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A17.98.2
A17.98.2
≤The The terminal designations

This propagation model is not reciprocal with respect to designations of the transmitting/base station and the receiver/mobile station/terminal. It is primarily intended for use with broadcasting and mobile services where the transmitter/base antenna is above the level of local clutter.

...

The value of h1 to be used in calculation should be obtained using the method given in § 3.1, 3.2 or in § 3.3 of P1546-4 as appropriate.

 

Land paths shorter than 15 km

For land paths less than 15 km, the following method is used:

 

Terrain information not available

In SEAMCAT, no terrain information is available. Therefore, the value of h1 is calculated according to path length, d, as follows:

                                                                                                                     Image Added      m for d <= 3 km                                 (Eq. 241232)

   

Mathinline
body${{h}_{1}}={{h}_{a}}$
   m for d ≤ 3 km

                                          

Mathinline
body${{h}_{1}}={{h}_{a}}+({{h}_{eff}}-{{h}_{a}})(d-3)/12$
      m for 3 km < d < 15 km

where ha is the antenna height above ground (e.g. height of the mast).

 

Land paths of 15 km or longer

For these paths:

                      

Mathinline
body${{h}_{1}}={{h}_{eff}}$
    m     (Eq. 242)

 

Transmitting/base antenna height, h1, in the range 10 m to 3 000 m

If the value of h1 coincides with one of the eight heights for which curves are provided, namely 10, 20, 37.5, 75, 150, 300, 600 or 1 200 m, the required field strength may be obtained directly from the plotted curves or the associated tabulations. Otherwise the required field strength should be interpolated or extrapolated from field strengths obtained from two curves using:

      

Mathinline
body$E={{E}_{inf}}+({{E}_{sup}}-{{E}_{inf}})\log ({{h}_{1}}/{{h}_{inf}})/\log ({{h}_{sup}}/{{h}_{inf}})$
  dB(μV/m)  (Eq. 243)

where:

                       hinf :        600 m if h1 > 1200 m, otherwise the nearest nominal effective height below h1

                      hsup :        1200 m if h1 > 1200 m, otherwise the nearest nominal effective height above h1

                      Einf :        field-strength value for hinf at the required distance

                     Esup :        field-strength value for hsup at the required distance.

...

                                          Image Added       m for 3 km < d < 15 km

where ha is the antenna height above ground (e.g. height of the mast).

 

Land paths of 15 km or longer

For these paths:

                          Image Added                   m                                              (Eq. 233)

 

Transmitting/base antenna height, h1, in the range 10 m to 3 000 m

If the value of h1 coincides with one of the eight heights for which curves are provided, namely 10, 20, 37.5, 75, 150, 300, 600 or 1 200 m, the required field strength may be obtained directly from the plotted curves or the associated tabulations. Otherwise the required field strength should be interpolated or extrapolated from field strengths obtained from two curves using:

           Image Added                         dB(μV/m)                 (Eq. 234)

where:

                       hinf :        600 m if h1 > 1200 m, otherwise the nearest nominal effective height below h1

                      hsup :        1200 m if h1 > 1200 m, otherwise the nearest nominal effective height above h1

                      Einf :        field-strength value for hinf at the required distance

                     Esup :        field-strength value for hsup at the required distance.

 

The field strength resulting from extrapolation for h1 > 1200 m should be limited if necessary such that it does not exceed the maximum defined in § 2 of Recommendation ITU-R P.1546-4.

This model is not valid for h1 > 3000 m.

 

Transmitting/base antenna height, h1, in the range 0 m to 10 m

For a land path, the field strength at the required distance d km for 0 £ h1 < 10 m is calculated using:

 

Interpolation of field strength as a function of distance

Figures 1 to 24 of Recommendation ITU-R P.1546-4 show field strength plotted against distance, d, the range 1 km to 1 000 km. No interpolation for distance is needed if field strengths are read directly from these graphs. For greater precision, and for computer implementation, field strengths should be obtained from the associated tabulations (see Annex 1 of ITU-R P.1546-4.

This model is not valid for h1 > 3000 m.

Transmitting/base antenna height, h1, in the range 0 m to 10 m
For a land path, the field strength at the required distance d km for 0 <= h1 < 10 m is calculated using:

Mathinline
body\[E={{E}_{zero}}+0.1{{h}_{1}}({{E}_{10}}-{{E}_{zero}})\]
       
Mathinline
bodydB(uV/m)
   (Eq. 244)

...

Mathinline
body${{E}_{zero}}={{E}_{10}}+0.5({{C}_{1020}}+{{C}_{h1neg10}})$

...

Mathinline
bodydB(uV/m)

...

Mathinline
body${{C}_{1020}}={{E}_{10}}-{{E}_{20}}$

...

Mathinline
body${{C}_{h1neg10}}$
: the correction Ch1 in dB calculated using equation (12) in § 4.3 of ITU-R P.1546-4 at the required distance for h1 = 
Mathinline
body-
 10 m
E10 and E20 : the field strengths in dB(μV/m)  calculated according to § 4.1 of ITU-R P.1546-4 at the required distance for h1 = 10 m and h1 = 20 m respectively..

Note that the corrections C1020 and

Mathinline
body${{C}_{h1neg10}}$
 should both evaluate to negative quantities.

Transmitting/base antenna height, h1, in the range 0 m to 10 m

For a land path, the field strength at the required distance d km for 0 £ h1 < 10 m is calculated using:

Unit
body$E={{E}_{zero}}+0.1{{h}_{1}}({{E}_{10}}-{{E}_{zero}})$
 dB(μV/m)    (Eq. XXX)

Unit
body${{E}_{zero}}={{E}_{10}}+0.5({{C}_{1020}}+{{C}_{h1neg10}})$
 dB(μV/m)    (Eq. XXXa)

Unit
body${{C}_{1020}}={{E}_{10}}-{{E}_{20}}$
 dB    (Eq. XXXb)

Interpolation of field strength as a function of distance

Figures 1 to 24 of Recommendation ITU-R P.1546-4 show field strength plotted against distance, d, the range 1 km to 1 000 km. No interpolation for distance is needed if field strengths are read directly from these graphs. For greater precision, and for computer implementation, field strengths should be obtained from the associated tabulations (see Annex 1 of ITU-R P.1546-4, § 3). In this case, unless d coincides with one of the tabulation distances given in Table 1, the field strength, E (dB(μV/m)), should be linearly interpolated for the logarithm of the distance using:

       

Mathinline
body$E={{E}_{inf}}+({{E}_{sup}}-{{E}_{inf}})\log (d/{{d}_{inf}})/\log ({{d}_{sup}}/{{d}_{inf}})$
   dB(μV/m)    (Eq. 247)

where:

                         :        distance for which the prediction is required

                       dinf :        nearest tabulation distance less than d

                      dsup :        nearest tabulation distance greater than d

                      Einf :        field-strength value for dinf

                     Esup :        field-strength value for dsup.

This model is not valid for values of d less than 1 km or greater than 1 000 km.

Interpolation and extrapolation of field strength as a function of frequency

Field-strength values for the required frequency should be obtained by interpolating between the values for the nominal frequency values of 100, 600 and 2000 MHz. In the case of frequencies below 100 MHz or above 2 000 MHz, the interpolation must be replaced by an extrapolation from the two nearer nominal frequency values. For most paths interpolation or extrapolation for log (frequency) can be used, but for some sea paths when the required frequency is less than 100 MHz it is necessary to use an alternative method.

For land paths, and for sea paths where the required frequency is greater than 100 MHz, the required field strength, E, should be calculated using:

                             

Mathinline
body$E={{E}_{inf}}+({{E}_{sup}}-{{E}_{inf}})\log (f/{{f}_{inf}})/\log ({{f}_{sup}}/{{f}_{inf}})$
  dB(μV/m)                (Eq. 248)

where:

                         f :        frequency for which the prediction is required (MHz)

                       finf :        lower nominal frequency (100 MHz if f < 600 MHz, 600 MHz otherwise)

                      fsup :        higher nominal frequency (600 MHz if f < 600 MHz, 2 000 MHz otherwise)

                      Einf :        field-strength value for finf

                     Esup :        field-strength value for fsup.

The field strength resulting from extrapolation for frequency above 2 000 MHz should be limited if necessary such that it does not exceed the maximum value given in § 2 of Recommendation ITU-R P.1546-4.

For sea paths where the required frequency is less than 100 MHz an alternative method should be used, based upon the path lengths at which 0.6 of the first Fresnel zone is just clear of obstruction by the sea surface. An approximate method for calculating this distance is given in § 17 of  Recommendation ITU-R P.1546-4.

The alternative method should be used if all of the following conditions are true:

  • The path is a sea path.
  • The required frequency is less than 100 MHz.
  • The required distance is less than the distance at which a sea path would have 0.6 Fresnel clearance at 600 MHz, given by D06(600, h1, 10) as given in § 17 of P1546-4.

If any of the above conditions is not true, then the normal interpolation/extrapolation method given by equation (14) should be used.

If all of the above conditions are true, the required field strength, E, should be calculated using:

            Image Removed      dB(μV/m)                                                                           for d <= df

                Image Removed       dB(μV/m)         for d > df

where:

                    Emax :        maximum field strength at the required distance as defined in § 2 of P1546-4

                       Image Removed     maximum field strength at distance df as defined in § 2 of P1546-4

...

, § 3). In this case, unless d coincides with one of the tabulation distances given in Table 1, the field strength, E (dB(mV/m)), should be linearly interpolated for the logarithm of the distance using:

            Image Added                        dB(μV/m)               (Eq. 235)

where:

                         :        distance for which the prediction is required

                       dinf :        nearest tabulation distance less than d

                      dsup :        nearest tabulation distance greater than d

                      Einf :        field-strength value for dinf

                     Esup :        field-strength value for dsup.

This model is not valid for values of d less than 1 km or greater than 1 000 km.

 

Interpolation and extrapolation of field strength as a function of frequency

Field-strength values for the required frequency should be obtained by interpolating between the values for the nominal frequency values of 100, 600 and 2000 MHz. In the case of frequencies below 100 MHz or above 2 000 MHz, the interpolation must be replaced by an extrapolation from the two nearer nominal frequency values. For most paths interpolation or extrapolation for log (frequency) can be used, but for some sea paths when the required frequency is less than 100 MHz it is necessary to use an alternative method.

For land paths, and for sea paths where the required frequency is greater than 100 MHz, the required field strength, E, should be calculated using:

                                Image Added    dB(μV/m)                (Eq. 236)

where:

                         f :        frequency for which the prediction is required (MHz)

                       finf :        lower nominal frequency (100 MHz if f < 600 MHz, 600 MHz otherwise)

                      fsup :        higher nominal frequency (600 MHz if f < 600 MHz, 2 000 MHz otherwise)

                      Einf :        field-strength value for finf

                     Esup :        field-strength value for fsup.

 

The field strength resulting from extrapolation for frequency above 2 000 MHz should be limited if necessary such that it does not exceed the maximum value given in § 2 of Recommendation ITU-R P.1546-4.

For sea paths where the required frequency is less than 100 MHz an alternative method should be used, based upon the path lengths at which 0.6 of the first Fresnel zone is just clear of obstruction by the sea surface. An approximate method for calculating this distance is given in § 17 of  Recommendation ITU-R P.1546-4.

The alternative method should be used if all of the following conditions are true:

  • The path is a sea path.
  • The required frequency is less than 100 MHz.
  • The required distance is less than the distance at which a sea path would have 0.6 Fresnel clearance at 600 MHz, given by D06(600, h1, 10) as given in § 17 of P1546-4.

                        df :       distance at which the path has 0.6 Fresnel clearance at the required frequency calculated as D06f, h1, 10) as given in § 17 of P1546-4

                    Ed600      field strength at distance d600 and the required frequency calculated using equation (14).

Interpolation of field strength as a function of percentage time

Field-strength values for a given percentage of time between 1% and 50% time should be calculated by interpolation between the nominal values 1% and 10% or between the nominal values 10% and 50% of time using:

...

Mathinline
body$E={{E}_{sup}}({{Q}_{inf}}-{{Q}_{t}})/({{Q}_{inf}}-{{Q}_{sup}})+{{E}_{inf}}({{Q}_{t}}-{{Q}_{sup}})/({{Q}_{inf}}-{{Q}_{sup}})$

...

 

If any of the above conditions is not true, then the normal interpolation/extrapolation method given by equation (14) should be used.

If all of the above conditions are true, the required field strength, E, should be calculated using:

            Image Added      dB(μV/m)                                                                           for d <= df

                Image Added       dB(μV/m)         for d > df

where:

                    Emax :        maximum field strength at the required distance as defined in § 2 of P1546-4

                       Image Added     maximum field strength at distance df as defined in § 2 of P1546-4

                         d600 :       distance at which the path has 0.6 Fresnel clearance at 600 MHz calculated as D06(600, h1, 10) as given in § 17 of P1546-4

                        df :       distance at which the path has 0.6 Fresnel clearance at the required frequency calculated as D06f, h1, 10) as given in § 17 of P1546-4

                    Ed600      field strength at distance d600 and the required frequency calculated using equation (14).

 

Interpolation of field strength as a function of percentage time

Field-strength values for a given percentage of time between 1% and 50% time should be calculated by interpolation between the nominal values 1% and 10% or between the nominal values 10% and 50% of time using:

                Image Added        dB(μV/m)    (Eq. 237)

where:

                         t :        percentage time for which the prediction is required

...

where Qi (x) is the inverse complementary cumulative normal distribution function.

 

This model is valid for field strengths exceeded for percentage times in the range 1% to 50% only. Extrapolation outside the range 1% to 50% time is not valid.

...

The field-strength values given by the land curves and associated tabulations in this model are for a reference receiving/mobile antenna at a height, R (m), representative of the height of the ground cover surrounding the receiving/mobile antenna, subject to a minimum height value of 10 m. Examples of reference heights are 20 m for an urban area, 30 m for a dense urban area and 10 m for a suburban area.

Anchor
T090T088T090
T088
Table 9088: Default clutter height in the ITU-R P.1546-4 model (when clutter height option not activated)

 

Selected environment

Assumed height of local clutter
m

Rural

10

Sub-urban

10

Urban

20

Dense urban

30

 

 

Where the receiving/mobile antenna is on land account should first be taken of the elevation angle of the arriving ray by calculating a modified representative clutter height R' (m), given by:

         

Mathinline
body${R}'=(1\,\,000dR-15{{h}_{1}})/(1\,\,000d-15)$
  m                                                 Image Added                  m                              (Eq. 250238)

where h1 and R (m) and distance d (km). Note that for h1 < 6.5d + R, R′ ≈ R. The value of R' must be limited if necessary such that it is not less than 1 m.

when the receiving/mobile antenna is in an urban environment the correction is then given by:

(Eq. 251)

...

Mathinline
body$=6.03-J(\nu )$

...

by:

             Correction        Image Added        dB    for h2 < R

...

Mathinline
body$={{K}_{h2}}\log ({{h}_{2}}/{R}')$

...

′                                                            (Eq. 239)

                            Image Added       dB      for h2 ≥ R

...

′                                                                         

where J(n) is given by equation (12a), and:

                         v =     

Mathinline
body${{K}_{nu}}\ \sqrt{{{h}_{dif}}{{\theta }_{clut}}}$
v =     Image Added

                      Image RemovedImage Added          m         

                       

Mathinline
body${{\theta }_{clut}}$
 =   
Mathinline
body$\arctan ({{h}_{dif}}/27)$
 degrees          Image Added        degrees          

                Image Removed    Image Added

        Image Removed               Image Added

                          f:        frequency (MHz).

In cases in an urban environment where R' is less than 10 m, the correction should be reduced by Khlog(10/R′). Where the receiving/mobile antenna is on land in a rural or open environment the correction is given by equation Image Removed Image Added  for all values of h2 with R' set to 10 m.

...

If a path of length less than 15 km covers buildings of uniform height over flat terrain, a correction representing the reduction of field strength due to building clutter should be added to the field strength. The correction is given by:

...

Mathinline
body$-3.3(\log (f))(1-0.85\log (d))(1-0.46\log (1+{{h}_{a}}-R))$

...

strength. The correction is given by:

                               Correction =  Image Added                (Eq. 240)

where ha is the antenna height above ground (m) (i.e. height of the mast) and R is representative of the height of the ground cover surrounding the receiving/mobile antenna as defined in § 9 of P1546Recommendation ITU-R P. 1546-4, which also represents the height of ground cover surrounding the transmitting/base antenna. This correction only applies when d is less than 15 km and h1 − R is less than 150 m.

 

Variation in path loss

Values of standard deviation are dependent on frequency and environment, and empirical studies have shown a considerable spread. Representative values for areas of 500 m ´ 500 m are given by the following expression (In SEAMCAT it is understood that the below equation only applies to the Mobile system and not to the Broadcasting systems):

...

Mathinline
body${{\sigma }_{L}}=K+1.3\log (f)$

...

to the Broadcasting systems):

                                                               Image Added         dB                                        (Eq. 241)

where:

                K =       1.2, for receivers with antennas below clutter height in urban or suburban environments for mobile systems with omnidirectional antennas at car-roof height

...

                         f :        required frequency (MHz).

 

In SEAMCAT depending on the selected system the standard deviation is defined as follow:

 

Mobile: when “< 2 km radius” and “< 50 km radius” is selected, 4 dB and 8 dB are added to the calculated standard deviation respectively. This responds to the note of the Recommendation stating that if the area over which the variability is to apply is greater than 500 m ´ 500 m, or if the variability is to relate to all areas at a given range, rather than the variation across individual areas, the value of sL will be greater. Empirical studies have suggested that location variability is increased (with respect to the small area values) by up to 4 dB for a 2 km radius and up to 8 dB for a 50 km radius.

...

Broadcasting, analogue: The standard deviation is defined as follow and no correction is added:

...

Mathinline
body${{\sigma }_{L}}=5.1+1.6\log (f)$

...

                                                        Image Added               dB                                       (Eq.

...

242)

In addition, SEAMCAT allows you to select a standard deviation value which overwrites any predefined value when selecting the “use user specified standard deviation” switch.