ITU-R SM 1271-1997 Efficient Spectrum Utilization Using Probabilistic Methods《使用概率的高效光谱利用》.pdf
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1、240 STD-ITU-R RECMN SM-II27L-ENGL 1997 m q855212 05343Z8 333 Rec. ITU-R SM.1271 RECOMMENDATION ITU-R SM. 127 1 EFFICIENT SPECTRUM UTILIZATION USING PROBABILISTIC METHODS (Question ITU-R 4Y1) (1997) The ITU Radiocommunication Assembly, considering that communications technology has advanced rapidly d
2、uring the past decade and the use of radiocommuni- a cation services by administrations has multiplied and placed new demands on the radio spectrum; b) c) d) through the application of probabilistic methods; e) spectrum sharing situations and spectrum utilization against performance standards; that
3、frequency sharing is one of the important aspects of efficient frequency spectrum utilization; that many guidelines and sharing criteria are based on the most unfavourable interference assumptions; that more efficient spectrum utilization may depend on the acceptance of performance criteria develope
4、d that the statistical characteristics of both the desired and interference signals would be necessary to evaluate recommends 1 probability of interference and its impact on system performance. 2. that in order to assess fully the interference potential of introducing a new system into the environme
5、nt, the probability of interference due to multiple interference sources should be considered using techniques such as those shown in Annex 1 and for calculation a probability of interference for base to mobile and mobile to base interference modes in a land mobile duplex system a methodology given
6、in Annex 2 should be used. NOTE 1 - Future examples will be included to explain how probabilistic methods be used to estimate characteristics of desired and interfering signals with the objective of increasing spectrum utilization. that in order to achieve more efficient spectrum utilization, admini
7、strations should consider the use of the ANNEX 1 (Example i) The calculation of the received voltage due to the radiation from multiple Co-frequency sources 1 Introduction There are many frequency sharing situations where interference may occur. In some situations the number and location of possible
8、 interfering sources are not known (e.g. when the interference is from land-mobile radio transmitters). In these situations, interference can be estimated using probabilistic methods. This example describes a method that clearly demonstrates the concept of calculating interference levels due to mult
9、iple sources using probabilistic methods. Consider, for the sake of simplicity, the case of an airborne receiver flying over an urban area. In this particular case the effects of the earth curvature can be neglected. The airborne antenna will be assumed to be a half-wave dipole with a cosine pattern
10、. The N interfering sources are assumed to be uniformly distributed over the area which is assumed to be circular of radius R as shown in Fig. 1. STDoITU-R RECMN SM*L27l-ENGL 1777 W 4855232 0539327 27T W 241 Rec. ITU-R SM.1271 FIGURE 1 Airborne receiver over an urban area with uniformly distributed
11、interference sources The objective will be to derive a simple expression for the probability density function of the received r.m.s. voltage at the receiving antenna terminals. This example is based on several simplifying assumptions as follows: - The number of the interfering transmitters, N, is la
12、rge. - The interfering transmitters are uniformly distributed, in geographical terms, over a circular area of radius R. - All interfering transmitters have equal amount of radiated power. - The receiver, which is subjected to interference from all the mobiles, is airborne at an altitude h, directly
13、above the centre of the circular area that contains all the interfering sources. - The propagation law from any interferer to the airborne receiver is approximated by the free-space propagation rule. 2 The method Considering the airborne receiver now flying over the urban area, the voltage at the re
14、ceiving antenna terminals can be written as follows: STD-ITU-R RECMN SM.1271-ENGL 1797 II 98552L2 0534330 TL m 242 Rec. ITU-R SM.1271 CA is the relationship between the field strength at an antenna and the voltage across its terminals when matched to a 50 L2 load: A(dJ is the complex antenna factor
15、which is related to the interferer-to-antenna distance di as follows: A(di) = a(di) (3) Ki and p; are the amplitude and phase of the field at the receiving antenna due to interferer i and are defined as follows: Ki = EL %) K, (4) whereEL is the specified field strength limit (MV/m) at a distance d (
16、m) from a single interfering source. K, is the interferer radiation pattern factor, accounting for the reduction of the mean level compared to the maximum level. di is the interferer-to-antenna distance in (m). where h is the wavelength and p(0) is the initial phase of the signal as it leaves source
17、 i. Equation (1) can therefore be rewritten as follows: where: where It can be easily shown that I v I follows a Rayleigh distribution such that: is uniformly distributed between O and 2.n. 2 2 where c2 = (N/2). E(vi ) is the expected value of vi. The r.m.s. voltage is v. = . From the variables alre
18、ady stated, the r.m.s. voltage can be calculated as follows: STD*ITU-R RECMN SMm1271-ENGL 1777 W Li855212 0534331 928 W Rec. ITU-R SM.1271 243 The antennddistance factor: is due to the combined effect of the receiving antenna pattern and the spread of the interfering sources over a given area and ma
19、y be calculated by considering the probability distribution of the interfering sources. Assuming a uniform distribution for purposes of simplicity, refemng to Fig. 1, the probability density function of the locationr of the interfering sources is given by: Since the earth curvature is negligible, th
20、e interferer-to-receiving antenna distance is given by: di = dr2 + h2 Also since we assumed a cosine law for the antenna: a(di) - hidi Thus the antenna factor is given by: a(di)ldi - hid? = hi r + h (2 “1 of which the expected value is: 1 R2 + h2 The above expression is suitable for computing the co
21、mbined radiation from many sources over a relatively small area, such as small towns where earth curvature can be neglected. For large cities where the earth curvature cannot be neglected, a relatively more complex formula can be obtained. 3 Conclusion In this example, we can see that in order to es
22、timate the effect of multiple sources of interference which have unknown locations, it is necessary to use probabilistic methods under the assumptions given in the Introduction. The two random variables, namely the received voltage and the antenna factor, have to be considered in their expected valu
23、e form. Equations (10) and (15) are example formulae for computing the interference voltage from the summation of a relatively large number of interfering sources. STD-ITU-R RECMFI SM-1271-ENGL 1597 Hl 4855232 0514332 bli m 244 Rec. ITU-R SM.1271 ANNEX 2 (Example 2) A methodology to calculate a prob
24、ability of interference for base station to mobile station and mobile station to base station interference modes in a land mobile duplex system 1 Introduction In land mobile systems, the reuse distance between Co-channel base stations is traditionally determined according to acceptable level of inte
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