Future In-Space Operations (FISO) Telecon Colloquium

Slides:



Advertisements
Similar presentations
Lunar Landing GN&C and Trajectory Design Go For Lunar Landing: From Terminal Descent to Touchdown Conference Panel 4: GN&C Ron Sostaric / NASA JSC March.
Advertisements

SPACECRAFT ACCIDENTS: EXAMINING THE PAST, IMPROVING THE FUTURE Apollo 13 Bryan Palaszewski working with the Digital Learning Network NASA Glenn Research.
STUDIES ON THE UTILIZATION OF SOLAR SAIL IN LUNAR-TRANSFER TRAJECTORY Zhao Yuhui 1,2, Liu Lin 1,2 1. Astronomy Department, Nanjing University, Nanjing,
15th AAS/AIAA Space Flight Mechanics Meeting, Copper Mountain, Colorado Low Energy Interplanetary Transfers Using the Halo Orbit Hopping Method with STK/Astrogator.
Dr. Andrew Ketsdever Lesson 3 MAE 5595
Space Engineering I – Part I
MAE 4262: ROCKETS AND MISSION ANALYSIS Orbital Mechanics and Hohmann Transfer Orbit Summary Mechanical and Aerospace Engineering Department Florida Institute.
Understand basic orbital mechanics and how orbits work Understand the different types of orbits used for different purposes Understand basic principles.
Orbital Operations – 2 Rendezvous & Proximity Operations
By Ian Lambert. Centuries of Exploration For hundreds of years, the telescope was the main way to observe the moon. The first advancement past the telescope.
Inner Guides=Text Boundary Outer Guides=Inner Boundary Asteroid Redirect Mission and Human Exploration Michele Gates Human Exploration and Operations Mission.
AAE450 Spring 2009 Arbitrary Payload Cost Optimization to LLO Tasks: Payload Cost / Mass Optimization (Launch to LLO) Disprove Momentum Transfer Alternative.
AAE450 Spring 2009 Final Sizing and Trajectory Design for 100 g/10kg Payloads [Levi Brown] [Mission Ops] March 12,
Earth-Moon Transport Doroteo Garcia Kazuya Suzuki Patrick Zeitouni.
AAE450 Senior Spacecraft Design Chris Bush Week 5: February 15 th, 2007 D&C Group High Thrust Trajectories ET, dE, aM.
ASEN 5050 SPACEFLIGHT DYNAMICS Orbit Transfers Prof. Jeffrey S. Parker University of Colorado – Boulder Lecture 10: Orbit Transfers 1.
Satellite communications and the environment of space Images: NASA.
Hypersonic Reentry Dynamics Faculty Advisors Professor Mease (UC Irvine) Dr. Helen Boussalis (CSULA) Student Assistants Katie Demko Shing Chi Chan 7/12/2015NASA.
Gravitational Potential Energy When we are close to the surface of the Earth we use the constant value of g. If we are at some altitude above the surface.
SNAP Spacecraft Orbit Design Stanford University Matthew Peet.
By: James Phommaxay, Andrew Fazekas, and Nick Chase.
Marco Concha Charles Petruzzo June 28, 2001 SuperNova/ Acceleration Probe (SNAP) Flight Dynamics.
Project Apollo. Apollo Mission of Apollo To establish the technology to meet other national interests in space To achieve preeminence in space for the.
Two Interesting (to me!) Topics Neither topic is in Goldstein. Taken from the undergraduate text by Marion & Thornton. Topic 1: Orbital or Space Dynamics.
2 AR Reading until 10:29. Student Planner May 4, 2015 Place this in the proper place SkyMap worksheet due May 6. You need planner, notes, pen/pencil Mercury.
Low-Thrust Transfers from GEO to Earth-Moon Lagrange Point Orbits Andrew Abraham Moravian College, 2013.
Comprehend the history and accomplishments of Project Mercury Comprehend the history and accomplishments of Project Gemini Comprehend the history and accomplishments.
Spacecraft Trajectories You Can Get There from Here! John F Santarius Lecture 9 Resources from Space NEEP 533/ Geology 533 / Astronomy 533 / EMA 601 University.
Advanced Space Exploration LEO Propellant Depot: Space Transportation Impedance Matching Space Access 2010 April 8-10, 2010 Dallas Bienhoff Manager, In-Space.
FAST LOW THRUST TRAJECTORIES FOR THE EXPLORATION OF THE SOLAR SYSTEM
Minimalist Mars Mission Establishing a Human Toehold on the Red Planet Executive Summary DevelopSpace MinMars Team.
Low Thrust Transfer to Sun-Earth L 1 and L 2 Points with a Constraint on the Thrust Direction LIBRATION POINT ORBITS AND APPLICATIONS Parador d'Aiguablava,
MAE 4262: ROCKETS AND MISSION ANALYSIS
America will send a new generation of explorers to the moon aboard NASA’s Orion crew exploration vehicle. After that, on to MARS!!!
The Cold War and the Space Race  At the conclusion of World War 2 both the United States and Russia set themselves up to be super powers  This rivalry.
Human Exploration of Mars Design Reference Architecture 5
ASEN 5050 SPACEFLIGHT DYNAMICS Interplanetary Prof. Jeffrey S. Parker University of Colorado – Boulder Lecture 29: Interplanetary 1.
How Far/How Fast. What are some important questions that you formed about your journey to the moon? List 2 or 3 of the most important things you need.
Final Version Gary Davis Robert Estes Scott Glubke Propulsion May 13-17, 2002 Micro Arcsecond X-ray Imaging Mission, Pathfinder (MAXIM-PF)
2 AR Reading until 10:29. Student Planner May 7, 2015 Place this in the proper place Vocabulary Test Monday You need planner, notes, pen/pencil, spacecraft.
NASA. National Aeronautics and Space Administration Founded in 1958 as a result of the Soviet Unions launch of Sputnik.
Launch Structure Challenge - Background Humans landed on the moon in 1969 – Apollo 11 space flight. In 2003, NASA started a new program (Ares) to send.
An Earth – Moon Transportation System Patrick Zeitouni Space Technology.
Image right: America’s first astronauts: (front row) Walter M. Schirra Jr., Donald K. "Deke" Slayton, John H. Glenn Jr., Scott Carpenter, (back row) Alan.
Workshop on Science Associated with the Lunar Exploration Architecture - Earth Science Subcommittee Theme: A Lunar-Based Earth Observatory Science Observations.
Space and Solar System Word wall. NASA National Aeronautics and Space Administration the federal agency that that deals with aeronautical research and.
The US Manned Space Program. OverviewOverview  The history and accomplishments of Project Mercury  The history and accomplishments of Project Gemini.
Goal to understand how Planetary Orbits work.
Gravity Assists and the use of the Slingshot method
Lunar Trajectories.
Technical Resource Allocations
MOM Mars Orbiter Mission ISRO
Gravity.
The Space Race How it all Began.
The Space Race How it all Began.
Space, the final frontier
Introduction to Astronautics
Space Travel Present & Future
What technology is used to discover objects outside of Earth’s atmosphere? By: chloe de beaupré.
  Robert Zubrin Pioneer Astronautics W. 8th Ave. unit A
Flight Dynamics Michael Mesarch Frank Vaughn Marco Concha 08/19/99
The space race Record RED info only!.
Sun – Earth System Questions
Fall Semester Test Review TEK 6.11
Space Technology and History
  Robert Zubrin Pioneer Astronautics W. 8th Ave. unit A
COMPARING ORBITS FOR THE LUNAR GATEWAY
Three Programs and One Goal
Jeopardy Q $100 Q $100 Q $100 Q $100 Q $100 Q $200 Q $200 Q $200
Presentation transcript:

Future In-Space Operations (FISO) Telecon Colloquium The L1 Orbit Used for Servicing (LOTUS): Enabling Human/Robotic Servicing Missions in the Earth-Moon System Brent Wm. Barbee Future In-Space Operations (FISO) Telecon Colloquium June 16th, 2010

Background NASA-GSFC is currently studying a suite of notional missions to inform a forthcoming congressional report on spacecraft servicing capabilities and concepts The 5th Notional Mission involves human/robotic servicing of a large Sun-Earth L2 (SEL2) telescope in the Earth-Moon system

Mission Profile A large telescope stationed at SEL2 returns to the Earth-Moon system and rendezvouses with a robotic servicing vehicle in a Lyapunov orbit about Earth- Moon L1 (EML1) A crew vehicle carrying astronauts launches to rendezvous with the servicer/telescope stack After servicing is complete, the crew vehicle returns to Earth and the telescope returns to SEL2 The robotic servicer spacecraft remains in orbit for 25 years

Telescope Considerations Minimize telescope maneuver magnitudes Conserve telescope propellant Avoid large thruster-induced accelerations Minimize telescope down-time Avoid excessive travel time to/from SEL2 Telescope is assumed to be a cooperative rendezvous target for the robotic servicer

Robotic Servicer Orbit Robotic servicing vehicle has a 25 year lifetime The orbit it inhabits in the Earth-Moon system must: Be easily accessed by both the crew vehicle and the telescope Require minimal station-keeping ΔV Remain well clear of the Van Allen Belts and GEO

Crew Vehicle Objectives Crew vehicle trajectory should: Maximize available time for servicing Provide a total round-trip flight time (launch to landing) of at most 21 days Offer a free return from launch if possible Stay clear of the Van Allen Belts and GEO Provide safe atmospheric re-entry Maximum atmospheric re-entry velocity of 11 km/s, as per Apollo 10 Notional Orion was assumed for crew vehicle

Robotic Servicer Trajectories

Telescope Trajectories Telescope can travel relatively easily between its SEL2 halo orbit and the EML1 Lyapunov orbit via low-energy transfers ΔV from SEL2 to EML1 = 45 – 50 m/s ΔV from EML1 to SEL2 < 1 m/s Flight time between EML1/SEL2 = 50 – 130 days Faster transfers are possible but require considerable ΔV Some telescope downtime will have to be tolerated in exchange increased lifetime from servicing

Rendezvous at EML1 The robotic servicer can rendezvous with and capture the telescope on the EML1 Lyapunov orbit relatively quickly for modest ΔV costs

Example EML1 Rendezvous The relative motion dynamics between spacecraft on a libration point orbit are completely different from the familiar relative motion dynamics between spacecraft in Earth orbit (LEO, GEO, etc.)

Crew Trajectory Alternatives The first option considered was to send the crew directly to the EML1 orbit and perform servicing there Crew has a free return from launch if necessary However, this only offered ~ 11 days for servicing, which was insufficient for the planned activities Outbound and inbound times are not selectable Additionally, the EML1 orbit experiences eclipses that can be 9 to 12 hours in length

Crew Trajectory Alternatives The second option considered was to place the crew onto a large 21 day long Highly Elliptical Orbit (HEO) about Earth Completely free return for the crew However, bringing the robotic servicer and telescope to this orbit within 1 – 3 days of launch and having them depart within 1 – 3 days of re-entry required > 2,000 m/s of ΔV from the robotic servicer and telescope, which is not permissible

Zero-Velocity Curve Analysis The next approach was to study the restricted three-body dynamics I noticed that there was a large volume of space around Earth that should be accessible from the EML1 orbit for very little ΔV …

The LOTUS Ultra-low departure ΔV from EML1 orbit is easily achieved by the servicer/telescope stack

The LOTUS in the Inertial Frame The LOTUS is a “HEO” with a high perigee Eccentricity of 0.54 Period of ~ 10 days The LOTUS perigee is 83,777 km, well above the Van Allen Belts and GEO

Crew Launch to a LOTUS Apogee

Crew Free Return From Launch The crew always has a free return from launch available from in case LOTUS insertion must be aborted

Servicing on the LOTUS The crew spends 16 days on the LOTUS 1 day is for AR&B with the servicer/telescope stack 15 days for servicing Meets requirements for the notional mission under consideration

Crew Return to Earth

Return to EML1 The LOTUS naturally returns to EML1 ~ 98 days after initial departure The servicer can easily reinsert into the EML1 Lyapunov orbit The telescope can easily continue past EML1 and transfer back to SEL2

Mission Summary Total crew vehicle ΔV (including 100 m/s for AR&B) is 2120 m/s Quite reasonable considering crew vehicles for lunar missions historically had a 2800 m/s capability Well within the notional Orion, Ares I, Ares V capability Total servicing time of 15 days Total round-trip time of 20.54 days

Trajectories in the Inertial Frame

LOTUS Eclipse Analysis Eclipses on the LOTUS are much reduced compared to the EML1 Lyapunov orbit Judicious choice of start date completely avoids eclipses during the LOTUS Worst case eclipse duration on the LOTUS is about 4 hours

Servicing Time Flexibility The 15 day servicing case shown here is only one possibility of many The advantage of the LOTUS is that the crew can arrive at / depart from any points on the LOTUS, making the servicing time selectable With a 21 day round-trip flight time limit, the maximum servicing time available is 19 days Launch into /depart from a LOTUS perigee 0.6 day flight time from launch to LOTUS insertion, same for de-orbit Launch C3 is -7.98 km2/s2 Insertion / De-Orbit ΔV is 1800 m/s Total crew vehicle ΔV of 3700 m/s, not unreasonable for such a low launch C3 and in light of historical and notional future mission capabilities

Summary and Conclusions The LOTUS offers key advantages for human/robotic servicing missions in the Earth-Moon system Selectable time on-orbit for servicing Low ΔV access to/from EML1 and therefore to/from SEL2 Avoidance of eclipses reduces battery size requirements, saving considerable spacecraft mass No orbit maintenance/station-keeping maneuvers required on LOTUS Launch C3 and ΔV requirements consistent with anticipated capabilities Crew always has a free return from launch if necessary LOTUS perigee is well above the Van Allen Belts and GEO Atmospheric re-entry velocity when de-orbiting from any point on the LOTUS is always ≤ 11 km/s