principles of the global positioning system, lecture 2

27
12.540 Principles of the Global Positioning System Lecture 02 Prof. Thomas Herring http://geoweb.mit.edu/~tah/12.540

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Page 1: Principles of the Global Positioning System, Lecture 2

12.540 Principles of the Global Positioning System

Lecture 02 Prof. Thomas Herring

http://geoweb.mit.edu/~tah/12.540

Page 2: Principles of the Global Positioning System, Lecture 2

Coordinate Systems

• Today we cover: – Definition of coordinates – Conventional “realization” of coordinates – Modern realizations using spaced based

geodetic systems (such as GPS).

02/13/12 12.540 Lec 02 2

Page 3: Principles of the Global Positioning System, Lecture 2

Coordinate system definition

• To define a coordinate system you need to define: – Its origin (3 component) – Its orientation (3 components, usually the

direction cosines of one axis and one component of another axes, and definition of handed-ness)

– Its scale (units)

02/13/12 12.540 Lec 02 3

Page 4: Principles of the Global Positioning System, Lecture 2

Coordinate system definition

• In all 7 quantities are needed to uniquely specify the frame.

• In practice these quantities are determined as the relationship between two different frames

• How do we measure coordinates • How do we define the frames

02/13/12 12.540 Lec 02 4

Page 5: Principles of the Global Positioning System, Lecture 2

Measuring coordinates

• Direct measurement (OK for graph paper) • Triangulation: Snell 1600s: Measure angles

of triangles and one-distance in base triangle • Distance measured with calibrated “chain” or

steel band (about 100 meters long) • “Baseline” was about 1 km long • Triangles can build from small to larges ones. • Technique used until 1950s.

02/13/12 12.540 Lec 02 5

Page 6: Principles of the Global Positioning System, Lecture 2

Measuring coordinates

• Small errors in the initial length measurement, would scale the whole network

• Because of the Earth is “nearly” flat, measuring angles in horizontal plane only allows “horizontal coordinates” to be determined.

• Another technique is needed for heights.

02/13/12 12.540 Lec 02 6

Page 7: Principles of the Global Positioning System, Lecture 2

Measuring coordinates

• In 1950s, electronic distance measurement (EDM) became available (out growth of radar)

• Used light travel times to measure distance (strictly, travel times of modulation on either radio, light or near-infrared signals)

02/13/12 12.540 Lec 02 7

Page 8: Principles of the Global Positioning System, Lecture 2

Measuring coordinates

• Advent of EDM allowed direct measurements of sides of triangles

• Since all distances measured less prone to scale errors.

• However, still only good for horizontal coordinates

02/13/12 12.540 Lec 02 8

Page 9: Principles of the Global Positioning System, Lecture 2

Accuracies

• Angles can be measured to about 1 arc second (5x10-6 radians)

• EDM measures distances to 1x10-6 (1part-per-million, ppm)

• Atmospheric refraction 300 ppm • Atmospheric bending can be 60” (more

effect on vertical angles)

02/13/12 12.540 Lec 02 9

Page 10: Principles of the Global Positioning System, Lecture 2

Height coordinates

• Two major techniques: – Measurement of vertical angles

(atmospheric refraction) – “Leveling” measurement of height

differences over short distances (<50 meters).

– Level lines were used to transfer height information from one location to another.

02/13/12 12.540 Lec 02 10

Page 11: Principles of the Global Positioning System, Lecture 2

Other methods

• Maps were made with “plotting tables” (small telescope and angular distance measurements-angle subtended by a known distance

• Aerial photogrammetry coordinates inferred from positions in photographs. Method used for most maps

02/13/12 12.540 Lec 02 11

Page 12: Principles of the Global Positioning System, Lecture 2

Other methods

• What is latitude and longitude • Based on spherical model what

quantities might be measured

• How does the rotation of the Earth appear when you look at the stars?

• Concept of astronomical coordinates

02/13/12 12.540 Lec 02 12

Page 13: Principles of the Global Positioning System, Lecture 2

Geodetic coordinates: Latitude North

Equator

Geoid

gravity direction

Normal to ellipsoid

ga

Local equipotenital surface Earth's surface

P

02/13/12 12.540 Lec 02 13

Page 14: Principles of the Global Positioning System, Lecture 2

Longitude

Longitude measured by time difference of astronomical events 02/13/12 12.540 Lec 02 14

Page 15: Principles of the Global Positioning System, Lecture 2

Astronomical coordinates

• Return to later but on the global scale these provide another method ofdetermining coordinates

• They also involve the Earth’s gravityfield

• Enters intrinsically in triangulation and trilateration through the planes anglesare measured in

02/13/12 12.540 Lec 02 15

Page 16: Principles of the Global Positioning System, Lecture 2

Height determination

• Height measurements historically are very labor intensive

• The figure on the next page shows how the technique called leveling is used to determine heights.

• In a country there is a primary leveling network, and other heights are determinedrelative to this network.

• The primary needs to have a monument spacing of about 50 km.

02/13/12 12.540 Lec 02 16

Page 17: Principles of the Global Positioning System, Lecture 2

Leveling• The process of leveling is to measure

height differences and to sum these to get the heights of other points.

Orthometric height of hill is h1+h2+h3

N is Geoid Height. Line at bottom is ellipsoid

02/13/12 12.540 Lec 02 17

Page 18: Principles of the Global Positioning System, Lecture 2

Leveling

• Using the instrument called a level, the heights on the staffs are read and the difference in the values is the height differences.

• The height differences are summed to get the height of the final point.

• For the primary control network: the separation of the staffs is between 25-50 meters.

• This type of chain of measurements must be stepped across the whole country (i.e., move across thecountry in 50 meter steps: Takes decades and wasdone).

02/13/12 12.540 Lec 02 18

Page 19: Principles of the Global Positioning System, Lecture 2

Leveling problems

• Because heights are determined by summing differences, system very prone to systematic errors; small biases in the height differences due to atmospheric bending, shadows on the graduations and many other types of problem

• Instrument accuracy is very good for first-order leveling: Height differences can be measured to tens of microns.

• Accuracy is thought to about 1 mm-per-square-root-km for first order leveling.

• Changes in the shapes of the equipotential surface with height above MSL also cause problems.

• The difference between ellipsoidal height and Orthometric height is the Geoid height

02/13/12 12.540 Lec 02 19

Page 20: Principles of the Global Positioning System, Lecture 2

Trigonometric Leveling

• When trying to go the tops of mountains, standard leveling does not work well. (Image trying to do this to the summit of Mt. Everest).

• For high peaks: A triangulation method is used call trigonometric leveling.

• Schematic is shown on the next slide • This is not as accurate as spirit leveling

because of atmospheric bending.

02/13/12 12.540 Lec 02 20

Page 21: Principles of the Global Positioning System, Lecture 2

Trigonometric Leveling schematic

• Method for trigonometric leveling. Method requires that distance D in known and the elevation angles are measured. Trigonometry is used to compute h

02/13/12 12.540 Lec 02 21

Page 22: Principles of the Global Positioning System, Lecture 2

Trigonometric Leveling

• In ideal cases, elevation angles at both ends are measured at the same time. This helps cancel atmospheric refraction errors.

• The distance D can be many tens of kilometers. In the case of Mt. Everest, D was over 100 km (the survey team was not even in the same country; they were in India and mountain is in Nepal).

• D is determined either by triangulation or after 1950 by electronic distance measurement (EDM) discussed later

• The heights of the instruments, called theodolites, above the ground point must be measured. Note: this instrument height measurement was not needed for leveling.

02/13/12 12.540 Lec 02 22

Page 23: Principles of the Global Positioning System, Lecture 2

Web sites about geodetic measurements

• http://sco.wisc.edu/surveying/networks.php Geodetic control for Wisconsin

• Try search “trilateration network” search. Finding maps of networks is now difficult (replaced with GPS networks)

• http://www.ngs.noaa.gov/ is web page of National Geodetic Survey which coordinates national coordinate systems

02/13/12 12.540 Lec 02 23

Page 24: Principles of the Global Positioning System, Lecture 2

Earth’s Gravity field

• All gravity fields satisfy Laplace’s equation in free space or material of density . If V is the gravitational potential then

02/13/12 12.540 Lec 02 24

Page 25: Principles of the Global Positioning System, Lecture 2

Solution to gravity potential

• The homogeneous form of this equation is a “classic” partial differential equation.

• In spherical coordinates solved by separation of variables, r=radius, =longitude and =co-latitude

V (r,,) R(r)g( )h() 02/13/12 12.540 Lec 02 25

Page 26: Principles of the Global Positioning System, Lecture 2

Summary

• Examined conventional methods of measuring coordinates

• Triangulation, trilateration and leveling

• Astronomical positioning uses external bodies and the direction of gravity field

• Continue with the use of the gravity field.

02/13/12 12.540 Lec 02 26

Page 27: Principles of the Global Positioning System, Lecture 2

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12.540 Principles of the Global Positioning SystemSpring 2012

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