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www.cst.com | CST EuMW 2010 Presentations| September 2010 | 1 A Glimpse into Multiphysic-Analyses using CST STUDIO SUITE™ Accounting for thermal heating effects and mechanical deformation in the electrical design

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Page 1: A Glimpse into Multiphysic-Analyses using · | CST EuMW 2010 Presentations| September 2010 | 1 A Glimpse into Multiphysic-Analyses using CST STUDIO SUITE™ Accounting for thermal

www.cst.com | CST EuMW 2010 Presentations| September 2010 | 1

A Glimpse into Multiphysic-Analyses

using

CST STUDIO SUITE™

Accounting for thermal heating effects and mechanical

deformation in the electrical design

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www.cst.com | CST EuMW 2010 Presentations| September 2010 | 2

EM-field computation

Thermal

analysis

Stress analysis /

deformation

EM-properties of deformed geometry

can be fed into sensitivity analysis

The Motivation …

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Thermal Simulation

Mechanical Stress Simulation

CST MPHYSICS STUDIOTM

Courtesy of Spinner GmbH, Germany

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Online Demo

Page 5: A Glimpse into Multiphysic-Analyses using · | CST EuMW 2010 Presentations| September 2010 | 1 A Glimpse into Multiphysic-Analyses using CST STUDIO SUITE™ Accounting for thermal

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Example : 2-Post Bandpass Filter

Rel Bandwidth:0.9 %

Page 6: A Glimpse into Multiphysic-Analyses using · | CST EuMW 2010 Presentations| September 2010 | 1 A Glimpse into Multiphysic-Analyses using CST STUDIO SUITE™ Accounting for thermal

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1) EM (FD tet)

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1D Results > |S| dB

Tchebychev Filter

===================

Order = 2

Bandwidth = 5 MHz

Center Frequency = 570 MHz

Passband ripple = 0,01 dB (1,100747 VSWR)

Return loss = -26,3828 dB

Normed g values:

-------------------------------------------

g1 = 0,4489

g2 = 0,4078

g3 = 1,1008

Corresponding coupling coefficients in MHz / (rel):

-------------------------------------------

k_E = 11,14 (0,0195413)

k1_2 = 11,69 (0,0205021)

k_out = 11,14 (0,0195413)

Group Delay Time

----------------

t_d1 = 57,153 ns

t_d2 = 51,922 ns

t_d3 = 0, ns

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Power Loss Dens. > loss (f=0.575)

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Power Loss Dens. > loss (f=0.575)

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Current Density (f=0.575)

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Export the Thermal losses

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2) Thermal Solver

Import the losses from EM FD

5000

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Thermal boundariesThermal volume losses as sourceThermal boundaries

Temperature Heat flow

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3) Mechanical Solver

FxKxBxM

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http://www.engineeringtoolbox.com/young-modulus-d_417.html

1 GPa = 1kN/mm2σ=ε.E

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Displacements > displacement1Define a displacement eg at a face (xyz) directly at the WG-Port

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Import a field source (from therm),

and activate it

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2D/3D Results > DisplacementTemperature change as source Mech. Displacements

Von Mises Stress Deformed Mesh

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Matrix to solve: QEK

[K]: symmetric, complex, contains geometry, material, frequency

xi, yi

Example: Linear Shape functions for a 2D element in xy

jkijkkjijkkjkjijk

kji

kji

kji

xxcyybxyyxa

ccc

bbb

aaa

yxN ;;;.,,12

1

xj, yj

xk, yk

k

j

i

kji

z

z

z

NNNz ],,[

zi

[E]: unkowns z

[Q]: Sources

kjinmdxdyx

N

x

N

x

N

x

Nk nm

ynm

xy

xnm ,,,;)(,

Example: electrostatic

4) Sensitivity ( Introduction)

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),(),(),(1

),(0

pEpKpEj

pS TT

Introduction to Sensitivity

S-Parameters:

[K] …left hand side, E (Fields at ports, p… any parameter

Ep

KE

p

Sj T

0

Sensitivity of S-parameter vs. parameter change:

Direct analytical derivation of

K-matrix elements via e.g. [N]

3D Fieldsolution

Same 3D Fieldsolution

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Numerical calculation of gradients is expensive and unstable

Here: Sensitivity of S-parameter vs. parameter change

no additional 3D solution required (only another S-Parameter computation)

Very efficient computation of sensitivities

Result: S-parameter ranges for tolerant parameters

Currently available for FD-Tet solver

Introduction to Sensitivity

Ep

KE

p

Sj T

0

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pp

SSS

p

MWSDnmnm .)3(

What is it good for?

The sensitivity helps estimate „new“ S-parameters due to the (small) change

of the parameter, at no extra cost

Suppose the parameter p changes by a quantity ∆p :

exact computation of the Sensitivity

(Approximated by 1st order Taylor expansion)

Introduction to Sensitivity

The various sensitivities are used in an optimizer to solve for ∆p as variables to

best fit the S-parameter goals.

∆p … face constraints

pp

SxSpxS

p

.)()(

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For every product, there are:Technical specifications

Fabrication tolerances

The fabrication tolerances will lead to some

products not fulfilling the specifications

Yield:

What is the Yield Analysis

Total

Passedyield

#

#

Gaussian

Uniform

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How is yield calculated typically?

Parameters vary according to a known probability curve

Repeat

Change the value of all parameters

Simulate

Check if specification (in our case for S-params.) is met

Until the number of simulations is statistically relevant

This is a large number of EM simulations - typicaly hundreds or thousands!!!

Knowing the sensitivity, there is no need to perform 3D simulations, at least ifthe parameters vary in a small range.

The efficiency of this new sensitivity analysis approach makes Monte-Carlo based yield analysis feasible even for complex multi-parametrical three-dimensional structures

Typical Approach vs. CST Approach

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Import the displacements

4) Sensitivity (based on mech. Displacements)

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Setup Sensitivity Analysis

4) Sensitivity

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Display S-parameter Sensitivity

4) Sensitivity

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Summary

Integrated workflow with

CST MPHYSICS STUDIO™

Ease-of-use: New solvers within

well known frontend

Accuracy of integrated solution and

solver technology

Wide application range due to tight

integration within CST STUDIO SUITE™

Thermal

Structural Mechanics

EM

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Thank you for your attention!