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Frequency Response Analysis

Frequency Response Analysis

This analysis uses the data of tutorial/17_freq_beam.

Analysis target

The analysis target is a cantilevered beam, and the geometry is shown in Figure 4.17.1 and the mesh data is shown in Figure 4.17.2.

Item Description Notes Reference
Type of analysis Frequency response analysis !SOLUTION,TYPE=EIGEN !SOLUTION,TYPE=DYNAMIC
Number of nodes 55
Number of elements 126
Element type Four node tetrahedral element !ELEMENT,TYPE=341
Material name Material-1 !MATERIAL,NAME=Material-1
Boundary conditions Restraint, Concentrated force, eigen value !EIGENREAD
Matrix solution CG/SSOR !SOLVER,METHOD=CG,PRECOND=1

Shape of the cantilever

Fig. 4.17.1 : Shape of the cantilever

Mesh data of the cantilever

Fig. 4.17.2 : Mesh data of the cantilever

Analysis content

The end of a cantilevered beam to be analyzed is fully constrained, and a frequency response analysis is performed by applying concentrated loads to two nodes at the opposite end.

After analyzing eigenvalues up to the 10th order under the same boundary conditions, the analysis is performed using eigenvalues and eigenvectors up to the 5th order. The analysis control data for frequency response analysis is shown below.

Analysis control data beam_eigen.cnt.

#  Control File for FISTR
!VERSION
 3
!WRITE,RESULT
!WRITE,VISUAL
!SOLUTION, TYPE=EIGEN
!EIGEN
 10, 1.0E-8, 60
!BOUNDARY
_PickedSet4, 1, 3, 0.0
!SOLVER,METHOD=CG,PRECOND=1,ITERLOG=NO,TIMELOG=YES
 10000, 1
 1.0e-8, 1.0, 0.0
!VISUAL,metod=PSR
!surface_num=1
!surface 1
!output_type=VTK
!END

Analysis control data beam_freq.cnt.

#  Control File for FISTR
!VERSION
 3
!WRITE,RESULT
!WRITE,VISUAL
!SOLUTION, TYPE=DYNAMIC
!DYNAMIC
 11 , 2
 14000, 16000, 20, 15000.0
 0.0, 6.6e-5
 1, 1, 0.0, 7.2E-7
 10, 2, 1
 1, 1, 1, 1, 1, 1
!EIGENREAD
 eigen_0.log
 1, 5
!BOUNDARY
_PickedSet4, 1, 3, 0.0
!FLOAD, LOAD CASE=2
_PickedSet5, 2, 1.
!FLOAD, LOAD CASE=2
_PickedSet6, 2, 1.
!SOLVER,METHOD=CG,PRECOND=1,ITERLOG=NO,TIMELOG=YES
 10000, 1
 1.0e-8, 1.0, 0.0
!VISUAL,metod=PSR
!surface_num=1
!surface 1
!output_type=VTK
!END

Analysis procedure

First, change hecmw_ctrl_eigen.dat to hecmw_ctrl.dat for eigenvalue analysis, and then run eigenvalue analysis.

Next, change hecmw_ctrl_freq.dat to hecmw_ctrl.dat and 0.log to eigen_0.log (which is specified in the control data for frequency response analysis), and then perform the frequency response analysis.

$ cp hecmw_ctrl_eigen.dat hecmw_ctrl.dat
$ fistr1 -t 4
$ mv 0.log eigen_0.log
$ cp hecmw_ctrl_freq.dat hecmw_ctrl.dat
$ fistr1 -t 4

Analysis results

The relationship between the frequency and displacement amplitude of a monitoring node (node number 1) specified in the analysis control data is shown in Figure 4.17.3, created using Microsoft Excel. A part of the analysis result log file is shown below as numerical data for the analysis results.

Relationship between frequency and displacement amplitude of the monitoring nodes

Fig.4.17.3 Relationship between frequency and displacement amplitude of the monitoring nodes

Log file 0.log

 fstr_setup: OK
 Rayleigh alpha:   0.0000000000000000     
 Rayleigh beta:   7.1999999999999999E-007
 read from=eigen_0.log
 start mode=           1
 end mode=           5
 start frequency:   14000.000000000000     
 end frequency:   16000.000000000000     
 number of the sampling points          20
 monitor nodeid=           1
   14100.000000000000      [Hz] :    8.3935554529723885E-002
   14100.000000000000      [Hz] :            1 .res
   14200.000000000000      [Hz] :    9.1211083509607632E-002
   14200.000000000000      [Hz] :            2 .res
   14300.000000000000      [Hz] :    9.9579777896922961E-002
   14300.000000000000      [Hz] :            3 .res
   14400.000000000000      [Hz] :   0.10914967594967491     
   14400.000000000000      [Hz] :            4 .res
   14500.000000000000      [Hz] :   0.11992223203326918     
   14500.000000000000      [Hz] :            5 .res
   14600.000000000000      [Hz] :   0.13164981801806747     
   14600.000000000000      [Hz] :            6 .res
   14700.000000000000      [Hz] :   0.14360931008440975     
   14700.000000000000      [Hz] :            7 .res
   14800.000000000000      [Hz] :   0.15436500205940235     
   14800.000000000000      [Hz] :            8 .res
   14900.000000000000      [Hz] :   0.16180768408076251     
   14900.000000000000      [Hz] :            9 .res
   15000.000000000000      [Hz] :   0.16388019610373711     
   15000.000000000000      [Hz] :           10 .res
   15100.000000000000      [Hz] :   0.15982110598747551     
   15100.000000000000      [Hz] :           11 .res
   15200.000000000000      [Hz] :   0.15074650286398145     
   15200.000000000000      [Hz] :           12 .res
   15300.000000000000      [Hz] :   0.13885370598993371     
   15300.000000000000      [Hz] :           13 .res
   15400.000000000000      [Hz] :   0.12618976409021948     
   15400.000000000000      [Hz] :           14 .res
   15500.000000000000      [Hz] :   0.11405716994112736     
   15500.000000000000      [Hz] :           15 .res
   15600.000000000000      [Hz] :   0.10306231010139058     
   15600.000000000000      [Hz] :           16 .res
   15700.000000000000      [Hz] :    9.3374567545990342E-002
   15700.000000000000      [Hz] :           17 .res
   15800.000000000000      [Hz] :    8.4945897112663621E-002
   15800.000000000000      [Hz] :           18 .res
   15900.000000000000      [Hz] :    7.7641947016103510E-002
   15900.000000000000      [Hz] :           19 .res
   16000.000000000000      [Hz] :    7.1307642422355627E-002
   16000.000000000000      [Hz] :           20 .res
 start time:   0.0000000000000000     
 end time:   6.6000000000000005E-005
 frequency:   15000.000000000000     
 node id:           1
 num disp:          10
 time=   0.0000000000000000       :            1 .res
 time=   0.0000000000000000       :            1 .vis
 time=   6.6000000000000003E-006  :            2 .res
 time=   6.6000000000000003E-006  :            2 .vis
 time=   1.3200000000000001E-005  :            3 .res
 time=   1.3200000000000001E-005  :            3 .vis
 time=   1.9800000000000000E-005  :            4 .res
 time=   1.9800000000000000E-005  :            4 .vis
 time=   2.6400000000000001E-005  :            5 .res
 time=   2.6400000000000001E-005  :            5 .vis
 time=   3.3000000000000003E-005  :            6 .res
 time=   3.3000000000000003E-005  :            6 .vis
 time=   3.9600000000000000E-005  :            7 .res
 time=   3.9600000000000000E-005  :            7 .vis
 time=   4.6200000000000005E-005  :            8 .res
 time=   4.6200000000000005E-005  :            8 .vis
 time=   5.2800000000000003E-005  :            9 .res
 time=   5.2800000000000003E-005  :            9 .vis
 time=   5.9400000000000000E-005  :           10 .res
 time=   5.9400000000000000E-005  :           10 .vis