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1 THE SPECIFICATIONS We will develop an algorithm that allows the robot to roam around an area as in Fig 93, but we will use the GPS to obtain the robot s position and use the information in combination with an array of coordinates that delimit the border of the area in which the robot must stay The algorithm will determine if the robot is about to cross any of the imaginary borders and turn away To achieve this goal, we have to specify a few things:.

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The magnitudes are related by E HZ0, where Z0 120p The direction of the line traced out by the tip of the electric field vector determines the polarization of the wave Keep in mind that the electric and magnetic fields are varying as functions of time The magnetic field varies exactly in phase with the electric field, and its amplitude is proportional to the electric field amplitude, so it is only necessary.

We will assume the array of coordinates de nes a fully enclosed area if all of the points are connected together with lines. The coordinate points are consecutive points. There is a line from the rst point to the second, then from the second to the third and so on.

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to consider the electric field in this discussion. The tip of the E vector may trace out a straight line, in which case the polarization is referred to as linear. Other forms of polarization, specifically elliptical and circular, will be introduced later. In the early days of radio, there was little chance of ambiguity in specifying the direction of polarization in relation to the surface of the earth. Most transmissions utilized linear polarization and were along terrestrial paths. Thus vertical polarization meant that the electric field was perpendicular to the earth s surface, and horizontal polarization meant that it was parallel to the earth s surface. Although the terms vertical and horizontal are used with satellite transmissions, the situation is not quite so clear. A linear polarized wave transmitted by a geostationary satellite may be designated vertical if its electric field is parallel to the earth s polar axis, but even so the electric field will be parallel to the earth at the equator. This situation will be clarified shortly. Suppose for the moment that horizontal and vertical are taken as the x and y axes of a right-hand set, as shown in Fig. 5.2a. A vertically polarized electric field can be described as Ey y Ey sinwt (5.1)

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Fig. 4-15

where y is the unit vector in the vertical direction and Ey is the peak value or amplitude of the electric field. Likewise, a horizontally polarized wave could be described by Ex x Ex sinwt (5.2)

The GPS reports the robot s center, so we will allow for the robot s radius in calculating the condition of crossing the boundary line (with a buffer zone). The boundary lines are imaginary, but we would like to have some indication of where they are for display purposes. Therefore, we will draw the lines on the screen to show where they are. We will designate these lines as invisible using the rInvisible command. This prevents the robot from seeing the imaginary drawn boundary as an obstacle. The algorithm will not use these lines in any other way to ascertain the boundary position; only the array of coordinates will designate the boundaries. We will have obstacles in the area and therefore we will incorporate obstacle avoidance in the algorithm. To simplify the math, we will not consider in what way the robot is about to cross the boundary. We will design an algorithm to make the robot think that the boundary lines are walls. The robot will avoid these virtual walls as if they were obstacles. The above means that the algorithm for obstacle avoidance and boundary avoidance are the same (subroutine Reverse of Fig. 9.3). However, the way of determining the boundary crossing (as opposed to object detection) is different and will rely on the GPS to determine if the robot is about to violate the boundary limits. The secret for the new algorithm will be the subroutine TestViolation and the array of coordinates (we will call it Boundary).

These two fields would trace out the straight lines shown in Fig. 5.2b. Now consider the situation where both fields are present simultaneously.

CHAP. 4]