Orbital Mechanics Overview 2

Information about Orbital Mechanics Overview 2

Published on January 11, 2008

Author: Ubert

Source: authorstream.com

Content

Orbital Mechanics Overview 2:  Orbital Mechanics Overview 2 MAE 155B G. Nacouzi Orbital Mechanics Overview 2:  Orbital Mechanics Overview 2 Summary of first quarter overview Keplerian motion Classical orbit parameters Orbital perturbations Central body observation Coverage examples using Excel Project workshop Introduction: Orbital Mechanics:  Introduction: Orbital Mechanics Motion of satellite is influenced by the gravity field of multiple bodies, however, two body assumption is usually sufficient. Earth orbiting satellite Two Body approach: Central body is earth, assume it has only gravitational influence on S/C, assume M >> m (M, m ~ mass of earth & S/C) Gravity effects of secondary bodies including sun, moon and other planets in solar system are ignored Gravitational potential function is given by:  = GM/r Solution assumes bodies are spherically symmetric, point sources (Earth oblateness not accounted for) Only gravity and centrifugal forces are present Two Body Motion (or Keplerian Motion):  Two Body Motion (or Keplerian Motion) Closed form solution for 2 body exists, no explicit soltn exists for N >2, numerical approach needed Gravitational field on body is given by: Fg = M m G/R2 where, M~ Mass of central body; m~ Mass of Satellite G~ Universal gravity constant R~ distance between centers of bodies For a S/C in Low Earth Orbit (LEO), the gravity forces are: Earth: 0.9 g Sun: 6E-4 g Moon: 3E-6 g Jupiter: 3E-8 g Elliptical Orbit Geometry & Nomenclature:  Elliptical Orbit Geometry & Nomenclature Periapsis Apoapsis Line of Apsides  R a c V Rp b Line of Apsides connects Apoapsis, central body & Periapsis Apogee~ Apoapsis; Perigee~ Periapsis (earth nomenclature) S/C position defined by R & ,  is called true anomaly R = [Rp (1+e)]/[1+ e cos()] Elliptical Orbit Definition:  Elliptical Orbit Definition Orbit is defined using the 6 classical orbital elements: Eccentricity, semi-major axis, true anomaly: position of SC on the orbit inclination, i, is the angle between orbit plane and equatorial plane Argument of Periapsis (). Angle from Ascending Node (AN) to Periapsis. AN: Pt where S/C crosses equatorial plane South to North - Longitude of Ascending Node ()~Angle from Vernal Equinox (vector from center of earth to sun on first day of spring) and ascending node Sources of Orbital Perturbations:  Sources of Orbital Perturbations Several external forces cause perturbation to spacecraft orbit 3rd body effects, e.g., sun, moon, other planets Unsymmetrical central bodies (‘oblateness’ caused by rotation rate of body): Earth: Requator = 6378 km, Rpolar = 6357 km Space Environment: Solar Pressure, drag from rarefied atmosphere Reference: C. Brown, ‘Elements of SC Design’ Relative Importance of Orbit Perturbations:  Relative Importance of Orbit Perturbations J2 term accounts for effect from oblate earth Principal effect above 100 km altitude Other terms may also be important depending on application, mission, etc... Reference: Spacecraft Systems Engineering, Fortescue & Stark Principal Orbital Perturbations:  Principal Orbital Perturbations Earth ‘oblateness’ results in an unsymmetric gravity potential given by: where ae = equatorial radius, Pn ~ Legendre Polynomial Jn ~ zonal harmonics, w ~ sin (SC declination) J2 term causes measurable perturbation which must be accounted for. Main effects: Regression of nodes Rotation of apsides Note: J2~1E-3, J3~1E-6 Orbital Perturbation Effects: Regression of Nodes:  Orbital Perturbation Effects: Regression of Nodes Regression of Nodes: Equatorial bulge causes component of gravity vector acting on SC to be slightly out of orbit plane This out of orbit plane component causes a slight precession of the orbit plane. The resulting orbital rotation is called regression of nodes and is approximated using the dominant gravity harmonics term, J2 Regression of Nodes:  Regression of Nodes Regression of nodes is approximated by: Where,  ~ Longitude of the ascending node; R~ Mean equatorial radius J2 ~ Zonal coeff.(for earth = 0.001082) n ~ mean motion (sqrt(GM/a3)), a~ semimajor axis Note: Although regression rate is small for Geo., it is cumulative and must be accounted for Orbital Perturbation: Rotation of Apsides:  Orbital Perturbation: Rotation of Apsides  Rotation of apsides caused by earth oblateness is similar to regression of nodes. The phenomenon is caused by a higher acceleration near the equator and a resulting overshoot at periapsis. This only occurs in elliptical orbits. The rate of rotation is given by: Ground Track:  Ground Track Defined as the trace of nadir positions, as a function of time, on the central body. Ground track is influenced by: S/C orbit Rotation of central body Orbit perturbations Trace is calculated using spherical trigonometry (no perturbances) sin (La) = sin (i) sin ALa Lo =  + asin(tan (La)/tan(i))+Re where: Ala ~ (ascending node to SC)  ~ Longitude of ascending node I ~ Inclination Re~Earth rotation rate= 0.0042t (add to west. longitudes, subtract for eastern longitude) Example Ground Trace:  Example Ground Trace Spacecraft Horizon:  Spacecraft Horizon SC horizon forms a circle on the spherical surface of the central body, within circle: SC can be seen from central body Line of sight communication can be established SC can observe the central body Central Body Observation:  Central Body Observation From simple trigonometry: sin(h) = Rs/(Rs+hs) Dh = (Rs+hs) cos(h) Sw~ Swath width = 2 h Rs

Related presentations


Other presentations created by Ubert

Deltas
09. 01. 2008
0 views

Deltas

Perfumes
10. 01. 2008
0 views

Perfumes

Powerpoint Programas Co 12
11. 01. 2008
0 views

Powerpoint Programas Co 12

Religion and Everyday Life
14. 01. 2008
0 views

Religion and Everyday Life

English Monolingual Lexicography
14. 01. 2008
0 views

English Monolingual Lexicography

AquaticBiome APES
15. 01. 2008
0 views

AquaticBiome APES

ww5
15. 01. 2008
0 views

ww5

geos112gw
16. 01. 2008
0 views

geos112gw

session 37 Adrienne Jeffries
17. 01. 2008
0 views

session 37 Adrienne Jeffries

Calibration Management
18. 01. 2008
0 views

Calibration Management

PROCUREMENT WORKSHOP MRanger
22. 01. 2008
0 views

PROCUREMENT WORKSHOP MRanger

Life of a slave 2
24. 01. 2008
0 views

Life of a slave 2

Starting a Voices group final
04. 02. 2008
0 views

Starting a Voices group final

application programming
04. 02. 2008
0 views

application programming

Top 10 final
22. 01. 2008
0 views

Top 10 final

2006 opslesson11a
28. 01. 2008
0 views

2006 opslesson11a

amoussou
29. 01. 2008
0 views

amoussou

StarryM 0703
24. 01. 2008
0 views

StarryM 0703

2007524105753299
15. 01. 2008
0 views

2007524105753299

Renal pathology for web
25. 02. 2008
0 views

Renal pathology for web

Chapter 10 Spirit of Baroque
26. 02. 2008
0 views

Chapter 10 Spirit of Baroque

Scharf Sleep September21 1st
28. 02. 2008
0 views

Scharf Sleep September21 1st

earlyeuropeanmedicine
11. 03. 2008
0 views

earlyeuropeanmedicine

Hansford Ucam Ozone
20. 02. 2008
0 views

Hansford Ucam Ozone

AAS207Excite
19. 03. 2008
0 views

AAS207Excite

aetna presentation
15. 01. 2008
0 views

aetna presentation

no09
21. 03. 2008
0 views

no09

Desert
03. 04. 2008
0 views

Desert

Session 6 Malaysia MMU
08. 04. 2008
0 views

Session 6 Malaysia MMU

3490 Class 8
16. 04. 2008
0 views

3490 Class 8

2007041716325228351
24. 04. 2008
0 views

2007041716325228351

Cassini Huygens
09. 01. 2008
0 views

Cassini Huygens

ngupdate 2008
08. 05. 2008
0 views

ngupdate 2008

1 20080331132330
02. 05. 2008
0 views

1 20080331132330

Wedding Gown Ideas
05. 02. 2008
0 views

Wedding Gown Ideas

DeepImpact
09. 01. 2008
0 views

DeepImpact

T1Wk10 Wave Properties
14. 02. 2008
0 views

T1Wk10 Wave Properties

denardi sab06 srw
13. 01. 2008
0 views

denardi sab06 srw

BusinessLaw
04. 02. 2008
0 views

BusinessLaw