Attachment rad had

This document pretains to SES-MOD-20021022-01806 for Modification on a Satellite Earth Station filing.

IBFS_SESMOD2002102201806_289311

Educational Media Foundation                                                   Exhibit A
5700 West Oaks Boulevard ♦ Rocklin ♦ California ♦ 95765

                            Radiofrequency Radiation Hazard Study

In the facility proposed in this application, Educational Media Foundation (“EMF”) will
use two 3.8-meter elliptical antennas, normally configured so that only one antenna is
transmitting at a given time (the other normally acts as a backup antenna). The earth
station transmitting equipment and antennas are located within a controlled area and
are not accessible to the general public. Entry is restricted to employees who have
been made fully aware of the potential for human exposure and can exercise control
over their exposure.

For this study, EMF has used the FCC’s guidelines and procedures for evaluating
environmental effects of radio frequency (RF) emissions, as expressed in OET-65,
August 1997, for frequencies between 300KHz and 100GHz. Since the equipment is
not accessible to the general public, occupational (controlled) exposure maximum
power density limits are used in this study.

EMF’s Ku-Band satellite earth station will be equipped with amplifiers having a
maximum output of 50 watts. One transmitter will feed one of the 3.8m antennas via a
transmission link having 5.83 dB loss. Therefore, the following calculations are based
on a maximum output power at the antenna flange of 13.06 watts:

Antenna Surface: The maximum power density directly in front of the antenna may be
expressed as:

                            4P
              S surface =
                             A

      where: S surface = maximum power density at the antenna surface
                    P = power fed to the antenna
                    A = physical area of the aperture antenna

Using the parameters for EMF’s antennas:

      S surface = (4)(13.06 watts) / ( )(3.8 meters/2)2
      S surface = 52.24 watts / 11.34 m2
      S surface = 4.61 watts / m2
      S surface = 0.46 mW / cm2

Near-Field Region: In the near field of the main beam, the power density can reach a
maximum before it begins to decrease with distance. The extent of the near field can
be described by the following equation:

                                 D2
                        Rnf =
                                 4λ


      where:            Rnf = extent of near field
                        D = maximum diameter
                          = wavelength

Using the parameters for this antenna:
         = 0.0207 meters (at 14.5 GHz)
       Rnf = (3.8 meters)2 / (4)(0.0207 meters)
       Rnf = 14.44 / 0.083 meters
       Rnf = 174.6 meters

The magnitude of the on-axis power density varies according to location in the near
field. However, the maximum value of the near field on axis power density can be
expressed by the following equation:

                        16ηP
               S nf =
                        πD 2

      where:            Snf = maximum near field power density
                           = aperture efficiency
                        P = power fed to the antenna
                        D = antenna diameter

Using the parameters for this antenna:

                  = 0.65
               P = 13.06 watts
               Snf = (16)(0.65)(13.06 watts) /( )(3.8 meters)2
               Snf = 135.832 watts / 45.365 meters2
               Snf = 2.99 watts / meter2
               Snf = 0.3 mW / cm2

Far Field Region: For purposes of evaluating RF exposure, the distance to the
beginning of the far field region can be approximated by the following equation:

                      0.6 D 2
               R ff =
                        λ

      where:            Rff = distance to the beginning of far field
                        D = diameter of antenna
                           = wavelength

Using the parameters for this antenna:

      Rff = (0.6)(3.8 meters)2 / 0.0207 meters
      Rff = 419.1 meters

The power density in the far field region of the antenna pattern decreases inversely as
the square of the distance. The power density in the far field region of the radiation


pattern can be estimated by the equation:

                          PG
                S ff =
                         4πR 2

       where:              Sff = power density (on axis)
                           P = power fed to antenna
                           G = power gain of the antenna in the direction of interest
                           R = distance to the point of interest

Using the parameters for this antenna:
       Sff = (13.06 watts)(53.2 dBi) / (4)( )(419.1)2
       Sff = 2728789 / 2206690
       Sff = 1.24 watts/meter2
       Sff = 0.12 mW/cm2

Main Reflector – Feed Horn Region

The RF energy radiated from the feed system is confined to a conical shape whose
vertex is located at the feed and extends outward to the main reflector surface. This
power density at any point in this region is expressed by the equation:

                           P
                S feed =
                           A

       where:              Sfeed = Power density at the feed horn
                           P = Radiated transmitted power in watts
                           A = Cross sectional area of the conical region in meters2

At the feed horn, the power density is:

       Sfeed = 13.06 watts / ( )(0.1 / 2)2
       Sfeed = 1662.95 watts/meter2
       Sfeed = 166.3 mW/cm2



Document Created: 2002-11-13 11:55:44
Document Modified: 2002-11-13 11:55:44

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