Attachment Exhibit D

This document pretains to SES-LIC-20151203-00906 for License on a Satellite Earth Station filing.

IBFS_SESLIC2015120300906_1089088

RADIATION HAZARD EVALUATION For Suman 3.7 Site Id: Anthem_PWM Antenna Id: HUB3_7A 1 Overview Determining the region around an antenna where radiation hazardous to human health is a consideration of many factors. With a parabolic dish antenna, the region is highly directional and the actual hazardous region is dependent on the antenna elevation angle. The following formulae are used to determine the near and far field regions. These regions are in the main beam of the radiation pattern, which we will assume consists of a conical angle extending +/- 3 degrees from the center axis of the antenna. The analysis contained herein predicts the radiation levels around the proposed antenna. The calculations contained in this report are in accordance with FCC guidelines as contained in CFR 47 Part 1.1310 and OET Bulletin 65. The maximum level of non-ionizing radiation to which the general public is exposed is defined for controlled and uncontrolled environments as follows: Exposure Limit Environment Power Duration Controlled - (applicable to system operators and technicians in the service area of the antenna): 5 mW/cm2 6 Minutes Uncontrolled - (applicable to general public in proximity of the antenna): 1 mW/cm2 30 Minutes 2.1 Earth Station Technical Parameters - Input Data 1A Antenna Diameter - Standard Parabola 3.7 meters 1B Antenna Diameter - Elliptical Reflector meters 1B1 Major Axis Diameter meters 1B2 Minor Axis Diameter meters 2 G = Antenna Isotropic Gain 52.3 dBi 3 h = Nominal Antenna Efficiency 68 Percent 4 Nominal Frequency 14.25 GHz 5 Maximum Transmit Power Amplifier Size 360.00 Watts 6 Number of Carriers 1 each 7 W/G Loss from Transmitter to Feed 0 dB 8 Multicarrier Fixed Backoff 0 dB 9 Desired Object Clearance Height 2 meters 2.2 Earth Station Technical Parameters - Calculated Data 10 A = Antenna Surface Area 10.75 sq meters 10A Standard Parabolic Reflector 10.75210086 sq meters 10B Elliptical Reflector 0.00 sq meters 11 D = Effective Antenna Diameter 3.7 meters 12 Total Transmit Power 360.00 Watts 13 P = Total Feed Input Power (watts) 360.00 Watts 14 E = Maximum E/S EIRP - Calculated 77.86 dBW 15 λ = Wavelength (= c/f in m/GHz) 0.0210 m/GHz 16 p = Pi 3.14159 17 Rnf = Near Field Limit (D2/4λ) 163 meters 535 feet 18 Rff = Far Field Limit (Rff=0.6D2/λ ) 390 meters 1280 feet 19 Rnf to Rff = Transition Region 163 to 390 meters 535 to 1280 feet 3 Power Density at the Antenna Surface The power density at the reflector surface is expected to exceed the safe limits. The reflector is not accessible to the public and will not present a hazard. Terminal operators and technicians receive training identifying the area as presenting high exposure levels. Procedures are incorporated requiring that transmitters are not operating when access to the reflector surface is required. The power density at the antenna reflector surface can be calculated by the expression: PDREFL = 4P/A = 13.39 mW/cm2 Where: P = Total power at the feed, milliwatts A = Total area of reflector, sq cm Evaluation: Controlled Environment (less than 5 mW/cm2 in 6 minutes): HAZARD Uncontrolled environment (less than 1 mW/cm2 in 30 minutes): Mitigation Required 4 On-Axis Power Density in the Near Field Region The Radiating Near Field Region for a parabolic, circular reflector, is defined as extending from the reflector to a distance equal to the diameter squared divided by twice the wavelength. This distance is referred to as the Rayleigh distance. In this region the power is nearly all contained within a cylinder of radius 0.5D. As a safety measure the highest possible power density is applied to the whole of this region. The power density in the Near Field Region of the antenna can be calculated by the expression:

16*P*h/̟*D2 = 9.11 mW/cm 2 Where: P = Total power at the feed, milliwatts h = Nominal antenna efficiency D = Effective antenna diameter, meters Evaluation: Controlled Environment (less than 5 mW/cm2 in 6 minutes): HAZARD Uncontrolled environment (less than 1 mW/cm2 in 30 minutes): Mitigation Required 5 On-Axis Power Density in the Transition Region The transition region is located between the Near Field and Far Field regions. The power density begins to vary inversely with distance from the antenna in the transition region. The maximum power density in this region will not exceed the power density calculated for the Near Field region. Once again the power density figures are for the On- Axis and contained with a cylinder extending within +/- 1 degree of beam center. Where the antennas are normally operated at an elevation angle typically greater than 10°, the actual safe distance in front of the antenna may be found in paragraph 10. The formula for the calculation is used to evaluate the power density at any given distance in the transition as expressed below: The power density in the On-Axis Transition Region can be calculated by the expression: PDt=(PDnf)(Rnf)/R Where: PDnf = The Near Field power density, mW/cm2 Rnf = Near Field maximum distance, meters R = Distance to point of interest For: 163 < R < 390 meters Evaluation: Controlled Environment Safe Operating Distance, meters: 297 meters Uncontrolled environment Safe Operating Distance, meters: 1485 meters 6 On-Axis Power Density in the Far Field Region The On-Axis power density in the far field region (PDff) varies inversely with the square of the distance. The calculation is performed below: The Power Density at the start of the Far Field region can be calculated by the expression: E-10log(4pR2) 15.05 dBW/m2 antilog((E-10log(4pR2)/10)/10 3.20 mW/cm 2 Evaluation: Controlled Environment (less than 5 mW/cm2 in 6 minutes): SAFE Uncontrolled environment (less than 1 mW/cm2 in 30 minutes): Mitigation Required 7 Off-Axis Power Density Levels at the Far Field Limit and Beyond In the far field region, the power is distributed in a pattern of 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) 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 0.0299 mW/cm² Evaluation: 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, off axis gain reduction techniques may be used to further reduce the power density levels. 8 Off-Axis Power Density Levels at 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 near field main beam power density. This may be calculated as follows: PDnf(off-axis) = PDnf/100 = 0.0911 mW/cm² 9 Region Between the Feed Horn and Reflector/Sub-Reflector Transmissions from the feed horn are directed toward the main reflector or the sub-reflector depending on the type of antenna (prime focus, Gregorian or Cassegrain). The transmission is confined within a conical shape defined by the feed horn. The energy between the feedhorn and the reflector/sub-reflector is assumed to be in excess of any limit for

feed horn. The energy between the feedhorn and the reflector/sub-reflector is assumed to be in excess of any limit for permissible exposure. This region is not accessible to the general public, and operators and technicians should be suitable trained and procedures in place to preclude access to this region during active transmission. 10 Evaluation of Safe Occupancy Area in Front of the Antenna The distance (L) from a vertical axis passing through the dish center to a safe off-axis point in front of the antenna can be determined based on the dish diameter. Assuming a flat terrain and a point on the horizontal plane with the center point of the antenna, the relationship is determined by the following formula: L = (D/sin a) + (2h - D - 2)/(2 tan a) Where: a = minimum elevation angle of antenna D = Dish diameter in meters h = Maximum height of object to be cleared, meters For distances equal to or greater than determined by the equation above, the radiation hazard will be below safe levels For: D= 3.7 meters h= 2 meters Safe distance for the following elevation angles (a): a - Elevation Angle (degrees) L - Safe Distance 10 16.49 meters 15 11.12 meters 20 8.48 meters 25 6.93 meters 30 5.93 meters 40 4.74 meters 50 4.12 meters 5.95 27.54 meters Site Specific 11 Mitigation Analysis Mitigation of accessibility to hazardous regions may take several forms depending on the antenna application and location. In instances such as mobile applications, the antenna may be located such that the hazardous region is not accessible during operation. An example may be in a mobile configuration where the antenna is located on top of a vehicle during operation. In other fixed installation instances the hazardous area may be fenced off to prevent access. In areas where only operators and technicians have access, training in safeguards and proper markings of hazardous areas may be sufficient. This analysis tool is designed to identify the hazardous exposure regions around an operating antenna system in accordance with the defined power density limits in CFR 47, part 1.1310 and OET bulletin 65. 12 Conclusion Based upon the above analysis, it is concluded that harmful levles of radiation may exist in those regions noted for both the Controlled and Uncontrolled environment. The antenna will either be installed on the roof of a buiding, the roof of a vehicle, or on the ground. A ground mounted antenna earth station will be surrounded by a fence, which will restrict any public access. All earth stations will be 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 might be working or otherwise present in or near the direct path of the main beam. The applicant will ensure the main beam of the antenna will be pointed at least one diameter away from any building, or other obstacles in those areas that exceed the MPE levels. Since one diameter removed from the center of the main beam will lower levels by at least 20 dB, or by a factor of 100, these potential hazards do not exist for eihter the public, or for the earth station personnel. Finally, the earth station's operating personnel will not have access to areas that exceed the MPE levels, while the earth station is in operation. The transmitter will be turned off during periods of maintenance, so that the MPE standard of 5.0 mW/cm² will be complied with for those regions in close proximity to the main reflector, which could be occupied by operating personnel.

RADIATION HAZARD EVALUATION For Suman 3.7 Site Id: Anthem_STL Antenna Id: HUB3_7A 1 Overview Determining the region around an antenna where radiation hazardous to human health is a consideration of many factors. With a parabolic dish antenna, the region is highly directional and the actual hazardous region is dependent on the antenna elevation angle. The following formulae are used to determine the near and far field regions. These regions are in the main beam of the radiation pattern, which we will assume consists of a conical angle extending +/- 3 degrees from the center axis of the antenna. The analysis contained herein predicts the radiation levels around the proposed antenna. The calculations contained in this report are in accordance with FCC guidelines as contained in CFR 47 Part 1.1310 and OET Bulletin 65. The maximum level of non-ionizing radiation to which the general public is exposed is defined for controlled and uncontrolled environments as follows: Exposure Limit Environment Power Duration Controlled - (applicable to system operators and technicians in the service area of the antenna): 5 mW/cm2 6 Minutes Uncontrolled - (applicable to general public in proximity of the antenna): 1 mW/cm2 30 Minutes 2.1 Earth Station Technical Parameters - Input Data 1A Antenna Diameter - Standard Parabola 3.7 meters 1B Antenna Diameter - Elliptical Reflector meters 1B1 Major Axis Diameter meters 1B2 Minor Axis Diameter meters 2 G = Antenna Isotropic Gain 52.3 dBi 3 h = Nominal Antenna Efficiency 68 Percent 4 Nominal Frequency 14.25 GHz 5 Maximum Transmit Power Amplifier Size 360.00 Watts 6 Number of Carriers 1 each 7 W/G Loss from Transmitter to Feed 0 dB 8 Multicarrier Fixed Backoff 0 dB 9 Desired Object Clearance Height 2 meters 2.2 Earth Station Technical Parameters - Calculated Data 10 A = Antenna Surface Area 10.75 sq meters 10A Standard Parabolic Reflector 10.75210086 sq meters 10B Elliptical Reflector 0.00 sq meters 11 D = Effective Antenna Diameter 3.7 meters 12 Total Transmit Power 360.00 Watts 13 P = Total Feed Input Power (watts) 360.00 Watts 14 E = Maximum E/S EIRP - Calculated 77.86 dBW 15 λ = Wavelength (= c/f in m/GHz) 0.0210 m/GHz 16 p = Pi 3.14159 17 Rnf = Near Field Limit (D2/4λ) 163 meters 535 feet 18 Rff = Far Field Limit (Rff=0.6D2/λ ) 390 meters 1280 feet 19 Rnf to Rff = Transition Region 163 to 390 meters 535 to 1280 feet 3 Power Density at the Antenna Surface The power density at the reflector surface is expected to exceed the safe limits. The reflector is not accessible to the public and will not present a hazard. Terminal operators and technicians receive training identifying the area as presenting high exposure levels. Procedures are incorporated requiring that transmitters are not operating when access to the reflector surface is required. The power density at the antenna reflector surface can be calculated by the expression: PDREFL = 4P/A = 13.39 mW/cm2 Where: P = Total power at the feed, milliwatts A = Total area of reflector, sq cm Evaluation: Controlled Environment (less than 5 mW/cm2 in 6 minutes): HAZARD Uncontrolled environment (less than 1 mW/cm2 in 30 minutes): Mitigation Required 4 On-Axis Power Density in the Near Field Region The Radiating Near Field Region for a parabolic, circular reflector, is defined as extending from the reflector to a distance equal to the diameter squared divided by twice the wavelength. This distance is referred to as the Rayleigh distance. In this region the power is nearly all contained within a cylinder of radius 0.5D. As a safety measure the highest possible power density is applied to the whole of this region. The power density in the Near Field Region of the antenna can be calculated by the expression:

16*P*h/̟*D2 = 9.11 mW/cm 2 Where: P = Total power at the feed, milliwatts h = Nominal antenna efficiency D = Effective antenna diameter, meters Evaluation: Controlled Environment (less than 5 mW/cm2 in 6 minutes): HAZARD Uncontrolled environment (less than 1 mW/cm2 in 30 minutes): Mitigation Required 5 On-Axis Power Density in the Transition Region The transition region is located between the Near Field and Far Field regions. The power density begins to vary inversely with distance from the antenna in the transition region. The maximum power density in this region will not exceed the power density calculated for the Near Field region. Once again the power density figures are for the On- Axis and contained with a cylinder extending within +/- 1 degree of beam center. Where the antennas are normally operated at an elevation angle typically greater than 10°, the actual safe distance in front of the antenna may be found in paragraph 10. The formula for the calculation is used to evaluate the power density at any given distance in the transition as expressed below: The power density in the On-Axis Transition Region can be calculated by the expression: PDt=(PDnf)(Rnf)/R Where: PDnf = The Near Field power density, mW/cm2 Rnf = Near Field maximum distance, meters R = Distance to point of interest For: 163 < R < 390 meters Evaluation: Controlled Environment Safe Operating Distance, meters: 297 meters Uncontrolled environment Safe Operating Distance, meters: 1485 meters 6 On-Axis Power Density in the Far Field Region The On-Axis power density in the far field region (PDff) varies inversely with the square of the distance. The calculation is performed below: The Power Density at the start of the Far Field region can be calculated by the expression: E-10log(4pR2) 15.05 dBW/m2 antilog((E-10log(4pR2)/10)/10 3.20 mW/cm 2 Evaluation: Controlled Environment (less than 5 mW/cm2 in 6 minutes): SAFE Uncontrolled environment (less than 1 mW/cm2 in 30 minutes): Mitigation Required 7 Off-Axis Power Density Levels at the Far Field Limit and Beyond In the far field region, the power is distributed in a pattern of 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) 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 0.0299 mW/cm² Evaluation: 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, off axis gain reduction techniques may be used to further reduce the power density levels. 8 Off-Axis Power Density Levels at 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 near field main beam power density. This may be calculated as follows: PDnf(off-axis) = PDnf/100 = 0.0911 mW/cm² 9 Region Between the Feed Horn and Reflector/Sub-Reflector Transmissions from the feed horn are directed toward the main reflector or the sub-reflector depending on the type of antenna (prime focus, Gregorian or Cassegrain). The transmission is confined within a conical shape defined by the feed horn. The energy between the feedhorn and the reflector/sub-reflector is assumed to be in excess of any limit for

feed horn. The energy between the feedhorn and the reflector/sub-reflector is assumed to be in excess of any limit for permissible exposure. This region is not accessible to the general public, and operators and technicians should be suitable trained and procedures in place to preclude access to this region during active transmission. 10 Evaluation of Safe Occupancy Area in Front of the Antenna The distance (L) from a vertical axis passing through the dish center to a safe off-axis point in front of the antenna can be determined based on the dish diameter. Assuming a flat terrain and a point on the horizontal plane with the center point of the antenna, the relationship is determined by the following formula: L = (D/sin a) + (2h - D - 2)/(2 tan a) Where: a = minimum elevation angle of antenna D = Dish diameter in meters h = Maximum height of object to be cleared, meters For distances equal to or greater than determined by the equation above, the radiation hazard will be below safe levels For: D= 3.7 meters h= 2 meters Safe distance for the following elevation angles (a): a - Elevation Angle (degrees) L - Safe Distance 10 16.49 meters 15 11.12 meters 20 8.48 meters 25 6.93 meters 30 5.93 meters 40 4.74 meters 50 4.12 meters 5.95 27.54 meters Site Specific 11 Mitigation Analysis Mitigation of accessibility to hazardous regions may take several forms depending on the antenna application and location. In instances such as mobile applications, the antenna may be located such that the hazardous region is not accessible during operation. An example may be in a mobile configuration where the antenna is located on top of a vehicle during operation. In other fixed installation instances the hazardous area may be fenced off to prevent access. In areas where only operators and technicians have access, training in safeguards and proper markings of hazardous areas may be sufficient. This analysis tool is designed to identify the hazardous exposure regions around an operating antenna system in accordance with the defined power density limits in CFR 47, part 1.1310 and OET bulletin 65. 12 Conclusion Based upon the above analysis, it is concluded that harmful levles of radiation may exist in those regions noted for both the Controlled and Uncontrolled environment. The antenna will either be installed on the roof of a buiding, the roof of a vehicle, or on the ground. A ground mounted antenna earth station will be surrounded by a fence, which will restrict any public access. All earth stations will be 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 might be working or otherwise present in or near the direct path of the main beam. The applicant will ensure the main beam of the antenna will be pointed at least one diameter away from any building, or other obstacles in those areas that exceed the MPE levels. Since one diameter removed from the center of the main beam will lower levels by at least 20 dB, or by a factor of 100, these potential hazards do not exist for eihter the public, or for the earth station personnel. Finally, the earth station's operating personnel will not have access to areas that exceed the MPE levels, while the earth station is in operation. The transmitter will be turned off during periods of maintenance, so that the MPE standard of 5.0 mW/cm² will be complied with for those regions in close proximity to the main reflector, which could be occupied by operating personnel.

RADIATION HAZARD EVALUATION For GD Satcom 4.8 Site Id: Anthem_SHD Antenna Id: HUB4_8A 1 Overview Determining the region around an antenna where radiation hazardous to human health is a consideration of many factors. With a parabolic dish antenna, the region is highly directional and the actual hazardous region is dependent on the antenna elevation angle. The following formulae are used to determine the near and far field regions. These regions are in the main beam of the radiation pattern, which we will assume consists of a conical angle extending +/- 3 degrees from the center axis of the antenna. The analysis contained herein predicts the radiation levels around the proposed antenna. The calculations contained in this report are in accordance with FCC guidelines as contained in CFR 47 Part 1.1310 and OET Bulletin 65. The maximum level of non-ionizing radiation to which the general public is exposed is defined for controlled and uncontrolled environments as follows: Exposure Limit Environment Power Duration Controlled - (applicable to system operators and technicians in the service area of the antenna): 5 mW/cm2 6 Minutes Uncontrolled - (applicable to general public in proximity of the antenna): 1 mW/cm2 30 Minutes 2.1 Earth Station Technical Parameters - Input Data 1A Antenna Diameter - Standard Parabola 4.8 meters 1B Antenna Diameter - Elliptical Reflector meters 1B1 Major Axis Diameter meters 1B2 Minor Axis Diameter meters 2 G = Antenna Isotropic Gain 55.2 dBi 3 h = Nominal Antenna Efficiency 68 Percent 4 Nominal Frequency 14.25 GHz 5 Maximum Transmit Power Amplifier Size 360.00 Watts 6 Number of Carriers 1 each 7 W/G Loss from Transmitter to Feed 0 dB 8 Multicarrier Fixed Backoff 0 dB 9 Desired Object Clearance Height 2 meters 2.2 Earth Station Technical Parameters - Calculated Data 10 A = Antenna Surface Area 18.10 sq meters 10A Standard Parabolic Reflector 18.09557368 sq meters 10B Elliptical Reflector 0.00 sq meters 11 D = Effective Antenna Diameter 4.8 meters 12 Total Transmit Power 360.00 Watts 13 P = Total Feed Input Power (watts) 360.00 Watts 14 E = Maximum E/S EIRP - Calculated 80.76 dBW 15 λ = Wavelength (= c/f in m/GHz) 0.0210 m/GHz 16 p = Pi 3.14159 17 Rnf = Near Field Limit (D2/4λ) 274 meters 899 feet 18 Rff = Far Field Limit (Rff=0.6D2/λ ) 657 meters 2156 feet 19 Rnf to Rff = Transition Region 274 to 657 meters 899 to 2156 feet 3 Power Density at the Antenna Surface The power density at the reflector surface is expected to exceed the safe limits. The reflector is not accessible to the public and will not present a hazard. Terminal operators and technicians receive training identifying the area as presenting high exposure levels. Procedures are incorporated requiring that transmitters are not operating when access to the reflector surface is required. The power density at the antenna reflector surface can be calculated by the expression: PDREFL = 4P/A = 7.96 mW/cm2 Where: P = Total power at the feed, milliwatts A = Total area of reflector, sq cm Evaluation: Controlled Environment (less than 5 mW/cm2 in 6 minutes): HAZARD Uncontrolled environment (less than 1 mW/cm2 in 30 minutes): Mitigation Required 4 On-Axis Power Density in the Near Field Region The Radiating Near Field Region for a parabolic, circular reflector, is defined as extending from the reflector to a distance equal to the diameter squared divided by twice the wavelength. This distance is referred to as the Rayleigh distance. In this region the power is nearly all contained within a cylinder of radius 0.5D. As a safety measure the highest possible power density is applied to the whole of this region. The power density in the Near Field Region of the antenna can be calculated by the expression:

16*P*h/̟*D2 = 5.41 mW/cm 2 Where: P = Total power at the feed, milliwatts h = Nominal antenna efficiency D = Effective antenna diameter, meters Evaluation: Controlled Environment (less than 5 mW/cm2 in 6 minutes): HAZARD Uncontrolled environment (less than 1 mW/cm2 in 30 minutes): Mitigation Required 5 On-Axis Power Density in the Transition Region The transition region is located between the Near Field and Far Field regions. The power density begins to vary inversely with distance from the antenna in the transition region. The maximum power density in this region will not exceed the power density calculated for the Near Field region. Once again the power density figures are for the On- Axis and contained with a cylinder extending within +/- 1 degree of beam center. Where the antennas are normally operated at an elevation angle typically greater than 10°, the actual safe distance in front of the antenna may be found in paragraph 10. The formula for the calculation is used to evaluate the power density at any given distance in the transition as expressed below: The power density in the On-Axis Transition Region can be calculated by the expression: PDt=(PDnf)(Rnf)/R Where: PDnf = The Near Field power density, mW/cm2 Rnf = Near Field maximum distance, meters R = Distance to point of interest For: 274 < R < 657 meters Evaluation: Controlled Environment Safe Operating Distance, meters: 296 meters Uncontrolled environment Safe Operating Distance, meters: 1482 meters 6 On-Axis Power Density in the Far Field Region The On-Axis power density in the far field region (PDff) varies inversely with the square of the distance. The calculation is performed below: The Power Density at the start of the Far Field region can be calculated by the expression: E-10log(4pR2) 13.42 dBW/m2 antilog((E-10log(4pR2)/10)/10 2.20 mW/cm 2 Evaluation: Controlled Environment (less than 5 mW/cm2 in 6 minutes): SAFE Uncontrolled environment (less than 1 mW/cm2 in 30 minutes): Mitigation Required 7 Off-Axis Power Density Levels at the Far Field Limit and Beyond In the far field region, the power is distributed in a pattern of 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) 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 0.0105 mW/cm² Evaluation: 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, off axis gain reduction techniques may be used to further reduce the power density levels. 8 Off-Axis Power Density Levels at 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 near field main beam power density. This may be calculated as follows: PDnf(off-axis) = PDnf/100 = 0.0541 mW/cm² 9 Region Between the Feed Horn and Reflector/Sub-Reflector Transmissions from the feed horn are directed toward the main reflector or the sub-reflector depending on the type of antenna (prime focus, Gregorian or Cassegrain). The transmission is confined within a conical shape defined by the feed horn. The energy between the feedhorn and the reflector/sub-reflector is assumed to be in excess of any limit for

feed horn. The energy between the feedhorn and the reflector/sub-reflector is assumed to be in excess of any limit for permissible exposure. This region is not accessible to the general public, and operators and technicians should be suitable trained and procedures in place to preclude access to this region during active transmission. 10 Evaluation of Safe Occupancy Area in Front of the Antenna The distance (L) from a vertical axis passing through the dish center to a safe off-axis point in front of the antenna can be determined based on the dish diameter. Assuming a flat terrain and a point on the horizontal plane with the center point of the antenna, the relationship is determined by the following formula: L = (D/sin a) + (2h - D - 2)/(2 tan a) Where: a = minimum elevation angle of antenna D = Dish diameter in meters h = Maximum height of object to be cleared, meters For distances equal to or greater than determined by the equation above, the radiation hazard will be below safe levels For: D= 4.8 meters h= 2 meters Safe distance for the following elevation angles (a): a - Elevation Angle (degrees) L - Safe Distance 10 19.70 meters 15 13.32 meters 20 10.19 meters 25 8.36 meters 30 7.18 meters 40 5.80 meters 50 5.09 meters 6.00 32.60 meters Site Specific 11 Mitigation Analysis Mitigation of accessibility to hazardous regions may take several forms depending on the antenna application and location. In instances such as mobile applications, the antenna may be located such that the hazardous region is not accessible during operation. An example may be in a mobile configuration where the antenna is located on top of a vehicle during operation. In other fixed installation instances the hazardous area may be fenced off to prevent access. In areas where only operators and technicians have access, training in safeguards and proper markings of hazardous areas may be sufficient. This analysis tool is designed to identify the hazardous exposure regions around an operating antenna system in accordance with the defined power density limits in CFR 47, part 1.1310 and OET bulletin 65. 12 Conclusion Based upon the above analysis, it is concluded that harmful levles of radiation may exist in those regions noted for both the Controlled and Uncontrolled environment. The antenna will either be installed on the roof of a buiding, the roof of a vehicle, or on the ground. A ground mounted antenna earth station will be surrounded by a fence, which will restrict any public access. All earth stations will be 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 might be working or otherwise present in or near the direct path of the main beam. The applicant will ensure the main beam of the antenna will be pointed at least one diameter away from any building, or other obstacles in those areas that exceed the MPE levels. Since one diameter removed from the center of the main beam will lower levels by at least 20 dB, or by a factor of 100, these potential hazards do not exist for eihter the public, or for the earth station personnel. Finally, the earth station's operating personnel will not have access to areas that exceed the MPE levels, while the earth station is in operation. The transmitter will be turned off during periods of maintenance, so that the MPE standard of 5.0 mW/cm² will be complied with for those regions in close proximity to the main reflector, which could be occupied by operating personnel.

RADIATION HAZARD EVALUATION For GD Satcom 1.2 Site Id: Remote Antenna Id: REM1_2A 1 Overview Determining the region around an antenna where radiation hazardous to human health is a consideration of many factors. With a parabolic dish antenna, the region is highly directional and the actual hazardous region is dependent on the antenna elevation angle. The following formulae are used to determine the near and far field regions. These regions are in the main beam of the radiation pattern, which we will assume consists of a conical angle extending +/- 3 degrees from the center axis of the antenna. The analysis contained herein predicts the radiation levels around the proposed antenna. The calculations contained in this report are in accordance with FCC guidelines as contained in CFR 47 Part 1.1310 and OET Bulletin 65. The maximum level of non-ionizing radiation to which the general public is exposed is defined for controlled and uncontrolled environments as follows: Exposure Limit Environment Power Duration Controlled - (applicable to system operators and technicians in the service area of the antenna): 5 mW/cm2 6 Minutes Uncontrolled - (applicable to general public in proximity of the antenna): 1 mW/cm2 30 Minutes 2.1 Earth Station Technical Parameters - Input Data 1A Antenna Diameter - Standard Parabola 1.2 meters 1B Antenna Diameter - Elliptical Reflector meters 1B1 Major Axis Diameter meters 1B2 Minor Axis Diameter meters 2 G = Antenna Isotropic Gain 43 dBi 3 h = Nominal Antenna Efficiency 68 Percent 4 Nominal Frequency 14.25 GHz 5 Maximum Transmit Power Amplifier Size 100.00 Watts 6 Number of Carriers 1 each 7 W/G Loss from Transmitter to Feed 0 dB 8 Multicarrier Fixed Backoff 0 dB 9 Desired Object Clearance Height 2 meters 2.2 Earth Station Technical Parameters - Calculated Data 10 A = Antenna Surface Area 1.13 sq meters 10A Standard Parabolic Reflector 1.130973355 sq meters 10B Elliptical Reflector 0.00 sq meters 11 D = Effective Antenna Diameter 1.2 meters 12 Total Transmit Power 100.00 Watts 13 P = Total Feed Input Power (watts) 100.00 Watts 14 E = Maximum E/S EIRP - Calculated 63.00 dBW 15 λ = Wavelength (= c/f in m/GHz) 0.0210 m/GHz 16 p = Pi 3.14159 17 Rnf = Near Field Limit (D2/4λ) 17 meters 56 feet 18 Rff = Far Field Limit (Rff=0.6D2/λ ) 41 meters 135 feet 19 Rnf to Rff = Transition Region 17 to 41 meters 56 to 135 feet 3 Power Density at the Antenna Surface The power density at the reflector surface is expected to exceed the safe limits. The reflector is not accessible to the public and will not present a hazard. Terminal operators and technicians receive training identifying the area as presenting high exposure levels. Procedures are incorporated requiring that transmitters are not operating when access to the reflector surface is required. The power density at the antenna reflector surface can be calculated by the expression: PDREFL = 4P/A = 35.37 mW/cm2 Where: P = Total power at the feed, milliwatts A = Total area of reflector, sq cm Evaluation: Controlled Environment (less than 5 mW/cm2 in 6 minutes): HAZARD Uncontrolled environment (less than 1 mW/cm2 in 30 minutes): Mitigation Required 4 On-Axis Power Density in the Near Field Region The Radiating Near Field Region for a parabolic, circular reflector, is defined as extending from the reflector to a distance equal to the diameter squared divided by twice the wavelength. This distance is referred to as the Rayleigh distance. In this region the power is nearly all contained within a cylinder of radius 0.5D. As a safety measure the highest possible power density is applied to the whole of this region. The power density in the Near Field Region of the antenna can be calculated by the expression:

16*P*h/̟*D2 = 24.05 mW/cm 2 Where: P = Total power at the feed, milliwatts h = Nominal antenna efficiency D = Effective antenna diameter, meters Evaluation: Controlled Environment (less than 5 mW/cm2 in 6 minutes): HAZARD Uncontrolled environment (less than 1 mW/cm2 in 30 minutes): Mitigation Required 5 On-Axis Power Density in the Transition Region The transition region is located between the Near Field and Far Field regions. The power density begins to vary inversely with distance from the antenna in the transition region. The maximum power density in this region will not exceed the power density calculated for the Near Field region. Once again the power density figures are for the On- Axis and contained with a cylinder extending within +/- 1 degree of beam center. Where the antennas are normally operated at an elevation angle typically greater than 10°, the actual safe distance in front of the antenna may be found in paragraph 10. The formula for the calculation is used to evaluate the power density at any given distance in the transition as expressed below: The power density in the On-Axis Transition Region can be calculated by the expression: PDt=(PDnf)(Rnf)/R Where: PDnf = The Near Field power density, mW/cm2 Rnf = Near Field maximum distance, meters R = Distance to point of interest For: 17 < R < 41 meters Evaluation: Controlled Environment Safe Operating Distance, meters: 82 meters Uncontrolled environment Safe Operating Distance, meters: 409 meters 6 On-Axis Power Density in the Far Field Region The On-Axis power density in the far field region (PDff) varies inversely with the square of the distance. The calculation is performed below: The Power Density at the start of the Far Field region can be calculated by the expression: E-10log(4pR2) 19.75 dBW/m2 antilog((E-10log(4pR2)/10)/10 9.45 mW/cm 2 Evaluation: Controlled Environment (less than 5 mW/cm2 in 6 minutes): HAZARD Uncontrolled environment (less than 1 mW/cm2 in 30 minutes): Mitigation Required 7 Off-Axis Power Density Levels at the Far Field Limit and Beyond In the far field region, the power is distributed in a pattern of 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) 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 0.7503 mW/cm² Evaluation: 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, off axis gain reduction techniques may be used to further reduce the power density levels. 8 Off-Axis Power Density Levels at 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 near field main beam power density. This may be calculated as follows: PDnf(off-axis) = PDnf/100 = 0.2405 mW/cm² 9 Region Between the Feed Horn and Reflector/Sub-Reflector Transmissions from the feed horn are directed toward the main reflector or the sub-reflector depending on the type of antenna (prime focus, Gregorian or Cassegrain). The transmission is confined within a conical shape defined by the feed horn. The energy between the feedhorn and the reflector/sub-reflector is assumed to be in excess of any limit for

feed horn. The energy between the feedhorn and the reflector/sub-reflector is assumed to be in excess of any limit for permissible exposure. This region is not accessible to the general public, and operators and technicians should be suitable trained and procedures in place to preclude access to this region during active transmission. 10 Evaluation of Safe Occupancy Area in Front of the Antenna The distance (L) from a vertical axis passing through the dish center to a safe off-axis point in front of the antenna can be determined based on the dish diameter. Assuming a flat terrain and a point on the horizontal plane with the center point of the antenna, the relationship is determined by the following formula: L = (D/sin a) + (2h - D - 2)/(2 tan a) Where: a = minimum elevation angle of antenna D = Dish diameter in meters h = Maximum height of object to be cleared, meters For distances equal to or greater than determined by the equation above, the radiation hazard will be below safe levels For: D= 1.2 meters h= 2 meters Safe distance for the following elevation angles (a): a - Elevation Angle (degrees) L - Safe Distance 10 9.18 meters 15 6.13 meters 20 4.61 meters 25 3.70 meters 30 3.09 meters 40 2.34 meters 50 1.90 meters 5.00 18.34 meters Site Specific 11 Mitigation Analysis Mitigation of accessibility to hazardous regions may take several forms depending on the antenna application and location. In instances such as mobile applications, the antenna may be located such that the hazardous region is not accessible during operation. An example may be in a mobile configuration where the antenna is located on top of a vehicle during operation. In other fixed installation instances the hazardous area may be fenced off to prevent access. In areas where only operators and technicians have access, training in safeguards and proper markings of hazardous areas may be sufficient. This analysis tool is designed to identify the hazardous exposure regions around an operating antenna system in accordance with the defined power density limits in CFR 47, part 1.1310 and OET bulletin 65. 12 Conclusion Based upon the above analysis, it is concluded that harmful levles of radiation may exist in those regions noted for both the Controlled and Uncontrolled environment. The antenna will either be installed on the roof of a buiding, the roof of a vehicle, or on the ground. A ground mounted antenna earth station will be surrounded by a fence, which will restrict any public access. All earth stations will be 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 might be working or otherwise present in or near the direct path of the main beam. The applicant will ensure the main beam of the antenna will be pointed at least one diameter away from any building, or other obstacles in those areas that exceed the MPE levels. Since one diameter removed from the center of the main beam will lower levels by at least 20 dB, or by a factor of 100, these potential hazards do not exist for eihter the public, or for the earth station personnel. Finally, the earth station's operating personnel will not have access to areas that exceed the MPE levels, while the earth station is in operation. The transmitter will be turned off during periods of maintenance, so that the MPE standard of 5.0 mW/cm² will be complied with for those regions in close proximity to the main reflector, which could be occupied by operating personnel.

RADIATION HAZARD EVALUATION For GD Satcom 1.8 Site Id: Remote Antenna Id: REM1_8A 1 Overview Determining the region around an antenna where radiation hazardous to human health is a consideration of many factors. With a parabolic dish antenna, the region is highly directional and the actual hazardous region is dependent on the antenna elevation angle. The following formulae are used to determine the near and far field regions. These regions are in the main beam of the radiation pattern, which we will assume consists of a conical angle extending +/- 3 degrees from the center axis of the antenna. The analysis contained herein predicts the radiation levels around the proposed antenna. The calculations contained in this report are in accordance with FCC guidelines as contained in CFR 47 Part 1.1310 and OET Bulletin 65. The maximum level of non-ionizing radiation to which the general public is exposed is defined for controlled and uncontrolled environments as follows: Exposure Limit Environment Power Duration Controlled - (applicable to system operators and technicians in the service area of the antenna): 5 mW/cm2 6 Minutes Uncontrolled - (applicable to general public in proximity of the antenna): 1 mW/cm2 30 Minutes 2.1 Earth Station Technical Parameters - Input Data 1A Antenna Diameter - Standard Parabola 1.8 meters 1B Antenna Diameter - Elliptical Reflector meters 1B1 Major Axis Diameter meters 1B2 Minor Axis Diameter meters 2 G = Antenna Isotropic Gain 46.7 dBi 3 h = Nominal Antenna Efficiency 68 Percent 4 Nominal Frequency 14.25 GHz 5 Maximum Transmit Power Amplifier Size 200.00 Watts 6 Number of Carriers 1 each 7 W/G Loss from Transmitter to Feed 0 dB 8 Multicarrier Fixed Backoff 0 dB 9 Desired Object Clearance Height 2 meters 2.2 Earth Station Technical Parameters - Calculated Data 10 A = Antenna Surface Area 2.54 sq meters 10A Standard Parabolic Reflector 2.544690049 sq meters 10B Elliptical Reflector 0.00 sq meters 11 D = Effective Antenna Diameter 1.8 meters 12 Total Transmit Power 200.00 Watts 13 P = Total Feed Input Power (watts) 200.00 Watts 14 E = Maximum E/S EIRP - Calculated 69.71 dBW 15 λ = Wavelength (= c/f in m/GHz) 0.0210 m/GHz 16 p = Pi 3.14159 17 Rnf = Near Field Limit (D2/4λ) 39 meters 128 feet 18 Rff = Far Field Limit (Rff=0.6D2/λ ) 92 meters 302 feet 19 Rnf to Rff = Transition Region 39 to 92 meters 128 to 302 feet 3 Power Density at the Antenna Surface The power density at the reflector surface is expected to exceed the safe limits. The reflector is not accessible to the public and will not present a hazard. Terminal operators and technicians receive training identifying the area as presenting high exposure levels. Procedures are incorporated requiring that transmitters are not operating when access to the reflector surface is required. The power density at the antenna reflector surface can be calculated by the expression: PDREFL = 4P/A = 31.44 mW/cm2 Where: P = Total power at the feed, milliwatts A = Total area of reflector, sq cm Evaluation: Controlled Environment (less than 5 mW/cm2 in 6 minutes): HAZARD Uncontrolled environment (less than 1 mW/cm2 in 30 minutes): Mitigation Required 4 On-Axis Power Density in the Near Field Region The Radiating Near Field Region for a parabolic, circular reflector, is defined as extending from the reflector to a distance equal to the diameter squared divided by twice the wavelength. This distance is referred to as the Rayleigh distance. In this region the power is nearly all contained within a cylinder of radius 0.5D. As a safety measure the highest possible power density is applied to the whole of this region. The power density in the Near Field Region of the antenna can be calculated by the expression:

16*P*h/̟*D2 = 21.38 mW/cm 2 Where: P = Total power at the feed, milliwatts h = Nominal antenna efficiency D = Effective antenna diameter, meters Evaluation: Controlled Environment (less than 5 mW/cm2 in 6 minutes): HAZARD Uncontrolled environment (less than 1 mW/cm2 in 30 minutes): Mitigation Required 5 On-Axis Power Density in the Transition Region The transition region is located between the Near Field and Far Field regions. The power density begins to vary inversely with distance from the antenna in the transition region. The maximum power density in this region will not exceed the power density calculated for the Near Field region. Once again the power density figures are for the On- Axis and contained with a cylinder extending within +/- 1 degree of beam center. Where the antennas are normally operated at an elevation angle typically greater than 10°, the actual safe distance in front of the antenna may be found in paragraph 10. The formula for the calculation is used to evaluate the power density at any given distance in the transition as expressed below: The power density in the On-Axis Transition Region can be calculated by the expression: PDt=(PDnf)(Rnf)/R Where: PDnf = The Near Field power density, mW/cm2 Rnf = Near Field maximum distance, meters R = Distance to point of interest For: 39 < R < 92 meters Evaluation: Controlled Environment Safe Operating Distance, meters: 167 meters Uncontrolled environment Safe Operating Distance, meters: 834 meters 6 On-Axis Power Density in the Far Field Region The On-Axis power density in the far field region (PDff) varies inversely with the square of the distance. The calculation is performed below: The Power Density at the start of the Far Field region can be calculated by the expression: E-10log(4pR2) 19.44 dBW/m2 antilog((E-10log(4pR2)/10)/10 8.80 mW/cm 2 Evaluation: Controlled Environment (less than 5 mW/cm2 in 6 minutes): HAZARD Uncontrolled environment (less than 1 mW/cm2 in 30 minutes): Mitigation Required 7 Off-Axis Power Density Levels at the Far Field Limit and Beyond In the far field region, the power is distributed in a pattern of 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) 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 0.2980 mW/cm² Evaluation: 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, off axis gain reduction techniques may be used to further reduce the power density levels. 8 Off-Axis Power Density Levels at 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 near field main beam power density. This may be calculated as follows: PDnf(off-axis) = PDnf/100 = 0.2138 mW/cm² 9 Region Between the Feed Horn and Reflector/Sub-Reflector Transmissions from the feed horn are directed toward the main reflector or the sub-reflector depending on the type of antenna (prime focus, Gregorian or Cassegrain). The transmission is confined within a conical shape defined by the feed horn. The energy between the feedhorn and the reflector/sub-reflector is assumed to be in excess of any limit for

feed horn. The energy between the feedhorn and the reflector/sub-reflector is assumed to be in excess of any limit for permissible exposure. This region is not accessible to the general public, and operators and technicians should be suitable trained and procedures in place to preclude access to this region during active transmission. 10 Evaluation of Safe Occupancy Area in Front of the Antenna The distance (L) from a vertical axis passing through the dish center to a safe off-axis point in front of the antenna can be determined based on the dish diameter. Assuming a flat terrain and a point on the horizontal plane with the center point of the antenna, the relationship is determined by the following formula: L = (D/sin a) + (2h - D - 2)/(2 tan a) Where: a = minimum elevation angle of antenna D = Dish diameter in meters h = Maximum height of object to be cleared, meters For distances equal to or greater than determined by the equation above, the radiation hazard will be below safe levels For: D= 1.8 meters h= 2 meters Safe distance for the following elevation angles (a): a - Elevation Angle (degrees) L - Safe Distance 10 10.93 meters 15 7.33 meters 20 5.54 meters 25 4.47 meters 30 3.77 meters 40 2.92 meters 50 2.43 meters 5.00 21.80 meters Site Specific 11 Mitigation Analysis Mitigation of accessibility to hazardous regions may take several forms depending on the antenna application and location. In instances such as mobile applications, the antenna may be located such that the hazardous region is not accessible during operation. An example may be in a mobile configuration where the antenna is located on top of a vehicle during operation. In other fixed installation instances the hazardous area may be fenced off to prevent access. In areas where only operators and technicians have access, training in safeguards and proper markings of hazardous areas may be sufficient. This analysis tool is designed to identify the hazardous exposure regions around an operating antenna system in accordance with the defined power density limits in CFR 47, part 1.1310 and OET bulletin 65. 12 Conclusion Based upon the above analysis, it is concluded that harmful levles of radiation may exist in those regions noted for both the Controlled and Uncontrolled environment. The antenna will either be installed on the roof of a buiding, the roof of a vehicle, or on the ground. A ground mounted antenna earth station will be surrounded by a fence, which will restrict any public access. All earth stations will be 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 might be working or otherwise present in or near the direct path of the main beam. The applicant will ensure the main beam of the antenna will be pointed at least one diameter away from any building, or other obstacles in those areas that exceed the MPE levels. Since one diameter removed from the center of the main beam will lower levels by at least 20 dB, or by a factor of 100, these potential hazards do not exist for eihter the public, or for the earth station personnel. Finally, the earth station's operating personnel will not have access to areas that exceed the MPE levels, while the earth station is in operation. The transmitter will be turned off during periods of maintenance, so that the MPE standard of 5.0 mW/cm² will be complied with for those regions in close proximity to the main reflector, which could be occupied by operating personnel.

RADIATION HAZARD EVALUATION For AVL 1.8 Site Id: Remote Antenna Id: REM1_8B 1 Overview Determining the region around an antenna where radiation hazardous to human health is a consideration of many factors. With a parabolic dish antenna, the region is highly directional and the actual hazardous region is dependent on the antenna elevation angle. The following formulae are used to determine the near and far field regions. These regions are in the main beam of the radiation pattern, which we will assume consists of a conical angle extending +/- 3 degrees from the center axis of the antenna. The analysis contained herein predicts the radiation levels around the proposed antenna. The calculations contained in this report are in accordance with FCC guidelines as contained in CFR 47 Part 1.1310 and OET Bulletin 65. The maximum level of non-ionizing radiation to which the general public is exposed is defined for controlled and uncontrolled environments as follows: Exposure Limit Environment Power Duration Controlled - (applicable to system operators and technicians in the service area of the antenna): 5 mW/cm2 6 Minutes Uncontrolled - (applicable to general public in proximity of the antenna): 1 mW/cm2 30 Minutes 2.1 Earth Station Technical Parameters - Input Data 1A Antenna Diameter - Standard Parabola 1.8 meters 1B Antenna Diameter - Elliptical Reflector meters 1B1 Major Axis Diameter meters 1B2 Minor Axis Diameter meters 2 G = Antenna Isotropic Gain 46.8 dBi 3 h = Nominal Antenna Efficiency 68 Percent 4 Nominal Frequency 14.25 GHz 5 Maximum Transmit Power Amplifier Size 250.00 Watts 6 Number of Carriers 1 each 7 W/G Loss from Transmitter to Feed 0 dB 8 Multicarrier Fixed Backoff 0 dB 9 Desired Object Clearance Height 2 meters 2.2 Earth Station Technical Parameters - Calculated Data 10 A = Antenna Surface Area 2.54 sq meters 10A Standard Parabolic Reflector 2.544690049 sq meters 10B Elliptical Reflector 0.00 sq meters 11 D = Effective Antenna Diameter 1.8 meters 12 Total Transmit Power 250.00 Watts 13 P = Total Feed Input Power (watts) 250.00 Watts 14 E = Maximum E/S EIRP - Calculated 70.78 dBW 15 λ = Wavelength (= c/f in m/GHz) 0.0210 m/GHz 16 p = Pi 3.14159 17 Rnf = Near Field Limit (D2/4λ) 39 meters 128 feet 18 Rff = Far Field Limit (Rff=0.6D2/λ ) 92 meters 302 feet 19 Rnf to Rff = Transition Region 39 to 92 meters 128 to 302 feet 3 Power Density at the Antenna Surface The power density at the reflector surface is expected to exceed the safe limits. The reflector is not accessible to the public and will not present a hazard. Terminal operators and technicians receive training identifying the area as presenting high exposure levels. Procedures are incorporated requiring that transmitters are not operating when access to the reflector surface is required. The power density at the antenna reflector surface can be calculated by the expression: PDREFL = 4P/A = 39.3 mW/cm2 Where: P = Total power at the feed, milliwatts A = Total area of reflector, sq cm Evaluation: Controlled Environment (less than 5 mW/cm2 in 6 minutes): HAZARD Uncontrolled environment (less than 1 mW/cm2 in 30 minutes): Mitigation Required 4 On-Axis Power Density in the Near Field Region The Radiating Near Field Region for a parabolic, circular reflector, is defined as extending from the reflector to a distance equal to the diameter squared divided by twice the wavelength. This distance is referred to as the Rayleigh distance. In this region the power is nearly all contained within a cylinder of radius 0.5D. As a safety measure the highest possible power density is applied to the whole of this region. The power density in the Near Field Region of the antenna can be calculated by the expression:

16*P*h/̟*D2 = 26.72 mW/cm 2 Where: P = Total power at the feed, milliwatts h = Nominal antenna efficiency D = Effective antenna diameter, meters Evaluation: Controlled Environment (less than 5 mW/cm2 in 6 minutes): HAZARD Uncontrolled environment (less than 1 mW/cm2 in 30 minutes): Mitigation Required 5 On-Axis Power Density in the Transition Region The transition region is located between the Near Field and Far Field regions. The power density begins to vary inversely with distance from the antenna in the transition region. The maximum power density in this region will not exceed the power density calculated for the Near Field region. Once again the power density figures are for the On- Axis and contained with a cylinder extending within +/- 1 degree of beam center. Where the antennas are normally operated at an elevation angle typically greater than 10°, the actual safe distance in front of the antenna may be found in paragraph 10. The formula for the calculation is used to evaluate the power density at any given distance in the transition as expressed below: The power density in the On-Axis Transition Region can be calculated by the expression: PDt=(PDnf)(Rnf)/R Where: PDnf = The Near Field power density, mW/cm2 Rnf = Near Field maximum distance, meters R = Distance to point of interest For: 39 < R < 92 meters Evaluation: Controlled Environment Safe Operating Distance, meters: 208 meters Uncontrolled environment Safe Operating Distance, meters: 1042 meters 6 On-Axis Power Density in the Far Field Region The On-Axis power density in the far field region (PDff) varies inversely with the square of the distance. The calculation is performed below: The Power Density at the start of the Far Field region can be calculated by the expression: E-10log(4pR2) 20.51 dBW/m2 antilog((E-10log(4pR2)/10)/10 11.25 mW/cm 2 Evaluation: Controlled Environment (less than 5 mW/cm2 in 6 minutes): HAZARD Uncontrolled environment (less than 1 mW/cm2 in 30 minutes): Mitigation Required 7 Off-Axis Power Density Levels at the Far Field Limit and Beyond In the far field region, the power is distributed in a pattern of 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) 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 0.3725 mW/cm² Evaluation: 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, off axis gain reduction techniques may be used to further reduce the power density levels. 8 Off-Axis Power Density Levels at 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 near field main beam power density. This may be calculated as follows: PDnf(off-axis) = PDnf/100 = 0.2672 mW/cm² 9 Region Between the Feed Horn and Reflector/Sub-Reflector Transmissions from the feed horn are directed toward the main reflector or the sub-reflector depending on the type of antenna (prime focus, Gregorian or Cassegrain). The transmission is confined within a conical shape defined by the feed horn. The energy between the feedhorn and the reflector/sub-reflector is assumed to be in excess of any limit for

feed horn. The energy between the feedhorn and the reflector/sub-reflector is assumed to be in excess of any limit for permissible exposure. This region is not accessible to the general public, and operators and technicians should be suitable trained and procedures in place to preclude access to this region during active transmission. 10 Evaluation of Safe Occupancy Area in Front of the Antenna The distance (L) from a vertical axis passing through the dish center to a safe off-axis point in front of the antenna can be determined based on the dish diameter. Assuming a flat terrain and a point on the horizontal plane with the center point of the antenna, the relationship is determined by the following formula: L = (D/sin a) + (2h - D - 2)/(2 tan a) Where: a = minimum elevation angle of antenna D = Dish diameter in meters h = Maximum height of object to be cleared, meters For distances equal to or greater than determined by the equation above, the radiation hazard will be below safe levels For: D= 1.8 meters h= 2 meters Safe distance for the following elevation angles (a): a - Elevation Angle (degrees) L - Safe Distance 10 10.93 meters 15 7.33 meters 20 5.54 meters 25 4.47 meters 30 3.77 meters 40 2.92 meters 50 2.43 meters 5.00 21.80 meters Site Specific 11 Mitigation Analysis Mitigation of accessibility to hazardous regions may take several forms depending on the antenna application and location. In instances such as mobile applications, the antenna may be located such that the hazardous region is not accessible during operation. An example may be in a mobile configuration where the antenna is located on top of a vehicle during operation. In other fixed installation instances the hazardous area may be fenced off to prevent access. In areas where only operators and technicians have access, training in safeguards and proper markings of hazardous areas may be sufficient. This analysis tool is designed to identify the hazardous exposure regions around an operating antenna system in accordance with the defined power density limits in CFR 47, part 1.1310 and OET bulletin 65. 12 Conclusion Based upon the above analysis, it is concluded that harmful levles of radiation may exist in those regions noted for both the Controlled and Uncontrolled environment. The antenna will either be installed on the roof of a buiding, the roof of a vehicle, or on the ground. A ground mounted antenna earth station will be surrounded by a fence, which will restrict any public access. All earth stations will be 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 might be working or otherwise present in or near the direct path of the main beam. The applicant will ensure the main beam of the antenna will be pointed at least one diameter away from any building, or other obstacles in those areas that exceed the MPE levels. Since one diameter removed from the center of the main beam will lower levels by at least 20 dB, or by a factor of 100, these potential hazards do not exist for eihter the public, or for the earth station personnel. Finally, the earth station's operating personnel will not have access to areas that exceed the MPE levels, while the earth station is in operation. The transmitter will be turned off during periods of maintenance, so that the MPE standard of 5.0 mW/cm² will be complied with for those regions in close proximity to the main reflector, which could be occupied by operating personnel.

RADIATION HAZARD EVALUATION For AVL 1.8 Site Id: Remote Antenna Id: REM1_8C 1 Overview Determining the region around an antenna where radiation hazardous to human health is a consideration of many factors. With a parabolic dish antenna, the region is highly directional and the actual hazardous region is dependent on the antenna elevation angle. The following formulae are used to determine the near and far field regions. These regions are in the main beam of the radiation pattern, which we will assume consists of a conical angle extending +/- 3 degrees from the center axis of the antenna. The analysis contained herein predicts the radiation levels around the proposed antenna. The calculations contained in this report are in accordance with FCC guidelines as contained in CFR 47 Part 1.1310 and OET Bulletin 65. The maximum level of non-ionizing radiation to which the general public is exposed is defined for controlled and uncontrolled environments as follows: Exposure Limit Environment Power Duration Controlled - (applicable to system operators and technicians in the service area of the antenna): 5 mW/cm2 6 Minutes Uncontrolled - (applicable to general public in proximity of the antenna): 1 mW/cm2 30 Minutes 2.1 Earth Station Technical Parameters - Input Data 1A Antenna Diameter - Standard Parabola 1.8 meters 1B Antenna Diameter - Elliptical Reflector meters 1B1 Major Axis Diameter meters 1B2 Minor Axis Diameter meters 2 G = Antenna Isotropic Gain 46.7 dBi 3 h = Nominal Antenna Efficiency 68 Percent 4 Nominal Frequency 14.25 GHz 5 Maximum Transmit Power Amplifier Size 250.00 Watts 6 Number of Carriers 1 each 7 W/G Loss from Transmitter to Feed 0 dB 8 Multicarrier Fixed Backoff 0 dB 9 Desired Object Clearance Height 2 meters 2.2 Earth Station Technical Parameters - Calculated Data 10 A = Antenna Surface Area 2.54 sq meters 10A Standard Parabolic Reflector 2.544690049 sq meters 10B Elliptical Reflector 0.00 sq meters 11 D = Effective Antenna Diameter 1.8 meters 12 Total Transmit Power 250.00 Watts 13 P = Total Feed Input Power (watts) 250.00 Watts 14 E = Maximum E/S EIRP - Calculated 70.68 dBW 15 λ = Wavelength (= c/f in m/GHz) 0.0210 m/GHz 16 p = Pi 3.14159 17 Rnf = Near Field Limit (D2/4λ) 39 meters 128 feet 18 Rff = Far Field Limit (Rff=0.6D2/λ ) 92 meters 302 feet 19 Rnf to Rff = Transition Region 39 to 92 meters 128 to 302 feet 3 Power Density at the Antenna Surface The power density at the reflector surface is expected to exceed the safe limits. The reflector is not accessible to the public and will not present a hazard. Terminal operators and technicians receive training identifying the area as presenting high exposure levels. Procedures are incorporated requiring that transmitters are not operating when access to the reflector surface is required. The power density at the antenna reflector surface can be calculated by the expression: PDREFL = 4P/A = 39.3 mW/cm2 Where: P = Total power at the feed, milliwatts A = Total area of reflector, sq cm Evaluation: Controlled Environment (less than 5 mW/cm2 in 6 minutes): HAZARD Uncontrolled environment (less than 1 mW/cm2 in 30 minutes): Mitigation Required 4 On-Axis Power Density in the Near Field Region The Radiating Near Field Region for a parabolic, circular reflector, is defined as extending from the reflector to a distance equal to the diameter squared divided by twice the wavelength. This distance is referred to as the Rayleigh distance. In this region the power is nearly all contained within a cylinder of radius 0.5D. As a safety measure the highest possible power density is applied to the whole of this region. The power density in the Near Field Region of the antenna can be calculated by the expression:

16*P*h/̟*D2 = 26.72 mW/cm 2 Where: P = Total power at the feed, milliwatts h = Nominal antenna efficiency D = Effective antenna diameter, meters Evaluation: Controlled Environment (less than 5 mW/cm2 in 6 minutes): HAZARD Uncontrolled environment (less than 1 mW/cm2 in 30 minutes): Mitigation Required 5 On-Axis Power Density in the Transition Region The transition region is located between the Near Field and Far Field regions. The power density begins to vary inversely with distance from the antenna in the transition region. The maximum power density in this region will not exceed the power density calculated for the Near Field region. Once again the power density figures are for the On- Axis and contained with a cylinder extending within +/- 1 degree of beam center. Where the antennas are normally operated at an elevation angle typically greater than 10°, the actual safe distance in front of the antenna may be found in paragraph 10. The formula for the calculation is used to evaluate the power density at any given distance in the transition as expressed below: The power density in the On-Axis Transition Region can be calculated by the expression: PDt=(PDnf)(Rnf)/R Where: PDnf = The Near Field power density, mW/cm2 Rnf = Near Field maximum distance, meters R = Distance to point of interest For: 39 < R < 92 meters Evaluation: Controlled Environment Safe Operating Distance, meters: 208 meters Uncontrolled environment Safe Operating Distance, meters: 1042 meters 6 On-Axis Power Density in the Far Field Region The On-Axis power density in the far field region (PDff) varies inversely with the square of the distance. The calculation is performed below: The Power Density at the start of the Far Field region can be calculated by the expression: E-10log(4pR2) 20.41 dBW/m2 antilog((E-10log(4pR2)/10)/10 10.99 mW/cm 2 Evaluation: Controlled Environment (less than 5 mW/cm2 in 6 minutes): HAZARD Uncontrolled environment (less than 1 mW/cm2 in 30 minutes): Mitigation Required 7 Off-Axis Power Density Levels at the Far Field Limit and Beyond In the far field region, the power is distributed in a pattern of 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) 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 0.3725 mW/cm² Evaluation: 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, off axis gain reduction techniques may be used to further reduce the power density levels. 8 Off-Axis Power Density Levels at 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 near field main beam power density. This may be calculated as follows: PDnf(off-axis) = PDnf/100 = 0.2672 mW/cm² 9 Region Between the Feed Horn and Reflector/Sub-Reflector Transmissions from the feed horn are directed toward the main reflector or the sub-reflector depending on the type of antenna (prime focus, Gregorian or Cassegrain). The transmission is confined within a conical shape defined by the feed horn. The energy between the feedhorn and the reflector/sub-reflector is assumed to be in excess of any limit for

feed horn. The energy between the feedhorn and the reflector/sub-reflector is assumed to be in excess of any limit for permissible exposure. This region is not accessible to the general public, and operators and technicians should be suitable trained and procedures in place to preclude access to this region during active transmission. 10 Evaluation of Safe Occupancy Area in Front of the Antenna The distance (L) from a vertical axis passing through the dish center to a safe off-axis point in front of the antenna can be determined based on the dish diameter. Assuming a flat terrain and a point on the horizontal plane with the center point of the antenna, the relationship is determined by the following formula: L = (D/sin a) + (2h - D - 2)/(2 tan a) Where: a = minimum elevation angle of antenna D = Dish diameter in meters h = Maximum height of object to be cleared, meters For distances equal to or greater than determined by the equation above, the radiation hazard will be below safe levels For: D= 1.8 meters h= 2 meters Safe distance for the following elevation angles (a): a - Elevation Angle (degrees) L - Safe Distance 10 10.93 meters 15 7.33 meters 20 5.54 meters 25 4.47 meters 30 3.77 meters 40 2.92 meters 50 2.43 meters 5.00 21.80 meters Site Specific 11 Mitigation Analysis Mitigation of accessibility to hazardous regions may take several forms depending on the antenna application and location. In instances such as mobile applications, the antenna may be located such that the hazardous region is not accessible during operation. An example may be in a mobile configuration where the antenna is located on top of a vehicle during operation. In other fixed installation instances the hazardous area may be fenced off to prevent access. In areas where only operators and technicians have access, training in safeguards and proper markings of hazardous areas may be sufficient. This analysis tool is designed to identify the hazardous exposure regions around an operating antenna system in accordance with the defined power density limits in CFR 47, part 1.1310 and OET bulletin 65. 12 Conclusion Based upon the above analysis, it is concluded that harmful levles of radiation may exist in those regions noted for both the Controlled and Uncontrolled environment. The antenna will either be installed on the roof of a buiding, the roof of a vehicle, or on the ground. A ground mounted antenna earth station will be surrounded by a fence, which will restrict any public access. All earth stations will be 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 might be working or otherwise present in or near the direct path of the main beam. The applicant will ensure the main beam of the antenna will be pointed at least one diameter away from any building, or other obstacles in those areas that exceed the MPE levels. Since one diameter removed from the center of the main beam will lower levels by at least 20 dB, or by a factor of 100, these potential hazards do not exist for eihter the public, or for the earth station personnel. Finally, the earth station's operating personnel will not have access to areas that exceed the MPE levels, while the earth station is in operation. The transmitter will be turned off during periods of maintenance, so that the MPE standard of 5.0 mW/cm² will be complied with for those regions in close proximity to the main reflector, which could be occupied by operating personnel.

RADIATION HAZARD EVALUATION For GD Satcom 2.4 Site Id: Remote Antenna Id: REM2_4A 1 Overview Determining the region around an antenna where radiation hazardous to human health is a consideration of many factors. With a parabolic dish antenna, the region is highly directional and the actual hazardous region is dependent on the antenna elevation angle. The following formulae are used to determine the near and far field regions. These regions are in the main beam of the radiation pattern, which we will assume consists of a conical angle extending +/- 3 degrees from the center axis of the antenna. The analysis contained herein predicts the radiation levels around the proposed antenna. The calculations contained in this report are in accordance with FCC guidelines as contained in CFR 47 Part 1.1310 and OET Bulletin 65. The maximum level of non-ionizing radiation to which the general public is exposed is defined for controlled and uncontrolled environments as follows: Exposure Limit Environment Power Duration Controlled - (applicable to system operators and technicians in the service area of the antenna): 5 mW/cm2 6 Minutes Uncontrolled - (applicable to general public in proximity of the antenna): 1 mW/cm2 30 Minutes 2.1 Earth Station Technical Parameters - Input Data 1A Antenna Diameter - Standard Parabola 2.4 meters 1B Antenna Diameter - Elliptical Reflector meters 1B1 Major Axis Diameter meters 1B2 Minor Axis Diameter meters 2 G = Antenna Isotropic Gain 49.2 dBi 3 h = Nominal Antenna Efficiency 68 Percent 4 Nominal Frequency 14.25 GHz 5 Maximum Transmit Power Amplifier Size 300.00 Watts 6 Number of Carriers 1 each 7 W/G Loss from Transmitter to Feed 0 dB 8 Multicarrier Fixed Backoff 0 dB 9 Desired Object Clearance Height 2 meters 2.2 Earth Station Technical Parameters - Calculated Data 10 A = Antenna Surface Area 4.52 sq meters 10A Standard Parabolic Reflector 4.523893421 sq meters 10B Elliptical Reflector 0.00 sq meters 11 D = Effective Antenna Diameter 2.4 meters 12 Total Transmit Power 300.00 Watts 13 P = Total Feed Input Power (watts) 300.00 Watts 14 E = Maximum E/S EIRP - Calculated 73.97 dBW 15 λ = Wavelength (= c/f in m/GHz) 0.0210 m/GHz 16 p = Pi 3.14159 17 Rnf = Near Field Limit (D2/4λ) 68 meters 223 feet 18 Rff = Far Field Limit (Rff=0.6D2/λ ) 164 meters 538 feet 19 Rnf to Rff = Transition Region 68 to 164 meters 223 to 538 feet 3 Power Density at the Antenna Surface The power density at the reflector surface is expected to exceed the safe limits. The reflector is not accessible to the public and will not present a hazard. Terminal operators and technicians receive training identifying the area as presenting high exposure levels. Procedures are incorporated requiring that transmitters are not operating when access to the reflector surface is required. The power density at the antenna reflector surface can be calculated by the expression: PDREFL = 4P/A = 26.53 mW/cm2 Where: P = Total power at the feed, milliwatts A = Total area of reflector, sq cm Evaluation: Controlled Environment (less than 5 mW/cm2 in 6 minutes): HAZARD Uncontrolled environment (less than 1 mW/cm2 in 30 minutes): Mitigation Required 4 On-Axis Power Density in the Near Field Region The Radiating Near Field Region for a parabolic, circular reflector, is defined as extending from the reflector to a distance equal to the diameter squared divided by twice the wavelength. This distance is referred to as the Rayleigh distance. In this region the power is nearly all contained within a cylinder of radius 0.5D. As a safety measure the highest possible power density is applied to the whole of this region. The power density in the Near Field Region of the antenna can be calculated by the expression:

16*P*h/̟*D2 = 18.04 mW/cm 2 Where: P = Total power at the feed, milliwatts h = Nominal antenna efficiency D = Effective antenna diameter, meters Evaluation: Controlled Environment (less than 5 mW/cm2 in 6 minutes): HAZARD Uncontrolled environment (less than 1 mW/cm2 in 30 minutes): Mitigation Required 5 On-Axis Power Density in the Transition Region The transition region is located between the Near Field and Far Field regions. The power density begins to vary inversely with distance from the antenna in the transition region. The maximum power density in this region will not exceed the power density calculated for the Near Field region. Once again the power density figures are for the On- Axis and contained with a cylinder extending within +/- 1 degree of beam center. Where the antennas are normally operated at an elevation angle typically greater than 10°, the actual safe distance in front of the antenna may be found in paragraph 10. The formula for the calculation is used to evaluate the power density at any given distance in the transition as expressed below: The power density in the On-Axis Transition Region can be calculated by the expression: PDt=(PDnf)(Rnf)/R Where: PDnf = The Near Field power density, mW/cm2 Rnf = Near Field maximum distance, meters R = Distance to point of interest For: 68 < R < 164 meters Evaluation: Controlled Environment Safe Operating Distance, meters: 245 meters Uncontrolled environment Safe Operating Distance, meters: 1227 meters 6 On-Axis Power Density in the Far Field Region The On-Axis power density in the far field region (PDff) varies inversely with the square of the distance. The calculation is performed below: The Power Density at the start of the Far Field region can be calculated by the expression: E-10log(4pR2) 18.68 dBW/m2 antilog((E-10log(4pR2)/10)/10 7.38 mW/cm 2 Evaluation: Controlled Environment (less than 5 mW/cm2 in 6 minutes): HAZARD Uncontrolled environment (less than 1 mW/cm2 in 30 minutes): Mitigation Required 7 Off-Axis Power Density Levels at the Far Field Limit and Beyond In the far field region, the power is distributed in a pattern of 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) 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 0.1407 mW/cm² Evaluation: 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, off axis gain reduction techniques may be used to further reduce the power density levels. 8 Off-Axis Power Density Levels at 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 near field main beam power density. This may be calculated as follows: PDnf(off-axis) = PDnf/100 = 0.1804 mW/cm² 9 Region Between the Feed Horn and Reflector/Sub-Reflector Transmissions from the feed horn are directed toward the main reflector or the sub-reflector depending on the type of antenna (prime focus, Gregorian or Cassegrain). The transmission is confined within a conical shape defined by the feed horn. The energy between the feedhorn and the reflector/sub-reflector is assumed to be in excess of any limit for

feed horn. The energy between the feedhorn and the reflector/sub-reflector is assumed to be in excess of any limit for permissible exposure. This region is not accessible to the general public, and operators and technicians should be suitable trained and procedures in place to preclude access to this region during active transmission. 10 Evaluation of Safe Occupancy Area in Front of the Antenna The distance (L) from a vertical axis passing through the dish center to a safe off-axis point in front of the antenna can be determined based on the dish diameter. Assuming a flat terrain and a point on the horizontal plane with the center point of the antenna, the relationship is determined by the following formula: L = (D/sin a) + (2h - D - 2)/(2 tan a) Where: a = minimum elevation angle of antenna D = Dish diameter in meters h = Maximum height of object to be cleared, meters For distances equal to or greater than determined by the equation above, the radiation hazard will be below safe levels For: D= 2.4 meters h= 2 meters Safe distance for the following elevation angles (a): a - Elevation Angle (degrees) L - Safe Distance 10 12.69 meters 15 8.53 meters 20 6.47 meters 25 5.25 meters 30 4.45 meters 40 3.50 meters 50 2.97 meters 5.00 25.25 meters Site Specific 11 Mitigation Analysis Mitigation of accessibility to hazardous regions may take several forms depending on the antenna application and location. In instances such as mobile applications, the antenna may be located such that the hazardous region is not accessible during operation. An example may be in a mobile configuration where the antenna is located on top of a vehicle during operation. In other fixed installation instances the hazardous area may be fenced off to prevent access. In areas where only operators and technicians have access, training in safeguards and proper markings of hazardous areas may be sufficient. This analysis tool is designed to identify the hazardous exposure regions around an operating antenna system in accordance with the defined power density limits in CFR 47, part 1.1310 and OET bulletin 65. 12 Conclusion Based upon the above analysis, it is concluded that harmful levles of radiation may exist in those regions noted for both the Controlled and Uncontrolled environment. The antenna will either be installed on the roof of a buiding, the roof of a vehicle, or on the ground. A ground mounted antenna earth station will be surrounded by a fence, which will restrict any public access. All earth stations will be 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 might be working or otherwise present in or near the direct path of the main beam. The applicant will ensure the main beam of the antenna will be pointed at least one diameter away from any building, or other obstacles in those areas that exceed the MPE levels. Since one diameter removed from the center of the main beam will lower levels by at least 20 dB, or by a factor of 100, these potential hazards do not exist for eihter the public, or for the earth station personnel. Finally, the earth station's operating personnel will not have access to areas that exceed the MPE levels, while the earth station is in operation. The transmitter will be turned off during periods of maintenance, so that the MPE standard of 5.0 mW/cm² will be complied with for those regions in close proximity to the main reflector, which could be occupied by operating personnel.

RADIATION HAZARD EVALUATION For Suman 3.7 Site Id: Remote Antenna Id: REM3_7A 1 Overview Determining the region around an antenna where radiation hazardous to human health is a consideration of many factors. With a parabolic dish antenna, the region is highly directional and the actual hazardous region is dependent on the antenna elevation angle. The following formulae are used to determine the near and far field regions. These regions are in the main beam of the radiation pattern, which we will assume consists of a conical angle extending +/- 3 degrees from the center axis of the antenna. The analysis contained herein predicts the radiation levels around the proposed antenna. The calculations contained in this report are in accordance with FCC guidelines as contained in CFR 47 Part 1.1310 and OET Bulletin 65. The maximum level of non-ionizing radiation to which the general public is exposed is defined for controlled and uncontrolled environments as follows: Exposure Limit Environment Power Duration Controlled - (applicable to system operators and technicians in the service area of the antenna): 5 mW/cm2 6 Minutes Uncontrolled - (applicable to general public in proximity of the antenna): 1 mW/cm2 30 Minutes 2.1 Earth Station Technical Parameters - Input Data 1A Antenna Diameter - Standard Parabola 3.7 meters 1B Antenna Diameter - Elliptical Reflector meters 1B1 Major Axis Diameter meters 1B2 Minor Axis Diameter meters 2 G = Antenna Isotropic Gain 52.3 dBi 3 h = Nominal Antenna Efficiency 68 Percent 4 Nominal Frequency 14.25 GHz 5 Maximum Transmit Power Amplifier Size 360.00 Watts 6 Number of Carriers 1 each 7 W/G Loss from Transmitter to Feed 0 dB 8 Multicarrier Fixed Backoff 0 dB 9 Desired Object Clearance Height 2 meters 2.2 Earth Station Technical Parameters - Calculated Data 10 A = Antenna Surface Area 10.75 sq meters 10A Standard Parabolic Reflector 10.75210086 sq meters 10B Elliptical Reflector 0.00 sq meters 11 D = Effective Antenna Diameter 3.7 meters 12 Total Transmit Power 360.00 Watts 13 P = Total Feed Input Power (watts) 360.00 Watts 14 E = Maximum E/S EIRP - Calculated 77.86 dBW 15 λ = Wavelength (= c/f in m/GHz) 0.0210 m/GHz 16 p = Pi 3.14159 17 Rnf = Near Field Limit (D2/4λ) 163 meters 535 feet 18 Rff = Far Field Limit (Rff=0.6D2/λ ) 390 meters 1280 feet 19 Rnf to Rff = Transition Region 163 to 390 meters 535 to 1280 feet 3 Power Density at the Antenna Surface The power density at the reflector surface is expected to exceed the safe limits. The reflector is not accessible to the public and will not present a hazard. Terminal operators and technicians receive training identifying the area as presenting high exposure levels. Procedures are incorporated requiring that transmitters are not operating when access to the reflector surface is required. The power density at the antenna reflector surface can be calculated by the expression: PDREFL = 4P/A = 13.39 mW/cm2 Where: P = Total power at the feed, milliwatts A = Total area of reflector, sq cm Evaluation: Controlled Environment (less than 5 mW/cm2 in 6 minutes): HAZARD Uncontrolled environment (less than 1 mW/cm2 in 30 minutes): Mitigation Required 4 On-Axis Power Density in the Near Field Region The Radiating Near Field Region for a parabolic, circular reflector, is defined as extending from the reflector to a distance equal to the diameter squared divided by twice the wavelength. This distance is referred to as the Rayleigh distance. In this region the power is nearly all contained within a cylinder of radius 0.5D. As a safety measure the highest possible power density is applied to the whole of this region. The power density in the Near Field Region of the antenna can be calculated by the expression:

16*P*h/̟*D2 = 9.11 mW/cm 2 Where: P = Total power at the feed, milliwatts h = Nominal antenna efficiency D = Effective antenna diameter, meters Evaluation: Controlled Environment (less than 5 mW/cm2 in 6 minutes): HAZARD Uncontrolled environment (less than 1 mW/cm2 in 30 minutes): Mitigation Required 5 On-Axis Power Density in the Transition Region The transition region is located between the Near Field and Far Field regions. The power density begins to vary inversely with distance from the antenna in the transition region. The maximum power density in this region will not exceed the power density calculated for the Near Field region. Once again the power density figures are for the On- Axis and contained with a cylinder extending within +/- 1 degree of beam center. Where the antennas are normally operated at an elevation angle typically greater than 10°, the actual safe distance in front of the antenna may be found in paragraph 10. The formula for the calculation is used to evaluate the power density at any given distance in the transition as expressed below: The power density in the On-Axis Transition Region can be calculated by the expression: PDt=(PDnf)(Rnf)/R Where: PDnf = The Near Field power density, mW/cm2 Rnf = Near Field maximum distance, meters R = Distance to point of interest For: 163 < R < 390 meters Evaluation: Controlled Environment Safe Operating Distance, meters: 297 meters Uncontrolled environment Safe Operating Distance, meters: 1485 meters 6 On-Axis Power Density in the Far Field Region The On-Axis power density in the far field region (PDff) varies inversely with the square of the distance. The calculation is performed below: The Power Density at the start of the Far Field region can be calculated by the expression: E-10log(4pR2) 15.05 dBW/m2 antilog((E-10log(4pR2)/10)/10 3.20 mW/cm 2 Evaluation: Controlled Environment (less than 5 mW/cm2 in 6 minutes): SAFE Uncontrolled environment (less than 1 mW/cm2 in 30 minutes): Mitigation Required 7 Off-Axis Power Density Levels at the Far Field Limit and Beyond In the far field region, the power is distributed in a pattern of 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) 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 0.0299 mW/cm² Evaluation: 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, off axis gain reduction techniques may be used to further reduce the power density levels. 8 Off-Axis Power Density Levels at 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 near field main beam power density. This may be calculated as follows: PDnf(off-axis) = PDnf/100 = 0.0911 mW/cm² 9 Region Between the Feed Horn and Reflector/Sub-Reflector Transmissions from the feed horn are directed toward the main reflector or the sub-reflector depending on the type of antenna (prime focus, Gregorian or Cassegrain). The transmission is confined within a conical shape defined by the feed horn. The energy between the feedhorn and the reflector/sub-reflector is assumed to be in excess of any limit for

feed horn. The energy between the feedhorn and the reflector/sub-reflector is assumed to be in excess of any limit for permissible exposure. This region is not accessible to the general public, and operators and technicians should be suitable trained and procedures in place to preclude access to this region during active transmission. 10 Evaluation of Safe Occupancy Area in Front of the Antenna The distance (L) from a vertical axis passing through the dish center to a safe off-axis point in front of the antenna can be determined based on the dish diameter. Assuming a flat terrain and a point on the horizontal plane with the center point of the antenna, the relationship is determined by the following formula: L = (D/sin a) + (2h - D - 2)/(2 tan a) Where: a = minimum elevation angle of antenna D = Dish diameter in meters h = Maximum height of object to be cleared, meters For distances equal to or greater than determined by the equation above, the radiation hazard will be below safe levels For: D= 3.7 meters h= 2 meters Safe distance for the following elevation angles (a): a - Elevation Angle (degrees) L - Safe Distance 10 16.49 meters 15 11.12 meters 20 8.48 meters 25 6.93 meters 30 5.93 meters 40 4.74 meters 50 4.12 meters 5.00 32.74 meters Site Specific 11 Mitigation Analysis Mitigation of accessibility to hazardous regions may take several forms depending on the antenna application and location. In instances such as mobile applications, the antenna may be located such that the hazardous region is not accessible during operation. An example may be in a mobile configuration where the antenna is located on top of a vehicle during operation. In other fixed installation instances the hazardous area may be fenced off to prevent access. In areas where only operators and technicians have access, training in safeguards and proper markings of hazardous areas may be sufficient. This analysis tool is designed to identify the hazardous exposure regions around an operating antenna system in accordance with the defined power density limits in CFR 47, part 1.1310 and OET bulletin 65. 12 Conclusion Based upon the above analysis, it is concluded that harmful levles of radiation may exist in those regions noted for both the Controlled and Uncontrolled environment. The antenna will either be installed on the roof of a buiding, the roof of a vehicle, or on the ground. A ground mounted antenna earth station will be surrounded by a fence, which will restrict any public access. All earth stations will be 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 might be working or otherwise present in or near the direct path of the main beam. The applicant will ensure the main beam of the antenna will be pointed at least one diameter away from any building, or other obstacles in those areas that exceed the MPE levels. Since one diameter removed from the center of the main beam will lower levels by at least 20 dB, or by a factor of 100, these potential hazards do not exist for eihter the public, or for the earth station personnel. Finally, the earth station's operating personnel will not have access to areas that exceed the MPE levels, while the earth station is in operation. The transmitter will be turned off during periods of maintenance, so that the MPE standard of 5.0 mW/cm² will be complied with for those regions in close proximity to the main reflector, which could be occupied by operating personnel.


Document Created: 2015-05-28 10:45:08
Document Modified: 2015-05-28 10:45:08
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