Thruster Principles
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Aerospace Engine Data
AEROSPACE ENGINE DATA Data for some concrete aerospace engines and their craft ................................................................................. 1 Data on rocket-engine types and comparison with large turbofans ................................................................... 1 Data on some large airliner engines ................................................................................................................... 2 Data on other aircraft engines and manufacturers .......................................................................................... 3 In this Appendix common to Aircraft propulsion and Space propulsion, data for thrust, weight, and specific fuel consumption, are presented for some different types of engines (Table 1), with some values of specific impulse and exit speed (Table 2), a plot of Mach number and specific impulse characteristic of different engine types (Fig. 1), and detailed characteristics of some modern turbofan engines, used in large airplanes (Table 3). DATA FOR SOME CONCRETE AEROSPACE ENGINES AND THEIR CRAFT Table 1. Thrust to weight ratio (F/W), for engines and their crafts, at take-off*, specific fuel consumption (TSFC), and initial and final mass of craft (intermediate values appear in [kN] when forces, and in tonnes [t] when masses). Engine Engine TSFC Whole craft Whole craft Whole craft mass, type thrust/weight (g/s)/kN type thrust/weight mini/mfin Trent 900 350/63=5.5 15.5 A380 4×350/5600=0.25 560/330=1.8 cruise 90/63=1.4 cruise 4×90/5000=0.1 CFM56-5A 110/23=4.8 16 -
An Assessment of Aerocapture and Applications to Future Missions
Post-Exit Atmospheric Flight Cruise Approach An Assessment of Aerocapture and Applications to Future Missions February 13, 2016 National Aeronautics and Space Administration An Assessment of Aerocapture Jet Propulsion Laboratory California Institute of Technology Pasadena, California and Applications to Future Missions Jet Propulsion Laboratory, California Institute of Technology for Planetary Science Division Science Mission Directorate NASA Work Performed under the Planetary Science Program Support Task ©2016. All rights reserved. D-97058 February 13, 2016 Authors Thomas R. Spilker, Independent Consultant Mark Hofstadter Chester S. Borden, JPL/Caltech Jessie M. Kawata Mark Adler, JPL/Caltech Damon Landau Michelle M. Munk, LaRC Daniel T. Lyons Richard W. Powell, LaRC Kim R. Reh Robert D. Braun, GIT Randii R. Wessen Patricia M. Beauchamp, JPL/Caltech NASA Ames Research Center James A. Cutts, JPL/Caltech Parul Agrawal Paul F. Wercinski, ARC Helen H. Hwang and the A-Team Paul F. Wercinski NASA Langley Research Center F. McNeil Cheatwood A-Team Study Participants Jeffrey A. Herath Jet Propulsion Laboratory, Caltech Michelle M. Munk Mark Adler Richard W. Powell Nitin Arora Johnson Space Center Patricia M. Beauchamp Ronald R. Sostaric Chester S. Borden Independent Consultant James A. Cutts Thomas R. Spilker Gregory L. Davis Georgia Institute of Technology John O. Elliott Prof. Robert D. Braun – External Reviewer Jefferey L. Hall Engineering and Science Directorate JPL D-97058 Foreword Aerocapture has been proposed for several missions over the last couple of decades, and the technologies have matured over time. This study was initiated because the NASA Planetary Science Division (PSD) had not revisited Aerocapture technologies for about a decade and with the upcoming study to send a mission to Uranus/Neptune initiated by the PSD we needed to determine the status of the technologies and assess their readiness for such a mission. -
Gravity-Assist Trajectories to Jupiter Using Nuclear Electric Propulsion
AAS 05-398 Gravity-Assist Trajectories to Jupiter Using Nuclear Electric Propulsion ∗ ϒ Daniel W. Parcher ∗∗ and Jon A. Sims ϒϒ This paper examines optimal low-thrust gravity-assist trajectories to Jupiter using nuclear electric propulsion. Three different Venus-Earth Gravity Assist (VEGA) types are presented and compared to other gravity-assist trajectories using combinations of Earth, Venus, and Mars. Families of solutions for a given gravity-assist combination are differentiated by the approximate transfer resonance or number of heliocentric revolutions between flybys and by the flyby types. Trajectories that minimize initial injection energy by using low resonance transfers or additional heliocentric revolutions on the first leg of the trajectory offer the most delivered mass given sufficient flight time. Trajectory families that use only Earth gravity assists offer the most delivered mass at most flight times examined, and are available frequently with little variation in performance. However, at least one of the VEGA trajectory types is among the top performers at all of the flight times considered. INTRODUCTION The use of planetary gravity assists is a proven technique to improve the performance of interplanetary trajectories as exemplified by the Voyager, Galileo, and Cassini missions. Another proven technique for enhancing the performance of space missions is the use of highly efficient electric propulsion systems. Electric propulsion can be used to increase the mass delivered to the destination and/or reduce the trip time over typical chemical propulsion systems.1,2 This technology has been demonstrated on the Deep Space 1 mission 3 − part of NASA’s New Millennium Program to validate technologies which can lower the cost and risk and enhance the performance of future missions. -
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 -
Helicopter Turboshafts
Helicopter Turboshafts Luke Stuyvenberg University of Colorado at Boulder Department of Aerospace Engineering The application of gas turbine engines in helicopters is discussed. The work- ings of turboshafts and the history of their use in helicopters is briefly described. Ideal cycle analyses of the Boeing 502-14 and of the General Electric T64 turboshaft engine are performed. I. Introduction to Turboshafts Turboshafts are an adaptation of gas turbine technology in which the principle output is shaft power from the expansion of hot gas through the turbine, rather than thrust from the exhaust of these gases. They have found a wide variety of applications ranging from air compression to auxiliary power generation to racing boat propulsion and more. This paper, however, will focus primarily on the application of turboshaft technology to providing main power for helicopters, to achieve extended vertical flight. II. Relationship to Turbojets As a variation of the gas turbine, turboshafts are very similar to turbojets. The operating principle is identical: atmospheric gases are ingested at the inlet, compressed, mixed with fuel and combusted, then expanded through a turbine which powers the compressor. There are two key diferences which separate turboshafts from turbojets, however. Figure 1. Basic Turboshaft Operation Note the absence of a mechanical connection between the HPT and LPT. An ideal turboshaft extracts with the HPT only the power necessary to turn the compressor, and with the LPT all remaining power from the expansion process. 1 of 10 American Institute of Aeronautics and Astronautics A. Emphasis on Shaft Power Unlike turbojets, the primary purpose of which is to produce thrust from the expanded gases, turboshafts are intended to extract shaft horsepower (shp). -
Session 6:Analytical Approximations for Low Thrust Maneuvers
Session 6: Analytical Approximations for Low Thrust Maneuvers As mentioned in the previous lecture, solving non-Keplerian problems in general requires the use of perturbation methods and many are only solvable through numerical integration. However, there are a few examples of low-thrust space propulsion maneuvers for which we can find approximate analytical expressions. In this lecture, we explore a couple of these maneuvers, both of which are useful because of their precision and practical value: i) climb or descent from a circular orbit with continuous thrust, and ii) in-orbit repositioning, or walking. Spiral Climb/Descent We start by writing the equations of motion in polar coordinates, 2 d2r �dθ � µ − r + = a (1) 2 2 r dt dt r 2 d θ 2 dr dθ aθ + = (2) 2 dt r dt dt r We assume continuous thrust in the angular direction, therefore ar = 0. If the acceleration force along θ is small, then we can safely assume the orbit will remain nearly circular and the semi-major axis will be just slightly different after one orbital period. Of course, small and slightly are vague words. To make the analysis rigorous, we need to be more precise. Let us say that for this approximation to be valid, the angular acceleration has to be much smaller than the corresponding centrifugal or gravitational forces (the last two terms in the LHS of Eq. (1)) and that the radial acceleration (the first term in the LHS in the same equation) is negligible. Given these assumptions, from Eq. (1), dθ r µ d2θ 3 r µ dr ≈ ! ≈ − (3) 3 2 5 dt r dt 2 r dt Substituting into Eq. -
Thrust Reverser
DC-10THRUST REVERSER Following an airplane accident in which inadver- tent thrust reverser deployment was considered a major contributor, the aviation industry and SAFETY the U.S. Federal Aviation Administration (FAA) adopted new criteria for evaluating the safety of ENHANCEMENT thrust reverser systems on commercial airplanes. Several airplane models were determined to be uncontrollable in some portions of the flight HARRY SLUSHER envelope after inadvertent deployment of the PROGRAM MANAGER AIRCRAFT MODIFICATION ENGINEERING thrust reverser. In response, Boeing and the BOEING COMMERCIAL AIRPLANES GROUP SAFETY FAA issued service bulletins and airworthiness AERO directives, respectively, for mandatory inspec- 39 tions and installation of thrust reverser actuation system locks on affected Boeing-designed airplanes. Boeing and the FAA are issuing similar documents for all models of the DC-10. air seal, fairing, and the aft frame; MODIFICATION OF THE THRUST a proposed AD for the indication reverser. This allows operators to stock and checks of the feedback rod-to-yoke 2 system on all models of the DC-10. neutral spare reversers and quickly The safety enhancement program REVERSER INDICATION SYSTEM oeing has initiated a four- alignment, translating cowl auto- An AD mandating the incorporation of configure them for any engine position. phased safety enhancement for the DC-10 is designed to improve restow function, position indication The second phase of the DC-10 safety B enhancement program involves modify- Boeing Service Bulletin DC10-78-060 The basic design elements of the program for thrust reverser the reliability of the thrust reverser for the overpressure shutoff valve, is expected by the end of 2000. -
The Solid Rocket Booster Auxiliary Power Unit - Meeting the Challenge
THE SOLID ROCKET BOOSTER AUXILIARY POWER UNIT - MEETING THE CHALLENGE Robert W. Hughes Structures and Propulsion Laboratory Marshall Space Flight Center, Alabama ABSTRACT The thrust vector control systems of the solid rocket boosters are turbine-powered, electrically controlled hydraulic systems which function through hydraulic actuators to gimbal the nozzles of the solid rocket boosters and provide vehicle steering for the Space Shuttle. Turbine power for the thrust vector control systems is provided through hydrazine fueled auxiliary power units which drive the hydraulic pumps. The solid rocket booster auxiliary power unit resulted from trade studies which indicated sig nificant advantages would result if an existing engine could be found to meet the program goal of 20 missions reusability and adapted to meet the seawater environments associated with ocean landings. During its maturation, the auxiliary power unit underwent many design iterations and provided its flight worthiness through full qualification programs both as a component and as part of the thrust vector control system. More significant, the auxiliary power unit has successfully completed six Shuttle missions. THE SOLID ROCKET BOOSTER CHALLENGE The challenge associated with the development of the Solid Rocket Booster (SRB) Auxiliary Power Unit (APU) was to develop a low cost reusable APU, compatible with an "operational" SRB. This challenge, as conceived, was to be one of adaptation more than innovation. As it turned out, the SRB APU development had elements of both. During the technical t~ade studies to select a SRB thrust vector control (TVC) system, several alternatives for providing hydraulic power were evaluated. A key factor in the choice of the final TVC system was the Orbiter APU development program, then in progress at Sundstrand Aviation. -
Thrust and Power Available, Maximum and Minimum Cruise Velocity, Effects of Altitude on Power Thrust Available
Module-2 Lecture-7 Cruise Flight - Thrust and Power available, Maximum and minimum cruise velocity, Effects of altitude on power Thrust available • As we have seen earlier, thrust and power requirements are dictated by the aero- dynamic characteristics and weight of the airplane. In contrast, thrust and power available are strictly associated with the engine of the aircraft. • The thrust delivered by typical reciprocating piston engines used in aircraft with propellers varies with velocity as shown in Figure 1(a). • It should be noted that the thrust at zero velocity (static thrust) is maximum and it decreases with increase in forward velocity. The reason for this behavior is that the blade tip of the propellers encounter compressibility problems leading to abrupt decrease in the available thrust near speed of sound. • However, as seen from Figure 1(b), the thrust delivered by a turbojet engine stays relatively constant with increase in velocity. Figure 1: Variation in available thrust with velocity of the (a) reciprocating engine- propeller powered aircraft and (b) turbojet engine powered aircraft 1 Power Power required for any aircraft is a characteristic of the aerodynamic design and weight of that aircraft. However, the power available, PA is a characteristic of the power plant (engine) of the aircraft. Typically, a piston engine generates power by burning fuel in the cylinders and then using this energy to move pistons in a reciprocating fashion (Figure 2). The power delivered to the piston driven propeller engine by the crankshaft is termed Figure 2: Schematic of a reciprocating engine as the shaft brake power P . -
Advisory Circular
Advisory U.S. Department of Transportation Circular Federal Aviation Administration Subject: RATINGS AND OPERATING Date: 6/28/10 AC No: 33.7-1 LIMITATIONS FOR TURBINE ENGINES Initiated by: ANE-111 (SECTIONS 33.7 AND 33.8) 1. Purpose. This advisory circular (AC) provides information and guidance on turbine engine compliance under part 33 of Title 14 of the Code of Federal Regulations (14 CFR), specifically §§ 33.7, Engine ratings and operating limitations, and 33.8, Selection of engine power and thrust ratings. This AC also provides information on preparing the data needed for the type certification data sheet (TCDS) specified in § 33.7(a). 2. Applicability. a. The guidance provided in this document is directed to applicants requesting certification of turbine engines, except that no specific guidance is provided for the augmented power or thrust (refer to § 33.7, paragraphs (c)(1)(i) and (iii)) and supersonic engines. For the purpose of this AC, any reference to power or thrust is for unaugmented power or thrust (refer to § 33.7, paragraphs (c)(1)(ii) and (iv)). b. This material is neither mandatory nor regulatory in nature and does not constitute a regulation. It describes acceptable means, but not the only means, for demonstrating compliance with the applicable regulations. The FAA will consider other methods of demonstrating compliance that an applicant may elect to present. Terms such as “should,” “shall,” “may,” and “must” are used only in the sense of ensuring applicability of this particular method of compliance when the acceptable method of compliance in this document is used. While these guidelines are not mandatory, they are derived from extensive FAA and industry experience in determining compliance with the relevant regulations. -
Study of a Crew Transfer Vehicle Using Aerocapture for Cycler Based Exploration of Mars by Larissa Balestrero Machado a Thesis S
Study of a Crew Transfer Vehicle Using Aerocapture for Cycler Based Exploration of Mars by Larissa Balestrero Machado A thesis submitted to the College of Engineering and Science of Florida Institute of Technology in partial fulfillment of the requirements for the degree of Master of Science in Aerospace Engineering Melbourne, Florida May, 2019 © Copyright 2019 Larissa Balestrero Machado. All Rights Reserved The author grants permission to make single copies ____________________ We the undersigned committee hereby approve the attached thesis, “Study of a Crew Transfer Vehicle Using Aerocapture for Cycler Based Exploration of Mars,” by Larissa Balestrero Machado. _________________________________________________ Markus Wilde, PhD Assistant Professor Department of Aerospace, Physics and Space Sciences _________________________________________________ Andrew Aldrin, PhD Associate Professor School of Arts and Communication _________________________________________________ Brian Kaplinger, PhD Assistant Professor Department of Aerospace, Physics and Space Sciences _________________________________________________ Daniel Batcheldor Professor and Head Department of Aerospace, Physics and Space Sciences Abstract Title: Study of a Crew Transfer Vehicle Using Aerocapture for Cycler Based Exploration of Mars Author: Larissa Balestrero Machado Advisor: Markus Wilde, PhD This thesis presents the results of a conceptual design and aerocapture analysis for a Crew Transfer Vehicle (CTV) designed to carry humans between Earth or Mars and a spacecraft on an Earth-Mars cycler trajectory. The thesis outlines a parametric design model for the Crew Transfer Vehicle and presents concepts for the integration of aerocapture maneuvers within a sustainable cycler architecture. The parametric design study is focused on reducing propellant demand and thus the overall mass of the system and cost of the mission. This is accomplished by using a combination of propulsive and aerodynamic braking for insertion into a low Mars orbit and into a low Earth orbit. -
An Optiomal APU for Passenger Aircraft
AIRCRAFT DESIGN AND SYSTEMS GROUP (AERO) An Optiomal APU for Passenger Aircraft Dieter Scholz Hamburg University of Applied Sciences Based on the two project reports of Independent Study. Johan Peterson and Tom Alisch No Funding. 5th CEAS Air and Space Conference 2015 Delft, 07.-11. September 2015 An Optional APU for Passenger Aircraft Content . Introduction . APU Description . APU History . APU Operation . APU – Stakeholder Views . APU Characteristics . Potential Savings without an APU . APU Alternatives . Summary and Conclusions Dieter Scholz 5th CEAS Air and Space Conference 2015 07.09.2015, Slide 2 An Optional APU For Passenger Aircraft Delft, 07.-11. September 2015 Aircraft Design and Systems Group (AERO) Introduction Proposal . Offer the APU only as an option. Aircraft prepared for possible addition of the APU later in the life of the aircraft. Research Hypothesis . An aircraft type with an optional APU (with the option not selected when the aircraft is ordered) has economical and ecological advantages in operation compared to an aircraft not offering an opt-out from the APU. Simple Argument for the Benefits of the Proposal . Omitting the APU all together saves mass (fuel, emissions) and costs (maintenance costs, purchase costs and depreciation) Heuristic (mental shortcut) and Warning . If saving money would be so easy, the aircraft without APU would have been considered already and would be on offer. There must be some economical disadvantage not having an APU! Dieter Scholz 5th CEAS Air and Space Conference 2015 07.09.2015, Slide 3 An Optional APU For Passenger Aircraft Delft, 07.-11. September 2015 Aircraft Design and Systems Group (AERO) Introduction Definition (AGARD): Dieter Scholz 5th CEAS Air and Space Conference 2015 07.09.2015, Slide 4 An Optional APU For Passenger Aircraft Delft, 07.-11.