Revolutionary Propulsion Concepts for Small Satellites
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Electric Propulsion System Scaling for Asteroid Capture-And-Return Missions
Electric propulsion system scaling for asteroid capture-and-return missions Justin M. Little⇤ and Edgar Y. Choueiri† Electric Propulsion and Plasma Dynamics Laboratory, Princeton University, Princeton, NJ, 08544 The requirements for an electric propulsion system needed to maximize the return mass of asteroid capture-and-return (ACR) missions are investigated in detail. An analytical model is presented for the mission time and mass balance of an ACR mission based on the propellant requirements of each mission phase. Edelbaum’s approximation is used for the Earth-escape phase. The asteroid rendezvous and return phases of the mission are modeled as a low-thrust optimal control problem with a lunar assist. The numerical solution to this problem is used to derive scaling laws for the propellant requirements based on the maneuver time, asteroid orbit, and propulsion system parameters. Constraining the rendezvous and return phases by the synodic period of the target asteroid, a semi- empirical equation is obtained for the optimum specific impulse and power supply. It was found analytically that the optimum power supply is one such that the mass of the propulsion system and power supply are approximately equal to the total mass of propellant used during the entire mission. Finally, it is shown that ACR missions, in general, are optimized using propulsion systems capable of processing 100 kW – 1 MW of power with specific impulses in the range 5,000 – 10,000 s, and have the potential to return asteroids on the order of 103 104 tons. − Nomenclature -
Orbital Fueling Architectures Leveraging Commercial Launch Vehicles for More Affordable Human Exploration
ORBITAL FUELING ARCHITECTURES LEVERAGING COMMERCIAL LAUNCH VEHICLES FOR MORE AFFORDABLE HUMAN EXPLORATION by DANIEL J TIFFIN Submitted in partial fulfillment of the requirements for the degree of: Master of Science Department of Mechanical and Aerospace Engineering CASE WESTERN RESERVE UNIVERSITY January, 2020 CASE WESTERN RESERVE UNIVERSITY SCHOOL OF GRADUATE STUDIES We hereby approve the thesis of DANIEL JOSEPH TIFFIN Candidate for the degree of Master of Science*. Committee Chair Paul Barnhart, PhD Committee Member Sunniva Collins, PhD Committee Member Yasuhiro Kamotani, PhD Date of Defense 21 November, 2019 *We also certify that written approval has been obtained for any proprietary material contained therein. 2 Table of Contents List of Tables................................................................................................................... 5 List of Figures ................................................................................................................. 6 List of Abbreviations ....................................................................................................... 8 1. Introduction and Background.................................................................................. 14 1.1 Human Exploration Campaigns ....................................................................... 21 1.1.1. Previous Mars Architectures ..................................................................... 21 1.1.2. Latest Mars Architecture ......................................................................... -
Conceptual Design and Optimization of Hybrid Rockets
University of Calgary PRISM: University of Calgary's Digital Repository Graduate Studies The Vault: Electronic Theses and Dissertations 2021-01-14 Conceptual Design and Optimization of Hybrid Rockets Messinger, Troy Leonard Messinger, T. L. (2021). Conceptual Design and Optimization of Hybrid Rockets (Unpublished master's thesis). University of Calgary, Calgary, AB. http://hdl.handle.net/1880/113011 master thesis University of Calgary graduate students retain copyright ownership and moral rights for their thesis. You may use this material in any way that is permitted by the Copyright Act or through licensing that has been assigned to the document. For uses that are not allowable under copyright legislation or licensing, you are required to seek permission. Downloaded from PRISM: https://prism.ucalgary.ca UNIVERSITY OF CALGARY Conceptual Design and Optimization of Hybrid Rockets by Troy Leonard Messinger A THESIS SUBMITTED TO THE FACULTY OF GRADUATE STUDIES IN PARTIAL FULFILLMENT OF THE REQUIREMENTS FOR THE DEGREE OF MASTER OF SCIENCE GRADUATE PROGRAM IN MECHANICAL ENGINEERING CALGARY, ALBERTA JANUARY, 2021 © Troy Leonard Messinger 2021 Abstract A framework was developed to perform conceptual multi-disciplinary design parametric and optimization studies of single-stage sub-orbital flight vehicles, and two-stage-to-orbit flight vehicles, that employ hybrid rocket engines as the principal means of propulsion. The framework was written in the Python programming language and incorporates many sub- disciplines to generate vehicle designs, model the relevant physics, and analyze flight perfor- mance. The relative performance (payload fraction capability) of different vehicle masses and feed system/propellant configurations was found. The major findings include conceptually viable pressure-fed and electric pump-fed two-stage-to-orbit configurations taking advan- tage of relatively low combustion pressures in increasing overall performance. -
19940015753.Pdf
National Aeronautics and Educational Product Space Administration Teachers I Grades 2-6 I Office of Education and Human Resources Education Division _o N N cO 0 u_ 0 N t_ I ,.-, CO ,4" U O" 0_ _ Z _ 0 0 tM < u Is LIJ I-. _-.q4" W_ O ul ,,_ W;Z. INWel I I,,-. UJ .... 0,. i,-,{ .... u4 uJ I-,- .. IU_ Z_ .1 i ! I i I j | ] ROCKETS Physical Science Teacher's Guide with Activities National Aeronautics and Space Administration Office of Human Resources and Education Education Division This publication is in the Public Domain and is not protected by copyright. Permission is not required for duplication. EP-291 July 1993 Acknowledgments This publication was developed for the National Aeronautics and Space Administra- tion with the assistance of the many educa- tors of the Aerospace Education Services Program, Oklahoma State University. Writer: Gregory L. Vogt, Ed.D. Teaching From Space Program NASA Johnson Space Center Houston, TX Editor: Carla R. Rosenberg Teaching From Space Program NASA Headquarters Washington, DC Table of Contents How To Use This Guide ............................... 1 Activities and Demonstration Matrix ............. 2 Brief History of Rockets ................................ 3 Rocket Principles ......................................... 8 Practical Rocketry ...................................... 12 Activities and Demonstrations .................... 19 Glossary ..................................................... 40 NASA Educational Materials And Suggested Readings .......................... 41 NASA Educational Resources ................... 42 Evaluation Card ..................................... Insert ii How To Use This Guide vehiclesockets arein theexistence.oldest formEarlyofrocketsself-containedwere in use more than two thousand years ago. Over a long and exciting history, rockets have evolved from simple tubes filled with black powder into mighty vehicles capable of launching a spacecraft out into the galaxy. -
Performance Modelling and Simulation of a 100 Km Hybrid Sounding Rocket
PERFORMANCE MODELLING AND SIMULATION OF A 100 KM HYBRID SOUNDING ROCKET Fiona Kay Leverone Submitted in fulfilment of the academic requirements for the degree of Master of Science in Mechanical Engineering, College of Agriculture, Engineering and Science, University of KwaZulu-Natal Supervisor: Mr Michael Brooks Co-Supervisor: Mr Jean-François Pitot de la Beaujardiere Co-Supervisor: Prof Lance Roberts December 2013 2. DECLARATION 1 - PLAGIARISM I, Fiona Leverone, declare that 1. The research reported in this thesis, except where otherwise indicated, is my original research. 2. This thesis has not been submitted for any degree or examination at any other university. 3. This thesis does not contain other persons’ data, pictures, graphs or other information, unless specifically acknowledged as being sourced from other persons. 4. This thesis does not contain other persons’ writing, unless specifically acknowledged as being sourced from other researchers. Where other written sources have been quoted, then: a. Their words have been re-written but the general information attributed to them has been referenced b. Where their exact words have been used, then their writing has been placed inside quotation marks, and referenced. 5. This thesis does not contain text, graphics or tables copied and pasted from the Internet, unless specifically acknowledged, and the source being detailed in the thesis and in the References sections. Signed ________________________ Date ___________ Miss Fiona Leverone As the candidate’s supervisor I have approved this dissertation for submission. Signed ________________________ Date ___________ Mr. Michael Brooks As the candidates co-supervisor I have approved this dissertation for submission. Signed ________________________ Date ___________ Mr. -
NEP Paper World Space Congress
IAC-02-S.4.02 PERFORMANCE REQUIREMENTS FOR A NUCLEAR ELECTRIC PROPULSION SYSTEM Larry Kos In-Space Technical Lead Engineer NASA Marshall Space Flight Center MSFC, Alabama, 35812 (USA) E-mail: [email protected] Les Johnson In-Space Transportation Technology Manager Advanced Space Transportation Program/TD15 NASA Marshall Space Flight Center MSFC, Alabama, 35812, (USA) E-mail: [email protected] Jonathan Jones Aerospace Engineer NASA Marshall Space Flight Center MSFC, Alabama, 35812 (USA) E-mail: [email protected] Ann Trausch Mission and System Analysis Lead NASA Marshall Space Flight Center MSFC, Alabama 35812 (USA) E-mail: [email protected] Bill Eberle Aerospace Engineer Gray Research Inc. Huntsville, Alabama 35806 (USA) E-mail: [email protected] Gordon Woodcock Technical Consultant Gray Research Inc. Huntsville, Alabama 35806 (USA) E-mail: [email protected] NASA is developing propulsion technologies potentially leading to the implementation of a nuclear electric propulsion system supporting robotic exploration of the solar system. The mission limitations imposed by the use of today’s predominantly chemical propulsion systems are many: long trip times, minimal science payload mass, minimal power at the destination for science, and the near-impossibility of encountering multiple targets or even orbiting distant destinations. Performance-based mission analysis, comparing a first generation nuclear electric propulsion system with chemical and solar electric propulsion was performed and will be described in the paper. Mission Characteristics and Challenges ________________ Copyright © 2002 by the American Institute of Aeronautics and Europa Lander Astronautics, Inc. No copyright is asserted in the United States under Title 17, U.S. -
19760011102.Pdf
XR-75-391 Contract 954205 MARS SURFACE SAMPLE RETURN TRADEOFF STUDIES Final Report October 1975 Approved Technical Director This report was performed for the Jet Propulsion Laboratory, California Institute of Technology, sponsored by the National Aeronautics and Space Administration under Contract NAS7-100. MARTIN MARIETTA CCRPORATION DENVER DIVISION Denver, Colorado 80201 Ihis report docllr~_ntsthe results of four specific study tasks defined by the JPL seady manager as critical to the evolving understanding of the lhrs Surface Sample Beturn (LISSR) mission. Task 1 campares the Mars mission opportunities in 1981, 1983184, 1986, 1988, and 1990 to detennine which mission modes are possible and appropriate for each. Task 2 mines the design features of the hardware systems used to return the saaple, in the Mars orbit rendezvous mode, to identify ways in which the probability of back contamination can be minimized. Task 3 loolcs into the hardware and performance trade offs between the options of direct entry of the returning sample capsule at Earth and the orbital capture of that capsule for recovery by the Shuttle. Task 4 explores the possibilities for increasing the landed weight at Mars, beyond that possible with zfnimally modified Viking lander, to support HSSR missi-n modes involvk-g heavier systems. Bode technical mesroranda were prepared in accordance with the Contract Schedule, Article 1, Paragraph a. (31, of JPL Contract No. 954205, Mars Surface Sample Return (lSSR) Tradeoff Studies. A technical memorandum is submitted for each of the four tasks in the Statement of Work as follows: Task 1: Compile mission performance data for the leading mission mode candidates for the 1981, 1984, 1986, 1988 and 1990 opportunities. -
Increasing Launch Rate and Payload Capabilities
Aerial Launch Vehicles: Increasing Launch Rate and Payload Capabilities Yves Tscheuschner1 and Alec B. Devereaux2 University of Colorado, Boulder, Colorado Two of man's greatest achievements have been the first flight at Kitty Hawk and pushing into the final frontier that is space. Air launch systems aim to combine these great achievements into a revolutionary way to deliver satellites, cargo and eventually people into space. Launching from an aircraft has many advantages, including the ability to launch at any inclination and from above bad weather, which could delay ground launches. While many concepts for launching rockets from an airplane have been developed, very few have made it past the drawing board. Only the Pegasus and, to a lesser extent, SpaceShipOne have truly shown the feasibility of such a system. However, a recent push for rapid, small payload to orbit launches by the military and a general need for cheaper, heavy lift options are leading to an increasing interest in air launch methods. In order for the efficiency and flexibility of the system to be realized, however, additional funding and research are necessary. Nomenclature ALASA = airborne launch assist space access ALS = air launch system DARPA = defense advanced research project agency LEO = low Earth orbit LOX = liquid oxygen RP-1 = rocket propellant 1 MAKS = Russian air launch system MECO = main engine cutoff SS1 = space ship one SS2 = space ship two I. Introduction W hat typically comes to mind when considering launching people or satellites to space are the towering rocket poised on the launch pad. These images are engraved in the minds of both the public and scientists alike. -
Rocket Equation
Rocket Equation & Multistaging PROFESSOR CHRIS CHATWIN LECTURE FOR SATELLITE AND SPACE SYSTEMS MSC UNIVERSITY OF SUSSEX SCHOOL OF ENGINEERING & INFORMATICS 25TH APRIL 2017 Orbital Mechanics & the Escape Velocity The motion of a space craft is that of a body with a certain momentum in a gravitational field The spacecraft moves under the combines effects of its momentum and the gravitational attraction towards the centre of the earth For a circular orbit V = wr (1) F = mrw2 = centripetal acceleration (2) And this is balanced by the gravitational attraction F = mMG / r2 (3) 퐺푀 1/2 퐺푀 1/2 푤 = 표푟 푉 = (4) 푟3 푟 Orbital Velocity V 퐺 = 6.67 × 10−11 N푚2푘푔2 Gravitational constant M = 5.97× 1024 kg Mass of the Earth 6 푟0 = 6.371× 10 푚 Hence V = 7900 m/s For a non-circular (eccentric) orbit 1 퐺푀푚2 = 1 + 휀 푐표푠휃 (5) 푟 ℎ2 ℎ = 푚푟푉 angular momentum (6) ℎ2 휀 = 2 − 1 eccentricity (7) 퐺푀푚 푟0 1 퐺푀 2 푉 = 1 + 휀 푐표푠휃 (8) 푟 Orbit type For ε = 0 circular orbit For ε = 1 parabolic orbit For ε > 1 hyperbolic orbit (interplanetary fly-by) Escape Velocity For ε = 1 a parabolic orbit, the orbit ceases to be closed and the space vehicle will not return In this case at r0 using equation (7) ℎ2 1 = 2 − 1 but ℎ = 푚푟푣 (9) 퐺푀푚 푟0 1 2 2 2 푚 푉0 푟0 2퐺푀 2 2 = 2 therefore 푉0 = (10) 퐺푀푚 푟0 푟0 퐺 = 6.67 × 10−11 N푚2푘푔2 Gravitational constant M = 5.975× 1024 kg Mass of the Earth 6 푟0 = 6.371× 10 푚 Mean earth radius 1 2퐺푀 2 푉0 = Escape velocity (11) 푟0 푉0= 11,185 m/s (~ 25,000 mph) 7,900 m/s to achieve a circular orbit (~18,000 mph) Newton’s 3rd Law & the Rocket Equation N3: “to every action there is an equal and opposite reaction” A rocket is a device that propels itself by emitting a jet of matter. -
PARAMETRIC ANALYSIS of PERFORMANCE and DESIGN CHARACTERISTICS for ADVANCED EARTH-TO-ORBIT SHUTTLES by Edwurd A
NASA TECHNICAL NOTE -6767 . PARAMETRIC ANALYSIS OF PERFORMANCE AND DESIGN CHARACTERISTICS FOR ADVANCED EARTH-TO-ORBIT SHUTTLES by Edwurd A. Willis, Jr., Wz'llium C. Struck, und John A. Pudratt Lewis Reseurch Center Clevelund, Ohio 44135 NATIONAL AERONAUTICS AND SPACE ADMINISTRATION WASHINGTON, D. C. APRIL 1972 f TECH LIBRARY KAFB, NM I111111 Hlll11111 Ill# 11111 11111 lllllIll1Ill -. -- 0133bOL 1. Report No. 2. Government Accession No. 3. Recipient's Catalog No. - NASA TN D-6767 4. Title and Subtitle PAR I 5. Report Date METRIC NALYSIS OF PERFORMA K! E ND April 1972 DESIGN CHARACTERISTICS FOR ADVANCED EARTH-TO- 6. Performing Organization Code ORBIT SHUTTLES 7. Author(s) 8. Performing Organization Report No. Edward A. Willis, Jr. ; William C. Strack; and John A. Padrutt E-6749 10. Work Unit No. 9. Performing Organization Name and Address 110-06 Lewis Research Center 11. Contract or Grant No. National Aeronautics and Space Administration Cleveland, Ohio 44135 13. Type of Report and Period Covered 12. Sponsoring Agency Name and Address Technical Note National Aeronautics and Space Administration 14. Sponsoring Agency Code Washington, D. C. 20546 ~~ .. ~~ 16. Abstract Performance, trajectory, and design characteristics are presented for (1) a single-stage shuttle with a single advanced rocket engine, (2) a single-stage shuttle with an initial parallel chemical-engine and advanced-engine burn followed by an advanced-engine sustainer burn (parallel-burn configuration), (3) a single-stage shuttle with an initial chemical-engine burn followed by an advanced-engine burn (tandem-burn configuration), and (4)a two-stage shuttle with a chemical-propulsion booster stage and an advanced-propulsion upper stage. -
Aeronautical Engineering
Aeronautical NASA SP-7037 (95) Engineering April 1978 A Continuing NASA Bibliography indexes National Space Administration Aeronautical Engineering Aer ering Aeronautical Engineerin igineerjng Aeronautical Engin ^il Engineering Aeronautical E nautical Engineering Aeronau Aeronautical Engineering Aer ^ring Aeronautical Engineering gineer jng Aeronautical Engirn al Engineering Aeronautical E nautical Engineering Aeronaut Aeronautical Engineering Aerc ring Aeronautical Engineering ACCESSION NUMBER RANGES Accession numbers cited in this Supplement fall within the following ranges: STAR(N-10000 Series) N78-13998—N78-15985 IAA (A-10000 Series) A78-17138—A78-20614 This bibliography was prepared by the NASA Scientific and Technical Information Facility operated for the National Aeronautics and Space Administration by Informatics Information NASA SP-7037(95) AERONAUTICAL ENGINEERING A Continuing Bibliography Supplement 95 A selection of annotated references to unclas- sified reports and journal articles that were introduced into the NASA scientific and tech- nical information system and announced in March 1978m • Scientific and Technical Aerospace Reports (STAR) • International Aerospace Abstracts (IAA) Scientific and Technical Information Office • 1978. National Aeronautics and Space Administration Washington, DC This Supplement is available from the National Technical Information Service (NTIS), Springfield, Virginia 22161, at the price code E02 ($475 domestic, $9 50 foreign) INTRODUCTION Under the terms of an interagency agreement with the Federal Aviation Administration this publication has been prepared by the National Aeronautics and Space Administration for the joint use of both agencies and the scientific and technical community concerned with the field of aeronautical engineering. The first issue of this bibliography was published in September 1970 and the first supplement in January 1971. Since that time, monthly supplements have been issued. -
Rocket Basics 1: Thrust and Specific Impulse
4. The Congreve Rocket ROCKET BASICS 1: THRUST AND SPECIFIC IMPULSE In a liquid-propellant rocket, a liquid fuel and oxidizer are injected into the com- bustion chamber where the chemical reaction of combustion occurs. The combustion process produces hot gases that expand through the nozzle, a duct with the varying cross section. , In solid rockets, both fuel and oxidizer are combined in a solid form, called the grain. The grain surface burns, producing hot gases that expand in the nozzle. The rate of the gas production and, correspondingly, pressure in the rocket is roughly proportional to the burning area of the grain. Thus, the introduction of a central bore in the grain allowed an increase in burning area (compared to “end burning”) and, consequently, resulted in an increase in chamber pressure and rocket thrust. Modern nozzles are usually converging-diverging (De Laval nozzle), with the flow accelerating to supersonic exhaust velocities in the diverging part. Early rockets had only a crudely formed converging part. If the pressure in the rocket is high enough, then the exhaust from a converging nozzle would occur at sonic velocity, that is, with the Mach number equal to unity. The rocket thrust T equals PPAeae TmUPPAmUeeae e mU eq m where m is the propellant mass flow (mass of the propellant leaving the rocket each second), Ue (exhaust velocity) is the velocity with which the propellant leaves the nozzle, Pe (exit pressure) is the propellant pressure at the nozzle exit, Pa (ambient 34 pressure) is the pressure in the surrounding air (about one atmosphere at sea level), and Ae is the area of the nozzle exit; Ueq is called the equivalent exhaust velocity.