Spacecraft Subsystems Part 4 ‒ Fundamentals of Propulsion
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On-Orbit Propulsion System Performance of ISS Visiting Vehicles
On-Orbit Propulsion System Performance of ISS Visiting Vehicles Mary Regina M. Martin*, Robert A. Swanson†, and Ulhas P. Kamath‡ The Boeing Company, Houston, TX 77059 and Francisco J. Hernandez§ and Victor Spencer** NASA Lyndon B. Johnson Space Center, Houston, TX 77058 The International Space Station (ISS) represents the culmination of over two decades of unprecedented global human endeavors to conceive, design, build and operate a research laboratory in space. Uninterrupted human presence in space since the inception of the ISS has been made possible by an international fleet of space vehicles facilitating crew rotation, delivery of science experiments and replenishment of propellants and supplies. On-orbit propulsion systems on both ISS and Visiting Vehicles are essential to the continuous operation of the ISS. This paper compares the ISS visiting vehicle propulsion systems by providing an overview of key design drivers, operational considerations and performance characteristics. Despite their differences in design, functionality, and purpose, all visiting vehicles must adhere to a common set of interface requirements along with safety and operational requirements. This paper addresses a wide variety of methods for satisfying these requirements and mitigating credible hazards anticipated during the on-orbit life of propulsion systems, as well as the seamless integration necessary for the continued operation of the ISS. Nomenclature ΔT = change in temperature in °C ΔV = change in velocity in m/s F = thrust in kgf (1 kgf = 9.807 N) Isp = specific impulse in seconds K1 = constant derived from the acceptance test data for each type of thruster K2 = constant derived from the acceptance test data for each type of thruster m = mass of propellant consumed in kg 2 Pavg = average pressure of all tanks feeding a thruster in kg/cm Ton = total on-time in seconds I. -
Spacecraft Propulsion
SPACECRAFT PROPULSION WITH THRUST AND PRECISION INTO SPACE SPACECRAFT PROPULSION THRUST AND PRECISION INTO SPACE ArianeGroup is a market leader in spacecraft propulsion systems and equipment. Since over 50 years, customers worldwide benefit from a competitive portfolio of high quality products and services. We cover the complete range of products and services related to orbital propulsion, from chemical monopropellant systems for smaller satellites to chemical bipropellant systems for larger platforms and completed with the electric propulsion portfolio based on the RIT technology. At ArianeGroup, customers have a single point of contact for the complete propulsion system at all phases of the value chain. From system design up to after-launch services. All key equipment of ArianeGroup propulsion systems (thrusters, propellant tanks and fluidic equipment) are produced in-house. 2 ALL ABOUT PRECISION With our orbital propulsion thrusters and engines our customers can be ensured that their mission requirements related to propulsion will be fulfilled with accurate precision. Our biggest orbital propulsion thruster, the 400N apogee engine, has placed hundreds of satellites in its final orbit With micro precision the RIT µX thruster brings space missions to the exact orbit 2 3 SPACECRAFT PROPULSION ELECTRIC PROPULSION Radio frequency ion propulsion for orbit raising, station keeping and deep space missions ArianeGroup’s electric space propulsion expertise is based on the space proven Radio Frequency Ion Technology (RIT). Within this field, we produce complete propulsion systems, modules, thrusters and related components. This technology features numerous advantages like high specific impulse therefore maximum propellant saving. Low system complexity is another strength of the RIT Technology. -
Chap21 Rockets Fundamentals.Pdf
Chapter 21.indd 449 1/9/08 12:12:24 PM There is an explanation for everything that a rocket does. The explanation is most always based on the laws of physics and the nature of rocket propellants. Experimentation is required to find out whether a new rocket will or will not work. Even today, with all the knowledge and expertise that exists in the field of rocketry, experimentation occasionally shows that certain ideas are not practical. In this chapter, we will look back in time to the early developers and users of rocketry. We will review some of the physical laws that apply to rocketry, discuss selected chemicals and their combinations, and identify the rocket systems and their components. We also will look at the basics of rocket propellant efficiency. bjectives Explain why a rocket engine is called a reaction engine. Identify the country that first used the rocket as a weapon. Compare the rocketry advancements made by Eichstadt, Congreve and Hale. Name the scientist who solved theoretically the means by which a rocket could escape the earth’s gravitational field. Describe the primary innovation in rocketry developed by Dr. Goddard and Dr. Oberth. Explain the difference between gravitation and gravity. Describe the contributions of Galileo and Newton. Explain Newton’s law of universal gravitation. State Newton’s three laws of motion. Define force, velocity, acceleration and momentum. Apply Newton’s three laws of motion to rocketry. Identify two ways to increase the thrust of a rocket. State the function of the combustion chamber, the throat, and nozzle in a rocket engine. -
Turbojet Runs Precursor to Hypersonic Engine Heat Exchanger Tests
Turbojet Runs Precursor to Hypersonic Engine Heat Exchanger Tests Aviation Week & Space Technology Guy Norris Tue, 2018-05-15 04:00 Advanced propulsion developer Reaction Engines is nearing its first step toward validating its novel air-breathing hybrid rocket design at hypersonic conditions by firing up a vintage General Electric J79 turbojet to act as a heat source for testing, expected later this month. The ex-military engine, formerly used in a McDonnell Douglas F-4, is a central element of Reaction’s specially developed high-temperature airflow test site, which will soon be commissioned at Front Range Airport, near Watkins, Colorado. The J79 will provide heated gas flow in excess of 1,000C (1,800F) which, together with conditioned ambient air, will be mixed to replicate inlet conditions representative of flight speeds up to and including Mach 5. The flow will verify the operability and performance of the pre-cooler heat exchanger (HTX), which is at the core of Reaction’s Sabre (synergistic air-breathing rocket engine). It is also key to extracting oxygen from the atmosphere to enable acceleration to hypersonic speed from a standing start. The HTX will chill airflow to minus 150C in less than 1/20th of a second, and pass it through a turbo- compressor and into the rocket combustion chamber where it will be burned with sub-cooled liquid hydrogen (LH) fuel. Beyond Mach 5, and at an altitude approaching 100,000 ft. the inlet will be closed and the engine will continue to operate as a closed-cycle rocket engine fueled by onboard liquid oxygen and LH. -
Specifics of Small Satellite Propulsion: Part 1
SSC01-XI-6 Specifics of Small Satellite Propulsion: Part 1 Vadim Zakirov and Martin Sweeting Surrey Space Centre University of Surrey Guildford, Surrey GU2 7XH, United Kingdom fax: +44 1483 879503 tel: +44 1483 879817 e-mail: [email protected] Peter Erichsen Space Systems Division Swedish Space Corporation P.O.Box 4207, Strandvägen 86, SE-171 04 Solna, Sweden fax: +46 8 98 70 69 tel: +46 8 627 6313 e-mail: [email protected] Timothy Lawrence European Office of Aerospace Research and Development 223/231 Old Marylebone Rd., London, NW1 5TH, United Kingdom fax: +44 2075 144960 tel: +44 2075 144285 e-mail: [email protected] Abstract. Small satellite propulsion is a subject of unique constraints and requirements. Based on University of Surrey experience in small satellite building and operation, these features are listed and explained. Available volume is often identified as the most severe constraint for a small satellite with power and cost being the other two major constraints. Mass is often only of secondary importance for small satellites. Propulsion dry mass fraction for a spacecraft grows upon the system scaling-down. For small spacecraft propulsion fraction can easily exceed 85%. In such a case, a combination of independent systems for multi- functional propulsion mission scenarios would aggravate the situation. Moreover, specific impulse is not a factor reflecting small satellite propulsion system performance since spacecraft velocity change is also a function of propulsion dry mass fraction. New conceptual and design solutions are suggested for small satellite propulsion with respect to its specific constraints and requirements. -
Space Propulsion Technology for Small Spacecraft
Space Propulsion Technology for Small Spacecraft The MIT Faculty has made this article openly available. Please share how this access benefits you. Your story matters. Citation Krejci, David, and Paulo Lozano. “Space Propulsion Technology for Small Spacecraft.” Proceedings of the IEEE, vol. 106, no. 3, Mar. 2018, pp. 362–78. As Published http://dx.doi.org/10.1109/JPROC.2017.2778747 Publisher Institute of Electrical and Electronics Engineers (IEEE) Version Author's final manuscript Citable link http://hdl.handle.net/1721.1/114401 Terms of Use Creative Commons Attribution-Noncommercial-Share Alike Detailed Terms http://creativecommons.org/licenses/by-nc-sa/4.0/ PROCC. OF THE IEEE, VOL. 106, NO. 3, MARCH 2018 362 Space Propulsion Technology for Small Spacecraft David Krejci and Paulo Lozano Abstract—As small satellites become more popular and capa- While designations for different satellite classes have been ble, strategies to provide in-space propulsion increase in impor- somehow ambiguous, a system mass based characterization tance. Applications range from orbital changes and maintenance, approach will be used in this work, in which the term ’Small attitude control and desaturation of reaction wheels to drag com- satellites’ will refer to satellites with total masses below pensation and de-orbit at spacecraft end-of-life. Space propulsion 500kg, with ’Nanosatellites’ for systems ranging from 1- can be enabled by chemical or electric means, each having 10kg, ’Picosatellites’ with masses between 0.1-1kg and ’Fem- different performance and scalability properties. The purpose tosatellites’ for spacecrafts below 0.1kg. In this category, the of this review is to describe the working principles of space popular Cubesat standard [13] will therefore be characterized propulsion technologies proposed so far for small spacecraft. -
Propulsion Systems Design and Integration Engineering Solutions for Space Science and Exploration
National Aeronautics and Space Administration Marshall Space Flight Center Propulsion Systems Design and Integration Engineering Solutions for Space Science and Exploration Engine Systems Main Propulsion Systems Spacecraft Propulsion Systems Advanced Propulsion The Propulsion Systems Design & Integration Division (ER20) provides technology development, system design, expert technical evaluation, and systems integration to advance the next generation of space transportation systems and assure continued safe operation of existing systems. ER20 responds directly to customers requiring system level technology and concept evaluation, analysis, and maturation, detailed system development and propulsion component integration, test verification planning, evaluation, and certifi- cation. The division also provides sustaining engineering for operations support for space transportation propulsion systems. ER20 provides engineering expertise for all transportation mission phases including boost, upper stage, in-space, and extraterrestrial descent/ascent applications. ER20 expertise includes liquid propulsion systems including cryogenics and storable propellants supporting a wide range of propulsion systems. Liquid systems expertise ranges from low thrust pres- sure fed in-space propulsion systems to high thrust, pump fed booster propulsion systems. In addition, this division supports non-chemical and nuclear propulsion and power systems, such as plasma systems and nuclear electric and thermal systems. Facilities available to the division include -
Liquid Propollant Rocket Engines
THERMAL TO MECHANICAL ENERGY CONVERSION: ENGINES AND REQUIREMENTS – Vol. II - Liquid Propellant Rocket Engines - V.M. Polyaev and V.A. Burkaltsev LIQUID PROPELLANT ROCKET ENGINES V.M. Polyaev and V.A. Burkaltsev Department of Rocket engines, Bauman Moscow State Technical University, Russia. Keywords: Liquid rocket engine, liquid rocket propellant, chamber, combustion products, pressure, temperature, density, cooling, supply system, turbopump assembly, gas generator, engine installation, thrust, specific impulse, specific mass. Contents 1. Introduction 2. LRE general information 3. Main LRE parameters 4. LRE structure and liquid rocket engine installations (LREI) schemes 5. Historical reference 6. LRE development tendencies 7. Conclusions Acknowledgment Glossary Bibliography Biographical Sketches 1. Introduction All chemical rocket engines have two common characteristics. They utilize chemical reactions in a thrust chamber to produce a high-pressure, high-temperature gas at the entrance to a converging-diverging exhaust nozzle. The hot propellant gas expands in flowing through the nozzle, and the expansion process converts a portion of the thermal energy released by the chemical reaction into kinetic energy associated with a high- velocity gaseous-exhaust jet. 2. LRE general information The liquid propellant rocket engine (LRE) is a direct reaction engine using the liquid rocket propellantUNESCO stored on a flight vehicle – board EOLSS for thrust creation. The liquid rocket propellant (LRP) is a substance in the liquid state which is capable to be converted intoSAMPLE a reactive gas jet discharging CHAPTERS from the engine and creating a thrust as a result of the exothermal reaction associated with heat release. LRP consists of liquid components. The propellant components can include one substance or a mixture of individual chemical substances. -
Aviation Fuels Technical Review
Aviation Fuels Technical Review | Chevron Products Aviation Fuels Company Technical Review Chevron Products Company 6001 Bollinger Canyon Road San Ramon, CA 94583 Chevron Products Company is a division of a wholly owned subsidiary of Chevron Corporation. http://www.chevron.com/productsservices/aviation/ © 2007 Chevron U.S.A. Inc. All rights reserved. Chevron and the Caltex, Chevron and Texaco hallmarks are federally registered trademarks of Chevron Intellectual Property LLC. Recycled/RecyclableRecycled/recyclable paper paper IDC 1114-099612 MS-9891 (11/14) Table of Contents Notes General Introduction ............................................................i 8 • Aviation Gasoline Performance ............................ 45 Performance Properties 1 • Aviation Turbine Fuel Introduction ........................... 1 Cleanliness Types of Fuel Safety Properties Fuel Consumption 9 • Aviation Gasoline 2 • Aviation Turbine Fuel Performance .........................3 Specifications and Test Methods .......................... 54 Performance Properties Specifications Cleanliness Future Fuels Safety Properties Test Methods Emissions 10 • Aviation Gasoline Composition ............................. 63 3 • Aviation Turbine Fuel Composition Specifications and Test Method ...............................14 Property/Composition Relationships Specifications Additives Test Methods 11 • Aviation Gasoline Refining ..................................... 66 4 • Aviation Turbine Fuel Composition ........................24 Alkylation Base Fuel Avgas Blending -
A Comparison of GEO Satellites Using Chemical and Electric Propulsion
A Comparison of GEO Satellites Using Chemical and Electric Propulsion David Thomas1 University of Colorado, Boulder, CO, 80309 May 4, 2016 A telecommunication satellite in a geostationary orbit requires a significant amount of propellant for station-keeping maneuvers, in addition to the propellant needed for transfer from GTO to the geostationary orbit. The propellant mass significantly increases the launch mass of the spacecraft, requiring a larger launch vehicle and increasing the cost of launch. However, low-thrust electric propulsion can lower the necessary propellant mass and reduce the launch cost. This paper seeks to explore the mass savings of electric propulsion through simple numerical simulations. Analysis indicates that the launch mass of an electric satellite is only 45% of that for a satellite with conventional, chemical propulsion. Nomenclature A = cross-sectional area (m2) AU = astronomical unit a = acceleration (m/s2) a = semi-major axis (km) CR = coefficient of reflectivity c = speed of light (299,792,458 m/s) ECEF = Earth-centered, Earth-fixed (coordinate frame) ECI = Earth-centered, inertial (coordinate frame) F = thrust (N) GEO = geostationary orbit GTO = geostationary transfer orbit 2 g0 = standard gravitational acceleration (9.81 m/s ) J2, J3 = Earth gravitational field parameters Isp = specific impulse (s) i = inclination (°) K = control gain LEO = low Earth orbit MMH = monomethylhydrazine MON = mixed oxides of nitrogen mi = initial mass (kg) mf = final mass (kg) R0 = one astronomical unit (149,597,870.7 km) RE = Earth radius (6,378.1363 km) r = position vector (km) SRP = solar radiation pressure r = orbital radius (km) t = time (s) V = speed (km/s) XIPS = xenon ion propulsion system 1 Aerospace Engineering Sciences, University of Colorado, Boulder, CO 80309. -
19820018505.Pdf
NASA CR 167885 NASA-CR-167885 19820018505 '." ....... _, 1.:.,. NI\S/\ - .. '.' 1 CHARACTERIZATION OF ADVANCED ELECTRIC PROPULSION SYSTEMS PREPARED FOR LEWIS RESEARCH CENTER NATIONAL AERONAUTICS AND SPACE ADMINISTRATION GRANT NAG 3-76 '" 1982 L':::""o' ," r;'S,;.R::~ CENTER Final Report I ;:"~~ I (.';1, VIRGINIA May 1982 Pradosh K. Ray Department of Mechanical Engineering Tuskegee Institute Tuskegee Institute, Alabama 1111111111111 1111 11111 1111111111 11111 1111 1111 NF02692 1. Report No. I 2. Government AcclISsion No. 3. Recipient's Catalog No. NASA CR 167885 4. Title and Subtitle 5. Report Date Characterization of Advanced Electric May, 1982 Propulsion Systems 6. Performing Organization Code 7.. Author(s) 8. Performing Organization Report No. Pradosh K. Ray 10. Work Unit No. 9. Performing Organization Nlme and Addr... Department of Mechanical Engineering 11. Contract or Grant No. Tuskegee Institute Tuskegee Institute, Alabama 36088 NAG 3-76 13. Type of Report and Period Covered 12. Sponsoring AgencV Name and Addresl June 1, 1980-January 31, 198;: National Aeronautics and Space Administration Washington, D.C. 20546 14. Sponsoring Agency Code 15. Supplementary Notes Grant Monitor--William Kerslake, NASA Lewis Research Center Cleveland, Ohio 44135 16. Abstract Characteristics of several advanced electric propulsion systems are evaluated and compared. The propulsion systems studied are mass driver, rail gun, MPD thruster, hydrogen free radical thruster and mercury electron bombardment ion engine. These are characterized by specific impulse, overall effiCiency, input power, average thrust, power to average thrust ratio and average thrust to dry weight ratio. Several important physical characteristics such as dry system mass, accelerator length, bore size and current pulse requirement are also evaluated in appropriate cases. -
Nasa Tm X-52391 Memorandum
. NASA TECHNICAL NASA TM X-52391 MEMORANDUM I GPO PRICE $ CSFTl PRlCE(S) $ Hard copy (HC) .- Microfiche (MF) - ff 653 July 65 EXPLORING IN AEROSPACE ROCKETRY 4. THERMODYNAMICS by Marshall C. Burrows Lewis Research Center Cleveland, Ohio Presented to Lewis Aerospace Explorers Cleveland, Ohio 1966 -67 N NATIONAL AERONAUTICS AND SPACE ADMINISTRATION WASHINGTON, D.C. 1968 EXPLORING IN AEROSPACE ROCKETRY 4. THERMODYNAMICS Marshall C. Burrows Presented to Lewis Aerospace Explorers Cleveland, Ohio 1966 -67 Advisor, James F. Connors NATIONAL AERONAUTICS AND SPACE ADMINISTRATION NASA Technical Chapter Memorandum 1 AEROSPACE ENVIRONMENT John C. Evvard ........................... X-52388 2 PROPULSION FUNDAMENTALS James F. Connors .......................... X-52389 3 CALCULATION OF ROCKET VERTICAL-FLIGHT PERFORMANCE John C. Evvard ............................ X-52390 4 THERMODYNAMICS I Marshall C. Burrows ........................ X-52391 5 MATERIALS William D. Klopp ........................... X - 523 92 6 SOLID-PROPELLANT ROCKET SYSTEMS Joseph F. McBride .......................... X-52393 7 LIQUID-PROPELLANT ROCKET SYSTEMS E. William Conrad .......................... X-52394 8 ZERO - GRAVITY EFFECTS William J. Masica .......................... X-52395 9 ROCKET TRAJECTORIES, DRAG, AND STABILITY Roger W. Luidens .......................... X-52396 10 SPACE MISSIONS Richard J. Weber. .......................... X - 52397 11 LAUNCH VEHICLES Arthur V. Zimmerman ........................ X-52398 12 INERTIAL GUIDANCE SYSTEMS Daniel J. Shramo ..........................