Attachment radiation-hazard2.4C

This document pretains to SES-MOD-20130117-00082 for Modification on a Satellite Earth Station filing.

IBFS_SESMOD2013011700082_981962

                   RADIATION HAZARD STUDY
                             ATCi
                     2.4m uplink C band
ATCi has evaluated the radio frequency environment in and
around
the proposed earth station and found it to be safe for
continuous
exposure of operating personnel and the general public.
Only the internal antenna structure, specifically the area
between
the feedhorn and the dish, shows a radio frequency
environment
that is considered excessive for continuous exposure of
personnel.
This area is sufficiently high above ground level that it
cannot
accidentally be entered without the aid of mechanical
equipment.
The supporting calculations that are submitted as part of
this
study show that the proposed earth station is
environmentally
safe, not only based on the criteria published in the
Occupational
Safety and Health Act (OSHA), but also in the light of
recent
recommendations for stricter control of radio frequency
radiation.
1.0 Station Parameters
Antenna Diameter (D) = 2.4 M
Operating Wavelength (λ) = .050 M
Antenna Gain (G) = 42 dBi
Transmitter RF Power (P) = 100.0 W (max)
2.0 Summary of Results
RF Power Density - Centerline of Near Field = 4.55 mw/cm²
RF Power Density - Far Field = 0.89 mw/cm²
*RF Power Density - Edge of Near Field = 0.0089 mw/cm²
*RF Power Density - Behind Antenna = 0.007 mw/cm²
* The density levels denoted by an asterisk are
representative
of the maximum radiation environment in or around the
proposed earth station to which the general public may be
exposed.

3.0 Near Field Evaluation
The earth station antenna that will be employed for this


service is designed to focus nearly all of the radiated
radio
frequency energy into a cylindrical beam with a diameter
only
slightly larger than that of the antenna dish. Any
intrusion
into this beam would impair the performance of this earth
station. This broadcaster has, therefore, selected a site
location for the antenna that will insure that the beam of
principle radio frequency radiation is clear of any
obstructions, buildings, etc. and cannot accidentally be
entered by the general public.
3.1 The near field cylindrical projection extends to a
distance
(d) that is defined by the following relationship:
d(nf)= D²/4λ
d(ff)= .6D²/λ
For the proposed antenna, the near field extends,
therefore,
to a distance of:
68.45 meters
And the far field extends, therefore, to a distance of:
164.25 meters
3.2 The maximum radio frequency power density within this
near field cylinder is a function of the antenna diameter
and transmitter power as follows:
W(nf) = 9.6P/πD²
For the proposed earth station, the maximum power density
in
the near field was computed not to exceed:
.89 mw/cm²
3.3 At the edge of the near field cylindrical beam, 0.7
antenna
diameter removed from its center, the power density is
attenuated at least 20 dB to 1/100th of the maximum near
field power. The power along the outside edge of the beam
will, therefore, not exceed:
0.0089 mw/cm²
3
4.0 Far Field Evaluation
Beyond the near field region, the cylindrical beam begins
to
spread gradually into a slightly tapered cone in accordance
with the published radiation pattern for the proposed
antenna. The specified antenna gain is realized and the
radiated power density decreases proportionally to the
inverse square of distance from the antenna.


4.1 For the purpose of determining the maximum power
density
within the far field, this broadcaster has conservatively
assumed that the full antenna gain is already realized at
the
limit of the near field cylindrical region. The radio
frequency power density in the far field region is given
by:
W(ff) = PG/4πd²
For the proposed earth station, the maximum radiated power
at
the point of transition between the near field and far
field
regions was computed not to exceed:
0.0005 mw/cm²
5.0 Off-Axis Evaluation
The proposed antenna meets or exceeds the performance
specifications under part #25 of the FCC rules. The off-
axis
gain of this antenna is, therefore, - 10dBi or less in any
direction more than 48° removed from the centerline of the
main beam.
5.1 The off-axis power density may be conservatively
evaluated
using the far field method of computation:
W (OA) = 0.1P/4πd²
Assuming a distance of 2 meters from the antenna, the
density
was calculated to be:
0.008 mw/cm²

6.0 Summary
6.1 The computed values for near field projection distance,
RF power density at the centerline, RF power density in the
far field, RF power density at the edge of the near field,
and RF power density behind the antenna are furnished by
the Engineering Department.

6.2 Radiation calculations verify that the actual
levels, which are accessible to the general given
the system design, do not exceed the OSHA maximum
of 5mw/cm² within the off-axis access areas of the
system. Antenna is also not accessible to the
general public.



Document Created: 2013-01-17 19:35:30
Document Modified: 2013-01-17 19:35:30

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