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The first Japanese geostationary satellite, Engineering Test Satellite Type II [Kiku-2], has been successfully placed at 130°E at the beginning of March 1977.Using beacon transmitters at three coherent frequencies of 1.7, 11.5 and 34.5 GHz which are installed in ETS-II, the Radio Research Laboratories (RRL) of the Ministry of Posts and Telecommunications (MOPT) conduct propagation experiments to obtain preliminary information for the Experimental Communication Satellite (ECS) experiment.The experimental system for propagation experiment with ETS-II is composed of a main receiving station, a rain radar, a radio-meter, meteorological instruments and data handling computers.The receiving data, including signal levels of co- and cross-polarization in these frequencies and phase differences between each of these frequencies and polarization, are sampled every 200 msec.The satellite-to-Earth propagation experiment at the highest frequency has been satisfactorily started on 11 March 1977.  相似文献   

12.
Liquid rocket engines for launch vehicles and space crafts as well as their subsystems need to be verified and qualified during hot-runs. A high test cadence combined with a flexible test team helps to reduce the cost for test verification during development/qualification as well as during acceptance testing for production. Test facility intelligence allows to test subsystems in the same manner as during complete engine system tests and will therefore reduce development time and cost.This paper gives an overview of the maturing of test engineering know how for rocket engine test stands as well as high altitude test stands for small propulsion thrusters at EADS-ST in Ottobrunn and Lampoldshausen and is split into two parts:
• Part 1 gives a historical overview of the EADS-ST test stands at Ottobrunn and Lampoldshausen since the beginning of Rocket propulsion activities in the 1960s.
• Part 2 gives an overview of the actual test capabilities and the test engineering know-how for test stand construction/adaptation and their use during running programs.
Examples of actual realised facility concepts are given to demonstrate cost saving potential for test programs in both cases for development/qualification issues as well as for production purposes.

Article Outline

1. Introduction
2. Historical overview
2.1. Ottobrunn
2.1.1. Air-breathing propulsion
2.2. Lampoldshausen
2.2.1. Attitude control systems
2.2.2. Launcher Propulsion
3. Today's status of hot firing test facilities at Lampoldshausen
4. Test facility engineering know how
5. Conclusion and outlook
References

1. Introduction

Test facilities are an indispensable element for the development and acceptance of space systems/subsystems and components. Hot-test facilities especially with environment simulation (e.g., altitude simulation) are very unique and are specifically designed to their needs.In Germany rocket propulsion developments were started during the 1950s in Ottobrunn near Munich. Beginning in the 1960s developments of attitude control engines and thruster for space crafts were started in Lampoldshausen. In addition to these two plants with test facilities and test capabilities, a third centre with test facilities operated by ERNO in Trauen was built up for the development of the ELDO Launcher (Europa III).In the frame of the consolidation of the different Space Propulsion activities within Dasa (Daimler-Benz Aerospace) in the 1990s as well as the creation of EADS-Space, all test activities were concentrated to the Lampoldshausen site, concluded in 2000.Main reasons for this concentration to one test site were:
• One EADS-ST test-centre in Germany.
• One EADS-ST Test and Engineering Team at one location.
• Multi-use of the three EADS test fields in Lampoldshausen instead of 10 facilities.
• Experts with test engineering know how for development and production programs at one location.
• Synergy effects for test facility modification/maintenance and field support together with DLR.
In addition, cost aspects, especially for test conductions have to be reduced. Therefore, the facility and test requirements have been changed by:
• Using more intelligence in the design and features of the facility (e.g., several test objectives to be tested during one hot-firing test).
• Use of test data for computer simulations as code calibration and therefore reduction of the total number of needed tests.
• Multi-function of test specialists with the main goal to reduce the test team size.
• Computer aided test set-up, firing sequencing and online documentation.

2. Historical overview

2.1. Ottobrunn

A complete overview of all technologies created since the mid of the 1950s is given by Hopmann in [1]. Within this chapter the focus was set on technologies and know how generated in the frame of the Ariane cyrogenic developments at P 59 and air-breathing propulsion [2] and [3].The start of the ARIANE 1 programme and the contract for the development of the HM7-A thrust chamber called for a new facility complex. The erection of the P 59 Test facility was the first high-pressure thrust chamber facility in Europe with a storage level of 800 bars. This high pressure gas was needed to feed the 400 bar LH2 and LOX vacuum insulated run-tanks. For this facility also a special valve test facility was erected in order to test the facility valves in advance to their integration into the test bench (Fig. 1).  相似文献   

13.
In the implementation of the space projects Rosetta and Mars Express, a large-scale series of experiments has been carried out on radio sounding circumsolar plasma by decimeter (S-band) and centimeter (X-band) signals of the Rosetta comet probe (from October 3 to October 31, 2010) and the Mars Express satellite of Mars (from December 25, 2010 to March 27, 2011). It was found that in the phase of ingress the spacecraft behind the Sun, the intensity of the frequency fluctuations increases in accordance with a power function whose argument is the solar offset distance of radio ray path, and when the spacecraft is removed from the Sun (the egress phase), frequency fluctuations are reduced. Periodic strong increases in the fluctuation level, exceeding by a factor of 3–12 the background values of this value determined by the regular radial dependences, are imposed on the regular dependences. It was found that increasing the fluctuations of radio waves alternates with the periodicity m × T or n × T, where m = 1/2, n = 1, аnd T is the synodic period of the Sun’s rotation (T ≈ 27 days). It was shown that the corotating structures associated with the interaction regions of different speed fluxes are formed in the area of solar wind acceleration and at distances of 6–20 solar radii already have a quasi-stationary character.  相似文献   

14.
Significant advances have been made during the last decade in several fields of solid propulsion: the advances have enabled new savings in the motor development phase and recurring costs, because they help limit the number of prototypes and tests.The purpose of the paper is to describe the improvements achieved by SNPE in solid grain technologies, making these technologies available for new developments in more efficient and reliable future SRMs: new energetic molecules, new solid propellants, new processes for grain manufacturing, quick response grain design tools associated with advanced models for grain performance predictions.Using its expertise in chemical synthesis, SNPE develops new molecules to fit new energetic material requirements.Tests based on new propellant formulations have produced good results in the propellant performance/safety behavior ratio. New processes have been developed simultaneously to reduce the manufacturing costs of the new propellants.In addition, the grain design has been optimized by using the latest generation of predictive theoretical tools supported by a large data bank of experimental parameters resulting from over 30 years' experience in solid propulsion:
• Computer-aided method for the preliminary grain design
• Advanced models for SRM operating and performance predictions

References

A Davenas, D Boury, M Calabro, B D'Andrea and A Mc Donald, Solid Propulsion for Space Applications: A Roadmap, 51st IAF Congress, Rio de Janeiro, Brazil (2000).
H Austruy, M Biagioni and Y Pelipenko, Improvement in Propellant and Process for Ariane 5 Boosters (1998) AIAA 98-35588.
Y Longevialle, M Golfier, H Graindorge and G Jacob, The use of new molecules in high performances energetic materials, NDIA Insensible munitions and energetic materials technology symposium, Tampa, Florida (1999).
A.T. Nielsen, J. Org. Chem. 55 (1990), pp. 1459–1466 US Patent 5 693 794, 30/09/1998. Full Text via CrossRef | View Record in Scopus | Cited By in Scopus (58)
Bescond P, Graindorge H, Mace H, EP 913374, 6/05/1999.
G Jacob, G Lacroix and V Destombes, Identification and analysis of impurities of HNIW, 31st Annual Conference of ICT (2000).
B D'Andrea, F Lillo, A Faure and C Perut, A New Generation of Solid Propellants for Space Launchers, 50th IAF Congress, Amsterdam, The Netherlands (1999).
D.W. Doll and G.K. Lund, Magnesium neutralized clean propellant (1991) AIAA 91-2560.
C. Beckman, Clean propellants for space launch boosters, Propulsion and Energetic Panel, 84th Symposium held in Aalesund, Norway (2921994).
B. D'Andrea, B. Lillo, A. Volpi, C. Zanotti and P. Giuliani, Advanced solid propellant composition for low environmental impact and negligible erosive effect, ISTS (1998) 98-a-1-12.
J.C Chastenet and A Mobuchon, Prediction of Air Bag Performance, 5 ISCP, Stresa, Italy (2000).
J. Thépénier, D. Ribereau and E. Giraud, Grain Design for thrust trace shaping in segmented solids for the SRBs IAF-99-S.2.09, 50th IAF Congress, Amsterdam, The Netherlands (1999).
J. Thépénier, D. Ribereau and E. Giraud, Application of advanced computational softwares in propellant grain analysis : a major contribution to future SRM development for space application IAF-97-S.4.06, 48th IAF Congress, Torino, Italy (97).
A. Davenas and J. Thépénier, Recent Progress in the prediction and analysis of the operation of Solid Rocket Motors IAF-98-S2.06, 49th IAF Congress, Melbourne, Australia (1998).
D. Ribéreau, P. Le Breton and E. Giraud, SRM 3D surface burnback computation using mixes stratification deduced from 3D grain filling simulation, AIAA 99-2802, 35th AIAA JPC Conference, Los Angeles, USA (1999).
Mary. Y; “Simulation de coulée gravitaire, validation du code MONTREAL.”, DEA mechanics report, 1995.
P. Le Breton, D. Ribéreau, F. Godfroy, R. Abgrall and S. Augoula, SRM Performance Analysis by coupling bidimensional surface burnback and Pressure field computations AIAA 98-3968, 34th AIAA JPC Conference, Cleveland, USA (1998).
P. Durand, B. Vieille, H. Lambare, P. Vuillermoz, G. Bourit and P. Steinfeld, A three dimensional CFD numerical Code dedicated to space propulsive flows AIAA 00-3864, 36th AIAA JPC Conference, Huntsville, USA (2000).
  相似文献   

15.
The results of studies of longitudinal and LT variations in parameters of the ionosphere–plasmasphere system, obtained using the Global Self-Consistent Model of the Thermosphere, Ionosphere and Protonosphere (GSM TIP), assimilation ionospheric model IRI Real-Time Assimilation Mapping (IRTAM), and satellite and ground-based observational data are presented in the paper. The study of the main morphological features of longitudinal and LT variations in the critical frequency of the ionospheric F2 layer (foF2) and total electron content (TEC) depending on latitude in the winter solstice during a solar-activity minimum (December 22, 2009) is carried out. It is shown that the variations in foF2 and TEC, on the whole, are identical, and so mutually substitutable, while creating empirical models of these parameters in quiet geomagnetic conditions. The longitudinal and LT variations in both foF2 and TEC are within an order of magnitude everywhere except for the equator anomaly region, where LT variation is larger by an order of magnitude than longitudinal variation. According to the results of the study, in the American longitudinal sector at all latitudes of the Southern (summer) Hemisphere, maxima of foF2 and TEC are formed. The near-equatorial and high-latitudinal maxima are separated out from these. The estimate of the contribution into the longitudinal variation in foF2 and TEC for various local time sectors and at various latitudes has been obtained for the first time. In the Southern (summer) Hemisphere, longitudinal variation in foF2 and TEC is formed in the nighttime.  相似文献   

16.
Using modern models of the plasmasphere and exosphere, radial profiles of the rates of ionization losses of protons with μ = 0.3–10 keV/nT (μ is the first adiabatic invariant) of the Earth’s radiation belts (ERBs) have been constructed. To calculate Coulomb losses of protons, we used the ISEE-1 satellite data at L = 3–9 and CRRES satellite data at L ≤ 3 (L is the McIlwain parameter). The relation of contributions of Coulomb losses and charge exchange in the rate of ionization losses of protons has been considered. We have discovered the effect of subtracting Coulomb losses from charge exchange of ERB protons for small μ and L, which can imitate a local particle source. It has been demonstrated that, with decreasing L, the rate of ionization losses of ERB protons decreases as a whole. The radial dependence of this rate only has a negative gradient in the narrow range (ΔL ~ 0.5) in the region of the plasmapause and only for protons with μ > 1.2 keV/nT.  相似文献   

17.
Radio bursts in the frequency range of 100–1500 kHz, recorded in 1997–2000 on the INTERBALL-1 satellite during the solar flares preceding the strong geomagnetic storms with D st < ?100 nT, are analyzed in this paper. The observed long-wave III-type radio bursts of solar origin at frequencies of 1460 and 780 kHz were characterized by large values of the flux S f = 10?15 ?10?17 W/m2 Hz and duration longer than 10 min. The rapid frequency drift of a modulated radio burst continued up to a frequency of 250 kHz, which testified that the exciting agent (a beam of energetic electrons) propagated from the Sun to the Earth. All such flares were characterized by the appearance of halo coronal mass ejections, observed by the LASCO/SOHO, and by the presence of a southward Bz-component of the IMF, measured on the ACE and WIND spacecraft. In addition, shortly after radio bursts, the INTERBALL-1 satellite has recorded the fluxes of energetic electrons with E > 40 keV.  相似文献   

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19.
This work is a continuation of investigation [1] of the behavior of the solar wind’s and interplanetary magnetic field’s parameters near the onset of geomagnetic storms for various types of solar wind streams. The data of the OMNI base for the 1976–2000 period are used in the analysis. The types of solar wind streams were determined, and the times of beginning (onsets) of magnetic storms were distributed in solar wind types as follows: CIR (121 storms), Sheath (22 storms), MC (113 storms), and “uncertain type” (367 storms). The growth of variations (hourly standard deviations) of the density and IMF magnitude was observed 5–10 hours before the onset only in the Sheath. For the CIR-, Sheath-and MC-induced storms the dependence between the minimum of the IMF B z-component and the minimum of the D st -index, as well as the dependence between the electric field E y of solar wind and the minimum of the D st -index are steeper than those for the “uncertain” solar wind type. The steepest D st vs. B z dependence is observed in the Sheath, and the steepest D st vs. E y dependence is observed in the MC.  相似文献   

20.
Attitude reorientation maneuvers were conducted three times on the transfer orbit to obtain the apogee kick motor firing attitude of the Medium Capacity Geostationary Communication Satellite for Experimental Purposes (CS) on the third apogee. After two attitude and five orbit maneuvers on the drift orbit, the CS attained geostationary orbit with station keeping accuracy of ±0.1° seven days after launch.  相似文献   

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