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Praise for Fundamentals of WiMAX

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3.2 The Broadband Wireless Channel: Pathloss and Shadowing 73Sidebar 3.2 Large PathLoss and Increased CapacityBe<strong>for</strong>e continuing, it should be noted that, somewhat counterintuitively,severe pathloss environments <strong>of</strong>ten are desirable in a multiuser wireless network,such as <strong>WiMAX</strong>. Why? Since many users are attempting to simultaneouslyaccess the network, both the uplink and the downlink generallybecome interference limited, which means that increasing the transmitpower <strong>of</strong> all users at once will not increase the overall network throughput.Instead, a lower interference level is preferable. In a cellular system withbase stations, most <strong>of</strong> the interfering transmitters are farther away than thedesired transmitter. Thus, their interference power will be attenuated moreseverely by a large path loss exponent than the desired signal. As noted inthe Sidebar 3.1, a large pathloss exponent can be caused in part by a highercarrier frequency. Example 3.1 will be instructive.Example 3.1Consider a user in the downlink <strong>of</strong> a cellular system, where the desiredbase station is at a distance <strong>of</strong> 500 meters, and numerous nearby interferingbase stations are transmitting at the same power level. If threeinterfering base stations are at a distance <strong>of</strong> 1 km, three at a distance <strong>of</strong>2 km, and ten at a distance <strong>of</strong> 4 km, use the empirical pathloss <strong>for</strong>mula t<strong>of</strong>ind the signal-to-interference ratio (SIR)—the noise is neglected—whenα =3 and when α =5.SolutionForα =3, the desired received power isP3 −3= PPd (0.5) ,rd , t o o(3.8)and the interference power isP3 −3 −3 −3= PPd ⎡⎣3(1) + 3(2) + 10(4) ⎤⎦.rI , t o o(3.9)The SIR expressions compute toPrd,SIR( α = 3) = = 28.25 = 14.5 dB,PrI ,SIR( α = 5) = 99.3 = 20 dB,(3.9)demonstrating that the overall system per<strong>for</strong>mance can be substantiallyimproved when the pathloss is in fact large. These calculations can beviewed as an upper bound, where the SINR γ < SIR , owing to the addition<strong>of</strong> noise. This means that as the pathloss worsens, microcells grow

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