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Monopropellant System
~™ mil ii ii nun mi iiiii iiiii (19) J European Patent Office Office europeen des brevets (11) EP 0 950 648 A1 (12) EUROPEAN PATENT APPLICATION (43) Date of publication:ation: (51) Int. CI.6: C06D 5/08 20.10.1999 Bulletin 1999/42 (21) Application number: 98201190.0 (22) Date of filing: 15.04.1998 (84) Designated Contracting States: (72) Inventors: AT BE CH CY DE DK ES Fl FR GB GR IE IT LI LU • van den Berg, Ronald Peter MC NL PT SE 2291 KJ Wateringen (NL) Designated Extension States: • Mul, Johannes Maria AL LT LV MK RO SI 2013 AE Haarlem (NL) • Elands, Petrus Johannes Maria (71) Applicant: 2804 LK Gouda (NL) NEDERLANDSE ORGANISATIE VOOR TOEGEPAST-NATUURWETENSCHAPPELIJK (74) Representative: ONDERZOEK Smulders, Theodorus A.H.J., Ir. et al TNO Vereenigde Octrooibureaux 2628 VK Delft (NL) Nieuwe Parklaan 97 2587 BN 's-Gravenhage (NL) (54) Monopropellant system (57) The invention is directed to a monopropellant composition for propulsion and/or gas generation, com- prising a solution of hydrazinium nitroformate (HNF) and/or ammonium dinitramide (ADN) in water and/or an alkanol. < CO CO o LO o Q_ LU Printed by Xerox (UK) Business Services 2.16.7/3.6 EP 0 950 648 A1 Description [0001] The present invention is in the area of monopropellant composition systems, for instance for spacecraft pro- pulsion, in emergency systems for jet fighters or in emergency gasgeneration systems for submarines. 5 [0002] Spacecraft propulsion is defined as that needed for the orientation (attitude control) and positioning (orbit con- trol including de-orbiting) of spacecraft after delivery into the required orbit by the launch vehicle. -
Turbopump Design and Analysis Approach for Nuclear Thermal Rockets
Turbopump Design and Analysis Approach for Nuclear Thermal Rockets Shu-cheng S. Chen1, Joseph P. Veres2, and James E. Fittje3 1NASA Glenn Research Center, Cleveland, Ohio 44135 2Chief, Compressor Branch, NASA Glenn Research Center, Cleveland, Ohio 44135 3Analex Corporation, 1100 Apollo Drive, Brook Park, Ohio 44142 1(216) 433-3585, [email protected] Abstract. A rocket propulsion system, whether it is a chemical rocket or a nuclear thermal rocket, is fairly complex in detail but rather simple in principle. Among all the interacting parts, three components stand out: they are pumps and turbines (turbopumps), and the thrust chamber. To obtain an understanding of the overall rocket propulsion system characteristics, one starts from analyzing the interactions among these three components. It is therefore of utmost importance to be able to satisfactorily characterize the turbopump, level by level, at all phases of a vehicle design cycle. Here at NASA Glenn Research Center, as the starting phase of a rocket engine design, specifically a Nuclear Thermal Rocket Engine design, we adopted the approach of using a high level system cycle analysis code (NESS) to obtain an initial analysis of the operational characteristics of a turbopump required in the propulsion system. A set of turbopump design codes (PumpDes and TurbDes) were then executed to obtain sizing and performance characteristics of the turbopump that were consistent with the mission requirements. A set of turbopump analyses codes (PUMPA and TURBA) were applied to obtain the full performance map for each of the turbopump components; a two dimensional layout of the turbopump based on these mean line analyses was also generated. -
Development of Turbopump for LE-9 Engine
Development of Turbopump for LE-9 Engine MIZUNO Tsutomu : P. E. Jp, Manager, Research & Engineering Development, Aero Engine, Space & Defense Business Area OGUCHI Hideo : Manager, Space Development Department, Aero Engine, Space & Defense Business Area NIIYAMA Kazuki : Ph. D., Manager, Space Development Department, Aero Engine, Space & Defense Business Area SHIMIYA Noriyuki : Space Development Department, Aero Engine, Space & Defense Business Area LE-9 is a new cryogenic booster engine with high performance, high reliability, and low cost, which is designed for H3 Rocket. It will be the first booster engine in the world with an expander bleed cycle. In the designing process, the performance requirements of the turbopump and other components can be concurrently evaluated by the mathematical model of the total engine system including evaluation with the simulated performance characteristic model of turbopump. This paper reports the design requirements of the LE-9 turbopump and their latest development status. Liquid oxygen 1. Introduction turbopump Liquid hydrogen The H3 rocket, intended to reduce cost and improve turbopump reliability with respect to the H-II A/B rockets currently in operation, is under development toward the launch of the first H3 test rocket in FY 2020. In rocket development, engine is an important factor determining reliability, cost, and performance, and as a new engine for the H3 rocket first stage, an LE-9 engine(1) is under development. A rocket engine uses a turbopump to raise the pressure of low-pressure propellant supplied from a tank, injects the pressurized propellant through an injector into a combustion chamber to combust it under high-temperature and high- pressure conditions. -
6. Chemical-Nuclear Propulsion MAE 342 2016
2/12/20 Chemical/Nuclear Propulsion Space System Design, MAE 342, Princeton University Robert Stengel • Thermal rockets • Performance parameters • Propellants and propellant storage Copyright 2016 by Robert Stengel. All rights reserved. For educational use only. http://www.princeton.edu/~stengel/MAE342.html 1 1 Chemical (Thermal) Rockets • Liquid/Gas Propellant –Monopropellant • Cold gas • Catalytic decomposition –Bipropellant • Separate oxidizer and fuel • Hypergolic (spontaneous) • Solid Propellant ignition –Mixed oxidizer and fuel • External ignition –External ignition • Storage –Burn to completion – Ambient temperature and pressure • Hybrid Propellant – Cryogenic –Liquid oxidizer, solid fuel – Pressurized tank –Throttlable –Throttlable –Start/stop cycling –Start/stop cycling 2 2 1 2/12/20 Cold Gas Thruster (used with inert gas) Moog Divert/Attitude Thruster and Valve 3 3 Monopropellant Hydrazine Thruster Aerojet Rocketdyne • Catalytic decomposition produces thrust • Reliable • Low performance • Toxic 4 4 2 2/12/20 Bi-Propellant Rocket Motor Thrust / Motor Weight ~ 70:1 5 5 Hypergolic, Storable Liquid- Propellant Thruster Titan 2 • Spontaneous combustion • Reliable • Corrosive, toxic 6 6 3 2/12/20 Pressure-Fed and Turbopump Engine Cycles Pressure-Fed Gas-Generator Rocket Rocket Cycle Cycle, with Nozzle Cooling 7 7 Staged Combustion Engine Cycles Staged Combustion Full-Flow Staged Rocket Cycle Combustion Rocket Cycle 8 8 4 2/12/20 German V-2 Rocket Motor, Fuel Injectors, and Turbopump 9 9 Combustion Chamber Injectors 10 10 5 2/12/20 -
Materials for Liquid Propulsion Systems
https://ntrs.nasa.gov/search.jsp?R=20160008869 2019-08-29T17:47:59+00:00Z CHAPTER 12 Materials for Liquid Propulsion Systems John A. Halchak Consultant, Los Angeles, California James L. Cannon NASA Marshall Space Flight Center, Huntsville, Alabama Corey Brown Aerojet-Rocketdyne, West Palm Beach, Florida 12.1 Introduction Earth to orbit launch vehicles are propelled by rocket engines and motors, both liquid and solid. This chapter will discuss liquid engines. The heart of a launch vehicle is its engine. The remainder of the vehicle (with the notable exceptions of the payload and guidance system) is an aero structure to support the propellant tanks which provide the fuel and oxidizer to feed the engine or engines. The basic principle behind a rocket engine is straightforward. The engine is a means to convert potential thermochemical energy of one or more propellants into exhaust jet kinetic energy. Fuel and oxidizer are burned in a combustion chamber where they create hot gases under high pressure. These hot gases are allowed to expand through a nozzle. The molecules of hot gas are first constricted by the throat of the nozzle (de-Laval nozzle) which forces them to accelerate; then as the nozzle flares outwards, they expand and further accelerate. It is the mass of the combustion gases times their velocity, reacting against the walls of the combustion chamber and nozzle, which produce thrust according to Newton’s third law: for every action there is an equal and opposite reaction. [1] Solid rocket motors are cheaper to manufacture and offer good values for their cost. -
The Modified Fuel Turbopump of 2Nd Stage Engine for H3 Launch Vehicle
DOI: 10.13009/EUCASS2017-189 7TH EUROPEAN CONFERENCE FOR AERONAUTICS AND SPACE SCIENCES (EUCASS) The Modified Fuel Turbopump of 2nd stage engine for H3 launch vehicle Naoki Nagao*, Hideaki Nanri*, Koichi Okita*, Yohei Ishizu**, Shinnosuke Yabuki** and Shinichiro Kohno** *Japan Aerospace Exploration Agency 2-1-1 Sengen, Tsukuba-shi, Ibaraki 305-8505 **IHI Corporation 229 Tonogaya Mizuho-machi, Nishitama-gun, Tokyo 190-1297 Abstract The turbine of fuel turbopump of 2nd stage engine for H3 launch vehicle was changed from a partial admission type to a full admission type to meet the requirement of longer firing duration in a flight. The full admission type had an advantage of increasing the efficiency because of the uniform flow in circumference direction, on the other hand, had a disadvantage of decreasing the efficiency caused with the smaller height of turbine blade. The design of turbine was carefully modified and it was verified with experiments that the turbine had 10% higher performance than the previous design. 1. Introduction The next generation Japanese mainstay launch vehicle; H3 launch vehicle, has been developed since April 2014 to increase the launch capability of domestic launchers and to enhance the international competitiveness based on the “Basic Plan on Space Policy” [1]. As the result of system study on H3 launch vehicle, the second stage engine of H- IIA/B rocket, named LE-5B-2 is modified and adopted to H3 launch vehicle, because the performance of LE-5B-2 almost meets the requirement of the system and the high reliability of LE-5B series has been proved in the long-term operation. -
Nuclear Propulsionfa Historical Perspective Stanley Gunn*,1 P.O
Space Policy 17 (2001) 291–298 Nuclear propulsionFa historical perspective Stanley Gunn*,1 P.O. Box 808, Moorpark, CA 93020-0808, USA Abstract Those who fear development of nuclear propulsion for space travel forget that considerable work on it has already been done, starting in the 1950s, and that the concept of a nuclear rocket was safely and successfully tested in the 1960s. This article describes the history of the US Nuclear Engine for Rocket Vehicle Application programme, with technical details of its development. Although funding for the programme ceased in the 1970s, there is no reason to suppose that the concept would not work today. r 2001 Published by Elsevier Science Ltd. Nuclear propulsion, at least in the lay community, has times was nothing short of watershed research, far- long been a misunderstood technology. More accu- ranging in concept and highly directed in terms of rately, it has been an unknown technology, existing in application. In viewof its potential for the future Ffor the shadowof over four decades of highly successful example in a piloted Mars missionFit is worth chemical propulsion techniques. Yet the truth of the examining this pioneering work in detail. matter is that nuclear propulsion is a viable option that could represent our best chance to put humans in motion towards distant planets in the first decades of the 21st century. Nuclear propulsion is inherently more 1. Nuclear vs. chemical propulsion efficient than chemical methods by a factor of at least two, is significantly simpler in overall concept and could All liquid rocket propulsion systems rely on the be applicable with contemporary vehicles. -
Preparation of Papers for AIAA Journals
https://ntrs.nasa.gov/search.jsp?R=20180006338 2019-08-31T18:40:27+00:00Z View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by NASA Technical Reports Server Overview of RS-25 Adaptation Hot-Fire Test Series for SLS, Status and Lessons Learned Naveen Vetcha,1 Matthew B. Strickland,2 Kenneth D. Philippart,3 and Thomas V. Giel Jr.4 Jacobs Space Exploration Group/ESSCA/NASA Marshall Space Flight Center, Huntsville, AL, 35812 USA This paper discusses the engine system design, hot-fire test history and analyses for the RS-25 Adaptation Engine test series, a major hot-fire test series supporting the Space Launch System (SLS) program. The RS-25 is an evolution of the Space Shuttle Main Engine (SSME). Since the SLS mission profile and engine operating conditions differ from that experienced by the SSME, a test program was needed to verify that SLS-unique requirements could be met by the adapted legacy engines. A series of 18 tests, including one engine acceptance test, was conducted from January 2015 to October 2017, to directly support Exploration Mission-1 (EM-1), the first flight of SLS. These tests were the first hot-firings of legacy SSME hardware since 2009. Major findings are described along with top level overview of the engine system. I. Introduction On October 11, 2010 President Barack Obama signed into law the National Aeronautics and Space Administration (NASA) authorization act of 2010. The law directed NASA to “develop a heavy lift launch vehicle as a follow on to the Space Shuttle that can -
RS-25: the Clark Kent of Engines for the Space Launch System
RS-25: The Clark Kent of Engines for the Space Launch System September 13, 2013; updated July 30, 2015 In the iconic comic-book series, “Superman,” the main character, Clark Kent, looks like your average Joe. Under the ruse of a three-piece suit and glasses, Kent’s true identity is “Superman,” who transforms into his mighty persona to do battle for the good of humankind. In the rocket engine world, the RS-25 is Clark Kent. Four RS-25 engines will power the core stage of NASA's Space Launch System (SLS)—NASA’s new heavy-lift launch vehicle. Towering more than 200 feet tall with a diameter of 27.6 feet, the core stage stores cryogenic liquid hydrogen and liquid oxygen that feeds the vehicle’s RS-25 engines. SLS will be the most powerful rocket in the world with the greatest capacity of any launch system ever built to support any destination, any payload and any mission, including NASA’s plans to send humans to a captured and relocated asteroid. The 70-metric-ton (77-ton) configuration will stand at 321 feet, which is taller than the Statue of Liberty. The RS-25, also known as the space shuttle main engine, is the first reusable rocket engine in history. Four RS-25 engines, like the one pictured above “During the 30-year run of the Space Shuttle Program, the undergoing a hot-fire test, power the core stage of NASA's Space Launch System (SLS)—NASA's heavy- RS-25 achieved very high demonstrated reliability,” said lift launch vehicle. -
Modular Impulsive Green Monopropellant Propulsion System (MIMPS-G): for Cubesats in LEO and to the Moon
aerospace Article Modular Impulsive Green Monopropellant Propulsion System (MIMPS-G): For CubeSats in LEO and to the Moon Ahmed E. S. Nosseir 1,2,* , Angelo Cervone 1,* and Angelo Pasini 2,* 1 Department of Space Engineering, Faculty of Aerospace Engineering, Delft University of Technology (TU Delft), 2629 Delft, The Netherlands 2 Sede di Ingegneria Aerospaziale, Dipt. di Ingegneria Civile e Industriale, Università di Pisa (UniPi), 56122 Pisa, Italy * Correspondence: [email protected] or [email protected] (A.E.S.N.); [email protected] (A.C.); [email protected] (A.P.) Abstract: Green propellants are currently considered as enabling technology that is revolutioniz- ing the development of high-performance space propulsion, especially for small-sized spacecraft. Modern space missions, either in LEO or interplanetary, require relatively high-thrust and impulsive capabilities to provide better control on the spacecraft, and to overcome the growing challenges, particularly related to overcrowded LEOs, and to modern space application orbital maneuver require- ments. Green monopropellants are gaining momentum in the design and development of small and modular liquid propulsion systems, especially for CubeSats, due to their favorable thermophysical properties and relatively high performance when compared to gaseous propellants, and perhaps simpler management when compared to bipropellants. Accordingly, a novel high-thrust modular impulsive green monopropellant propulsion system with a micro electric pump feed cycle is pro- posed. MIMPS-G500mN is designed to be capable of delivering 0.5 N thrust and offers theoretical total impulse I from 850 to 1350 N s per 1U and >3000 N s per 2U depending on the burnt mono- Citation: Nosseir, A.E.S.; Cervone, tot A.; Pasini, A. -
Space Shuttle Main Engine Orientation
BC98-04 Space Transportation System Training Data Space Shuttle Main Engine Orientation June 1998 Use this data for training purposes only Rocketdyne Propulsion & Power BOEING PROPRIETARY FORWARD This manual is the supporting handout material to a lecture presentation on the Space Shuttle Main Engine called the Abbreviated SSME Orientation Course. This course is a technically oriented discussion of the SSME, designed for personnel at any level who support SSME activities directly or indirectly. This manual is updated and improved as necessary by Betty McLaughlin. To request copies, or obtain information on classes, call Lori Circle at Rocketdyne (818) 586-2213 BOEING PROPRIETARY 1684-1a.ppt i BOEING PROPRIETARY TABLE OF CONTENT Acronyms and Abbreviations............................. v Low-Pressure Fuel Turbopump............................ 56 Shuttle Propulsion System................................. 2 HPOTP Pump Section............................................ 60 SSME Introduction............................................... 4 HPOTP Turbine Section......................................... 62 SSME Highlights................................................... 6 HPOTP Shaft Seals................................................. 64 Gimbal Bearing.................................................... 10 HPFTP Pump Section............................................ 68 Flexible Joints...................................................... 14 HPFTP Turbine Section......................................... 70 Powerhead........................................................... -
Low Cost Catalysts for Hydrazine Monopropellant Thrusters
See discussions, stats, and author profiles for this publication at: https://www.researchgate.net/publication/268483024 Low Cost Catalysts for Hydrazine Monopropellant Thrusters Conference Paper · August 2009 DOI: 10.2514/6.2009-5232 CITATIONS READS 2 53 5 authors, including: Jose Nivaldo Hinckel National Institute for Space Research, Brazil 27 PUBLICATIONS 50 CITATIONS SEE PROFILE All content following this page was uploaded by Jose Nivaldo Hinckel on 27 June 2018. The user has requested enhancement of the downloaded file. Low Cost Catalysts for Hydrazine Monopropellant Thrusters Jos´eNivaldo Hinckel∗ INPE/DMC, S˜aoJos´edos Campos, SP, 12201-970, Brazil Jos´eA. R. Jorge†Tur´ıbioG. Soares Neto†Marisa A. Zacharias†Jalusa A. L. Palandi‡ INPE/LCP, Cachoeira Paulista, SP, 12630-000, Brazil Hydrazine monopropellant engines are widely used in space missions; mainly in reaction control systems. The most widely used catalyst is the aluminum oxide supported iridium. It is also very expensive. The cost of the catalyst weights heavily, especially in the high thrust, short life thrusters used for roll control of launch vehicles. In this paper we present the results of testing of low cost catalysts in a 35 newton thruster. The catalysts tested were aluminum oxide supported ruthenium and a homogeneous catalyst, tungsten carbide. The test sequence included pre-heated and cold starts, pulsed and continuous firing modes, a range of feed pressure and life cycle that exceed the requirements of roll control systems. The start and energetic performance of the thruster matched very closely the performance of the iridium catalyst. Nomenclature ∗ C [m/s] Characteristic Velocity Pc [MPa] Chamber Pressure Cf Thrust Coefficient tig [ms] Ignition time F [N] Thrust tresp [ms] Response time ◦ Isp [m/s] Specific Impulse Tin [ C] Initial Temperature Pi [MPa] Injection Pressure I.