Attachment RadHaz2.pdf

This document pretains to SES-DBE-20100318-00326 for Database Entry on a Satellite Earth Station filing.

IBFS_SESDBE2010031800326_806054

4 COMSEARCH® 19700 Janelia Farm Blvd. Ashburn Virginia 20147 (703)—726—5500 November 24, 2009 Bill Buttrum ES WSA Comm NISC 222 7" Ave # 263 Anchorage, AK 99513 Re: Federal Aviation Administration Radiation Hazard Study Andrew 4.5 Meter Antenna 6 GHz — Center Frequency 6175 MHz Dear Mr. Buttrum, Attached is the radiation hazard study for the Andrew 4.5 meter antenna in support of the FCC filing for the Nikolski, Alaska site. If you have any questions, please call me at (703)—726—5665. Sincerely, COMSEARCH maleyOUeatebe Timothy O. Crutcher Senior Frequency Coordinator Microwave and Satellite Services Enclosure

Radiation Hazard Report Page 1 of 4 Analysis of Non—lonizing Radiation for a 4.5—Meter Earth Station System This report analyzes the non—lonizing radiation levels for a 4.5—meter earth station system. The analysis and calculations performed in this report comply with the methods described in the FCC Office of Engineering and Technology Bulletin, No. 65 first published in 1985 and revised in 1997 in Edition 97—01. The radiation safety limits used in the analysis are in conformance with the FCC R&O 96—326. Bulletin No. 65 and the FCC R&O specifies that there are two separate tiers of exposure limits that are dependant on the situation in which the exposure takes place and/or the status of the individuals who are subject to the exposure. The Maximum Permissible Exposure (MPE) limits for persons in a General Population/Uncontrolled environment are shown in Table 1. The General Population/Uncontrolled MPE is a function of transmit frequency and is for an exposure period of thirty minutes or less. The MPE limits for persons in an Occupational/Controlled environment are shown in Table 2. The Occupational MPE is a function of transmit frequency and is for an exposure period of six minutes or less. The purpose of the analysis described in this report is to determine the power flux density levels of the earth station in the far—field, near—field, transition region, between the subreflector or feed and main reflector surface, at the main reflector surface, and between the antenna edge and the ground and to compare these levels to the specified MPEs. Table 1. Limits for General Population/Uncontrolied Exposure (MPE) Frequency Range (MHz) __Power Density (mW/cm") 30—300 0.2 300—1500 Frequency (MHz)*(0.8/1200) 1500—100,000 1.0 Table 2. Limits for Occupational/Controlled Exposure (MPE) Frequency Range (MHz) ___Power Density (mW/em") 30—300 1.0 300—1500 Frequency (MHz)*(4.0/1200) 1500—100,000 5.0 Table 3. Formulas and Parameters Used for Determining Power Flux Densities Parameter Symbol Formula Value Units Antenna Diameter D Input 4.5 m Antenna Surface Area Asurtace 1 D*/ 4 15.90 m* Feed Flange Diameter Dis Input 9.4 cm Area of Feed Flange Ara x D;, °/4 68.96 om* Frequency F Input 6175 MHz Wavelength A 300 / F 0.048583 m Transmit Power P Input 0.83 W Antenna Gain (dBi) Gies Input 47.0 dBi Antenna Gain (factor) C 19Ce""° 50118.7 n/a Pi 1 Constant 3.1415927 n/a Antenna Efficiency n GM/(RD") 0.59 n/a

Radiation Hazard Report Page 2 of 4 1. Far Field Distance Calculation The distance to the beginning of the far field can be determined from the following equation: Distance to the Far Field Region Ry =0.60 D* /A (1) =250.1 m The maximum main beam power density in the far field can be determined from the following equation: On—Axis Power Density in the Far Field S;, =GP/(41R,") (2) = 0.053 W/m" = 0.005 mW/cm* 2. Near Field Calculation Power flux density is considered to be at a maximum value throughout the entire length of the defined Near Field region. The region is contained within a cylindrical volume having the same diameter as the antenna. Past the boundary of the Near Field region, the power density from the antenna decreases linearly with respect to increasing distance. The distance to the end of the Near Field can bedetermined from the following equation: Extent of the Near Field Ry =D*/ (4 2) (3) = 104.2 m The maximum power density in the Near Field can be determined from the following equation: Near Field Power Density Sy =16.0 1 P/(r D) (4) = 0.124 W/m* = 0.012 mW/cm* 3. Transition Region Calculation The Transition region is located between the Near and Far Field regions. The power density begins to decrease linearly with increasing distance in the Transition region. While the power density decreases inversely with distance in the Transition region, the power density decreases inversely with the square of the distance in the Far Field region. The maximum power density in the Transition region will not exceed that calculated for the Near Field region. The power density calculated in Section 1 is the highest power density the antenna can produce in any of the regions away from the antenna. The power density at a distance R, can be determined from the following equation: Transition Region Power Density St = Sn Rn/ Rt (5) = 0.012 mW/cm"

Radiation Hazard Report Page 3 of 4 4. Region between the Feed Assembly and the Antenna Reflector Transmissions from the feed assembly are directed toward the antenna reflector surface, and are confined within a conical shape defined by the type of feed assembly. The most common feed assemblies are waveguide flanges, horns or subreflectors. The energy between the feed assembly and reflector surface can be calculated by determining the power density at the feed assembly surface. This can be determined from the following equation: Power Density at the Feed Flange S = 4000 P / Ar (6) = 48.147 mW/cm"* 5. Main Reflector Region The power density in the main reflector is determined in the same manner as the power density at the feed assembly. The area is now the area of the reflector aperture and can be determined from the following equation: Power Density at the Reflector Surface Ssurtace =4 P / Asurtace (7) = 0.209 W/m* = 0.021 mW/cm* 6.. Region between the Reflector and the Ground Assuming uniform illumination of the reflector surface, the power density between the antenna and the ground can be determined from the following equation: Power Density between Reflector and Ground Sy =P / Asurtace (8) = 0.052 W/m* = 0.005 mW/cm*

Radiation Hazard Report Page 4 of 4 7. Summary of Calculations Table 4. Summary of Expected Radiation levels for Uncontrolled Environment Calculated Maximum Radiation Power Density Level Region (mW/cm") Hazard Assessment 1. Far Field (R; = 250.1 m) Sy 0.005 Satisfies FCC MPE 2. Near Field (Ry; = 104.2 m) Sry 0.012 Satisfies FCC MPE 3. Transition Region (Ry; < R;< R;) S; 0.012 Satisties FCC MPE 4. Between Feed Assembly and S 48.147 Potential Hazard Antenna Reflector 5. Main Reflector Sgurtace 0.021 Satisfies FCC MPE 6. Between Reflector and Ground Sy 0.005 Satisfies FCC MPE Table 5. Summary of Expected Radiation levels for Controlled Environment Calculated Maximum Radiation Power Density Region Level (mW/em*) Hazard Assessment 1. Far Field (Rg= 250.1 m) Sy 0.005 Satisfies FCC MPE 2. Near Field (R»; = 104.2 m) Sy 0.012 Satisfies FCC MPE 3. Transition Region (R; < R; < R;) S, 0.012 Satisfies FCC MPE 4. Between Feed Assembly and S 48.147 Potential Hazard Antenna Reflector 5. Main Reflector Ssurtace 0.021 Satisfies FCC MPE 6. Between Reflector and Ground Sq 0.005 Satisfies FCC MPE It is the applicant‘s responsibility to ensure that the public and operational personnel are not exposed to harmful levels of radiation. 8. Conclusions Based on the above analysis it is concluded that harmful levels of radiation will not exist in regions normally occupied by the public or the earth station‘s operating personnel. The transmitter will be turned off during antenna maintenance so that the FCC MPE of 5.0 mW/cm2 will be complied with for those regions with close proximity to the reflector that exceed acceptable levels.


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Document Modified: 2019-04-12 21:53:12
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