Attachment RadHaz

This document pretains to SES-LIC-20130325-00293 for License on a Satellite Earth Station filing.

IBFS_SESLIC2013032500293_991390

Analysis of Non-Ionizing Radiation for a 3.8 m Earth Station Antenna System This report analyzes the non-ionizing radiation levels for a 3.8 m 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 dependant 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 ≥ 87.651 m 1.0 mW/cm2 Satisfies FCC MPE Far field (Rff) = 411.825 m 0.219 mW/cm2 Satisfies FCC MPE Near field (Rnf) = 171.594 m 0.511 mW/cm2 Satisfies FCC MPE Transition region (Rt) (Rt) = Rnf < Rt < Rff 0.511 mW/cm2 Satisfies FCC MPE Main Reflector Surface (Ssurface) 0.786 mW/cm2 Satisfies FCC MPE Note, power density level in the area between the feed and the reflector surface is greater than the reflector surface and is assumed to be a potential hazard.

Conclusions The proposed earth station system will be located at a commercial satellite communications gateway facility with controlled access and will be serviced by trained personnel. While the power level at the reflector surface is below the threshold for uncontrolled or occupational access, levels between the reflector and the feed area are presumed to be a potential hazard; therefore, no access to this area will be permitted when the transmitter is turned on. Based on the above analysis it is concluded that no hazard exists for the public or for trained personnel.

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: Ssurface = maximum power density at the antenna surface Snf = maximum near-field power density St = power density in the transition region Sff = power density (on axis) Rnf = extent of near-field Rff = distance to the beginning of the far-field R = distance to point of interest Pa = 25 W maximum power amplifier output Lfs = 0.5 dB loss between power amplifier and antenna feed P = 22.3 W power fed to the antenna in Watts 2 A = 11.341 m physical area of the aperture antenna G = 2.093 x 105 power gain relative to an isotropic radiator D = 3.8 m diameter of antenna in meters F = 14250 frequency in MHz  = 0.021 m wavelength in meters (300/FMHz)  = 0.65 aperture efficiency Antenna Surface. The maximum power density directly in front of an antenna (e.g., at the antenna surface) can be approximated by the following equation: Ssurface = (4 * P) / A (1.1) = (4 * 22.3 W) / 11.341 m2 = 0.786 mW/cm2 Near Field Region. In the near-field or Fresnel region, 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 (D and  in same units): Rnf = D2 / (4 * ) (1.2) = (3.8 m)2 / (4 * 0.021 m) = 171.594 m

The magnitude of the on-axis (main beam) 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: Snf = (16 *  * P) / ( * D2) (1.3) = (16 * 0.65 * 22.3 W) / ( * (3.8 m)2) = 0.511 mW/cm2 Transition Region. Power density in the transition region decreases inversely with distance from the antenna, while power density in the far field (Fraunhofer region) of the antenna decreases inversely with the square of the distance. The transition region will then be the region extending from Rnf to Rff. If the location of interest falls within this transition region, the on-axis power density can be determined from the following equation: St = (Snf * Rnf) / R (1.4) = (0.511 mW/cm2 * 171.594 m) / R = (87.651 m * mW/cm2) / R where R is the location of interest in meters 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) /  (1.5) = (0.6 * (3.8 m)2) / 0.021 m = 411.825 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 *  * Rff2) (1.6) = (22.3 W * 2.093 * 105) / (4 *  * (411.825 m)2) = 0.219 mW/cm2

Safe Region for Uncontrolled Access. As given above, the power density in the far field region of the antenna pattern decreases inversely as the square of the distance. The distance to the point where the power density equals the 1 mW/cm2 level can be determined by the equation: R1 mW = ( (P * G) / (4 * π * 1 mW/cm2 * 10) )0.5 (1.7) = ( ( 22.3 W * 2.093 * 105) / (125.66 mW/cm^2) )0.5 = 192.641 m In this case, formula 1.7 is not applicable because the power level at the start of the far field region as calculated earlier by equation 1.6 is 0.219 mW/cm2 and therefore the 1.0 mW/cm2 power level lies in the transition region. Formula 1.4 may be manipulated as follows to determine the exact distance to the 5 mW/cm2 power level: R1 mW = (Snf * Rnf) / 1 mW/cm^2 (1.8) = (0.511 mW/cm2 * 171.594 m) / 1 mW/cm2 = 87.651 m


Document Created: 2011-01-25 15:31:32
Document Modified: 2011-01-25 15:31:32
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