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Chapter3 - Space Environment & Its Effects

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Chapter 3: Space Environment &


Its Effects to Orbit

Chapter outline
 Space Radiation
 Atmospheric Drag
 Third-Body Perturbations
 Non Spherical Earth
Space Environment
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Charged particles

Atmosphere Radiation

Non spherical earth


Magnetic field

Debris
Vacuum
Effects to Orbital Movement
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• Space Radiation
– Radiation from the Sun, produce radiation pressure
• Atmospheric Drag
– Drag from the atmosphere Earth
• Third-Body Perturbation
– Effects of Sun and Moon
• Non Spherical Earth
– perturbation
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Space Radiation
Nuclear Fusion
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• Nuclear fusion processes occur in the center of the


Sun at a temperature of , generates a energy of 26.3
MeV and neutron.
Solar Physics
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Radius
Mass
Particles within plasma 91% H, 8% He, 1% others
Mass density on average
Mass density at center
Luminosity
Effective radiation 5780 K
temperature
Solar constant 1.371 KW/m^2 0.3%
Distance to Earth on average
Distance to Earth at perihelion
Distance to Earth at aphelion
Sidereal rotation period at the 24.8 days
equator
Solar Wind
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• Properties of solar wind:


Chemical composition 96% protons, 4% &
electrons

Density 6 per/cm^3
Temperature 3500-500000K
Free path length 10^8 km
Velocity 200-400 km/s (slow)
600-2000 km/s (fast)

• The solar wind changes the shape of the magnetosphere


and also generates a strong magnetic field.
• The strong magnetic from the solar wind affects
operation of electrical devices in its area.
Momentum of Radiation
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• Waves not only carry energy but also momentum. The effect is very
small (we don’t ordinarily feel pressure from light).
Radiation Pressure
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• Want to relate the pressure felt by the paper to the


intensity of light

 For 100% absorption of light

 100% reflection of light


Example: Radiation Pressure
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Problem1: How much is the radiation pressure 1.5


m away from a 500 Watt light bulb?
Problem2: Calculate the radiation pressure of the
Sun to the Earth? (Distance from the Sun to Earth
is about 150 million Km, of the Sun)
Radiation Pressure Effect to Satellite
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• Radiation pressure force from the Sun

 For 100% absorption of light

 100% reflection of light

-
-
• Satellite above 800km altitude, acceleration from solar radiation
pressure is greater.
Example: Radiation Pressure
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• Example: A satellite has mass of 50kg and area


of . Calculate changes of velocity and distance
in 1 day. (assuming that it is 100% absorption of
light).
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Atmospheric Drag
General Information
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• Drag acts opposite the direction of the velocity


vector, thus slowing the satellite and removing
energy from the orbit.
• Satellite altitude:
- 120 to 160 km of the Earth’s surface, atmospheric
drag will bring it down in a few days.
- Final disintegration occurring at an altitude of
about 80 km.
- Above 600 km, drag is so weak that orbits usually
last more than 10 years – beyond a satellite’s
operational lifetime.
Satellite Decay
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• Explain: satellite decay due


to atmospheric drag from an
• The figure shows dropping apogee
eliptical orbit to a circular of a orbit
orbit.
Effects of Atmospheric Drag
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• Acceleration due to atmospheric drag:

- : drag coefficient (depend on the shape of


spacecraft 2.2 (averaged for typical spacecraft))
- : mass density of atmosphere (kg/m^3)
- : velocity of spacecraft (m/s)
- : area cross of spacecraft (m^2) (perpendicular to velocity
vector)
- : mass of spacecraft (kg)
Effects of Atmospheric Drag
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• For a circular orbit, we can approximate the changes in


semi-major axis, period, and velocity per revolution using
the following equations:

- : ballistic coefficient
- : orbital radius
• , , for a cycle.
Example1:
Effects of Atmospheric Drag
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• Calculate orbit decay/orbital & cycle/day?


For:

Height (km)

100 5.6*10^-7

200 2.5*10^-10

300 1.9*10^-11

500 5.2*10^-13
Example2:
Effects of Atmospheric Drag
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• A satellite is in a circular Earth orbit at an altitude of 400 km.


The satellite has a cylindrical shape 2 m in diameter by 4 m
long and has a mass of 1,000 kg. The satellite is traveling
with its long axis perpendicular to the velocity vector and it's
drag coefficient is 2.67. Calculate the perturbations due to
atmospheric drag.
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Third-Body Perturbation
Effects of the Sun and Moon
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• The gravitational forces of the Sun and Moon cause the change of
longitude of the ascending node and argument of perigee.
• Equations describe these effects:
- Longitude of the ascending node:
(degree/day)

- Argument of perigee:
(degree/day)
Example: Effects of the Sun and Moon
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• Calculate the perturbations in longitude of the ascending


node and argument of perigee caused by the Moon and
Sun for the International Space Station orbiting at an
altitude of 400 km, an inclination of 51.6 degrees, and
with an orbital period of 92.6 minutes.
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Non Spherical Earth


Gravitational Potential
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• GEO (Geographic coordinate system): Equation of


gravitational potential at :

- : latitude of object
- : equatorial radius (=6378.142 km)
- : Lagrange function
Effect of J2
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only consider

• The change of longitude of the ascending node:

• The change of argument of perigee:

- ,
Example: Effect of J2
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• A satellite is in an orbit with a semi-major axis of 7,500


km, an inclination of 28.5 degrees, and an eccentricity of
0.1. Calculate the J2 perturbations in longitude of the
ascending node and argument of perigee.
Effect of J2
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Effect of J2
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Perturbations
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Orbit design (Earth Orbiting)
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• Factors should be considered:


– Recurrent orbit
– No perturbation
– Usage of perturbation
– Constellation design
Recurrent orbit
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• The satellite periodically flies over the


earth surface after a whole number of
obits.

Earth rotation Perturbation


Satellite ground tracks
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Semi-concurrent orbit
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• If swath is small -> more detail of


observation
• Swath is small -> observation is
overlapped.
• Swath is big -> observation gap is
Swath
occurred.

Swath depends on altitude and field of view


No perturbation
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1) .
2)

3)
Usage of a certain perturbation
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• Sun-synchronous orbit (SSO): orbital plane should rotate about .

 It’ s useful because:

• Sun-shining angle would be almost constant (good for

Earth observation).

• Good for thermal design

-> SSO is the best for Earth observation.


Analytical Orbit Models
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• Variation of the elements

• where R(a, e, i. w, Q, M) is the disturbing potential and n is the mean


motion.
Orbit Determination
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• SGP4 model “Simplified General Perturbation Model No.4”


developed by North American Aerospace Defense Command
(NORAD).
• NORAD orbital elements are published in a two-line data format,
nickname “two-line elements”.
• https://www.celestrak.com/NORAD/documentation/tle-fmt.php
Two-line Element
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Two-line Element
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Two-line Element
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• https://www.n2yo.com/satellite/?s=25544
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