the expected mean and standard deviation values that buildings provide a mP7/sP7: certain degree of additional attenuation. In 16-4-4, is computed as: mP5 a) < Bnoise < Bmeas = 10 log(Bwant/Bnoise) mP5 where: the bandwidth of the considered radio receiver for the wanted signal Bwant: the bandwidth of the broadband disturbance Bnoise: the measurement bandwidth of measuring device. The relationships are as follows: b) Bmeas < Bnoise < Bwant = 10 log(Bnoise/Bmeas) mP5 c) and respectively, Bnoise > Bwant, = 10 log(Bwant/Bmeas) mP5 The value of is calculated by log(r/d) and the exact values of other parameters used in mP6 x•20 equation (20) are unfortunately not known. We believe that the parameters except for and mP5 mP6 would be determined by practical experiment and experience. Table 3 gives a representative example of the limit calculated by using the CISPR model above 1 GHz. TABLE 3 An example of the limit calculated by CISPR model above 1 GHz Actual field strength of the wanted signal, (EW) Gain of disturbance source, P1(dB) Mean value, Standard deviation, (dB) Mean value, Standard deviation, mw sw mP1 sP1 (dB(V/m)) (dB) (dB) 16 2 3 0.1 Gain of victim antenna, Victim is mobile, P2(dB) P3(dB) Mean value, Standard deviation, Mean value, Standard deviation, mP2 sP2 mP3 sP3 (dB) (dB) (dB) (dB) 3 0.1 5 0.1 Emission limit, Type of emission broadband correction, P4(dB) P5(dB) Mean (dB) Standard deviation, Mean value, Standard deviation, mP4 sP4 mP5 sP5 (dB) (dB) (dB) 1 0.1 1.000 0.1 Distance to victim, Building attenuation, P6(dB) P7(dB) Mean value, Standard deviation, Mean value, Standard deviation, mP6 sP6 mP7 sP7 (dB) (dB) (dB) (dB) 16.478 0.1 4.000 0.1 Limit for disturbance measured, (dB(V/m)) ELimit 40.3398
mP7/sP7: the expected mean and standard deviation values that buildings provide a certain degree of additional attenuation. In 16-4-4, mP5 is computed as: a) < Bnoise < Bmeas mP5 = 10 log(Bwant/Bnoise) where: Bwant: the bandwidth of the considered radio receiver for the wanted signal Bnoise: the bandwidth of the broadband disturbance the measurement bandwidth of measuring device. The relationships are as follows: b) Bmeas < Bnoise < Bwant mP5 = 10 log(Bnoise/Bmeas) c) Bnoise > and Bwant, respectively, mP5 = 10 log(Bwant/Bmeas) The value of mP6 is calculated by x•20 log(r/d) and the exact values of other parameters used in equation (20) are unfortunately not known. We believe that the parameters except for mP5 and mP6 would be determined by practical experiment and experience. Table 3 gives a representative example of the limit calculated by using the CISPR model above 1 GHz. TABLE 3 An example of the limit calculated by CISPR model above 1 GHz Actual field strength of the wanted signal, (EW) Gain of disturbance source, P1(dB) Mean value, mw (dB(V/m)) Standard deviation, sw (dB) Mean value, mP1 (dB) Standard deviation, sP1 (dB) 16 2 3 0.1 Gain of victim antenna, P2(dB) Victim is mobile, P3(dB) Mean value, mP2 (dB) Standard deviation, sP2 (dB) Mean value, mP3 (dB) Standard deviation, sP3 (dB) 3 0.1 5 0.1 Emission limit, P4(dB) Type of emission broadband correction, P5(dB) Mean mP4 (dB) Standard deviation, sP4 (dB) Mean value, mP5 (dB) Standard deviation, sP5 (dB) 1 0.1 1.000 0.1 Distance to victim, P6(dB) Building attenuation, P7(dB) Mean value, mP6 (dB) Standard deviation, sP6 (dB) Mean value, mP7 (dB) Standard deviation, sP7 (dB) 16.478 0.1 4.000 0.1 Limit for disturbance measured, ELimit (dB(V/m)) 40.3398
R-REP-SM.2180-2010-MSW-E.docx