ASEN 5050 SPACEFLIGHT DYNAMICS Mars Odyssey Prof. Jeffrey S. Parker University of Colorado – Boulder Lecture 12: Mars Odyssey 1 Announcements • Homework #4 is due right now • Homework #3 is re-active. Submit a new HW3 submission to the Dropbox or in person by Friday 10/3! – CAETE by Friday 10/10 – You can recover ½ of the points you lost, or get a 90%, whichever is higher. • Mid-term Exam will be handed out Friday, 10/17 and will be due Wed 10/22. (CAETE 10/29) – Take-home. Open book, open notes. – Once you start the exam you have to be finished within 24 hours. – It should take 2-3 hours. • Reading: Chapter 6 Lecture 12: Mars Odyssey 2 Grading • Homework grading – Tough. We’re dropping points pretty easily. • Units • Work • Not answering questions – This is a graduate course, so it takes pretty good work to get an A. At a minimum, you need to read the questions and provide answers to what we’re asking. – This class will ultimately be graded on a curve of some sort. It’s soooo much easier to give everyone a better grade than to knock everyone down at the end! Lecture 12: Mars Odyssey 3 HW3 • I’m posting the solutions online now. • If you missed anything, go redo it until your answers match the online solutions. • If you do, we’ll give you half of your points back, or a 90, whichever is higher. Lecture 12: Mars Odyssey 4 D2L • Request: – Please submit your answers in a Word Doc or a PDF – It’s fine to include code in a .zip file, but it’s harder to grade the HW if the HW is also included in the .zip file. Lecture 12: Mars Odyssey 5 Quiz #9 Lecture 12: Mars Odyssey 6 Quiz #9 Lecture 12: Mars Odyssey 7 Quiz #9 Lecture 12: Mars Odyssey 8 ASEN 5050 SPACEFLIGHT DYNAMICS Mars Odyssey Prof. Jeffrey S. Parker University of Colorado - Boulder Lecture 12: Mars Odyssey 9 ASEN 5050 SPACEFLIGHT DYNAMICS Launch Prof. Jeffrey S. Parker University of Colorado - Boulder Lecture 12: Mars Odyssey 10 Launch Launching a satellite: For a direct launch, the launch site latitude must be less than or equal to the desired inclination, otherwise we must change the inclination of the orbit. Lecture 12: Mars Odyssey 11 Right Spherical Triangle Lecture 12: Mars Odyssey 12 Launch We can show this using spherical trigonometry for a right spherical triangle (eq. C-23): i = inclination cos i = cos f gc sin b Thus, sinb = cos i cos f gc f gc = launch site latitude b = launch azimuth Because |sin b | ≤ 1, the launch latitude fgc ≤ i Cannot direct launch into orbit with inclination < fgc Another useful relation: sin fgc = sin(i) sin(w+n) Lecture 12: Mars Odyssey 13 Launch The launch site velocity is: v L = wÅ ´ rsite or v L = wÅ ´ rsite = wÅ rsite cos fgc Note all the velocity is Eastward in the SEZ system, so launching from the equator on a 90 azimuth may be best. The velocity at the equator is vL = 0.465 km/s. Westward launches must make this up, so difference is 0.93 km/s. Lecture 12: Mars Odyssey 14 Launch Azimuths Launch sites and allowable azimuths Lecture 12: Mars Odyssey 15 Launch Sites Lecture 12: Mars Odyssey 16 Noncoplanar Transfers Lecture 12: Mars Odyssey 17 Noncoplanar Transfers Launch window – select UT to achieve orbit’s desired initial nodal location (determine qgst) First determine launch azimuth b (inverse sine gives two possible answers: b and 180-b, for ascending (90 < u < 90) and descending (90 < u < 270) passes.) cos i sinb = cos f gc cos b Now, determine the auxiliary angle from: coslu = sin i The values lu and 360-lu represent prograde and retrograde orbits respectively. Lecture 12: Mars Odyssey lu = q LST - W but, q LST = q GST + l q GST = W + lu - l 18 Noncoplanar Transfers Tolerance on ascending node (±DW) creates “launch window”, or range of values of qGST. Once qGST is chosen: UT = q GST - q GST 0 wÅ Substitution of qGST0 for each day (GST at 0 hrs on that day) gives the launch time on each day. Dv is more complicated. Lecture 12: Mars Odyssey 19