Design and Simulation of a 1N Hydrogen Peroxide Monopropellant Thruster

Total Page:16

File Type:pdf, Size:1020Kb

Design and Simulation of a 1N Hydrogen Peroxide Monopropellant Thruster POLITECNICO DI MILANO School of Industrial and Information Engineering Master of Science in Aeronautical Engineering Design and simulation of a 1N hydrogen peroxide monopropellant thruster Supervisor: Prof. Luciano GALFETTI Master Thesis by: Andrea URAS 898198 Academic Year 2018 - 2019 Sommario L'utilizzo del perossido di idrogeno come monopropellente per applicazioni che richiedono bassi livelli di spinta `etornato ad essere di grande interesse negli ultimi anni. L'obiettivo principale `equello di trovare un sostituto dell'idrazina, altamente tossica e cancerogena, e il perossido di idrogeno ne rappresenta una valida alternativa per via del suo basso impatto ambientale. Questo lavoro di tesi si `eoccupato del design, del dimensionamento e della simulazione di Fluidodinamica Computazionale (CFD) di un monopropellente, alimentato ad acqua ossigenata, capace di produrre 1 Newton di spinta nel vuoto. Il design e il dimensionamento sono stati effettuati con l'ausilio di Chemical Equilib- rium with Applications (CEA), un software sviluppato della NASA utilizzato per appli- cazioni termochimiche. La simulazione CFD, effettuata con il software ANSYS® Fluent, ha riguardato l'analisi dell'ugello e della scia di scarico a diverse altitudini. Ci`oha permesso di valutare l’efficienza dell'ugello confrontando i parametri ideali con quelli ottenuti attraverso le simulazioni, mostrando come il propulsore risulti pi`uefficiente quando opera in regime adattato op- pure sottoespanso. Inoltre, `estato possibile apprezzare come la pressione esterna influenzi la struttura delle scia di scarico dell'ugello, composta da una serie di onde d'urto e di es- pansioni di Prandtl-Meyer. I Abstract The use of hydrogen peroxide as a monopropellant for low-thrust applications had a renewed interest in the last years. The main goal is to find a substitute for hydrazine, highly toxic and cancerogenic, and hydrogen peroxide represents a valid alternative for its low environmental impact. This thesis work concerned about design, sizing and Computational Fluid Dynamics (CFD) simulation of a hydrogen peroxide monopropellant thruster capable to produce 1 Newton of thrust in vacuum. The design and the sizing have been carried with the aid of Chemical Equilibrium with Applications (CEA), a software developed by NASA used for thermochemical applications. The CFD simulation, carried by means of ANSYS® Fluent software, concerned the analysis of the nozzle and the exhaust plume at different altitudes. It has been then pos- sible to evaluate the nozzle efficiency, comparing ideal parameters with the one obtained with the simulations, showing how the engine results to be more efficient in adapted or underexpanded regime. Moreover, it has been possible to observe how the external pres- sure influences the structure of the exhaust plume, composed of a series of oblique shocks and Prandtl-Meyer expansions. II Ringraziamenti Prima di tutto vorrei ringraziare la mia famiglia, la quale mi ha supportato, economica- mente e moralmente, per tutta la durata del mio percorso universitario e mi ha sempre sostenuto nelle scelte fatte. Senza di voi non sarebbe stato possibile tutto questo. Un grazie a quella che `estata per quasi due anni la mia seconda famiglia: Mattia, Fede e Luca. Con voi mi sono sentito a casa e non avrei potuto chiedere compagni di viaggio migliori. Insieme a loro vorrei ringraziare anche Andrea, Marco e Matteo che, nonostante non abbiano partecipato alla spedizione meneghina, fanno comunque parte della grande famiglia made in UniGe di CXVIII. Vorrei poi ringraziare anche gli amici della parentesi francese: Fede, che dopo Genova e Milano ha deciso che non poteva lasciarmi partire da solo per Poitiers, Fede Boni, Irene e, last but not least, Paola, una delle persone migliori che abbia mai conosciuto. Un grazie agli amici di sempre, Viola e Gli Amici del Mietitore, con cui sono cresciuto e che continuano ad essere una felice costante all'interno della mia vita. Grazie anche a Dario e Yuri, con cui ho condiviso gli ultimi mesi a Milano, e a Mario, che mi ha risolto parecchi problemi lasciandomi la sua stanza. Ringrazio il mio relatore, Professor Luciano Galfetti, il quale, nonostante tutti i prob- lemi e gli impegni, ha sempre trovato il modo di dedicarmi del tempo. Ringrazio anche il gi`acitato Mattia, il quale mi ha dato un aiuto non indifferente per quanto riguarda la parte di simulazione fluidodinamica. Ringrazio anche lo staff e gli altri ragazzi di SPLab che, proprio nel momento in cui stavamo iniziando a conoscerci, non ho avuto la possibilit`adi salutare per via della terribile emergenza che ha colpito il nostro paese negli ultimi mesi. III Nomenclature Acronyms ACS Attitude Control System ATO Assisted-Take-Off CEA Chemical Equilibrium with Applications CFD Computational Fluid Dynamics DLR Deutsches Zentrum f¨ur Luft- und Raumfahrt (German Aerospace Center) DNS Direct Numerical Simulation DSGS Dynamic Subgrid-scale ESA European Space Agency FVM Finite Volume Method GEO Geostationary Earth Orbit HTP High Test Peroxide HYPROGEO Hybrid Propulsion System for LEO, MEO and GEO transfer LEO Low Earth Orbit LES Large Eddy Simulation LPT Low pressure tank MEO Medium Earth Orbit MMH Monomethylhydrazine MON Mixed Oxides of Nitrogen NASA National Aeronautics and Space Administration NTO Nitrogen Tetroxide PDE Partial Differential Equation PTFE Polytetrafluoroethylene RACS Roll and Attitude Control System RANS Reynolds Average Navier-Stokes RATO Rocket-Assisted-Take-Off RCS Reaction Control System SME Small and Medium Enterprises UDMH Unsymmetrical Dimethyl Hydrazine Chemical formulas (g) Gaseous (l) Liquid Cr Chrome Cu Copper Fe Iron H2O2 Hydrogen peroxide H2O Water in vapour form H2 Hydrogen IV HO2 Hydroperoxyl radical H Atomic hydrogen Mn Manganese M Third body N2H4 Hydrazine N2O4 Nitrogen tetroxide O2 Oxygen OH Hydroxyl radical O Atomic oxygen Operators (∗)0 Fluctuating component in Reynolds average (∗)00 Fluctuating component in Favre average (∗)i,(∗)j,(∗)α,(∗)β Components along i, j, α, β direction (∗) Reynolds average (c∗) Filtered variable (f∗) Favre average Symbols (qΦ)P source term evaluated at cell centre αconv Convergent angle αdiv Divergent angle ∆Pi Pressure drop of injector ∆Pv Pressure drop of solenoid valve ∆Pcp Pressure drop in the catalyst pack ∆t Time step ∆V Velocity change ∆ Filter width in LES δij Kronecker Delta m_ p Propellant mass flow rate Area ratio Γ Diffusion term γ Ratio of the specific heats κ Reaction rate coefficient λ Thermal conductivity µ Viscosity µT Turbulent viscosity ν Kinematic viscosity νT Kinematic turbulent viscosity νt Subgrid viscosity ! Characteristic frequency of turbulence !r Reaction rate Ωv Volume of integration Φ Reaction scalar φ Bed loading ΦE Reaction scalar evaluated at center of "East" cell Φe Reaction scalar evaluated at "East" frontier of cell ΦP Reaction scalar evaluated at cell center ρ Density V ρe Exit nozzle density ρHTP Density of HTP ρIsp Density specific impulse σiα Stress tensor τ Turbulence time scale τij Subgrid stress term n Normal vector " Dissipation rate of turbulent kinetic energy A Pre-exponential factor Ac Chamber area Ae Nozzle exit area At Throat area At Throat area C Courant number c Chamber speed of sound c∗ Characteristic velocity ce Exit nozzle speed of sound CF Thrust coefficient Cp Specific heat at constant pressure Cs Smagorinsky coefficient Cµ, σk, σ, C1, C2, σ!, C!1, C!2, σΦ Empirical constants CDi Discharge coefficient of the injector CFCFD Thrust coefficient evaluated from CFD CFideal Ideal thrust coefficient d Mass diffusivity Dc Chamber diameter De Exit nozzle diameter Di Injector diameter Dt Throat diameter Ea Activation energy F Thrust G Generic filter g Acceleration of gravity h Enthalpy hS Enthalpy at constant entropy ISPvac Specific impulse in vacuum Isp Specific impulse k Turbulent kinetic energy Kv Flow coefficient of solenoid valve l∗ Length scale l0 Integral scale lk Kolmogorov lenght scale lm Mixing lenght Lconv Convergent length Lcp Catalyst pack length Ldiv Divergent length Me Exit nozzle Mach number mp Propellant mass VI mtot Total mass N Number of mesh points P Nozzle pressure p Pressure Pa Ambient pressure Pc Chamber pressure Pe Nozzle exit pressure Pk Production of turbulent kinetic energy PeCFD Exit nozzle pressure evaluated from CFD Peid Ideal exit nozzle pressure Ppt Propellant tank pressure qc Heat released by reaction QP Volumetric flow rate of the propellant qΦ Source term for scalar Φ R Gas constant Re Reynolds number Re0 Turbulent Reynolds number sm Mesh spacing Sij Strain rate tensor SG Specific gravity T Temperature t Time Tc Chamber temperature Te Exit nozzle temperature Tt Throat temperature Tad Adiabatic temperature tboost Boost time Tij Shear stress term to be solved in LES tres Residence time u Velocity 0 u0 RMS of velocity u∗ Velocity scale uτ Friction velocity V Nozzle velocity Ve Exit nozzle velocity VeCFD Exit nozzle velocity evaluated from CFD Veid Ideal exit nozzle velocity vprod Specific volume of products Vpt Propellant tank volume x, y Spatial coordinates Y Mass fraction y+ Dimensionless wall distance ∆h Enthalpy variation VII Contents 1 Introduction 1 1.1 Motivation . .1 1.2 Goal of the thesis . .1 1.3 Structure of the work . .2 2 State of the art 3 2.1 Hydrogen Peroxide for propulsion applications . .3 2.1.1 Historical background . .3 2.1.2 Current developments . .7 2.2 Theory of rocket propulsion . .8 2.2.1 Fundamental equations . 11 2.2.2 Expansion in convergent-divergent nozzle . 12 2.2.3 Plume structure . 13 2.3 Hydrogen Peroxide safety, handling and storage . 15 2.4 Decomposition of Hydrogen Peroxide . 21 2.4.1 Catalytic decomposition . 22 2.4.2 Thermal decomposition . 23 3 Preliminary design 25 3.1 Computation of operating parameters with NASA CEA code . 25 3.2 Sizing of the thruster . 26 3.3 Feed line design . 28 3.4 Example of research stand for experimental investigation . 30 4 CFD Simulation and modelization 31 4.1 Description and resolution of Navier-Stokes equations . 32 4.1.1 Direct Numerical Simulation (DNS) .
Recommended publications
  • Back to the the Future? 07> Probing the Kuiper Belt
    SpaceFlight A British Interplanetary Society publication Volume 62 No.7 July 2020 £5.25 SPACE PLANES: back to the the future? 07> Probing the Kuiper Belt 634089 The man behind the ISS 770038 Remembering Dr Fred Singer 9 CONTENTS Features 16 Multiple stations pledge We look at a critical assessment of the way science is conducted at the International Space Station and finds it wanting. 18 The man behind the ISS 16 The Editor reflects on the life of recently Letter from the Editor deceased Jim Beggs, the NASA Administrator for whom the building of the ISS was his We are particularly pleased this supreme achievement. month to have two features which cover the spectrum of 22 Why don’t we just wing it? astronautical activities. Nick Spall Nick Spall FBIS examines the balance between gives us his critical assessment of winged lifting vehicles and semi-ballistic both winged and blunt-body re-entry vehicles for human space capsules, arguing that the former have been flight and Alan Stern reports on his grossly overlooked. research at the very edge of the 26 Parallels with Apollo 18 connected solar system – the Kuiper Belt. David Baker looks beyond the initial return to the We think of the internet and Moon by astronauts and examines the plan for a how it helps us communicate and sustained presence on the lunar surface. stay in touch, especially in these times of difficulty. But the fact that 28 Probing further in the Kuiper Belt in less than a lifetime we have Alan Stern provides another update on the gone from a tiny bleeping ball in pioneering work of New Horizons.
    [Show full text]
  • 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.
    [Show full text]
  • Combustion Tap-Off Cycle
    College of Engineering Honors Program 12-10-2016 Combustion Tap-Off Cycle Nicole Shriver Embry-Riddle Aeronautical University, [email protected] Follow this and additional works at: https://commons.erau.edu/pr-honors-coe Part of the Aeronautical Vehicles Commons, Other Aerospace Engineering Commons, Propulsion and Power Commons, and the Space Vehicles Commons Scholarly Commons Citation Shriver, N. (2016). Combustion Tap-Off Cycle. , (). Retrieved from https://commons.erau.edu/pr-honors- coe/6 This Article is brought to you for free and open access by the Honors Program at Scholarly Commons. It has been accepted for inclusion in College of Engineering by an authorized administrator of Scholarly Commons. For more information, please contact [email protected]. Honors Directed Study: Combustion Tap-Off Cycle Date of Submission: December 10, 2016 by Nicole Shriver [email protected] Submitted to Dr. Michael Fabian Department of Aerospace Engineering College of Engineering In Partial Fulfillment Of the Requirements Of Honors Directed Study Fall 2016 1 1.0 INTRODUCTION The combustion tap-off cycle is also known as the “topping cycle” or “chamber bleed cycle.” It is an open liquid bipropellant cycle, usually of liquid hydrogen and liquid oxygen, that combines the fuel and oxidizer in the main combustion chamber. Gases from the edges of the combustion chamber are used to power the engine’s turbine and are expelled as exhaust. Figure 1.1 below shows a picture representation of the cycle. Figure 1.1: Combustion Tap-Off Cycle The combustion tap-off cycle is rather unconventional for rocket engines as it has only been put into practice with two engines.
    [Show full text]
  • 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.
    [Show full text]
  • Validation of a Simplified Model for Liquid Propellant Rocket Engine Combustion Chamber Design
    IOP Conference Series: Materials Science and Engineering PAPER • OPEN ACCESS Validation of a simplified model for liquid propellant rocket engine combustion chamber design To cite this article: M Hegazy et al 2020 IOP Conf. Ser.: Mater. Sci. Eng. 973 012003 View the article online for updates and enhancements. This content was downloaded from IP address 170.106.33.14 on 25/09/2021 at 23:25 AMME-19 IOP Publishing IOP Conf. Series: Materials Science and Engineering 973 (2020) 012003 doi:10.1088/1757-899X/973/1/012003 Validation of a simplified model for liquid propellant rocket engine combustion chamber design M Hegazy1, H Belal2, A Makled3 and M A Al-Sanabawy4 1 M.Sc. Student, Rocket Department, Military Technical College, Egypt 2 Assistant Professor, Rocket Department, Military Technical College, Egypt 3 Associate Professor. Zagazig University, Egypt 4 Associate Professor. Rocket Department, Military Technical College, Egypt [email protected] Abstract. The combustion phenomena inside the thrust chamber of the liquid propellant rocket engine are very complicated because of different paths for elementary processes. In this paper, the characteristic length (L*) approach for the combustion chamber design will be discussed compared to the effective length (Leff) approach. First, both methods are introduced then applied for real LPRE. The effective length methodology is introduced starting from the basic model until developing the empirical equations that may be used in the design process. The classical procedure of L* was found to over-estimate the required cylindrical length in addition to the inherent shortcoming of not giving insight where to move to enhance the design.
    [Show full text]
  • Cryogenic Technology & Rocket Engines
    ISSN (O): 2393-8609 International Journal of Aerospace and Mechanical Engineering Volume 2 – No.5, August 2015 Cryogenic Technology & Rocket Engines AKHIL GARG KARTIK JAKHU KISHAN SINGH ABHINAV B.Tech – Aerospace B.Tech – Aerospace B.Tech – Aerospace MAURYA Engg. Engg. Engg. B.Tech – Aerospace PUNJAB PUNJAB PUNJAB Engg. TECHNICAL TECHNICAL TECHNICAL PUNJAB UNIVERSITY, UNIVERSITY, UNIVERSITY, TECHNICAL JALANDHAR JALANDHAR JALANDHAR UNIVERSITY, akhilgarg.313@g kartik.lphawk@g kishansngh1996 JALANDHAR mail.com mail.com @gmail.com abhinavguru123 @gmail.com ABSTRACT 3.2 What is Cryogenic Rocket Engine? This paper is all about the rocket engine involving the use of A cryogenic rocket engine is a rocket engine that cryogenic technology at a cryogenic temperature (123K). This uses a cryogenic fuel or oxidizer, that is, its fuel or basically uses the liquid oxygen and liquid hydrogen as an oxidizer (or both) is gases liquefied and stored at oxidizer and fuel, which are very clean and non-pollutant very low temperatures. Notably, these engines were fuels compared to other hydrocarbon fuels like petrol, diesel, one of the main factors of the ultimate success in gasoline, LPG, CNG, etc., sometimes, liquid nitrogen is also reaching the Moon by the Saturn V rocket. used as an fuel. During World War II, when powerful rocket engines were first considered by the German, American and Keywords Soviet engineers independently, all discovered that Rocket engine, Cryogenic technology, Cryogenic temperature, rocket engines need high mass flow rate of both Liquid hydrogen and Oxygen. oxidizer and fuel to generate a sufficient thrust. At that time oxygen and low molecular weight 1.
    [Show full text]
  • Sidney Allan Ceng, Fraes 1909-1973
    frustration caused him to tend to withdraw somewhat broader front. This made him very vulnerable and it was from the company of others and thus give an appearance in this respect that his wife (Tommy) was such a tower of of aloofness. Those of us who were privileged to know strength to him throughout their long married life. Her him better recognised this as mere illusion for he could be death just over three years ago was a great blow to him. the most warm and charming of companions. His very Though now gone he will live on for as long as people keen sense of humour could always be relied upon to en­ are concerned with the problems of flight in a way that is liven any conversation and often even shone through much aptly described by words that Barry himself used of of his technical writing, whilst in the right circumstance he another, could use a caustic wit with quite devastating effect Above all he loved the simple things of life—the beauty of nature "He is not dead. Still on my mortal breath and the countryside. Walking was a favourite pastime of Swells a low music from his heart's desire. his as was also working in his garden and it is not un­ I am most proud, and you most cheated, Death, natural that this part of him is reflected so well in a num­ Knowing in bis closed book this deathless fire". ber of his poems. A man of great sensitivity he always Poems, 1925 reacted vigorously to any suggestion of man's inhumanity to man whether on a person to person level or on a H.
    [Show full text]
  • Solid Propellant Rocket Engines - V.M
    THERMAL TO MECHANICAL ENERGY CONVERSION: ENGINES AND REQUIREMENTS – Vol. II - Solid Propellant Rocket Engines - V.M. Polyaev and V.A. Burkaltsev SOLID PROPELLANT ROCKET ENGINES V.M. Polyaev and V.A. Burkaltsev Department of Rocket engines, Bauman Moscow State Technical University, Russia. Keywords: Combustion chamber, solid propellant load, pressure, temperature, nozzle, thrust, control, ignition, cartridge, aspect ratio, regime. Contents 1. Introduction 2. Historical information 3. SPRE scheme and main units 4. SPRE operation 5. Parameter optimization, the approach and results 6. Transient regime 7. Service 8. Development prospects 9. Conclusions Acknowledgments Glossary Bibliography Biographical Sketches 1. Introduction Solid propellant rocket engines (SPRE) are called the direct reaction engines, in which chemical energy of the solid propellant being placed in the combustion chamber is transformed at first to thermal energy, and then to kinetic energy of the combustion products thrown away with high velocity in the environment. The momentum of combustion products discharging through the nozzle is equal to the impulse of reactive force being created by the engine. 2. Historical information First of rocketsUNESCO known to us were rockets – with EOLSS primitive powder rocket engines used in China near 5000 years ago for pleasure and military aims (so-called "fiery arrows", Figure 1). SAMPLE CHAPTERS The first rocket propellant was black smoky powder (potassium saltpetre with charcoal mixture). In Russia, powder rockets appeared in the beginning of XVII century. In 1680, Tsar Peter I founded "rocket institution" in Moscow for firework rockets making. In 1717 lighting signal rockets existed for 200 years without changes. In the beginning of XIX century, Englishman Kongrev improved the "fiery arrows" having been borrowed from Hindus.
    [Show full text]
  • 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...........................................................
    [Show full text]
  • Apollo Rocket Propulsion Development
    REMEMBERING THE GIANTS APOLLO ROCKET PROPULSION DEVELOPMENT Editors: Steven C. Fisher Shamim A. Rahman John C. Stennis Space Center The NASA History Series National Aeronautics and Space Administration NASA History Division Office of External Relations Washington, DC December 2009 NASA SP-2009-4545 Library of Congress Cataloging-in-Publication Data Remembering the Giants: Apollo Rocket Propulsion Development / editors, Steven C. Fisher, Shamim A. Rahman. p. cm. -- (The NASA history series) Papers from a lecture series held April 25, 2006 at the John C. Stennis Space Center. Includes bibliographical references. 1. Saturn Project (U.S.)--Congresses. 2. Saturn launch vehicles--Congresses. 3. Project Apollo (U.S.)--Congresses. 4. Rocketry--Research--United States--History--20th century-- Congresses. I. Fisher, Steven C., 1949- II. Rahman, Shamim A., 1963- TL781.5.S3R46 2009 629.47’52--dc22 2009054178 Table of Contents Foreword ...............................................................................................................................7 Acknowledgments .................................................................................................................9 Welcome Remarks Richard Gilbrech ..........................................................................................................11 Steve Fisher ...................................................................................................................13 Chapter One - Robert Biggs, Rocketdyne - F-1 Saturn V First Stage Engine .......................15
    [Show full text]
  • Lesson 2: YOU're LAUNCHING a ROCKET!
    Adventures in Aerospace: Lesson 2 Volunteer’s Guide Key to Curriculum Formatting: ► Volunteer Directions ■ Volunteer Notes ♦ Volunteer-led Classroom Experiments Lesson 2: YOU’RE LAUNCHING A ROCKET! ► Begin the presentation by telling the class that this is “Lesson 2: You’re Launching a Rocket!” If this is your second visit, reintroduce yourself and the program. Briefly review key concepts from the first lesson, “You’re Piloting a Plane!” If this is your first visit, here is a suggested personal introduction: “Hello, my name is _____________, and I am a _________________ (position title) at Aerojet. I or another Aerojet volunteer will be visiting your class once over the next few months to speak to you about space exploration and space travel. We will learn about the basics of aerodynamics, rocket propulsion, and spaceflight to the space station, the moon, and future missions to Mars!” ► Answer any questions left over from the previous visit. MATERIALS NEEDED • AiA Multimedia Presentation (AMP) • DVD-ROM Page 1 of 11 Adventures in Aerospace: Lesson 2 Volunteer’s Guide • TV or projection screen • Handouts • Index cards ► See lesson to assess total equipment needs. LESSON OUTLINE Introduction Lesson Concepts Vocabulary Rockets vs. Airplanes Newton’s Laws • First Law • Second Law • Third Law What Type of Rocket Are You Launching? • Types of Engines Comparing and Contrasting Liquid Engines and Solid Motors Other Types of Rocket Engines Applying What We’ve Learned Experiment INTRODUCTION Rocket launches have mesmerized audiences, often entire nations, for centuries. What kind of power does it take to propel spacecraft out of the atmosphere and into the vacuum of space? This unit introduces you to rocket propulsion systems.
    [Show full text]
  • Design and Dynamic Characteristics of a Liquid-Propellant Thrust Chamber
    DESIGN AND DYNAMIC CHARACTERISTICS OF A LIQUID-PROPELLANT THRUST CHAMBER Avandelino Santana Junior Instituto de Aeronáutica e Espaço, Centro Técnico Aeroespacial, IAE/CTA, CEP 12228-904 - São José dos Campos, SP, Brasil. E-mail: [email protected] Luiz Carlos Sandoval Góes Instituto Tecnológico de Aeronáutica, ITA, CEP 12228-900 - São José dos Campos, SP, Brasil. E-mail: [email protected] Abstract. According to the national program for space activities (PNAE), which is elaborated by the Brazilian space agency (AEB), the liquid propulsion technology is essential in the de- velopment of the next launch vehicle, called VLS-2. The advantages of liquid-propellant rocket engines are their high performance compared to any other conventional chemical en- gine and their controllability in terms of thrust modulation. Undeniably, the most important component of these engines is the thrust chamber, which generates thrust by providing a vol- ume for combustion and converting thermal energy to kinetic energy. This paper presents the design and the dynamic analysis of a thrust chamber, which can be part of the future Brazil- ian rocket. The basic components of the thrust chamber assembly are described, a mathe- matical model for simulation of the system at nominal regime of operation is constructed, and the dynamic characteristics including the stability analysis are briefly discussed. Keywords: Liquid rocket engine, liquid propulsion, rocket engine design, dynamic modeling, dynamic analysis. 1. INTRODUCTION The design of an engine and its components is not a simple task, especially concerning liquid-propellant engine system, because it includes complex and multidisciplinary problems. Since rocket engines are airborne devices, a desirable thrust chamber combines lightweight construction with high performance, simplicity, and reliability (Sutton, 1986).
    [Show full text]