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EMI/EMC Characterization of Mixed Radio Frequency-Digital Circuits Yakup Bayram, Zulfiqar Khan, Taesik Yang and John L. Volakis Non-Linear RF Laboratory, ECE Dept. The Ohio State University 2015 Neil Ave., Columbus, OH, USA Patrick Roblin, Saek Joo Doo and Sukkeun Myoung ElectroScience Laboratory, ECE Dept. The Ohio State University 1320 Kinnear Road, Columbus, OH, 43212 USA

EMI/EMC Characterization of Mixed Radio …roblin/lsna/URSIindia.pdfEMI/EMC Characterization of Mixed Radio Frequency-Digital Circuits ... DC Line Output Line. Inverter ... GSM Band

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EMI/EMC Characterization of Mixed Radio Frequency-Digital Circuits

Yakup Bayram, Zulfiqar Khan, Taesik Yang and John L. Volakis

Non-Linear RF Laboratory, ECE Dept.The Ohio State University

2015 Neil Ave., Columbus, OH, USA

Patrick Roblin, Saek Joo Doo and Sukkeun Myoung

ElectroScience Laboratory, ECE Dept.The Ohio State University

1320 Kinnear Road, Columbus, OH, 43212 USA

RF-Digital Circuits Subject to Intentional EMIUnderstand and predict the effects of electromagnetic interference

on electronic systems

Cable Bundles Subject to HPM Sources Mixed Signal Circuits Subject to HPM Sources

combined full wave numerical EM tools such as MLFMM MoM and

Modal MoM with cable bundle toolssuch as CableMod and CRIPTE

Analysis Method:Integration of numerical EM tools with

circuit tools such as ADS and HSPICE forRF/Analog/Digital Circuit Simulation

A specific problem

Inverter Subject to EMI

Inverter Subject to EMI with

Different Type Modulations

UnmodulatedEMI

Pulse modulated

EMI

Multi tone modulated

EMI

Observed Effects

Input

UndisturbedOutput

Disturbed OutputEMI Effects on• Timing Characteristics• Logic Behaviors

Texas Instruments (TI SN74AUC1GU04) CMOS Inv• Optimized for 1.8V operation.• Minimum propagation delay tpd=0.6ns

for 30pF load. • Encrypted HSPICE Model for the inverter is used

in the simulations. • VDD=1.8V was used in our measurements.

InverterSignal Line

EMI Line(Acts as an antenna radiating nearby the inverter)

DC Line OutputLine

Inverter Operating at 1.0 GHz Unmodulated EMI at Inverter Out (Device level upset)

Signal Input

EMI Input

Input Signal @1.0GHzPulse width:300ps

Our LSNA does not capture DC response; therefore, output is off and DC correction is applied for the simulations !

Unperturbed

EMI at 1.0 GHz with 25dBm Power In

EMI at 1.0 GHz with 35dBm (Vemi=17.7V)

MeasurementADS+HSPICE (Validation Method 1)

Significant drop at the inverter output!Loss of saturation!

At the inverter outEMI coupling to only inverter in!

Device level upset!

STATE-OF-THE-ART in Coupled EM - Circuit Analysis

EM DomainEM

structure

Circuit DomainEM

structureCircuits

1. Partial Element Equivalent Circuit (PEEC) for both On & Off Board EMI

Entire EM structure is transformed into a circuit compatible form via lumped elements

Both time and frequency domain analysis

Exploit numerical advances in circuit domain

Numerically inefficient at high frequencies

2. TDIE, FDTD, MoM with MNA for both On & Off Board EMI

EM DomainEM

structureCircuits

Combine EM analysis with Circuits in EM domain

EM effects are fully capturedCannot exploit numerical advances customized for each domainDiscretisation is dictated by the parameters in both domain

3. S-Parameters

EM DomainEM

structure

Circuit DomainEM

structureCircuits

S-Parameters

Freedom to choose the best solver for each domainExploit numerical advances in each domainSuitable for optimization in both domainNumerically expensive for large number of portsCan handle only on-board EMI

Concurrent On & Off Board EMI Analysis

N PortS-Parameter

Network

1P

2P

iP

1+iP2+iP

NP

kincEr

incHr

PN+1

N+1 PortModal

S-ParameterNetwork

1P

2P

iP

1+iP

2+iP

NP

1+NP

ZLi+1

modal1+iV total

1+iVenforced

iV 1+

ZLi+2

modal2+iV total

2+iVenforced

iV 2+

ZLN

modalNV total

NVenforcedNV

ZL1

modal1Vtotal

1VenforcedV1

ZL2

total2V

enforcedV2 modal2V

ZLi

totaliV

enforcediV modal

iV

EMIV

External EMI Contributions

Conventional S-parameters Hybrid S-parameters

PPPPP

P

PPPPPPPPPPPP

PP P PP

P PP P

PPP

P

P

PPP

P PPP

Step1:Define additional port to represent external EM wave

Step3: Perform open circuit analysis to obtain Hybrid S-parameters from modal voltages

Hybrid S-Parameters for PCBs

⎥⎥⎥⎥⎥

⎢⎢⎢⎢⎢

⎥⎥⎥⎥⎥

⎢⎢⎢⎢⎢

=

⎥⎥⎥⎥⎥

⎢⎢⎢⎢⎢

+++++

+

+

+kN

kN

k

kNN

kNN

kN

kNN

kNN

kN

kN

kN

k

kN

kN

k

aa

a

HSSSHSSS

HSSS

bb

b

1

1

1,1,11,1

1,,1,

1,1,11,1

1

1

M

L

L

MOM

L

M

Step2: Solve EM structure with ports open and GPOF analysis along the transmission lines

Step4: Solve resulting network in circuit simulator

E

k

Key Advantages of the Proposed Method:• Concurrent On & Off Board EMI Analysis• Separate Analysis of EM Structure and Circuit Components (As opposed to combining whole problem into single system matrix)

- EM structure is analyzed at best via EM Solvers- Electronic devices are handled most efficiently with circuit solvers

• Efficient Analysis of RF-Digital Systems via SPICE or HBM

scatocrefref

refPCBEF

NrefN

scatocrefrefrefrefrefref

scatocrefref

scatocN

scatoc

NN

NNNNNN

NN

N

VZZZEZ

HSEa

VZZZaZZZZZZb

VbaZZbaZ

VaHZVIZV

V

aI

I

HZZZ

HZZZ

V

V

N

11

01

01

11111

1

1

1

1

1

1,,1,

1,1,11,11

||][ , Z

||Set

][][

][ where ,

1

−−−

+

+

−−−−−

+

++

+

⎟⎟⎠

⎞⎜⎜⎝

⎛+⎟

⎠⎞

⎜⎝⎛==

⎟⎟⎠

⎞⎜⎜⎝

⎛+⎟

⎠⎞

⎜⎝⎛+⎟

⎟⎠

⎞⎜⎜⎝

⎛−⎟

⎠⎞

⎜⎝⎛

⎟⎟⎠

⎞⎜⎜⎝

⎛+⎟

⎠⎞

⎜⎝⎛=

+−⎟⎠⎞

⎜⎝⎛=+

=+=⎥⎥⎥

⎢⎢⎢

⎥⎥⎥⎥

⎢⎢⎢⎢

⎥⎥⎥

⎢⎢⎢

⎡=

⎥⎥⎥

⎢⎢⎢

+

MM

L

MMLM

L

M

How to compute ?[ ]PCBEFHS −

Terminate each port on PCB open circuit and compute induced voltage at the ports.

ZLI=10 mA

y

z

x

h=2 mm

L=250 mm

radius=0.125mm

F=2 GHz3

ˆˆ)1500ˆ500ˆ1000(

0

.

zyxkk

ezyxE rjk

−+=

++= −

)

)

100Ω

A Pair of Transmission Lines subject to External EMI

Port1=250Ω and Port2=800ΩZL1=400Ω and ZL2=400Ω

enforcedV alVmod

Extracted Propagation Constants via Generalized Pencil of Functions (GPOF)

Ideal 24.18 41.88GPOF 24.69 42.7

enforcedk alkmod

yjyjyjscat ejejejV 03.4276.4269.24

1 )61.074.0()29.137.0()04.057.0( −+− −−+−−++=yjyjyj

scat ejejejV 84.4177.4246.242 )37.016.0()29.177.0()05.056.0( −+− −−+−−++=

EMI Port

Results

Constant Forced Voltage Sources

Intentional EMI on RF Power Amplifier, and impact on Digital Modulation Schemes

Free Scale MRF281S Class AB RF Power Amplifier

GSM Band

W-CDMA Band

Input MatchingNetwork

D

S

G

Gate Bias Network

Drain Bias Network

Output MatchingNetwork

RF Blocker RF Blocker

DCBlocker

DCBlockerIN

OUT

Designed by ElectroScience Lab EMI/EMC team in conjunction with Non-linear RF Lab

Optimized for best performancein GSM and W-CDMA Band

Agilent ESG 4438C

Anritsu MG3692A CW Generator

EM

I

Measurement and Post-Processing Setup-Device Level Upset-

VECTOR SIGNAL GENERATOR

Post-Processing in MATLAB

Mul

ti-to

neda

ta

LSNA

EMI is injected into gate of PA

Extraction of Gain

GSM BandW-CDMA Band

f0@ 0.94 GHz (GSM Band)EMI @ .95GHz Single Tone

Nonlinear region

P1dB=35 dBm

8dB degradation

Effects of Intentional EMI on Performance of Power Amplifier

Intentional EMI leads to significant degradation on gainof PA , partially due to that

o power is distributed over intermodulation products

o device heats up very quickly

EMI at 0.949GHzEMI Power=15dBm

Harmonic Balance Parameters:Order=4

Gain decreased by 3 dB

Without EMI

Degradation of Gain due to high power EMI-ADS Simulations-

Output Power

0.5 1.0 1.5 2.0 2.5 3.0 3.50.0 4.0

0

-50

50

RF_

spec

trum

m1m1indep(m1)=plot_vs(RF_spectrum, freq)=24.450Pavs=5.000000

9.400E8

0.5 1.0 1.5 2.0 2.5 3.0 3.50.0 4.0

0

-50

50

freq, GHz

RF_

spec

trum

m1m1indep(m1)=plot_vs(RF_spectrum, freq)=21.328Pavs=5.000000

9.400E8

Gain decreased since power is distributed over intermodulation products

EMI on Digital Modulation Schemes

Digital Modulation

Constant Envelope Non-constant Envelope

• In-band EMI Interference• Out-of-band EMI Interference

QPSKBPSK MSK

• In-band EMI Interference• Out-of-band EMI Interference

QAM16

Why digital modulation?• More Information Capacity• Higher Data Security• Better Quality

What are the observables?

How much power (in-band/out-of-band) is needed to fail a typical communication system

Which modulation scheme is more susceptible to EMIWhat modulation features play critical role in system level upsetEffects of Intentional EMI imposed onto devices on performance of communication system

Agilent ESG 4438C Anritsu MG3692A CW Generator

Serial/Parallel Converter

t0cosω

t0sinω

)(tI

)(tQ

)(ts

EM

I

Measurement and Post-Processing Setup-System Level Upset-

VECTOR SIGNAL GENERATOR

Post-Processing in MATLAB

Raw

dat

a

LSNA

Demodulation

ConstellationEVM analysis

EMI is injected into gate of PA

Error Vector Magnitude (EVM)

I

Q

Ideal Symbol

Measured Symbol Error Vector Magnitude(EVM)=

isiz

|| ii sz −

∑∑ −

=

ii

iii

RMS s

szEVM 2

2

||

||

EVM is a figure of merit for transmit modulation3GPP standard in assessing the quality of signal transmittedIt possesses direct relation with BER and SNR

Constant Envelope Modulation- QPSK

QPSK: Constellation Diagram

I

Q11

10

01

00

Quadrature Phase Shift Keying (QPSK)

Applications

• Digital Video Broadcasting-Satellite (DVB-S)• Code Division Multiple Access (CDMA)

• Wireless Local Loop

Serial/Parallel Converter

t0cosω

t0sinω

)(tI

)(tQ

)(ts

Performance : 2 bits/second/Hertz

QPSK: Performance of PA in NonLinear Region (No EMI)

MHzf 9400 =

Input @ 22dBm

MHzf 9400 =

Output

Intermodulation products due to high nonlinearity

MHz20

MHz20

64 bit random data sequence is input to the system

MHzf 9400 =

Input @ 2dBm

MHz20

EMI @18dBm

QPSK: Out-of-Band EMI (18 dBm : 0.63V)

Output

Device is forced to nonlinear region but very minimal effect on the performance

MHzfEMI 1885=

Intermodulationproducts

64 bit random data sequence is input to the system

BPSK: Performance of PA in Linear Region (No EMI)

I/Q at the output

64 bit random data sequence is input to the system

MHzf 9400 =

Input @ 9dBm

MHzf 9400 =

Output

MHz20

MHz20

MHzf 9400 =

Input @ 2dBm

MHz20

EMI @18dBm

BPSK: Out-of-Band EMI (18 dBm:0.63V)

Output

MHzfEMI 1885=

Intermodulationproducts

64 bit random data sequence is input to the system

Device is forced into nonlinear region by intentional EMI but strong effect on system performance

EVM Comparison for Modulation Sche me sIn-band EMI of -5 dBm (31.6 mV)

MSKBPSK

QAM16QPSK

0

0.05

0.1

0.15

0.2

0.25

0.3

0.35

0.4

EV

M (R

MS)

EVM Comparison for Modulation Sche me sIn-band EMI of 0 dBm (100 mV)

QPSK

MSK

QAM16

0

0.1

0.2

0.3

0.4

0.5

0.6

0.7

EV

M (R

MS)

EVM Comparison for Modulation SchemesOut-of-band EMI of 18 dBm (0.63V)

QPSK

MSK

BPSKQAM16

0

0.005

0.01

0.015

0.02

0.025

0.03

0.035

0.04

0.045

0.05

EV

M (R

MS)

Electronic systems employing constant amplitude modulation schemes are less susceptibleto intentional EMI than those employing varying modulation envelopes

Comparison of Modulation Schemes Subject to Intentional EMI

Constant envelope modulation schemes

In-band interference plays the most critical role in failing communication systems

Step 1: Scattering from Surrounding Structures

Step 2: EMI/EMC Analysis of Cables

Step 3: Scattered Fields from Cables

Step 4: Induced Current on PCB Interconnects

EMI/EMC Analysis In Presence of Complex Enclosures

Cascaded Cavity Structure with Penetrating Wires, Cables, Analog/Digital PCBs and Enclosed Cavitiesa) Compact Range/ Open Air Measurementsb) Shielding Effectiveness Study for 1-3 GHzc) Induced Voltages at loadsd) Coupling Between Penetrating and Shielded Cables

Tools/Methods

Printed Circuit Boards (PCBs) a) Hybrid S Parametersb) PEEC

Large Surrounding Structures1. Modal MoM (Green’s

Functions)2. EMCAR (MLFMM)

Interconnecting CablesTICE (Telegrapher’s IterativeCoupling Equations)

Proposed Hybrid Solution

Experiment/Validation

Scattered Field Einc(r) at locations of PCB Interconnects and Cables enclosed within Empty Enclosure

Eapt(r)

Zth

a) Terminate Cables connecting to PCB by Thevenin’s Equivalentb) TICE for Induced Current and Voltages on Cables

+-

+-

+-

+-

Vs Vs

a) Direct Coupling: PEEC with Incident Field as Voltage Sources

b) Indirect Coupling: Induced Current on Cables conductively flowing into PCB traces

Structure being tested

Compact Range Measurements

Empty Cavity

Cavity with Penetrating Wires

UH Cavity

Clemson Cavity

Timer

Timer Susceptibility Analysis

Ant

enna

The system level analysis will study two factors:

EMI on Automotive Systems: Timer Susceptibility(University of Maryland) Future Activity

• Effects of HPM pulse duration and repetition rate• Best direction and polarization to fail the device

IC Design of D-latch and Timer using MOSIS0.5μ and 1.5μ technology line. UMD will perform device level upset

while OSU will study system level upset in complex platforms.

T

Enable

TO1

O2

O3

O4