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Brussard, G., and D. V. Rogers. 1990. Propagation Considerations in Satellite Communication Systems. Proc. IEEE, Vol. 78, No. 7, July, pp. 1275 1282. CCIR Report 263-5. 1982. Ionospheric Effects upon Earth-Space Propagation. 15th Plenary Assembly, Vol. VI, Geneva, pp. 124 146. CCIR Report 564-2. 1982. Propagation Data Required for Space Telecommunication System. 15 Plenary Assembly, Vol. IX, Part 1, Geneva.

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GPS system relies on satellites in geosynchronous orbits around the earth that send microwave signals to any terrestrial receiver that knows how to read the encoded data The receivers use the data from three or more satellites to triangulate a position on the surface of earth This process is accurate to hundreds of feet (more or less depending on the receiver) This means that if you use this system you would be limited by this resolution One way to increase accuracy is to use an augmentation system that supplements the satellite data with local position references that enable some receivers to be accurate down to feet Such systems are used by some airports to enable aircrafts to land precisely on the centerline of a runway without the pilot ever seeing the runway.

Fig. 4-14

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CCIR Report 719-1. 1982. Attenuation by Atmospheric Gases. 15th Plenary Assembly, Vol. V, Geneva, pp. 138 150. Ippolito, L. J. 1986. Radiowave Propagation in Satellite Communications. Van Nostrand Reinhold, New York. Miya, K. (ed.). 1981. Satellite Communications Technology. KDD Engineering and Consulting, Japan.

These systems can be expensive and may still not be as precise as might be needed in some situations Another way to have a very accurate PS (positioning system) is to create one that implements an LPS (local PS) This system uses the same principles as the GPS but uses local radio transmitters and receivers to calculate positions in reference to a local grid These systems can be accurate down to inches or centimeters and are not overly costly and can be used effectively over a wide area The following algorithm will concentrate on developing the principles of using a PS and how to utilize the information to control the robot Later chapters will explore solutions around accuracy and even how to eliminate the need for a PS altogether 93.

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51 Introduction In the far field zone of a transmitting antenna, the radiated wave takes on the characteristics of a transverse electromagnetic (TEM) wave Far field zone refers to distances greater than 2D2/l from the antenna, where D is the largest linear dimension of the antenna and l is the wavelength For a parabolic antenna of 3 m diameter transmitting a 6-GHz wave (l 5 cm), the far field zone begins at approximately 360 m The TEM designation is illustrated in Fig 51, where it can be seen that both the magnetic field H and the electric field E are transverse to the direction of propagation, denoted by the propagation vector k E, H, and k represent vector quantities, and it is important to note their relative directions.

Consider each quadrant separately. In the rst quadrant, |x| = x and |y| = y. Hence, the equation becomes x + y = 1; that is, y = x + 1. This yields the line with slope 1 and y-intercept 1. This line intersects the x-axis at (1, 0). Hence, in the rst quadrant our graph consists of the line segment connecting (1, 0) and (0, 1) (see Fig. 4-15). In the second quadrant, where x is negative and y is positive, |x| = x and |y| = y, and our equation becomes x + y = 1, or y = x + 1. This yields

When one looks along the direction of propagation, the rotation from E to H is in the direction of rotation of a right-hand-threaded screw, and the vectors are said to form a right-hand set The wave always retains the directional properties of the right-hand set, even when reflected, for example One way of remembering how the right-hand set appears is to note that the letter E comes before H in the alphabet and rotation is from E to H when looking along the direction of propagation At great distances from the transmitting antenna, such as are normally encountered in radio systems, the TEM wave can be considered to be plane This means that the E and H vectors lie in a plane, which is at right angles to the vector k The vector k is said to be normal to the plane.

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