Power, Propulsion, and Thermal Preliminary Design Review James Black Matt Marcus Grant McLaughlin Michelle Sultzman
|
|
- Lindsey Underwood
- 5 years ago
- Views:
Transcription
1 Power, Propulsion, and Thermal Preliminary Design Review James Black Matt Marcus Grant McLaughlin Michelle Sultzman
2 Outline 1. Crew Systems Design Selection 2. Thermal Requirements and Design 3. Power Requirements and Design 4. Reaction Control System Design 2
3 Crew Systems Design Selection Selection dictated by placement requirements for thrusters and propellant tanks o o o Able to place thrusters around center of mass plane Crew Systems capsule modified to expand lower cavity between pressure vessel and hull to hold propulsion system New pressure vessel removes unused pressurized space, minimizing impact on crew systems layout Old Pressure Vessel (in green) New pressure vessel (in green) 3
4 Thermal Control System Requirements Must maintain cabin temperature in following cases: o o o o o Full sun (Translunar) Eclipse (LEO/LLO) Lunar surface - Dawn/Dusk/Polar Lunar surface - 45 Sun Angle Lunar surface - Noon Equatorial 4
5 Thermal Control System NASA requirement: Crew cabin temperature within range of 292 K to 300 K Simple heat exchanger between cabin air and fluid that circulates through external radiator o Reduces heat generation from refrigeration cycle o Limits radiator temperature to approximately cabin temperature Assuming all radiative surfaces coated with white paint o α= 0.2 o ε = 0.8 5
6 Multi-Layer Insulation Surface area of craft covered with multi-layer insulation determined by considering case of thermal equilibrium during eclipse T rad = Q int ε σ A tot + T env Q int = 1445 W, T env = 4 K A radiator = A total = 25 m 2 : K A radiator = 6 m 2 : K A radiator = 4.25 m 2 : K 6
7 Multi-Layer Insulation During eclipse: o Designing the craft to have an equilibrium temperature within acceptable range solely through use of insulation left too small of an area to effectively radiate heat during other phases of the mission o Instead craft will have an equilibrium temperature of 270 K, and will use a 500 W space heater to increase temperature of pressure vessel Final design: 19 m 2 of total surface area of 25 m 2 will be covered with MLI 7
8 Radiators Considered Additional radiators were necessary Initially considered radiators deployed like flower petals at the top of the cone o This design did not yield enough surface area for all thermal profiles 8
9 Radiators Selected Three double-sided circular radiator arrays, 8.44 m 2 on each side Radiator arrays, along with solar array of the same size (to be discussed later) will be folded out from the heat shield before docking with orbital propulsion module o Each array spaced 90 apart o Arrays not obstructing ingress/egress Each radiator contains two channels of coolant which can be turned on and off independently, allowing number of radiators used to vary in increments of 0.5 9
10 Radiator Array Configuration Radiator Solar Array Radiator Radiator 10
11 Radiators Radiators can rotate axially in order to have highest temperature control resolution possible Thermal equilibrium calculations were performed assuming radiator panels were oriented perpendicular to lunar surface o Rotating panels slightly will alter illuminated area of craft, and therefore increase or decrease equilibrium temperature for more precise thermal control 11
12 Thermal Equilibrium Calculations Assumed that all radiated heat from spacecraft is radiating directly into space Assumed that panels perpendicular to lunar surface will radiate from both sides o o 65% of heat will radiate into space 35% of heat will radiate toward Lunar surface Illuminated area changes with solar angle Internally generated heat comprised of power requirements of different systems at each phase and 116 W heat load per crew member (based on average 2400 kcal daily diet) 12
13 Spacecraft Thermal Control Cases Case Q int (W)* Illuminated Area (m 2 ) T env (K) Number of active panels T rad (K) Eclipse (space) Full Sun (space) Lunar Surface Dawn/Dusk/ Polar Lunar Surface - 45deg Solar Angle Lunar Equatorial Noon (space) 180 (moon) (space) 215 (moon) (space) 380 (moon) * Values presented on next slide 13
14 Mission Phase Power Requirements RCS (W) Life Support (W) Avionics (W) Lighting (W) Thermal (W) Total (W) LEO checkout Cis-Lunar Space LLO Loiter Lunar D/A Lunar Surface Ops Earth EDL W average, 1200 W Peak 14
15 Power Generation Power Systems Investigated o o o Lithium Ion Battery Powered LOX/LH2 Fuel Cell Solar Panels with rechargeable Lithium Ion Battery o Solar panels not active during launch, entry, eclipse Trade Study performed on total mass of each system for mission duration 15
16 Power Generation System Mass Trade Study 16
17 Power System Sizes Solar Panels/ Li-Ion Battery Solar Array: 8.44 m 2 Battery: 0.01 m 3, 10 kg Apollo Fuel Cell LOX tank: 0.08 m 3 LH2 tank: m 3 Fuel cell: 0.16 m 3
18 Power System Design Choice Solar Panel and Battery System chosen o o Smaller mass than fuel cell Battery large enough to power during phases when solar panels do not produce power 18
19 Propulsion Requirements Translational delta-v of 50 m/s Attitude hold in +/- 5 degree deadband for 3 days for return to earth Overcome 500 Nm pitch and yaw moments during ~3 minute reentry Rotate Spacecraft 10 times 180 degrees in <30 sec 19
20 Coordinate System +X +X +Z +Y 20
21 Moments of Inertia Assuming a hollow cone with wall thickness of 1/3 of the maximum radius o r = m o h = m o m = 4795 kg Moments are CCW about axis Ix = 1/6*m*r 2 = 2140 [kg*m 2 ] Iy = Iz = 1/3*m*(r 2 /4+h 2 ) = [kg*m 2 ] 21
22 Translational Propulsion Rocket Equation : V f -V i = I sp *g*exp(m i /M f ) I sp ~300 sec M i = 4795 kg M f = 4795-(Propellent Mass) Delta v = 50 m/s Account for thrusters firing at 50 degree angle from vertical for +x translation Propellent Mass = 125 kg 22
23 Translational Propulsion Maneuvers +X Front View Side View 23
24 Translational Propulsion Maneuvers -X Front View Side View 24
25 Translational Propulsion Maneuvers +Y, -Y Top View Front View 25
26 Translational Propulsion Maneuvers +Z, -Z Top View Side View 26
27 Rotational Propulsion Maneuvers: Roll roll about +X, -X Top View 27
28 Rotational Propulsion Maneuvers: Yaw Top View Left Side View Yaw about +Z, -Z Front View Right Side View 28
29 Rotational Propulsion Maneuvers: Pitch Top View Left Side View Pitch about +Y, -Y Front View Right Side View 29
30 Thrust Requirements: Pitch, Yaw The placement of the thrusters was determined from the constraint of the largest necessary moment for control: pitch and yaw Maximum aerodynamic moment for yaw and pitch: 500 Nm Assuming some control over the location of the center of gravity (CG), it is best to have the thrusters in the xy-plane at about 3/4 from the top 30
31 Thrust Requirements: Pitch and Yaw In atmospheric entry, translation forces do not need to be balanced Overcome 500 Nm pitch and yaw moments Two thrusters firing in the +x direction Thruster per Draco: 250 N Moment arm: 1.0 m F=mu m = 400 N 300s 9.81 m s 2 = kg/s Fraction of time burning: T f = 500/(800*1) Mass of propellent = T f *180* m *2 = kg 31
32 Thrust Requirements: Roll 1 2 τ I t2 + θ ot = θ θ o Assume angular rate = t=0 and t=30 Need equivalent of -30 Nm for 15 sec and 30 Nm for 15 sec Thrust of N per thruster (for perfectly coupled torque) Performed by two 400N Draco thrusters for 1.65 sec at 100% duty cycle 32
33 Attitude Trajectories Trajectories for various torques with initial angle and angular rate offsets Able to stay within 5 degree deadband with -75 Nm torque Well within limits of attitude control system 33
34 Thrust Requirements: Deadband Pitch and yaw performed by: o One thruster in the -x direction; arm = 1.4 m; thrust = 26.8 N o Two thrusters in the +x direction; arm 1 m; thrust = 18.8 N Voyager 1 and 2 have used only 50 kg of propellent since 1977 to maintain deadband 5 degree half deadband width = rad Fuel consumption decreases with increasing deadband width as shown above Can assume propellent used is very small for 3 days - on the order of 1 kg 34
35 Thruster Selection SpaceX Draco thrusters were selection: Similar mission design requirements Thrusters are flush with outer shell 400 N thrust covers all requirements 300 sec Isp Operates at different duty cycles for each reaction control objective Maneuver Thrust Duty Cycle Draco Thruster duty cycle = thrust time thrust time + drift time Pitch 250 N 63% Yaw 250 N 63% Roll 27 N/ 19 N 6.7%/4.9% Deadband 11 N 2.7% 35
36 Propellent Draco Thrusters: 300 sec Isp, 400 N thrust Nitrogen Textroxide (1.443 g/cm 3 ) ; Monomethylhydrozine (.875 g/cm 3 ) Both liquids 20 C Maneuver Propellent Mass (kg) Oxidizer Mass (kg) Fuel Mass (kg) 50 m/s delta v in x direction Deadband attitude hold for 3 days 500 Nm pitch and yaw moments 180 degree roll in <30 sec; 10 times ~1 kg ~.7 ~ kg Total
37 Fuel and Oxidizer tanks Mass of tank = 299.8*(vol. m 3 ) + 2 Assume 2 mm thickness for tanks Fuel and Oxidizer stored as liquids at 20 C Oxidizer Tank empty Mass (kg) Fuel Tank empty Mass (kg) Oxidizer Tank inner Volume (m 3 ) Fuel Tank inner Volume (m 3 )
38 References Akin, David et Al. Minimum Functionality Lunar Habitation Element. University of Maryland Space Systems Laboratory Print. Akin, David. (2012) Rocket Propulsion [PDF]. Retrieved from Akin, David. (2012) Power Systems Design [PDF]. Retrieved from Akin, David. (2012) Thermal Analysis and Design [PDF]. Retrieved from Allen, Christopher et Al. Guidelines and Capabilities for Designing Human Missions. TM NASA JSC, Print. Dragon Overview. SpaceX. Website < Foley, John. Control of a Spacecraft Using a Reaction Control System. < Gilmore, D.G. Spacecraft Thermal Control Handbook. AIAA
39 References Liquid Rocket Propellants. Website < Solo lunar flyby using standard Falcon 9 and Dragon. Forum post. 18 Dec < Typical Onboard Systems. Basics of Space Flight: Section II. Jet Propulsion Laboratory. Website < Thruster Mass Estimation. Delft University of Technology. Website < Washay, Marvin, Prokopius, Paul R. The Fuel Cell in Space: Yesterday, Today and Tomorrow. TM London: NASA, Print. 39
ENAE483: Principles of Space System Design Power Propulsion Thermal System
Power Propulsion Thermal System Team B4: Ben Abresch Jason Burr Kevin Lee Scott Wingate November 8th, 2012 Presentation Overview Mission Guidelines Project Specifications Initial Design Power Thermal Insulation
More informationPower, Propulsion and Thermal Design Project. Jesse Cummings Shimon Gewirtz Siddharth Parachuru Dennis Sanchez Alexander Slafkosky
Power, Propulsion and Thermal Design Project Jesse Cummings Shimon Gewirtz Siddharth Parachuru Dennis Sanchez Alexander Slafkosky Mission Itinerary Days 1-3: Voyage to moon Days 4-7: On the lunar surface
More informationPower, Propulsion and Thermal Design Project ENAE483 Fall 2012
Power, Propulsion and Thermal Design Project ENAE483 Fall 2012 Team B8: Josh Sloane Matt Rich Rajesh Yalamanchili Kiran Patel Introduction This project is an extension of Team A2's Crew Systems Project
More informationPPT Design Project. ENAE483 November 8, 2010 Stef Bilyk, Kip Hart, John Pino, Tim Russell
PPT Design Project ENAE483 November 8, 2010 Stef Bilyk, Kip Hart, John Pino, Tim Russell Project Overview 1) Design the power system, reaction control system, and perform the thermal equilibrium calculations
More informationENAE 483: Principles of Space System Design Loads, Structures, and Mechanisms
ENAE 483: Principles of Space System Design Loads, Structures, and Mechanisms Team: Vera Klimchenko Kevin Lee Kenneth Murphy Brendan Smyth October 29 th, 2012 Presentation Overview Project Overview Mission
More informationBravoSat: Optimizing the Delta-V Capability of a CubeSat Mission. with Novel Plasma Propulsion Technology ISSC 2013
BravoSat: Optimizing the Delta-V Capability of a CubeSat Mission with Novel Plasma Propulsion Technology Sara Spangelo, NASA JPL, Caltech Benjamin Longmier, University of Michigan Interplanetary Small
More informationMass Estimating Relationships MARYLAND. Review of iterative design approach Mass Estimating Relationships (MERs) Sample vehicle design analysis
Mass Estimating Relationships Review of iterative design approach Mass Estimating Relationships (MERs) Sample vehicle design analysis 2006 David L. Akin - All rights reserved http://spacecraft.ssl.umd.edu
More informationSOLAR ROCKET PROPULSION Ground and Space Technology Demonstration. Dr. Michael Holmes, AFRL/PRSS
SOLAR ROCKET PROPULSION Ground and Space Technology Demonstration Dr. Michael Holmes, AFRL/PRSS Solar Thermal Propulsion Concept Parabolic Mirror Sun Create thrust by collecting and focusing sunlight to
More information11.1 Survey of Spacecraft Propulsion Systems
11.1 Survey of Spacecraft Propulsion Systems 11.1 Survey of Spacecraft Propulsion Systems In the progressing Space Age, spacecrafts such as satellites and space probes are the key to space exploration,
More information1. (a) Describe the difference between over-expanded, under-expanded and ideallyexpanded
Code No: R05322106 Set No. 1 1. (a) Describe the difference between over-expanded, under-expanded and ideallyexpanded rocket nozzles. (b) While on its way into orbit a space shuttle with an initial mass
More informationDesign of Attitude Determination and Control Subsystem
Design of Attitude Determination and Control Subsystem 1) Control Modes and Requirements Control Modes: Control Modes Explanation 1 ) Spin-Up Mode - Acquisition of Stability through spin-up maneuver -
More informationENAE 483/788D FINAL EXAMINATION FALL, 2015
ENAE 48/788D FINAL EXAMINATION FALL, 2015 No phones, computers, or internet-enabled devices. Use the spaces following the questions to write your answers; you can also use the backs of the pages as necessary,
More informationThermal Systems Design
Thermal Systems Design Fundamentals of heat transfer Radiative equilibrium Surface properties Non-ideal effects Internal power generation Environmental temperatures Conduction Thermal system components
More informationSolar Thermal Propulsion
AM A A A01-414 AIAA 2001-77 Solar Thermal Propulsion SOLAR THERMAL PROPULSION FOR AN INTERSTELLAR PROBE Ronald W. Lyman, Mark E. Ewing, Ramesh S. Krishnan, Dean M. Lester, Thiokol Propulsion Brigham City,
More informationElectrically Propelled Cargo Spacecraft for Sustained Lunar Supply Operations
42nd AIAA/ASME/SAE/ASEE Joint Propulsion Conference & Exhibit 9-12 July 2006, Sacramento, California AIAA 2006-4435 Electrically Propelled Cargo Spacecraft for Sustained Lunar Supply Operations Christian
More informationA little more about costing Review of iterative design approach Mass Estimating Relationships (MERs) Sample vehicle design analysis
A little more about costing Review of iterative design approach (MERs) Sample vehicle design analysis 2004 David L. Akin - All rights reserved http://spacecraft.ssl. umd.edu Internal Rate of Return Discount
More informationParametric Design MARYLAND. The Design Process Regression Analysis Level I Design Example: Project Diana U N I V E R S I T Y O F.
Parametric Design The Design Process Regression Analysis Level I Design Example: U N I V E R S I T Y O F MARYLAND 2003 David L. Akin - All rights reserved http://spacecraft.ssl.umd.edu Parametric Design
More informationMARYLAND. The Design Process Regression Analysis Level I Design Example: UMd Exploration Initiative U N I V E R S I T Y O F.
Parametric Design The Design Process Regression Analysis Level I Design Example: UMd Exploration Initiative U N I V E R S I T Y O F MARYLAND 2004 David L. Akin - All rights reserved http://spacecraft.ssl.
More informationEnd of Life Re-orbiting The Meteosat-5 Experience
End of Life Re-orbiting The Meteosat-5 Experience Milan EUMETSAT, Darmstadt, Germany This article illustrates the orbit maneuver sequence performed during Meteosat- 5 End of Life (EOL) re-orbiting operations
More informationGeneration X. Attitude Control Systems (ACS) Aprille Ericsson Dave Olney Josephine San. July 27, 2000
Generation X Attitude Control Systems (ACS) Aprille Ericsson Dave Olney Josephine San July 27, 2000 ACS Overview Requirements Assumptions Disturbance Torque Assessment Component and Control Mode Recommendations
More informationGeneral Remarks and Instructions
Delft University of Technology Faculty of Aerospace Engineering 1 st Year Examination: AE1201 Aerospace Design and System Engineering Elements I Date: 25 August 2010, Time: 9.00, Duration: 3 hrs. General
More informationSPACE SHUTTLE ROLL MANEUVER
SPACE SHUTTLE ROLL MANEUVER Instructional Objectives Students will analyze space shuttle schematics and data to: demonstrate graph and schematic interpretation skills; apply integration techniques to evaluate
More informationFacts Largest Moon of Saturn. Has an atmosphere containing mostly Nitrogen and methane. 1 gram on Earth would weigh 0.14g on Titan. Only know moon in
Titan Martin E Facts Largest Moon of Saturn. Has an atmosphere containing mostly Nitrogen and methane. 1 gram on Earth would weigh 0.14g on Titan. Only know moon in our solar system to have a dense atmosphere.
More informationPreliminary Design Review: Loads, Structures, and Mechanisms. Michael Cunningham, Shimon Gewirtz, Rajesh Yalamanchili, Thomas Noyes
Preliminary Design Review: Loads, Structures, and Mechanisms Michael Cunningham, Shimon Gewirtz, Rajesh Yalamanchili, Thomas Noyes Crew Cabin Structure Height of ~3.7m from heat shield to top of the cone
More informationMission Analysis of Sample Return from Jovian Trojan Asteroid by Solar Power Sail
Trans. JSASS Aerospace Tech. Japan Vol. 12, No. ists29, pp. Pk_43-Pk_50, 2014 Original Paper Mission Analysis of Sample Return from Jovian Trojan Asteroid by Solar Power Sail By Jun MATSUMOTO 1), Ryu FUNASE
More informationShen Ge ECAPS LLC. Yvonne Vigue-Rodi Adelante Sciences Corporation May 6, 2016 AIAA Houston Annual Technical Symposium
Feasibility of Transferring On-Orbit Components of the International Space Station for Solar System Exploration Shen Ge ECAPS LLC Yvonne Vigue-Rodi Adelante Sciences Corporation May 6, 2016 AIAA Houston
More informationLow-Energy Return from Europa
Low-Energy Return from Europa 176 days duration. 4 minutes total engine use time. Whenever necessary, the radiation shield magnetic field generators should be set to 100%. Start Orbit5S Load file Europa
More informationMission Design Options for Solar-C Plan-A
Solar-C Science Definition Meeting Nov. 18, 2008, ISAS Mission Design Options for Solar-C Plan-A Y. Kawakatsu (JAXA) M. Morimoto (JAXA) J. A. Atchison (Cornell U.) J. Kawaguchi (JAXA) 1 Introduction 2
More informationSELENE TRANSLUNAR TRAJECTORY AND LUNAR ORBIT INJECTION
SELENE TRANSLUNAR TRAJECTORY AND LUNAR ORBIT INJECTION Yasuihiro Kawakatsu (*1) Ken Nakajima (*2), Masahiro Ogasawara (*3), Yutaka Kaneko (*1), Yoshisada Takizawa (*1) (*1) National Space Development Agency
More informationSmall Satellite Aerocapture for Increased Mass Delivered to Venus and Beyond
Small Satellite Aerocapture for Increased Mass Delivered to Venus and Beyond Adam Nelessen / Alex Austin / Joshua Ravich / Bill Strauss NASA Jet Propulsion Laboratory Ethiraj Venkatapathy / Robin Beck
More informationIV. Rocket Propulsion Systems. A. Overview
IV. Rocket Propulsion Systems A. Overview by J. M. Seitzman for AE 4451 Jet and Rocket Propulsion Seitzman Rocket Overview-1 Rocket Definition Rocket Device that provides thrust to a vehicle by accelerating
More informationPropulsion Systems Design MARYLAND. Rocket engine basics Survey of the technologies Propellant feed systems Propulsion systems design
Propulsion Systems Design Rocket engine basics Survey of the technologies Propellant feed systems Propulsion systems design 2008 David L. Akin - All rights reserved http://spacecraft.ssl.umd.edu 1 Propulsion
More informationOrbit Design Marcelo Suárez. 6th Science Meeting; Seattle, WA, USA July 2010
Orbit Design Marcelo Suárez Orbit Design Requirements The following Science Requirements provided drivers for Orbit Design: Global Coverage: the entire extent (100%) of the ice-free ocean surface to at
More informationTHE TRAJECTORY CONTROL STRATEGIES FOR AKATSUKI RE-INSERTION INTO THE VENUS ORBIT
THE TRAJECTORY CONTROL STRATEGIES FOR AKATSUKI RE-INSERTION INTO THE VENUS ORBIT Chikako Hirose (), Nobuaki Ishii (), Yasuhiro Kawakatsu (), Chiaki Ukai (), and Hiroshi Terada () () JAXA, 3-- Yoshinodai
More informationNAVIGATION & MISSION DESIGN BRANCH
c o d e 5 9 5 National Aeronautics and Space Administration Michael Mesarch Michael.A.Mesarch@nasa.gov NAVIGATION & MISSION DESIGN BRANCH www.nasa.gov Outline Orbital Elements Orbital Precession Differential
More informationPreliminary Development of an Experimental Lightweight Pulsed Plasma Thruster for Solar Sail Attitude Control
Preliminary Development of an Experimental Lightweight Pulsed Plasma Thruster for Solar Sail Attitude Control Kevin Pryor, Bong Wie, and Pavlos Mikellides Arizona State University 18 th Annual AIAA/USU
More informationThe Interstellar Boundary Explorer (IBEX) Mission Design: A Pegasus Class Mission to a High Energy Orbit
The Interstellar Boundary Explorer (IBEX) Mission Design: A Pegasus Class Mission to a High Energy Orbit Ryan Tyler, D.J. McComas, Howard Runge, John Scherrer, Mark Tapley 1 IBEX Science Requirements IBEX
More informationRocket Propulsion Overview
Rocket Propulsion Overview Seitzman Rocket Overview-1 Rocket Definition Rocket Device that provides thrust to a vehicle by accelerating some matter (the propellant) and exhausting it from the rocket Most
More informationInSight Spacecraft Launch for Mission to Interior of Mars
InSight Spacecraft Launch for Mission to Interior of Mars InSight is a robotic scientific explorer to investigate the deep interior of Mars set to launch May 5, 2018. It is scheduled to land on Mars November
More informationA Study of CPS Stages for Missions beyond LEO Final Distribution
A Study of CPS Stages for Missions beyond LEO Final Distribution 31 May 2012 Atlanta, GA Mark Schaffer Senior Aerospace Engineer, Advanced Concepts Group mark.schaffer@sei.aero 1+770.379.8013 1 Introduction
More informationThe Design Process Level I Design Example: Low-Cost Lunar Exploration Amplification on Initial Concept Review
Parametric Design The Design Process Level I Design Example: Low-Cost Lunar Exploration Amplification on Initial Concept Review U N I V E R S I T Y O F MARYLAND 2008 David L. Akin - All rights reserved
More informationMIKE HAWES VICE PRESIDENT & ORION PROGRAM MANAGER
MIKE HAWES VICE PRESIDENT & ORION PROGRAM MANAGER NASA S EXPLORATION SYSTEM EXPLORATION DESTINATIONS 100s of Miles 1,000s of Miles 10,000s of Miles 100,000s of Miles 1,000,000s of Miles 10,000,000s of
More informationSmall Satellite Aerocapture for Increased Mass Delivered to Venus and Beyond
Small Satellite Aerocapture for Increased Mass Delivered to Venus and Beyond Adam Nelessen / Alex Austin / Joshua Ravich / Bill Strauss NASA Jet Propulsion Laboratory Ethiraj Venkatapathy / Robin Beck
More informationATTITUDE CONTROL MECHANIZATION TO DE-ORBIT SATELLITES USING SOLAR SAILS
IAA-AAS-DyCoSS2-14-07-02 ATTITUDE CONTROL MECHANIZATION TO DE-ORBIT SATELLITES USING SOLAR SAILS Ozan Tekinalp, * Omer Atas INTRODUCTION Utilization of solar sails for the de-orbiting of satellites is
More informationPRELIMINAJ3.:( 6/8/92 SOFTWARE REQUIREMENTS SPECIFICATION FOR THE DSPSE GUIDANCE, NAVIGATION, AND CONTROL CSCI. Prepared by
PRELIMINAJ3.:( SOFTWARE REQUIREMENTS SPECIFICATION FOR THE DSPSE GUIDANCE, NAVIGATION, AND CONTROL CSCI Prepared by Space Applications Corporation 6/8/92.. 1 SCOPE 1.1 IDENTIFICATION 1.2 OVERVIEW This
More informationParametric Design MARYLAND. The Design Process Level I Design Example: Low-Cost Lunar Exploration U N I V E R S I T Y O F
Parametric Design The Design Process Level I Design Example: Low-Cost Lunar Exploration U N I V E R S I T Y O F MARYLAND 2005 David L. Akin - All rights reserved http://spacecraft.ssl.umd.edu Parametric
More informationProject of Lithuanian Nano-Satellite
Project of Lithuanian Nano-Satellite Domantas BRUČAS 1), Vidmantas TOMKUS 2), Romualdas Zykus 2), Raimundas Bastys 2) 1) Department of Aviation Mechanics, Vilnius Gediminas Technical University/Space Science
More informationIAC-13,C4,P,44.p1,x17254 THE DYNAMIC OPERATON OF A HIGH Q EMDRIVE MICROWAVE THRUSTER. Roger Shawyer C.Eng. MIET. FRAeS. SPR Ltd UK
IAC-13,C4,P,44.p1,x1754 THE DYNAMIC OPERATON OF A HIGH Q EMDRIVE MICROWAVE THRUSTER Roger Shawyer C.Eng. MIET. FRAeS SPR Ltd UK sprltd@emdrive.com ABSTRACT The static operation of an EmDrive microwave
More informationASTOS for Low Thrust Mission Analysis
ASTOS for Low Thrust Mission Analysis 3rd Astrodynamics Workshop, Oct. 26, ESTEC Overview Low Thrust Trajectory Computation Description of the Optimal Control Problem Trajectory Optimization and Mission
More informationDevelopment of Microwave Engine
Development of Microwave Engine IEPC-01-224 Shin SATORI*, Hiroyuki OKAMOTO**, Ted Mitsuteru SUGIKI**, Yoshinori AOKI #, Atsushi NAGATA #, Yasumasa ITO** and Takayoshi KIZAKI # * Hokkaido Institute of Technology
More informationA Notional Round Trip To The Trans-Lunar Libration Point (EML2)
Many specialists in the astrodynamics field are currently studying trajectories between Earth and the trans-lunar libration point (EML2). Located about 60,000 km beyond the Moon from Earth, EML2 is a strategic
More informationThermal Systems Design MARYLAND. Fundamentals of heat transfer Radiative equilibrium Surface properties Non-ideal effects
Thermal Systems Design Fundamentals of heat transfer Radiative equilibrium Surface properties Non-ideal effects Internal power generation Environmental temperatures Conduction Thermal system components
More informationUNIT HW ROTATION ANSWER KEY
Conceptual Questions UNIT HW ROTATION ANSWER KEY 1) D_What type of linear acceleration does an object moving with constant linear speed (st) in a circular path experience? A) free fall C) linear acceleration
More informationPropulsion Systems Design
Propulsion Systems Design Rocket engine basics Survey of the technologies Propellant feed systems Propulsion systems design 1 2016 David L. Akin - All rights reserved http://spacecraft.ssl.umd.edu Liquid
More informationCongreve Rockets This rockets were invented by Englishman, Sir William Congreve. Congreve successfully demonstrated a solid fuel rocket in 1805, and
Congreve Rockets This rockets were invented by Englishman, Sir William Congreve. Congreve successfully demonstrated a solid fuel rocket in 1805, and the following year his rockets were used in action for
More informationDARE Mission and Spacecraft Overview
DARE Mission and Spacecraft Overview October 6, 2010 Lisa Hardaway, PhD Mike Weiss, Scott Mitchell, Susan Borutzki, John Iacometti, Grant Helling The information contained herein is the private property
More informationTechnology of Rocket
Technology of Rocket Parts of Rocket There are four major parts of rocket Structural system Propulsion system Guidance system Payload system Structural system The structural system of a rocket includes
More informationQuadrotor Modeling and Control
16-311 Introduction to Robotics Guest Lecture on Aerial Robotics Quadrotor Modeling and Control Nathan Michael February 05, 2014 Lecture Outline Modeling: Dynamic model from first principles Propeller
More informationBifrost: A 4 th Generation Launch Architecture Concept
Bifrost: A 4 th Generation Launch Architecture Concept Rohrschneider, R.R., Young, D., St.Germain, B., Brown, N., Crowley, J., Maatsch, J., Olds, J.R. (Advisor) Abstract Space Systems Design Lab School
More informationDesign And Analysis Of Thrust Chamber Of A Cryogenic Rocket Engine S. Senthilkumar 1, Dr. P. Maniiarasan 2,Christy Oomman Jacob 2, T.
Design And Analysis Of Thrust Chamber Of A Cryogenic Rocket Engine S. Senthilkumar 1, Dr. P. Maniiarasan 2,Christy Oomman Jacob 2, T. Vinitha 2 1 Research Scholar, Department of Mechanical Engineering,
More informationIMPACT OF SPACE DEBRIS MITIGATION REQUIREMENTS ON THE MISSION DESIGN OF ESA SPACECRAFT
IMPACT OF SPACE DEBRIS MITIGATION REQUIREMENTS ON THE MISSION DESIGN OF ESA SPACECRAFT Rüdiger Jehn (1), Florian Renk (1) (1 ) European Space Operations Centre, Robert-Bosch-Str. 5, 64293 Darmstadt, Germany,
More informationAndrea Sainati, Anupam Parihar, Stephen Kwan Seklam 31 A Very Low Altitude Constellation For Earth Observation
Andrea Sainati, Anupam Parihar, Stephen Kwan Seklam 31 A Very Low Altitude Constellation For Earth Observation Andrea Sainati, Anupam Parihar, Stephen Kwan Seklam MSc students, Department of Aerospace
More informationSpacecraft Bus / Platform
Spacecraft Bus / Platform Propulsion Thrusters ADCS: Attitude Determination and Control Subsystem Shield CDH: Command and Data Handling Subsystem Payload Communication Thermal Power Structure and Mechanisms
More informationHayabusa Status and Proximity Operation. As of September 2nd, 2005
Hayabusa Status and Proximity Operation As of September 2nd, 2005 2005/9/2 0 What is Hayabusa? World s First Round-trip Interplanetary Flight HAYABUSA Challenge to Asteroid Sample Return Touch-down + Dimensions
More informationLecture D30 - Orbit Transfers
J. Peraire 16.07 Dynamics Fall 004 Version 1.1 Lecture D30 - Orbit Transfers In this lecture, we will consider how to transfer from one orbit, or trajectory, to another. One of the assumptions that we
More informationLunette: Satellite to Satellite Gravity Mapping of the Moon
Lunette: Satellite to Satellite Gravity Mapping of the Moon Maria Short 9th ILEWG International Conference on Exploration and Utilisation n of the Moon Authors: M. Short, C. Short, A. Philip, J. Gryzmisch,
More informationSpace Travel on a Shoestring: CubeSat Beyond LEO
Space Travel on a Shoestring: CubeSat Beyond LEO Massimiliano Vasile, Willem van der Weg, Marilena Di Carlo Department of Mechanical and Aerospace Engineering University of Strathclyde, Glasgow 5th Interplanetary
More informationXENON RESISTOJETS AS SECONDARY PROPULSION ON EP SPACECRAFTS AND PERFORMANCE RESULTS OF RESISTOJETS USING XENON
XENON RESISTOJETS AS SECONDARY PROPULSION ON EP SPACECRAFTS AND PERFORMANCE RESULTS OF RESISTOJETS USING XENON D. Nicolini (a), D. Robertson (a), E. Chesta (a), G. Saccoccia (a), D. Gibbon (b), A. Baker
More informationDesign of Orbits and Spacecraft Systems Engineering. Scott Schoneman 13 November 03
Design of Orbits and Spacecraft Systems Engineering Scott Schoneman 13 November 03 Introduction Why did satellites or spacecraft in the space run in this orbit, not in that orbit? How do we design the
More informationSolar Reflector Gravity Tractor for Asteroid Collision Avoidance
olar eflector Gravity Tractor for steroid Collision voidance r. Jeff Wesley Fisher Fisher I/ strodynamics pecialist Conference & Exhibit Honolulu, HI 0 ugust, 008 4 1 3 I/ strodynamics 008080 GT Created:
More informationFORMOSAT-3 Satellite Thermal Control Design and Analysis *
Journal of Aeronautics, Astronautics and Aviation, Series A, Vol.39, No.4, pp.287-292 (27) 287 Technical Note FORMOSAT-3 Satellite Thermal Control Design and Analysis * Ming-Shong Chang **, Chia-Ray Chen,
More informationNew Worlds Observer Final Report Appendix E. Section E: Starshades Subsection E.6: Starshade Spacecraft Lead Author: Amy Lo
Section E: Starshades Subsection E.6: Starshade Spacecraft Lead Author: Amy Lo Introduction Starshade Spacecraft Functional Requirements The main function of the starshade spacecraft is to: 1) support
More informationDARPA Lunar Study: Reducing the technical risk associated with lunar resource utilization and lunar surface presence
Space Missions DARPA Lunar Study: Reducing the technical risk associated with lunar resource utilization and lunar surface presence International Lunar Conference 2005 Toronto, Canada Paul Fulford 1, Karen
More informationENAE 791 Course Overview
ENAE 791 Challenges of launch and entry Course goals Web-based Content Syllabus Policies Project Content 1 2016 David L. Akin - All rights reserved http://spacecraft.ssl.umd.edu Space Transportation System
More informationTRAJECTORY DESIGN FOR JOVIAN TROJAN ASTEROID EXPLORATION VIA SOLAR POWER SAIL. Kanagawa, Japan ,
TRAJECTORY DESIGN FOR JOVIAN TROJAN ASTEROID EXPLORATION VIA SOLAR POWER SAIL Takanao Saiki (), Yoji Shirasawa (), Osamu Mori () and Jun ichiro Kawaguchi (4) ()()()(4) Japan Aerospace Exploration Agency,
More informationResults found by the CNES team (team #4)
3 rd Global Trajectory Optimisation Competition (GTOC3) organized by the Aerospace Propulsion Group of the Dipartimento di Energetica at Politecnico di Torino Results found by the CNES team (team #4) Presented
More informationAll questions are of equal value. No marks are subtracted for wrong answers.
(1:30 PM 4:30 PM) Page 1 of 6 All questions are of equal value. No marks are subtracted for wrong answers. Record all answers on the computer score sheet provided. USE PENCIL ONLY! Black pen will look
More informationJPL ISM STP Study Summary
JPL ISM STP Study Summary Nitin Arora, Jonathan Murphy, Leon Alkalai, Jonathan Sauder and JPL Team-X Study Team Detailed Team-X report can also be provided if needed High-level Team-X Mission Requirements
More informationComparison of Return to Launch Site Options for a Reusable Booster Stage
Comparison of Return to Launch Site Options for a Reusable Booster Stage Barry Mark Hellman Space System Design Lab (SSDL) School of Aerospace Engineering USAF ASC/XRE barry.hellman@wpafb.af.mil Advisor
More informationSatellite Orbital Maneuvers and Transfers. Dr Ugur GUVEN
Satellite Orbital Maneuvers and Transfers Dr Ugur GUVEN Orbit Maneuvers At some point during the lifetime of most space vehicles or satellites, we must change one or more of the orbital elements. For example,
More informationPhysicsAndMathsTutor.com 1
PhysicsAndMathsTutor.com 1 Q1. A grinding wheel is used to sharpen chisels in a school workshop. A chisel is forced against the edge of the grinding wheel so that the tangential force on the wheel is a
More informationHayabusa Asteroid Explorer Powered by Ion Engines on the way to Earth
Hayabusa Asteroid Explorer Powered by Ion Engines on the way to Earth IEPC-2009-267 Presented at the 31st International Electric Propulsion Conference, University of Michigan Ann Arbor, Michigan USA Hitoshi
More informationPowered Space Flight
Powered Space Flight KOIZUMI Hiroyuki ( 小泉宏之 ) Graduate School of Frontier Sciences, Department of Advanced Energy & Department of Aeronautics and Astronautics ( 基盤科学研究系先端エネルギー工学専攻, 工学系航空宇宙工学専攻兼担 ) Scope
More informationEVALUATION OF A SPACECRAFT TRAJECTORY DEVIATION DUE TO THE LUNAR ALBEDO
ISSN 76-58 nd International Congress of Mechanical Engineering (COBEM 3) November 3-7, 3, Ribeirão Preto, SP, Brazil Copyright 3 by ABCM EVALUATION OF A SPACECRAFT TRAJECTORY DEVIATION DUE TO THE LUNAR
More informationLAUNCHES AND LAUNCH VEHICLES. Dr. Marwah Ahmed
LAUNCHES AND LAUNCH VEHICLES Dr. Marwah Ahmed Outlines 2 Video (5:06 min) : https://youtu.be/8t2eyedy7p4 Introduction Expendable Launch Vehicles (ELVs) Placing Satellite into GEO Orbit Introduction 3 Introduction
More informationEntry, Descent and Landing Technology Advancement
Entry, Descent and Landing Technology Advancement Dr. Robert D. Braun May 2, 2017 EDL Technology Investments Have Enabled Seven Increasingly-Complex Successful U.S. Landings on Mars Sojourner: 25 kg, 1997
More informationA STUDY OF CRYOGENIC PROPULSIVE STAGES FOR HUMAN EXPLORATION BEYOND LOW EARTH ORBIT
A STUDY OF CRYOGENIC PROPULSIVE STAGES FOR HUMAN EXPLORATION BEYOND LOW EARTH ORBIT Mark Schaffer SpaceWorks Enterprises, Inc., United States, mark.schaffer@sei.aero Chauncey Wenner United Launch Alliance,
More informationToward Venus orbit insertion of Akatsuki
Toward Venus orbit insertion of Akatsuki Takeshi Imamura (JAXA, Japan) Lightning and Airglow Camera Mid-IR Camera UV Imager Ultra-Stable Oscillator 1µm Camera 2µm Camera Development and launch Objective:
More informationRobotic Mobility Above the Surface
Free Space Relative Orbital Motion Airless Major Bodies (moons) 1 2016 David L. Akin - All rights reserved http://spacecraft.ssl.umd.edu Propulsive Motion in Free Space Basic motion governed by Newton
More informationLecture Module 5: Introduction to Attitude Stabilization and Control
1 Lecture Module 5: Introduction to Attitude Stabilization and Control Lectures 1-3 Stability is referred to as a system s behaviour to external/internal disturbances (small) in/from equilibrium states.
More informationESSE Payload Design. 1.2 Introduction to Space Missions
ESSE4360 - Payload Design 1.2 Introduction to Space Missions Earth, Moon, Mars, and Beyond Department of Earth and Space Science and Engineering Room 255, Petrie Science and Engineering Building Tel: 416-736
More informationA Concept Study of the All-Electric Satellite s Attitude and Orbit Control System in Orbit Raising
Journal of Automation and Control Engineering Vol., No., December A Concept Study of the All-Electric Satellite s Attitude and Orbit Control System in Orbit Raising Yoshinobu Sasaki Japan Aerospace Exploration
More informationENAE 483/788D MIDTERM FALL, 2018 NAME: a 3 = a = 42970] 1. So after one sol, the subspacecraft point would have gone 88773
ENAE 483/788D MIDTERM FALL, 208 NAME: One 8.5 x piece of paper allowed for notes (both sides). No Internet-enabled devices allowed. Put your name on the cover page, and on each page if you disassemble
More informationFlight Demonstration of Electrostatic Thruster Under Micro-Gravity
Flight Demonstration of Electrostatic Thruster Under Micro-Gravity Shin SATORI*, Hiroyuki MAE**, Hiroyuki OKAMOTO**, Ted Mitsuteru SUGIKI**, Yoshinori AOKI # and Atsushi NAGATA # * Hokkaido Institute of
More informationLow Thrust Mission Trajectories to Near Earth Asteroids
Low Thrust Mission Trajectories to Near Earth Asteroids Pratik Saripalli Graduate Research Assistant, College Park, Maryland, 20740, USA Eric Cardiff NASA Goddard Space Flight Center, Greenbelt, Maryland,
More informationA Regional Microsatellite Constellation with Electric Propulsion In Support of Tuscan Agriculture
Berlin, 20 th - 24 th 2015 University of Pisa 10 th IAA Symposium on Small Satellites for Earth Observation Student Conference A Regional Microsatellite Constellation with Electric Propulsion In Support
More informationPhysics 2210 Fall 2011 David Ailion EXAM 4
Dd Physics 2210 Fall 2011 David Ailion EXAM 4 PLEASE FILL IN THE INFORMATION BELOW: Name (printed): Name (signed): Student ID Number (unid): u Discussion Instructor: Marc Lindley Jon Paul Lundquist Peter
More informationINVESTIGATION OF PULSED PLASMA THRUSTERS FOR SPACECRAFT ATTITUDE CONTROL
IEPC-97-128 813 INVESTIGATION OF PULSED PLASMA THRUSTERS FOR SPACECRAFT ATTITUDE CONTROL N.J. Meckel, R.J. Cassady, R.D. Osborne, W.A. Hoskins, R.M. Myers PRIMEX Aerospace Company Redmond, WA. ABSTRACT
More informationAstromechanics. 6. Changing Orbits
Astromechanics 6. Changing Orbits Once an orbit is established in the two body problem, it will remain the same size (semi major axis) and shape (eccentricity) in the original orbit plane. In order to
More information