Attachment Exhibit C

This document pretains to SES-MOD-20120207-00151 for Modification on a Satellite Earth Station filing.

IBFS_SESMOD2012020700151_938393

                                           Exhibit C
                                   Radiation Hazard Analysis
                               GATR 1.2m Ku-Band Antenna



This analysis predicts the radiation levels around a proposed earth station complex, comprised of
one (reflector) type antennas. This report is developed in accordance with the prediction methods
contained in OET Bulletin No. 65, Evaluating Compliance with FCC Guidelines for Human
Exposure to Radio Frequency Electromagnetic Fields, Edition 97-01, pp 26-30. The maximum
level of non-ionizing radiation to which employees may be exposed is limited to a power density
level of 5 milliwatts per square centimeter (5 mW/cm2) averaged over any 6 minute period in a
controlled environment and the maximum level of non-ionizing radiation to which the general
public is exposed is limited to a power density level of 1 milliwatt per square centimeter (1
mW/cm2) averaged over any 30 minute period in a uncontrolled environment. Note that the
worse-case radiation hazards exist along the beam axis. Under normal circumstances, it is highly
unlikely that the antenna axis will be aligned with any occupied area since that would represent a
blockage to the desired signals, thus rendering the link unusable.

Earth Station Technical Parameter Table
Antenna Actual Diameter               1.2 meters
Antenna Surface Area                  1.1 sq. meters
Antenna Isotropic Gain                42.6 dBi
Number of Identical Adjacent Antennas 1
Nominal Antenna Efficiency (ε)        57.00%
Nominal Frequency                     14.25 GHz
Nominal Wavelength (λ)                0.0211 meters
Maximum Transmit Power / Carrier      33.2 Watts
Number of Carriers                    1
Total Transmit Power                  33.2 Watts
W/G Loss from Transmitter to Feed     0.0 dB
Total Feed Input Power                33.20 Watts
Near Field Limit                      Rnf = D²/4λ =17.10 meters
Far Field Limit                       Rff = 0.6 D²/λ = 41.04 meters
Transition Region                     Rnf to Rff

In the following sections, the power density in the above regions, as well as other critically
important areas will be calculated and evaluated. The calculations are done in the order discussed
in OET Bulletin 65.

1.0 At the Antenna Surface

The power density at the reflector surface can be calculated from the expression:

 PDrefl = 4P/A = 11.742 mW/cm² (1)
 Where: P = total power at feed, milliwatts
          A = Total area of reflector, sq. cm




                                                                                                 1


In the normal range of transmit powers for satellite antennas, the power densities at or around the
reflector surface will exceed safe levels. This area will not be accessible to the general public.
Operators and technicians will receive training specifying this area as a high exposure area.
Procedures will be established that will assure that all transmitters are rerouted or turned off
before access by maintenance personnel to this area is possible.

2.0 On-Axis Near Field Region

The geometrical limits of the radiated power in the near field approximate a cylindrical volume
with a diameter equal to that of the antenna. In the near field, the power density is neither uniform
nor does its value vary uniformly with distance from the antenna. For the purpose of considering
radiation hazard it is assumed that the on-axis flux density is at its maximum value throughout the
length of this region. The length of this region, i.e., the distance from the antenna to the end of the
near field, is computed as Rnf above.

The maximum power density in the near field is given by:

 PDnf = (16ε P)/(π D²) =     6.693 mW/cm² (2)
                             from 0 to 17.10 meters
Evaluation
 Uncontrolled Environment:        Does Not Meet Uncontrolled Limits
 Controlled Environment:          Does Not Meet Controlled Limits

3.0 On-Axis Transition Region

The transition region is located between the near and far field regions. As stated in Bulletin 65,
the power density begins to vary inversely with distance in the transition region. The maximum
power density in the transition region will not exceed that calculated for the near field region, and
the transition region begins at that value. The maximum value for a given distance within the
transition region may be computed for the point of interest according to:

 PDt =       (PDnf)(Rnf)/R = dependent on R (3)
 where:      PDnf = near field power density
             Rnf = near field distance
             R = distance to point of interest
 For:        17.10 < R < 41.0 meters

We use Eq (3) to determine the safe on-axis distances required for the two occupancy conditions:

Evaluation

 Uncontrolled Environment Safe Operating Distance,(meters), Rsafeu:          114.5
 Controlled Environment Safe Operating Distance,(meters), Rsafec:            22.9

4.0 On-Axis Far-Field Region

The on- axis power density in the far field region (PDff) varies inversely with the square of the
distance as follows:




                                                                                                     2


 PDff = PG/(4πR²) = dependent on R (4)
 where: P = total power at feed
        G = Numeric Antenna gain in the direction of interest relative to isotropic radiator
        R = distance to the point of interest
 For: R > Rff = 41.0 meters
        PDff = 2.867 mW/cm² at Rff

We use Eq (4) to determine the safe on-axis distances required for the two occupancy conditions:

Evaluation

 Uncontrolled Environment Safe Operating Distance,(meters), Rsafeu :       See Section 3
 Controlled Environment Safe Operating Distance,(meters), Rsafec :         See Section 3

5.0 Off-Axis Levels at the FarField Limit and Beyond

In the far field region, the power is distributed in a pattern of maxima and minima (sidelobes) as a
function of the off-axis angle between the antenna center line and the point of interest. Off-axis
power density in the far field can be estimated using the antenna radiation patterns prescribed for
the antenna in use. Usually this will correspond to the antenna gain pattern envelope defined by
the FCC or the ITU, which takes the form of:

 Goff = 32 - 25log(Θ)
 for Θ from 1 to 48 degrees; -10 dBi from 48 to 180 degrees
 (Applicable for commonly used satellite transmit antennas)

Considering that satellite antenna beams are aimed skyward, power density in the far field will
usually not be a problem except at low look angles. In these cases, the off axis gain reduction may
be used to further reduce the power density levels.

For example: At one (1) degree off axis At the far-field limit, we can calculate the power density
as:

Goff = 32 - 25log(1) = 32 - 0 dBi = 1585 numeric

 PD1 deg off-axis = PDffx 1585/G = 0.249 mW/cm² (5)

6.0 Off-Axis power density in the Near Field and Transitional Regions

According to Bulletin 65, off-axis calculations in the near field may be performed as follows:
assuming that the point of interest is at least one antenna diameter removed from the center of the
main beam, the power density at that point is at least a factor of 100 (20 dB) less than the value
calculated for the equivalent on-axis power density in the main beam. Therefore, for regions at
least D meters away from the center line of the dish, whether behind, below, or in front under of
the antenna's main beam, the power density exposure is at least 20 dB below the main beam level
as follows:

 PDnf(off-axis) = PDnf /100 = 0.06693 mW/cm² at D off axis (6)




                                                                                                  3


See Section 8 for the calculation of the distance vs. elevation angle required to achieve this rule
for a given object height.

7.0 Region Between the Feed Horn and Sub-reflector

Transmissions from the feed horn are directed toward the subreflector surface, and are confined
within a conical shape defined by the feed horn. The energy between the feed horn and
subreflector is conceded to be in excess of any limits for maximum permissible exposure. This
area will not be accessible to the general public. Operators and technicians should receive training
specifying this area as a high exposure area. Procedures must be established that will assure that
all transmitters are rerouted or turned off before access by maintenance personnel to this area is
possible.

8.0 Evaluation of Safe Occupancy Area in Front of Antenna

The distance (S) from a vertical axis passing through the dish center to a safe off axis location in
front of the antenna can be determined based on the dish diameter rule (Item 6.0). Assuming a flat
terrain in front of the antenna, the relationship is:

 S = (D/ sin α) + (2h - D - 2)/(2 tan α) (7)
 Where: α = minimum elevation angle of antenna
         D = dish diameter in meters
         h = maximum height of object to be cleared, meters

For distances equal or greater than determined by equation (7), the radiation hazard will be below
safe levels for all but the most powerful stations (> 4 kilowatts RF at the feed).

   For          D=           1.2 meters
                h=           2.0 meters
   Then:
                α            S
                5            18.3 meters
                10           9.2meters
                15           6.1 meters
                20           4.6 meters
                25           3.7 meters

9.0 Summary

The earth station site will be protected from uncontrolled access with barriers and other
means. There will also be proper emission warning signs placed and all operating
personnel will be aware of the human exposure levels at and around the earth station. The
applicant agrees to abide by the conditions specified in Condition 5208 provided below:

Condition 5208 - The licensee shall take all necessary measures to ensure that the
antenna does not create potential exposure of humans to radiofrequency radiation
in excess of the FCC exposure limits defined in 47 CFR 1.1307(b) and 1.1310 wherever
such exposures might occur. Measures must be taken to ensure compliance with limits for
both occupational/controlled exposure and for general population/uncontrolled


                                                                                                      4


exposure, as defined in these rule sections. Compliance can be accomplished in most
cases by appropriate restrictions such as fencing. Requirements for restrictions can be
determined by predictions based on calculations, modeling or by field measurements. The
FCC's OET Bulletin 65 (available on-line at www.fcc.gov/oet/rfsafety) provides
information on predicting exposure levels and on methods for ensuring compliance,
including the use of warning and alerting signs and protective equipment for worker.



The following table summarizes all of the above calculations:




                                                                                     5


Table : Summaryof All RadHaz Parameters                                        |GATR Technologies
Parameter                              [Abbe                          Unis     |Formin
Din#                                                          Hub
Antenna Diameter                             pr                12]_meters
Antenns Centerine                            is                1.0| meters
Antena Suface Area                           Sa                1.1]   maes® [n* DFY4
Antenna Ground Elevaton                      ce                 0.0|_meters
Frequency ofOpcration                        G                125| ofe
Wavelengh                                    X               00211] meters_|/f
HPA Ouput Power                              Pres              332] wars
HPA to Antenna Loss                          .                  0.0|__ dB |includes output backof®
Transmit Power at Flange                     o                 152] aBw _|10 * LorPred—Ls
                                                              3320] wars
Artenna Gain                                 G..               126) am
                                                           18277 8) wa
P                                        m               31415007] wa
Antenna Aperture Eficiency               n                  s7o0t| wa |6,, / @1* DeY
T. Reflector Surface Region Calculations
Refector Surface Power Densiy            |PDas              11742          las* pom*D)
                                                            11.742| miWiom |Does Not Meet Uncontrolled Limits
                                                                           [Does Not Meet Controlled Limits
2. OnAxis Near Field Calculations
Extent ofNear Field                          Re              17.10] meters [D" /( *D
                                                             500 fer
Near Field Power Densty                      PDat            seo3|    W‘       las* 1 * 2y m °D
                                                             6693] mWiem® |Does Not Meet Uncontrolled Linits
                                                                          [Does Not Meet Controlled Limits
3. On—Axis Transition Region Calculations
Extnt ofTransiion Resion (min)            Ire                17.10]  meters [D" /( *D
Extct ofTransiion Region (min)                               5609|    fer
Extnt ofTransiion Resion (mas)            Ire                4104]   metes_|(06* D3 A
Extct ofTransiion Region (man)                              1Bi61]    fea
Werst Case Transtion Resion Power Densty |PDir               sess|   W_|ae*n*P)(n*D)
                                                             6693]  mWiem® |Does Not Meet Uncontrolled Linits
                                                                            [Does Not Meet Controlled Limits
Uncontroled Environment Safe Operaing Dista Rou               113|     m    __|PDad*@abRen
Conolled Emvironment Safe Operating Distaned sc                229|    m    __|PDad*@abRec
4. On—Axis Far Field Caleulations
Disance tothe Far Field Region               lee              41.0| meters _|06*D% A
                                                            1Bi61] fea
On—Axis Power Densit in the Far Field        eog             mer|     We‘      |G,*P/G+ntR®)
                                                             2.867| mWicm" |Meets Controlled Limits
5. OMAxis Levels at the Far Ficld Limit and Beyond
Refector Surface Power Densiy             pps                o249| Wir‘        |(G., * P)/(4 * m * RF)*(GonGes)
Gon‘Ges at example angle 0 1 degre                           ao87              (Goa= 37 — 25tbe®
                                                             aoas              [Meets Uncontrolled Limits

Power density 1100 ofWfor one diameter PDs                  os93)              as * 1 +2( "D5100
removed
                                                           o.ose93           " |Meets Uncontrolled Limits
8. OfF—Axis Safe Distances from Earth Station                                  5= D mm+ Ch—D — 3@ ima)
a ~minimum elevation angle ofantemna                             3|    dz
    maximum height ofobject to be cleared. meters              20|     m
GD = Ground Elevation Delta anterna—cbstacld                   00|     m
levation angle                                       5        8 3      m
                                                    10         $2]     m
                                                    is         61l     m
                                                    20         16\     m
                                                    2s         37|     m

anve: anasmmma e oxe puwer ueroey miou se s a umm iopeuercs puprmouoer nououen capusaee on pru
ECC OE&T Buletin No. 65, Edtion 9701 August 1997, Append Apage 67



Document Created: 2012-02-07 14:42:47
Document Modified: 2012-02-07 14:42:47

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