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    Available online at www.sciencedirect.com

    Physics Procedia 12 (2011) 308316

    1875-3892 2011 Published by Elsevier Ltd.

    doi:10.1016/j.phpro.2011.03.138

    LiM 2011

    Analysis of the Laser Drilling Process for the Combination with a

    Single-Lip Deep Hole Drilling Process with Small Diameters

    Dirk Biermanna, Markus Heilmanna*

    aInstitute of Machining Technology, Technische Universitt Dortmund, Baroper Str. 301, 44227 Dortmund, Germany

    Abstract

    Due to the tendency of downsizing of components, also the industrial relevance of bore holes with small diameters and high

    length-to-diameter ratios rises with the growing requirements on parts. In these applications, the combination of laser pre-drilling

    and single-lip deep hole drilling can shorten the process chain in machining components with non-planar surfaces, or can reduce

    tool wear in machining case-hardened materials. In this research, the combination of these processes was realized and

    investigated for the very first time.

    Keywords:Hybrid machining; single-lip deep hole drilling; laser drilling; combination of drilling processes

    1. Motivation / State of the Art

    Because of increasing requirements on components concerning their specific properties, e. g. increasing power

    density or miniaturization, the dimensions of parts diminish in size. For the production of these parts, adaptations of

    the manufacturing processes used as well as the development of new technologies are necessary. This tendency is of

    particular relevance in the automotive industry, the information technology industry as well as for medical and

    biomedical products [1-2]. In various applications, the production of bore holes with a high length-to-diameter ratio

    and small diameters is required. For the production of deep holes with small diameters different manufacturing

    processes can be used. In this context single-lip deep hole drilling (SLD), laser drilling, electro discharge machining

    (EDM), electron beam machining (EBM) and electro chemical machining (ECM) were used. Each of the processes

    mentioned above provides specific properties, especially concerning diameter range, drilling depth, accuracy,

    repeatability and process time [3-6]. The combination of different processes for bore hole production can enhance

    the bore hole quality and can shorten the production time. One possibility for a hybrid process for micro machining

    is the combination of laser pre-drilling and counter-boring by EDM drilling [7].

    The motivation for the approach presented is based on applications, where the conditions at the beginning of the

    deep hole drilling process are unfavorable. Examples are the production of deep holes in non-planar or case-

    hardened surfaces [8]. In this research, the combination of the production processes laser drilling and single-lip deep

    *Corresponding author. Tel.: 0049 231 755 6426; Fax: 0049 231 755 5141.

    E-mail address: [email protected].

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    Dirk Biermann and Markus Heilmann / Physics Procedia 12 (2011) 308316 309

    hole drilling was analyzed for the very first time. The aim of this investigation is the manufacturing of a pilot-hole

    by a laser for guiding the single-lip drill (SLD) in the process phase of pre-drilling (Figure 1). With the new

    approach, a reduction of the process time in machining workpieces with planar surfaces as well as a shortening of

    the process chain for the production of deep holes at non-planar surfaces is intended. Furthermore, a decrease in tool

    wear is aspired by laser drilling through a hardened layer. To realize these aims, an innovative machine tool concept

    was developed that integrates a Nd:YAG laser for laser drilling on a conventional deep hole drilling machine tool.

    Using this machine tool, the utilization of laser processes and single-lip deep hole drilling in one setup is possible.

    Figure 1. Process combination of laser drilling and single-lip deep hole drilling for the production of deep holes

    2. Experimental

    For the experimental investigations, a prototypical machine tool was designed and built. This machine tool

    consists of a Nd:YAG-laser, that is integrated into a conventional deep hole drilling machine tool for small

    diameters. The results of this combination is that both, a single-lip deep hole drilling process and a laser drilling

    process, can be carried out using the same machine tool and the same workpiece fixture. In this adapted machinetool, the single-lip deep hole drilling process is designed for a tool diameter range from d = 0.5 mm up to d = 6 mm.

    The laser drilling process can be carried out in four different operating principles such as single-pulse, percussion,

    trepanning and helical drilling. The laser used has a peak power of P = 8,000 W and a pulse duration of

    t = 0.08,1 ms. The machine tool used as well as the experimental setup for laser drilling and single-lip deep hole

    drilling is shown in Figure 2.

    Single-Lip Deep Hole Drilling:

    Borehole diameter: d = 0.5 mm up to 6 mm

    Spindle power: P = 4 kW

    Number of revolutions: nmax = 36.000 1/min

    Feed velocity: vfmax

    = 15.000 mm/min

    Drilling depth: ltmax = 450 mm

    TBT ML-200: Prototype Single-Lip Deep Hole Drilling Machine Tool with an Integrated Laser

    Laser:

    Laser power: P = 80 W

    Peak power: P = 0.5,,8 kW

    Peak energy: E = 0.04,,8 Joule

    Pulse duration: t = 0.08,,1 ms

    Figure 2. Machine tool for single-lip deep hole drilling and laser drilling

    Single-lip deep hole drillingPilot -hole by laser drilling

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    310 Dirk Biermann and Markus Heilmann / Physics Procedia 12 (2011) 308316

    In these experiments, for the mechanical drilling, single-lip tools with a diameter of d = 0.5 mm were chosen. The

    tools consisted of a homogenous, uncoated cemented carbide substrate (ISO HW-K15) and contained an internal

    cooling lubricant supply channel. As workpiece material, a stainless steel with an austenitic structure, so-called

    AISI 316L, was used. The cooling lubrication concept was an internal oil supply using a high oil pressure of

    p = 200 bar. The process parameters such as cutting speed and feed were varied. The range of the cutting speed was

    kept between vc= 30,...,50 m/min, and the range of feed amounted between f = 0.5,...,0.7 m/rev.

    3. Results and Discussion

    3.1. Process design for laser pre-drilling

    In the first step of the experiments conducted, the laser drilling process was analyzed with the aim of the

    identification of suitable laser parameters that allow the manufacturing of bore holes meeting the requirements the

    deep hole drilling process demands on a guiding assistance. The targeted pilot-hole dimensions are named in

    Figure 3.

    Figure 3. Definition of the targeted pilot-hole dimensions

    For the guiding assistance of a single-lip deep hole drilling tool, the pilot-hole must have a diameter with a low

    tolerance of dmax=500+ 10m. This tolerance is necessary to avoid the contact of the deep hole drilling tool with the

    bore hole wall while moving it into the pilot-hole. Furthermore, this pilot-hole must have a low roundness deviation

    to avoid contact of the cutting edge with the workpiece material during the positioning of the tool into the laser

    drilled hole. The depth of the pilot-hole must be at least 1.5 of the tool diameter. This is founded in the distance of

    the tool tip to the guide pad. Especially in laser drilling, a hardening at the bore hole ground and at the bore hole

    wall can occur which can lead to high mechanical loads on the deep hole drilling tool. Due to that, the influence on

    the peripheral zone also should be low. To fulfill these requirements, a variation of laser parameters was conducted

    and the resulting bore holes were evaluated concerning the targeted values diameter, roundness deviation, drilling

    depth, surface roughness and peripheral zone. For every laser parameter combination repetitions were performed to

    analyze the repeatability of the laser processes. At first the laser drilling strategies single-pulse, percussion and

    helical drilling were realized. The influence of the laser drilling strategy on the bore hole diameter is shown in

    Figure 4.

    The results show, that the use of percussion laser drilling is unsuitable for the production of laser pilot holes

    under the conditions viewed. The diameter is significantly lower as the targeted value and the bore hole shows a

    high roundness deviation. This is based on the higher amount of material molten by the laser. A part of this material

    Target values:

    Pilot-hole diameter: D = 500,,510 m

    Pilot-hole depth: l = 0.75,,1.5 mm

    Roundness dev.: tk < 10 m

    1.53xd

    d+0.01

    Definition of targeted pilot-hole dimensions

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    Dirk Biermann and Markus Heilmann / Physics Procedia 12 (2011) 308316 311

    solidifies at the bore hole wall before it exists the bore hole, recast-layers occurs. These layers reduce the bore hole

    diameter and influence the roundness of the bore hole negatively. This effect also occurs in helical laser drilling. In

    contrast to percussion drilling, the bore hole diameter can be adjusted by an adaption of the diameter of the helix D H.

    Due to the creation of recast layers, the reproducibility of the diameter is lower than in single-pulse drilling. Another

    disadvantage is the longer process time. In single-pulse laser drilling, the aimed diameter is approximately reached

    with the laser parameters presented. Furthermore, the bore holes produced show qualitatively a high accuracy. Incombination with the shorter production times the single-pulse laser drilling was identified as the most convenient

    laser drilling strategy for the production of pilot holes. Because of that, this strategy is viewed in the following.

    Figure 4. Influence of the laser drilling strategy on the bore hole diameter

    In the single-pulse laser drilling experiments conducted, the variables pulse duration and peak power have shown

    the highest impact on the bore hole quality. Because of that, in the following the influence of these parameters will

    be discussed. As named before, the main requirement of a pilot-hole for the guiding assistance of a deep hole

    drilling tool is its diameter and roundness accuracy (Figure 5).

    The increasing pulse duration shows the tendency of leading to growing bore hole diameters and to decreasing

    roundness deviations. Due to absorption, reflection and heat transportation effects, the laser influenced area

    increases and the diameter increases when using longer pulse durations. In the parameter range viewed, the impact

    of the pulse duration on the roundness deviation is reciprocally to its effect on the diameter. In the experiments with

    the lowest pulse duration the highest roundness deviations result. Furthermore, the scanning electron microscopy

    views of the bore holes produced using the lowest pulse duration show a significant deviation of the bore hole

    cylindricity. This deviation can lead to a contact of the single-lip deep hole drilling tool with the bore hole wall in

    the process phase of positioning the deep hole drilling tool in the pilot hole. This contact can effect tool wear or tool

    200 m 200 m 200 m 200 m 200 m

    Laser: Nd:YAG Workpiece material: AISI 316L

    Peak power: P = 7000 W Pulse duration: = 1 ms

    Pulse frequency: f = 10 Hz Number of pulses: n = varied

    Focus position: sf = 0 mm Process gas: Compr. air

    200

    300

    400

    m

    600

    Percussion

    drilling

    Helical drilling

    DH = 0.1 mm

    Helical drilling

    DH = 0.2 mm

    Helical drilling

    DH = 0.25 mm

    Single-pulse

    drilling

    Percussion / helical drilling

    Number of pulses: n = 250

    DiameterD

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    312 Dirk Biermann and Markus Heilmann / Physics Procedia 12 (2011) 308316

    Figure 5. Influence of the pulse duration and peak power on the diameter and the roundness deviation

    breakages in the area of the cutting edge corner. The occurring deviation can be explained by the Gaussian-shaped

    distribution of intensity. At low pulse durations, the energy of the laser is only at the center of the laser beam

    sufficient for material ablation. Due to effects leading to a loss of power, such as reflection, this area is reduced by

    increasing drilling depth and the conical bore hole shape is created.

    The peak power shows also an impact on the bore hole diameter. With increasing peak power, the diameter also

    increases. Based on effects such as absorption, heat transportation and reflection with higher peak power thediameter also increases.

    Beside the bore hole diameter and roundness deviation, the pulse duration shows an influence on the drilling

    depth. This is presented in Figure 6. In the realized pulse duration range, the drilling depth increases degressively.

    Due to that, the ablation rate decrease with the drilling process progress. This can also be explained by the Gaussian-

    shaped distribution of intensity. Furthermore, the radiation incidence angle increase because of the conical shape of

    the bore hole occurring in the laser drilling process and the connected change in absorption conditions. Another

    aspect can be a plasma resulting from the vaporized metal. This plasma can absorb the laser light [10, 11].

    = 0.5 ms= 0.25 ms

    P=8000W

    = 1 ms

    P=6000W

    P=7000

    W

    Laser: Nd:YAG Workpiece material: AISI 316L

    Peak power: P = varied Pulse duration: = varied

    Pulse frequency: - Number of pulses: n = 1

    Focus position: sf = 0 mm Process gas: Compr. air

    200 m 200 m 200 m

    200 m 200 m 200 m

    200 m 200 m 200 m

    D = 526 m

    D = 505 m

    D = 493 m

    D = 455 m

    D = 448 m

    D = 435 m

    D = 507 m

    D = 489 m

    D = 480 mtk= 39 m tk= 15 m tk= 29 m

    tk= 42 m tk= 12 m tk= 22 m

    tk= 28 m tk= 20 m tk= 24 m

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    Dirk Biermann and Markus Heilmann / Physics Procedia 12 (2011) 308316 313

    Figure 6. Influence of the pulse duration and the peak power on the drilling depth

    Beside the requirements on the geometric tolerances of the bore hole, the pilot-hole produced by laser should also

    have a low surface roughness as well as no significant impact on the peripheral zone. For the evaluation of these two

    bore hole properties, cross-sections of the bore holes were produced. The surface roughness was detected using the

    3D-confocal whitelight microscopy. For the evaluation of the impact of the laser drilling process on the peripheral

    zone, microhardness was measured in the peripheral zone with defined distances to the bore hole wall. The results of

    this analysis are presented in Figure 7.

    Figure 7. Influence of the pulse duration and the peak power on the surface quality and the impact on the peripheral zone

    In the laser drilling experiments using single-pulse laser drilling, a high surface quality was reached. In these

    experiments, the peak power shows no influence on the surface quality but the pulse duration does. Due to the

    higher drilling depth reached at higher pulse durations, more material must come out of the bore hole at increasing

    0

    1

    mm

    3

    0 0.25 0.5 ms 1

    Drillingdepthlt

    Pulse duration

    lt /

    Drillingdepthlt

    Laser: Nd:YAG Workpiece material: AISI 316L

    Peak power: P = varied Pulse duration: = varied

    Pulse frequency: - Number of pulses: n = 1

    Focus position: sf = 0 mm Process gas: Compr. air

    P = 7000 W

    0

    1

    mm

    3

    0 6000 7000 W 9000

    Peak power P

    = 0.5 ms

    Laser: Nd:YAG Workpiece material: AISI 316L

    Peak power: P = varied Pulse duration: = variedPulse frequency: - Number of pulses: n = 1

    Focus position: sf = 0 mm Process gas: Compr. air

    0.0

    0.10.2

    0.3

    0.4

    0.5

    m

    0.7

    0.0

    0.51.0

    1.5

    2.0

    2.5

    m

    3.5

    = 0.5 ms

    P = 7000 W

    = 0.5 ms

    P = 8000 W

    = 1.0 ms

    P = 8000 W

    Ro

    ughnessdepthRz

    RoughnessRa

    200

    240

    280

    320

    HV0.05

    400

    0 60 120 m 240

    MicrohardnessHm

    = 1.0 ms

    P = 8000 W

    Distance to the bore hole surface s

    Rz

    Ra

    Surface quality Peripheral zone

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    314 Dirk Biermann and Markus Heilmann / Physics Procedia 12 (2011) 308316

    distances. Both facts benefit the formation of recast-layers that influences the surface quality negatively. In

    comparison to percussion drilling, in single-pulse drilling this effect is significantly lower. Furthermore, the standard

    deviation of the surface quality reached is relatively high. Based on the assumption that high values for surface

    roughness correlates with recast-layers, for the laser drilling process with the highest surface roughness,

    microhardness of the peripheral zone was measured. The measurements show no significant influence of the laser

    drilling process on the peripheral zone. The microhardness values detected alternate in the area of the hardness ofthe material tested.

    The experiments have shown that the production of bore holes for the use as a guiding assistance for deep hole

    drilling tools by laser is possible. For the aimed manufacturing task single-pulse laser drilling is the most applicable

    laser drilling strategy. To fulfill the requirements on the bore hole quality, an analysis of the influences of the laser

    parameters were done. With a peak power of P = 8,000 W, pulse durations between = 0.51 ms and compressed

    air as process gas, bore holes can be produced meeting all requirements on a guiding assistance for single-lip deep

    hole drilling. Only the roundness deviation is on a higher level than the targeted values.

    3.2. Combination of laser drilling and single lip deep hole drilling

    After the identification of suitable process parameters for laser drilling, the combination of laser and single-lip

    deep hole drilling was done. Therefore, pilot-holes were produced using the laser parameter combinations allowingthe production of bore holes meeting the named requirements. After the production of the pilot-holes, the single-lip

    deep hole drilling process was performed using the same fixture. For the pre-drilling process an adapted strategy

    was necessary. To avoid a deflection of the asymmetric tool when rotating it, the tool was driven into the pilot-hole

    at a low spindle speed of n = 3,000 min-1. The feed motion was stopped at a distance from the base of the pilot-hole

    of s = 0.3 mm. At this position the spindle speed was increased up to n = 25,465 min-1

    which corresponds to a

    cutting speed of vc= 40 m/min and the targeted feed velocity was started. The tool life reached with these cutting

    parameters is comparable to the tool life travel path reached in the single-lip deep hole drilling process using a

    boring bush. Furthermore, the bore hole quality reached in the process combining laser and single-lip deep hole

    drilling is also comparable to the conventional process. This is shown on the example of the surface quality after

    laser drilling and after single-lip deep hole drilling (Figure 8).

    The surface roughness reached by laser pilot drilling amounts to Rz = 1.72 m for the laser parameters used.

    After the drilling experiments, a surface roughness of Rz = 1.43 m was measured in the area where the laser pilot-

    hole was. The single-lip drill smoothed the surface created by laser drilling. This can also be seen in the SEM-views

    presented. In the phase of positioning the deep hole drilling tool into the laser drilled pilot-hole the cutting edge

    corner of the deep hole drilling tool removes surface irregularities coming from the laser drilling process.

    Furthermore, the guide pad of the single-lip deep hole drilling tool smoothened the bore hole surface of the pilot-

    hole at the beginning of the deep hole drilling process. Here, the occurring radial forces are supported by the guide

    pad to the bore hole wall and effects an smoothening of the bore hole surface. The surface roughness reached in the

    area of the pilot-hole corresponds to the value reached in the deep hole drilling process at higher drilling depths. The

    combination of laser drilling and single-lip deep hole drilling has no influence of the surface quality of the bore

    holes produced.

    The work done presents a new technique for the production of deep holes with small diameters. Based on the

    process combination of laser drilling and single-lip deep hole drilling the process specific disadvantages of bothprocess can be eliminated. With this combination, bore holes with a high length-to-diameter ratio can be produced

    by a high accuracy in comparatively short process times. The feasibility of the process combination is presented in

    this work and provides the opportunity for machining workpieces with non-planar faces. Here, a process time

    reduction can be reached in comparison to conventional process chains consisting of a face milling, a pre-drilling

    and a deep hole drilling process. In addition, tool wear can be reduced in machining case-hardened workpieces.

    Here, the laser ablates the hardened material and the mechanical drill only works in the softer material.

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    Dirk Biermann and Markus Heilmann / Physics Procedia 12 (2011) 308316 315

    Figure 8. Comparison of surface quality in laser pre-drilling and single-lip deep hole drilling

    4. Conclusions

    In the investigations carried out a combination of laser pre-drilling and single-lip deep hole drilling with a tool

    diameter of d = 0.5 mm was realized for the very first time. Main requirements on the laser pre-drilling are the

    diameter, the roundness deviation, the surface integrity as well as a low impact on the peripheral zone of the bore

    hole. In comparison to the laser drilling strategies percussion and helical drilling it has been shown, that single-pulselaser drilling is the most applicable strategy for the production of pilot holes under consideration of the experimental

    boundaries used. In single-pulse drilling, the pulse duration and the peak power has shown the highest impact on

    bore hole quality. With an adaption of the laser parameters it is possible to produce bore holes which are suitable for

    the use as a guiding assistance in single-lip deep hole processes. It has been proved that the combination of these

    two processes is comparable to conventional deep hole drilling processes using a boring bush as guiding assistance

    with respect to tool life and bore hole quality.

    In future, the process combination presented will be adapted for machining workpieces with non-planar surfaces

    as well as for machining case-hardened workpieces. In conclusion, the feasibility of the combination of laser pre-

    drilling and single-lip deep hole drilling has been demonstrated in this research. This technique provides the

    opportunities to shorten the process chain of milling, pre-drilling and deep hole drilling in machining components

    with non-planar surfaces as well as to reduce tool wear in machining case-hardened workpieces.

    0.0

    0.1

    0.2

    0.3

    0.4

    0.5

    m

    0.7

    0.0

    0.5

    1.0

    1.5

    2.0

    2.5

    m

    3.5

    Single-pulse laser drillingDeep hole drilling

    Bore hole entrance

    Deep hole drilling

    Bore hole exit

    RoughnessdepthRz

    RoughnessRa

    c = 0.08 mm

    500 m

    Laser: Nd:YAG Tool: Single-lip drill, d = 0.5 mm

    Peak power: P = 8,000 W Cutting speed: vc = 40 m/min

    Pulse duration: = 0,5 ms Feed rate: f = 0.5 m/rev.

    Number of pulses: n = 1 Drilling depth: lt = 12.5 mm

    Focus position: sf = 0 mm Cooling lubricant: Oil

    Process gas: Compr. air Coolant pressure: p = 200 bar Workpiece material: AISI 316L

    Rz

    Ra

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    316 Dirk Biermann and Markus Heilmann / Physics Procedia 12 (2011) 308316

    Acknowledgement

    This work was supported by the German Research Foundation (DFG) under the grant We 1723/78.

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