 0 and 12 hours Figure 4 1 1 Typical EOL Battery Charge Profile During RITA Operation Outside Eclipses E W Configuration 4 2 RITA Operated Also During Eclipses Anti Earth Th
21. usefully utilised during satellite repositioning being the payload off during this phase 2 3 AOCS Operation IPS is normally operated daily but time for orbit determination has to be allowed A seven days AOCS cycle has been considered e g N S correction every day except for the 7th day dedicated to the orbit determination Table 2 3 1 provides the IPS operating requirements for the two _ thrusters allocation arrangements Longer sailing time e g 14 or 28 days cycles increases the number of IPS operating days thus slightly increasing the system efficiency EWSK manoeuvres are still operated with chemical thrusters operation of IPS and chemical systems cannot be done contemporary Operating Nodes per orbit 2 1 12 or 36 Operating days year outside eclipses only _also during eclipses Table 2 3 1 IPS Operating Constraints 2 4 RITA Redundancy Scheme Due to the beam grid geometry adopted and the use of a RF field for the propellant ionisation the RIT thrusters are characterised by a lifetime in excess of 20 000 hours for all versions of thrust levels Consequently considering a minimum lifetime qualification factor of 1 3 all mission requirements can be met with a 2 2 thrusters redundancy scheme in both Anti Earth and E W configurations 2 5 RITA Operation During Eclipses NSSK manoeuvres never take place during eclipses so that the solar array can always be used to power at least partially the RITA I
22. y discharge during both sunlight and eclipse periods The maximum stress is obviously reached at EOL when the power available from the SA is reaching the minimum In order to maintain the batteries stress within the limits it could be necessary to increase the SA size The expected NiH batteries cycles are function of the DOD Ref 3 For 31 electrolyte concentration the following cycles are expected e 70 000 for 30 DOD e 25 000 for 60 DOD e 9 000 for 90 DOD In order to evaluate the overall batteries stress the accumulated cycles x DOD over the lifetime is assumed not to exceed the value of 450 000 a factor of 2 margin from a maximum of 900 000 cycles x DOD achievable with 90 DOD For 15 years mission time the worst case computed overall batteries stress expressed as cycles x DOD are lt 302 000 for S C Category 1 e lt 236 000 for S C Category 2 e lt 193 000 for S C Category 3 e lt 133 000 for S C Category 4 IEPC 97 184 1127 On the above basis the combined batteries stress due to eclipses and RITA operation are well within the allowable value and enough margin is available for the increased satellite in orbit lifetime e g 20 years Therefore no increase of the SA size has to be considered for IPS operaton due to battery stress requirement However to achieve these performances the guidelines recommended by batteries manufacturers and in particular the optimum Charge and Discharge cycles o

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