time nvh analysis – chassis example
DESCRIPTION
This is an example of a virtual dynamic test. A chassis of a car was modeled and a vertical impulse loading was applied at one of front corner points. Time histories were obtained at select chassis locations and they were translated to frequency domain by applying Fast Fourier Transform (FFT) to extract mode shapes and frequencies for 12 sampling points.TRANSCRIPT
Chapter 14: Time NVH Analysis – Chassis Example
14 Time NVH Analysis – Chassis Example
Summary 231
Introduction 232
Requested Solutions 232
Model Details Time NVH scheme 232
FEM Solution 233
Results 235
Modeling Tips 237
Input File(s) 238
231CHAPTER 14
Time NVH Analysis – Chassis Example
SummaryTitle Chapter 14: Time NVH Analysis – Chassis Example
Features A potentially nonlinear periodic transient dynamic response of a chassis sub-frame analysis is followed by a fast Fourier transform to extract the modes and frequencies that characterize the dynamic solution which is compared to traditional linear modal analysis.
Geometry
Material properties , ,
Analysis type TIMNVH analysis (SOL 700)
Boundary conditions Free
Applied loads Vertical impulse load applied at point
Element type 4-node shell element
FE results Transient response, FFT, mode shapes and frequencies
L4
W1 W2
L1 L2 L3
W1= 993W2= 1,182L1= 1,518L2= 865L3= 927L4= 361Size of rectangular hollow beam: 53x111 to 53x191 depending on locations.Thickness of shell: 3.5
Units: mm
A F
G L
E 2.10x105N mm2= 0.3= 7.89x10 9– ton mm
3=
A
A
CB
HD
EF
G
I J
KL
1.00E-06
1.00E-05
1.00E-04
1.00E-03
1.00E-02
1.00E-01
0.00E+00 2.00E+01 4.00E+01 6.00E+01 8.00E+01 1.00E+02 1.20E+02 1.40E+02 1.60E+02
Am
plit
ude
Frequency (Hz)
901581
901641
901697
901865
902061
902097
902580
902595
902609
902797
902996
903063
MD Demonstration Problems
CHAPTER 14232
IntroductionThis is an example of a virtual dynamic test. A chassis of a car was modeled and a vertical impulse loading was applied at one of front corner points. Time histories were obtained at select chassis locations and they were translated to frequency domain by applying Fast Fourier Transform (FFT) to extract mode shapes and frequencies for 12 sampling points.
Requested SolutionsAcceleration time histories are obtained at 12 points and they are translated to a frequency domain. Dynamic properties such as modal natural frequencies and mode shapes are then computed. The results are then compared with those of Nastran SOL 103 for validation purposes.
Model Details Time NVH scheme
Figure 14-1 Flow Chart of TIMNVH Scheme
MD Nastran bdf Model (impulse loading)
Obtain Time-history Results - Displacement - Velocity - Acceleration (default)
Time domain results -> Frequency domain results
Extract dynamic properties: Natural frequencies and Mode shapes (f06 and modes.out files)
SOL 700
FFT
Find and compare peaks
Add PARAM, S700NVH1, TIMNAT and TIMSML cards
Re-run MD Nastran SOL 700
Use primary time history or FFT results
No
Final dynamic properties Is acceptable? Yes
233CHAPTER 14
Time NVH Analysis – Chassis Example
FEM SolutionThere are two models. The first model is the initial run to determine the rough dynamic properties of the structure and second model is a re-run of the first job to find the accurate and final results using the previous time history results.
Applied Load and Selected Location for Time HistoryTo compute the dynamic responses of the chassis, a vertical impulse load is applied at the front corner as shown in Figure 14-2. Using FORCE and TABLED entries as shown below, a maximum of 0.01 tons impulse point loading is applied to node 902517.
FORCE 3 902517 0 .01 0. 0. -1.TABLED1 1 -10. 0. 0. 0. .001 1. .002 0. 10. 0. ENDT
The acceleration time histories at 12 points on the chassis are computed (see Figure 14-2) to obtain the modal responses.
Figure 14-2 Applied Impulse Loading and Nodes Selected for Getting the Acceleration Responses
Primary JobThe end time in transient run is defined by using 100 time steps at 0.4e-4 sec. for each increment. The end time is the product of these two entries. Notice here, the time increment is only for the first step. The actual number of time increments and the exact value of the time steps are determined by MD Nastran solver during the analysis. The time step is a function of the smallest element dimension during the simulation.
TSTEPNL 1 100 .01 1 ADAPT 2 10
TIMNVH defines the Time NVH analysis as explained below.
TIMNVH, 1, , , 1.0, 1000., 3, 0.0005, 2,++, 0, 3, 1, 0.015, 0, 3, 13, .0030,+
0 2 4 6 8 100.000
0.005
0.010
Time (ms)
Load (ton)
A
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The range of natural frequencies to obtain is from 1.0 Hz to 1000 Hz and translational degrees of freedom for z-direction is only considered (3). The sampling rate is 0.0005 seconds. The peaking criterion is two, which means that a peak is selected if the amplitude of the number of increasing and decreasing points around a peak is equal or greater than 2.
Acceleration is selected for the response (0) and translational eigenvectors are only requested as ASCII format (3). Eigenvalues are normalized by 1.0 (1) and 0.015 is selected as CLOSE value which means if there are two modes which distance is smaller than 0.015 Hz, it is assumed to be the same mode. ACII file format of natural frequencies and eigenvalues are asked (0) and translational time histories of z-direction are requested (3). Frequency-amplitude data of z-direction are requested (13) and a peak whose amplitude is less than 0.0030 times the maximum amplitude is ignored (.0030)
+, 901581, 901641, 901697, 901865, 902061, 902097, , ,++, 902580, 902595, 902609, 902797, 902996, 903063
The grid points 901581, 901641, 901697, 901865, 902061, 902097, 902580, 902595, 902609, 902797, 902996 and 903063 are selected to obtain time history responses for Time NVH analysis.
TIMNVH,1, , , 1.0, 1000., 3,.0005, 2,++, 0, 3, 1, 0.015, 0, 3, 13, .0030,++, 901581, 901641, 901697, 901865, 902061, 902097, , ,++, 902580, 902595, 902609, 902797, 902996, 903063
Re-running JobTo find the accurate modal properties, a re-run is required using the previous time history data. Only three entries are different from the initial job;
PARAM, S700NVH, TIMNVH and TIMNAT
The value of PARAM, S700NVH is assigned to 1 for using the previous time history binary data (binout0000). In TIMNVH entry, the PEAK option (in the first line) is changed from 2 to –2, which will require defining the TIMNAT entry.
TIMNAT is used to specify the natural frequencies selected from amplitude-frequency plot from the initial run. The natural frequencies close to 35, 43, 49, 101, and 108 Hz’s are obtained as the natural frequencies.
PARAM,S700NVH1,1TIMNVH,1, , , 1.0, 1000., 3,.0005, -2,++, 0, 3, 1, 0.015, 0, 3, 13, .0030,++, 901581, 901641, 901697, 901865, 902061, 902097, , ,++, 902580, 902595, 902609, 902797, 902996, 903063 TIMNAT,1,35.,43.,49.,101.,108.
235CHAPTER 14
Time NVH Analysis – Chassis Example
ResultsThere are three result files from Time Domain NVH analysis.
• mode.out: Results for the natural frequencies and eigenvalues.
• ampl-freq- 00901865-3.txt: amplitude-frequency output of degree of freedom =3 at grid point 901865.
• time-hist- 00901865-3.txt: time history output of degree of freedom =3 at grid point 901865.
From the ampl-freq-*** files, the frequency-amplitude plots are shown in Figure 14-3. Using the plot, the modal frequencies are specified in TIMNAT option to refine the dynamic property results.
Figure 14-3 Frequency-Amplitude Plots At 12 Nodes
1.00E-06
1.00E-05
1.00E-04
1.00E-03
1.00E-02
1.00E-01
0.00E+00 2.00E+01 4.00E+01 6.00E+01 8.00E+01 1.00E+02 1.20E+02 1.40E+02 1.60E+02
Am
plit
ude
Frequency (Hz)
901581
901641
901697
901865
902061
902097
902580
902595
902609
902797
902996
903063
A
CB
HD
EF
G
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KL
1 2
3
4 5
6 7
MD Demonstration Problems
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Figure 14-4 Comparison of Mode Shapes and Frequencies for SOL 103 and SOL 700
The small peaks for modes 4 and 5 are barely observable in Figure 14-3 and arise because of the selection of the type of impulse loading. These lateral modes exhibit a low participation when the impulse loading is vertical. For a certain set of impulse loads, certain modes may not be excited and the FFT only picks up the excited modes that significantly participate in the transient response.
Mode SOL103 SOL 700 Diff(%) Comparison
1 36.0170 35.0002 2.82% Vertical motion dominant
2 43.9523 43.0002 2.17% Vertical motion dominant
3 52.5065 49.0003 6.68% Lateral motion dominant
4 67.4281 Small peak - Lateral motion dominant
5 84.7220 Small peak - Lateral motion dominant
6 101.9688 101.0005 0.95% Vertical motion dominant
7 111.0159 108.0005 2.72% Vertical motion dominant
36.01735.000
43.95243.000
52.50649.000
67.428 -
84.722 -
111.016108.001
101.969 101.001
SOL 103 Frequency HzSOL 700 Frequency Hz
1 2 3
4
Mode #
5 6
7
237CHAPTER 14
Time NVH Analysis – Chassis Example
Results show that even though the vertical mode shapes of modes 2 and 3 are similar, their amplitude and lateral modes are quite different. The results are compared in Figure 14-5.
Figure 14-5 Comparison of Vertical Mode Shapes Between Mode 2 and 3
Sample OutputThe final response from the FFT steps for the 12 sampling points are contained in a file called modes.out which contains the eigenvalues (frequencies) and eigenvectors (mode shapes) in the form:
Modeling TipsTo get more accurate data, options of TIMNVH and TSTEPNL entry could be changed. For example, increasing the end time (defined as 1 second in this analysis) can result in higher resolution (the frequency increment in the frequency-amplitude plot). The resolution is determined as:
Vertical mode shape of mode 2 Vertical mode shape of mode 3
MODES 1 5EI GV 1 3. 500018E+01 901581- 3. 32998498E- 02- 2. 49243337E- 04 7. 08997618E- 01 901641- 4. 29914555E- 02 7. 70991520E- 05- 1. 08571907E- 01 901697- 4. 15069142E- 02 2. 55256359E- 04- 6. 31611930E- 01 901865 4. 37855265E- 02- 1. 51550001E- 04- 4. 18557096E- 01 902061 7. 97601410E- 02 4. 34427876E- 04 5. 67705213E- 01 902097 8. 68013598E- 02 8. 02417982E- 03 1. 00000000E+00 902580- 3. 38588683E- 02 2. 97715028E- 04 7. 28400224E- 01 902595- 4. 37831381E- 02 2. 30181446E- 04- 9. 77437006E- 02 902609- 4. 24521220E- 02- 1. 61168521E- 04- 6. 35288211E- 01 902797 4. 11242103E- 02- 3. 00773060E- 04- 4. 29582120E- 01 902996 7. 69986448E- 02 7. 40153667E- 04 5. 51699503E- 01 903063 8. 41026922E- 02- 3. 47784987E- 03 9. 82653769E- 01
} Frequency
x-component y-component
eigenvector
z-component
SampleGrid IDS
1 mode { st
1sample end time - sample start time
------------------------------------------------------------------------------------------ 11 sec 0 sec–
------------------------------------- 1 Hz= =
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CHAPTER 14238
To increase the maximum frequency in the frequency-amplitude plots, the sampling rate which is defined as 0.015 seconds in this example decreases. The maximum frequency of this example is computed as:
Input File(s)
File Description
nug_14a.dat Initial run to find rough dynamic properties
nug_14b.dat Re-run to compute accurate dynamic properties
nug_14c.dat SOL 103 model
112--- sampling rate ------------------------------------------ 1
12--- 0.015 sec -------------------------------- 133.33 Hz= =