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IOSR Journal of Mechanical and Civil Engineering (IOSR-JMCE)
e-ISSN: 2278-1684,p-ISSN: 2320-334X, Volume 13, Issue 2 Ver. I (Mar. - Apr. 2016), PP 117-120
www.iosrjournals.org
DOI: 10.9790/1684-130201121124 www.iosrjournals.org 121 | Page
Modal Analysis Of High Speed Milling Spindle By
Experimental Approach
Suhas D. Upase1
, M. C. Swami2
1
(M.E. Machine Design Student of Mechanical Department, M. S. Bidve Engineering College,
Latur,Maharashtra,India.)
2
(Faculty of Mechanical Department, M. S. Bidve Engineering College, Latur, Maharashtra, India.)
Abstract: In this paper we determine the natural frequency of highest speed milling spindle for length
335.4mm and 16000 rpm speed based on modal analysis. This paper taking the high speed milling spimdle of
M.S. bar which is derived and presented by using finite element model in ansys software.This model takes into
account bearing support contact interface , which is established by spring damper element COMBIN 14 for
giving cushioning effect to spindle.Furthermore, the modal analysis has done by means of Ansys commercial
software. After that this result is compaired with experimental result provided by FFT analyzer.The results show
that the natural resonance region speed is far greater than the designed milling spindle.
Keywords: Milling Spindle, Finite Element analysis, FFT analyzer,ANSYS.
I. Introduction
In today’s prosperous industrial development, with the multifarious design of products and reduction of
production cycle, high speed machining technology has been widely adopted by manufacturers [1].The great
development of the science and technology, the high frequency spindles has been taken place of the normal
mechanical spindles more and more, and also be used for the numerical control machine with great effects. The
need of productivity increased so the higher speed machining requirements increases, this led to the
development of new bearings, power electronics and inverter systems. Today, the overwhelming majority of
machine tools are equipped with motorized spindles. Unlike externally driven spindles, the motorized spindles
do not require mechanical transmission elements like gears and couplings [2].
High-speed motorized spindle is an important component of the high-speed machine tools its
performance decides the level of the whole machine tools development to some extent. Especially for high
speed machine tools with high accuracy, the influence of vibration is even more serious. The safety and
reliability due to imperfect dynamic performance have become the primary problem of structural design and
machine operation. Therefore, the dynamic performance research of the high-speed motorized spindle has an
important theoretical and practical significance [3]. As the FEM (finite element method) has become an
essential solution technique in many areas of engineering concerned static and dynamic process, the FEM is
utilized in the design of motorized spindle bearing system [4].
The main aim of this paper is to develop a finite element model of the high speed motorized spindle.
The modal simulation is conducted by using ANSYS commercial software. This result is analyzes and verified
by experimental approach.
II. Modal Analysis By FEA
Milling motorized spindle vibration is inevitable during milling, which not only changes the relative
position of work pieces and milling cutters to influence the machining accuracy, but also accelerates the wears
of milling cutter, further influencing the machining accuracy. Research shows that the processing quality largely
depends on the vibration produced by machine [14]. The influence of vibration is more serious in specially for
high speed machine tools with high accuracy.
First create the spindle model by using FEA with considering following elements.
1) Beam 3 (2D-Elastic) Element description :-BEAM 3 is suitable for analyzing slender to moderately line
2D structures. This element consist of 8 elements (9 nodes) of different c/s area. Shear deformation effects
are also considered.
2) Combin 14 Spring Damper :- Combin 14 element which can be applied to simulate springs and dampers
is provided in ANSYS commerical software[14]. This element has torsional or longitudinal capability in
one, two, or three dimensional applications. The purely rotational element is in torsional spring- damper
option, which gives three degree of freedom at each node i.e roatations about the nodal x, y, and z axes
without considering bending or axial loads.
Modal Analysis Of High Speed Milling Spindle By Experimental Approach
DOI: 10.9790/1684-130201121124 www.iosrjournals.org 122 | Page
Specifications
 Young’s modulus – 2.1e5 N/mm2
 Poisson’s ratio – 0.27
 Density – 7.8 e-6 kg/mm3
 Front bearings diameter - 65 x 100 x 18 (Triplet)
 Rear bearingdiameter - 55 x 90 x 18 (Duplex)
 Total Length of spindle – 335.4 mm
Table .1 Element wise c/s area and moment of inertia of spindle.
Element Sr.
No.
Diameter in mm
do di
Area in mm2
(π/4)*(do
2
-di
2
)
Moment of inertia mm4
(π/64)* (do
2
-di
2
)
Height
In mm
1 65 34.475 2.384*e3 806.9*e3 65
2 65 35 2.356*e3 802.58*e3 65
3 65 35 2.356*e3 802.58*e3 65
4 72 35 3.109*e3 1245.5*e3 72
5 72 35 2.356*e3 802.58*e3 65
6 60 35 1.865*e3 562.5*e3 60
7 55 35 1.413*e3 375.5*e3 55
8 55 35 1.413*e3 375.5*e3 55
By cosidering the table.1. data and given specification of material create the FEA modal (2D).
Specimen preparation
The test specimen geometry is as shown in Fig. 1. One testing specimen is prepared as per
standard specifications with following or given dimensions. Manufacture the spindle using Mild Steel as a
material on lathe machine.
Fig. 1. Schematic representation(drawing) ofM.S. Spindle specimen for production.
Experimentation
The modal analysis test of spindle was performed on FFT Analyzer machine. The detailed results are
shown in fig. 2 , fig. 3 and table. 3.For conducting experiment we use the following instruments.
1] Accelerometer2] Impact hammer
3] DAQ- FFT (Fast Fourier Transform) 4] Industrial PC (with FPM software)
Applications
1] Modal testing 2] Order tracking 3] Spectrum analysis
4] Waveform recording 5] Real time octave analysis 6] Sound quality
Fig. 2.shows the real manufactured specimen as per specification of given drawing. After that this
specimen kept on FFT machine to free vibration analysis or modal analysis. Free modal analysis result gives on
monitor in the form of Waveform i.e frequency v/s db (decibel). From that table consider only frequencies.
Modal Analysis Of High Speed Milling Spindle By Experimental Approach
DOI: 10.9790/1684-130201121124 www.iosrjournals.org 123 | Page
Fig. 2. Testing spindle specimen as per drawing
Fig. 3. Modal Analysis results on FFT Analyzer
III. Results
The manufactured specimen as per drawing Kept on FFT analyzer machine and after conducting
experiment we got the modal analysis results which are recorded in fig.3 . and Table.3 .
The table.3.shows the different frequencies in which at one frequency the given specimen resonates.In the
range 67 Hz to 401 Hz.From fig.3.select a node from the graph, where it gives peak vibration those are listed in
table 3.
The fig.4 . shows the modal analysis result by FEA which gives different sets of frequencies for
given specifications.
Now compair or match the both results it is seen that frequencies 422 Hz by FEA and 401 Hz by
experimental are nearer so that it is observed that 422 Hz frequency is the resonate limit or its natural
frequency.
Fig. 4 . Modal analysis result of given specification spindle by FEA
Details of Set of frequencies given by FEAmethod tabulated in the below table.
Table. 2. List of Frequencies by FEA from modal analysis result
SET 1 2 3 4 5 6 7 8 9 10
FREQY
70.80 77.81 93.926 99.82 251.39 255.97 422.37 568.90 699.31 879.10
Modal Analysis Of High Speed Milling Spindle By Experimental Approach
DOI: 10.9790/1684-130201121124 www.iosrjournals.org 124 | Page
Table.3 . Experimental Modal analysis result fore by FFTAnalyzer.
IV. Conclusions
It is observed that by seeing the both results we determine the natural frequency at which it starts to
vibrate at maximum peak level. So based on above results final conclusions are as follows.
1. The modal analysis shows that no resonance occurs in predicted results & it is verified with experimental
results.
2. The modal analysis result compare with experimental result then we got nearer422 Hz natural frequency
so at this frequency its critical rotating speed is 25320 rpm, which is away from the 16000 rpm of designed
spindle.
References
[1] Z.C. Lin, and J.S. Chang, “The building of spindle thermaldisplacement model of high speed machine center”, Int. J.
Adv.Manuf. Technol., vol. 34, pp. 556-566, Sept. 2007
[2] E. Abele, Y. Altintas, and C. Brecher, “Machine tool spindleunits”, CIRP Annals – Manuf. Technol., vol. 59, pp. 781-
802, 2010.
[3] C. Li, Y. Ding, and B. Lu, “Development and Key Technology inHigh Speed Cutting”, J. Qingdao Technol. Univ., vol. 30, pp. 7-
16,Feb. 2009.
[4] W. Li, H. Pu, Q. Liu, G. Chen, and S. Zhang, “ANSYS-Baseddynamic analysis of high-
speed motorized spindle”, Int. Conf.Comput. Eng. Technol., 2009, pp. 336-340
[5] J. K. Choi, and D. G. Lee, “Characteristics of a spindle bearingsystem with a gear located on the bearing span”. Int. J. Mech. T
ool.Manuf. Pergamon, vol. 37, pp. 171-173, Aug. 1997.
[6] J. K. Choi, and D. G. Lee, “Thermal characteristics of the spindlebearing system with a gear located on the bearing span”, I
nt. J.Mech. Tool. Manufact. Pergamon, vol. 38, pp. 1017-1030, Sept.1998.
[7] J.-S. Chen, and Y.-W. Hwang, “Centrifugal force induceddynamics of a motorized high-
speed spindle”, Int. J. Adv. Manuf.Technol., vol. 30, pp. 10-19, Aug. 2006.
[8] A. G. Rehorn, “Spindle Dynamics: Identification, Modeling andEffects”, M. S. thesis, University of Western Ontario, Ont
ario,Canada, 2001
[9] E. V. Bordatchev, and R. Henriksen, “State space modeling ofmachine tool spindle units using subspace identificat
ion”,Proceedings of the 2nd IASTED International Conference onControl and Application, 1999, pp. 120-123.
[10] E. V. Bordatchev, “Modeling and parameter identification of theimpulse response matrix of mechanical systems”, Proceeding
s of SPIE - The International Society for Optical Engineering, 1998, pp.106-117.
[11] A. G. Rehorn, J. Jiang, P. E. Orban, and E. Bordatchev, “Modelling and experimental investigation of spindle and cutter dynam
ics for a high-precision machining center”, Int. J. Adv. Manuf.Technol., vol. 24, pp. 806-815, Dec. 2004.
[12] W. Xie, “The FEM Analysis of Dynamic and Static Characteristicof High Speed Motorized Spindle”, M. S. thesis, Harbin Institut
e of Technology, Harbin, PRC, 2001.
[13] R. A. Burton, and H. E. Staph, “Thermally Activated Seizure ofAngular Contact Bearings”. A.S.L.E.Transactions, vol. 10, pp
. 408-417, Oct. 1967
[14] Deping Liu, Hang Zhangny Su, Tao& Yufeny Su, “ Finite element analysis of high speed motorized spindle based on Ansys”, The
open mechanical engineering journal 2011,volume 5,1-10.
[15] Joaquim de Ciurana, Guillem Quintanaand Francisco Javier Campa, “Machinetoolsforhighperformancemachining”,Machine
tool spindles, 2009,75-127, DOI:10.1007/978-1-84800- 380-4_3.
[16] Dr.Sinan Badrawy, “Dynamic modellingand analysis of motorized milling spindlesforoptimizing thespindle cutting
erformance”,Engineering Manager Moore Nanotechnology Systems, LLC
[17] Osamu Maeda, Yuzhong Cao, YusufAltintas, “Expert spindle design system”International Journal of Machine Tools &Man
ufacture 45 (2005) Pages537–548.
Sr. No. Frequency (HZ) Db(decibel)
1 32 -0.939
2 61 -11.59
3 138 -30.74
4 172 -26.94
5 401 -12.14

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T130201121124

  • 1. IOSR Journal of Mechanical and Civil Engineering (IOSR-JMCE) e-ISSN: 2278-1684,p-ISSN: 2320-334X, Volume 13, Issue 2 Ver. I (Mar. - Apr. 2016), PP 117-120 www.iosrjournals.org DOI: 10.9790/1684-130201121124 www.iosrjournals.org 121 | Page Modal Analysis Of High Speed Milling Spindle By Experimental Approach Suhas D. Upase1 , M. C. Swami2 1 (M.E. Machine Design Student of Mechanical Department, M. S. Bidve Engineering College, Latur,Maharashtra,India.) 2 (Faculty of Mechanical Department, M. S. Bidve Engineering College, Latur, Maharashtra, India.) Abstract: In this paper we determine the natural frequency of highest speed milling spindle for length 335.4mm and 16000 rpm speed based on modal analysis. This paper taking the high speed milling spimdle of M.S. bar which is derived and presented by using finite element model in ansys software.This model takes into account bearing support contact interface , which is established by spring damper element COMBIN 14 for giving cushioning effect to spindle.Furthermore, the modal analysis has done by means of Ansys commercial software. After that this result is compaired with experimental result provided by FFT analyzer.The results show that the natural resonance region speed is far greater than the designed milling spindle. Keywords: Milling Spindle, Finite Element analysis, FFT analyzer,ANSYS. I. Introduction In today’s prosperous industrial development, with the multifarious design of products and reduction of production cycle, high speed machining technology has been widely adopted by manufacturers [1].The great development of the science and technology, the high frequency spindles has been taken place of the normal mechanical spindles more and more, and also be used for the numerical control machine with great effects. The need of productivity increased so the higher speed machining requirements increases, this led to the development of new bearings, power electronics and inverter systems. Today, the overwhelming majority of machine tools are equipped with motorized spindles. Unlike externally driven spindles, the motorized spindles do not require mechanical transmission elements like gears and couplings [2]. High-speed motorized spindle is an important component of the high-speed machine tools its performance decides the level of the whole machine tools development to some extent. Especially for high speed machine tools with high accuracy, the influence of vibration is even more serious. The safety and reliability due to imperfect dynamic performance have become the primary problem of structural design and machine operation. Therefore, the dynamic performance research of the high-speed motorized spindle has an important theoretical and practical significance [3]. As the FEM (finite element method) has become an essential solution technique in many areas of engineering concerned static and dynamic process, the FEM is utilized in the design of motorized spindle bearing system [4]. The main aim of this paper is to develop a finite element model of the high speed motorized spindle. The modal simulation is conducted by using ANSYS commercial software. This result is analyzes and verified by experimental approach. II. Modal Analysis By FEA Milling motorized spindle vibration is inevitable during milling, which not only changes the relative position of work pieces and milling cutters to influence the machining accuracy, but also accelerates the wears of milling cutter, further influencing the machining accuracy. Research shows that the processing quality largely depends on the vibration produced by machine [14]. The influence of vibration is more serious in specially for high speed machine tools with high accuracy. First create the spindle model by using FEA with considering following elements. 1) Beam 3 (2D-Elastic) Element description :-BEAM 3 is suitable for analyzing slender to moderately line 2D structures. This element consist of 8 elements (9 nodes) of different c/s area. Shear deformation effects are also considered. 2) Combin 14 Spring Damper :- Combin 14 element which can be applied to simulate springs and dampers is provided in ANSYS commerical software[14]. This element has torsional or longitudinal capability in one, two, or three dimensional applications. The purely rotational element is in torsional spring- damper option, which gives three degree of freedom at each node i.e roatations about the nodal x, y, and z axes without considering bending or axial loads.
  • 2. Modal Analysis Of High Speed Milling Spindle By Experimental Approach DOI: 10.9790/1684-130201121124 www.iosrjournals.org 122 | Page Specifications  Young’s modulus – 2.1e5 N/mm2  Poisson’s ratio – 0.27  Density – 7.8 e-6 kg/mm3  Front bearings diameter - 65 x 100 x 18 (Triplet)  Rear bearingdiameter - 55 x 90 x 18 (Duplex)  Total Length of spindle – 335.4 mm Table .1 Element wise c/s area and moment of inertia of spindle. Element Sr. No. Diameter in mm do di Area in mm2 (π/4)*(do 2 -di 2 ) Moment of inertia mm4 (π/64)* (do 2 -di 2 ) Height In mm 1 65 34.475 2.384*e3 806.9*e3 65 2 65 35 2.356*e3 802.58*e3 65 3 65 35 2.356*e3 802.58*e3 65 4 72 35 3.109*e3 1245.5*e3 72 5 72 35 2.356*e3 802.58*e3 65 6 60 35 1.865*e3 562.5*e3 60 7 55 35 1.413*e3 375.5*e3 55 8 55 35 1.413*e3 375.5*e3 55 By cosidering the table.1. data and given specification of material create the FEA modal (2D). Specimen preparation The test specimen geometry is as shown in Fig. 1. One testing specimen is prepared as per standard specifications with following or given dimensions. Manufacture the spindle using Mild Steel as a material on lathe machine. Fig. 1. Schematic representation(drawing) ofM.S. Spindle specimen for production. Experimentation The modal analysis test of spindle was performed on FFT Analyzer machine. The detailed results are shown in fig. 2 , fig. 3 and table. 3.For conducting experiment we use the following instruments. 1] Accelerometer2] Impact hammer 3] DAQ- FFT (Fast Fourier Transform) 4] Industrial PC (with FPM software) Applications 1] Modal testing 2] Order tracking 3] Spectrum analysis 4] Waveform recording 5] Real time octave analysis 6] Sound quality Fig. 2.shows the real manufactured specimen as per specification of given drawing. After that this specimen kept on FFT machine to free vibration analysis or modal analysis. Free modal analysis result gives on monitor in the form of Waveform i.e frequency v/s db (decibel). From that table consider only frequencies.
  • 3. Modal Analysis Of High Speed Milling Spindle By Experimental Approach DOI: 10.9790/1684-130201121124 www.iosrjournals.org 123 | Page Fig. 2. Testing spindle specimen as per drawing Fig. 3. Modal Analysis results on FFT Analyzer III. Results The manufactured specimen as per drawing Kept on FFT analyzer machine and after conducting experiment we got the modal analysis results which are recorded in fig.3 . and Table.3 . The table.3.shows the different frequencies in which at one frequency the given specimen resonates.In the range 67 Hz to 401 Hz.From fig.3.select a node from the graph, where it gives peak vibration those are listed in table 3. The fig.4 . shows the modal analysis result by FEA which gives different sets of frequencies for given specifications. Now compair or match the both results it is seen that frequencies 422 Hz by FEA and 401 Hz by experimental are nearer so that it is observed that 422 Hz frequency is the resonate limit or its natural frequency. Fig. 4 . Modal analysis result of given specification spindle by FEA Details of Set of frequencies given by FEAmethod tabulated in the below table. Table. 2. List of Frequencies by FEA from modal analysis result SET 1 2 3 4 5 6 7 8 9 10 FREQY 70.80 77.81 93.926 99.82 251.39 255.97 422.37 568.90 699.31 879.10
  • 4. Modal Analysis Of High Speed Milling Spindle By Experimental Approach DOI: 10.9790/1684-130201121124 www.iosrjournals.org 124 | Page Table.3 . Experimental Modal analysis result fore by FFTAnalyzer. IV. Conclusions It is observed that by seeing the both results we determine the natural frequency at which it starts to vibrate at maximum peak level. So based on above results final conclusions are as follows. 1. The modal analysis shows that no resonance occurs in predicted results & it is verified with experimental results. 2. The modal analysis result compare with experimental result then we got nearer422 Hz natural frequency so at this frequency its critical rotating speed is 25320 rpm, which is away from the 16000 rpm of designed spindle. References [1] Z.C. Lin, and J.S. Chang, “The building of spindle thermaldisplacement model of high speed machine center”, Int. J. Adv.Manuf. Technol., vol. 34, pp. 556-566, Sept. 2007 [2] E. Abele, Y. Altintas, and C. Brecher, “Machine tool spindleunits”, CIRP Annals – Manuf. Technol., vol. 59, pp. 781- 802, 2010. [3] C. Li, Y. Ding, and B. Lu, “Development and Key Technology inHigh Speed Cutting”, J. Qingdao Technol. Univ., vol. 30, pp. 7- 16,Feb. 2009. [4] W. Li, H. Pu, Q. Liu, G. Chen, and S. Zhang, “ANSYS-Baseddynamic analysis of high- speed motorized spindle”, Int. Conf.Comput. Eng. Technol., 2009, pp. 336-340 [5] J. K. Choi, and D. G. Lee, “Characteristics of a spindle bearingsystem with a gear located on the bearing span”. Int. J. Mech. T ool.Manuf. Pergamon, vol. 37, pp. 171-173, Aug. 1997. [6] J. K. Choi, and D. G. Lee, “Thermal characteristics of the spindlebearing system with a gear located on the bearing span”, I nt. J.Mech. Tool. Manufact. Pergamon, vol. 38, pp. 1017-1030, Sept.1998. [7] J.-S. Chen, and Y.-W. Hwang, “Centrifugal force induceddynamics of a motorized high- speed spindle”, Int. J. Adv. Manuf.Technol., vol. 30, pp. 10-19, Aug. 2006. [8] A. G. Rehorn, “Spindle Dynamics: Identification, Modeling andEffects”, M. S. thesis, University of Western Ontario, Ont ario,Canada, 2001 [9] E. V. Bordatchev, and R. Henriksen, “State space modeling ofmachine tool spindle units using subspace identificat ion”,Proceedings of the 2nd IASTED International Conference onControl and Application, 1999, pp. 120-123. [10] E. V. Bordatchev, “Modeling and parameter identification of theimpulse response matrix of mechanical systems”, Proceeding s of SPIE - The International Society for Optical Engineering, 1998, pp.106-117. [11] A. G. Rehorn, J. Jiang, P. E. Orban, and E. Bordatchev, “Modelling and experimental investigation of spindle and cutter dynam ics for a high-precision machining center”, Int. J. Adv. Manuf.Technol., vol. 24, pp. 806-815, Dec. 2004. [12] W. Xie, “The FEM Analysis of Dynamic and Static Characteristicof High Speed Motorized Spindle”, M. S. thesis, Harbin Institut e of Technology, Harbin, PRC, 2001. [13] R. A. Burton, and H. E. Staph, “Thermally Activated Seizure ofAngular Contact Bearings”. A.S.L.E.Transactions, vol. 10, pp . 408-417, Oct. 1967 [14] Deping Liu, Hang Zhangny Su, Tao& Yufeny Su, “ Finite element analysis of high speed motorized spindle based on Ansys”, The open mechanical engineering journal 2011,volume 5,1-10. [15] Joaquim de Ciurana, Guillem Quintanaand Francisco Javier Campa, “Machinetoolsforhighperformancemachining”,Machine tool spindles, 2009,75-127, DOI:10.1007/978-1-84800- 380-4_3. [16] Dr.Sinan Badrawy, “Dynamic modellingand analysis of motorized milling spindlesforoptimizing thespindle cutting erformance”,Engineering Manager Moore Nanotechnology Systems, LLC [17] Osamu Maeda, Yuzhong Cao, YusufAltintas, “Expert spindle design system”International Journal of Machine Tools &Man ufacture 45 (2005) Pages537–548. Sr. No. Frequency (HZ) Db(decibel) 1 32 -0.939 2 61 -11.59 3 138 -30.74 4 172 -26.94 5 401 -12.14