University of Colorado Boulder ASEN 6008 Interplanetary Mission Design Spring 2015 Kate Davis Real Life 1.

Slides:



Advertisements
Similar presentations
Chapter #7 The Solar System.
Advertisements

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
The Sun in the Sky And how it changes in the course of the year.
Mission To Mars In Kerbal Space Program, Where distances are 1/9 real world values.
. Mr. K. NASA/GRC/LTP Part 5 Pathfinder’s Path II.
AAE450 Spring 2009 LEO Atmospheric Drag Analysis and Lunar Orbit Circularization [Andrew Damon] [Mission Ops] February 19,
Chapter 6: Maneuvering in Space By: Antonio Batiste.
GN/MAE1551 Orbital Mechanics Overview 3 MAE 155 G. Nacouzi.
Interstellar Real Estate: Location, Location, Location Defining the Habitable Zone What makes Earth the perfect home for life as we know it? Students in.
The Gas Giants Astronomy 311 Professor Lee Carkner Lecture 16.
ASEN 5050 SPACEFLIGHT DYNAMICS Orbit Transfers Prof. Jeffrey S. Parker University of Colorado – Boulder Lecture 10: Orbit Transfers 1.
ASEN 5050 SPACEFLIGHT DYNAMICS Conversions, f & g, Orbit Transfers Prof. Jeffrey S. Parker University of Colorado – Boulder Lecture 9: Conversions, Orbit.
Motion, Forces and Energy Gravitation Part 2 Initially we assumed that the gravitational force on a body is constant. But now we know that the acceleration.
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: Zoey Bland!! Date: may 14 th Mrs. Lower.  I'm doing Saturn and I'm trying to figure out why do scientists consider Saturn a gas giant?  What is.
Space Mhurrin. First we found out about the planet Jupiter for home work. Then we went round the other groups to find out about other planets.
By: ? & ? Grade 6-1 The Planet’s chart PlanetPeriod of rotation Orbiting the sun Mercury59 days88 days Venus243 days225 days Earth23.9 hours days.
Astronomical Units & Light Years Project. Distance in Space An ellipse is an oval-shaped path. An astronomical unit (AU) is the average distance between.
AE 1350 Lecture #14 Introduction to Astronautics.
Two Interesting (to me!) Topics Neither topic is in Goldstein. Taken from the undergraduate text by Marion & Thornton. Topic 1: Orbital or Space Dynamics.
Mercury  The closest planet to the sun.  It has no moons.  It has 38% gravity.  It takes 88 days to orbit the sun.
HSC Science Teacher Professional Development Program Physics
ASEN 5050 SPACEFLIGHT DYNAMICS Two-Body Motion Prof. Jeffrey S. Parker University of Colorado – Boulder Lecture 3: The Two Body Problem 1.
Gravitation Part II One of the very first telescopic observations ever was Galileo’s discovery of moons orbiting Jupiter. Here two moons are visible,
AIM: The Movement of the Earth
The law of orbits:  All planets move in elliptical orbits, with the sun at one focus.
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.
Module 4: The Wanderers Activity 1: Solar System Orbits.
Kepler’s Laws 1. The orbits of the planets are ellipses, with the sun at one focus of the ellipse. 2. The line joining the planet to the sun sweeps out.
Star trekkers The earth this a part of a vast and complex universe that operates on a set of constant principals.
Colorado Space Grant Consortium Gateway To Space ASEN 1400 / ASTR 2500 Class #21 Gateway To Space ASEN 1400 / ASTR 2500 Class #21 T-25.
FAST LOW THRUST TRAJECTORIES FOR THE EXPLORATION OF THE SOLAR SYSTEM
ARO309 - Astronautics and Spacecraft Design
Orbital Mechanics Principles of Space Systems Design U N I V E R S I T Y O F MARYLAND Orbital Mechanics Energy and velocity in orbit Elliptical orbit parameters.
Motions of the Earth ….it ’ s what moves us. Two motions of the Earth Rotation - Circular movement of an object around an axis Revolution -The movement.
Planets By Meagan Caine.
ASEN 5050 SPACEFLIGHT DYNAMICS Three-Body Orbits Prof. Jeffrey S. Parker University of Colorado – Boulder Lecture 24: General Perturbations 1.
Space.
Physics 231 Topic 9: Gravitation Alex Brown October 30, 2015.
University of Colorado Boulder ASEN 6008 Interplanetary Mission Design Spring 2015 Kate Davis Multi-Rev Solutions 1.
Sea Launch/Zenit Thrust: 8,180,000 N Fueled Weight: 450,000 kg Payload to LEO: 13,740 kg Cost per launch: $100,000,000 Cost per kg: $7,300 Launches: 31/28.
Uniform Circular Motion. Q: You are swinging a ball around in a circle on a string. Suddenly the string breaks. Where does the ball go? A) out from the.
ASEN 5050 SPACEFLIGHT DYNAMICS Orbit Transfers
Orbital Mechanics Orbital Mechanics refers to the general description of how bodies move in force fields (such as gravity) given that energy and momentum.
5 th Grade MidYear Science Review, Space Science Aldine ISD 2009/2010.
4.2b SKM & PP 1 Exponents: Scientific Notation. 4.2b SKM & PP 2 Think about this?
University of Colorado Boulder ASEN 6008 Interplanetary Mission Design Spring 2015 Kate Davis Tisserand Plots 1.
Bit of Administration …. Lab 2Lab 2 –New observation dates: March 22 - April 5 No need to duplicate observations in hand!No need to duplicate observations.
By: Claire 4B. The Moon It is the satellite of earth The moon has the diameter of about 3,476 It looks similar to mercury.
ASEN 5050 SPACEFLIGHT DYNAMICS Interplanetary Prof. Jeffrey S. Parker University of Colorado – Boulder Lecture 29: Interplanetary 1.
The solar system What is the solar system? The Sun, its planets and other objects in orbit are all together known as the solar system.
How fast do the Planets move? INVESTIGATION What is the order of the planets, from closest to the sun to furthest away? How fast are you travelling right.
Kepler’s Laws of Planetary Motion - 3 Laws -. Elliptical Orbits Planets travel in elliptical orbits with the sun at one focus. Furthest point = Aphelion.
Mission Development: Putting It All Together ASEN 6008 Interplanetary Mission Design.
Presented by: Jamie Quinnell Jean Moiso Gus Mashensic.
P5 – Space for reflection Lesson 1 – circular motion.
1AAE 450 Spring 2008 Scott Breitengross Mar 27, 2008 Trajectory group, Delta V, Saturn V, Feasability Determination, 1 kg Final Design Final Presentation.
If it is known that A is directly proportional to B, how would A change if B is increased by a factor of 2? 1. Increase by a factor of 2 2. Increase by.
ASTR Spring 2008 Joel E. Tohline, Alumni Professor 247 Nicholson Hall [Slides from Lecture15]
Bell Work What are Kepler’s three laws about planetary motion?
Universal Gravitation and Kepler’s Laws
RAP 1. _____sun centered view of the solar system 2._____keeps a tornado going 3. _____discovered sunspots, Venus has phases, 4 moons of Jupiter 4. _____.
The Planets of Our Solar System Mercury.
Jeopardy $100 People Moon Phases Planets Revolution and Rotation Extra Space $200 $300 $400 $500 $400 $300 $200 $100 $500 $400 $300 $200 $100 $500 $400.
Gravity Assists and the use of the Slingshot method
The Gas Giants Astronomy 311 Professor Lee Carkner Lecture 16.
Kepler’s Laws of Orbital Motion
Bellwork 12/22 What kinds of design differences would there be in planning a mission to Jupiter versus sending a satellite into Earth’s orbit?
Presentation transcript:

University of Colorado Boulder ASEN 6008 Interplanetary Mission Design Spring 2015 Kate Davis Real Life 1

University of Colorado Boulder  Mission designers are focused on one primary task: 1. Satisfy the scientists (or other customer) A.Maximize the delivered mass i.Minimize the launch energy ii.Minimize the arrival velocity iii.Minimize the deep space fuel costs B.Minimize the transfer duration C.Minimize risk 2

University of Colorado Boulder  Your boss asks you to give a reasonable estimate for the ΔV required to enter orbit about Uranus. ◦ You already know the Vis-Viva equation and can relate a V ∞ to an orbit insertion ΔV.  Let’s assume r p = 50,000 km; r a = 10 6 km. ◦ She gives you 5 minutes to answer.  0 th order estimate ◦ She gives you 15 minutes to answer  1 st order estimate ◦ She gives you 1 hour to answer  Low-fidelity estimate ◦ She gives you 1+ days to answer  High-fidelity estimate 3

University of Colorado Boulder  How would you provide an estimate of the orbit insertion ΔV at Uranus given:  5 minutes?  Keep it very simple: ◦ Planar ◦ Ignore C 3 ◦ Ignore TOF 4

University of Colorado Boulder  How would you provide an estimate of the orbit insertion ΔV at Uranus given:  5 minutes?  Guess the arrival V ∞ ◦ If you don’t have a better guess, go with 0 km/s ◦ rp = 50,000 km ◦ 0 km/s  367 m/s orbit insertion ◦ “Absolute minimum of 367 m/s!” ◦ (and then multiply it by 4) “Probably more like 1300 m/s” ◦ If you had a better guess: 5

University of Colorado Boulder  How would you provide an estimate of the orbit insertion ΔV at Uranus given:  15 minutes?  Estimate the best possible path from Earth or another planet to Uranus. ◦ Now we can consider gravity assists! ◦ Question: is it possible to get a V ∞ of 0 km/s? ◦ Question 2: if we had a perfect alignment, would we want to get the BIGGEST boost possible from Jupiter or another planet? 6

University of Colorado Boulder  Ignoring timing, launch, orbits, and TOF considerations, what is the “perfect” planetary alignment to minimize orbit insertion ΔV? 7 Sun Planet 1 Uranus’ Orbit Well, a Hohmann Transfer!

University of Colorado Boulder  Can a gravity assist from Planet 1 improve the transfer at all? ◦ Only TOF or non-coplanar accommodations. 8 Sun Planet 1 Uranus’ Orbit Well, a Hohmann Transfer! If you flew by “harder” you could: -Raise Ra -Lower Rp -Change inc -Change AOP All of these generally increase V ∞ If you flew by “harder” you could: -Raise Ra -Lower Rp -Change inc -Change AOP All of these generally increase V ∞ To minimize V ∞ at arrival, you want to maximize the perihelion radius. The way to do that is to place the final gravity assist at periapse. To minimize V ∞ at arrival, you want to maximize the perihelion radius. The way to do that is to place the final gravity assist at periapse.

University of Colorado Boulder  Best possible transfers from previous orbits. 9 Uranus Saturn Jupiter

University of Colorado Boulder  Best possible transfers from previous orbits. 10 “If we fly by Saturn, then the best possible ΔV is only 418 m/s!” (multiply that by 3) “More likely, we’re talking about 1200 m/s”. “If we fly by Jupiter, then the best possible ΔV is only 548 m/s!” (multiply that by 3) “More likely, we’re talking about 1500 m/s”.

University of Colorado Boulder  How would you provide an estimate of the orbit insertion ΔV at Uranus given:  1 hour?  Generate a Pork Chop Plot from each planet to Uranus and assume that we can minimize the arrival V ∞. ◦ Now we can consider orbital variations and phasing. 11

University of Colorado Boulder 12

University of Colorado Boulder  Best possible transfers from previous orbits.  This is an improvement! But man, that’s a long mission ◦ 20 years? Not in my boss’ career span “The best you can possible do using a Jupiter Gravity Assist is a ΔV of 587 m/s” (double that to account for reducing TOF) “We’re talking along the lines of 1100 m/s” 13 Min V ∞ ~ 2.6 km/s ΔV ~ 587 m/s

University of Colorado Boulder 14 Reduce TOF to 11 years. V ∞ : 5.5 km/s Probably want it down to 7 years or less. V ∞ : 8 km/s… Reduce TOF to 11 years. V ∞ : 5.5 km/s Probably want it down to 7 years or less. V ∞ : 8 km/s…

University of Colorado Boulder “The best you can do with a Jupiter Gravity Assist, no Saturn Gravity Assist, and low TOF is a ΔV of m/s” (add more margin to account for getting to Jupiter!) 15

University of Colorado Boulder  Then of course if you have 1+ week, you can design a full interplanetary mission and answer their question more confidently. 16

University of Colorado Boulder  One of the points I’m working on making: you don’t want to depart a planet going too fast. 17 The optimal Uranus arrival conditions required an outbound V ∞ departing Jupiter of about 4 km/s.