Page 269 - Integrated Wireless Propagation Models
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                                                           M i c r o c e  I   P r e   d i c t i o n  M o d e I s   247
               4.5.4.2  Recursive Model43
               This is a mathematical model for calculating path losses along streets surrounded by build­
               ings, that are much taller than the height of the antennas. The method is recursive and
               suited for ray- or path-tracing techniques. The procedure works in cases of perpendicular
               street crossings, any arbitrary angles in street crossings, and bent streets with linear seg­
               ments. The method is reciprocal, computer efficient, and simple to use. Before using the
               procedure, one needs some basic information regarding street orientation and transmitter
               location. Then the model can handle these cases by choosing appropriate parameter values.
                  This model is an intermediate model between an empirical model and a physical model.
               It uses the concepts of GTD /UTD for NLOS propagation at the street intersections where
               diffraction and reflection points exist. The model breaks down the radio path between the
               base station and the mobile into a number of segments interconnected by nodes.
                  An illusory distance for each ray path is calculated according to the recursive expres­
               sions as
                                           k i  = k i_1 + d i_1 X q(8 i_1 )
                                                                                (4.5.4.2.1)
                                           d i  = k i  x si_1 + d i_1
               where the initial values of k and d are
                                      0
                                            0
                                                                                (4.5.4.2.2)
                  In Fig. 4.5.4.2.1, solid lines indicate the path of the propagating wave between the
               transmitter T and the receiver R . The path change directions at the nodal point, j =  1
                          x
                                           x
               and  j  = 2, with the angles 8 1  and 8 • The illusory distance d" is calculated for each straight
                                          2
               line. In Fig. 4.5.4.2.1, the number n of straight lines along the ray path is 3. The physical
               distance r is the line segment in meters following the jth node.
                       i
                  The path loss is determined by the parameter qi ' The angle at which the path turns
               at node j is 8 (degrees). When angle 8 increases, the illusory distance d" is increased
                          i
                                                i
               according to the following equation:
                                                                                (4.5.4.2.3)





















               FIGURE 4.5.4.2.1  Recursive model-example of street orientation.
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