Title: Kenneth John Webb
1COMPARING EMISSION MEASUREMENTS IN A
REVERBERATION CHAMBER AND A SEMI-ANECHOIC CHAMBER
- By
- Kenneth John Webb
- Principal EMC Engineer
2Agenda
- Purpose of Project
- Overview of Project
- Dipole Data
- Laptop Data
- Summary and Conclusions
3Purpose of Project
- Validate Reverb Chamber (RC) Calibration
- To define a possible test method for performing
emissions in a RC - Comparing results in a RC to conventional test
results in an Anechoic Chamber (AC) - Determine if equation is valid
- Power density to V/m equation
- Use of CCF, ACF, IL, CLF defined later
4Overview of Project
- Perform Calibration in RC
- Test a known source
- Test in RC and AC
- Calculate E-field using different techniques
- Validates method
- Test and unknown source
- Test in RC and AC
- Use methods derived on known source
5Why Measure Emissions in a Reverb Chamber?
- New Robust Test Method
- Test all sides of the unit
- Cost of reverb chamber is less than conventional
anechoic rooms - Measure total fields emanating from unit
- Test systems without multiple antenna positions
or unit orientations - Less setup time from susceptibility testing to
emissions testing
6Emissions in Reverb Chamber
7Reverb Chamber Physical Characteristics
8Typical Tuner
9Calibration Summary
- Meets the calibration requirements of DO-160D
Change 1 from 400MHz to 18GHz. - Uniformity is marginal from 100-200 MHz, the
allowed standard deviation is acceptable. Above
1 GHz, chamber uniformity is acceptable. - Antenna vs probe exceeds the allowed /-3 dB
tolerances using the log periodic antenna. - Using the EMCO 3106 antenna from 400MHz to 2GHz
allowed acceptable results - Obtained calibration factors needed for emissions
testing
10Emission Comparison Methodology
11Emission Comparison
- Use data collected in calibration for CCF, ACF,
CLF ,and IL - Use equation given in IEC 61000-4-21 for power
density to E-field conversion - Measure a known source (dipole antenna) and an
unknown source (Laptop computer) - Use basic test methods in AC
- Develop a new method for RC
12Dipole Testing
13Dipole Antenna
- Estimated 127dBuV/m with 20dBm
- Signal generator not linear, but used same one
for both AC and RC tests - AC will use conventional method
- Use AF
- Place RCV antenna in H and V polarities
- Dipole in H only
- RC new method
- No direct illumination
14Dipole Antenna in AC
15Dipole Antenna AC Data
16Dipole Antenna in RC
17Summary of Equations
18Dipole Antenna RC Data
- ERadiated (V/m) is the estimated field strength
produced by the dipole antenna - R was assumed to be 1m since the final
measurement is in volts per meter. - D is the equivalent directivity of the dipole.
- Determining the correct value would be an
interesting experiment. For the purposes of this
paper, 1.7 was used. - Power into antenna was not linear
- Same signal generator was used for both anechoic
and reverb chamber data - ?Tx, ?Rx the antenna efficiency factors for the
transmit and receive antenna respectively - Used 0.75 for a log periodic antenna and 0.9 for
a horn antenna
19Antenna Calibration Factor
- Equation 5.4-1
- Needed for emissions calculations for max power
radiated - Takes into account the antenna losses, gain, and
efficiency
20CCF
- CCF or Chamber Calibration Factor from eqn 5.7-1
- CCF is the normalized average received power
- PAveRec is the average received power over one
tuner rotation - PInput is the forward power averaged over one
tuner rotation. - Used emission field level calculations for
average recevied power
21ACF and CLF
- The chamber loading factor (CLF) is calculated
using equation 5.7-2. - CCF is from equation 5.7-1
- ACF is from equation 5.4-1
- Also used for emissions level calculations
- Used with Insertion Loss equation 8.4-1 for max
received power
22IL
- IL is from equation 5.4-1
- Also used for emissions level calculations
- Use with max radiated power
- IL is the normalized maximum received power
- Calculated during calibration
23Dipole Antenna RC Data, No CCF applied
24Dipole RC and AC DataNo CCF
25Dipole RC Data Retest
- The retest data collected was for information
only - Performed manually using mode stirred approach
- Verify data collection techinique
26Dipole RC Data Retest, No CCF applied, Mode
Stirred
27RC Dipole Data with CCF or CLF/IL
28RC Dipole Data with CCF, AVG to MAX
29RC Dipole Data with CCFAC and RC Data
30RC Dipole Data with CCFdB Delta
31RC Dipole Data with CCFdB Delta
32Dipole Summary
- Excellent correlation.
- 2dB delta between rooms for the dipole
measurements can be considered validation of the
test method. - Use the RSS or MAX of the horizontal and vertical
polarities - Must use CCF for AVG Power
- Use CLF and IL for MAX power
- Retest RC data with mode stirring also has good
correlation to AC - Verifies mode stirring technique using equation
for average power
33Dipole Summary Tuned or Stirred?
34Laptop Testing
35Laptop Setup in AC
36Laptop Setup in AC
37Laptop Setup in AC
38Laptop Setup in AC
39Laptop Setup in RC
40Laptop Setup in RC
41Sample Laptop Data RC
42Laptop Data in RC with CCF
43RC Laptop Data CCF vs CLF
44Ambient in RC with CCF
45Laptop RC Data
- Ambient is a concern
- RS testing may be leaking RF
- 50MHz emissions for info only
- CCF vs CLF about 5 to 10dB different
- Used both to compare the data
46Laptop Measurements in AC
47Laptop Measurements in AC
48Laptop Measurements in AC
49Laptop Measurements in AC
50Laptop Measurements in AC
51Laptop Measurements in AC
52Laptop Measurements in AC
53Laptop Measurements in AC
54Laptop Measurements in AC
55Laptop Measurements in AC
56Laptop Measurements in AC
57Laptop Measurements in AC
58AC vs RC CCF Laptop Data
59RC CCF vs AC Data
60RC CCF vs AC Data Delta
61RC CCF vs AC Data Delta
62RC CCF vs AC Data
63RC CCF vs AC Data
64RC CCF vs AC Data
65RC CCF vs AC Data
66AC vs RC CCF Laptop Data
67RC CLF vs AC Data
68RC CLF vs AC Data
69RC CLF vs AC Data
70RC CLF vs AC Data
71RC CLF vs AC Data
72Conclusions
- Laptop data not as good a correlation as the
dipole data - The maximum AC data was the best correlation to
the RC CCF or CLF data for the Laptop - The RSS or MAX was the best for the dipole
- Several spikes that were within 10-20dB of each
other for the Laptop data - The dwell time of 50ms may not have been long
enough to capture the full amplitude. - May be due to dwell time of RC data
- Tuner speed may need to be increased/decreased
- Use of MAX vs AVG equations for E-field
73Conclusions
- Assumption that the Laptop rotation (in six
different orientations) could be correlated to
the reverb chamber data may be incorrect. - A Laptop orientation (other than the 90 degree
changes) may have a higher amplitude emissions. - The frequency accuracy may also have been
different between the two test methods. - Frequencies may have been off
- The tuner may modulate the emissions and change
the frequency slightly.
74Conclusions
- The method for performing the test and the
equation used to calculate the E-fields does
appear to have an overall correlation and
usefulness. - Generally, the RC had a higher amplitude when
using average power equation and mode-stirring - Data trend was similar
- Dipole measurements within 2dB
- Future testing is definite
- Spherical dipole radiator
- Different dwell/sweep times
75Questions??