Attachment Sea Tel RadHaz Exh

This document pretains to SES-MOD-20110629-00765 for Modification on a Satellite Earth Station filing.

IBFS_SESMOD2011062900765_890292

EXHIBIT FOR SEA TEL RADIATION HAZARD REPORTS INCLUDES RADIATION HAZARD REPORTS FOR SEA TEL 1 METER ANTENNA SEA TEL 1.2 METER ANTENNA SEA TEL 1.5 METER ANTENNA

SGeqir) 400%, 400b, 4009 + 4040 withn 4 wot+ uC Exhibit Radiation Hazard Report Page 1 of 5 Analysis of Non—lonizing Radiation for a 1.0—Meter Earth Station System This report analyzes the non—ionizing radiation levels for a 1.0—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/Uncontrolled Exposure (MPE) Frequency Range (MHz) Power Density (mW/icm") 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 (mWiecm") 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 Symbo! Formula Value Units Antenna Diameter D Input 1.0 m Antenna Surface Area Asurface 1 D/ 4 0.79 m* Feed Flange Diameter Dra Input 2.0 cm Area of Feed Flange Afa x D; 4 3.14 cm* Frequency F Input 14250 MHz Wavelength A 300 /F 0.021053 m Transmit Power P Input 3.37 W Antenna Gain (dBi) Ges Input 40.6 dBi Antenna Gain (factor) G 1 00e 11481.5 n/a Pi . T Constant . 3. 1415927 n/a Antenna Efficiency m G*/(r°D") 0.52 n/a

. Exhibit Radiation Hazard Report Page 2 of 5 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) = 28.5 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/(4 t Ry*) (2) = 3.791 W/im* = 0.379 mW/icm* 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 be determined from the following equation: Extent of the Near Field Ry = D/ (4 2) (3) =11.9 m The maximum power density in the Near Field can be determined from the following equation: Near Field Power Density Sa = 16.0 1 P / (1 D) (4) = 8.849 W/im* = 0.885 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 S =SirRu/R (5) __= 0.885 mW/cm*

Exhibit Radiation Hazard Report Page 3 of 5 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 Sia = 4000 P / Ajj (6) = 4290.817 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 Ssurface 7 4 P / Asurtface (7) = 17.163 W/im* = 1.716 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 / Asurface (8) = 4.291 W/im = 0.429 mW/icm*

Exhibit Radiation Hazard Report — Page 4 of 5 7. Summary of Calculations Table 4. Summary of Expected Radiation levels for Uncontrolled Environment Calculated Maximum Radiation Power Density Level Region (mW/icm?) Hazard Assessment 1. Far Field (R; = 28.5 m) Sq¢ 0.379 Satisfies FCC MPE 2. Near Field (R,; = 11.9 m) Sn 0.885 Satisfies FCC MPE 3. Transition Region (Ry, < R, < Ry) S; 0.885 Satisfies FCC MPE 4. Between Feed Assembly and Sta 4290.817 Potential Hazard Antenna Reflector 5. Main Reflector Scurface ____1.716 Potential Hazard 6. Between Reflector and Ground Sq 0.429 Satisfies FCC MPE Table 5. Summary of Expected Radiation levels for Controlled Environment Calculated Maximum Radiation Power Density Region Level (mW/cm*) Hazard Assessment 1. Far Field (R;= 28.5 m) Sr¢ 0.379 Satisfies FCC MPE 2. Near Field (R,,; = 11.9 m) Sat 0.885 Satisfies FCC MPE 3. Transition Region (Ry < R, < Rg) S; 0.885 Satisfies FCC MPE 4. Between Feed Assembly and Sta 4290.817 Potential Hazard Antenna Reflector . 5. Main Reflector Ssurface 1.716 Satisfies FCC MPE 6. Between Reflector and Ground Sq 0.429 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.

Exhibit Radiation Hazard Report Page 5 of 5 8. Conclusions Based upon the above analysis, it is concluded that harmful levels of radiation may exist in those regions noted for the Uncontrolled (Table 4) environment. The earth station will marked with the standard radiation hazard warnings, as well as the area in the vicinity of the earth station, to inform those in the general population, who may be working, or otherwise present on the roof, deck, and in or near, the main beam of the antenna. Finally, occupational exposure will be limited, and the transmitter will be turned off during periods of maintenance, so that the MPE standard of 5.0 mw/icm**2 will be complied with for those regions in close proximity to the main reflector, and subreflector, which could be occupied by operating personnel. 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 ofhumans to radiofrequency radiation in excess ofthe 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 limitsfor both occupational/controlled exposure andfor general population/uncontrolled exposure, as defined in these rule sections. Compliance can be accomplished in most cases by appropriate restrictions such asfencing. Requirementsfor restrictions can be determined by predictions based on calculations, modeling or byfield measurements. The FCC‘s OET Bulletin 65 (available on—line at www.fee.gov/oet/rfsafety) provides information on predicting exposure levels and on methodsfor ensuring compliance, including the use of warning and alerting signs andprotective equipmentfor worker.

Seq To) 1| meter wilthy B wat}k RUC Exhibit Radiation Hazard Report — SeaTel Model 4009 Page 1 of 5 gqlséo ’7’003,1—,‘00@, 4oD — Analysis of Non—lonizing Radiation for a 1.0—Meter Earth Station System This report analyzes the non—ionizing radiation levels for a 1.0—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/Uncontrolled Exposure (MPE) Frequency Range (MHz) Power Density (mW/icm‘*) 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/icm") 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 1.0 m Antenna Surface Area Asurface 1 D/ 4 0.79 m* Feed Flange Diameter Dia _ Input 8.1 ocm Area of Feed Flange Afa x Di *4 51.53 cm* Frequency F Input 14250 MHz Wavelength A 300 /F 0.021053 m Transmit Power P Input 6.70 W Antenna Gain (dBi) Ges Input 40.6 dBi Antenna Gain (factor) G_ 1 9c 11481.5 n/a Pi T Constant 3.1415927 n/a Antenna Efficiency n G/(r‘D") 0.52 n/a

Exhibit Radiation Hazard Report — SeaTel Model 4009 Page 2 of 5 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 R; =0.60 D/A (1) = 28.5 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/(4 1 Ry") (2) = 7.537 W/im" = 0.754 mWi/icm* 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 be determined from the following equation: Extent of the Near Field Ry = D/ (4 A) (3) =11.9 m The maximum power density in the Near Field can be determined from the following equation: Near Field Power Density Si =16.0 1 P / (1 D) (4) = 17.594 W/m* = 1.759 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 Regidn Power Density S =Sir Rnu/R (5) = 1.759 mW/icm*

Exhibit Radiation Hazard Report — SeaTel Model 4009 Page 3 of 5 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 /A (6) = 520.086 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 Ssurface 4 P / Asurface (7) = 34.123 Wim" = 3.412 mW/icm* 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 s;, = P / Agurtace (8) = 8.531 W/m" = 0.853 mW/cm*

Exhibit Radiation Hazard Report — SeaTel Model 4009 Page 4 of 5 7. Summary of Calculations Table 4. Summary of Expected Radiation levels for Uncontrolled Environment Calculated Maximum Radiation Power Density Level Region (mW/icm*) Hazard Assessment 1. Far Field (R; = 28.5 m) S¢ ©0.754 Satisfies FCC MPE 2. Near Field (Ry;= 11.9 m) Sn 1.759 Potential Hazard 3. Transition Region (Ry; < R, < Ry) St 1.759 Potential Hazard 4. Between Feed Assembly and Sra 520.086 Potential Hazard Antenna Reflector 5. Main Reflector Scurtace ___3.412 Potential Hazard 6. Between Reflector and Ground Sq 0.853 Satisfies FCC MPE Table 5. Summary of Expected Radiation levels for Controlled Environment Calculated Maximum Radiation Power Density Region Level (mW/cm*) Hazard Assessment 1. Far Field (R; = 28.5 m) S¢ 0.754 Satisfies FCC MPE 2. Near Field (R,; = 11.9 m) Sor 1.759 Satisfies FCC MPE 3. Transition Region (Ry < R, < Ry) St 1.759 Satisfies FCC MPE 4. Between Feed Assembly and Sta 520.086 Potential Hazard Antenna Reflector 5. Main Reflector Ssurface 3.412 Satisfies FCC MPE 6. Between Reflector and Ground Sq ‘0.853 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.

Exhibit Radiation Hazard Report — SeaTel Model 4009 Page 5 of 5 8. Conclusions Based upon the above analysis, it is concluded that harmful levels of radiation may exist in those regions noted for the Uncontrolled (Table 4) environment. The earth station will be mounted aboard a ship, and it is recommended that the lower edge of the antenna should be at least 2 meters above the deck. If this is not the case, additional procedures will be instituted to insure the safety of the Public in the vicinity of the antenna. The applicant will ensure that the main beam of the antenna will be pointed at least one diameter away from any buildings, or other obstacles in those areas that exceed the MPE levels. Since one diameter removed from the center of the main beam the levels are down at least 20 dB, or by a factor of 100, public safety will be ensured. The earth station will marked with the standard radiation hazard warnings, as well as the area in the vicinity of the earth station, to inform those in the general population, who may be working, or otherwise present on the roof, deck, and in or near, the main beam of the antenna. Finally, occupational exposure will be limited, and the transmitter will be turned off during periods of maintenance, so that the MPE standard of 5.0 mw/icm**2 will be complied with for those regions in close proximity to the main reflector, and subreflector, which could be occupied by operating personnel.

Seqie) 4ooY ayc 50(0 wi+h & wat4+ RPUC Exhibit Radiation Hazard Report Page 1 of 5 Analysis of Non—lonizing Radiation for a 1.2—Meter Earth Station System This report analyzes the non—ionizing radiation levels for a 1.2—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/Uncontrolled Exposure (MPE) Frequency Range (MHz) Power Density (mWicm") 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/icm*) 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 1.2 m Antenna Surface Area Asurface 1 D/ 4 1.13 m* Feed Flange Diameter Dra Input 2.0 cm Area of Feed Flange Afa x Dra */4 3.14 cm* Frequency F Input 14250 MHz Wavelength A 300 /F 0.021053 m Transmit Power P Input _: 6.73 W Antenna Gain (dBi) Ges Input 43.0 dBi Antenna Gain (factor) G 1 00e 19952.6 n/a Pi 1 Constant 3.1415927 n/a Antenna Efficiency n G/(r°D") 0.62 n/a

Exhibit Radiation Hazard Report Page 2 of 5 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) = 41.0 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/(4 1 Ry") (2) = 6.344 W/im* = 0.634 mW/icm* 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 be determined from the following equation: Extent of the Near Field Ry = D/ (4 2) (3) = 17.1 m The maximum power density in the Near Field can be determined from the following equation: Near Field Power Density Si = 16.0 1 P / (1 D) (4) = 14.811 W/im* =1.481 mW/icm* 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 = SRa /R (5) = 1.481 mW/icm*

Exhibit Radiation Hazard Report Page 3 of 5 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;a = 4000 P / Ara (6) = 8568.902 mW/icm* 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 Ssurface Z4 P / Asurtace (7) = 23.803 W/m* = 2.380 mW/icm* 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 Syg =P / Asurface (8) = 5.951 W/m* = 0.595 mW/cm*

. Exhibit Radiatiokn Hazard Report Page 4 of 5 7. Summary of Calculations Table 4. Summary of Expected Radiation levels fo'r Uncontrolled Environment Calculated Maximum Radiation Power Density Level Region (mW/icm?) Hazard Assessment 1. Far Field (R;=41.0 m) Sq 0.634 Satisfies FCC MPE 2. Near Field (Ry=17.1 m) Say 1.481 Potential Hazard 3. Transition Region (Ry < R, < Ry) St 1.481 Potential Hazard 4. Between Feed Assembly and Sta 8568.902 Potential Hazard Antenna Reflector 5. Main Reflector Ssurface 2.380 Potential Hazard 6. Between Reflector and Ground Sq 0.595 Satisfies FCC MPE Table 5. Summary of Expected Radiation levels for Controlled Environment Calculated Maximum Radiation Power Density Region Level (mW/cm") Hazard Assessment 1. Far Field (Rg;= 41.0 m) Sg¢ :0.634 Satisfies FCC MPE 2. Near Field (R,; =17.1 m) Sn 1.481 Satisfies FCC MPE 3. Transition Region (Ry < R, < Ry) S; 1.481 Satisfies FCC MPE 4. Between Feed Assembly and Sta 8568.902 Potential Hazard Antenna Reflector 5. Main Reflector Ssurface 2.380 Satisfies FCC MPE 6. Between Reflector and Ground Sq 0.595 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.

Exhibit Radiation Hazard Report Page 5 of 5 8. Conclusions Based upon the above analysis, it is concluded that harmful levels of radiation may exist in those regions noted for the Uncontrolled (Table 4) environment. The earth station will be mounted aboard a ship, and it is recommended that the lower edge of the antenna should be at least 2 meters above the deck. If this is not the case, additional procedures will be instituted to ensure the safety of the Public in the vicinity of the antenna. The applicant will ensure that the main beam of the antenna will be pointed at least one diameter away from any buildings, or other obstacies in those areas that exceed the MPE levels. Since one diameter removed from the center of the main beam the levels are down at least 20 dB, or by a factor of 100, public safety will be ensured. The earth station will marked with the standard radiation hazard warnings, as well as the area in the vicinity of the earth station, to inform those in the general population, who may be working, or otherwise present on the roof, deck, and in or near, the main beam of the antenna. Finally, occupational exposure will be limited, and the transmitter will be turned off during periods of maintenance, so that the MPE standard of 5.0 mw/icm**2 will be complied with for those regions in close proximity to the main reflector, and subreflector, which could be occupied by operating personnel. 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 ofhumans to radiofrequency radiation in excess ofthe 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 limitsfor both occupational/controlled exposure andfor general population/uncontrolled exposure, as defined in these rule sections. Compliance can be accomplished in most cases by appropriate restrictions such asfencing. Requirementsfor restrictions can be determined by predictions based on calculations, modeling or byfield measurements. The FCC‘s OET Bulletin 65 (available on—line at www.fee.gov/oet/rfsafety) provides information on predicting exposure levels and on methodsfor ensuring compliance, including the use of warning and alerting signs andprotective equipmentfor worker.

Sea Tel bool and LopI with 8 woats YEUC Exhibit Radiation Hazard Report Page 1 of 5 Analysis of Non—lonizing Radiation for a 1.5—Meter Earth Station System This report analyzes the non—ionizing radiation levels for a 1.5—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/Uncontrolled Exposure (MPE) Frequency Range (MHz) Power Density ({mW/icm*) 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 (mWicm*) 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 Symbo! Formula Value Units Antenna Diameter D Input 1.5 m Antenna Surface Area Asurface x D/ 4 _ 1.77 m* Feed Flange Diameter Dra Input 5.6 cm Area of Feed Flange Afa x Drj /4 24.63 cm* Frequency F Input 14250 MHz Wavelength A 300 / F 0.021053 m Transmit Power P Input 6.73 W Antenna Gain (dBi) Ges Input 45.1 dBi Antenna Gain (factor) G 1 00e# 32359.4 n/a Pi I Constant 3.1415927 n/a Antenna Efficiency m G*/(r°D") 0.65 n/a

Exhibit Radiation Hazard Report Page 2 of 5 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) = 64.1 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/(4 1 Ry*) (2) = 4.215 W/m* = 0.421 mW/icm* 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 be determined from the following equation: Extent of the Near Field Ry = D* / (4 A) (3) = 26.7 m The maximum power density in the Near Field can be determined from the following equation: Near Field Power Density ' Si =16.0 1 P / (x D) (4) - = 9.839 W/m* = 0.984 mW/icm* 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 Se = SRa/R (5) = 0.984 mW/cm*

. Exhibit Radiation Hazard Report Page 3 of 5 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;@ 2 4000 P / Ajj (6) = 1092.972 mW/icm* 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 7 4 P / Asurtace (7) = 15.234 W/m* = 1.523 mW/cm* 6. Region between the Reflector and the Ground Assuming uniform iumination 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 Sg =P / Agurtace (8) = 3.808 W/m = 0.381 mW/icm*

Exhibit Radiation Hazard Report | Page 4 of 5 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;= 64.1 m) ‘S¢ 0.421 Satisfies FCC MPE 2. Near Field (R,; = 26.7 m) Sn 0.984 Satisfies FCC MPE 3. Transition Region (Ry < R, < Rj) St 0.984 Satisfies FCC MPE 4. Between Feed Assembly and Sta 1092.972 Potential Hazard Antenna Reflector 5. Main Reflector Ssurface 1.523 Potential Hazard 6. Between Reflector and Ground Sq 0.381 Satisfies FCC MPE Table 5. Summary of Expected Radiation levels for Controlled Environment Calculated Maximum Radiation Power Density Region Level (mWicm*) Hazard Assessment 1. Far Field (Rg= 64.1 m) S¢ 0.421 Satisfies FCC MPE 2. Near Field (R,; = 26.7 m) Sn 0.984 Satisfies FCC MPE 3. Transition Region (Ry < R, < R;) S; 0.984 Satisfies FCC MPE 4. Between Feed Assembly and Sta 1092.972 Potential Hazard Antenna Reflector 5. Main Reflector Ssurtace 1.523 Satisfies FCC MPE 6. Between Reflector and Ground Sq 0.381 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.

Exhibit Radiation Hazard Report Page 5 of 5 8. Conclusions Based upon the above analysis, it is concluded that harmful levels of radiation may exist in those regions noted for the Uncontrolled (Table 4) environment. The earth station will marked with the standard radiation hazard warnings, as well as the area in the vicinity of the earth station, to inform those in the general population, who may be working, or otherwise present on the roof, deck, and in or near, the main beam of the antenna. Finally, occupational exposure will be limited, and the transmitter will be turned off during periods of maintenance, so that the MPE standard of 5.0 mw/icm**2 will be complied with for those regions in close proximity to the main reflector, and subreflector, which could be occupied by operating personnel. 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 ofhumans 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 limitsfor both occupational/controlled exposure andfor general population/uncontrolled exposure, as defined in these rule sections. Compliance can be accomplished in most cases by appropriate restrictions such asfencing. Requirementsfor restrictions can be determined by predictions based on calculations, modeling or byfield measurements. The FCC‘s OET Bulletin 65 (available on—line at www.fee.gov/cet/rfsafety) provides information on predicting exposure levels and on methodsfor ensuring compliance, including the use of warning and alerting signs andprotective equipmentfor worker.


Document Created: 2019-04-20 07:52:53
Document Modified: 2019-04-20 07:52:53
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