Title: Basic Orbital Mechanics
1Basic Orbital Mechanics
2Introduction
- 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
3Training Topics
- Kepler and Newton
- Orbital Elements
- Ground Traces
- Orbit Types
- Orbit Perturbations
4Planetary 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
5Kepler
- 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
6Ellipse
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
7Keplers First Law
- The orbit of each planet is an ellipse, with the
Sun at one focus
8Keplers Second Law
- The line joining the planet to the Sun sweeps out
equal areas in equal times
9Keplers 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
10Newton
- Building upon the work of Kepler and others,
Isaac Newton put forward his laws of motion and
formulated his law of universal gravitation
11Newtons 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
12Newton 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
13Newton in simpler terms
- Amount of curve depends on initial speed and
direction
14Newton in simpler terms
- Satellites must have a balance of
Speed Gravity No orbit Orbit No Orbit
(too slow)
(too fast)
15Satellite orbits
- The initial speed and direction of an orbiting
satellite creates an ellipse with the Earth at
one focus
16Satellite 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.)
17Satellite 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
18Satellite 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
19Semi-Major Axis (Size)
Semi-Major Axis (a)
FOCUS
APOGEE
PERIGEE
Focal Length (c)
Focal Length (c)
20Eccentricity (Shape)
a
e .75
?
?
c
e .45
?
?
c
e 0
?
c
Eccentricity (e) c/a
21Inclination (Tilt)
Inclination Angle 0? to lt 90 ?
Equatorial Plane
Ascending Node
Inclined Prograde Orbit
22Inclination (Tilt)
Inclination Angle gt90? to lt 180 ?
Equatorial Plane
Inclined Retrograde Orbit
Ascending Node
23Right Ascension of Ascending Node (Direction)
Inclined Prograde Orbit
0? First Point of Aries
0?
180?
Ascending Node
Line of Nodes
24Right 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
25Argument of Perigee (Rotation)
Argument of Perigee is the angular distance
between the ascending node and the point of
perigee
Perigee
Equatorial Plane
Ascending Node
26True 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
27Epoch Time
- The epoch time is an exact specification of the
date and time at which a given Keplerian element
set is valid
28Ground 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
29Ground 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
30Ground 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
31Nodal 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
32GROUND TRACESWestward Regression
Pictures and animation courtesy of Capt Troy
Endicott, Det 1 533 TRS, Schriever AFB, AETC
33Orbit 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
34Orbit 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
35Orbit 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
36Launch Azimuth
The desired orbit inclination determines the
azimuth of launch.
Vandenberg AFB
Patrick AFB
Safety constrains possible launch azimuths
37Orbit Types
- Low Earth Orbit (LEO)
- Sun Synchronous
- Polar
- Medium Earth Orbit (MEO)
- Geosynchronous/Geostationary Earth Orbit (GEO)
- Highly inclined orbits
- Molniya
38Low Earth Orbits
- Up to 520 miles
- Common missions
- Manned (shuttle)
- Reconnaissance
- Communications
39LEO
40Polar Orbits
- Inclination of 90 degrees
- Missions
- Mapping
- Surveillance
41Sun 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)
42Sun Synchronous
43Medium Earth Orbit
- Also called semi-synchronous
- 10,900 miles high inclination
- Missions
- Navigation (GPS, GLONASS)
44MEO
45Geosynchronous 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
46GEO
- GEO spacecraft appear to hang motionless above
one position on the Earths surface - Missions
- Communications
- Weather
47GEO
48Highly Elliptical Orbits
- 63.4-116.6 degree inclination
- 200-23,800 mile altitude
- Missions
- Comm relay (Molniya)
49Molniya 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
50Molniya Orbit
51GROUND TRACESHighly Elliptical Orbit
Pictures and animation courtesy of Capt Troy
Endicott, Det 1 533 TRS, Schriever AFB, AETC
52Orbit 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
53Summary
54Backup Charts
55(No Transcript)