simulating dielectric and conductor lossimapsne.org/virtualcds/2016/2016...
TRANSCRIPT
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Simulating Dielectric and Conductor Loss
Including surface roughness
Tracey Vincent
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Overview
Loss components
Conductor:
Skin effect
Simulating surface roughness:
Tabulated surface impedance: Hammerstad, Huray
3D models- Periodic surface, random surface
Effective Dielectric method – (Dr. M. Koledintseva )
Dielectric:
Theory and parameters
Nth order curve fitting
Using Measurements and Simulation to extract material parameters
Discussion and conclusion
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Mismatch
Conductor
Dielectric
Loss
Coupling
Radiative
Loss Components
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Simulating Conductor Loss
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ohms/meter 1
SRDC
ohms/meter
ohms/meter 1
P
R
PR
S
AC
P is the circumference of the
conductor, δ is skin depth. The δP
is the equivalent cross-section
area.
S is the cross-section area of the
conductor.
σ is the volume conductivity.
Current is homogenous.
Current density increases at extremities at RF frequencies
2
Cross-sectional area of round conductor
At DC
Current density
fills cross-
section
At AC
Current density
moves toward
extremities
At GHz frequencies
Current density
concentrated at
extremities
Skin Effect Theory
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i r
thigh
Field = 0
Surface
impedance
Alternative
Skin Effect – Lossy Metal
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Change conductivity.
Narrow band “quick”
parameterization:
Broadband material type: tabulated surface
impedance parameterization. Huray, Hammerstad
models
Surface Roughness Parameterization - Features
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40mm long microstrip model
FR4 dielectric substrate –εr=4.3, tg δ=0.025
Comparison of Results for Simple Model
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FR4 dielectric substrate –εr=3.5, tg δ=0.06
50mm long stripline model
Measured and Simulated Data for Stripline
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Analytical Face surface. Periodic example.
Equation, such as polynomial can be used to
generate non-smooth trace.
Example is periodic trace: w=Ra*sin(b00u).
All of these waveforms have same
average roughness Ra
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Face Distortion Surface
Trace generated has random distortions, specifications are: peak to peak height,
average distance between peaks
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Reference: Koledintseva, Razmadze, Gafarov, De,
Drewniak, Hinaga “PCB Conductor Surface Roughness
as a Layer with Effective Material Parameters”
Electromagnetic Compatibility (EMC), 2012 IEEE
International Symposium 2012
New Analytical Method “Roughness Dielectric”- Concept
Ar
(μm)
Λr
(μm)
Ar/Λr
Ra
(μm)
Rz
(μm)
Rrms
(μm)
STD 7.98 10.62 0.75 1.56 8.41 1.91
VLP 3.35 7.28 0.46 0.75 4.19 0.92
HVLP 1.65 4.69 0.35 0.35 2.29 0.44
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“Roughness Dielectric”- Extracting the parameters
Reference: Koul, Koledintseva, Hinaga, Drewniak
“Differential Extrapolation Method for Separating
Dielectric and Rough Conductor Losses in Printed
Circuit Boards” IEEE Trans, 2012.
a + b = K1 c + e = K2 d + f = K3
22 fedcbaT
Curve fitting co-efficients are generated K1 ~ √ω , K2
~ ω, and K3 ~ ω²
K1(0), K2(0), and K3(0) corresponds with smooth
conductor, allow separation of surface roughness loss
and dielectric loss. K co-efficients relate to Ar
Dielectric material (smooth) 3D object with extracted
“roughness” parameters can be included in simulation
to simulate roughness impact
“smooth”
conductor
contribution
/skin effect
Dielectric
contribution
Roughness
contribution
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“Roughness Dielectric”- Concept
Tr foil
Copper foil
conductors
Foil side
‘roughness
dielectric’
Laminate fiberglass filled
composite dielectric
• Laminate dielectric parameters are extracted from DERM2
(for both and ).
• Heights of ERD Tr foil are taken 2Ar foil, respectively.
• Line length for this model = 15,410 mils
Cross section
view - Not to
scale for
presentation
purposes only
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Comparison of S21 Results
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Design Curves
Design curves - can tie the ERD parameters to the roughness factor so design engineer does not have to do extrapolation
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Simulating Dielectric Loss
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Dielectric Loss Theory – 1st Order Debye Dispersion
0
10
20
30
40
50
60
70
80
0.1 1 10 100 1000
f (GHz)
ε' ε" ε static
ε infinity
Relaxation frequency
'DK
'
"tan
DF
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0E
0E
Such dielectric behavior can be modeled by including many relaxation terms, each
localized around different frequency.
Common PCB/package dielectric materials exhibit gradual change in dielectric
constant over a very broadband frequency range.
Dielectric Material Theory
Relaxation Process
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Definition: in any passive circuit, the effect always has to follow the cause.
Sources of non-causality: Measurement, simulation (resonance, round error,
interpolation, and extrapolation), and data manipulation.
Time domain solvers are broadband, curve fitting will retain causality.
“The man who shoots faster than his shadow“
.....“The shadow shoots the man?!?“
Dielectric Loss – Causality
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0
''
1
)(
j
r
0
'
'
1
)(
j
j
N
i
i
r
i
Why nth order? The transient solver is broadband (often more broadband that device modeled),
dispersive materials: fit required.
nth order Debye/Lorentz fit more accurate than simple Debye or Lorentz models.
Dielectric Loss – Curve fitting Nth Orders
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Curve Fitting Comparison – S21 Results
40mm long microstrip model
FR4 dielectric substrate –εr=4.3, tg δ=0.025
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Dielectric Loss – Curve Fitting Nth Orders – S21 Results
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What if you don’t have sufficient material properties for your simulation?
They can be extrapolated (and simulation can help)
Simulation can be used to Characterize Dielectric properties.
Different methods: Full Sheet Method, Ring Resonator, 2 through lines
Dielectric Loss Characterization
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Reference: E. Engin
“Extraction of Dielectric
Constant and Loss Tangent
Using New Rapid Plane Solver
and Analytical Debye
Modeling for Printed Circuit
Boards”, IEEE MTT 2010.
CST
FSR with Electric Shield - Results
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Extracted DK and DF
Cavity measurement
1st resonance
2nd resonance
3rd resonance
Extracting dielectric parameters with FSR
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Novel thru-line technique: calibration standards
Thru and Line are much larger than 𝜆
4
Longer length increases sensitivity to substrate
loss
MACRO for automated extraction
Research by CST and Czech Technical
University in Prague.
Dielectric Loss Characterization – Ring
Resonator
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Dielectric Loss Characterization – Two Through
lines
ε' ε”
High quality end-launch connectors should be used in order to keep constant error model of the coaxial to microstrip line transition (NO soldering of the connectors!)
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Automatic extraction Macro
1(a) Extracts complex permittivity from
measurement of two lines* (Thru, Line)
using 3D EM line model.
1(b) Extracts complex permittivity from
directly measured S-parameters of a
section of homogeneous transmission
line (transmission coefficient egL) stored
in Touchstone file using 3D EM line
model. Multiline calkit and NIST
Multiline TRL calibration technique is
usually used for this option.
1(c) Extracts DUT S-parameters using
just Thru and Line calibration
standards*.
* 1st tier calibration at coaxial line is required.
(a)
(b)
(c)
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40mm long microstrip model
FR4 dielectric substrate –εr=4.3, tg δ=0.025
Curve Fitting Comparison – S21 Results
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Dielectric Loss – Curve Fitting Nth Orders – S21
Results
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Where Does the Power go? Separating the
Components
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Current density Surface current
E field
Where Does the Power go? Monitoring the
Fields
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Materials properties
Dielectric: eps=3.6, tgd=0.01 Debye 3rd order
Copper = 4.1e7 S/m with inclusion of surface roughness with TSI (H&J model)
Real Case Example
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S-Parameter and TDR Results
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More information: webinars
https://www.cst.com/Events/Webinars#
Questions?