![Page 1: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/1.jpg)
Reverberation Chambers for EM Applications
Christopher L. HollowayJohn Ladbury, Galen Koepke, and Dave Hill
National Institute of Standards and TechnologyElectromagnetics Division
Boulder, Colorado303-497-6184, email: [email protected]
![Page 2: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/2.jpg)
OPEN AREA TEST SITES (OATS)
Problems:AmbientsReflectionsScanningInterferencePositioning
![Page 3: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/3.jpg)
TEMProblems:
High FrequenciesReflectionsTest VolumePositioning
![Page 4: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/4.jpg)
GTEM
Problems:Test VolumeUniformity Along CellPositioning
![Page 5: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/5.jpg)
ANECHOIC CHAMBER
Problems:Low FrequenciesReflectionsPositioning
![Page 6: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/6.jpg)
REVERBERATION CHAMBER
Why use reverberation chamber?
![Page 7: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/7.jpg)
The Classical OATS Measurements
The classic emissions test and standard limits (i.e, testing a product above a ground plane at a specified antenna separation and height) have their origins in interference problems with TV reception.
![Page 8: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/8.jpg)
Emissions Test Standard Problem
One problem with the emissions test standard is that it is based on an interference paradigm (interference to terrestrial broadcast TV) that is, in general, no longer valid nor realistic today. In a recent report, the FCC indicated that 85 % of US households receive their TV service from either cable, direct broadcast satellite (DBS), or other multichannel video programming distribution service, and that only a small fraction of US households receive their TV via direct terrestrial broadcast.
Coupling to TV antennas designed to receive terrestrial broadcast may no longer be an issue.
![Page 9: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/9.jpg)
EMC Environment Today
• In recent years, a proliferation of communication devices that are subject to interference have been introduced into the marketplace.
• Today, cell phones and pagers are used in confined offices containing personal computers (PCs). Many different products containing microprocessors (e.g., TVs, VCRs, PCs, microwave ovens, cell phones, etc.) may be operating in the same room.
• Different electronic products may also be operating within metallic enclosures (e.g., cars and airplanes). The walls, ceiling, and floor of an office, a room, a car, or an airplane may or may not be highly conducting.
• Hence, emissions from electric devices in these types of enclosures will likely be quite different from emissions at an OATS. In fact, the environment may more likely behave as either a reverberation chamber or a free space environment.
![Page 10: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/10.jpg)
Where Should We Test?• Thus, would it not be better to perform tests more appropriate to
today's electromagnetic environment?
• Tests should be Shielded, Repeatable, Simple, Inexpensive, Fast, Thorough, …
![Page 11: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/11.jpg)
Commercial Solutions…
• Stirrer
• Turntable
![Page 12: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/12.jpg)
Reverberation Chamber
D-U-TTransmit Antenna
Receive AntennaProbe(s)
Signal GeneratorAmplifierDirectional couplerPower Meter(s)etc.
Motor Control
Control and MonitoringInstrumentation forDevice-under-test
Receive Instrumentation:Spectrum AnalyzerReceiver, ScopesProbe Systemetc.
![Page 13: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/13.jpg)
Fields in a Metal Box (A Shielded Room)
•In a metal box, the fields have well defined modal field distributions.
Locations in the chamber with very high field values Locations in the chamber with very low field values
Frozen Food
![Page 14: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/14.jpg)
Fields in a Metal Box with Small Scatterer
In a metal box, the fields have well defined modal field distributions.
Small changes in locations where very high field values occur Small changes in locations where very low field values occur
![Page 15: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/15.jpg)
Fields in a Metal Box with Large Scatterer (Paddle)
Large changes in locations where very high field values occur
Large changes in locations where very low field values occur
In fact, after one fan rotation, all locations in the chamber will have the same maxima and minima fields.
![Page 16: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/16.jpg)
Stirring MethodTIME DOMAIN
Click to play paddle rotation
750MHz
Paddle
![Page 17: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/17.jpg)
Field Variations with Rotating Stirrer
![Page 18: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/18.jpg)
Reverberation Chamber: All Shape and Sizes
Large ChamberSmall Chamber
Moving walls
![Page 19: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/19.jpg)
Reverberation Chamber with Moving Wall
![Page 20: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/20.jpg)
Original Applications• Radiated Immunity
componentslarge systems
• Radiated Emissions• Shielding
cablesconnectorsmaterials
• Antenna efficiency• Calibrate rf probes• RF/MW Spectrograph
absorption properties
• Material heating• Biological effects• Conductivity and
material properties
![Page 21: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/21.jpg)
Wireless Applications• Radiated power of mobile phones
• Gain obtained by using diversity antennas in fading environments
• Antenna efficiency measurements
• Measurements on multiple-input multiple-output (MIMO) systems
• Emulated channel testing in Rayleigh multipath environments
• Emulated channel testing in Rician multipath environments
• Measurements of receiver sensitivity of mobile terminals
• Investigating biological effects of cell-phone base-station RF exposure
![Page 22: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/22.jpg)
Fundamentals• A Reverberation Chamber is an electrically large,
multi-moded, high-Q (reflective) cavity or room.
• Electromagnetic theory using mode or plane-wave integral techniques provides several cavity field properties (mode density, Q and losses, E2, etc.)
• Changing boundary conditions, antenna or probe location, or frequency will introduce a new cavity environment to measure (sample)
• The composite effects of multiple cavity electromagnetic environments are best described by statistical models
![Page 23: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/23.jpg)
Sampling Considerations
• How many samples do we need?time / budget constraintsacceptable uncertaintiesstandards may dictate
• Sampling rates may not be identicalequipment-under-testinstrumentationprobes
• How long to dwell at each sample?
![Page 24: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/24.jpg)
Sampling Considerations• How are samples generated?
change boundary conditionschange device-under-test and antenna locationschange frequency (bandwidth limits)
• Samples must be independentChanges are ‘large enough’
• Measurement time proportional to number of samples (time = $$)
![Page 25: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/25.jpg)
Sampling Considerations
Techniques to Generate Samples• Mechanical techniques
Paddle(s) or Tuner(s)• stepped (tuned)• continuous (stirred)
Device-under-test and antenna positionMoving walls (conductive fabric, etc.)
• Electrical techniques (immunity tests)Frequency stirring
• stepped or swept• random (noise modulation)
• Hybrid techniques
![Page 26: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/26.jpg)
Measurement Procedures
Calibrate and Initialize system
Establish Fields in Chamber
Measure response of EUT, probes, receive antenna, etc.
Generate new environment i.e. move paddle move antennas change frequency, etc.
END<N =N
![Page 27: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/27.jpg)
EM Applications
![Page 28: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/28.jpg)
HIDING Emission Problems
![Page 29: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/29.jpg)
YOU CANNOT HIDE IN Reverberation Chamber
In reverberation chambers you cannot hide emission problems.
Reverberation chambers will find problems.
![Page 30: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/30.jpg)
Unethical Practices
• The current measurement methodologies of a product can easily miss radiation problem of a products.
• That is, energy propagation in a direction that a received antenna would miss.
• Not to suggest that companies would be unethical, but we have been told the individuals have setup products for emission measurements in such a manner to ensure that emission problems would not be detected.
![Page 31: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/31.jpg)
Unethical Practices
• Secondly, not to suggest companies are unethical once can, but we have also been told that some individual have lists of OATS around the world with their corresponding ambient noise sources.
• Thus, if one had a product that has an emission problem at frequency “x”, and it is known that one particular OATS at some site in the world as a ambient noise problem at the same frequency “x”, then a product could be tested and possible certified on the OATS, in which the product emission problems would not showing up.
![Page 32: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/32.jpg)
One Possible Solution
• These two possible ways of hiding emission problems cannot be accomplished in a reverberation chamber.
• In reverberation chambers you cannot hide emission problems.
• Reverberation chambers will find problems.
• If reverberation chambers are to be used, new standards are needed.
![Page 33: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/33.jpg)
EMISSION LIMITS
0 200 400 600 800 1000Frequency (MHz)
0.0E+0
1.0E-4
2.0E-4
3.0E-4
4.0E-4
5.0E-4
6.0E-4
|Em
ax |
(V
/m)
Class A: based on 10 m separation
Class B: based on 3 m separation
•Devices and/or products are tested for emissions to ensure that electromagnetic field strengths emitted by the device and/or product are below a maximum specified electric (E) field strength over the frequency range of 30 MHz to 1 GHz.
•These products are tested either on an open area test site (OATS) or in a semi-anechoic chamber.
•Products are tested for either Class A (commercial electronics) or Class B (consumer electronics) limits, Class A equipment have protection limits at 10 m, and Class B equipment have protection limits at 3 m.
![Page 34: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/34.jpg)
Total Radiated Power for Reverberation Chambers
0 100 200 300 400 500 600 700 800 900 1000Frequency (MHz)
-65
-60
-55
-50
-45
-40
P tot
al
(dBm
)
Class A: based on 10 m separation
Class B: based on 3 m separation
Class A: average limit
Class B: average limit
Holloway et al., IEEE EMC Symposium
![Page 35: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/35.jpg)
Emission Measurements
200 300 400 500 600 700 800 900 1000Frequency (Hz)
-60
-56
-52
-48
-44
E-fie
ld (
dBV/
m)
Reverb Chamber
OATS
Relate total radiated power in reverberation chambers to measurements made on OATS with dipole correlation algorithms.
Spherical Dipole
200 400 600 800 1000Frequency (Hz)
-64
-60
-56
-52
-48
E-fie
ld [
dBV/
m]
Reverb Chamber
Anechoic Chamber
![Page 36: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/36.jpg)
Emissions Measurements of Devices
Total Radiated Power Comparison Max Field Comparison
![Page 37: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/37.jpg)
Shielding Properties of Materials
The conventional methods usesnormal incident plane-waves, i.e.,Coaxial TEM fixtures.
Ei E
t
⎟⎟⎠
⎞⎜⎜⎝
⎛−=
i
t
PP
LogSE 1010
However, these approaches determine SE for only a very limited set of incident wave conditions.
In most applications, materials are exposed to complex EM environments where fields areincident on the material with various polarizations and angles of incidence.
Therefore, a test methodology that better represents this type of environment would be beneficial.
![Page 38: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/38.jpg)
Nested Reverberation Chamber
Sample
![Page 39: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/39.jpg)
Nested Reverberation Chamber
⎟⎟⎠
⎞⎜⎜⎝
⎛−=
nsintx
sintx
sinrQ
nsinrQ
sor
nsor
nsinr
sinr
PP
PP
PP
PP
LogSE,,
,,
,,
,,
,,
,,
,,
,,103 10
C.L. Holloway, D. Hill, J. Ladbury, G. Koepke, and R. Garzia, “Shielding effectiveness measurements of materials in nested reverberation chambers,” IEEE Trans. on Electromagnetic Compatibility, vol. 45, no. 2, pp. 350-356, May, 2003.
Sample
![Page 40: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/40.jpg)
Nested Reverberation Chamber
1 10Frequency (GHz)
0
10
20
30
40
50
60
70
80
SE (d
B)
a
Material 1
Material 2
Material 3
Material 4
1 10Frequency (GHz)
10
20
30
40
50
60
70
80
90
SE (d
B)
a
Material 2: with coating
Material 2: with no coating
1 10Frequency (GHz)
0
10
20
30
40
50
60
70
80
90
SE (d
B)
aSE3: Chamber A
SE3: Chamber B
SE1: Chamber A
SE1: Chamber B
Different Materials
Different Chamber Sizes
Edge Effects
![Page 41: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/41.jpg)
Loading Effects: Rat in a Cage
![Page 42: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/42.jpg)
Research Goal
• To provide a way to gain intuition into loaded chamber responses to better help measurements
• Ultimately correlate measured and modeled data, and use models to predict what we cant measure.
• Develop a fast and efficient numerical code to explore multiple chamber topologies. (FDTD)
Descritize in to FDTD Grid
Predict Stirred Fields Computationally to give us insight into chamber measurements in a loaded environment
Take Real System
Simulate
![Page 43: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/43.jpg)
Measurements of Fake Rats
![Page 44: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/44.jpg)
Large Lossy Body
Lossy Body Configuration
Distributed Lossy Bodies
Periodic Lossy Bodies
![Page 45: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/45.jpg)
Measuring Shielding for “small” Enclosures
Pout
Pin
SE= -10 Log(Pin / Pout ): with frequency stirring
reverb chamber
“small” enclosure
![Page 46: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/46.jpg)
Problem with “small” Enclosures: Measuring the Fields Inside
•The “rule-of thumb” for antennas positioning in a chamber is ½ wavelength from the wall. This is because the tangential component of the E-field is zero are the wall.
Thus, small monopole (or loop) probes attached to the wall can be used to determine the power in the center of a “small” enclosure.
•However, Hill (IEEE Trans on EMC, 2005) has recently shown that the statistics for the normal component of the E-field at the wall are the same for the field in the center of the chamber.
![Page 47: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/47.jpg)
Comparison with Different Reverberation Chamber Approaches
port 1
port 3port 2
port 1
port 4
port 2
port 1
port 3port 2
port 1
port 4
port 2
Mode-Stirred with a Horn Antenna: SE => S31
Mode-Stirred with a Monopole Antenna: SE => S41
Frequency Stirring with a Horn Antenna: SE => S31
Frequency Stirring with a Monopole Antenna: SE => S41
![Page 48: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/48.jpg)
Comparison with Different Approaches
0
2
4
6
8
10
12
14
16
18
20
1000 2000 3000 4000 5000 6000 7000 8000 9000 10000
Frequency (MHz)
SE (d
B)
mode_stirring_horn
freq_stirring_horn
mode_stirring_monopole
freq_stirring_monopole
0
2
4
6
8
10
12
14
16
18
20
1000 2000 3000 4000 5000 6000 7000 8000 9000 10000
Frequency (MHz)
SE (d
B)
mode_stirring_horn
freq_stirring_horn
mode_stirring_monopole
freq_stirring_monopole
0
2
4
6
8
10
12
14
16
18
20
1000 2000 3000 4000 5000 6000 7000 8000 9000 10000
Frequency (MHz)
SE (d
B)
mode_stirring_horn
freq_stirring_horn
mode_stirring_monopole
freq_stirring_monopole
0
2
4
6
8
10
12
14
16
18
20
1000 2000 3000 4000 5000 6000 7000 8000 9000 10000
Frequency (MHz)
SE (d
B)
mode_stirring_horn
freq_stirring_horn
mode_stirring_monopole
freq_stirring_monopole
(c) narrow slot aperture
(a) open aperture (b) half-filled aperture
(d) generic aperture
![Page 49: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/49.jpg)
Different Probe Lengths and Locations
0
5
10
15
20
25
30
35
40
45
50
3000 4000 5000 6000 7000 8000 9000 10000 11000 12000Frequency (MHz)
SE (d
B)
Position 1, probe length=1.3 cm
Position 2, probe length=1.3 cm
Position 1, probe length=2.5 cm
Position 2, probe length=2.5 cm
a=0.5 cm
a=0.95 cm
0
5
10
15
20
25
30
2 2.5 3 3.5 4
Frequency (GHz)
SE (d
B)
probe location 1probe location 2probe location 3probe location 4
![Page 50: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/50.jpg)
Antenna Measurement:
![Page 51: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/51.jpg)
NIST Reverberation Chamber and Experimental Set-up
Dual-Ridged Horn used as receive antenna
Two paddles used
Antenna Under Test (AUT)
![Page 52: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/52.jpg)
Experimental Results to Compared to Horn Antenna
Results presented here are for relative total radiated power (RTRP)referenced to either a Horn or to a small Loop. For a Horn we have:
Horn
AUT
PPPowerRadiatedTotal =
where PAUT is the received power in the chamber when transmitting on the antenna under test (AUT), and PHorn is the received power in the chamber when transmitting on the horn. All antennas were connected to a 50 ohm cable, so results include both mismatch and efficiency (ohmic loss) effects.
If we assume the horn is the “best” antenna available, then thesemeasurements will show how “well” an antenna is performing.
![Page 53: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/53.jpg)
Ten-Layer Spherical 612 MHz Structure
8 mm Loop for 612 MHz antenna
612 MHz antenna: loop with ten-layer spherical material
![Page 54: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/54.jpg)
Ten-Layer Spherical 612 MHz Structure
Comparison to Horn
Comparison to Loops
-25
-20
-15
-10
-5
0
500 550 600 650 700 750 800 850 900 950 1000
Frequency (MHz)
Tota
l Rad
iate
d Po
wer
Rel
ativ
e to
Hor
n (d
B)
Ten-Layer Spherical Structure8 mm Loop for 612 MHz Antenna32mm Loop Antenna
-10
-5
0
5
10
15
20
500 550 600 650 700 750 800 850 900 950 1000Frequency (MHz)
Tota
l Rad
iate
d Po
wer
Rel
ativ
e to
Loo
ps (d
B)
Comparison to 8 mm Loop
Comparison to 32 mm Loop
![Page 55: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/55.jpg)
Magnetic Antenna
New Magnetic Antenna Comparison to Horn
Loop Antenna
-50
-45
-40
-35
-30
-25
-20
-15
-10
-5
0
5
200 250 300 350 400
Frequency (MHz)
Tota
l Rad
iate
d Po
wer
Rel
ativ
e to
Hor
n (d
B)
Magnetic EZ-Antenna: Ground Plane-Center of ChamberMagnetic EZ-Antenna: No Ground Plane-Center of ChamberMagnetic EZ-Antenna: On Chamber Wall3 cm Loop antenna
![Page 56: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/56.jpg)
Can NOT Measurement Directivity
-70
-60
-50
-40
-30
-20
-10
0
0 20 40 60 80 100 120 140 160 180 200
Location
P (d
Bm
)
nor-xscan w/o material
nor-xscan w metamaterialNear-Field Antenna Tests
![Page 57: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/57.jpg)
Multipath Environments
![Page 58: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/58.jpg)
Multipath EnvironmentsExtensive measurements have shown that when light of sight (LOS) path is present the radio multipath environment is well approximated by a Ricean channel, and when no LOS is present the channel is well approximated by a Rayleigh channel:
∑=
+++=N
nnncncLOS tffAtfAE
1
])(2cos[)2cos( φππ
The Amplitude of E is either Rayleigh or Ricean depending if a LOS path is present.
Urban Environment Rural Environment
![Page 59: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/59.jpg)
Ricean K-factor
componentsscatteredcomponentdirectk = or )(10 kLogK =
K=10 dBK=4 dB
K=1 dBK= - dB(Rayleigh)
∞
k-factor:
![Page 60: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/60.jpg)
Ricean K-factors and rms Delay Spreads
Besides chancing the K-factor, we need to vary its decay rate.
![Page 61: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/61.jpg)
Standardization of Wireless Measurements
Can we use a reverberation chambers for a reliable and repeatable test facilities that has the capability of simulating any multipath environment for the testing of wireless communications devices?
If so, such a test facility will be useful in wireless measurement standards.
![Page 62: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/62.jpg)
Reverberation Chambers are Natural Multipath Environments
![Page 63: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/63.jpg)
Typical Reverberation Chambers Set-up
Antenna pointing away from probe (DUT)
Paddle
Transmitting Antenna
metallic walls
DUT
a
a
A Rayleigh test environment
Can we generate a Ricean environment?
![Page 64: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/64.jpg)
Chamber Set-up for Ricean Environment
Antenna pointing toward (DUT)
We will show that by varying the characteristics of the reverberation chamber and/or the antenna configurations in the chamber, any desired Rician K-factor can be obtained.
Paddle
DUT
Transmitting Antenna
metallic walls
![Page 65: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/65.jpg)
Reverberation Chamber Ricean Environment
223
rD
QVKλ
=
It can be shown: see Holloway et al, IEEE Trans on Antenna and Propag., 2006.
Note:•We see that K is proportional to D. This suggests that if an antenna with a well defined antenna
pattern is used, it can be rotated with respect to the DUT, thereby changing the K-factor. •Secondly, we see that if r is large, K is small (approaching a Rayleigh environment);
if r is small, K is large. This suggests that if the separation distance between the antenna and the DUT is varied, then the K-factor can also be changed to some desired value.
•Next we see that by varying Q (the chamber quality factor), the K-factor can be changed to some desired value. The Q of the chamber can easily be varied by simply loading the chamber with lossy materials.
Also, if K becomes small, the distribution approaches Rayleigh.
Thus, varying all these different quantities in a judicious manner can result in controllable K-factor over a reasonably large range.
![Page 66: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/66.jpg)
Measured K-factor for Different Antenna Separation
Each set of curves represents a different distance of separation. The thick black curve running over each data set represents the K-factor obtained by using d determined in the anechoic chamber.
1.0E-04
1.0E-03
1.0E-02
1.0E-01
1.0E+00
1.0E+01
1.0E+02
1000 2000 3000 4000 5000 6000 7000
Frequency (MHz)
K-fa
ctor
0.5 m 1 m separation
2 m separation
![Page 67: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/67.jpg)
Measured K-factor for Chamber Loading
The thick black curve running over each data set represents the K-factor obtained by using d determined in the anechoic chamber.
1.0E-02
1.0E-01
1.0E+00
1.0E+01
1.0E+02
1.0E+03
1000 2000 3000 4000 5000 6000 7000
Frequency (MHz)
K-fa
ctor
2 pcs absorber
6 pcs absorber
0 pcs absorber
![Page 68: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/68.jpg)
Measured K-factor for Different Antenna Rotations
The thick black curve running over each data set represents the K-factor obtained by using d determined in the anechoic chamber. Each data set was taken at 1 m separation and with 4 pieces of absorber in the chamber.
1.0E-03
1.0E-02
1.0E-01
1.0E+00
1.0E+01
1.0E+02
1000 2000 3000 4000 5000 6000 7000
Frequeency (MHz)
K-fa
ctor
90 degrees
30 degrees
0 degrees
![Page 69: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/69.jpg)
Measured K-factor for Different Antenna Polarizations
The thick black curve running over each data set represents the K-factor obtained by using d determined in the anechoic chamber. Each data set was taken at 1 m separation and with 4 pieces of absorber in the chamber.
1.0E-04
1.0E-03
1.0E-02
1.0E-01
1.0E+00
1.0E+01
1.0E+02
1.0E+03
1000 2000 3000 4000 5000 6000 7000
Frequency (MHz)
K-fa
ctor
cross-polarized
45 degree polarization
co-polarized
![Page 70: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/70.jpg)
Simulating Propagation Environments with Different Impulse Responses and rms Delay Spreads
![Page 71: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/71.jpg)
S21 Measurements: Loading the Chamber
![Page 72: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/72.jpg)
Impulse Responses and Power Delay Profiles
Loading the Chamber
2)()( thPDP =τ
Power Delay Profile:
where h(t) is the Fourier transform of S21 (ω)
![Page 73: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/73.jpg)
rms Delay Spreads
∫
∫∞
∞
−
=
0
0
2
dttP
dttPt o
rms
)(
)()( τ
τ
∫
∫∞
∞
=
0
0
dttP
dtttP
o
)(
)(
τ
One characteristic of the PDP that has been shown to be particularly important in wireless systems that use digital modulation is the rms delay spread of the PDP:
where τo is the mean delay of the propagation channel, given by
![Page 74: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/74.jpg)
rms Delay Spreads vs Threshold Levels
![Page 75: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/75.jpg)
Impulse Responses and rms Delay Spreads (200 MHz band filter on S21 data)
![Page 76: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/76.jpg)
rms Delay Spreads from Q measurements
2
22
11
1222
))(())ln((
)()(ln)ln(
KKQ
rms+−
−+−
+−+−−
=α
αααα
αεαααω
τ
where K is the k-factor and α
threshold.
Thus, once we have Q, we can estimate τrms
![Page 77: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/77.jpg)
Impulse Responses and rms Delay Spreads for Different Ricean K-factors
![Page 78: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/78.jpg)
BER Measurements - setupAgilent 4438C Vector Signal Generator
Agilent 89600 Vector Signal Analyzer
External trigger
Firewire connectionto control VSA
GPIB connectionto control VSG
Reverberation chamber
![Page 79: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/79.jpg)
BER Measurements
BER for a 243 ksps BPSK signal
BER for a 786 ksps BPSK signal
![Page 80: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/80.jpg)
BER Measurements
Demodulated 768ksps BPSK signal in I-Q diagram
![Page 81: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/81.jpg)
How Well Can we Simulate a Real Environment?Power Delay Profile in an oil refinery.
![Page 82: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/82.jpg)
How Well Can we Simulate a Real Environment?
BER measurement in a laboratory.
![Page 83: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/83.jpg)
Wireless Measurements
1. Reverberation chambers represent reliable and repeatable test facilities that have the capability of simulating any multipath environment for the testing of wireless communications devices.
2. Such a test facility will be useful in the testing of the operation and functionality of the new emerging wireless devices in the future.
3. Such a test facility will be useful in wireless measurements standards.
![Page 84: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/84.jpg)
Summary
• Reverberation chamber measurements are thorough and robust.
• Proper sampling techniques reduce measurement uncertainties
• Statistical models help minimize the number of samples required
![Page 85: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/85.jpg)
Summary
• Reverberation chambers capture radiated power (total within the measurement bandwidth)
• Results are insensitive to EUT placement in the chamber
• Results are independent of EUT or antenna radiation pattern
• Enclosed system free from external interference
![Page 86: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/86.jpg)
Rome’s Old Chamber
![Page 87: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/87.jpg)
Rome’s New Chamber
![Page 88: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/88.jpg)
Rome’s New Chamber
![Page 89: Reverberation Chambers for EM Applicationsweb.mst.edu/~jfan/slides/Holloway3.pdfReverberation Chambers for EM Applications Christopher L. Holloway John Ladbury, Galen Koepke, and Dave](https://reader030.vdocument.in/reader030/viewer/2022040521/5e7c443f41ab156e3f5dd8f5/html5/thumbnails/89.jpg)
Reverberation Chamber Standards
• International Standard IEC 61000-4-21: Testing and measurement techniques – Reverberation chamber test methods