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IOSR Journal of Mechanical and Civil Engineering (IOSR-JMCE)
e-ISSN: 2278-1684,p-ISSN: 2320-334X, Volume 13, Issue 1 Ver. III (Jan. - Feb. 2016), PP 12-19
www.iosrjournals.org
DOI: 10.9790/1684-13131219 www.iosrjournals.org 12 | Page
Design And Analysis Of High Speed Milling Spindle For Minimum
Deflection
Suhas D. Upase
1
, M. C. Swami
2
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.)
3
(Faculty of Mechanical Department, G. N. D. Engineering College, Bidar, Karnataka, India.)
Abstract: In this paper high speed milling spindle design of 16000rpm with minimum static deflection has
been determined by varying bearing stiffness, span length between bearings and front bearing inner diameter. In
present work intially we design different diameter spindles like 55, 60, 65 and differnet bearing stiffness of
respective diamenter by keeping 150
contact angle . Further we evaluate the deflection of the spindle nose, static
analysis and optimum bearing span length by theoretical analysis and compaire with ANSYS results. The result
shows that the span length and bearing siffness has significant effect on spindle deflection.
Keywords: High speed spindle, Static deflection, Bearing stiffness,Ansys software .
I. Introduction
The main mechanical component in machining centers is spindle. The spindle rotates at high speed with
holding different cutter, to machines a material assembled to machine tool table. Finishing quality of workpiece
and productivity directely affected by static and dynamic stffness of the spindle. The bearing arrangement is
important factor for spindle design. In machine tools spindles are rotating drive shafts that act as axes for cutting
tools or to hold cutting instruments.High speed spindles have important component of any type of high machining
process whether in CNC, tool machining centers and oyher process components. Motorized spindle have been
developed to achive high speed rotation, which equipped with bulit in motor as a part of spindle for eliminating the
power transmission devices like gears, belts.
Fig. 1 High frequency milling spindle arrangements [7]
II. Static Stiffness Analysis.
2.1. Introduction
Static stiffness is one of the important performances of machine tools. Hence it must be correctly defined
and related parameters of spindle must be properly determined. Since power loss will be there in terms of
mechanical effciency, but as compared to conventional belt drive system where around 20-30%, here it has been
reduced to 10-15%.
Design And Analysis Of High Speed Milling Spindle For Minimum Deflection
DOI: 10.9790/1684-13131219 www.iosrjournals.org 13 | Page
Hence the available power at the spindle is assumed to be around 8.5 to 9 KW. Stiffness of the spindle is
defined as its ability to resist deflection under the action of cutting force.[11]
As shown in fig. 2 when a force exerted on the spindle nose is P, the displacement at the spindle nose in the same
direction as that of P is ‘δ’ and correlation stiffness is defined as K = P/δ
Using carbide cutting tool, cutting speed to cut thestainless steel material is 120 m/min.[9]
The cutting force P can be calculated from the unit powerconcept referring to the following equations:[7]
P = 6120 Nm/ V kgf ---------(Eqn.-1)
where, Nm=power of the motor at the spindle=9 KW=9x103
W
V =cutting speed =120 m/min=2 m/sec
Therefore,
P=6120*9/120 =459 kgf
P= 4502.8 N
III. High Speed Millingspindle
3.1. Features of milling high speed spindle to be designed
The spindle rotates at 16000 rpm with power rating 9 KW. Spindle is mounted on ball bearing of150
angular contact. In analysis the stiffness of outer diameter of spindle is near about inner diameter of bearing.
3.2 Rigidity analysis by analytical (Determination of spindle deflection)
Unit deflection of the spindle due to its own bending under the cutting force and also deflection caused
due to elasticity of bearing.
Fig. 2 Deflection of the spindle nose
The deflection of the spindle nose 'δ' for an unloaded spindle due to load P is given by [5]
δ = δ1 + δ2
------- (Eqn. 2)
Where, δ1= Deflection due to radial yielding of the bearings in mm
δ2 = Deflection due to elastic bending of the spindle in mm
a = Length of overhang in mm
L = Bearing span in mm
E = Young's modulus of Spindle material in N/mm2
P = Cutting force in N
SA = Stiffness of the front bearing N/mm
SB = Stiffness of the rear bearing in N/mm
IL = Second moment of area of the shaft at the span in mm4
Ia = Second moment of area of the shaft at the overhang in mm4
3.3 Arrangements of Bearing
Two different bearing arrangements ‘A’ and ‘B’ are considered for the design. Angular contact ball
bearings with 15° contact angle are used with medium preloading. The bearing arrangement ‘A’, with duplex
bearing set at the front, in which a pair of angular contact ball bearings are arranged in back-to-back and the duplex
bearing set at the rear mounted in back-to-back fashion. The bearing arrangement ‘B’, with triplet bearing set at the
front, in which one pair of angular contact ball bearings are arranged in tandem with respect to each other and
back-to-back with respect to a single angular contact ball bearing and the duplex bearing set at the rear mounted in
back-to-back fashion. The triplet bearing and duplex bearing sets are shown in fig. 3.
Design And Analysis Of High Speed Milling Spindle For Minimum Deflection
DOI: 10.9790/1684-13131219 www.iosrjournals.org 14 | Page
Fig. 3 bearing arrangements (a) Triplet bearing, (b) Duplex bearing [8]
The stiffness can be calculated for 150
contact angle [2], for medium preloading and for 55, 60, 65
mm diameters bearings. From the FAG Spindle Bearing catalogue: [6]
For Triplet arrangement, Stiffness K = 1.36*6*Ca
For Duplex arrangement, Stiffness K = 6*Ca
Where Ca = stiffness value of the bearing in N/m
1) For dia. 60 mm front triplet bearing , axial rigidity (axial stiffness value) for medium preloading condition
is Ca =71.6 N/m. [8]
K= 1.36*6*71.6= 582.64 N/m.
2) For dia. 55 mm front duplex bearing , axial rigidity (axial stiffness value) for medium preloading condition is
Ca =67.2 N/m. [8]
K= 6*67.2= 403.2 N/m
Specifications, size, & stiffness of different bearings is given and calculated by FAG Spindle Bearings is
shown in the table
Table: 1Specifications, size, & stiffness of different bearings[8]
Sl.
No
Details
Type and
Specification
Size
Details
Stiffness
(N/µm)
Load
rating
dynamic
C (kN)
Load
rating
static
Co
(kN)
Attainable
Speed in
(r/min)
1A
Front
bearing
HSS 7011
CT P4S
Duplex
d=55mm
D=90mm
B=18mm
403.2 1860 1900 20000
2A
Front
bearing
HSS 7012
CT P4S
Duplex
d=60mm
D=95mm
B=18mm
428.4 1930 2000 19000
3A
Front
bearing
HSS 7013
CT P4S
Duplex
d=65mm
D=100mm
B=18mm
453.0 2000 2160 17000
1B
Front
bearing
HSS 7011
CT P4S
Triplet
d=55mm
D=90mm
B=18mm
548.3 1860 1900 20000
2B
Front
bearing
HSS 7012
CT P4S
Triplet
d=60mm
D=95mm
B=18mm
582.64 1930 2000 19000
3B
Front
bearing
HSS 7013
CT P4S
Triplet
d=65mm
D=100mm
B=18mm
616.08 2000 2160 17000
4R
Rear
bearing
HSS 7011
CT P4S
Duplex
d=55mm
D=90mm
B=18mm
403.2 1860 1900 20000
3.4 Optimum Bearing Span Length
The front bearing set should be positioned to minimize the overhang of the spindle nose. It is required to
optimize the bearing spacing 'L0' for maximum spindle stiffness. This requires examination of relative
combinations to deflection, which arise from both bearing deflections and spindle bearing. By using bearings with
a smaller cross section, larger spindle diameters can be used without changing the housing bore diameter or slightly
increasing the housing bore diameter. This increases the bending rigidity of spindle and leads to increase in overall
rigidity. Initially optimum bearing span is calculated using eq. 3for each configuration. Fig.4.shows the influence
of spread on spindle deflection at point of load. Details of different bearing arrangements and calculated optimum
bearing span length (L0) are listed in table .
Equation to calculate Optimum Bearing Span Length is [11]
---------- (Eqn. 3)
Where,
L0 = Static optimum Bearing Span Length in mm
Design And Analysis Of High Speed Milling Spindle For Minimum Deflection
DOI: 10.9790/1684-13131219 www.iosrjournals.org 15 | Page
Q =Trial value for iterative determination of L0 = 4a
Fig. 4Influence of spread on spindle deflection at point of load
3.5. Calculation to find Optimum Bearing Span Length:
E = Young’s modulus = 2.1x105
N/mm2
SA= Stiffness of front bearing = 403.2x103
N/mm ( for dia. 55mm)
SB = Stiffness of rear bearing = 403.2x103
N/mm ( for dia. 55mm )
Ia = Second moment of area = it is calculated and found to be 379.84x103
mm4
IL = Second moment of area of the shaft at the span in mm4
= it is calculated and found to be 562.5x103
N/mm
a = Length of overhang = 65 mm
Q = Trial value for iterative determination of L0 = 4xa = 4x65 = 260
For First trial value take Q =260mm, therefore
L1 = 202.12mm
For second trial value take Q =202.12mm, therefore
L2= 193.10mm
For third trial value take Q =193.10mm, therefore
L3 = 191.62mm
For fourth trial value take Q =191.62mm, therefore
L4 = 191.37mm=L0
Table: 2 Details of different bearing arrangements with optimum bearing span length (L0).
Sl.
N
o
Front bearings Bearing
Stiffnes
s N/µm
Rear
bearin
gs
Beari
ng
Stiffn
ess
N/µm
Attainabl
e speed in
rpm
Optimum
bearing
span
length ‘L0’
mm
‘A
’
Ø55 x 90 x 18
Duplex
403.2
Ø55 x
90 x 18
Duplex
403.2
20000 193.33
Ø60 x 95 x 18
Duplex
428.4 19000 205.52
Ø65 x 100 x18
Duplex
453.0 17000 222.39
‘B
’
Ø55 x 90 x 18
Triplet
548.3
Ø55 x
90 x 18
Duplex
403.2
20000 175.53
Ø60 x 95 x 18
Triplet
582.64 19000 186.49
Ø65 x 100 x18
Triplet
616.08 17000 199.85
Analylitical analysis has been carried to evaluate stiffness of the spindle and to optimize the design to
have maximum spindle nose deflection. Varying the span length from 140 mm to 230 mm. This span length
variation becomes important to accommodate the integral motor rotor. By considering overhang of the spindle
is around 65 mm from front bearing center and spindle nose size BT-40 taper also the flange. Front
bearingdiameter is varied from 55 to 65 mm to evaluate its role in imparting the stiffness to the spindle system.
Design And Analysis Of High Speed Milling Spindle For Minimum Deflection
DOI: 10.9790/1684-13131219 www.iosrjournals.org 16 | Page
3.5. Calculation of spindle deflection
------------(Eqn. 2)
Where,
a = Length of overhang in mm = 65 mm
L = Bearing span in mm = 140 mm
E = Young's modulus of Spindle material in N/mm2
= 2.1x105
N/mm2
P = Cutting force in N =4502.8 N
SA = Stiffness of the front bearing N/mm = 403.2x103
N/mm (for dia. 55mm)
SB = Stiffness of the rear bearing in N/mm = 403.2x103
N/mm (for dia. 55mm)
IL = Second moment of area of the shaft at the span in mm4
= it is calculated and found to be 562.5x103
mm4
=  x (604
– 354
)/64 = 562.5x103
mm4
Ia = Second moment of area of the shaft at the overhang in mm4
Consider BT-40 Taper. Front taper side is 44.45mm and rear taper is 24.5mm.
Average Diameter at the mid of BT-40 Taper is = (44.45+24.5) / 2 = 34.475mm
Ia = Second moment of area = it is calculated for 55, 60 and 65mm and found to be
=  x (554
– 34.4754
)/64 = 379.84x103
mm4
=  x (604
– 34.4754
)/64 = 566.83x103
mm4
=  x (654
– 34.4754
)/64 = 806.9x103
mm4
eq. 3.3 For bearing A type and front & rear dia. is 55mm then deflection is found to be
δ = 39.07x10-3
mm.
Variations of deflection and stiffness values for bearing arrangements ‘A’ and ‘B’ are given in following table.
Table: 3 Variations ofDeflections and Stiffness for bearing arrangements ‘A’ & ‘B’ .
Optimum deflection and stiffness values for bearing arrangements ‘A’ and ‘B’ are given in the table 4.
Table: 4 Optimum Deflections and Stiffness for bearing arrangements ‘A’, ‘B’.
Front bearing dia
mm
A B
Span length
mm
Δ
µm
K
N/ µm
Span
length
Mm
Δ
µm
K
N/ µm
55 210 36.69 122.7 190 31.47 142.9
60 200 33.84 133.06 190 28.9 155.8
65 200 31.80 141.6 180 27.08 166.2
The diameter of the spindle between the bearings has more influence on the rigidity as is evident from
the table3. This diameter could be varied to the extent of a maximum of 65 mm from the practical
considerations. To accommodate the integral motor rotor, the span length is taken as 200 mm [Table 2]. At the
65 mm diameter & 200mm span length, the stiffness of the arrangement ‘B’has a value of around 166.2 N/µm
and the deflection of the spindle nose based on static analysis is around 27.08 micron. From the point of view
of static analysis, bearing arrangement type ‘B’ is chosen as an optimum design.
Sr. No. Front
bearing
dia.mm
Span
Length
Mm
Bearing arrangement ‘A’ Bearing arrangement ‘B’
Deflection δ
µm
Stiffness K
N/µm
Deflection δ
µm
Stiffness K
N/µm
1 55 140 to 230 39.07 to 36.81 115.2 to 122.3 32.70 to 31.91 137.5 to 141.1
2 60 140 to 230 35.93 to 34.00 125.3 to 132.4 29.97 to 29.43 150.2 to 155.0
3 65 140 to 230 33.67 to 32.03 133.7 to 140.5 27.99 to 27.70 160.8 to 162.5
Design And Analysis Of High Speed Milling Spindle For Minimum Deflection
DOI: 10.9790/1684-13131219 www.iosrjournals.org 17 | Page
Fig. 5 Deflection at the nose for bearing arrangements (front bearing dia 55mm)
Fig. 6 Deflection at the nose for bearing arrangements (front bearing dia 60mm)
Fig. 7 Deflection at the nose for bearing arrangements (front bearing dia 65mm)
Fig. 5 to 7 shows the effect of bearing elasticity and spindle deflection on the overall rigidity.Variation of
deflection and the stiffness when the bearing span is changed from 140 to 230 mm is not significant. This gives the
designer flexibility in sizing the span to accommodate the integral induction motor [11]. As there is not much
difference in the spindle stiffness in 180mm, 190mm, 200mm span length, to accommodate the integral motor
200mm span length will be considered
IV. Static Stiffness Analysis By Fem
4.1 Element Description: Beam Elements
There are several element types used for FE analysis such as solid, plane and beam elements. For the
spindle analysis for the bearing spans optimization, beam elements are the most suitable because the shapes of the
spindle and the cutting tool are roughly cylindrical. Besides a time consuming iteration method will be used for the
optimization, so the calculation time for the dynamic properties in each iteration step must be as short as possible.
In order to shorten the calculation time, the simplest elements (the beam elements ) are the most suitable type.[11]
Design And Analysis Of High Speed Milling Spindle For Minimum Deflection
DOI: 10.9790/1684-13131219 www.iosrjournals.org 18 | Page
4.2 Static Stiffness Analysis
The geometric model is created in ANSYS. The finite element model is built using BEAM3 and COMBIN14
element[11].
4.2.1 Material properties
For the static analysis of the spindle, the following propertiesare used:[11]
 Modulus of elasticity =210 GPa
Poisson’sratio =0.27
 Density =7.8×10
-6
kg/mm
3
4.2.2 Boundary Conditions
The spindle is modeled using BEAM3 and COMBIN14 elements. A tangential force of4502.8 N is
applied at the spindle nose as shown in fig. 8.
Fig.8 FEM showing Boundary Condition[11]
Table: 5 Comparison of Theoretical & FEA values for deflection and stiffness at the spindle nose whenspan
length= 200 mm with‘B’ type bearing arrangement.[11]
4.3 Static Results
The deflection at the spindle nose in Y direction is computed for various configurations and results are
obtained for different diameters of spindle at the front bearing with ‘B’ type arrangement and span length of
200 mm as shown in fig. 9.
Fig.9Deflection at the spindle nose (front bearing Ø65mm, span length =200 mm)
Span length
Mm
THEORETICAL ANSYS
Deflection at
spindle nose
µm
Stiffness
N/µm
Deflection at
spindle nose
µm
Stiffness
N/µm
170 27.14 165.9 23.72 189.8
180 27.08 166.2 23.94 188.0
190 27.07 166.3 24.24 185.7
200 27.14 165.9 24.60 183.0
Design And Analysis Of High Speed Milling Spindle For Minimum Deflection
DOI: 10.9790/1684-13131219 www.iosrjournals.org 19 | Page
Table:6Comparison of Theoretical & FEA values for deflection and stiffness at the spindle nose when the s
pan length various from
170 mm to 200 mm for the front bearing with diameter of 65 mm with ‘B’ type Bearing arrangement [11]
The deflection at the spindle nose in Y direction and the stiffness vlaues obtained through theoretical
calculations and ANSYS are given in the table.5 and 6. The diamenter could be varied to the extent of a maximum
of 65 mm from the practical considerations. The stiffness obtained by ANSYS of the optimized spindle with given
configuration is around 183.0 N/ µm at the span length of 200 mm.
In this we consider Triplet bearing set arrangement ‘B’for the front end of the spindle, in which one pair of
angular contact ball bearings are arranged in tandem with respect to each other and back-to-back with respect to a
single angular contact ball bearing. Tandem bearing pair will carry both radial and axial loads equally shared. [11]
4.4 Analysis of Results
The deflection of the spindle nose in Y direction is function of bearing stiffness, span length and diameter
of the spindle bearing for a given overhang. The deflection of the spindle nose in Y direction affects the machining
accuracy.[11]
V. Conclusions
 Span length between bearing is varied from 140 to 230 mm which gives flexibility in sizing the span to
accommodate the integral induction motor.
 From results it is clear that Rigidity of the spindle is depends on the diameter of the spindle between the
bearing. So from practical considerations of bearing speed, the diameter of the spindle varied from 55 to 65 mm
maximum and result shows that 65mm diameter spindle for the arrangement ‘B’ has getting a stiffness value
165.9 N/µm and 27.14 mm is the deflection of the spindle nose based on static analysis for above arrangement.
Therefore bearing arrangement type ‘B’ is chosen as an optimum design from static analysis results.
 The effect of front bearing stiffness is on overall stiffness, hence locate higher siffness bearings at the front.
 Rigidity analysis was carried out by using ANSYS and the result gives good correlation between theoretical
calculation and ANSYS result.
References.
[1]. ANSYS Basic Analysis Procedures Guide, 002184, Aug2005, www.ansys.com.Book of Spindles, www.dynospindles.com.
[2]. CMTI Hand Book, Machine Tool Design Hand Book Tata McGraw-Hill Company Limited, 1983,421-588
[3]. Daniel P. Soroka, Hardinge Inc. One Hardinge Dr.Elmira,NY 14902 Hard Turning and the Machine Tool.
[4]. dsoroka@hardinge.com
[5]. Dr.Sinan Badrawy, Dynamic Modeling and Analysis ofMotorized Milling Spindles, Moore Nanotechnology Systems,LLC, 2003.
[6]. FAG Spindle Bearings Catalogue, AC 41 130/7 EA ·March 2008, www.fag.com.
[7]. HMT, Production Technology, Tata McGraw HillPublication, 1980, 7
th
Print, page 186-198.
[8]. INA-FAG BEARINX
®
-online Spindle Calculation-SCHAEFFLER GROUP Industrial.
[9]. Lipka I, Harkany, Determination of the optimum bearingdistance of cantilever shafts with two supports, Mach. Tool.
Research Transactions, 45 (1964) 65-80.
[10]. Machine Manual, VMC 1000, The Mysore Kirloskercompany, Harihar.
[11]. Anandkumar Telang, Static stiffness analysis of high frequency milling spindle, eISSN:2319-1163/ pISSN:2321-7308
[12]. Modal analysis using ANSYS,www.mece.ualberta.ca/tutorials/ansys.
[13]. Momir Sarenac, Stiffness of Machine Tool Spindle as amainfactor for treatment accuracy-UDC 62-113,624.046,Mechanical
Engineering Vol.1, No 6, 1999, pp. 665 – 674. Spindle Basics, 2008, www.spindlesworld.com.
[14]. Technical Specifications for IBAG-Motor Spindles,IBAG Switzerland AG, 1999, www.ibag.ch.
[15]. TIMKEN, Machine Tool Spindle, 1M-07-02 No. 5911,www.timken.com.
[16]. Yung C. Shin, Analysis of bearing configuration effectson high speed spindles, International Journal of Machine
Tools & Manufacture, 44 (2004) 347–364.83, 421-588.
Diameter at
Front bearing
Mm
THEORETICAL ANSYS
Deflection at
spindle nose
µm
Stiffness
N/µm
Deflection at
spindle nose
µm
Stiffness
N/µm
55 31.50 142.8 25.07 179.6
60 28.96 155.4 24.19 186.1
65 27.14 165.9 24.60 183.0

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B013131219

  • 1. IOSR Journal of Mechanical and Civil Engineering (IOSR-JMCE) e-ISSN: 2278-1684,p-ISSN: 2320-334X, Volume 13, Issue 1 Ver. III (Jan. - Feb. 2016), PP 12-19 www.iosrjournals.org DOI: 10.9790/1684-13131219 www.iosrjournals.org 12 | Page Design And Analysis Of High Speed Milling Spindle For Minimum Deflection Suhas D. Upase 1 , M. C. Swami 2 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.) 3 (Faculty of Mechanical Department, G. N. D. Engineering College, Bidar, Karnataka, India.) Abstract: In this paper high speed milling spindle design of 16000rpm with minimum static deflection has been determined by varying bearing stiffness, span length between bearings and front bearing inner diameter. In present work intially we design different diameter spindles like 55, 60, 65 and differnet bearing stiffness of respective diamenter by keeping 150 contact angle . Further we evaluate the deflection of the spindle nose, static analysis and optimum bearing span length by theoretical analysis and compaire with ANSYS results. The result shows that the span length and bearing siffness has significant effect on spindle deflection. Keywords: High speed spindle, Static deflection, Bearing stiffness,Ansys software . I. Introduction The main mechanical component in machining centers is spindle. The spindle rotates at high speed with holding different cutter, to machines a material assembled to machine tool table. Finishing quality of workpiece and productivity directely affected by static and dynamic stffness of the spindle. The bearing arrangement is important factor for spindle design. In machine tools spindles are rotating drive shafts that act as axes for cutting tools or to hold cutting instruments.High speed spindles have important component of any type of high machining process whether in CNC, tool machining centers and oyher process components. Motorized spindle have been developed to achive high speed rotation, which equipped with bulit in motor as a part of spindle for eliminating the power transmission devices like gears, belts. Fig. 1 High frequency milling spindle arrangements [7] II. Static Stiffness Analysis. 2.1. Introduction Static stiffness is one of the important performances of machine tools. Hence it must be correctly defined and related parameters of spindle must be properly determined. Since power loss will be there in terms of mechanical effciency, but as compared to conventional belt drive system where around 20-30%, here it has been reduced to 10-15%.
  • 2. Design And Analysis Of High Speed Milling Spindle For Minimum Deflection DOI: 10.9790/1684-13131219 www.iosrjournals.org 13 | Page Hence the available power at the spindle is assumed to be around 8.5 to 9 KW. Stiffness of the spindle is defined as its ability to resist deflection under the action of cutting force.[11] As shown in fig. 2 when a force exerted on the spindle nose is P, the displacement at the spindle nose in the same direction as that of P is ‘δ’ and correlation stiffness is defined as K = P/δ Using carbide cutting tool, cutting speed to cut thestainless steel material is 120 m/min.[9] The cutting force P can be calculated from the unit powerconcept referring to the following equations:[7] P = 6120 Nm/ V kgf ---------(Eqn.-1) where, Nm=power of the motor at the spindle=9 KW=9x103 W V =cutting speed =120 m/min=2 m/sec Therefore, P=6120*9/120 =459 kgf P= 4502.8 N III. High Speed Millingspindle 3.1. Features of milling high speed spindle to be designed The spindle rotates at 16000 rpm with power rating 9 KW. Spindle is mounted on ball bearing of150 angular contact. In analysis the stiffness of outer diameter of spindle is near about inner diameter of bearing. 3.2 Rigidity analysis by analytical (Determination of spindle deflection) Unit deflection of the spindle due to its own bending under the cutting force and also deflection caused due to elasticity of bearing. Fig. 2 Deflection of the spindle nose The deflection of the spindle nose 'δ' for an unloaded spindle due to load P is given by [5] δ = δ1 + δ2 ------- (Eqn. 2) Where, δ1= Deflection due to radial yielding of the bearings in mm δ2 = Deflection due to elastic bending of the spindle in mm a = Length of overhang in mm L = Bearing span in mm E = Young's modulus of Spindle material in N/mm2 P = Cutting force in N SA = Stiffness of the front bearing N/mm SB = Stiffness of the rear bearing in N/mm IL = Second moment of area of the shaft at the span in mm4 Ia = Second moment of area of the shaft at the overhang in mm4 3.3 Arrangements of Bearing Two different bearing arrangements ‘A’ and ‘B’ are considered for the design. Angular contact ball bearings with 15° contact angle are used with medium preloading. The bearing arrangement ‘A’, with duplex bearing set at the front, in which a pair of angular contact ball bearings are arranged in back-to-back and the duplex bearing set at the rear mounted in back-to-back fashion. The bearing arrangement ‘B’, with triplet bearing set at the front, in which one pair of angular contact ball bearings are arranged in tandem with respect to each other and back-to-back with respect to a single angular contact ball bearing and the duplex bearing set at the rear mounted in back-to-back fashion. The triplet bearing and duplex bearing sets are shown in fig. 3.
  • 3. Design And Analysis Of High Speed Milling Spindle For Minimum Deflection DOI: 10.9790/1684-13131219 www.iosrjournals.org 14 | Page Fig. 3 bearing arrangements (a) Triplet bearing, (b) Duplex bearing [8] The stiffness can be calculated for 150 contact angle [2], for medium preloading and for 55, 60, 65 mm diameters bearings. From the FAG Spindle Bearing catalogue: [6] For Triplet arrangement, Stiffness K = 1.36*6*Ca For Duplex arrangement, Stiffness K = 6*Ca Where Ca = stiffness value of the bearing in N/m 1) For dia. 60 mm front triplet bearing , axial rigidity (axial stiffness value) for medium preloading condition is Ca =71.6 N/m. [8] K= 1.36*6*71.6= 582.64 N/m. 2) For dia. 55 mm front duplex bearing , axial rigidity (axial stiffness value) for medium preloading condition is Ca =67.2 N/m. [8] K= 6*67.2= 403.2 N/m Specifications, size, & stiffness of different bearings is given and calculated by FAG Spindle Bearings is shown in the table Table: 1Specifications, size, & stiffness of different bearings[8] Sl. No Details Type and Specification Size Details Stiffness (N/µm) Load rating dynamic C (kN) Load rating static Co (kN) Attainable Speed in (r/min) 1A Front bearing HSS 7011 CT P4S Duplex d=55mm D=90mm B=18mm 403.2 1860 1900 20000 2A Front bearing HSS 7012 CT P4S Duplex d=60mm D=95mm B=18mm 428.4 1930 2000 19000 3A Front bearing HSS 7013 CT P4S Duplex d=65mm D=100mm B=18mm 453.0 2000 2160 17000 1B Front bearing HSS 7011 CT P4S Triplet d=55mm D=90mm B=18mm 548.3 1860 1900 20000 2B Front bearing HSS 7012 CT P4S Triplet d=60mm D=95mm B=18mm 582.64 1930 2000 19000 3B Front bearing HSS 7013 CT P4S Triplet d=65mm D=100mm B=18mm 616.08 2000 2160 17000 4R Rear bearing HSS 7011 CT P4S Duplex d=55mm D=90mm B=18mm 403.2 1860 1900 20000 3.4 Optimum Bearing Span Length The front bearing set should be positioned to minimize the overhang of the spindle nose. It is required to optimize the bearing spacing 'L0' for maximum spindle stiffness. This requires examination of relative combinations to deflection, which arise from both bearing deflections and spindle bearing. By using bearings with a smaller cross section, larger spindle diameters can be used without changing the housing bore diameter or slightly increasing the housing bore diameter. This increases the bending rigidity of spindle and leads to increase in overall rigidity. Initially optimum bearing span is calculated using eq. 3for each configuration. Fig.4.shows the influence of spread on spindle deflection at point of load. Details of different bearing arrangements and calculated optimum bearing span length (L0) are listed in table . Equation to calculate Optimum Bearing Span Length is [11] ---------- (Eqn. 3) Where, L0 = Static optimum Bearing Span Length in mm
  • 4. Design And Analysis Of High Speed Milling Spindle For Minimum Deflection DOI: 10.9790/1684-13131219 www.iosrjournals.org 15 | Page Q =Trial value for iterative determination of L0 = 4a Fig. 4Influence of spread on spindle deflection at point of load 3.5. Calculation to find Optimum Bearing Span Length: E = Young’s modulus = 2.1x105 N/mm2 SA= Stiffness of front bearing = 403.2x103 N/mm ( for dia. 55mm) SB = Stiffness of rear bearing = 403.2x103 N/mm ( for dia. 55mm ) Ia = Second moment of area = it is calculated and found to be 379.84x103 mm4 IL = Second moment of area of the shaft at the span in mm4 = it is calculated and found to be 562.5x103 N/mm a = Length of overhang = 65 mm Q = Trial value for iterative determination of L0 = 4xa = 4x65 = 260 For First trial value take Q =260mm, therefore L1 = 202.12mm For second trial value take Q =202.12mm, therefore L2= 193.10mm For third trial value take Q =193.10mm, therefore L3 = 191.62mm For fourth trial value take Q =191.62mm, therefore L4 = 191.37mm=L0 Table: 2 Details of different bearing arrangements with optimum bearing span length (L0). Sl. N o Front bearings Bearing Stiffnes s N/µm Rear bearin gs Beari ng Stiffn ess N/µm Attainabl e speed in rpm Optimum bearing span length ‘L0’ mm ‘A ’ Ø55 x 90 x 18 Duplex 403.2 Ø55 x 90 x 18 Duplex 403.2 20000 193.33 Ø60 x 95 x 18 Duplex 428.4 19000 205.52 Ø65 x 100 x18 Duplex 453.0 17000 222.39 ‘B ’ Ø55 x 90 x 18 Triplet 548.3 Ø55 x 90 x 18 Duplex 403.2 20000 175.53 Ø60 x 95 x 18 Triplet 582.64 19000 186.49 Ø65 x 100 x18 Triplet 616.08 17000 199.85 Analylitical analysis has been carried to evaluate stiffness of the spindle and to optimize the design to have maximum spindle nose deflection. Varying the span length from 140 mm to 230 mm. This span length variation becomes important to accommodate the integral motor rotor. By considering overhang of the spindle is around 65 mm from front bearing center and spindle nose size BT-40 taper also the flange. Front bearingdiameter is varied from 55 to 65 mm to evaluate its role in imparting the stiffness to the spindle system.
  • 5. Design And Analysis Of High Speed Milling Spindle For Minimum Deflection DOI: 10.9790/1684-13131219 www.iosrjournals.org 16 | Page 3.5. Calculation of spindle deflection ------------(Eqn. 2) Where, a = Length of overhang in mm = 65 mm L = Bearing span in mm = 140 mm E = Young's modulus of Spindle material in N/mm2 = 2.1x105 N/mm2 P = Cutting force in N =4502.8 N SA = Stiffness of the front bearing N/mm = 403.2x103 N/mm (for dia. 55mm) SB = Stiffness of the rear bearing in N/mm = 403.2x103 N/mm (for dia. 55mm) IL = Second moment of area of the shaft at the span in mm4 = it is calculated and found to be 562.5x103 mm4 =  x (604 – 354 )/64 = 562.5x103 mm4 Ia = Second moment of area of the shaft at the overhang in mm4 Consider BT-40 Taper. Front taper side is 44.45mm and rear taper is 24.5mm. Average Diameter at the mid of BT-40 Taper is = (44.45+24.5) / 2 = 34.475mm Ia = Second moment of area = it is calculated for 55, 60 and 65mm and found to be =  x (554 – 34.4754 )/64 = 379.84x103 mm4 =  x (604 – 34.4754 )/64 = 566.83x103 mm4 =  x (654 – 34.4754 )/64 = 806.9x103 mm4 eq. 3.3 For bearing A type and front & rear dia. is 55mm then deflection is found to be δ = 39.07x10-3 mm. Variations of deflection and stiffness values for bearing arrangements ‘A’ and ‘B’ are given in following table. Table: 3 Variations ofDeflections and Stiffness for bearing arrangements ‘A’ & ‘B’ . Optimum deflection and stiffness values for bearing arrangements ‘A’ and ‘B’ are given in the table 4. Table: 4 Optimum Deflections and Stiffness for bearing arrangements ‘A’, ‘B’. Front bearing dia mm A B Span length mm Δ µm K N/ µm Span length Mm Δ µm K N/ µm 55 210 36.69 122.7 190 31.47 142.9 60 200 33.84 133.06 190 28.9 155.8 65 200 31.80 141.6 180 27.08 166.2 The diameter of the spindle between the bearings has more influence on the rigidity as is evident from the table3. This diameter could be varied to the extent of a maximum of 65 mm from the practical considerations. To accommodate the integral motor rotor, the span length is taken as 200 mm [Table 2]. At the 65 mm diameter & 200mm span length, the stiffness of the arrangement ‘B’has a value of around 166.2 N/µm and the deflection of the spindle nose based on static analysis is around 27.08 micron. From the point of view of static analysis, bearing arrangement type ‘B’ is chosen as an optimum design. Sr. No. Front bearing dia.mm Span Length Mm Bearing arrangement ‘A’ Bearing arrangement ‘B’ Deflection δ µm Stiffness K N/µm Deflection δ µm Stiffness K N/µm 1 55 140 to 230 39.07 to 36.81 115.2 to 122.3 32.70 to 31.91 137.5 to 141.1 2 60 140 to 230 35.93 to 34.00 125.3 to 132.4 29.97 to 29.43 150.2 to 155.0 3 65 140 to 230 33.67 to 32.03 133.7 to 140.5 27.99 to 27.70 160.8 to 162.5
  • 6. Design And Analysis Of High Speed Milling Spindle For Minimum Deflection DOI: 10.9790/1684-13131219 www.iosrjournals.org 17 | Page Fig. 5 Deflection at the nose for bearing arrangements (front bearing dia 55mm) Fig. 6 Deflection at the nose for bearing arrangements (front bearing dia 60mm) Fig. 7 Deflection at the nose for bearing arrangements (front bearing dia 65mm) Fig. 5 to 7 shows the effect of bearing elasticity and spindle deflection on the overall rigidity.Variation of deflection and the stiffness when the bearing span is changed from 140 to 230 mm is not significant. This gives the designer flexibility in sizing the span to accommodate the integral induction motor [11]. As there is not much difference in the spindle stiffness in 180mm, 190mm, 200mm span length, to accommodate the integral motor 200mm span length will be considered IV. Static Stiffness Analysis By Fem 4.1 Element Description: Beam Elements There are several element types used for FE analysis such as solid, plane and beam elements. For the spindle analysis for the bearing spans optimization, beam elements are the most suitable because the shapes of the spindle and the cutting tool are roughly cylindrical. Besides a time consuming iteration method will be used for the optimization, so the calculation time for the dynamic properties in each iteration step must be as short as possible. In order to shorten the calculation time, the simplest elements (the beam elements ) are the most suitable type.[11]
  • 7. Design And Analysis Of High Speed Milling Spindle For Minimum Deflection DOI: 10.9790/1684-13131219 www.iosrjournals.org 18 | Page 4.2 Static Stiffness Analysis The geometric model is created in ANSYS. The finite element model is built using BEAM3 and COMBIN14 element[11]. 4.2.1 Material properties For the static analysis of the spindle, the following propertiesare used:[11]  Modulus of elasticity =210 GPa Poisson’sratio =0.27  Density =7.8×10 -6 kg/mm 3 4.2.2 Boundary Conditions The spindle is modeled using BEAM3 and COMBIN14 elements. A tangential force of4502.8 N is applied at the spindle nose as shown in fig. 8. Fig.8 FEM showing Boundary Condition[11] Table: 5 Comparison of Theoretical & FEA values for deflection and stiffness at the spindle nose whenspan length= 200 mm with‘B’ type bearing arrangement.[11] 4.3 Static Results The deflection at the spindle nose in Y direction is computed for various configurations and results are obtained for different diameters of spindle at the front bearing with ‘B’ type arrangement and span length of 200 mm as shown in fig. 9. Fig.9Deflection at the spindle nose (front bearing Ø65mm, span length =200 mm) Span length Mm THEORETICAL ANSYS Deflection at spindle nose µm Stiffness N/µm Deflection at spindle nose µm Stiffness N/µm 170 27.14 165.9 23.72 189.8 180 27.08 166.2 23.94 188.0 190 27.07 166.3 24.24 185.7 200 27.14 165.9 24.60 183.0
  • 8. Design And Analysis Of High Speed Milling Spindle For Minimum Deflection DOI: 10.9790/1684-13131219 www.iosrjournals.org 19 | Page Table:6Comparison of Theoretical & FEA values for deflection and stiffness at the spindle nose when the s pan length various from 170 mm to 200 mm for the front bearing with diameter of 65 mm with ‘B’ type Bearing arrangement [11] The deflection at the spindle nose in Y direction and the stiffness vlaues obtained through theoretical calculations and ANSYS are given in the table.5 and 6. The diamenter could be varied to the extent of a maximum of 65 mm from the practical considerations. The stiffness obtained by ANSYS of the optimized spindle with given configuration is around 183.0 N/ µm at the span length of 200 mm. In this we consider Triplet bearing set arrangement ‘B’for the front end of the spindle, in which one pair of angular contact ball bearings are arranged in tandem with respect to each other and back-to-back with respect to a single angular contact ball bearing. Tandem bearing pair will carry both radial and axial loads equally shared. [11] 4.4 Analysis of Results The deflection of the spindle nose in Y direction is function of bearing stiffness, span length and diameter of the spindle bearing for a given overhang. The deflection of the spindle nose in Y direction affects the machining accuracy.[11] V. Conclusions  Span length between bearing is varied from 140 to 230 mm which gives flexibility in sizing the span to accommodate the integral induction motor.  From results it is clear that Rigidity of the spindle is depends on the diameter of the spindle between the bearing. So from practical considerations of bearing speed, the diameter of the spindle varied from 55 to 65 mm maximum and result shows that 65mm diameter spindle for the arrangement ‘B’ has getting a stiffness value 165.9 N/µm and 27.14 mm is the deflection of the spindle nose based on static analysis for above arrangement. Therefore bearing arrangement type ‘B’ is chosen as an optimum design from static analysis results.  The effect of front bearing stiffness is on overall stiffness, hence locate higher siffness bearings at the front.  Rigidity analysis was carried out by using ANSYS and the result gives good correlation between theoretical calculation and ANSYS result. References. [1]. ANSYS Basic Analysis Procedures Guide, 002184, Aug2005, www.ansys.com.Book of Spindles, www.dynospindles.com. [2]. CMTI Hand Book, Machine Tool Design Hand Book Tata McGraw-Hill Company Limited, 1983,421-588 [3]. Daniel P. Soroka, Hardinge Inc. One Hardinge Dr.Elmira,NY 14902 Hard Turning and the Machine Tool. [4]. dsoroka@hardinge.com [5]. Dr.Sinan Badrawy, Dynamic Modeling and Analysis ofMotorized Milling Spindles, Moore Nanotechnology Systems,LLC, 2003. [6]. FAG Spindle Bearings Catalogue, AC 41 130/7 EA ·March 2008, www.fag.com. [7]. HMT, Production Technology, Tata McGraw HillPublication, 1980, 7 th Print, page 186-198. [8]. INA-FAG BEARINX ® -online Spindle Calculation-SCHAEFFLER GROUP Industrial. [9]. Lipka I, Harkany, Determination of the optimum bearingdistance of cantilever shafts with two supports, Mach. Tool. Research Transactions, 45 (1964) 65-80. [10]. Machine Manual, VMC 1000, The Mysore Kirloskercompany, Harihar. [11]. Anandkumar Telang, Static stiffness analysis of high frequency milling spindle, eISSN:2319-1163/ pISSN:2321-7308 [12]. Modal analysis using ANSYS,www.mece.ualberta.ca/tutorials/ansys. [13]. Momir Sarenac, Stiffness of Machine Tool Spindle as amainfactor for treatment accuracy-UDC 62-113,624.046,Mechanical Engineering Vol.1, No 6, 1999, pp. 665 – 674. Spindle Basics, 2008, www.spindlesworld.com. [14]. Technical Specifications for IBAG-Motor Spindles,IBAG Switzerland AG, 1999, www.ibag.ch. [15]. TIMKEN, Machine Tool Spindle, 1M-07-02 No. 5911,www.timken.com. [16]. Yung C. Shin, Analysis of bearing configuration effectson high speed spindles, International Journal of Machine Tools & Manufacture, 44 (2004) 347–364.83, 421-588. Diameter at Front bearing Mm THEORETICAL ANSYS Deflection at spindle nose µm Stiffness N/µm Deflection at spindle nose µm Stiffness N/µm 55 31.50 142.8 25.07 179.6 60 28.96 155.4 24.19 186.1 65 27.14 165.9 24.60 183.0