Attachment Exhibit B

This document pretains to SES-LIC-20130219-00187 for License on a Satellite Earth Station filing.

IBFS_SESLIC2013021900187_986515

                                         FCC Form 312
                                           Exhibit B
                                       RF Hazard Analysis


Analysis of Non-Ionizing Radiation for VMT-2100-10 Earth Station Antenna System

This report analyzes the non-ionizing radiation levels for the VMT-2100-10 earth station antenna
system.

The FCC’s Office of Engineering Technology’s Bulletin No. 65 specifies that there are two
separate tiers of exposure limits that are dependent upon the situation in which the exposure
takes place and/or the status of the individuals who are subject to the exposure. The two tiers are
General Population / Uncontrolled environment, and an Occupational / Controlled environment.

The applicable exposure limit for the General Population / Uncontrolled environment, i.e., areas
that people may enter freely, at this frequency of operation is 1 mW/cm^2 average power density
over a 30 minute period.

The applicable exposure limit for the Occupational / Controlled environment, i.e., areas that only
authorized / trained personnel have access to, at this frequency of operation is 5 mW/cm^2
average power density over a 6 minute period.


Summary of expected radiation levels for an Uncontrolled environment


Region                        Maximum Power Density                  Hazard Assessment

Safe region range (R) ≥ 0.712 m       1.0 mW/cm2                     Satisfies FCC MPE

Far field (Rff) = 0.208 m             11.7 mW/cm2                    Potential Hazard



Conclusions

The proposed earth station system will generally be mounted in a location away from users such
as on the top of a train, commercial vehicle, or automobile. During operation, the user will be
greater than 0.712 m away from the unit. Exposure is further reduced by the fact that the
maximum antenna gain (used in this analysis) occurs at a 90 degree elevation angle and is reduced
by at least 50% at an elevation angle of 15 degrees and by the fact that the device uses burst
transmissions at much less than the 100% duty cycle used for this analysis.

Based on the above analysis it is concluded that no hazard exists for the public.


Analysis

The analysis and calculations that follow in this report are performed in compliance with the
methods described in the OET Bulletin No. 65.

Definition of terms

The terms are used in the formulas here are defined as follows:
S = power density at the specified distance
Rff = distance to the beginning of the far-field
R = 0.712 m (28 in)           distance to point of interest
P=8W                          power fed to the antenna in Watts
D = 0.251 m                   effective diameter of antenna array
G = 7.95                      power gain relative to an isotropic radiator
F = 1660.5                    frequency in MHz
A. = 0.181 m                  wavelength in meters (300/FMHz)

Far-Field Region. The power density in the far-field or Fraunhofer region of the
antenna pattern decreases inversely as the square of the distance. The distance to the start of the
far field can be calculated by the following equation:

Rff    = (0.6 * D2) / A.

       = (0.6 * (0.251 m)2) / 0.181 m

       = 0.208 m

The power density at the start of the far-field region of the radiation pattern can be
estimated by the equation:

Sff    = (P * G) / (4 * it * Rff2)

       = (8 W * 7.95) / (4 * it * (0.208 m)2)

       = 11.7 mW/cm2


The power density at the point of interest in the far-field region of the radiation pattern can be
estimated by the equation:

Sff    = (P * G) / (4 * it * R2)

       = (8 W * 7.95) / (4 * it * (0.712 m)2)

       = 0.998 mW/cm2



Document Created: 2013-02-19 16:18:07
Document Modified: 2013-02-19 16:18:07

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