ARO 309 Astronautics and Spacecraft Design Winter 2014

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ARO 309 - Astronautics and Spacecraft Design Winter 2014 Try Lam Cal. Poly Pomona

ARO 309 - Astronautics and Spacecraft Design Winter 2014 Try Lam Cal. Poly Pomona Aerospace Engineering

Introductions Class Materials at http: //www. trylam. com/2014 w_aro 309/ • Course: ARO 309:

Introductions Class Materials at http: //www. trylam. com/2014 w_aro 309/ • Course: ARO 309: Astronautics and Spacecraft Design (3 units) • Description: Space mission and trajectory design. Kepler’s laws. Orbits, hyperbolic escape trajectories, interplanetary transfers, gravity assists. Special orbits including geostationary, Molniya, sunsynchronous. [Kepler's equation, orbit determination, attitude dynamics and control. ] • Prerequisite: C or better in ME 215 (dynamics) • Section 01: 5: 30 PM – 6: 45 PM MW (15900) Room 17 -1211 Section 02: 7: 00 PM – 8: 15 PM MW (15901) Room 17 -1211 • Holidays: 1/20 • Text Book: H. Curtis, Orbital Mechanics for Engineering Students, Butterworth-Heinemann (preference: 2 nd Edition) • Grades: 10% Homework, 25% Midterm, 25% Final, 40% Quizzes (4 x 10% each)

Introductions • Things you should know (or willing to learn) to be successful in

Introductions • Things you should know (or willing to learn) to be successful in this class – Basic Math – Dynamics – Basic programing/scripting

What are we studying?

What are we studying?

What are we studying?

What are we studying?

Earth Orbiters

Earth Orbiters

Pork Chop Plot

Pork Chop Plot

High Thrust Interplanetary Transfer

High Thrust Interplanetary Transfer

Low-Thrust Interplanetary Transfer

Low-Thrust Interplanetary Transfer

Low-Thrust Europa End Game

Low-Thrust Europa End Game

Low-Thrust Europa End Game

Low-Thrust Europa End Game

Low-Thrust Europa End Game

Low-Thrust Europa End Game

Orbit Stability Stable for > 100 days Enceladus Orbit

Orbit Stability Stable for > 100 days Enceladus Orbit

Juno

Juno

Other Missions

Other Missions

Other Missions

Other Missions

Lecture 01 and 02: Two-Body Dynamics: Conics Chapter 2

Lecture 01 and 02: Two-Body Dynamics: Conics Chapter 2

Equations of Motion

Equations of Motion

Equations of Motion • Fundamental Equations of Motion for 2 -Body Motion

Equations of Motion • Fundamental Equations of Motion for 2 -Body Motion

Conic Equation From 2 -body equation to conic equation

Conic Equation From 2 -body equation to conic equation

Angular Momentum Other Useful Equations

Angular Momentum Other Useful Equations

Energy NOTE: ε = 0 (parabolic), ε > 0 (escape), ε < 0 (capture:

Energy NOTE: ε = 0 (parabolic), ε > 0 (escape), ε < 0 (capture: elliptical and circular)

Conics

Conics

Circular Orbits

Circular Orbits

Elliptical Orbits

Elliptical Orbits

Elliptical Orbits

Elliptical Orbits

Elliptical Orbits

Elliptical Orbits

Parabolic Orbits • Parabolic orbits are borderline case between an open hyperbolic and a

Parabolic Orbits • Parabolic orbits are borderline case between an open hyperbolic and a closed elliptical orbit NOTE: as v 180°, then r ∞

Hyperbolic Orbits

Hyperbolic Orbits

Hyperbolic Orbits Hyperbolic excess speed

Hyperbolic Orbits Hyperbolic excess speed

Properties of Conics 0<e<1

Properties of Conics 0<e<1

Conic Properties

Conic Properties

Vis-Viva Equation Vis-viva equation Mean Motion

Vis-Viva Equation Vis-viva equation Mean Motion

Perifocal Frame “natural frame” for an orbit centered at the focus with x-axis to

Perifocal Frame “natural frame” for an orbit centered at the focus with x-axis to periapsis and zaxis toward the angular momentum vector

Perifocal Frame FROM THEN

Perifocal Frame FROM THEN

Lagrange Coefficients • Future estimated state as a function of current state Solving unit

Lagrange Coefficients • Future estimated state as a function of current state Solving unit vector based on initial conditions Where and

Lagrange Coefficients • Steps finding state at a future Δθ using Lagrange Coefficients 1.

Lagrange Coefficients • Steps finding state at a future Δθ using Lagrange Coefficients 1. Find r 0 and v 0 from the given position and velocity vector 2. Find vr 0 (last slide) 3. Find the constant angular momentum, h 4. Find r (last slide) 5. Find f, g, fdot, gdot 6. Find r and v

Lagrange Coefficients • Example (from book)

Lagrange Coefficients • Example (from book)

Lagrange Coefficients • Example (from book)

Lagrange Coefficients • Example (from book)

Lagrange Coefficients • Example (from book)

Lagrange Coefficients • Example (from book)

Lagrange Coefficients • Example (from book) Since Vr 0 is < 0 we know

Lagrange Coefficients • Example (from book) Since Vr 0 is < 0 we know that S/C is approaching periapsis (so 180°<θ<360°) ALSO

CR 3 BP • Circular Restricted Three Body Problem (CR 3 BP)

CR 3 BP • Circular Restricted Three Body Problem (CR 3 BP)

CR 3 BP Kinematics (LHS):

CR 3 BP Kinematics (LHS):

CR 3 BP Kinematics (RHS):

CR 3 BP Kinematics (RHS):

CR 3 BP Lyapunov Orbit CR 3 BP Plots are in the rotating frame

CR 3 BP Lyapunov Orbit CR 3 BP Plots are in the rotating frame Tadpole Orbit DRO Horseshoe Orbit

CR 3 BP: Equilibrium Points Equilibrium points or Libration points or Lagrange points L

CR 3 BP: Equilibrium Points Equilibrium points or Libration points or Lagrange points L 4 L 3 L 1 L 2 Jacobi Constant L 5