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Andreas Reil
Product Manager Microwave Imaging
1 MIP
Prepared for
Material meets millimeter wave (mmW)
COMPANY RESTRICTED
Overview
2
Applications in Plastics
Material meets millimeter wave
mmW Imaging
18.06.2019
mmW Imaging
Material meets millimeter wave 318.06.2019
Frequency
0Hz 1 kHz 1MHz 1GHz 1THz 1PHz 1EHz
Cellphones infrared ultra-violet
77 GHz automotive radar
Audio AM Radio FM Radio Radar visible light X-Ray
mmW Imaging
Material meets millimeter wave 418.06.2019
mmW Imaging
18.06.2019 Material meets millimeter wave 5
x / m
y / m
MIP / dB, default QPS reconstructionBMWi3, position: m90
-0.5 0 0.5-1
-0.8
-0.6
-0.4
-0.2
0
0.2
0.4
0.6
0.8
1
x / m
y / m
MIP / dB, default QPS reconstructionBMWi3, position: m180
-0.5 0 0.5-1
-0.8
-0.6
-0.4
-0.2
0
0.2
0.4
0.6
0.8
1
Honda CBR BMW i3 - side BMW i3 - front
QAR
Automotive Radome Testing
06.05.2019 360° High Resolution RCS Measurements 7
Find hidden
structures in
design radomes
PCB sample with copper structure.
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Material meets millimeter wave 9
Reasons for blindspots within the radome
Why spatially resolved reflectivity images are important
Transmission
Reflection
Absorption
Radome
18.06.2019
2018-07-13 QAR customer training 10
COMPANY RESTRICTED
2018-07-13 QAR customer training 11
COMPANY RESTRICTED
2018-07-13 QAR customer training 12
COMPANY RESTRICTED
2018-07-13 QAR customer training 13
COMPANY RESTRICTED
Radar angular measurement technology
Material meets millimeter wave 14
𝜑1𝜑2𝜑3𝜑4𝜑5
𝛼
Sampling points
Estimate azimuth / elevation angles from
phase differences / amplitudes at the
receive antennas of the phased array
𝛼 = sin−1𝜆 ∙ ∆𝜑
2𝜋𝑑
∆𝜑
𝑑
𝑑
∆𝜑
𝛼
𝜆
Physical distance between antennas
Phase difference
Angle of arrival
wavelength
18.06.2019
Radar angular measurement technology
Material meets millimeter wave 15
𝜑1𝜑2𝜑3𝜑4𝜑5
𝛼
Phase fronts traveling
towards the radar.
∆𝜑
𝑑
𝑑
∆𝜑
𝛼
𝜆
Physical distance between antennas
Phase difference
Angle of arrival
wavelength
𝛼 = sin−1𝜆 ∙ ∆𝜑
2𝜋𝑑
∆𝜑1 ≠ ∆𝜑2 ≠ ∆𝜑3 ≠ ∆𝜑4 ≠ ∆𝜑5
Phase estimation is wrong
18.06.2019
Radar angular measurement technology
Material meets millimeter wave 16
𝛼
Phase fronts traveling
towards the radar.
∆𝜑l The radar is slightly moved.
l The distance between the antennas is
changed.
l Another algorithm is used for angle of
arrival estimation during post processing.
Or, more general, if:
l Another radar / radome combination is
used.
𝜑1𝜑2𝜑3𝜑4𝜑5
𝑑
Measuring the angle error does not lead
to useful results, if:
An alternative method has to be used.
18.06.2019
Radar angular measurement technology
Material meets millimeter wave 17
Angular inaccuracies are
caused by inhomogeneity.
Inhomogeneity of the radome
is measured by the QAR.
A threshold can be defined
for either each car, or the
whole fleet. Every radar is
then measured using the
same technique.
18.06.2019
18
Comparison of measurement methods
Corner reflector
Radome
Radar
Meas. Point=====================#1#2#3
2wayatt.
1.2dB1.4dB1.6dB
AzimuthError
0.2°0.1°0.3°
Method
Descr.
Result
Corner reflectors Network Analyzer R&S®QAR
Radome
Material meets millimeter wave18.06.2019
19
Comparison of measurement methods
Corner reflector
Radome
Radar
Meas. Point=====================#1#2#3
2wayatt.
1.2dB1.4dB1.6dB
AzimuthError
0.2°0.1°0.3°
Method
Descr.
Result
Corner reflectors Network Analyzer R&S®QAR
Radome
Cheap & Quick
Estimation &
selective,
Radar dependent
Material meets millimeter wave18.06.2019
20
Comparison of measurement methods
Corner reflector
Radome
Radar
Meas. Point=====================#1#2#3
2wayatt.
1.2dB1.4dB1.6dB
AzimuthError
0.2°0.1°0.3°
Method
Descr.
Result
Corner reflectors Network Analyzer R&S®QAR
Radome
Material meets millimeter wave18.06.2019
21
Comparison of measurement methods
Corner reflector
Radome
Radar
Meas. Point=====================#1#2#3
2wayatt.
1.2dB1.4dB1.6dB
AzimuthError
0.2°0.1°0.3°
Method
Descr.
Result
Corner reflectors Network Analyzer R&S®QAR
Radome
Precise measurement
Slow and selective
Calibration required
Experts for operation
Material meets millimeter wave18.06.2019
22
Comparison of measurement methods
Corner reflector
Radome
Radar
Meas. Point=====================#1#2#3
2wayatt.
1.2dB1.4dB1.6dB
AzimuthError
0.2°0.1°0.3°
Method
Descr.
Result
Corner reflectors Network Analyzer R&S®QAR
Radome
Material meets millimeter wave18.06.2019
23
Comparison of measurement methods
Corner reflector
Radome
Radar
Meas. Point=====================#1#2#3
2wayatt.
1.2dB1.4dB1.6dB
AzimuthError
0.2°0.1°0.3°
Method
Descr.
Result
Corner reflectors Network Analyzer R&S®QAR
Radome
Spatially resolved
Easy to operate
Time saving
Equipment necessary
Material meets millimeter wave18.06.2019
24
Comparison of measurement methods
Corner reflector
Radome
Radar
Meas. Point=====================#1#2#3
2wayatt.
1.2dB1.4dB1.6dB
AzimuthError
0.2°0.1°0.3°
Method
Descr.
Result
Corner reflectors Network Analyzer R&S®QAR
Radome
Material meets millimeter wave
Radome
18.06.2019
The R&S QAR radome tester
18.06.2019 Material meets millimeter wave 25
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Summary
Your benefits
Material meets millimeter wave 26
Increase quality
Reduce measurement time
Reduced costs
Due to the possibility of
100% testing in production
Measurement cycle of the
instrument is ~ 7s
Much easier to operate as
a vector network analyzer
18.06.2019
27
Thank You
Material meets millimeter wave18.06.2019