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  • 8/11/2019 Microwave Drilling with Litz Wire using a Domestic Applicator

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    Bonfring International Journal of Industrial Engineering and Management Science, Vol. 4, No. 3, August 2014 125

    Microwave Drilling with Litz Wire using a

    Domestic ApplicatorNitin K. Lautre, Apurbba K. Sharma, Pradeep Kumar and Shantanu Das

    Abstract ---The work presented in the paper shows a way

    to drill a blind hole on perspex material at 2.45 GHz

    frequency of microwaves using a domestic applicator of 700

    W maximum powers. The approach was based on the

    approach was based on the application of a Litz wire coax as

    a monopole, to act like a drill bit with a heat source. The

    methodology involves no rotary but, single linear movement of

    tool inside a microwave applicator for drilling. A computer

    simulation on COMSOL for about 50 minute each run, was

    also used to show the heat distribution inside microwave

    applicator. The result of computer simulation helped to locate

    the optimized position of Litz wire inside the applicator for

    optimum heat generation. The experimental results show the

    feasibility of microwave drilling and limitations on perspex

    specimen in the used applicator. The work presented involves

    a new approach in the area of microwave drilling of materials

    on a customized domestic microwave setup.

    Keywords--- Applicator, COMSOL, Drilling, Litz,

    Microwave, Perspex

    I. INTRODUCTION

    ICROWAVE energy and drilling process are two

    different popular areas in the field of engineering.

    Microwave concepts are relatively newer to that of drilling.Many of the researchers have tried to overcome the limitation

    of traditional drilling process with the newer emerging

    concepts. Microwave drilling is one such approach presented

    in the year 2000 [1]. The importances of some of applications

    in the area of microwave material processing are rising interms of their popularity and consequently researched [2]. The

    active research areas include microwave assisted sintering,material interaction, modeling, equipment and its design,

    measurements, etc. Most of the research works in microwave

    assisted material processing however are limited to processing

    of ceramics followed by composites.

    Nitin K. Lautre, Research Scholar, Department of Mechanical and

    Industrial Engineering, Indian Institute of Technology, Roorkee, India. E-

    mail:[email protected]

    Dr. Apurbba K. Sharma, Associate Professor, Department of Mechanical

    and Industrial Engineering, Indian Institute of Technology, Roorkee, India. E-

    mail:[email protected]

    Dr. Pradeep Kumar, Professor, Department of Mechanical and Industrial

    Engineering, Indian Institute of Technology, Roorkee, India. E-

    mail:[email protected]

    Shantanu Das, Scientist - H, Reactor and Control Division, Bhabha

    Atomic Research Center, Mumbai, India. E-

    mail:[email protected]

    DOI: 10.9756/BIJIEMS.6053

    Majority of the work reported was confined to

    metallurgical processing of material. However, microwaveassisted mechanical processes received very less attention.

    Some of the developments in the areas of application of

    microwaves for various processes like sintering, cladding,

    melting, coating, glazing, joining, cladding and co-axial cableassisted drilling, etc. are reported [3] [8]. The area of

    microwave drilling on various materials like concrete, glass,

    ceramics, basalts, silicon, and bones are well envisaged and

    explored [9] [12]. The application of bone drilling in

    biomedical engineering, electronics industry and aeronauticalengineering involves the majority of recent drilling

    applications for small size holes [13] [18].

    Researchers have tried to drill hole in perspex of 2.5 mmthick through a 1064 nm diode laser. The power of 1 W

    without decrease in pressure and 2.45 W at a low pressure of

    60 mm Hg of air was used to drill a hole [19]. A carefulcontrol of various parameters like the preparation of precise

    nozzle diameter, its focal point, lens effect, speed of cut,

    cutting power, standoff distance, hole circularity, spatter

    thickness, material removal rate and assists gas pressure

    adjustment add complexity. These controls hinder the drilling

    process for attaining a high aspect ratio holes with low taperratio [20] [22]. An attempt is made to use different

    wavelength the degrade perspex to cause burning, cracking,

    boiling in and around the imposed laser part and nearby. Thewavelength varied from near infrared (1064 nm) to visible

    (532 nm) to ultraviolet ( 266 nm) wavelength. At 266 nm the

    photo chemical dissociation by covalent bond breaking

    (photo-ablation) was more dominating than thermal ablation in

    perspex [23] [24]. A high aspect ratio of 300- 600 for holeranging from 10 100 micron is reported [25] [26]. For

    blind holes a surface modification is prepared by exposing

    perspex to laser beam. The thermochemical damages due tocarbonization of perspex into small spots are reported [27]

    [28]. Conventionally the drilling of perspex establishes the

    significant parameter to be controlled for effective drilled hole

    as the speed, feed rate, thrust force, tool wear, delamination

    [29] [30] and hole shrinkage. A high speed steel drill bit is

    related significantly with power and acoustic emission. Theacoustic emission is unavoidable and is due to assembly of

    mechanically vibrating and rotating system [31]]. Microwave

    drilling makes an attempt to minimize the problem observed inconventional and non conventional (laser) drilling process.

    It has been found that very few researchers are active in

    the domain of microwave drilling at present. The behavior of

    microwave drilling in a closed applicator is infact, highlycomplex as it is governed by various phenomena. Concepts

    like dielectric behavior of material in high temperature, hot

    spot formation, thermal runaway as well as safety

    M

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    Bo fring Internation l Journal of Industrial Engineering

    co

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    ERIMENTAL S

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    figure 1, was

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    ETUP AND CUS

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    to the speci. The specime

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    e Basic Appli

    and Management

    ISSN 2277

    Science, Vol. 4, o. 3, August 201 126

    ents in the fi

    mostly depebit and ambi

    -

    ss of microwthaacrylate)

    so highlights

    or for the proc

    e to simulatedrilling in

    TOMIZATION

    model: HR-1

    rilling trials. I

    of cooking f

    a hole of 12on, the hole

    applicator.

    00 W whichptible time ins

    ep of 1 minut

    h a cylindri

    sed to coverangement of

    the entry of

    e applicatoruter diameter

    ter copper str

    the cylindri

    a monopole t

    he length of c

    avelength (/ntered monop

    crowave sou

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    endicular to

    isc was remoe target mate

    as placed ins

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    g brick. Th

    ting platform

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    5056 | 2014 Bo

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    Figure 3:

    etron

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    seded glass inrability and le

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    Spectroscopy

    n figure 4. Th

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    MMA Work

    heet

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    pplicator with

    ustomized ap

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    ing point of a

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    aerospace an

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    spectrum o

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    iece Specime

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    Coax Cable

    plicator are

    e reflective

    ent material.

    the incidentskin depth

    due to theting air film

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    in figure 3.

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    Coax

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    waveguide

    n

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    Bonfring International Journal of Industrial Engineering and Management Science, Vol. 4, No. 3, August 2014 127

    Figure 4: EDS Spectrum of PMMA Specimen

    The drill bit chosen for the experimentation was a coax

    cable with twisted strands of copper wire commonly known asLitz wire as shown in figure 5(a). These wires are commonly

    used for carrying AC (Alternating Current) at low frequency

    upto 1 MHz. It has a group of seven copper wire strands eachof diameter 0.6 mm. After winding of these individual

    wires, the diameter of the drill bit tool was maintained at 2.1

    mm.

    The diameter of individual wire was so selected to reducethe skin effect as its effectiveness increases if wire diameter is

    less than the twice the skin depth. For copper at 2.45 GHz, the

    skin depth is 1.35 m. A copper wire of 2.7 m will be very

    thin and less stiff to act as a drill bit. The Litz wire used was

    of Suhner make, RG 213/U, 50 ohm as shown in figure 5(b).

    The bunch of wounded wire of 2.1 mm was surrounded by adielectric material shield of 7.3 mm. This diameter ( 7.3

    mm) was less than the top hole drilled 12 mm, which allows

    the monopole of group of wire to enter along with dielectriccover inside the applicator. The dielectric cover was further

    surrounded by criss cross woven thin copper straps as shown

    in figure 5(a), which are finally covered by a protective plastic

    cover.

    Figure 5: (a) Coax litz wire (b) Specification on Coax Cable

    The criss cross or basket weaved copper straps donot keep

    two straps or wire parallel to each other causing cancellation

    of wire magnetic field between successive twists. Also, at

    higher frequencies more and more signals are transferred in

    the outermost layer of the coax becomes effective. The finalouter diameter after the plastic cover for the coax was 10.26

    mm. Since the arrangement was of monopole entry the copper

    straps are spread to increase the overall diameter beyond 12mm to restrict the entry of copper strap and outer protective

    cover inside the applicator.

    The cross section of the Litz wire has typically arranged

    wire relative to each other as shown in figure 6. The wire iswound in such a way that they form a hexagonal honeycomb

    shape grid with central wire inside the grid. This arrangement

    has the capability to induce eddy current on the nearby wire,

    and hence improves the current flow over the Litz wire. Since

    the wire cross sections is circular and twisted over each otherand are equally spaced wire, it leads to six void patches as

    shown in figure 6. These voids are acting as insulator and are

    unavoidable.

    Figure 6: Cross section of Litz wire

    III. COMSOLSIMULATION

    The experimentation for microwave irradiation requires an

    idea of the temperature distribution inside the applicator

    without the presence of stirrer and rotary plate. A simulationtool (COMSOL of 4.3 version 0.151) was used to simulate the

    temperature profile for effectively positioning the workpiece

    and drill bit in the applicator. The geometrical model with

    exact size of the microwave cavity is shown in figure 7. Thedimensions of the applicator used are 285 X 277 X 182 (L X B

    X H) mm. The grids of predrilled hole on either side of

    vertical face was ignored in simulation, as theses holes are to

    release the gases trapped in the cavity through forcedconvection.

    2.1 mm

    0.6 mm

    (a)(b)

    Wire bunch,

    2.1 mm

    Copper straps

    Dielectric

    cover,7.3 mm

    Outer plastic,

    10.26 mm

    cover

    void

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    Bonfring International Journal of Industrial Engineering and Management Science, Vol. 4, No. 3, August 2014 128

    Figure 7: Geometrical Model of the Experimental Setup

    A frequency transient study was performed at power ratingof 700 W with power application cycle time of less than 3

    minute. In order to estimate the variation of heat in theapplicator, a series of simulation runs were performed for

    microwave heating. Each run inside the microwave oven

    module was iterating and converging for a cycle time of about50 minute. The other parameters selected during simulation

    were model definition of air, no heat transfer, port boundary,

    meet boundaries to respective domains.

    The variation of electric field and resistive losses as

    obtained through simulation are shown in figure 8(a). It is

    clear from the figure that throughout the irradiation trial, the

    tool and the workpiece will be within the safe limit and theheat variations are cyclic. It was also seen that the higher

    heating envelope was away from the center of the applicator.

    As pointed out, the temperature distributions are more uniformaway from the center axis of the cavity [32]. The overheatingof the coax was thus not possible for low exposure time (30 s).

    The resistive heating in W/m3was more around the brick asshown in figure 8(b). The smaller size of specimen also helps

    the working atmosphere to be maintained at lower initial

    temperature variation without interfering the resistive heating

    area.

    Figure 8: Variation in (a) Electric Field and (b) Resistive

    Losses in Microwave Applicator

    In order to find out the optimum coordinates for effectivemicrowave heating inside the applicator, Table 1 has been

    constructed from the simulation results. The temperature

    variation of three times the melting point of PMMA was

    assumed from the center to around the brick. It is concluded

    from the data that for the application of less than 480 OC (~

    160 * 3 times) temperature near the drilling zone, the ideal

    location for the drill bit will be about the center, as it will notinterfere the high electric field generated around the brick

    area.

    Since the top face drilled hole may not permit any x-ychange; the data of z-axis along the drill bit height was

    effective. The z axis data help to allow a particular length ofcoax inside the applicator for optimized heat concentration for

    drilling. The optimum entry distance for the drill bit was H -142 mm = 40 mm as shown in figure 9. The condition of Litz

    wire become sensitive, if the entry distance of about 40 mm

    was not maintained. A burnout was observed due to sudden

    rise in temperature at coax in 2 minute, as shown in figure 10.The burnout had not only burnt the start portion of drill bit but,

    also melted the dielectric cover over it. This clears the

    temperature range generated at drill bit end in the microwave

    applicator. A need of research for good and tolerable dielectric

    cover to withstand such elevated temperature is considerableto prevent the dielectric cover burn outs.

    Table 1: Variation of Temperature with Coordinated ofApplicator

    x y z Temp (OC)

    0.1079 0.1472 0.14146 438.1342

    0.09441 0.09193 0.14214 643.2254

    0.25801 0.1199 0.14247 741.0294

    0.255 0.11098 0.14276 827.4488

    0.06919 0.053 0.14277 832.0689

    0.08321 0.13952 0.14283 850.6143

    0.08078 0.06883 0.14285 856.7601

    Figure 9: Optimized Entry of the Drill Bit from Top

    Figure 10: Burnt Litz Wire

    B

    coax

    Magnetron

    PMMA

    L

    H

    Brick

    Resistive

    heatinElectric

    field

    variation

    (a) (b)

    40 mm

    H

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    BoBo fring Internation l Journal of Industrial Engineering

    to

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    figure 11.

    igure 11: Drill

    It was observ

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    A scanning edrilled PMM

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    terial coming

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    e drill does n

    terial to a part

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    hole

    . RESULT

    re performed

    ole. The exper

    does not in and circulati

    ece platform

    through simue the brick

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    as manually

    e of about 2

    le was drilled

    ed Hole on P

    ed that the hol

    tz wire (figu

    e (HAZ) arofication the H

    as measured t

    and the HAZ

    which gets eof drill into P

    oax in PMM

    mm of blind h

    ectron MicrosA specimen i

    section of Li

    uated porousr hot conditi

    out from the

    at the top sue Litz wire a

    t have any ca

    icular directio

    re 12: HAZ o

    HAZ

    AND DISCUSS

    s per the sim

    imentation wa

    olved compleng motor. Pri

    was adjusted

    lation. The Pnd beneath t

    then insertedonopole. Th

    controlled. It

    o 3 minute at

    on PMMA sp

    MA Specime

    e was exact re

    e 6). In addit

    nd the hole wZ are shown

    o about 0.8 m

    was generall

    acuated by mMMA specim

    specimen w

    ole as shown i

    cope (SEM) ishown in fig

    tz wire was ea

    aterial due ton was also s

    specimen ma

    rface with sipd the wall of

    vity or gap to

    .

    PMMA Spec

    HA

    and Management

    ISSN 2277-

    ION

    lated parame

    s performed

    waveguider to starting

    to the optimi

    MA workpie circular w

    in the circaxial movemas observed t

    700 W maxim

    ecimen as sho

    with Litz Wi

    plica of the cr

    on to the hol

    as also observin figure 12;

    thick. The a

    occupied by

    icrowave heaten. The depth

    as measured

    n figure 13.

    age obtainedre 14. The tr

    sily visible in

    drill penetrateen. The por

    y be having l

    hon action atthe drilled h

    direct the por

    imen

    Science, Vol. 4, o. 3, August 201 129

    ers

    ith

    ndthe

    ed

    eceve

    larenthat

    um

    wn

    5056 | 2014 Bo

    re

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    show tweight

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    nfring

    Figure 13:

    14: SEM Ima

    EDS spectra

    ole were also

    d that the co (reference:

    . The weight

    o be 59.3 % aal changes at

    tion. In additi

    re observed

    with atom

    vely. This clprocess tool

    ticle lost by

    d of the wor

    e presence opercentage of

    by 5.86 % a

    and zinc parti

    Penetration D

    ge of Drilled

    analysis of

    attempted as

    position of tfigure 4) aft

    percentages o

    nd 19.06 %.higher tempe

    on to these a

    with weight p

    c percentage

    ars the fact t(Litz wire) h

    he tool was f

    piece; further

    traces of copcarbon and ox

    nd 15.78 % r

    les of the drill

    Depth of

    lind hole

    epth of Drill B

    ole on PMM

    he bottom su

    hown in figu

    e PMMA gor the micro

    carbon and

    he change isature during

    small traces o

    ercentage of

    of 2.38 %

    at during thas also experi

    rther accumu

    analysis of th

    per and zincygen in the bl

    espectively, to

    bit.

    it

    Specimen

    rface of the

    e 15. It was

    t marginallyave drilling

    xygen were

    ndicative ofmelting and

    copper and

    9.77 % and

    nd 2.81 %

    microwaveenced wear.

    lated on the

    ese particles

    lement. Thend hole was

    accumulate

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    Bonfring International Journal of Industrial Engineering and Management Science, Vol. 4, No. 3, August 2014 131

    ISSN 2277-5056 | 2014 Bonfring

    [30] A. Faraz and D. Biermann, "Subsequent Drilling on Pilot Holes inWoven Carbon Fibre Reinforced Plastic Epoxy Laminates: The Effect of

    Drill Chisel Edge on Delamination", Proceedings of the Institution of

    Mechanical Engineers, Part B: Journal of Engineering Manufacture, pp.

    1493 1504, 2011.

    [31] S. Arul, L. Vijayaraghavan and S. K. Malhotra, "Online Monitoring ofAcoustic Emission for Quality Control in Drilling of Polymeric

    Composites", Journal of Materials Processing Technology, vol. 185, pp.

    184 190, 2007.

    [32] K. Pitchai, S. L. Birla, J. Subbiah and D. D. Jones, HeatingPerformance Assesment of Domestic Microwave Ovens, International

    Microwave Power Institutes 44th Annual Symposium, pp. 1-7, 2010.Nitin K. Lautre is working as a Research Scholar in

    the department of Mechanical and Industrial

    Engineering, Indian Institute of Technology, Roorkee,India. He obtained his graduate and post-graduate

    degree in Mechanical and Industrial engineering

    respectively from Nagpur University. He has an

    industrial experience of about 01 year seven month inone of the Bharat Ratna defence company. He has a

    teaching experience of about 12 years and handled

    various student projects. He is member of various societies and presented

    paper in Japan and USA. He has in his credit about 30 conference and six

    journal papers. His research interest is Non-conventional machining andhybrid machining processes.

    Dr. Apurbba K. Sharma, currently working as

    Associate Professor in the Department of Mechanicaland Industrial Engineering at the Indian Institute of

    Technology Roorkee, India. He obtained his Bachelor'sDegree in Mechanical Engineering from Dibrugarh

    University and Master's and Doctoral Degrees from

    Indian Institute of Technology Madras, India. He has

    guided five Ph.D students and currently supervising sixdoctoral theses. He has published more than 55 articles

    in journals and 67 articles in international conferences. He is a reviewer to

    various international journals. He holds one Indian Patent to his credit and has

    filed four more recently. Currently, he is Principal Investigator for three

    externally funded projects.

    Dr. Pradeep Kumar is working as a Professor in the

    Department of Mechanical and Industrial Engineering

    at Indian Institute of Technology Roorkee, (formerly

    University of Roorkee), India. He earned his BS inIndustrial Engineering in 1982, his MS in Production

    Engineering in 1989 and his PhD in 1994, all from the

    University of Roorkee, Roorkee, India. He has also

    served DRF Industries and the Steel Authority of India

    Ltd as a Production Engineer for four years. Hisresearch interests include quality engineering, reliability analysis, product and

    process design, optimization, non-conventional machining processes, and

    metal casting. He has published 55 papers in national and international

    journals and conference proceedings. He has supervised 25 Ph.D theses, 82M.Tech dissertations and several Graduate theses. He was honored as

    outstanding teacher in the year 2005 and 2009. He completed 9 sponsored

    projects and currently working on 8 research projects. He also holds various

    administrative post and membership of various esteemed societies.

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