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LMS
INTERNATIONAL
CMC - TPA training - May, 2005 1
Transfer path analysis
P
LMS
INTERNATIONAL
CMC - TPA training - May, 2005 2
Transfer path analysis
Application background
 Structureborne noise - structural path between source and receiver
 from engine
 from suspension
 from exhaust, gearbox, drive-line
 Airborne noise - no structural path between source and receiver
 engine noise
 aerodynamic noise
 radiated noise from panels
 What are the main contributors, the important transfer paths ?
Treated in ASQ
LMS
INTERNATIONAL
CMC - TPA training - May, 2005 3
Transfer path analysis
Principles
 Simplify noise/vibration path into source-receiver-transfer system
Transfer
- structure
- sound field
Receiver
- human ear
- steering wheel
Source
- connection between
excitation source and
target structure
LMS
INTERNATIONAL
CMC - TPA training - May, 2005 4
 Quantification of source-receiver-transfer system
Transfer path analysis
Principles
Transfer
- vibro-(acoustic) FRF
- Pa/N or (m2/s)/N
Receiver
- pressure or acceleration
- Pa or m2/s
Source
- force
- N
LMS
INTERNATIONAL
CMC - TPA training - May, 2005 5
Transfer path analysis
Principles
 Structure-borne noise/vibration breakdown and ranking
 Preceiver =  Pi
 Partial contribution Pi
 Pi = Fi . Hi
PF
Source : N Transfer : Pa/N
 Xreceiver =  Xi
 Xi = Fi . Hi
XF
Source : N Transfer : (m/s2)/N
:
:
:
:
LMS
INTERNATIONAL
CMC - TPA training - May, 2005 6
Transfer path analysis
Two applications
 Transfer path ranking, contribution analysis
 Preceiver =  FiHi
PF
 source or transfer problem ?
 post processing for FBS, ASQ, FE calculations
 Multiple force estimation methods
Fi ?
LMS
INTERNATIONAL
CMC - TPA training - May, 2005 7
Transfer path analysis
Source identification
 Complex dynamic stiffness method
 Acceleration measurements
 Mount rates
 Full matrix inversion
 Acceleration measurements
 FRF measurements (full matrix)
 Driving point inversion
 Acceleration measurements
 Driving point FRF
measurements
LMS
INTERNATIONAL
CMC - TPA training - May, 2005 8
Transfer path analysis
Complex dynamic stiffness method
t
x


s
x


       
 



 t
s X
X
K
F 


 Acceleration measurements on both sides of
mount
 Stiffness characteristics of mount
LMS
INTERNATIONAL
CMC - TPA training - May, 2005 9
Transfer path analysis
Complex dynamic stiffness determination

 determination of stiffness in three direction
 rotational degrees of freedom neglected
 cross-coupling effects neglected
 Automatic integration/differentiation of mount stiffness data
 Behavior of mounts is not very linear
 apply correct pre-load
 temperature effects may be important
 adapt excitation according to actual operational conditions
 
 



X
F
K 
)
(
LMS
INTERNATIONAL
CMC - TPA training - May, 2005 10
Transfer path analysis
Complex dynamic stiffness determination
Mount
Ground
Mass (pre-load)
F
vert
x

 hor
x


LMS
INTERNATIONAL
CMC - TPA training - May, 2005 11
Transfer path analysis
Inverse method
F1
x4
x3
T14
T13
F2
T24
T23
 
  2
24
1
14
2
1
4
2
23
1
13
2
1
3
.
.
,
.
.
,
F
T
F
T
F
F
f
x
F
T
F
T
F
F
f
x






F : excitation
X : response
T : transfer function



















2
1
24
14
23
13
4
3
F
F
T
T
T
T
x
x




















4
3
1
24
14
23
13
2
1
x
x
T
T
T
T
F
F
LMS
INTERNATIONAL
CMC - TPA training - May, 2005 12
Transfer path analysis
Inverse method : example
Operational measurements
 acceleration at three points
Laboratory measurements
 full FRF matrix between
excitation at point 1 and
response at the other points
1
x


1001
x


1002
x


1
1001
1002
Finput
LMS
INTERNATIONAL
CMC - TPA training - May, 2005 13
1001
1002
F1
oper ?
Transfer path analysis
Inverse method : example






























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












LMS
INTERNATIONAL
CMC - TPA training - May, 2005 14
Transfer path analysis
Singular value decomposition
 Singular value decomposition of transfer function matrix
       
   





n
i
n
i
i
m
i
nxn
mxn
mxm
mxn
V
U
V
U
H
1
*
*

 
















0
0
0
0
0
0
0
2
1
n
mxn













M : number of responses
N : number of sources
M  N
LMS
INTERNATIONAL
CMC - TPA training - May, 2005 15
Transfer path analysis
Singular value decomposition
 Example : 28x15 accelerance FRF matrix
LMS
INTERNATIONAL
CMC - TPA training - May, 2005 16
Transfer path analysis
Singular value decomposition
   
   
   
     
   













n
i
m
i
i
n
i
T
mxm
nxm
nxn
mxm
mxn
T
nxn
nxm
U
V
U
V
U
V
H
1
*
1
1
1
1
1
1

 Matrix inversion by singular value decomposition
 




















0
0
0
0
0
0
0
0
0
0
1
1
2
1
1
1
n
nxm










LMS
INTERNATIONAL
CMC - TPA training - May, 2005 17
 Matrix inversion by singular value decomposition
Over determination allowed (M  N)
 Least squares estimate
 Calculation of condition number : upper bound for
multiplication coefficient of relative error
Transfer path analysis
Singular value decomposition
n
number
condition

1
_ 
LMS
INTERNATIONAL
CMC - TPA training - May, 2005 18
 Improving the matrix condition
 Delete p singular values : condition number drops
 Three possibilities : number, relative, absolute
 Overdetermination : 2/1
Transfer path analysis
Singular value decomposition
p
n
number
condition



1
_ n-p > n
LMS
INTERNATIONAL
CMC - TPA training - May, 2005 19
Transfer path analysis
Number criterium
LMS
INTERNATIONAL
CMC - TPA training - May, 2005 20
Transfer path analysis
Relative criterium
LMS
INTERNATIONAL
CMC - TPA training - May, 2005 21
Transfer path analysis
Relation condition number / overdetermination
LMS
INTERNATIONAL
CMC - TPA training - May, 2005 22
Transfer path analysis
Selection of overdetermination points
 Overdetermination : 2n responses to estimate n forces
 Location of OD points
 good coherence with signal in transfer path
 not to close to transfer path : no extra information
 3 extra points in one direction better then 1point measured in 3
directions
 Pressure response can be included in matrix inversion
LMS
INTERNATIONAL
CMC - TPA training - May, 2005 23
Transfer path analysis
SVD example : fully trimmed car
Original FRFs + condition number Elements from inverted matrix
LMS
INTERNATIONAL
CMC - TPA training - May, 2005 24
Transfer path analysis
SVD example : body in white
Original FRFs + condition number Elements from inverted matrix
LMS
INTERNATIONAL
CMC - TPA training - May, 2005 25
Transfer path analysis
Transfer functions
 Measured in uncoupled condition
 engine, drive-line removed
 suspension removed
 Follows from substructuring formulation
 P=HA+BFi=HB([HA+HB+K-1]-1HAFi)=HBFc
HA HB
K
source target
Fc
Fi P
TPA
LMS
INTERNATIONAL
CMC - TPA training - May, 2005 26
Transfer path analysis
Transfer functions
 Always check
 Linearity
 Coherence
 Reciprocity
 Impact or shaker testing
 Coherence with hammer excitation
 Misalignment of shaker
 Small errors become important after matrix inversion
Excitation
direction
LMS
INTERNATIONAL
CMC - TPA training - May, 2005 27
Transfer path analysis
Vibro-acoustic reciprocity
i
j
j
i
PF
F
P
Q
x
H 


F1
F2
Pj
1
x


2
x


Qj
 Reduction of measurement effort
j
i
Q
x
unit
define )
(
LMS
INTERNATIONAL
CMC - TPA training - May, 2005 28
Transfer path analysis
Volume velocity source
 Volume velocity sources
 Sufficiently excite cavity and/or structure : high power
 Not influenced by acoustic boundary
 Ease of use : constant calibration factor
 Omni-directional
LMS
INTERNATIONAL
CMC - TPA training - May, 2005 29
Transfer path analysis
Features : easy model definition
 Model definition based on PID and SID annotations
mic:1:S
body:2
body:1
Data type Primary ID Secondary ID
Force body:1:+Z -
body:2:+Z -
Pressure mic:1:S -
FRF mic:1:S body:1:+Z
mic:1:S body:2:+Z
LMS
INTERNATIONAL
CMC - TPA training - May, 2005 30
x1 x2 ... xr
x11…x21…xr1
PCA
Force
id.
TPA
x12…x22…xr2 x1m…x2m…xrm
x11…x21…xr1 x12…x22…xr2 x1m…x2m…xrm
f11…f21…fn1 f12…f22…fn2 f1m…f2m…fnm
phenomenon 1 phenomenon 2 phenomenon m
Transfer path analysis
Features: support of multi-reference problems
 Support of single
reference problems :
engine noise e.g.
 Multi-reference
problems (road
noise e.g.) require
Principal
Component Analysis
LMS
INTERNATIONAL
CMC - TPA training - May, 2005 31
Transfer path analysis
Features : structure and air-borne problems
 Study contribution of structure and air-borne noise in one
analysis : Preceiver =  Fi . Hi
PF+  Qi’ . Hi’
AA
 Pre-processor required for Panel Contribution Analysis
LMS
INTERNATIONAL
CMC - TPA training - May, 2005 32
Transfer path analysis
Extensions to TPA
 Easy data grouping mechanism in post-processing
 grouping based on PID
 simplifying visualization
 Frequency spectra, ordercuts and autopowers (new) supported
 Automatic squaring of FRFs in case of autopowers
 Condition calculation : specify frequency range

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Transfer path analysis

  • 1. LMS INTERNATIONAL CMC - TPA training - May, 2005 1 Transfer path analysis P
  • 2. LMS INTERNATIONAL CMC - TPA training - May, 2005 2 Transfer path analysis Application background  Structureborne noise - structural path between source and receiver  from engine  from suspension  from exhaust, gearbox, drive-line  Airborne noise - no structural path between source and receiver  engine noise  aerodynamic noise  radiated noise from panels  What are the main contributors, the important transfer paths ? Treated in ASQ
  • 3. LMS INTERNATIONAL CMC - TPA training - May, 2005 3 Transfer path analysis Principles  Simplify noise/vibration path into source-receiver-transfer system Transfer - structure - sound field Receiver - human ear - steering wheel Source - connection between excitation source and target structure
  • 4. LMS INTERNATIONAL CMC - TPA training - May, 2005 4  Quantification of source-receiver-transfer system Transfer path analysis Principles Transfer - vibro-(acoustic) FRF - Pa/N or (m2/s)/N Receiver - pressure or acceleration - Pa or m2/s Source - force - N
  • 5. LMS INTERNATIONAL CMC - TPA training - May, 2005 5 Transfer path analysis Principles  Structure-borne noise/vibration breakdown and ranking  Preceiver =  Pi  Partial contribution Pi  Pi = Fi . Hi PF Source : N Transfer : Pa/N  Xreceiver =  Xi  Xi = Fi . Hi XF Source : N Transfer : (m/s2)/N : : : :
  • 6. LMS INTERNATIONAL CMC - TPA training - May, 2005 6 Transfer path analysis Two applications  Transfer path ranking, contribution analysis  Preceiver =  FiHi PF  source or transfer problem ?  post processing for FBS, ASQ, FE calculations  Multiple force estimation methods Fi ?
  • 7. LMS INTERNATIONAL CMC - TPA training - May, 2005 7 Transfer path analysis Source identification  Complex dynamic stiffness method  Acceleration measurements  Mount rates  Full matrix inversion  Acceleration measurements  FRF measurements (full matrix)  Driving point inversion  Acceleration measurements  Driving point FRF measurements
  • 8. LMS INTERNATIONAL CMC - TPA training - May, 2005 8 Transfer path analysis Complex dynamic stiffness method t x   s x                 t s X X K F     Acceleration measurements on both sides of mount  Stiffness characteristics of mount
  • 9. LMS INTERNATIONAL CMC - TPA training - May, 2005 9 Transfer path analysis Complex dynamic stiffness determination   determination of stiffness in three direction  rotational degrees of freedom neglected  cross-coupling effects neglected  Automatic integration/differentiation of mount stiffness data  Behavior of mounts is not very linear  apply correct pre-load  temperature effects may be important  adapt excitation according to actual operational conditions        X F K  ) (
  • 10. LMS INTERNATIONAL CMC - TPA training - May, 2005 10 Transfer path analysis Complex dynamic stiffness determination Mount Ground Mass (pre-load) F vert x   hor x  
  • 11. LMS INTERNATIONAL CMC - TPA training - May, 2005 11 Transfer path analysis Inverse method F1 x4 x3 T14 T13 F2 T24 T23     2 24 1 14 2 1 4 2 23 1 13 2 1 3 . . , . . , F T F T F F f x F T F T F F f x       F : excitation X : response T : transfer function                    2 1 24 14 23 13 4 3 F F T T T T x x                     4 3 1 24 14 23 13 2 1 x x T T T T F F
  • 12. LMS INTERNATIONAL CMC - TPA training - May, 2005 12 Transfer path analysis Inverse method : example Operational measurements  acceleration at three points Laboratory measurements  full FRF matrix between excitation at point 1 and response at the other points 1 x   1001 x   1002 x   1 1001 1002 Finput
  • 13. LMS INTERNATIONAL CMC - TPA training - May, 2005 13 1001 1002 F1 oper ? Transfer path analysis Inverse method : example                               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            
  • 14. LMS INTERNATIONAL CMC - TPA training - May, 2005 14 Transfer path analysis Singular value decomposition  Singular value decomposition of transfer function matrix                  n i n i i m i nxn mxn mxm mxn V U V U H 1 * *                    0 0 0 0 0 0 0 2 1 n mxn              M : number of responses N : number of sources M  N
  • 15. LMS INTERNATIONAL CMC - TPA training - May, 2005 15 Transfer path analysis Singular value decomposition  Example : 28x15 accelerance FRF matrix
  • 16. LMS INTERNATIONAL CMC - TPA training - May, 2005 16 Transfer path analysis Singular value decomposition                                    n i m i i n i T mxm nxm nxn mxm mxn T nxn nxm U V U V U V H 1 * 1 1 1 1 1 1   Matrix inversion by singular value decomposition                       0 0 0 0 0 0 0 0 0 0 1 1 2 1 1 1 n nxm          
  • 17. LMS INTERNATIONAL CMC - TPA training - May, 2005 17  Matrix inversion by singular value decomposition Over determination allowed (M  N)  Least squares estimate  Calculation of condition number : upper bound for multiplication coefficient of relative error Transfer path analysis Singular value decomposition n number condition  1 _ 
  • 18. LMS INTERNATIONAL CMC - TPA training - May, 2005 18  Improving the matrix condition  Delete p singular values : condition number drops  Three possibilities : number, relative, absolute  Overdetermination : 2/1 Transfer path analysis Singular value decomposition p n number condition    1 _ n-p > n
  • 19. LMS INTERNATIONAL CMC - TPA training - May, 2005 19 Transfer path analysis Number criterium
  • 20. LMS INTERNATIONAL CMC - TPA training - May, 2005 20 Transfer path analysis Relative criterium
  • 21. LMS INTERNATIONAL CMC - TPA training - May, 2005 21 Transfer path analysis Relation condition number / overdetermination
  • 22. LMS INTERNATIONAL CMC - TPA training - May, 2005 22 Transfer path analysis Selection of overdetermination points  Overdetermination : 2n responses to estimate n forces  Location of OD points  good coherence with signal in transfer path  not to close to transfer path : no extra information  3 extra points in one direction better then 1point measured in 3 directions  Pressure response can be included in matrix inversion
  • 23. LMS INTERNATIONAL CMC - TPA training - May, 2005 23 Transfer path analysis SVD example : fully trimmed car Original FRFs + condition number Elements from inverted matrix
  • 24. LMS INTERNATIONAL CMC - TPA training - May, 2005 24 Transfer path analysis SVD example : body in white Original FRFs + condition number Elements from inverted matrix
  • 25. LMS INTERNATIONAL CMC - TPA training - May, 2005 25 Transfer path analysis Transfer functions  Measured in uncoupled condition  engine, drive-line removed  suspension removed  Follows from substructuring formulation  P=HA+BFi=HB([HA+HB+K-1]-1HAFi)=HBFc HA HB K source target Fc Fi P TPA
  • 26. LMS INTERNATIONAL CMC - TPA training - May, 2005 26 Transfer path analysis Transfer functions  Always check  Linearity  Coherence  Reciprocity  Impact or shaker testing  Coherence with hammer excitation  Misalignment of shaker  Small errors become important after matrix inversion Excitation direction
  • 27. LMS INTERNATIONAL CMC - TPA training - May, 2005 27 Transfer path analysis Vibro-acoustic reciprocity i j j i PF F P Q x H    F1 F2 Pj 1 x   2 x   Qj  Reduction of measurement effort j i Q x unit define ) (
  • 28. LMS INTERNATIONAL CMC - TPA training - May, 2005 28 Transfer path analysis Volume velocity source  Volume velocity sources  Sufficiently excite cavity and/or structure : high power  Not influenced by acoustic boundary  Ease of use : constant calibration factor  Omni-directional
  • 29. LMS INTERNATIONAL CMC - TPA training - May, 2005 29 Transfer path analysis Features : easy model definition  Model definition based on PID and SID annotations mic:1:S body:2 body:1 Data type Primary ID Secondary ID Force body:1:+Z - body:2:+Z - Pressure mic:1:S - FRF mic:1:S body:1:+Z mic:1:S body:2:+Z
  • 30. LMS INTERNATIONAL CMC - TPA training - May, 2005 30 x1 x2 ... xr x11…x21…xr1 PCA Force id. TPA x12…x22…xr2 x1m…x2m…xrm x11…x21…xr1 x12…x22…xr2 x1m…x2m…xrm f11…f21…fn1 f12…f22…fn2 f1m…f2m…fnm phenomenon 1 phenomenon 2 phenomenon m Transfer path analysis Features: support of multi-reference problems  Support of single reference problems : engine noise e.g.  Multi-reference problems (road noise e.g.) require Principal Component Analysis
  • 31. LMS INTERNATIONAL CMC - TPA training - May, 2005 31 Transfer path analysis Features : structure and air-borne problems  Study contribution of structure and air-borne noise in one analysis : Preceiver =  Fi . Hi PF+  Qi’ . Hi’ AA  Pre-processor required for Panel Contribution Analysis
  • 32. LMS INTERNATIONAL CMC - TPA training - May, 2005 32 Transfer path analysis Extensions to TPA  Easy data grouping mechanism in post-processing  grouping based on PID  simplifying visualization  Frequency spectra, ordercuts and autopowers (new) supported  Automatic squaring of FRFs in case of autopowers  Condition calculation : specify frequency range