Title: A Brief Introduction to the Global Positioning System (GPS)
1A Brief Introduction to the Global Positioning
System (GPS) CMPE-118 Lecture
2Global Positioning System (GPS)
- Satellite Navigation system
- Multilateration based on one-way ranging signals
from 24 satellites in orbit - Operated by the United States Air Force
- Nominal Accuracy
- 10 m (Stand Alone)
- 1-5 m (Code Differential)
- 0.01 m (Carrier Differential)
3Navigation Terminology
- Navigation
- Answer the to the question Where am I?
- Implies the use of some agreed upon coordinate
system - Related Terminology
- Guidance Deciding what to do with your
navigation information - Control Orienting yourself/vehicle to follow out
the guidance decision. - Area of Study GNC
- Guidance, Navigation, Control
4Latitude (Parallels) are formed by the
intersection of the surface of the earth with a
plane parallel to the equatorial plane
Longitude (Meridians) are formed by the
intersection of the surface of the earth with a
plane containing the earths axis.
5Latitude, Longitude and Altitude
- One of many coordinate systems used to described
a location on the surface of the earth - Latitude parallels measured from the Equator.
- North is
- Longitude meridians measured from Greenwich
Observatory. - East is
- Altitude measured above reference datum MSL
- Normally Up is
6Stability of Clocks
- Clock stability is directly related to Navigation
because Earth rotates 15/hour. - Difference between local celestial time and
reference yields Longitude. - Atomic clocks are too big and too expensive for
general use.
Figure from Hewlett-Packard Application Note
1289 The Science of Timekeeping by D. W. Allan,
Neil Ashby and Cliff Hodge.
7Position Fixing Methods
- Bearing and range (r-q) position fixing (DME-VOR)
- Dual bearing (q-q) position fixing (VOR-VOR)
- Range (r-r) position fixing (DME-DME, GPS)
- Hyperbolic position fixing (LORAN, Omega)
From Kyton and Fried, Avionics Navigation
Systems, 2nd Ed., pp. 113.
8r-r Position Fixing (2-D)
Assuming you can make the range measurements ri ,
where i 1,2,3, then the following three
equations can be formed
9Fundamentals of Position Fixing
- The figure on the previous page raises to
important questions - How do you estimate or measure the ranges?
- How do you solve the equations for the unknown x
and y? - The range based on measuring the time-of-flight
of a RF signal that leaves the transmitter at t
t1 and arrives at the user at t t2 is given by - In the presence of a clock error, dt ( b/c), the
range estimate (or measurement) becomes
10GPS Pseudoranges
SV 1
SV 2
As a user located at point X, the true range
measurements to the three GPS satellites are
SV 3
Your GPS receiver, however, measures r1, r2 and
r3. These range measurement are called
pseudoranges.
11Psueodranges and Satellite Geometry
Geometry plays a role in the accuracy of the
final solution.
12GPS Position Fixing
13Solving Navigation Equations
- Solve the r-r equations
- Easy and give you insight into the linearization
process - GPS navigation equations.
- The r-r position fixing system of equations where
three independent range measurements are
available was given as
14Linearization by Expansion
Exact Equations you would solve in an ideal world
Equations the you can or will solve
15Linearization by Expansion (2)
16Linearization by Expansion (3)
Taking the difference between the true and
estimated values,
Normally you have more equations than unknowns.
Thus, you can do a least squares solution. That
is,
17Linearization by Expansion (4)
Because we dont have true ranges, but
pseudo-ranges, we augment the G matrix with a
column of ones for the time bias. We need at
least 3 measurements for the 2-D solution.
18Least Squares Solution
For the moment, without proof, we state that the
least squares solution is given by,
- Algorithm for solving the navigation equation
- 1) Pick an initial guess for x and y
- 2) Compute for as many measurements as you
have - 3) Form for all measurements and then form
- 4) Solve for
- 5) Update your initial guesses for x and y as
follows - 6) Repeat until convergence
19Iterated Solution Numerical Example
- Solution is done in MATLAB
- Assumes an initial position of 0,0,0
- Walks solution in to the final position
- Redraws the range circles at each iteration
20GPS Signal Structure
- GPS broadcasts a modulated carrier on L1 (1575.42
MHz) - Pseudo-Random Noise (PRN) sequence of 1023
chips used to spread the signal - PRN is carefully chosen to have unique auto and
crosscorrelation properties - All signal components generated from the same
10.23 MHz satellite clock
21GPS L1 Signal Generation
22GPS Signal De-Spreading
- In order to use the PRN code correlation
properties to de-spread the GPS signal, need to
recover code down to baseband (no carrier) - Use trigonometric identities to mix down and
remove the carrier
23Graphical Depiction of De-Spreading
24PRN Auto- and Cross-Correlation
25PRN Correlation Example
26Initial Acquisition Search
- Assume 1 channel 1 ms dwell period
- Exhaustive search (if real time) requires
- (32) x (2046) x (20) x 1ms 1309 seconds
- 12 channel assumption requires
- (1309) / 12 109 seconds
27Typical Search Results
28Things to remember about GPS
- Navigation is a hard problem, and only recently
has GPS made this easy! - GPS is a r-r system that has precise clocks on
board that give you position and your time bias. - PRN signal has correlation properties that allow
you to find the signal in the noise even without
any knowledge of position.
29Questions?
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32Latitude Determination Using Polaris
Actual location of Polaris is 89o 05
The Sky Above Palo Alto on Jan 6, 2002
33Instruments of Navigation
An Astrolabe
A Sextant
34View Through a Sextant
Easier to align Suns (or other celestial
bodys) limb with the horizon.
35Latitude Determination Using the Sun
36 The Longitude Problem
- Celestial map changes because of Earths 15 o/hr
(approximately) rotation rate.
37Longitude Determination
- Longitude Determination Methods
- Methods based on time
- Compare the time between a clocks at the current
location and some other reference point. - Requires Stable Clocks
- Celestial Methods
- Eclipses of Jupiters Moons
- Lunar Distance Method
38Fundamentals of Radionavigation
- Radio Frequency (RF) signals emanating from a
source or sources. - The generators of the RF signal are at known
locations - RF signals are used to determine range or bearing
to the known location
39Classification of Radio Frequencies
Propagation characteristic of RF signals is a
function of their frequency
40Line of Sight Transmission
- VHF (VOR, ILS Localizer) and UHF (ILS Glide
Slope, TACAN/DME) are line of sight systems. - Limited Coverage area
- LORAN and OMEGA are over the horizon systems
- Large coverage area
- In the case of Omega, coverage was global
- Frequency band in which GPS operates makes it a
line of sight system. However, because of the
location of the satellites, it is able to cover a
large geographic area.
41INS and Radionavigation Systems
INS is not a radionavigation system but is
normally used in conjunction with such systems
42Phases of Flight
- The required navigation accuracy and reliability
(i.e., integrity, continuity and availability)
depend on the phase of flight - Currently, as well as in the past, this meant
that an aircraft had to be equipped with various
navigation systems.
43VHF Omni-directional Range (VOR)
- Provides Bearing (Y) Information
- Operates 112 118 MHz
- Accuracy 1o to 2 o.
- Principles of Operation (Enge et. al.
Terrestrial Radionavigation, pp. 81) - Transmits 2 Signals
- 1st Signal has azimuth dependent phase
- 2nd Signal is a reference
- D between the phases of signal 1st and 2nd
signal is Y
44Distance Measuring Equipment (DME)
- Measures Slant Range (r)
- Operates between 962 and 1213 MHz
- Based on Radar Principle
- Airborne unit sends a pair of pulses
- Ground Station receives pulses
- After short delay (50 ms) ground station resends
the pulses back - Airborne unit receives the signal and calculates
range by using the following equation
r
45Instrument Landing System (ILS)
- Used extensively during approach and landing to
provides vertical and lateral guidance - Principle of Operation
- Lateral guidance provided by a signal called the
Localizer (108-112 MHz) - Vertical guidance provided by another signal
called the Glide Slope (329-335 MHz) - Distance along the approach path provided by
marker beacons (75 MHz)
46Time Scales
Earth
An Apparent Solar Day
- Sidereal Time Based on the time required by
Earth to complete one revolution about its axis
relative to distant stars. - Apparent Solar Day - Time required for Earth to
complete one revolution with respect to the sun - Mean Solar Time - Same as apparent solar day
except it is based on - Hypothetical earth
- Rotating in a circular orbit around the sun.
- Axis of rotation perpendicular to the orbital
plane - Same as Greenwich Mean Time (GMT)
Sun
Earths Orbit
47Universal Atomic Time
- Universal Time (UT) Time based on astronomical
observations - UT0 Mean Solar Time measured at the prime
meridian - UT1 UT0 Corrected for Earths irregular spin
rate and polar motion - International Atomic Time (TAI)
- Based on Ce-133 Atom
- Coordinated Universal Time (UTC)
- Set to agree with UT1 on January 1, 1958.
- Leap seconds introduced to keep it within 0.9
seconds of UT1
48GPS Time
- GPS Time (GPST) A continuous time scale (no
leap seconds) - Based on Cesium and Rubidium standards
- Steered to be within fractions of a microsecond
modulo one second from UTC - Thus GPST-UTC whole number of seconds a
fraction of a microsecond. - GPS time information transmitted by the
satellites include - GPS second of the week - 604,800 seconds per week
- GPS week number 1024 weeks per epoch
49GPS Time (2)
- GPS satellites carry atomic clocks
- Rubidium and/or Cesium frequency standards
- Satellite clocks monitored by MCS
- Clock bias is modeled as a quadratic
- Parameters of the Quadratic are uploaded to
Satellites which in turn broadcasts them as the
navigation message - Sub-frame 1 of the navigation message
- Clock correction term Dtr takes into account
relativistic effects - Account for speed and location in the gravitation
potential of the clocks - Net effect results in satellite clocks gaining
38.4 msec per day - Compensated for by setting the satellite
fundamental frequency of 10.23 MHz 0.00455 Hz
lower.
50GPS Coordinate Frames
- Inertial Frame of Reference Defined to be a
non-accelerating or rotating coordinate frame of
reference - e.g., Earth Centered Inertial (ECI)
- Required for analysis of satellite motion,
inertial navigation, etc. - Not convenient for terrestrial navigation
- Coordinate systems you will mostly encounter in
GPS are - Earth Centered Earth Fixed (ECEF)
- East-North-Up (ENU)
- Geodetic Coordinates
- Other coordinate systems used in navigation
- North-East-Down (NED) used widely in aircraft
navigation, guidance and control applications - Wander-Azimuth
51Coordinate Frame Relationships
- Geodetic coordinates (f, l, h) to ECEF
- ECEF to Geodetic coordinates
- Iterative algorithm
- See Wgsxyz2lla.m in toolbox
52Geometry of Earth (1)
- Crude Approximation
- A sphere
- R0 6378.137 km
- A spherical model is only good for back of the
envelope type of calculations - Need a more precise model for navigation
applications (especially inertial navigation) - A more accurate model is an ellipsoid
- Parameters of the mathematical ellipsoid are
defined in WGS-84
53Geometry of Earth (2)
- Topographic Surface
- Shape assumed by Earths crust.
- Very complicated shape not amenable to
mathematical modeling - Geoid
- An equipotential surface of Earth's gravity field
which best fits, in a least squares sense, global
Mean Sea Level (MSL). - Reference Ellipsoid
- Mathematical fit to the geoid that happens to be
an ellipsoid of revolution and minimizes the
mean-square deviation of local gravity and the
normal to the ellipsoid
54WGS-84 Reference Ellipsoid
- Some geometric facts about the WGS-84 Reference
Ellipsoid - Semi-major axis ( a ) 6378137 m
- Semi-minor axis ( b ) 6356752 m
- Flattening ( f ) 1-(b/a) 1/(298.25722)
- Eccentricity ( e ) f(2-f)1/2 0.081819191
- Given the WGS-84 Ellipsoid parameters, the
following are derived quantities - RNS
- REW
55Geoidal Heights
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57Orbital Mechanics
- Keplers Law
- Based on observations made by Tycho Brahe
(1546-1601) - First Law Each planet revolves around the Sun in
an elliptical path, with the Sun occupying one of
the foci of the ellipse. - Second Law The straight line joining the Sun and
a planet sweeps out equal areas in equal
intervals of time. - Third Law The squares of the planets' orbital
periods are proportional to the cubes of the
semi-major axes of their orbits. - Explanation came later Isaac Newton (1642-1727)
- Universal Law of Gravitation,
where
combined with his second law leads to
58Six Keplerian Elements
- Recast the two-body equation of motion.
- Characterize orbital ellipse
- Semi-major Axis (A)
- Eccentricity (e)
- Characterize orbits orientation in space
- Inclination (i)
- Right Ascension of the Ascending Node (W)
- Characterize ellipses orientation in orbital
plane - Argument of Perigee (w)
- Position of the satellite in the orbit
- True anomaly (n)
- Sometimes it is convenient to sum n and w to form
a new variable called argument of latitude
59GPS Orbital Parameters
- Perturbed Orbits - quasi-Keplerian 15 element set
- Non-central gravitational force
- gravitational fields of the sun and moon
- solar pressure
- Additional 9 parameters
- Three to account for the rate of changes
- Right Ascension of the Ascending Node (W-dot)
- Inclination (i-dot)
- Mean motion (n-dot)
- Three pairs (6 parameter total) to correct
- Argument of latitude
- Orbit radius
- Inclination angle
60GPS Constellation and Orbits
- Nominal Constellation 24 Satellites.
- At present more than 24 satellites on orbit.
- Semi-major axis 26,560 km
- Eccentricity less than 0.01
- Period approximately 11 h 58 min
- Six orbital planes
- Planes designated A through F
- Inclination of 550 relative to the equatorial
plane - RAAN, W, for the six orbital planes separated by
600. - Four Satellites per orbital plane.
Satellites in a given orbital plane are
distributed unevenly to minimize the impact of a
single satellite failure.
61GPS Ephemeris Calculation
- Compute the satellites position in the orbital
coordinate frame - Solve Kepler's equation ( E M e sin E ) for
eccentric anomaly at epoch k, Ek. - Solution requires iteration if orbit is
non-circular - Compute the true anomaly, nk
- Compute the argument of latitude Fk
- Use Fk to compute the corrections for argument of
latitude, radius and inclination then apply the
computed corrections. - Compute the x and y coordinates (xk and yk) of
the satellite in its orbit. - Covert the computed xk and yk position into
ECEF coordinates - Compute the correction for the longitude of the
ascending node. - Apply the correction to the longitude of the
ascending node. - Compute the ECEF coordinates
62GPS Almanac
- A subset of clock and ephemeris parameters.
- Limited to seven parameters and the associated
reference time (toe) - Square root of semi-major axis ((A)1/2)
- Eccentricity (e)
- Inclination (i)
- Longitude of ascending node (W0)
- Rate of right ascension (W-dot)
- Argument of perigee (w)
- Mean anomaly (M)
- Reduced precision
- Allows determining approximate position of
satellites - All satellites broadcast almanac data for all
other satellites in the constellation - Sub-frames 4 and 5 of the navigation message
- Updated less frequently than the ephemeris
parameters in sub-frames 2 and 3.