Journal of Mechanical Engineering and Automation

p-ISSN: 2163-2405    e-ISSN: 2163-2413

2015;  5(1): 56-66

doi:10.5923/j.jmea.20150501.07

Force Modelling in High Speed End- Milling of Super Alloys

Sunday J. Ojolo1, Olumuyiwa J. Agunsoye2, Oluwole Adesina3, Gbeminiyi Musbau Sobamowo1

1Department of Mechanical Engineering, University of Lagos, Akoka-Yaba, Nigeria

2Department ofMetallurgical and Materials Engineering, University of Lagos, Akoka-Yaba, Nigeria

3Department of Mechanical Engineering, Yaba College of Technology, Yaba, Nigeria

Correspondence to: Sunday J. Ojolo, Department of Mechanical Engineering, University of Lagos, Akoka-Yaba, Nigeria.

Email:

Copyright © 2015 Scientific & Academic Publishing. All Rights Reserved.

Abstract

Temperature field in metal cutting process is one of the most important phenomena in machining process. Temperature rise in machining directly or indirectly determines other cutting parameters such as tool life, tool wear, thermal deformation, surface quality and mechanics of chip formation. The variation in temperature of a cutting tool in end milling is more complicated than any other machining operation especially in high speed machining. It is therefore very important to investigate the temperature distribution on the cutting tool–work piece interface in end milling operation. The determination of the temperature field is carried out by the analysis of heat transfer in metal cutting zone. Most studies previously carried out on the temperature distribution model analysis were based on analytical model and with the used of conventional machining that is continuous cutting in nature. The limitations discovered in the models and validated experiments include the oversimplified assumptions which affect the accuracy of the models. In metal cutting process, thermo-mechanical coupling is required and to carry out any temperature field determination successfully, there is need to address the issue of various forces acting during cutting and the frictional effect on the tool-work piece interface. Most previous studies on the temperature field either neglected the effect of friction or assumed it to be constant. The friction model at the tool-work interface and tool-chip interface in metal cutting play a vital role in influencing the modelling process and the accuracy of predicted cutting forces, stress, and temperature distribution. In this work, mechanistic model was adopted to establish the cutting forces and also a new coefficient of friction was also established. This can be used to simulate the cutting process in order to enhance the machining quality especially surface finish and monitor the wear of tool. The cutting force model developed can be used to predict the various forces during machining of end milling through Mechanistic approach. The model gives room for understanding of the cutting patterns and surface integrity, tool life and machine stability. The model would be useful to simulate the cutting process in order to enhance machining quality.

Keywords: Force, Temperature, Machining

Cite this paper: Sunday J. Ojolo, Olumuyiwa J. Agunsoye, Oluwole Adesina, Gbeminiyi Musbau Sobamowo, Force Modelling in High Speed End- Milling of Super Alloys, Journal of Mechanical Engineering and Automation, Vol. 5 No. 1, 2015, pp. 56-66. doi: 10.5923/j.jmea.20150501.07.

1. Introduction

Machining process is one of the branches of manufacturing system that involves metal removal from a work piece to give a desired shape or geometry. It represents a substantial part of manufacturing industry today. Most manufacturing industries engaging in metal cutting processes in their operations include aerospace, automobile, chemical processing and die-mould factories as well. Machining operation comprise of substantial portion of the world’s infrastructure [1]. It is estimated that 15% of the cost of all mechanical components manufactured worldwide is derived from machining operation [2, 3]. The domestic expenditure on machining was estimated between 3% and 10% of the annual United State’s gross domestic product (GDP) i.e. $240 to $350 billion for 1998 [4, 5]. It is obvious that machining is very important in technical and economic development of a nation. Machining operations consume a huge amount of money annually worldwide. Over US$ 100 billion is spent annually worldwide on metal parts finishing processes such as turning, milling, boring and other cutting operations. It has also been noted that the machining industry converts about 10% of all the metals produced into swarfs [6].
In order to improve the performance of metal cutting process, the throughput and the quality of the components produced, there is need to establish the relationship between the output variables such as tool life, cutting force, surface roughness, through the optimization of some input variables such as feed rate, depth of cut, cutting speed and this may lead to appreciable performance of machine operation. The cutting force is one of the variables that have direct or indirect effect on other output variables and is also one of the factors that influence the performance of milling operation, the tool life as well as the dimensional accuracy of the work piece. Many attempts were made in the past in analysing force patterns as an indication of tool wear of the end milling process. Comprehensive review of cutting force modelling for milling process have been done by Smith [7] and Ehman et al [8]. The first analytical approach was presented by Merchant [9], based on the shear angle determination using minimum energy principle. The model analysed the geometric relation between the shear and chip flow directions. Stephenson and Wu [10] proposed an upper bound model for oblique cutting based on numerical minimisation of weighted sum of plastic and friction work. Armaego and Whitfield [11] used the single shear plane model and assumed that chip length ratio in the oblique cutting is the same as that in orthogonal cutting obtained from the normal shear angle. Shamato and Altintas [12] proposed theoretical shear angle prediction approach in oblique machining by employing minimum energy principle with basic assumptions that the deformation occurs on a single shear plane produced discontinuity velocity. Oxley [13] introduced a new parallel sided shear zone model for the machining predictive theory by considering geometric method and influence on temperature, strain rate and strain on flow stress. Mourfki et al [14] developed a thermo mechanical model of oblique cutting for HSM; this model makes an assumption that hydrostatic pressure is constant in primary shear zone. Fontaine et al [15] applied Mourfki et al [16] model to cutting force prediction in ball end milling.
The plastic deformation of metal cutting process is regarded as quasi-static since it is assumed that the inertial forces due to plastic flow may be neglected. Johnson and Mellon [17]; Yang and Park [18]; Budak et al [19]; Yun and Shao [20]; and Lazoglu [21] used mechanistic model to predict the cutting force, where the cutting force is estimated by dividing the cutting edge into small elements and applying a simple mathematical formulation. This system requires large amount of data gathered and stored in the cutting databases, the limitation is that the databases do not provide physical mechanism on the cutting process. However due to complex mechanisms such as high strain rates, high temperature gradients and combined elastic and plastic deformations the analytical models are unable to completely characterize the phenomena that occur on the rake and flank face of the cutting insert. Mechanistic model considered the effect of process noise factor (run out tool, tool wear, and inhomogeneity of the material in the process response. Montogomery and Altintas [22]; Yucesan and Altintas [23] used mechanistic models to predict the cutting force based on a method developed by Sabberwal [24] based on the assumption that the cutting force is proportional to the chip cross sectional area. Kline et al [25]; Budak and Altintas [26] used mechanistic model for force predictions and has been extended to predict associated machine component deflection and form error. Budak [27] developed a model of force prediction that was used to check available machine power but process optimization cannot be carried under unstable conditions. Based on all the analysis of the available model enumerated, and in order to predict and optimize accurate milling process, a mechanistic cutting forces model need to be developed

2. Model Development

Braghini et al [28] and Vizan et al [29] stated that mechanistic model can be further divided into analytical and numerical depending on the method of solution. It has been adopted by many researchers in the analysis of the milling process. This process generally refers to the estimation of cutting force by means of the uncut chip thickness and the calibration coefficient known as the speed cutting force. To develop the mechanistic model the following assumptions were used:
(i) the run out effect is ignored since the rigid system is used,
(ii) there is no built up edge formation on the cutter and,
(iii) wear occur at high speeds is negligible.
Figure 1. The shematic diagram of the milling process
Consider the milling process shown in Figure 1. For a point on the cutting tooth, the differential milling forces, correspond to an infinitesimal element thickness in the tangential, radial and axial direction respectively. The dFtj is the differential milling force in tangential direction
(1)
The differential milling force in radial direction is given by equation 2
(2)
is the differential milling force in radial direction.
(3)
The general chip thickness equation for active cutting point on a cutter in the milling operation without run out can be approximated as:
(4)
where,
(5)
The tangential, radial and axial forces can be resolved in x, y and z directions as given by the equation
(6)
(7)
(8)
(9)
By substituting for the value of h and ϕj in equation (9), then it becomes
(10)
Integrating the above equation within the immersion part of the tool, between the boundary conditions of lower and upper axial engagement limits of flutes
(11)
(12)
But, recall that the immersion angle is given by the equation (5)
Then substitute for in equation (9),
(13)
So, the differential milling force in x-direction is given by:
(14)
(15)
Then equation (16) gives the value of the force on one cutting edge or flute in x-direction
(16)
The summation of forces in the four flutes milling cutter is given by equation (17)
(17)
so also the derivation of y-components of forces can be deduced.
The differential milling force in y direction is given by the equation (18)
(18)
Substitute for in equation (19) and integrate between the lower and upper limits, so we have:
(19)
then,
(20)
Also, equation (21) gives the value of force in one cutting edge or flute in y-direction
(21)
The total cuting force in y- direction is given by equation (22)
(22)
The differential milling force in Z- direction is given by equation (23)
(23)
Then substitute the value of (h)
(24)
Then, is given by:
(25)
Lastly, equation (26) gives the value of the force in z-direction in one cutting edge or flute
(26)
Equation (27) gives the total forces in z- direction of the four flutes
(27)
The total forces acting in all the x, y and z directions is given by equation (28)
(28)
(29)
But,
(30)
(31)
Recall, from equation (5) the expression for , we have
In this work, Arrazolla (2008) expression for coefficient of friction was adopted
(32)
Substitute for the value of immersion angle in equation (3.32), we have
(33)

3. Results and Discussions

3.1. Effect of Number of flute Engagement on the Milling Operation

Figure 2a-2c show the variation of axial engagement of the cut portion of the flute with immersion angle at different angular orientation of the cutter, 0°, 90° and 180° respectively. From the figure, as axial engagement of the cut portion of the flute increases, the immersion angle decreases. Also, it can be observedthat, as the cutter rotates, it generates points on the surface of work piece, these points move along the axial direction due to helical flutes, completing the surface profile at certain feed position along x-axis. This indicates that the first flutes would be the first to disengage while the fourth flute would be the last to disengage. The same result for figure 2(b) and 2(c) but only that the cutting tool engaged the work piece at different immersion angle. The immersion angle increased from -3.5 to 0 for first flute; -2.0 to 1.6 for second flute; -0.2 to 3.1 for third flute; and 1.1 to 4.8for fourth flute as the axial distance decresed from 30 mm to 0 mm.
Figure 2(a-c). The graph of immersion angle against Axial Distance

3.2. Effect of Tool Geometryonthe Cutting Force

Figure 3a-d show the profile of the cutting forces of different flutes with respect to the axial distance travelled by the cutting tool. The sinusoidal wave pattern shows the directional movement of the cutting tool on the work piece while is being engaged for the four number of flutes considered. The model shows that cutting forces in end milling operation may periodically fluctuate with the number of tooth passes and also cutting forces are significantly influenced by the trochoidal trajectory of the cutting tool. The cutting force fluctuates between -200N and +200N when the first and second flutes are in engagement; and -350N to +350N when the third and fourth flutes were engaged in cutting.
Figure 3(a-d). Axial force against axial distance
Figure 4. Cutting forces against cutter rotation angle

3.3. Effects of Cutting Force on the Angular Rotation of the Cutter

Figure 4 shows the cutting action of the 4- flutes. The cutting force in feed direction (Fx) is a combination of tangential and radial forces,so also the normal directional force (Fy) and axial force is only force acting in axial direction. The amplitude is well predicted in Fx and Fy components while an offset appears in Fz. It is due to material flow that occurred around the cutting edge. This material flow associated with shearing occuring at the clearance face leads to ploughing force. The direction of this ploughing is mainly normal to the tool envelope and at the tool tip, this directionis very close to the z- direction. The charactristics of Fx and Fy are sinusoidal while Fz is about the straight line. In Fx and Fy cutting system, there is an intermittent cutting action of one cutting edge after another during half revolution, so that the cutting forces are varied in one revolution of the cutter. However, in Fz system cutting edges cuts simultaneously during one revolution of the cutter and there is superposition of two opposite and symmetrical forces with respect to tool axis. The result is that there is a constant z axis force.This is attributed to the fact that two cutting edges perform cutting action simultaneously during every 100° of cutting range, so there is a force during every 100° of rotation angle. The cutting force in the feed direction was maximum (300N) at 40° cuter rotation and minimum (-200N) at 150° cutter rotation. The highest cutting force (400N) was obtained in the normal direction when the cuter rotaion was 100°.

3.4. Effect of Friction on the Axial Distance in Milling Operation

The graph in fig 5a–b show a linear relationship between the coefficient of friction and axial distance of the cutting tool, thus the higher the axial distance when the flutes are engaged in cutting action the higher the coefficient of friction between the work piece due to different immersion angle. From figure 5a it can be deduced that the coefficient of friction of first flutes is between 0.22-0.33 which means the friction along the cutting tool is not constant but varied.Lower values of friction coefficients (0.01-0.15) were obtained when the fourth flute is engaged in cutting.

4. Conclusions

Modeling of friction and forces in end milling represents a very useful tool for predictions of operational behavior of the system. A cutting force model was developed that can be used to predict the various forces during machining of end milling through Mechanistic approach. The model gives room for understanding of the cutting patterns and surface integrity, tool life and machine stability. The model would be useful to simulate the cutting process in order to enhance machining quality.
Figure 5(a-b). Coefficient of friction against axial distance
It can be concluded that:
The immersion angle increased from -3.5 to 0 for first flute; -2.0 to 1.6 for second flute; -0.2 to 3.1 for third flute; and 1.1 to 4.8for fourth flute as the axial distance decresed from 30 mm to 0 mm.
The cutting force fluctuates between -200N and +200N when the first and second flutes are in engagement; and -350N to +350N when the third and fourth flutes were engaged in cutting.
The cutting force in the feed direction was maximum (300N) at 40° cuter rotation and minimum (-200N) at 150° cutter rotation. The highest cutting force (400N) was obtained in the normal direction when the cuter rotaion was 100°.
Lower values of friction coefficients (0.01-0.15) were obtained when the fourth flute is engaged in cutting.

References

[1]  M. A. Davies, B. Dutteree, J. Pratt, A.J. Schnant, and J.Bryan, 1998. On the Dynamics of high speed milling with long slender end mills.Annals of CIRP 47 (1): 5-60.
[2]  M.E. Merchant, 1998 Proceeding of the first CIRP International Workshop on Modelling of Machining Operation, Atlanta , GA, USA.
[3]  W. Endres, R. Devor, S. Kapoor, 1995. A dual mechanism approach to the prediction of machining force I: model development ASME Journal, 117 (4): 526-533.
[4]  A.Hans, Y. Soons, L. Simone 1995 Precision in Machining research challenges, Gaithersburg, MD:National Institute of Standard and Technology NISTIR 5628.
[5]  M. Shaw, 1984. Metal Cutting Principles Clarendon Press, Oxford.
[6]  N.B. D. Mohd, 2012. The effect of cryogenic cutting tools on machining difficult cut material. A Master thesis submitted to University Tun Hussein Onn, Malaysia.
[7]  S.Smith, J. Thisty, 1991. An overview of modeling and simulation of the milling process ASME Journal of Engineering for Industry, 113: 169-175.
[8]  K.F. Ehman, S.G. Kapoor, R.E. Devor, R. I. Lazoglu, 1997. Machining process modelling: A Review. ASME Journal of Manufacturing Science and Engineering,119:655-663.
[9]  M.E. Merchant, 1945. Mechanics of Metal Cutting Process. Journal of Applied Physics,16: 267-318.
[10]  D.A. Stephenson, S.M. Wu, 1988. Computer models for the cutting mechanics of three- dimensional cutting processes Part I. Theory and numerical method. Journal of Engineering for Industry, 110: 32-37.
[11]  E.J.A. Armaego, R.C. Whitfield, 1985. Computer based modeling of popular machining operation for force and power predictions. Annal of the CIRP, 34: 65-69.
[12]  E. Shamoto, Y. Altintas, 1999. Prediction of Shear angle in cutting with maximum shear stress and minimum energy principles.Journal of Manufacturing Science and Technology, 121:399-407.
[13]  P.L.B. Oxley 1989 Mechanics of Machining. Analytical approach to assessing machinability, Halisted Press, New York.
[14]  A. Moufki, D. Dudzinski, A. Molinari, M. Rausch, 2000. Thermo-visco-plasticmodeling of oblique cutting: forces and chip flow predictions, Journal of Mechanical Sciences, 42 (6): 1205–1232.
[15]  A. Moufki, A. Devillez, D. Dudzinski, A. Molinari, 2004. Thermomechanical modelling of oblique cutting and experimental validation, International Journal of Machine Tools and Manufacture, 44(9): 971–989.
[16]  M. Fontaine, A. Deillez, A., Mourfki, D. Dundzinski, 2006. Predictive force model for ball- end milling and experimental validations with a wavelike form machining test.International Journal of Machine Tools and Manufacture, 46:367-380.
[17]  W. Johnson, P.B. Mellor, 1983. Engineering plasticity, John Willey & Sons New York
[18]  M. Yang, H. Park, 1991. The prediction of cutting force coefficient in ball-end milling. International Journal of machine tools and manufactures, 31 (1): 45-54.
[19]  E. Budak, Y. Altintas, E.J.A. Armaego, 1996. Prediction of milling force coefficient from orthogonal cutting data ASME Journal of manufacturing science and Engineering, 118: 216-224.
[20]  W.S. Yun, D.W. Chao, 2001. Cutting force prediction using cutting conditions independent coefficient in end milling. International Journal of Machine Tools and Manufactures, 47: 463-478.
[21]  I. Lazoglu, 2003. Prediction of tool and chip temperature in continuous and interrupted machining. International Journal of Machine Tools and Manufacture, 42: (9) 1011-1022.
[22]  D. Montogomery, Y. Altintas, 1991. Mechanism of cutting force and surface generation in dynamic milling. Transaction of ASME Journal of Engineering for Industry, 113: 160-168.
[23]  G. Yucesan, Y. Altintas, 1996. Prediction of ball; end milling forces. ASME Journal of Engineering for Industry, 118: 95-103.
[24]  A. Sabberwal, 1962. Cutting forces in down milling. International Journal for Machine tool, 2: 27-41.
[25]  W. Kline, R. Devor, I. Linberg, 1982. The prediction of cutting force in end milling. International Journal for Machine tool Res 22 (1); 20-22.
[26]  E. Budak, Y. Altintas, E.J.A. Armarego, 1996. Prediction of milling force coefficients from orthogonal cutting data. Journal of Manufacturing Science and Engineering, 118: 216–224.
[27]  E. Budak, 2005. Analytical model for high performance milling. International Journal of Machine Tool and Manufacture, 46: 476-488.
[28]  M.C. Shaw, N.H. Cook, P.A. Smith, 1952.The mechanics of three-dimensional cutting operations.Transactions of the ASME, 74: 1055–1064.
[29]  A. Braghini Jr., C. Valente, R. Coelho, and G. Medalha, 2003. Experimental evaluationof cutting force parameters applying mechanistic model in orthogonal milling. Journal of the Brazilian Society of Mechanical Sciences and Engineering, 25(3):247-253.
[30]  A. Vizan, J. Hernandez, H. Perez andM. Guzman, 2007. Estimation of cutting forcesin micro-milling through the determination of specificcutting pressures. International Journal of Computer Integrated Manufacturing, 190:18-22.