See the Product Information Bulletin included with your shipment for information
on ETS-Lindgren calibration services.
Service Procedures
For the steps to return a system or system component to ETS-Lindgren for
service, see the Product Information Bulletin included with your shipment.
follow the safety information in the
ETS-Lindgren Product Information Bulletin included with your shipment.
Maintenance | 13
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14 | Maintenance
Page 15
3.0 Specifications
Electrical Specifications
Model 7605 Model 7606
Frequency Range: 30 Hz–100 kHz 30 Hz–100 kHz
Wire: AWG-12
Enameled Copper
Number of Turns: 20 51
Maximum Input Current: 15 A Continuous NA
Connector: Banana Jack (Pair) Type BNC Female
Resistance of Winding
(Approximate):
Inductance
(Approximate):
40 mΩ 3.9 Ω
71.8 µH 175 µH
7-41
Litz Copper
Physical Specifications
The windings on both models have square cross sections with dimensions of
approximately 12 mm for the Model 7605 Radiating Loop and approximately
3.175 mm for the Model 7606 Radiating Sensor.
Height: 5.89 cm (2.32 in) 13.46 cm (5.30 in)
Base Width: NA 5.08 cm (2.00 in)
Base Depth: NA 1.90 cm (0.75 in)
Model 7605 Model 7606
Mean Loop Diameter: 12.0 cm 4.0 cm
Specifications | 15
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16 | Specifications
Page 17
4.0 Theory of Operation
Schematic of 7605/7606 in Calibration Configuration
The following illustration shows the Model 7605 Radiating Loop and the
Model 7606 Radiating Sensor as loops or coils separated by a calibration
distance of 5 cm.
Theory of Operation | 17
Page 18
Model 7605
Model 7605 is used alone to produce an AC magnetic field to test Equipment
Under Test (EUT) for susceptibility (immunity) to magnetic fields in the frequency
range from 30 Hz to 100 kHz. It consists of 20 turns of AWG-12 enamel-insulated
copper wire close-wound with an average diameter of 12 cm. It is capable of
carrying 15 A rms, but if this level of coil current is sustained for long periods, the
coil will become warm. It has a coil resistance of approximately 40 mΩ and an
inductance of approximately 71.8 µH.
EQUATION 1
Equation 1 derived from [7] gives the relationship between coil current and
magnetic flux density.
Equation 1 may be simplified for computation as shown in equation 2.
EQUATION 2
18 | Theory of Operation
Page 19
Model 7606
Model 7606 is used with Model 7605 to calibrate the 7605 and other
instrumentation used in tests. With 51 turns of wire in a 4-cm diameter loop, it
has an effective area of 640 cm
the sensitivity of measurements with a given instrument by more than 30 dB over
a small, single-turn loop. The response is tabulated in the Conversion Factors for Model 7606 table on page 21 (and is proportional to the frequency shown in
Figure RS101-1 in Method RS101 of MIL-STD-462D).
2
(an effective diameter of 28.6 cm), improving
The voltage induced in the loop, e
number of turns, the frequency, and the average flux density within the area of
the loop. Equation 3 derived from [8] gives this relationship.
, is proportional to the area of the loop, the
i
EQUATION 3
For the Model 7606, the open-circuit loop-terminal induced voltage in microvolts
for a magnetic flux density in picotesla is given in equation 4.
EQUATION 4
The general equation for the conversion factor is given by equation 5 and
equation 6, and includes the effects of loop impedance and load impedance.
Theory of Operation | 19
Page 20
EQUATION 5
EQUATION 6
For the Model 7606, equation 6 becomes equation 7.
EQUATION 7
The values in the following table were calculated from equation 5 and equation 7
using a 50 Ω load and a 600 Ω load. (These values are the same as in
Figure RS101-1 in MIL-STD-462D.)
20 | Theory of Operation
Page 21
CONVERSION FACTORS FOR MODEL 7606
This table shows that below 15 kHz there is less than 1 dB difference between
the values of the conversion factors for the loop loaded in 50 Ω and in 600 Ω
(open circuit), and over most of the range the difference is less than 0.6 dB. To
find values of the correction factor between these values, use the interpolation in
equation 8.
Frequency (kHz)
0.03 99.01 98.41
0.1 88.56 87.96
1 68.56 67.96
3 59.03 58.42
7 51.41 51.06
10 48.73 47.96
13 46.57 45.68
15 45.42 44.44
17 44.44 43.35
20 43.20 41.94
23 42.18 40.73
27 41.07 39.34
30 40.39 38.43
35 39.46 37.09
Conversion Factor, dB(pT/µV)
50 Ω 600 Ω
40 38.72 35.94
45 38.13 34.92
50 37.66 34.01
70 36.46 31.13
100 35.66 28.10
Theory of Operation | 21
Page 22
EQUATION 8
22 | Theory of Operation
Page 23
5.0 MIL-STD-462D Method RS101 Testing
Before connecting any components, follow the
safety information in the ETS-Lindgren
Product Information Bulletin included with your
shipment.
The normal design application of the Model 7605 Radiating Loop and
Model 7606 Radiating Sensor is the MIL-STD-462D Method RS101 EMI testing.
Additional applications are possible, but only the application to Method RS101 is
discussed here.
Method RS101 requires two distinct activities: test setup calibration and exposure
of the Equipment Under Test (EUT) to specified magnetic flux densities.
Operational Cautions
Large magnetic fields are produced during
testing, particularly at low frequencies. They are
capable of affecting calculators and watches,
and at the RS101 worst-case limits, they exceed
the levels which the Swedish government [10]
has set for video display terminals. Therefore,
take these precautions:
• Keep all calculators, watches, rings, and
other metallic objects at least one meter
from the Model 7605 during testing.
• Keep your head and torso at least 90 cm
from the Model 7605 during testing below
400 Hz.
The Model 7606 may be damaged by large
currents, so do not connect it to the
signal source, and do not leave it in place
during testing.
MIL-STD-462D Method RS101 Testing | 23
Page 24
Assembly for Calibration
For test setup calibration, Model 7605 and Model 7606 are assembled together.
When assembled, the two loops are parallel to each other and coaxial with their
centers precisely 5 cm apart.
Do not over tighten the nylon bolt. Tighten it to
only finger tight; do not use a wrench.
Over tightening may cause the bolt to break,
blocking the bolt hole and making calibration
impossible.
1. Place the Model 7606 into the slot
in the body of the Model 7605, with
the BNC connector positioned
outside Model 7605 and pointing
upward.
2. Insert the 3/8–16 nylon bolt. Tighten
to finger tight.
24 | MIL-STD-462D Method RS101 Testing
Page 25
Method RS101 Calibration
Mount the Model 7605/Model 7606 assembly on a non-metallic tripod. This helps
prevent interaction between the assembly and the surroundings, and allows the
operator to be hands-free near the instrumentation.
Block Diagram – Calibration Test Setup
During calibration, keep the assembly several diameters away from metal
objects. Space the current probe and other instrumentation at least one meter
from the assembly to keep it from the influence of the Model 7605.
REQUIRED INSTRUMENTATION
• Model 7605/Model 7606 assembly
• Signal source—see page 26 for more information
• Two measuring instruments—see page 27 for more information
• Current probe—see page 27 for more information
MIL-STD-462D Method RS101 Testing | 25
Page 26
ABOUT THE SIGNAL SOURCE
The signal source may be a signal generator followed by a power amplifier or
current amplifier. The signal generator may be a manual signal generator, a
tracking generator (part of a spectrum analyzer or EMI meter), or a
computer-controlled signal generator. A 30 W power amplifier with an output
impedance of 0.5 Ω will drive the Model 7605 to about 15 A and produce up to
183 dB(pT) at the end of the built-in 5 cm spacer. When the amplifier is set to the
30 W output level, it produces a current of almost 15 A in the Model 7605, but the
actual amplifier power output is only about 9 W; the 30 W amplifier is needed to
be able to provide enough current from a 0.5 Ω source.
At the lower end of the frequency range, it would be better to use an amplifier
with output impedance lower than 0.5 Ω. For example, if the amplifier had a
source impedance of only 0.125 Ω, the power output capability would need to be
only 9.5 W. However, amplifiers and matching transformers to provide an output
impedance of 0.125 Ω are not readily available in the EMC test equipment
marketplace, but those providing 0.5 Ω are; they are typically found in an
EMC laboratory equipped for MIL-STD-462 testing.
The power amplifier and coupling transformer used for Method CS101 tests may
be used for RS101 tests, but the amplifier does not need as much power for
RS101 tests. Higher impedance amplifiers may be practical at the higher
frequencies where much less current is needed to produce the flux densities
required in the RS101 EMI susceptibility tests.
26 | MIL-STD-462D Method RS101 Testing
Page 27
ABOUT THE MEASURING INSTRUMENTS
The measuring instruments can be radio-noise or EMI meters, calibrated
receivers, spectrum analyzers, or other tunable (narrowband) voltmeters. These
instruments must be accurately calibrated with appropriate correction factors
available across the frequency range. A number of possible instruments are
available. Some instruments, for example, certain automatic spectrum analyzers,
may require no correction factors, since they self-calibrate and internally
generate and apply a correction factor at each frequency.
A single instrument can be used for both Measuring Instrument A and
Measuring Instrument B indicated in the illustration on page 25. If this is done:
•The Model 7606 should be loaded by a 50 Ω dummy load while the
output of the current probe is being measured.
•More importantly, the output of the current probe must be loaded by a
50 Ω dummy load when the output of the Model 7606 is being
measured.
Failure to load the current probe in 50 Ω while the measuring
instrument is not connected to it may result in unpredictable changes
in the impedance inserted into the line by the current probe. This may
then cause an unknown change in the current flowing in the
Model 7605.
For convenience during the susceptibility testing of the EUT, a spectrum analyzer
with a tracking generator may be used for measuring instrument A.
ABOUT THE CURRENT PROBE
The current probe may be a low-frequency EMI measuring clamp-on
current probe designed to cover the frequency range from 30 Hz to 100 kHz;
several manufacturers offer this type of probe. The accuracy of the individual
calibration is important because it is a key element in setting the test current
during EMI measurements.
The transfer admittance (or impedance) should be individually calibrated over the
frequency range. Usually, the probe calibration by the manufacturer is adequate,
but do not rely on a probe that has a calibration reported at a single frequency or
has a single conversion factor that is to be applied across the entire frequency
range.
MIL-STD-462D Method RS101 Testing | 27
Page 28
CALIBRATION STEPS
1. Set the signal source to a frequency of 1 kHz and adjust the output to
provide a magnetic flux density of 110 dB(pT) as determined by the
reading obtained on instrument A and the relationship
B = 160 dB(pT/A). This requires a current of -50 dB(A) or 3.16 mA.
To determine the current, algebraically add the current probe
correction factor in dB(S) to the reading in dB(mV) on instrument A; for
example:
2. Measure the voltage output in dB(µV) from the Model 7606 on
instrument B.
3. Verify that the output from the Model 7606 is 42 dB(µV) ±3 dB, and
record this value.
If the output from Model 7606 is not within ±3 dB of 42 dB(µV), verify the source
current is set correctly, and then look for other causes. Some possible causes
are:
• Inaccuracy in either or both measuring instruments.
• Malfunction of either or both measuring instruments.
• Inaccuracy in the current probe.
• Loose clamping or other malfunction of the current probe.
• Damage to the current probe.
• Magnetic-field coupling between Model 7605 and the current probe or
measuring instruments.
•Loose fit between Model 7605 and Model 7606, or other incorrect
assembly.
• Damage to Model 7605 or Model 7606.
• Metallic objects, particularly magnetic materials, in close proximity to
Model 7605 and Model 7606.
28 | MIL-STD-462D Method RS101 Testing
Page 29
If all instrumentation is operating properly and is accurately calibrated, readjust
the source to produce the correct output from the Model 7606. Use the ratio (or
difference in dB) between the initial setting of the source to the corrected setting
of the source as a correction factor in the later EMI susceptibility measurements.
Disassembly for Method RS101 Testing
Before disassembling Model 7605 and Model 7606, verify that the test signal
source is turned off or the output is reduced to zero.
1. Remove the 7605/7606 assembly from the tripod.
2. Unscrew the nylon bolt.
3. Remove the Model 7606 from the Model 7605.
MIL-STD-462D Method RS101 Testing | 29
Page 30
Method RS101 Testing
Block Diagram – RS101 Test Setup
This diagram shows EUT and these items of instrumentation:
• Model 7605
• Test signal source
• Current probe
• Measuring instrument
• Line Impedance Stabilization Network (LISN) in the EUT power line
• One or more pieces of input/output stimulating and monitoring
equipment for exercising the EUT and monitoring performance
All instrumentation, including the current probe, must be outside of the
influence of the Model 7605 magnetic field. A spacing of one meter
should be adequate.
30 | MIL-STD-462D Method RS101 Testing
Page 31
Testing EUT for susceptibility (immunity) consists of three processes: starting the
EUT, selecting test frequencies (may be done semi automatically), and testing
the EUT at the selected frequencies (done manually).
START THE EUT
Turn on the EUT, allow it to stabilize, and then verify it is operating properly.
Make sure the input/output stimulation and monitoring equipment is operating
satisfactorily.
SELECT TEST FREQUENCIES
Testing – Showing Application of Model 7605
1. Position the Model 7605 so that the built-in spacer is flat against one
surface of the EUT. This places it parallel to and 5 cm from the EUT.
MIL-STD-462D Method RS101 Testing | 31
Page 32
2. Drive the Model 7605 with sufficient current to produce a magnetic flux
density 10 dB greater than the applicable limit in MIL-STD-46ID [9], but
do not exceed 15 A; for example, 183 dB(pT). The following chart
shows the Model 7605 coil current at the RS101 limits.
3. Scan the frequency range from 30 Hz to 100 kHz. The scan rate may
be three times faster than the rates specified in Table III of
MIL-STD-462D.
In the 30 Hz to 100 kHz range the specified rates are 0.02f
per second for analog scans and 0.01f
steps (1% steps) for stepped
0
scans; so for these frequency selecting scans, the scan rates can be
per second for analog scans and 3% steps for stepped scans.
0.06f
0
32 | MIL-STD-462D Method RS101 Testing
0
Page 33
Stepped scans must dwell at each frequency for one second. f
tuned frequency, not the starting frequency. Usually, for analog scans,
the frequency range is broken into octave or decade bands and the
scan rate is changed at each band. The following table shows
suggested bands and analog scan rates. For stepped scans, the
frequencies may be computed using equation 9.
Frequency Band Analog Scan Rate Total Scan Time
30 Hz–100 Hz 2 Hz/s 35 s
100 Hz–200 Hz 8 Hz/s 12.5 s
200 Hz–400 Hz 17 Hz/s 11.8 s
400 Hz–700 Hz 32 Hz/s 9.3 s
700 Hz–1.5 kHz 61 Hz/s 13.1 s
1.5 kHz–3 kHz 127 Hz/s 11.8 s
3 kHz–6 kHz 250 Hz/s 12 s
6 kHz–10 kHz 460 Hz/s 8.7 s
10 kHz–20 kHz 850 Hz/s 11.8 s
20 kHz–40 kHz 1.7 kHz/s 11.8 s
is the
0
40 kHz–100 kHz 3.8 kHz/s 15.9 s
Suggested Scan Rates for Analog Scanning
EQUATION 9
4. If susceptibility is noted, select three or more test frequencies per
octave at frequencies where susceptibilities are present. For example,
if five frequencies within an octave show susceptible responses, select
at least three of them for further testing. The three selected should be
those with the maximum indication of susceptibility.
MIL-STD-462D Method RS101 Testing | 33
Page 34
5. Reposition the Model 7605 successively to a location in each 30 cm by
30 cm area on each surface of the EUT and repeat the previous steps.
6. From the total set of data where susceptibility was noticed, select three
frequencies in each octave of the frequency range from 30 Hz to
100 kHz where susceptibility was found.
TESTING THE EUT
At each frequency determined as a result of selecting test frequencies, apply the
current to the Model 7605 that corresponds to the applicable limit in
MIL-STD-461D. For accuracy in this process, calculate the required loop current
using equation 10. Move the loop to search for all possible locations of
susceptibility, including cables, connectors, cabinet seams, vents, and so on.
EQUATION 10
Model 7606 Calibration Calculations
The Model 7606 is designed to conform to MIL-STD-462D. This sensor is
electrically very small, which permits performance calculation based on
geometry. In the table on page 21 the performance is shown in the form of a
conversion factor which is used to convert the output voltage, in dB(µV), to the
magnetic flux density, in dB(pT), of the field in which the coil is immersed.
The tolerances in manufacturing are a maximum of 0.05 mm (0.002 inches).
These tolerances in worst-case combination cause a maximum error of ±0.06 dB.
The best accuracy with which the conversion factor can be measured is ±1 dB,
and larger errors are probable. Therefore, the conversion factor is not measured,
but is instead calculated to provide the best possible accuracy (absolute error
≤0.06 dB).
34 | MIL-STD-462D Method RS101 Testing
Page 35
CALIBRATION BY CALCULATION
Following are the equations used in calculation of Model 7606 performance,
along with a sample calculation.
The absolute value of the ratio of the magnetic flux density to the voltage across
the connected load, BV
EQUATION 11
, is given by equation 11.
L
The coil resistance, R
resistance of the wire; or, it can be measured with a low-resistance bridge. The
length of the wire is the product of the average circumference of the winding and
the number of turns. This is shown in equation 12.
, is found from the length of wire in the coil and the unit
c
EQUATION 12
The coil inductance, L, is found from equation 13.
MIL-STD-462D Method RS101 Testing | 35
Page 36
EQUATION 13
The ratio |B/VL| is put in decibels by equation 14 to become the correction factor,
CF.
EQUATION 14
Sample Calculation:
The maximum uncertainty because of dimensional tolerances is ±0.06 dB;
therefore, this calculated correction factor has a range of 98.95 dB to 99.07 dB.
For ordinary measurement work, such as the measurements for RS101, it is
reasonable to round this correction factor to 99.0 dB.
36 | MIL-STD-462D Method RS101 Testing
Page 37
TRACEABILITY TO NIST
The traceability to NIST is through the mechanical measurements and
mechanical calibration of the tools used to manufacture the Model 7606. It can
be proven mathematically that for such an electrically small sensor, the
performance can be accurately calculated based on the dimensions of the
sensor. Thus, the traceability of the manufacturing tools to NIST provides
traceability of the electrical performance of the sensor to NIST.
MIL-STD-462D Method RS101 Testing | 37
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38 | MIL-STD-462D Method RS101 Testing
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Appendix A: Warranty
See the Product Information Bulletin included with your shipment for
the complete ETS-Lindgren warranty for your Model 7605 Radiating
Loop and Model 7606 Radiating Sensor.
DURATION OF WARRANTIES FOR MODEL 7605/MODEL 7606
All product warranties, except the warranty of title, and all remedies for warranty
failures are limited to two years.
Product Warranted Duration of Warranty Period
Model 7605 Radiating Loop 2 Years
Model 7606 Radiating Sensor 2 Years
Warranty | 39
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