| |||||||||||||||
SPECIFIC ABSORPTION RATE (SAR)
Chris ZombolasView article as a pdf (248 kB)
Specific Absorption Rate (SAR)
| |||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
SAR Limits |
Occupational Workers |
Non-occupational workers |
Whole Body |
0.4 W/kg |
0.08 W/kg |
Localised Exposure:*Head and Trunk*Hands and Feet |
- | - |
10 W/kg |
2 W/kg |
|
20 W/kg |
4 W/kg |
*SAR measured in a 10g cube of tissue
Australia |
USA |
Europe |
Japan |
New Zealand |
|
ACA |
ANSIC95.1 |
ENV50166 |
TTC/MPT |
NZS2772 |
|
| Whole Body | 0.4 W/kg |
0.4 W/kg |
0.4 W/kg |
0.4 W/kg |
0.4 W/kg |
Spatial Peak |
10 W/kg |
8 W/kg |
10 W/kg |
8 W/kg |
10 W/kg |
Averaging Time |
6 min |
6 min |
6 min |
6 min |
6 min |
Averaging Time |
10g |
1g |
10g |
10g |
10g |
Shape |
Cube |
Cube |
Cube |
Cube |
Cube |
Australia |
USA |
Europe |
Japan |
New Zealand |
|
ACA |
ANSIC95.1 |
ENV50166 |
TTC/MPT |
NZS2772 |
|
| Whole Body | 0.08 W/kg |
0.08 W/kg |
0.08 W/kg |
0.04 W/kg |
0.08 W/kg |
Spatial Peak |
2W/kg |
1.6 W/kg |
2 W/kg |
2 W/kg |
2 W/kg |
Averaging Time |
6 min |
30 min |
6 min |
6 min |
|
Averaging Time |
10g |
1g |
10g |
10g |
10g |
Shape |
Cube |
Cube |
Cube |
Cube |
Cube |
In Europe and Australia, the SAR limit for MTE is 2 mW/g (2 W/kg) and
measured as an average over a 10 gram cube of tissue. In the USA and
Canada, MTE must comply with the 1.6 mW/g (1.6 W/kg) SAR limit measured
as an average in a 1 gram cube of tissue.
As can be seen from the table of SAR limits, it will not be possible to
determine worldwide compliance by testing to one limit or one standard
until international harmonisation occurs. In the meantime, manufacturers
must ensure that MTE meets the SAR limits of each target market, and
testing must be performed to the appropriate standard.
SAR is the most reliable predictor of thermally related health effects.
SAR evaluations present very restrictive specifications since very tight
margins are set with respect to the maximum permitted exposure, based on
spatially averaged peak absorption. Temperature rise measurements in a
tissue simulating liquid are extremely difficult to perform due to the
very small temperature increments to be measured (< 0.010C rise). The
effects of heat diffusion compound the measurement difficulties.
| Brain Tissue | 900 MHz | 1800 MHz | ||
| Grey brain matter | 51.4 | 1.06 | 49.5 | 1.44 |
| White brain matter | 34.0 | 0.59 | 32.6 | 0.84 |
| Homogeneous medium | 42.5 | 0.85 | 41.0 | 0.85 |
= relative permittivity
= conductivity
| Ingredients | 900 MHz | 1800 MHz |
| Water | 10.3 ℓ | 11.44 ℓ |
| Cellulose | 64.0 g | 63.8 g |
| Salt | 177.4 g | - |
| Sugar | 14.88 kg | 13.72 kg |
| Preventol | 26.8 g | 24.7 g |
| 20.0 ℓ | 20.0 ℓ | |
| Dielectric Parameters At 200C | |
|
The measurement of Electric field is the most convenient method as
E-field probes have fast time response and adequate sensitivity for SAR
measurements. The measurement of Electric field strength in the extreme
near field of the radiating antenna is however very difficult, and the
difficulties are further compounded by the interaction of the radiating
source(s) with the human body. SAR results depend on various parameters,
such as position of the RF source near the human body, posture, size,
anatomy and many other factors. The absorption and distribution of
electromagnetic energy in the body are very complex phenomena that
depend on the mass, shape and size of the body, the orientation of the
body with respect to the field vectors and the electrical properties of
both the body and environmental factors. Accurate repeatable measurement
of the electromagnetic field within human tissue and in the extreme near
field of transmitters is therefore a difficult task. The complexity of
the field distributions places great demands on measurement probes with
respect to spherical isotropy, linear response, spatial resolution,
minimal field disturbances and boundary effects.
The SAR measurement system must perform precise measurements in the
extreme near field within simulated human tissue. Ideally, it should
have sufficient flexibility in the measurement data evaluations and
visualisation capabilities to allow testing of a variety of MTE and
similar devices. It generally consists of a computer controlled high
precision robotics system to position the SAR probe, robot controller,
extreme near-field measurement probes, probe alignment sensor, and the
phantom (mannequin) containing the biological tissue equivalent liquid.
A precision 6 axis robot is generally required to precisely position the
probe at the points of maximum electromagnetic field. The SAR
measurements are made in shell models (phantoms) filled with
tissue-simulating liquids of similar dielectric properties to that of human tissue.
One of the major difficulties encountered in SAR compliance
measurements, is the location of the site of maximum SAR for a given MTE.
When the site is located, more detailed measurements are then made,
using a finer, cube-like lattice. This cube-like lattice must be located
so as to overlap the SAR maxima obtained from the previous measurement.
The entire MTE must be scanned since the location of the peak SAR is not
known nor is it intuitively obvious. In modern phones, the location of
the SAR maximum is often not at the antenna, but on the surface of the
phone in the vicinity of the keypad, display or earpiece. It is often
located at the point of closest contact with the body.
The SAR measurement probe is equipped with an integrated, non-metallic
optical sensor so that its position relative to any surface of the
phantom is automatically determined with a high degree of precision. The
robot positioner must have six axis so that it can position the probe
tip normal (or very close to normal) to the curved surface of the head
phantom. The broadband E-field probes must have excellent isotropy
(typically 0.2 dB) and a spatial resolution of less than 1mm. Precise
methods are required for traceable probe calibrations in air and in the simulated tissue.
The E-field measurements must be rapidly transmitted by an optical link
to a PC for data processing. Extremely low noise and low drift
instrumentation amplifiers are necessary in the data acquisition
section. The effects and parameters causing distortion of probe
performance in the extreme near-field, near the phantom surface must be
compensated by the calibration of the probes and by numerical modelling.
The SAR values for given tissue masses (eg 10g or 1g) are than
calculated by means of three-dimensional polynominal integration.
1. The E-field measurement system should be highly automated, with a
typical measurement time of less than 30 minutes.
2. The standard mannequin or phantom should not underestimate the SAR in
the human tissue equivalent liquid.
3. The reference head phantom (SAM) must be used for devices used at the
ear and both left and right ear should be tested.
4. The SAR measurement is performed at maximum MTE output power for each
band and protocol. Multiple frequencies are tested in each band, usually
in the centre and at each end of the band.
5. Testing is performed in the Touch Position and the 15 degree Tilt
position. The phone positioner should place the phone in an exact
pre-defined position, with a very high order of repeatability.
6. Testing should be performed with antennas both retracted and extended
7. Measurement uncertainties should be accurately assessed (better than
30% for devices used at the ear)
8. The system should perform visualisation of the SAR distribution
around the surface of the MTE in the 3 planes and inside the phantom.
(head or flat phantom).
9. Extremely high positioning accuracy for the E-field probe (<0.1mm).
This requires that the probe tip be positioned normal to the surface of
the phantom.
10. Scanning for location of spatial peak must be accurate – high order
spatial resolution and accuracy is required. This is more critical when
testing at higher frequencies, say 5-6 GHz.
11. Very sensitive, RF dosimetric probes calibrated in the same tissue
simulating liquid must be used. Accurate measurement of liquid
dielectric properties is essential for each MTE operating frequency
band. Dielectric parameters of the brain simulating liquid must be
accurately measured prior to each test.
12. Calibration/system validation should be performed routinely prior to
testing.
13. The MTE must be operated via air-link at maximum output power.
Interconnecting leads or power supple connections may disturb the
measurements. A base-station simulator and a shielded test chamber are
required.
14. The software must have powerful computational and post measurement
data processing capability.
Commercially available systems range from single dimension, 3 axis
and 6 axis positioners (robots). The systems necessary to perform the
SAR measurements involve sophisticated measurement techniques, complex
calculations and modelling software. The cost of commercially available
systems vary greatly, as does the quality and performance
specifications. When commissioning SAR testing it is strongly
recommended that the test house be accredited for testing to the latest
SAR standards such as EN50361 and IEEE 1528. In Australia and some other
countries, regulations specify that the SAR test house be specifically
accredited for SAR testing. Accredited SAR testing provides a high
confidence level that the SAR measurements are accurate and that your
product complies with government requirements.
Chris Zombolas
Technical Director of EMC Technologies, Melbourne Australia
A NATA accredited test house for SAR measurements.
|
www.emctech.com.au |