Radiation Hazard Analyss

0015-EX-CM-2018 Text Documents

ViaSat, Inc.

2018-01-31ELS_204087

              Viasat, Inc.


     Radiation Hazard Analysis


75 cm, 1.8 m Fixed and Temporary Earth Stations
   Global Mantarray M40 Mobile Earth Station




               January 2018


Contents

1 Introduction                  2

2 Earth Station Description     2

3 Explanation of the Analysis   3

4 Results of Analysis           4

5 Conclusion                    4

6 Analysis                      5


1 Introduction

        This analysis calculates the non-ionizing radiation levels for three types of Viasat,
Inc, (“Viasat") earth station terminals (“ES terminal") namely, 75 cm and 180 cm fixed and
temporary fixed ES terminals and the Global Mantarray M40, or GM40 aeronautical earth
stations in motion (“ESIM”). These three types represent typical antenna performance for
terminals used under this experimental license operating on ViaSat-2 located at 69.9 W.L.
The calculations performed in this analysis comply with the methods described in FCC
Office of Engineering and Technology Bulletin, Number 65 (Edition 97-01) (“Bulletin 65").
This analysis demonstrates that Viasat ES terminals are compliant and will not result in
exposure levels exceeding the applicable radiation exposure limits.

        Bulletin 65 and section 1.1310 of the Commission's rules specify two separate tiers
of exposure limits: one for Occupational/Controlled Exposures and one for General
Population/Uncontrolled Exposures. Limits for Occupational/Controlled Exposures apply
in situations when persons are exposed as a consequence of their employment and are fully
aware of and can control their exposure. These limits also apply in situations when a
person is transient through a location where such limits would otherwise apply provided
the person is made aware of the potential for exposure. The limits for General
Population/Uncontrolled Exposure apply in situations in which the general public may be
exposed, or in which persons that are exposed as a consequence of their employment may
not be fully aware of the potential for exposure or cannot exercise control over their
exposure. Viasat will typically deploy its ES terminals in General Population/Uncontrolled
Environments (though in many cases the 1.8 m class ES terminal will be installed in an
enterprise environment with controlled access). Accordingly, this analysis discusses only
the Maximum Permissible Exposure (MPE) limit for those types of exposures, which is a
power density equal to 1 milliwatt per centimeter squared averaged over a thirty minute
period.

        As described in the definitional section of this document, this report analyzes the
maximum power density levels in the vicinity of a ES terminal antenna in five regions: (1)
the far field, (2) the near field, (3) the transition region between near field and far field, (4)
near the main reflector surface, and (5) between the main reflector and the feed. These
radiation regions were analyzed using the definitions and formulas in Bulletin 65 for
aperture antennas. The results of this analysis are summarized in Table 1 and Table 2,
which identify the potential exposure under nominal operating conditions and worst-case
conditions, respectively.

2 ES Terminal Description

       The ES terminals transmits bursts of information at designated times that are
assigned to the terminal by the network. The length and carrier frequency of each
transmission burst depend on the ES terminal's traffic requirements. In normal operation,


the ES terminal transmits burst traffic to the network with a nominal duty cycle of less than
6.25%.

        The ES terminal incorporates two “fail safe" features that limit the potential for
human exposure. First, the transmitter is not enabled until the receive down link
connection to the satellite has been established and an acceptable down link bit error rate
has been achieved. The transmitter is disabled very quickly, in less than 40 milliseconds, if
a loss of down connectivity occurs. This includes the case where human interference causes
degradation in the link. Transmissions will not resume until approximately 10 seconds
after downlink communications have been reestablished. Secondly, the terminal's
transmitter is not capable of operating in a continuous transmit mode of operation. The ES
terminal's outdoor unit incorporates a watchdog timer that will shut down the transmitter
if it remains in a continuous transmit state for more than 10 seconds. Under these
conditions, the transmitter will be turned off briefly then resume normal operation after an
internal reset has occurred.

3 Explanation of the Analysis

       The “Calculated Values" in Table 1, Table 2 and Table 3 show the exposure rates
calculated using the formulae from the Office of Engineering and Technology Bulletin
Number 65 (Edition 97-01) for a system with continuous (100% transmit duty cycle)
transmission. The Viasat network, however, is based on so-called “shared pipes". Viasat
terminals transmit short bursts of data periodically as instructed by the network and are
neither designed for nor capable of continuous transmission. Therefore, in order to
compute the effective radiated energy of a Viasat ES terminal, the terminal’s transmitter
duty cycle has been used to adjust the values calculated in accordance with Bulletin
Number 65. To do this, the average power during the averaging period is calculated as the
maximum transmitter peak transmit power output adjusted by the duty cycle of 6.25%.

        The MPE level calculations for the area labeled “Between feed and reflector" are
calculated based on the “fail safe" features of the Viasat ES Terminal. When the receive
signal is lost due to signal blockage, the transmitter is shut down until the receive downlink
is restored. The transmitter is shutdown in less than 40 milliseconds of the loss of the
downlink. Since the areas of high field strength near the reflector and the feed are very
sensitive to blockage of the down link, this “fail safe" feature minimizes the potential for
human exposure in the area between the feed and reflector. If the blockage due to human
exposure occurs in these areas, the down link will be interrupted causing the transmitter to
turn off almost immediately and it will remain off until the blockage is removed. After the
blockage is removed, the ES terminal will have to reacquire the receive downlink and wait
to be invited back into the network before the transmitter will be enabled. The complete
downlink recovery time is 10 seconds. Accordingly, the average power value would be
multiplied by 0.004 because the transmitter cannot transmit more than 0.4% of any rolling
30 minute period (the period over which the power density is averaged) with significant
blockage near the sub reflector and between the sub-reflector and the feed.


4 Results of Analysis

This analysis demonstrates that the Viasat ES terminals satisfy Commission requirements
because neither terminal would exceed the MPE limit of 1 milliwatt per centimeter squared
averaged over a thirty minute period when operated in the network as designed. In
particular, a fail-safe feature greatly reduces the chance of human exposure between the
feed and the reflector surface: a small blockage in this area is sufficient to cause
transmissions to cease. If the down link (receive signal) is interrupted by an object in this
area, the uplink (transmit signal) is shut down in less than 40 milliseconds and the receiver
down link recovery time is 10 seconds. The uplink will remain off until the blockage is
removed and the downlink recovery is complete. This feature, coupled with the terminal's
use of uplink power control and the non-continuous operation, ensures that the general
population will not be exposed to harmful levels of radiation that exceed Commission
standards.

5 Conclusion

This radiation hazard analysis demonstrates that Viasat ES terminals will not result in
exposure levels exceeding the applicable radiation exposure limits.


6 Analysis

Definitions
Near Field Region
The near field region is an elliptical volume co-incident with the boresight of the main
                                                                                      2
beam extending outward from the main reflector. The length of the near field is π·π‘šπ‘šπ‘š      /
(4πœ†) meters. The larger dimension οΏ½π·π‘šπ‘šπ‘š οΏ½ of the elliptical antenna is used in place of the
diameter of a circular antenna to calculate the worst case length of the near field.

Transition Region
The transition region is located between the near field region and the far field region. This
region has a power density that decreases inversely with increasing distance. Therefore the
power density in the transition region will be less than the power density in the near field
for the purpose of evaluating potential exposure.

Far Field Region
The far field region extends outward from the main reflector, beginning at a distance of
        2
οΏ½0.6 βˆ™ π·π‘šπ‘šπ‘š οΏ½/πœ† meters where the larger diameter of the elliptical antenna is π·π‘šπ‘šπ‘š . The
maximum power density is calculated using the equation recommended in Bulletin 65.

Region Between the Main Reflector and the Feed
The power radiated from the feed toward the reflector is conical in shape with the vertex at
the feed. The maximum power is at the feed mouth and can be estimated as four times the
transmit power divided by the area of the feed mouth. Note: as described above, automatic
transmit inhibit will activate when blockage between the reflector and feed occurs.

Power Density on the Antenna Surface.
The maximum power density directly in front of an antenna (e.g., at the antenna surface)
can be approximated as four times the transmit power divided by the area of the antenna
surface. Note: as described above, automatic transmit inhibit will activate when blockage
between the reflector and feed occurs.


                                     Table 1
                        Radiation from 75 cm ES Terminal
Input Parameters
Antenna Aperture Major Axis:                                  Dmaj := 77 cm
Antenna Aperture Minor Axis:                                  Dmin := 72 cm
Diameter of Feed Mouth                                        Dfeed := 5.46 cm
Frequency of Operation:                                       F := 30 GHz
Max Power into Antenna:                                       P := 25 W
Aperture Efficiency:                                          η := 0.515


Calculated Values
                                 𝑐
Wavelength:                 πœ†β‰”πΉ                         πœ† = 0.999 𝑐𝑐



                                     πœ‹π·π‘šπ‘šπ‘š π·π‘šπ‘šπ‘š
Area of Reflector:          π΄π‘Ÿπ‘Ÿπ‘Ÿ ≔                      π΄π‘Ÿπ‘Ÿπ‘Ÿ = 0.435 π‘š2
                                            4




                                        2
                                      πœ‹π·π‘“π‘“π‘“π‘“
Area of Feed Mouth:         𝐴𝑓𝑓𝑓𝑓 ≔                     𝐴𝑓𝑓𝑓𝑓 = 23.42 π‘π‘š2
                                           4




                                 4πœ‚πœ‚π΄π‘Ÿπ‘Ÿπ‘Ÿ
Antenna Gain:               𝐺≔                          𝐺 = 2.822 × 104
                                     πœ†2
                                                        𝐺 = 44.5 𝑑𝑑𝑑


                                      2
                                     π·π‘šπ‘šπ‘š
Length of Near Field:       𝑅𝑛𝑛 ≔                       𝑅𝑛𝑛 = 14.8 π‘š
                                      4πœ†




EIRP:                       𝐸𝐸𝐸𝐸 ≔ 𝑃𝑃                   𝐸𝐸𝐸𝐸 = 58.0 𝑑𝑑𝑑


                                             2
                                            π·π‘šπ‘šπ‘š
Beginning of Far Field:     𝑅𝑓𝑓 ≔ 0.6 οΏ½             οΏ½   𝑅𝑓𝑓 = 36.0 π‘š
                                                πœ†


Power Density Calculations
Far Field:
         𝑃𝑃                        π‘šπ‘š
𝑆𝑓𝑓 ≔      2    6.25%𝑆𝑓𝑓 = 0.277
        4πœ‹π‘…π‘“π‘“                      𝑐𝑐2



Near Field:
         16πœ‚πœ‚                      π‘šπ‘š
𝑆𝑛𝑛 ≔      2    6.25%𝑆𝑛𝑛 = 0.691
        πœ‹π·π‘šπ‘šπ‘š                      𝑐𝑐2


Transition Region: Power density is less than the maximum near field region power density
and greater than the minimum far field region power density.

Area between Main Reflector and Feed:
          4𝑃                               π‘šπ‘š
π‘†π‘Ÿπ‘Ÿπ‘Ÿ ≔          6.25% π‘₯ 0.4%π‘†π‘Ÿπ‘Ÿπ‘Ÿ = 0.006
         π΄π‘Ÿπ‘Ÿπ‘Ÿ                              𝑐𝑐2


Thus, the power density in each region is below the MPE limit for General
                                              π‘šπ‘š
Population/Uncontrolled Environments of 1.0 𝑐𝑐2.


                                     Table 2
                       Radiation from 180 cm ES Terminal
Input Parameters
Antenna Aperture Major Axis:                                  Dmaj := 189.6 cm
Antenna Aperture Minor Axis:                                  Dmin := 181.0 cm
Diameter of Feed Mouth                                        Dfeed := 5:46 cm
Frequency of Operation:                                       F := 30 GHz
Max Power into Antenna:                                       P := 25 W
Aperture Efficiency:                                          η := 0.515 cm


Calculated Values
                                  𝑐
Wavelength:                 πœ†β‰”πΉ                         πœ† = 0.999 𝑐𝑐



                                      πœ‹π·π‘šπ‘šπ‘š π·π‘šπ‘šπ‘š
Area of Reflector:          π΄π‘Ÿπ‘Ÿπ‘Ÿ ≔                      π΄π‘Ÿπ‘Ÿπ‘Ÿ = 2.7 π‘š2
                                            4




                                         2
                                       πœ‹π·π‘“π‘“π‘“π‘“
Area of Feed Mouth:         𝐴𝑓𝑓𝑓𝑓 ≔                     𝐴𝑓𝑓𝑓𝑓 = 23.42 π‘π‘š2
                                           4




                                  4πœ‚πœ‚π΄π‘Ÿπ‘Ÿπ‘Ÿ
Antenna Gain:               𝐺≔                          𝐺 = 1.747 × 105
                                      πœ†2
                                                        𝐺 = 52.4 𝑑𝑑𝑑


Length of Near Field:       𝑅𝑛𝑛                         𝑅𝑛𝑛 = 89.9 π‘š



EIRP:                       𝐸𝐸𝐸𝐸 ≔ 𝑃𝑃                   𝐸𝐸𝐸𝐸 = 65.9 𝑑𝑑𝑑


                                            2
                                           π·π‘šπ‘šπ‘š
Beginning of Far Field:     𝑅𝑓𝑓 ≔ 0.6 οΏ½             οΏ½   𝑅𝑓𝑓 = 215.8 π‘š
                                                πœ†


Power Density Calculations
Far Field:
         𝑃𝑃                        π‘šπ‘š
𝑆𝑓𝑓 ≔      2    6.25%𝑆𝑓𝑓 = 0.047
        4πœ‹π‘…π‘“π‘“                      𝑐𝑐2


Near Field:
         16πœ‚πœ‚                      π‘šπ‘š
𝑆𝑛𝑛 ≔      2    6.25%𝑆𝑛𝑛 = 0.114
        πœ‹π·π‘šπ‘šπ‘š                      𝑐𝑐2


Transition Region: Power density is less than the maximum near field region power density
and greater than the minimum far field region power density.

Area between Main Reflector and Feed:
          4𝑃                                π‘šπ‘š
π‘†π‘Ÿπ‘Ÿπ‘Ÿ ≔          6.25% π‘₯ 0.4%π‘†π‘Ÿπ‘Ÿπ‘Ÿ = 0.0009
         π΄π‘Ÿπ‘Ÿπ‘Ÿ                               𝑐𝑐2


Thus, the power density in each region is below the MPE limit for General
                                              π‘šπ‘š
Population/Uncontrolled Environments of 1.0 𝑐𝑐2.


                                     Table 3
                        Radiation from GM40 ES Terminal
Input Parameters
Antenna Aperture Major Axis:                                 Dmaj := 76.7 cm
Antenna Aperture Minor Axis:                                 Dmin := 15.3 cm
Frequency of Operation:                                      F := 30 GHz
Max Power into Antenna:                                      P := 31.6 W
Aperture Efficiency:                                         η := 0.75
Calculated Values
                                 𝑐
Wavelength:                 πœ†β‰”πΉ                        πœ† = 0.999 𝑐𝑐



Area of Reflector:          π΄π‘Ÿπ‘Ÿπ‘Ÿ ≔ π·π‘šπ‘šπ‘š π·π‘šπ‘šπ‘š           π΄π‘Ÿπ‘Ÿπ‘Ÿ = 0.118 π‘š2



                                 4πœ‚πœ‚π΄π‘Ÿπ‘Ÿπ‘Ÿ
Antenna Gain:               𝐺≔                         𝐺 = 1.029 × 104
                                     πœ†2
                                                       𝐺 = 40.5 𝑑𝑑𝑑


                                      2
                                     π·π‘šπ‘šπ‘š
Length of Near Field:       𝑅𝑛𝑛 ≔                      𝑅𝑛𝑛 = 14.7 π‘š
                                      4πœ†




EIRP:                       𝐸𝐸𝐸𝐸 ≔ 𝑃𝑃                  𝐸𝐸𝐸𝐸 = 58.0 𝑑𝑑𝑑


                                             2
                                            π·π‘šπ‘šπ‘š
Beginning of Far Field:     𝑅𝑓𝑓 ≔ 0.6 οΏ½            οΏ½   𝑅𝑓𝑓 = 35.3 π‘š
                                             πœ†


Power Density Calculations
Far Field:
         𝑃𝑃                       π‘šπ‘š
𝑆𝑓𝑓 ≔      2    6.25%𝑆𝑓𝑓 = 0.13
        4πœ‹π‘…π‘“π‘“                     𝑐𝑐2



Near Field:
         16πœ‚πœ‚                    π‘šπ‘š
𝑆𝑛𝑛 ≔      2    6.25%𝑆𝑛𝑛 = 1.3
        πœ‹π·π‘šπ‘šπ‘š                    𝑐𝑐2


Transition Region: Power density is less than the maximum near field region power density
and greater than the minimum far field region power density.


Aperature:
          4𝑃                              π‘šπ‘š
π‘†π‘Žπ‘Žπ‘Ž ≔          6.25% π‘₯ 0.4%π‘†π‘Žπ‘Žπ‘Ž = 0.03
         π΄π‘Žπ‘Žπ‘Ž                             𝑐𝑐2



Document Created: 2018-01-31 09:44:51
Document Modified: 2018-01-31 09:44:51

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