Characteristics of cutting forces and chip formation in machining of titanium alloys Authors: S. Sun, M. Brandt, M.S. Dargusch October 5, 2010 Presented.

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Presentation transcript:

Characteristics of cutting forces and chip formation in machining of titanium alloys Authors: S. Sun, M. Brandt, M.S. Dargusch October 5, 2010 Presented by: Chris Vidmar

Introduction Titanium alloys are seeing increasing demands due to superior properties such as ▫Excellent strength-to-weight ratio ▫Strong corrosion resistance ▫Retains high strength at high temperature Classified as hard to machine ▫Low thermal conductivity ▫High chemical reactivity ▫Low modulus of elasticity

Introduction (cont.) High-cost and time consuming process is driving research efforts to understand the cutting process and chip formation. Segmented chip formation is due to localized shearing, which results in cyclic forces, causing chatter and limiting material removal rate An understanding of these dynamic cutting forces will lead to increased understanding of chip formation and tool wear.

References [ 1] R.R. Boyer, An overview on the use of titanium in the aerospace industry, Materials Science and Engineering 213A (1996), pp. 103–114.[ 1] [2] E.O. Ezugwu, J. Bonney and Y. Yamane, An overview of the machinability of aeroengine alloys, Journal of Materials Processing Technology 134 (2003), pp. 233–253.[2] [3] E.O. Ezugwu and Z.M. Wang, Titanium alloys and their machinability—a review, Journal of Materials Processing Technology 68 (1997), pp. 262– 274.[3] [4] J.I. Hughes, A.R.C. Sharman and K. Ridgway, The effect of cutting tool material and edge geometry on tool life and workpiece surface integrity, Proceedings of the Institution of Mechanical Engineers Part B: Journal of Engineering Manufacture 220 (2006), pp. 93–107.[4] [5] A. Vyas and M.C. Shaw, Mechanics of saw-tooth chip formation in metal cutting, Journal of Manufacturing Science and Engineering—Transactions of the ASME 211 (1999), pp. 163–172.[5] [6] T. Obikawa and E. Usui, Computational machining of titanium alloy—finite element modeling and a few results, Journal of Manufacturing Science and Engineering—Transactions of the ASME 118 (1996), pp. 208–215.[6] [7] R. Komanduri and B.F.V. Turkovich, New observations on the mechanism of chip formation when machining titanium alloys, Wear 69 (1981), pp. 179–188.[7] [8] J. Barry, G. Byrne and D. Lennon, Observations on chip formation and acoustic emission in machining Ti–6Al–4V alloy, International Journal of Machine Tools and Manufacture 41 (2001), pp. 1055–1070.[8] [9] R. Komanduri and Z.-B. Hou, On the thermoplastic shear instability in the machining of a titanium alloy (Ti–6Al–4V), Metallurgical and Materials Transactions 33A (2002), pp. 2995–3010.[9] [10] A.M. Davis, S.E. Fick and C.J. Evans, Dynamic measurement of shear band formation in precision hard turning, Liber Amicorum for Prof. Paul Vanherck, Katholieke Universiteit Leuven (1996), pp. 215–224.[10] [11] J. Barry and G. Byrne, Study on acoustic emission in machining hardened steels. Part 1: acoustic emission during saw-tooth chip formation, Proceedings of the Institution of Mechanical Engineers Part B: Journal of Engineering Manufacture 215 (2001), pp. 1549–1559.[11] [12] R. Komanduri, Some clarifications on the mechanics of chip formation when machining titanium alloys, Wear 76 (1982), pp. 15–34.[12] [13] A.E. Bayoumi and J.Q. Xie, Some metallurgical aspects of chip formation in cutting Ti–6 wt% Al–4 wt% V alloy, Materials Science and Engineering 190A (1995), pp. 173–180.[13] [14] J.D.P. Velásquez, B. Bolle, P. Chevrier, G. Geandier and A. Tidu, Metallurgical study on chips obtained by high speed machining of a Ti–6 wt% Al– 4 wt% V alloy, Materials Science and Engineering 452–453A (2007), pp. 469–474.[14] [15] D.G. Flom, R. Komanduri and M. Lee, High-speed machining of metals, Annual Review of Materials Science 14 (1984), pp. 231–278.[15] [16] G.R. Johnson, W.H. Cook, A constitutive model and data for metals subjected to large strains, high strain rates and high temperature, in: Proceedings of the Seventh International Symposium on Ballistics, The Hague, The Netherlands, 1983, pp. 541–547.[16] [17] G.L. Wulf, High-strain rate compression of titanium and some titanium alloys, International Journal of Mechanical Sciences 21 (1979), pp. 713– 718.[17] [18] P. Follansbee and G.T. Gray, An analysis of the low temperature low- and high-strain rate deformation of Ti–6Al–4V, Metallurgical Transactions 20A (1989), pp. 863–874.[18] [19] G. Sutter and A. Molinari, Analysis of cutting force components and friction in high speed machining, Journal of Manufacturing Science and Engineering—Transactions of the ASME 127 (2005), pp. 245–250.[19] [20] G. Poulachon and A.L. Moisan, Hard turning: chip formation mechanisms and metallurgical aspects, Journal of Manufacturing Science and Engineering—Transactions of the ASME 122 (2000), pp. 406–412.[20]

Materials and experimental procedures Ti6Al4V bar with a diameter of 60 mm 3.5 hp Hafco Metal Master lathe (Model AL540) by dry machining with a CNMX1204A2-SMH13A-type tool supplied by Sandvik 3-component force sensor (PCB Model 260A01) with an upper frequency limit of 90 kHz feed force (F X ), thrust force (F Y ) and cutting force (F Z ),

Results Three sections: 1.Influence of feed rate 2.Effect of cutting speed 3.Characteristics of the cyclic force

Influence of feed rate Severe tool vibration at feeds less than mm Cutting forces increase with increasing feed (exception between and due to high tool vibration) Tool vibration constant at 260 Hz, independent of feed Increasing force amplitude, drop after mm feed Vibration can be eliminated by changing tool entry angle or increasing feed rate

Effect of cutting speed Force frequency increases linearly with cutting speed Amplitude variation decreases with increasing cutting speed, except for where the frequencies were multiples of 260 Hz (the intrinsic harmonic frequency of the cutting) Due to increasing temperature, which reduces modulus of elasticity

Effect of cutting speed (cont.) Average cutting forced increased up to 21 m/min due to strain hardening Decreased dramatically from 21 to 57 m/min (attributed to thermal softening) Small increase from 57 to 75 Constant from 75 to 113 followed by gradual decrease Due to dramatic increase in strength with strain rate (makes increasing cutting speed difficult) Force increased linearly with depth, frequency remained constant

Effect of cutting speed (cont.) Continuous chip formation and static cutting forces possible at low cutting speeds in certain sections due to inhomogeneous structure Static cutting forces reduce and disappear at 75 m/min Cyclic force dominates above 75 m/min resulting in purely segmented chips

Characteristics of the cyclic force Chip segmentation frequency and cyclic force frequency show very good correlation Cyclic force is the result of chip segmentation Cyclic frequency is directly proportional to cutting speed and indirectly proportional to feed rate Amplitude increase linearly with depth of cut and is inversely proportional to cutting speed Equations don’t always apply

Conclusions Both segmented and continuous chips possible at low cutting speeds Maximum cyclic force always 1.18 times higher than static force regardless of depth Segmented chips only above 75 m/min Cyclic force directly proportional to cutting speed and indirectly proportional feet rate Amplitude increases with increasing depth and feed rate and decreases with speeds from 67 m/min except when the cyclic force frequency matched the machine harmonic frequency Force decreases with cutting sped due to thermal hardening, except from 10 to 21 and 57 to 75 attributed to two phases of strain rate hardening Authors suggest that a new physical model be developed to explain segmented chip formation

Useful? Effective for industries involved in mass production of titanium parts (aerospace) Data can be useful in maximizing machining efficiency of titanium by minimizing forces and maximizing speeds to produce products quicker at lower costs Reducing vibrations can improve surface finish and increase tool life