Research activities in Liège Ir. V. Beauvois , Ir. S. Coets, Ir. M. Renard and Ir. Ph. Camus
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Transcript of Research activities in Liège Ir. V. Beauvois , Ir. S. Coets, Ir. M. Renard and Ir. Ph. Camus
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Research activities in Liège
Ir. V. Beauvois, Ir. S. Coets, Ir. M. Renardand Ir. Ph. Camus
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1st Research interest:conducted and radiated emissions
measurements on large systems
Ir. V. Beauvois, Ir. S. Coets and Ir. M. Renard(Sorrento 2002 and Zurich 2003)
in coll. With Johan Catrysse (KHBO, Oostende, Belgium)
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Conducted Emission – Introduction
In the low frequency range [150kHz - 30MHz] ,conducted emission measurements are performed with:
a LISN (Line Impedance Stabilized Network) which
a passive voltage probe if LISN unavailable (i.e.
if currents too large)
prevents the EUT from the noise coming from the mains
provides a defined impedance at the point of measurement
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Conducted Emission - Measurement
Setup
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Conducted Emission - Problems encountered
With the LISN, the measurement is always performed at point 1b
The point of measurement is ‘‘standardized’’ (fixed)
Oppositely, the voltage probe (point 2) can be placed anywhere between points 1b and 3, depending on the ‘‘accessibility’’ of the EUT
Which signal voltage is measured (distributed impedancebetween 1b and 3 not negligible) ??
Solution: introduction of a new concept: the six-pole
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Conducted Emission - Six-pole Concept
In this research, only single-phased situations are considered
concept of the six-pole
If three-phased situations with neutral (3P + N + PE)
ten-pole
If three-phased situations without neutral (3P + PE)
eight-pole
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Cond. Emission - More accurate model
H1 : six-pole between mains and point of measurement (1b or 2)
EUT emission signal voltage
H2 : six-pole between point of measurement and EUT
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Cond. Emission - Actual and Future Works
As the tests performed without LISN may not be compared with those performed with LISN, the next steps of the study are:
create a ‘‘virtual’’ power mains network similar to the LISN ’s one and perform measurements with the help of this ‘‘LISN-equivalent network’’
for instance by the use of an EMI filter instead of the LISN an alternating method to the LISN could then be reached
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Cond. Emission - Actual and Future Works (contd)
• time domain and frequency domain measurements are done.• alternate measurement methods :
- classical passive voltage probe (one or twowith differential method)
- alternate probes and clamps (capacitive clamp,EM clamp, current probe)
improve the sensitivity of the measurements and the signal -processing to get more accurate results
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Radiated emission - Introduction
Theoretical test configuration:
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Radiated emission - Problems encountered
Noise coming from the environment.
Multiple reflexions « against » the environment which leads to an over-estimation or an under-estimation of the emission of the EUT.
The measurement cannot necessarily be performed at a 10 meters distance from the EUT.
How many measurements are to be done? And where?
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Radiated emission - Solutions to consider
Retrieve the right signal from noise by using a differential method.
As the measurements cannot be performed at a 10 meters (or 3 meters) distance, perform near-field measurements in addition with a near-field far-field transformation.
Take into account the reflecting characteristics of the global environment
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2nd Research interest:Characterization and modelling of
embedded systems emissions
Ir. V. Beauvois, Ir. Ph. Camus
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Architecture of embedded systems
µcontroller
Main clock
Memory
I/OController
Analog and Power Section
Sensors and Actuators
Level shifters
Power Supply
Data Transmission
Lines
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Fast switching occurs on the bus and transmission lines which leads to current pulses. Current pulses produce electromagnetic emissions radiated through the P.C.B. traces, integrated circuits pads and connected cables. For a given architecture and software, the current waveforms on the board connections can be evaluated - they are related to electromagnetic emission.
By mean of Fourier transform the spectrum can be computed and compared with EMC limits.
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Typical waveforms – Data bus
0 50 100 150 200 250 300 350 4000
1
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Boucle while(1); durée =100 µs
t (µs)
0 20 40 60 80 100 120 140 1600
1000
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f (kHz)
Data bus,address busand control signalare combined(summation) in time domain. As signals are synchronous(one main clock) phase isthe same for each signalat a given frequency-> spectrum can be easilycomputed.One simple loop on
80C320 Dallas
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Typical waveforms – Power supply
• White filtered noise for analog parts• Simple pulse noise for switched circuits
7805 linear regulator(white noise with cut off frequency near 1 MHz)
and MAX232 level shifter (245 kHz and harmonics)
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Typical waveforms – Analog and Power section
• Classification into families of circuits with same noise signatures• White filtered noise and switching noise.
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First results and actual works
Conducted and radiated emission of a 80C320 boardwere measured for different codes and comparedwith computed spectrum : • computed spectrum components occur• at the same frequency as in the measurement on a real circuit ;• variation of amplitude follows a similar envelope.
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Actual and Future Works
• Characterization of a great number of boards : same CPU with different clocks and different peripherals, … • Better modelling of switching process and relationship with conducted and radiated noise. • VHDL modelling of CPU to gain a better comprehension of processor noise sources, synthesis into an FPGA and measurements in anechoic chamber. • Development of software tools to predict noise behaviour of embedded systems.