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P ( ) 0 One can simplify the 2D Poisson equation into a one-dimensional (ID) Laplace equation along the direction of the channel by making some simplifying assumptions about the boundary conditions in the y direction (normal the Si/SiO 2 interface). Assuming that the potential, (D in the direction normal to the Si/SiO 2 interface can be described by a parabolic function with coefficients co, c 1, and c2 : 4D y) = co (x) +- I (x, C (x)y + c 2 (x)y 2 (3.83) be modeled. In earlier chapters we developed path-loss models based on narrowband measurements, and we utilized them in wideband applications as well. As shown in Eq. (3.2.1), received signal strength is an inverse function of the frequency, and therefore the received signal strength at the lower end of the UWB system spectrum can be much higher than that found at the higher end of the spectrum. At this point one might question whether we can still apply narrowband path-loss modeling techniques to UWB radio propagation. Assuming a perfect transmitter ampli er, a perfect antenna with the same gain at all frequencies of an UWB system, and free-space propagation, from Eq. (3.2.1) the received signal strength as a function of frequency is given by Pr (f ) = Pt Gt Gr 4 d Preferred Applications
formulation, this calls for participants to engage in an examination of
FIGURE 10.1 ESTABLISHING JOINT ACCOUNTABILITIES
INDEX
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