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Basic Orbital Mechanics

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Title: Basic Orbital Mechanics


1
Basic Orbital Mechanics
  • Jeff Crum
  • 23 Aug 01

2
Introduction
  • Orbital mechanics is the study of the motions of
    artificial satellites and space vehicles moving
    under the influence of forces such as gravity,
    atmospheric drag, thrust, etc.
  • Modern offshoot of celestial mechanics, the study
    of the motions of the moon, planets, and stars

3
Training Topics
  • Kepler and Newton
  • Orbital Elements
  • Ground Traces
  • Orbit Types
  • Orbit Perturbations

4
Planetary motion
  • The problem of accurately describing the motions
    of planets has challenged observers for centuries
  • Early theories held that the Earth was the center
    of the universe and all other heavenly bodies
    traveled in perfect circles about the Earth
  • In 1543, Nicolaus Copernicus published his
    heliocentric theory that postulated that the Sun
    was the center of the universe, and that all
    planetsincluding the Earth, revolved about it in
    perfect circles

5
Kepler
  • Johannes Kepler agreed with Copernicus
    revolutionary and highly controversial theory
  • Using thousands of astronomical observations from
    the Danish astronomer Tycho Brahe, Kepler tried
    in vain to fit the motion of the planet Mars to a
    circular orbit
  • Kepler finally discovered the answer planets
    travel not in circles, but ellipses about the sun

6
Ellipse
GEOMETRIC CENTER
Semi-Minor Axis (b)
FOCUS
FOCUS
Semi-Major Axis (a)
Focal Length (c)
MAJOR AXIS
MINOR AXIS
  • Based on the results of his observations, Kepler
    published his three laws of planetary motion

7
Keplers First Law
  • The orbit of each planet is an ellipse, with the
    Sun at one focus

8
Keplers Second Law
  • The line joining the planet to the Sun sweeps out
    equal areas in equal times

9
Keplers Third Law
  • The square of a planets orbital period is in
    direct proportion to the cube of the semi-major
    axis
  • Orbital period (P) time required to make one
    complete revolution around the sun
  • P2 ? a3
  • For example, Mercury, the closest planet to the
    Sun, completes an orbit in 88 days
  • Pluto, the furthest planet from the Sun,
    completes an orbit every 248 years

10
Newton
  • Building upon the work of Kepler and others,
    Isaac Newton put forward his laws of motion and
    formulated his law of universal gravitation

11
Newtons Laws of Motion
  • First Law A body at rest remains at rest, and a
    body in motion continues to move at a constant
    velocity unless acted upon by an external force
  • Second Law A force (F) acting on a body gives it
    an acceleration (a) which is in the direction of
    the force and has a magnitude inversely
    proportional to the mass of the body (m)
  • F ma
  • Third Law Whenever a body exerts a force on
    another body, the latter exerts a force of equal
    magnitude and opposite direction on the former

12
Newton in simpler terms
  • Objects in motion want to travel in straight
    lines at constant speed (Newtons first law)
  • But
  • Force of gravity causes the path to curve

13
Newton in simpler terms
  • Amount of curve depends on initial speed and
    direction

14
Newton in simpler terms
  • Satellites must have a balance of

Speed Gravity No orbit Orbit No Orbit
(too slow)
(too fast)
15
Satellite orbits
  • The initial speed and direction of an orbiting
    satellite creates an ellipse with the Earth at
    one focus

16
Satellite orbits
  • Apogee highest altitude, lowest speed
  • Perigee lowest altitude, fastest speed

Perigee
Apogee
Note In generic terms, periapsis is the point in
an orbit closest to the primary focus, and
apoapsis is the farthest point. These terms are
usually modified to apply to the body being
orbited (e.g., perihelion/aphelion for the Sun,
perigee/apogee for the Earth, perijove/apojove
for Jupiter, etc.)
17
Satellite Orbits
Orbit size determines satellite period, or time
to make one orbit
DMSP 510 miles 110 minutes
GPS 10900 miles 11 hrs, 58 min
DSP 22300 miles 23 hrs, 56 min
18
Satellite Orbits
  • Orbital element set
  • Semi-Major Axis.. Size
  • Eccentricity. Shape
  • Inclination.. Tilt
  • Right Ascension of the
  • Ascending Node.. Direction
  • Argument of Perigee. Rotation
  • True Anomaly Position
  • Epoch Time. Time Stamp

19
Semi-Major Axis (Size)
Semi-Major Axis (a)
FOCUS
APOGEE
PERIGEE
Focal Length (c)
Focal Length (c)
20
Eccentricity (Shape)
a
e .75
?
?
c
e .45
?
?
c
e 0
?
c
Eccentricity (e) c/a
21
Inclination (Tilt)
Inclination Angle 0? to lt 90 ?
Equatorial Plane
Ascending Node
Inclined Prograde Orbit
22
Inclination (Tilt)
Inclination Angle gt90? to lt 180 ?
Equatorial Plane
Inclined Retrograde Orbit
Ascending Node
23
Right Ascension of Ascending Node (Direction)
Inclined Prograde Orbit
0? First Point of Aries
0?
180?
Ascending Node
Line of Nodes
24
Right Ascension of Ascending Node (Direction)
5
GPS constellation has 6 orbit planes, all
inclined at 55
1
6
Each orbit plane is spaced 60 from the previous
plane
2
4
3
25
Argument of Perigee (Rotation)
Argument of Perigee is the angular distance
between the ascending node and the point of
perigee
Perigee
Equatorial Plane
Ascending Node
26
True Anomaly
True Anomaly is the angular distance between
perigee and some point in the orbit. Usually
this is used to describe where an SV is in the
orbit at a given time.
Equatorial Plane
Perigee
27
Epoch Time
  • The epoch time is an exact specification of the
    date and time at which a given Keplerian element
    set is valid

28
Ground Trace
  • A ground trace is the projection of a satellites
    orbit onto the earths surface
  • Note that the highest northern and southern
    latitudes reached by a satellites ground trace
    is equal to the satellites orbital inclination
  • If inclination gt 90, then highest latitude of
    the ground trace is 180 minus the orbit
    inclination

29
Ground Trace
  • Consider an orbit of a satellite to lie in a
    plane that passes through the center of a
    theoretically spherical Earth
  • The trace of this plane on the surface of a
    non-rotating Earth is a great circle
  • If the Earth did not rotate, the satellite would
    retrace the same ground over and over

30
Ground Trace
  • If we consider a rotating Earth, the orbital
    plane of a satellite remains fixed in space as
    the Earth turns under it
  • Effect of Earths rotation is to displace the
    ground trace on each successive revolution of the
    satellite
  • Ground trace displaced by the number of degrees
    the Earth rotates during on orbital period
  • This displacement is called nodal regression

31
Nodal Regression
  • Earths rotation causes the ground trace to
    regress westward for each successive orbit
  • Earth rotates approximately 15 per hour
  • Nodal regression (orbit period in hours) 15
  • A satellite in a polar orbit has the potential to
    overfly all the Earths surface
  • If the time required for one complete rotation of
    the Earth is an exact multiple of the satellites
    period, then eventually the satellite will
    retrace exactly the same path as it did on some
    previous revolution

32
GROUND TRACESWestward Regression
Pictures and animation courtesy of Capt Troy
Endicott, Det 1 533 TRS, Schriever AFB, AETC
33
Orbit Types
  • Satellites use a wide variety of orbits to
    fulfill their missions
  • Factors determining orbit type
  • Mission requirements
  • Booster capability and cost
  • Satellite and orbital mechanics

34
Orbit Types
  • For a spacecraft to achieve orbit, it must be
    launched to an elevation above the Earths
    atmosphere and accelerated to orbital velocity
  • The most energy efficient orbit is a direct, low
    inclination orbit
  • To achieve this orbit, the spacecraft is launched
    in an eastward direction from a site near the
    Earths equator
  • The rotational speed of the Earth contributes to
    the spacecrafts final orbital speed
  • e.g. A due east launch from the Cape (28.5 deg
    north latitude) results in a free ride of 915
    mph

35
Orbit Types
  • Launching a spacecraft in a direction other than
    east, or from a site far from the equator,
    results in an orbit of higher inclination
  • High inclination orbits are less able to take
    advantage of the initial speed provided by the
    Earths rotation
  • Launch vehicle must provide greater energy to
    attain orbital velocity

36
Launch Azimuth
The desired orbit inclination determines the
azimuth of launch.
Vandenberg AFB
Patrick AFB
Safety constrains possible launch azimuths
37
Orbit Types
  • Low Earth Orbit (LEO)
  • Sun Synchronous
  • Polar
  • Medium Earth Orbit (MEO)
  • Geosynchronous/Geostationary Earth Orbit (GEO)
  • Highly inclined orbits
  • Molniya

38
Low Earth Orbits
  • Up to 520 miles
  • Common missions
  • Manned (shuttle)
  • Reconnaissance
  • Communications

39
LEO
40
Polar Orbits
  • Inclination of 90 degrees
  • Missions
  • Mapping
  • Surveillance

41
Sun Synchronous
  • 460-520 miles
  • Near-polar inclination
  • Orbital plane precesses with the same period as
    the Earths solar period
  • Satellite crosses perigee at the same local time
    every orbit
  • Common missions
  • Earth sensing (LANDSAT)
  • Weather (DMSP/NOAA)

42
Sun Synchronous
43
Medium Earth Orbit
  • Also called semi-synchronous
  • 10,900 miles high inclination
  • Missions
  • Navigation (GPS, GLONASS)

44
MEO
45
Geosynchronous and Geostationary
  • Geosynchronous
  • Altitude 22,300 miles
  • Period 24 hours
  • Any inclination
  • Does not have to be circular
  • Geostationary
  • Altitude 22,300 miles
  • Period 24 hours
  • Inclination near zero
  • Eccentricity nearly zero

46
GEO
  • GEO spacecraft appear to hang motionless above
    one position on the Earths surface
  • Missions
  • Communications
  • Weather

47
GEO
48
Highly Elliptical Orbits
  • 63.4-116.6 degree inclination
  • 200-23,800 mile altitude
  • Missions
  • Comm relay (Molniya)

49
Molniya Orbits
  • Many Russian cities are at high northern
    latitudes where it is impractical to use GEO
    satellites for telecommunications
  • GEO satellites appear either low on the horizon
    or are not visible at all
  • Molniya orbit has a 12 hour period at high
    eccentricity and inclination (63.4)
  • Satellite spends most of its time near apogee, so
    for approximately 11 hours of each orbit the
    satellite is above the horizon for high northern
    latitudes

50
Molniya Orbit
51
GROUND TRACESHighly Elliptical Orbit
Pictures and animation courtesy of Capt Troy
Endicott, Det 1 533 TRS, Schriever AFB, AETC
52
Orbit Perturbations
  • Any disturbance in the regular motion of a
    satellite resulting from a force other than those
    causing regular motion
  • Non-spherical earth
  • Atmospheric drag
  • Sun/moon gravity
  • Space environment

53
Summary
  • TBD

54
Backup Charts
55
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