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Introduction to Transfer Path Analysis

Realize innovation.Restricted © Siemens AG 2016

31-01-2019

Unrestricted © Siemens AG 2019Page 2 Siemens PLM Software

Transfer path analysis for mechanical industry The basics, from theory to practice

1 • What is TPA ?

2 • Practical considerations

3 • Strain TPA

4 • Time TPA

5 • Component TPA

31-01-2019

Unrestricted © Siemens AG 2019Page 3 Siemens PLM Software

Transfer path analysis for mechanical industry The basics, from theory to practice

1 • What is TPA ?

2 • Practical considerations

3 • Strain TPA

4 • Time TPA

5 • Component TPA

31-01-2019

Unrestricted © Siemens AG 2019Page 4 Siemens PLM Software

Transfer Path AnalysisIntroduction

air-bornestructure-

borne

structure-

borne

Transfer path analysis quantifies and visualizes the strengths of selected sources and their contribution via multiple transmission paths to a selected receiver signal

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20.00

80.00

dB Pa2

Transfer Path Analysis Source-transfer-receiver approach

Most time spent during a TPA is on measuring:• Fi and Qj during operation• FRF functions correctly

X =Source (Fi,Qj) Transfer (FRF) Receiver (yk)

==

+=p

1jjjk

n

1iiikk Q*FRFF*FRFy

=

structural airborne=

MeasuredCalculated

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Transfer Path AnalysisStep 1: Which path is contributing?

air-bornestructure-

borne

structure-

borne

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Transfer Path AnalysisStep 2: Why is path contributing?

== =

XX X

criticaldynamics

criticalloads

worst casescenario

SourceStructural / Acoustic

Loads

Transmitter

ReceiverNoise &

Vibration

System characteristics

!

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System Engineering for NVHSource-transfer-receiver model

• Generic structured way to analyze NVH characteristics

• Founded in Test, used in both Simulation and Test

Pa

Mea

sure

d..

Tota

l

be_f

:18:

X..

be_f

:18:

Y..

be_f

:18:

Z..

be_f

:501

8:X

..

be_f

:501

8:Y

..

be_f

:501

8:Z

.. be_r

:9:X

..

be_r

:9:Y

.. be_r

:9:Z

..

be_r

:500

9:X

..

be_r

:500

9:Y

..

be_r

:500

9:Z

..

sh_f

:30:

X..

sh_f

:30:

Y..

sh_f

:30:

Z..

sh_f

:503

0:X

..

sh_f

:503

0:Y

..

sh_f

:503

0:Z

..

sh_r

:32:

X..

sh_r

:32:

Y..

sh_r

:32:

Z..

sh_r

:503

2:X

..

sh_r

:503

2:Y

..

sh_r

:503

2:Z

..

subf

:20:

X..

subf

:20:

Y..

subf

:20:

Z..

subf

:502

0:X

..

subf

:502

0:Y

..

subf

:502

0:Z

..

10.00

60.00

dB(A

)Pa

sh_r:32:Z

0.00 350.00Hz

RMS Sum

Spectrum: PRCM:0001:S

Spectrum: PRCM:0002:S

Spectrum: PRCM:0004:S

Spectrum: PRCM:0003:S

Spectrum: PRCM:0006:S

Spectrum: PRCM:0005:S-40.00

50.00

dB(A

)

Pa

Contribution at path or group (case vs. rpm or frequency) A

X =Source Transfer Receiver

EngineTransmission

Steering wheel vibrations

Seat vibrations

Noise issues

Road input HVAC

Exhaust

==

+=p

1jjjk

n

1iiikk Q*FRFF*FRFy

=

structural airborne

=

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Hybrid Modeling – Example Engine Noise inside Cabin

Benefits of hybrid modeling:• Spend less time correlating

components. Use test representation of components in a system assembly.

• Promotes component reuse – FE model of new component and reuse of test data from legacy/previous programs.

• Smaller models Rapid design iteration (e.g. when tuning mounts).

• NVH targets can be cascaded to suppliers.

FE Representation

(FE/) Test FRF or Modes Representation

Hybrid or FE Assembly

Loads Responses

FE Representation

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Hybrid Modeling – Use Case 2(AUTO OEM)

• Test Tire Component

• Equivalent model of a damper

• FE models of Subframe, Suspension Arms, Knuckle, Strut and Brake

(Courtesy: A Hybrid Full Vehicle Model for Structure Borne Road Noise Prediction – SAE Paper 2005-01-2467)

Focus Modeling accuracy

Damping Test Rig

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Hybrid Full Vehicle Road Noise Evaluation (Simcenter and NX Nastran)

Full Vehiclein Simcenter

Trimmed bodyMeasured FRFsin LMS Test.Lab

tyre/wheelMeasured FRFsin LMS Test.Lab

SuspensionFEM

NX.Nastranrun

Loads, e.g. from

Test.Lab

Assembly Simcenter

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NVH Results –Post-processing in Simcenter Noise and Vibration Modeling

Insight• Identify the problem

Contributions• Modal Contribution Analysis• Panel Contributions Analysis• Grid Contributions Analysis• Path Contributions Analysis• Energy Contribution Analysis

Understanding Response• Operational Deflection

Shapes• Equivalent Radiated Power

ProblemFrequency

Which Modes?

Which Path?

Which Grids?

Which Panels ?

Which ODS ?

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Transfer Path AnalysisWhat needs to be measured?

During operations:• Forces going into the structure, requires in general quiet some measurements• Acoustical sources• Target locationsIn the lab: measurement of the FRF, is also a tedious job

In general, TPA is a measurement intensive application

FRF2

FRF3

FRF1

F1 F2

Q3 Measured during operations

Measured in the lab

==

+=p

1j

jjk

n

1i

iikk Q*NTFF*NTFy

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OPA method

Only operational measurements required:• Accelerations at the force locations• Pressures at the Acoustical sources• Target locations

Fast method, takes ±1 day of measurements

Transmissibility method

=

structural airborne

=

T2

T3

T1

a1 a2

p3

y

Measured

Calculated

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OPA method: Potential problems for wrong results: cross-coupling

Where each acceleration/pressure can be written as:

332211 pTaTaTy ++=

332211 ... QHfHfHa iiii ++=

Measured

Calculated

T2

T3

T1

a1 a2

p3

y

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OPA method: Potential problems for wrong results: cross-coupling

E.g.

Normally

Or the acceleration for a path is normally proportional to the force at that location

3322221122 ... QHfHfHa ++=

332112222 .. QHfHfH +

H22

H32

H12

f1 f2

Q3

a2

22 fa

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OPA method: Potential problems for wrong results: cross-coupling

With cross coupling it can happen that e.g.

Or the acceleration at one location is caused by a force at another location, causing this path, e.g. 2, to be considered to be the largest contribution while the cause is due to a force at another location

332222112 .. QHfHfH +

133221122 fatforceduepTaTandaTaT

H22

H32

H12

f1 f2

Q3

a2

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Transfer path analysis for mechanical industry The basics, from theory to practice

1 • What is TPA ?

2 • Practical considerations

3 • Strain TPA

4 • Time TPA

5 • Component TPA

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Transfer Path AnalysisOperational measurements

During operations:• Forces going into the structure, requires in general quiet some measurements• Acoustical sources• Target locations

In the lab: measurement of the FRF, is also a tedious job

In general, TPA is a measurement intensive application

FRF2

FRF3

FRF1

F1 F2

Q3 Measured during operations

Measured in the lab

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Test Based TPA Process Overview

Step 1: PreparationStep 2: Operational Measurements

Step 3: FRF MeasurementsStep 4: TPA

4

3

21

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Excitation Hardware: Simcenter QSources

Transfer Path Analysis: Requirements: One integrated process

Step 1: PreparationStep 2: Operational Measurements

Step 3: FRF Measurements

EASY & PRODUCTIVE

COMPLETE

INSIGHT

CONVINCE & INNOVATE

PARTNER

MIMO Sine Testing

Impact Testing MIMO FRF Testing

Signature Testing

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Transfer Path Analysis: Simcenter QSourcesRequirements: Efficient & Accurate FRF Acquisition

Reciprocal FRF excitation hardware Fast installation High noise levels(>100dB) Internal sound source strength

measurement Omni-directional sources

Direct FRF excitation hardware Miniaturized to the maximum Efficient installation, auto-alignment and no

external support necessary Integrated force and local acceleration sensors Enables excitation at body engine/suspension

interfaces Wide frequency range

EASY & PRODUCTIVE

COMPLETE

INSIGHT

CONVINCE & INNOVATE

PARTNER

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Transfer Path Analysis: Requirements: All Load Estimation Methods

Load Estimation Methods

AirborneStructural

Direct Measured

Mount Stiffness

Single Path InversionSingle Source –Multiple Indicator

Matrix InversionMultiple Source –Multiple Indicator

Simcenter OPAXMultiple Source –Limited Indicator

EASY & PRODUCTIVE

COMPLETE

INSIGHT

CONVINCE & INNOVATE

PARTNER

Step 4: TPA

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Transfer Path AnalysisLoad identification: mount stiffness method

2

piaiii

))(a)(a(*)(K)(F

=

operational accelerations at both sides of mount

mount stiffness

||

||

operational FORCES

||

Source

mountsactive side

passive side

...Fi

Bodyapi

aai

Ki...

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Source

mountsactive side

a1

passive side

aq av

ai

…... Fi

Body

Hiq

indicator accelerations

FRF matrix

||

=

)(a

)(a

)(a

.

)(H)(H)(H

)(H)(H)(H

)(H)(H)(H

)(F

)(F

)(F

v

2

1

1

nvv2v1

2n2212

1n2111

n

2

1

||

operational forces

||

Transfer Path AnalysisLoad identification: matrix inversion method

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Transfer Path AnalysisMeasurements - Loads

Direct Measured Direct measured forces

Mount Stiffness

Single Path InversionSingle Source –Multiple Indicator

Matrix InversionMultiple Source –Multiple Indicator

=

oper

oper

oper

oper

x

x

x

F

x

F

x

F

x

F

1002

1001

1

1

1

1002

1

1001

1

1

1

=

oper

m

oper

n

mm

n

oper

n

oper

x

x

F

x

F

x

F

x

F

x

F

F

...

...

.........

...

...

1

1

1

1

1

1

1

ts XXKF =

Structural

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Transfer Path AnalysisMeasurements - Loads

Direct Measured Direct measured forces

Mount Stiffness

Single Path InversionSingle Source –Multiple Indicator

Matrix InversionMultiple Source –Multiple Indicator

Simcenter OPAXMultiple Source –Limited number of Indicator

=

oper

oper

oper

oper

x

x

x

F

x

F

x

F

x

F

1002

1001

1

1

1

1002

1

1001

1

1

1

=

oper

m

oper

n

mm

n

oper

n

oper

x

x

F

x

F

x

F

x

F

x

F

F

...

...

.........

...

...

1

1

1

1

1

1

1

ts XXKF =

Structural

Assume model => reduce indicators by identifying reduced set of model parameters

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Transfer Path AnalysisMeasurements Simcenter OPAX

• Soft mounts

• Hard mounts

= piaiii aaparametersFHP ,,

2

= piai

ii

aaKF

2

= ai

ii

aKF

(dis)advantages

• Limited set of FRFs required

• No disassembly into trimmed-body condition (depends on the expected accuracy)

• Limited body-information (compared to Matrix-Inversion)

Frequency

Dyn

amic

stif

fnes

s mount stiffnessband estimator model

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Body

F2’F1

y = F1 x FRF1 + F2’ x FRF2

FRF measurement without removing source

Only valid if

F2’ x FRF2 << F1 x FRF1

Transfer Path AnalysisMeasurements – Transfer functions – Removal of source

Body

F2

F1

y = F1 x FRF1 + F2 x FRF2

Operational condition

Body

F2 = 0F1

y = F1 x FRF1

Correct method for FRF measurement

Use only when:

• Coupling is weak between paths

• Able to hit at force location

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Demo

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Transfer path analysis for mechanical industry The basics, from theory to practice

1 • What is TPA ?

2 • Practical considerations

3 • Strain TPA

4 • Time TPA

5 • Component TPA

31-01-2019

Unrestricted © Siemens AG 2019Page 32 Siemens PLM Software

Strain-based load identificationProblem definition: Closely coupled paths example

Road Noise TPA:

• 72 paths/loads examined

• Some forces very close together

2 times 3 forces to be identified that are very close together

Fz1Fz2

Fx1

Fy1

Fy2Fx2

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Strain-based load identification Problem Definition: Matrix Inversion

Example TPA Result: Important Path Contributions

Interior Microphone

Seat Acceleration

Measured ResponseCalculated Response (Accel TPA)Calculated Response (Strain TPA)

Both Acceleration and Strain Based TPA provide a good

quality target response synthesis

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Strain-based load identification Problem Definition: Matrix Inversion

Example TPA Result: Interior Noise

Example TPA Result: Important Path Contributions

Peak in noise level resulting from Tire Cavity Mode

Example TPA Result: set of identified Body Lads

‘Red Load’ – Load of Path 2

Based on this quick TPA acceleration result evaluation Path # 2 has an important contribution to the

interior noise Path # 2 high contribution level seems to be

related to a high force level

However, Path # 2 is the vertical load of the connection of a lateral suspension link to the body. Can this result be trusted?

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Solution Evaluation and ValidationMatrix Inversion for Road Noise studies

Acc. based Loads for a Lateral Suspension Link

Even though the target synthesis is nearly identical for the 2 TPA

methods, the identified loads however, are completely different.

Strain based Loads for a Lateral Suspension Link

Which load set is most reliable?For a Lateral Link a high Y-dir load is expected, with low level loads in X-dir

and Z-dir.

Body Load in X-directionBody Load in Y-directionBody Load in Z-direction

Factor 30!

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Strain-based load identification Problem Definition: Matrix Inversion

2 Z-dir Acceleration TPA based Loads

Acceleration TPA the 2 loads are in counter-phase over the full

frequency range

Comparison and Analysis of 2 close-by forces in Z-

direction

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Strain-based load identification Problem Definition: Matrix Inversion What is the problem?

)()()(1

aHF =

Condition Number for an example structure with a high number of inputs

Acceleration FRF Matrix Condition number is much higher as the Strain FRF Matrix Condition number

Accurate load identification using the Acceleration FRF Matrix can be problematic

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Transfer path analysis for mechanical industry The basics, from theory to practice

1 • What is TPA ?

2 • Practical considerations

3 • Strain TPA

4 • Time TPA

5 • Component TPA

31-01-2019

Unrestricted © Siemens AG 2019Page 39 Siemens PLM Software

FRF, K

Frequency domain TPA vs. Time domain TPA

FRF Filter FRF Filter ==

== X

NTF

Freq

uenc

y D

omai

n TP

ATi

me

Dom

ain

TPA

Auralization, Signature Analysis, Sound Quality metrics ...

Indicators (orders, spectra)

Loads (orders, spectra)

Path contributions (orders, spectra)

Indicators (time traces)

Frequencysource model

Frequencytransfer model

Loads (time traces) Path contributions (time traces)

440.0020.00 HzFSUB:0105:-Y (CH1)

4500.00

900.00

rpm

Tach

o1 (T

1)

-10.00

-110.00

dB g

440.0020.00 HzFSUB:0105:+Y (CH1)

4500.00

900.00

rpm

Tach

o1 (T

1)

20.00

-80.00

dB N

440.0020.00 HzFRLE:S (CH2)

4500.00

900.00

rpm

Tach

o1 (T

1)

70.00

-30.00

dB Pa

120.000.00 s

0.60

-0.70

Rea

lg

1.00

0.00

Ampl

itude

X

120.000.00 s

24.00

-24.00

Rea

lN

1.00

0.00

Am

plitu

de

120.000.00 s

0.10

-0.12

Rea

lP

a

1.00

0.00

Am

plitu

de

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0 500100 200 300 40050 150 250 350 45025Hz

0

24

10

20

4

8

1416

Ampl

itude

(m/s

2)/N

Frequency domain TPA vs. Time domain TPA

Frequency Domain TPA

Order analysis Spectrum analysis

Run-up & run-down Stationary: e.g. road noise

Analysis as a function of rpm/frequency

Component editing Source and NTFs

Auralization Not directly possible

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Frequency domain TPA vs. Time domain TPA

Frequency Domain TPA

Order analysis Spectrum analysis

Run-up & run-down Stationary: e.g. road noise

Analysis as a function of rpm/frequency

Component editing Source and NTFs

Auralization Not directly possible

Time Domain TPA

Time traces:

Run-up & run-down Stationary: e.g. road noise Transient: e.g. engine start-up Semi-stationary: e.g. idle noise,

frequency modulation …

Analysis as a function of time

Component editing Source and NTFs

Auralization Audio replay

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Time-Domain TPA for PBNInstrumentation

Lr

=

yk

NTFki

W

12k

d

x = 0 x = -

= targets (measured & predicted)

= indicators (measured)= sources (to be identified)

Qi

Hji

=uj

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Time-Domain TPA for PBN Force / target response calculations

transmissionexhaustenginetire

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Time-Domain TPA for PBN PBN Contribution Analysis – Example in 3rd gear

11.75-5.00 mVehicle Position

70.00

20.00

30

40

50

60

25

35

45

55

65

23

28

33

38

43

48

53

58

63

68

dB(A

)Pa

4.57

Curve 4.57 m68.18 dB(A)68.08 dB(A)63.68 dB(A)52.90 dB(A)53.64 dB(A)62.45 dB(A)53.77 dB(A)61.63 dB(A)54.44 dB(A)

F Left SideF Left Side - TotalF Left Side - Pow ertrainF Left Side - ExhaustF Left Side - TailpipeF Left Side - Tire_FLF Left Side - Tire_FRF Left Side - Tire_RLF Left Side - Tire_RR

11.75-5.00 mVehicle Position

70.00

20.00

30

40

50

60

25

35

45

55

65

23

28

33

38

43

48

53

58

63

68

dB(A

)Pa

5.14

Curve 5.14 m68.23 dB(A)68.21 dB(A)64.15 dB(A)56.00 dB(A)56.59 dB(A)54.55 dB(A)60.85 dB(A)54.62 dB(A)61.13 dB(A)

F Right SideF Right Side - TotalF Right Side - Pow ertrainF Right Side - ExhaustF Right Side - TailpipeF Right Side - Tire_FLF Right Side - Tire_FRF Right Side - Tire_RLF Right Side - Tire_RR

Left Right

Good match between measured I-PBN result and synthesized ASQ I-PBN result

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Demo

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Transfer path analysis for mechanical industry The basics, from theory to practice

1 • What is TPA ?

2 • Practical considerations

3 • Strain TPA

4 • Time TPA

5 • Component TPA

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Unrestricted © Siemens AG 2019Page 47 Siemens PLM Software

Blocked force/free velocity principle

Source A 21SOURCE MECHANISM

Blocked

Source A 21SOURCE MECHANISM

Free

𝐹2𝐵𝑙1. Blocked Force

2. Free Velocity

𝐴2𝐹𝑟𝑒𝑒

𝐹2𝐵𝑙= 𝐻22

𝐴 −1 𝐴2𝐹𝑟𝑒𝑒

Blocked force/free velocity is a property of the component independent of the environment it’s assembled in

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Converting Blocked Force (spring connection) to assembly connection forces

ComponentA

StructureB1

2 3

4Responses

K

𝐹2𝑟 = 𝐹3𝑟 = 𝐻22𝐴 +𝐻33

𝐵 + 𝐾−1 −1 ∗ 𝐻22𝐴 ∗ 𝐹2𝑏𝑙

𝐴

Sourceforce

𝐹2𝑟 = 𝐹3𝑟 = 𝐻22𝐴 +𝐻33

𝐵 + 𝐾−1 −1 ∗ 𝑣2𝑓𝑟𝑒𝑒𝐴

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Example ApplicationsSteering System

Source Mechanism InvariantSource Synth. Model Sub-Receiver Receiver

Steering System

BlockedForces &

Impedances Mount Pos.

SubframeFEM/TEST

FRF

BodyFEM/TEST

FRF

Invariant Source Load (TEST) Full System Transfer Function

bench

1

A

𝑎𝑖𝐶xx

x

𝐻𝑖1𝐶

𝐹𝑏𝑙𝐴

𝐹𝑏𝑙𝐴 = 𝐻𝑖1

𝐶 −1 ∗ 𝑎𝑖𝐶

𝐹𝑏𝑙𝐴

3𝑝

1 2

AB

𝐹𝑟

𝐹𝑟 = 𝐻11𝐴 + 𝐻22

𝐵 + 𝐾−1 −1 ∗ 𝐻11𝐴 ∗ 𝐹𝑏𝑙

𝐴

𝑝 = 𝐻32𝐵 ∗ 𝐹𝑟

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Example ApplicationsRoad Noise - Tire

Source Mechanism

TireRoadNoise

Invariant Source Load (TEST)

Example: Invariance of wheel center blocked force: Strongly coupled

system & coupled to very different vehicles

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Concept: Component Based TPATest components and virtual assemble components

Engine

Exhaust

Tyres

MountEPS

(H)EV

Wiper System

Transmission

HVAC

Benefits:• Can try out different car variants before there is a prototype.• Can use this technique for component target setting Less surprises

when assembling the vehicle.• Can find out worst case combination and limit validation/testing to this

configuration Intelligent reduced testing

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Thank You

Filip DeblauweTechnical Manager Test Solutions CoEInterleuvenlaan 683001 LeuvenBelgium

Phone: +32 16 384 437

E-mail:[email protected]

siemens.com