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Non-Traditional Machining




          ME 338: Manufacturing Processes II
        Instructor: Ramesh Singh; Notes: Profs.   1
                  Singh/Melkote/Colton
Introduction
• Machining is a broad term to describe
  removal of material from a workpiece.
• Machining categories:
  – Cutting involves single-point or multipoint cutting
    tools, each with a clearly defined geometry.
  – Abrasive processes, such as grinding.
  – Nontraditional machining, utilizing electrical,
    chemical, and optical sources of energy.



                       ME 338: Manufacturing Processes II
                     Instructor: Ramesh Singh; Notes: Profs.   2
                               Singh/Melkote/Colton
Nontraditional Machining
• Ultrasonic Machining (USM)
• Water-Jet Machining & Abrasive-Jet
  Machining
• Chemical Machining
• Electrochemical Machining (ECM)
• Electrical-Discharge Machining (EDM)
• High-Energy-Beam Machining
  – Laser-beam machining (LBM)
  – Electron-beam machining (EBM)



                ME 338: Manufacturing Processes II
              Instructor: Ramesh Singh; Notes: Profs.   3
                        Singh/Melkote/Colton
Traditional vs. Nontraditional
• Primary source of energy
   – Traditional: mechanical.
   – Nontraditional: electrical, chemical, optical
• Primary method of material removal
   – Traditional: shearing
   – Nontraditional: does not use shearing
     (e.g., abrasive water jet cutting uses
     erosion)                                                         Water jet machining




                                                                               Grinding

     2D cutting process
                              ME 338: Manufacturing Processes II
                            Instructor: Ramesh Singh; Notes: Profs.                         4
                                      Singh/Melkote/Colton
Why Nontraditional Machining?
• Situations where traditional machining processes are
  unsatisfactory or uneconomical:
   – Workpiece material is too hard, strong, or tough.
   – Workpiece is too flexible to resist cutting forces or too difficult
     to clamp.
   – Part shape is very complex with internal or external profiles
     or small holes.
   – Requirements for surface finish and tolerances are very high.
   – Temperature rise or residual stresses are undesirable or
     unacceptable.




                            ME 338: Manufacturing Processes II
                          Instructor: Ramesh Singh; Notes: Profs.          5
                                    Singh/Melkote/Colton
Ultrasonic Machining (USM)
• Process description
   – The tool, which is negative of the
     workpiece, is vibrated at low
     amplitude (0.013 to 0.08 mm) and
     high frequency (about 20 kHz) in an
     abrasive grit slurry at the workpiece
     surface.
   – The slurry also carries away the
     debris from the cutting area.
   – The tool is gradually moved down
     maintaining a constant gap of
     approximately 0.1 mm between the
     tool and workpiece surface.


                              ME 338: Manufacturing Processes II
                            Instructor: Ramesh Singh; Notes: Profs.   6
                                      Singh/Melkote/Colton
USM (Cont.)
• Cracks are generated due to the high stresses produced
  by particles striking a surface.
• The time of contact between the particle and the surface
  is given by:
                   1/ 5
      5r  c 0 
  t0 ≈                  (10 − 100 µ s )                   Force of a particle on surface:
      c0  v 
                                                                  F = d (mv) / dt
r: radius of a spherical particle
c0: workpiece elastic wave velocity = E / ρ                   Average force of a particle
                                                              striking the surface:
v: velocity of particle striking surface
                                                                   Fave = 2mv / t 0

                                    ME 338: Manufacturing Processes II
                                  Instructor: Ramesh Singh; Notes: Profs.               7
                                            Singh/Melkote/Colton
USM (Cont.)
• Example: Explain what change, if any, takes place in the
  magnitude of the impact force of a particle in ultrasonic
  machining as the temperature of the workpiece is
  increased.
  Solution:
                Here, m and v are constant.
                                1/ 5
                   5r  c 0                      1            1
               t0 =                  ⇒ t0 ∝             ∝
                   c0  v                      c04 / 5       E 2/5

         When temperature increases, E decreases
         and t0 increases. Hence, F decreases.

                           ME 338: Manufacturing Processes II
                         Instructor: Ramesh Singh; Notes: Profs.      8
                                   Singh/Melkote/Colton
USM (Cont.)
               Assuming hemispherical brittle fracture


                                                                             3
                                                                  2π  D 
                                                             V=       
                                                                   3 2
                                                             D ≈ 2 dh
                                                                  2π
                                                             V=      (dh) 3 / 2
                                                                   3
MRR = ηV Z f
where V = volume removed by a single grain
       f = frequency of operation
      Z = number of particles impacting per cycle
      η = efficiency

                     ME 338: Manufacturing Processes II
                   Instructor: Ramesh Singh; Notes: Profs.                       9
                             Singh/Melkote/Colton
USM (Cont.)
• Applications
   – USM is best suited for hard, brittle materials, such as ceramics,
     carbides, glass, precious stones, and hardened steels. (Why?)

• Capability
   – With fine abrasives, tolerance of 0.0125 mm or better can be held.
     Ra varies between 0.2 – 1.6 µm.

• Pros & Cons:
   – Pros: precise machining of brittle materials; makes tiny holes (0.3
     mm); does not produce electric, thermal, chemical damage
     because it removes material mechanically.
   – Cons: low material removal rate (typically 0.8 cm3/min); tool wears
     rapidly; machining area and depth are limited.


                             ME 338: Manufacturing Processes II
                           Instructor: Ramesh Singh; Notes: Profs.       10
                                     Singh/Melkote/Colton
USM Parts



Ceramic




     ME 338: Manufacturing Processes II
   Instructor: Ramesh Singh; Notes: Profs.   11
             Singh/Melkote/Colton
Water-Jet Machining (WJM)
                                                           also called hydrodynamic machining




WJM is a form of micro erosion. It          The extreme pressure of the accelerated
works by forcing a large volume of          water particles contacts a small area of the
water through a small orifice in the        workpiece and acts like a saw and cuts a
nozzle.                                     narrow groove in the material.
                   http://www.flowcorp.com/waterjet-resources.cfm?id=360
                                     ME 338: Manufacturing Processes II
                                   Instructor: Ramesh Singh; Notes: Profs.             12
                                             Singh/Melkote/Colton
WJM (Cont.)
• Pros: no need for predrilled holes, no heat, no workpiece
  deflection (hence suitable for flexible materials), minimal
  burr, environmentally friendly.
• Cons: limited to material with naturally occurring small
  cracks or softer material.
• Applications:
   – Mostly used to cut lower strength materials such as wood,
     plastics, rubber, paper, leather, composite, etc.
   – Food preparation
   – Good for materials that cannot withstand high temperatures of
     other methods for stress distortion or metallurgical reasons.



                            ME 338: Manufacturing Processes II
                          Instructor: Ramesh Singh; Notes: Profs.    13
                                    Singh/Melkote/Colton
WJM Examples




                                     PWB (printed wire board)

     ME 338: Manufacturing Processes II
   Instructor: Ramesh Singh; Notes: Profs.                 14
             Singh/Melkote/Colton
Abrasive Water-Jet Machining
            (AWJM)
The water jet contains
abrasive particles such as
silicon carbide, thus
increasing MRR.
Metallic materials can be
cut. Particularly suitable for
heat-sensitive materials.




                            ME 338: Manufacturing Processes II
                          Instructor: Ramesh Singh; Notes: Profs.   15
                                    Singh/Melkote/Colton
AWJM Parts


                                                     Bullet Proof Glass Part




Steel rack (75 mm thick)

                                                                     Ceramic Part


                                                                     Source: http://www.waterjets.org/

                             ME 338: Manufacturing Processes II
                           Instructor: Ramesh Singh; Notes: Profs.                             16
                                     Singh/Melkote/Colton
Abrasive-Jet Machining (AJM)




A high-velocity jet of dry air,             The gas supply pressure is on
nitrogen, or carbon dioxide                 the order of 850 kPa (125 psi)
containing abrasive particles is            and the jet velocity can be as
aimed at the workpiece surface              high as 300 m/s and is
under controlled conditions.                controlled by a valve.

                            ME 338: Manufacturing Processes II
                          Instructor: Ramesh Singh; Notes: Profs.            17
                                    Singh/Melkote/Colton
AJM Process Capability
• Material removal
  – Typical cutting speeds vary between 25 -125 mm/min

• Dimensional Tolerances
  – Typical range ±2 - ±5 µm

• Surface Finish
  – Typical Ra values vary from 0.3 - 2.3 µm



                       ME 338: Manufacturing Processes II
                     Instructor: Ramesh Singh; Notes: Profs.   18
                               Singh/Melkote/Colton
AJM Applications & Limitations
• Applications
   – Can cut traditionally hard to cut materials, e.g., composites,
     ceramics, glass
   – Good for materials that cannot stand high temperatures


• Limitations
   – Expensive process
   – Flaring can become large
   – Not suitable for mass production because of high
     maintenance requirements



                           ME 338: Manufacturing Processes II
                         Instructor: Ramesh Singh; Notes: Profs.      19
                                   Singh/Melkote/Colton
Chemical Machining (CM)
• Chemical machining, basically an etching process, is the oldest
  nontraditional machining process.
• Material is removed from a surface by chemical dissolution using
  chemical reagents, or etchants, such as acids and alkaline
  solutions.
• The workpiece is immersed in a bath containing an etchant. The
  area that are not required to be etched are masked with “cut and
  peel” tapes, paints, or polymeric materials.
• In chemical milling, shallow cavities are produced on plates,
  sheets, forgings, and extrusions for overall reduction of weight
  (e.g., in aerospace industry). Depths of removal can be as much as
  12 mm.




                             ME 338: Manufacturing Processes II
                           Instructor: Ramesh Singh; Notes: Profs.     20
                                     Singh/Melkote/Colton
CM (Cont.)
• Chemical blanking is used to produce features which
  penetrate through the material via chemical dissolution.
  The metal that is to be blanked is
   – thoroughly cleaned with solvents.
   – coated and the image of the part is imprinted.
   – soaked in a solvent that removes the coating, except in the
     protected areas.
   – spray etched to dissolve the unprotected areas and leave the
     finished part.




                            ME 338: Manufacturing Processes II
                          Instructor: Ramesh Singh; Notes: Profs.   21
                                    Singh/Melkote/Colton
CM (Cont.)
• Typical applications
   – Chemical blanking: burr-free
     etching of printed-circuit boards
     (PCB), decorative panels, thin
     sheet-metal stampings, and the
     production of complex or small
     shapes.
   – Chemical milling: weight
     reduction of space launch
     vehicles.

         Pros: low setup, maintenance, and tooling costs; small,
         delicate parts can be machined; suitable for low production
         runs on intricate designs.
         Cons: slow (0.025-0.1 mm/min); surface defects; chemicals
         can be extremely dangerous to health.
                               ME 338: Manufacturing Processes II
                             Instructor: Ramesh Singh; Notes: Profs.   22
                                       Singh/Melkote/Colton
Electrochemical Machining (ECM)
                 • Process description:
                       – In ECM, a dc voltage (10-25 v) is
                         applied across the gap between a
                         pre-shaped cathode tool and an
                         anode workpiece. The workpiece
                         is dissolved by an
                         electrochemical reaction to the
                         shape of the tool.
                       – The electrolyte flows at high
                         speed (10-60 m/s) through the
                         gap (0.1-0.6 mm) to dissipate
                         heat and wash away the
                         dissolved metal.

             ME 338: Manufacturing Processes II
           Instructor: Ramesh Singh; Notes: Profs.       23
                     Singh/Melkote/Colton
ECM (Cont.)
• The material removal rate by ECM is given by:

                       MRR = C I η
where, MRR=mm3/min, I=current in amperes,
      η=current efficiency, which typically ranges from 90-100%,
      C is a material constant in mm3/A·min.


   Feed rate (mm/min):         f = MRR / A0
               Assuming a cavity with uniform cross-sectional area A0

                             ME 338: Manufacturing Processes II
                           Instructor: Ramesh Singh; Notes: Profs.   24
                                     Singh/Melkote/Colton
ECM (Cont.)
• Pros: high shape complexity
  possible, high MRR possible, high-
  strength materials, mirror surface
  finish possible.

• Cons: workpiece must be
  electrically conductive; very high
  tooling (dedicated) and equipment
  costs; high power consumption.

• Applications: complex cavities in
  high-strength materials, esp. in
  aerospace industry for mass
  production of turbine blades.


                               ME 338: Manufacturing Processes II
                             Instructor: Ramesh Singh; Notes: Profs.   25
                                       Singh/Melkote/Colton
EDM-History




    ME 338: Manufacturing Processes II
  Instructor: Ramesh Singh; Notes: Profs.   26
            Singh/Melkote/Colton
Electrical Discharge Machining
                 (EDM)
                                                  EDM is a thermal erosion
                                                  process whereby material
                                                  is melted and vaporized
                                                  from an electrically
                                                  conducive workpiece
                                                  immersed in a liquid
                                                  dielectric with a series of
                                                  spark discharges between
                                                  the tool electrode and the
                                                  workpiece created by a
                                                  power supply.
EDM is one of the most accurate
while quite affordable mfg process.

                             ME 338: Manufacturing Processes II
                           Instructor: Ramesh Singh; Notes: Profs.              27
                                     Singh/Melkote/Colton
EDM (Cont.)
The EDM system consists
of a shaped tool or wire
electrode, and the part. The
part is connected to a
power supply to create a
potential difference between
the workpiece and the tool.
When the potential
difference is sufficiently
high, a transient spark               The dielectric fluid 1) acts as an
discharges through the                insulator until the potential is
fluid, removing a very small          sufficiently high, 2) acts as a
amount of metal from the              flushing medium, and 3) provides
workpiece.                            a cooling medium.

                                 ME 338: Manufacturing Processes II
                               Instructor: Ramesh Singh; Notes: Profs.     28
                                         Singh/Melkote/Colton
Process-Basics




     ME 338: Manufacturing Processes II
   Instructor: Ramesh Singh; Notes: Profs.   29
             Singh/Melkote/Colton
EDM (Cont.)
 MRR is basically a function of the current and the melting point of
 the workpiece material. An approximate empirical relationship is:
                           4    −1.23        MRR=mm3/min
       MRR = 4 × 10 I T        w
                                             I=current in amperes
                                             Tw=melting point of workpiece (ºC)
Wear rate of electrode:

Wt = 11× 10 3 I Tt −2.38                               Wear ratio of workpiece
                                                       to electrode:
Wt=mm3/min
Tt=melting point of electrode material (ºC)                 R = 2.25 Tr−2.3
                                                         Tr=ratio of workpiece to
                                                         electrode melting points (ºC)
                                 ME 338: Manufacturing Processes II
                               Instructor: Ramesh Singh; Notes: Profs.                   30
                                         Singh/Melkote/Colton
MRR - EDM

                                                     Metal removal is function of pulse energy
  • Experimental Approach
                                                      and frequency:
                                                     h = K1Wn
               TOOL
                (-)                                  D= K2Wn
                                                     where W        = Pulse energy, J




                                        DC VOLTAGE
                                                              h     = height of crater, mm
                                                              D     = diameter of crater, mm
                                                              K1, K2 = constants depending
                           h                                           on electrode materials
                D                                                      and dielectric
                                                              n      = constant depending on
             WORKPIECE                                                 work tool combination
                (+)                                  The crater volume from geometry,
                                                                 π 3          
     Scheme of Crater Formation                              Vc = h D 2 + h 2 
                                                                  6 4         
         MRR = Vc f η                                   π 3 2        2  3n
where f = frequency of operation and η = efficiency Vc = K1  K 2 + K1 W
                                                        6 4           

                                    ME 338: Manufacturing Processes II
                                  Instructor: Ramesh Singh; Notes: Profs.                 31
                                            Singh/Melkote/Colton
Volume of the crater




        ME 338: Manufacturing Processes II
      Instructor: Ramesh Singh; Notes: Profs.   32
                Singh/Melkote/Colton
EDM Process Capability
• MRR
   – Range from 2 to 400 mm3/min. High rates produce rough finish,
     having a molten and recast structure with poor surface integrity
     and low fatigue properties.
• Dimensional Tolerances
   – Function of the material being processed
   – Typically between ±0.005 - ±0.125 mm
• Surface Finish
   – Depends on current density and material being machined
   – Ra varies from 0.05 – 12.5 µm
   – New techniques use an oscillating electrode, providing very fine
     surface finishes.


                            ME 338: Manufacturing Processes II
                          Instructor: Ramesh Singh; Notes: Profs.       33
                                    Singh/Melkote/Colton
EDM Applications
Widely used in aerospace, moldmaking, and die casting to produce die
cavities, small deep holes, narrow slots, turbine blades, and intricate shapes.




  Cavities produced by EDM                                  Stepped cavities

                                ME 338: Manufacturing Processes II
                              Instructor: Ramesh Singh; Notes: Profs.          34
                                        Singh/Melkote/Colton
EDM Limitations
• Limitations
  – A hard skin, or recast layer is produced which may be
    undesirable in some cases.
  – Beneath the recast layer is a heat affected zone which
    may be softer than parent material.
  – Finishing cuts are needed at low MRR.
  – Produces slightly tapered holes, specially if blind.




                       ME 338: Manufacturing Processes II
                     Instructor: Ramesh Singh; Notes: Profs.   35
                               Singh/Melkote/Colton
Wire EDM




A wire travels along a prescribed path,
cutting the workpiece, with the discharge
sparks acting like cutting teeth.

                          ME 338: Manufacturing Processes II
                        Instructor: Ramesh Singh; Notes: Profs.   36
                                  Singh/Melkote/Colton
Wire EDM (Cont.)
   MRR in Wire EDM

   MRR = V f h b


    where, b = d w + 2s

MRR = mm3/min
Vf = feed rate of wire into the
workpiece in mm/min
h = workpiece thickness or           dw = wire diameter in mm
height in mm                         s = gap between wire and workpiece in mm

                                    ME 338: Manufacturing Processes II
                                  Instructor: Ramesh Singh; Notes: Profs.       37
                                            Singh/Melkote/Colton
Wire EDM Parts




      ME 338: Manufacturing Processes II
    Instructor: Ramesh Singh; Notes: Profs.   38
              Singh/Melkote/Colton
Example
• Example: You have to machine the following part from a
  85mmx75mmx20mm steel block. You have to choose
  between EDM and Conventional machining. Your
  objective is to minimize the cutting power required, which
  process will you choose?
                                                                                       12.5

Assumptions:
   – EDM process:
                                                                                       40
      • Wire diameter: dw=0.2 mm
      • Gap: s=0.1 mm
   – Conventional machining:                                                           10
      • Negative of the part has to be                                                 12.5
        removed
                                                     12.5   20        20   20   12.5
                              ME 338: Manufacturing Processes II
                            Instructor: Ramesh Singh; Notes: Profs.                     39
                                      Singh/Melkote/Colton
Example
Solution:
- EDM process
   VEDM = lc*(dw+2s)*t = 1440 mm3
- Conventional machining
   VM= Vtotal – Vpart = 99500 mm3
- Power comparison
                                     u M VM u EDM VEDM
   We will choose machining if             ≤
                                       tM       t EDM
   let’s assume tEDM=αtM
                            u EDM VEDM
   then machining if α ≤
                                    u M VM
                        ME 338: Manufacturing Processes II
                      Instructor: Ramesh Singh; Notes: Profs.   40
                                Singh/Melkote/Colton
Reverse micro-EDM
• Fabrication of high aspect ratio micro-electrode arrays




• Potential application in machining hole arrays via micro-
  EDM/ECM


                         ME 338: Manufacturing Processes II
                       Instructor: Ramesh Singh; Notes: Profs.   41
                                 Singh/Melkote/Colton
Arrays Fabricated via R µ-EDM @IITB




     6x6 array                                   4x4 array
               ME 338: Manufacturing Processes II
             Instructor: Ramesh Singh; Notes: Profs.         42
                       Singh/Melkote/Colton
Experimental Setup




       ME 338: Manufacturing Processes II
     Instructor: Ramesh Singh; Notes: Profs.   43
               Singh/Melkote/Colton
Fabricated Texture




      ME 338: Manufacturing Processes II
    Instructor: Ramesh Singh; Notes: Profs.   44
              Singh/Melkote/Colton
High-Energy-Beam Machining

  • Laser-Beam Machining (LBM)

  • Electron-Beam Machining (EBM)

  • Focused Ion-Beam Machining


              ME 338: Manufacturing Processes II
            Instructor: Ramesh Singh; Notes: Profs.   45
                      Singh/Melkote/Colton
Laser-Beam Machining (LBM)
• Laser Concept
  – Add energy to make electrons “jump” to higher energy orbit
  – Electron “relaxes” and moves to equilibrium at ground-state
    energy level
  – Emits a photon in this process (key laser component)
  – Two mirrors reflect the photons back and forth and “excite” more
    electrons
  – One mirror is partially reflective to allow some light to pass
    through: creates narrow laser beam




                           ME 338: Manufacturing Processes II
                         Instructor: Ramesh Singh; Notes: Profs.   46
                                   Singh/Melkote/Colton
LBM (Cont.)
            Excited
            State

Electron                  Ground
                          State                                        Photon




                                   Nucleus


                          Orbits

       Electron is                                 Electron relaxes
       energized to the                            to ground state
       excited state                               and photon is
                                                   produced

              Photon Emission Model
                               ME 338: Manufacturing Processes II
                             Instructor: Ramesh Singh; Notes: Profs.            47
                                       Singh/Melkote/Colton
LBM (Cont.)
• More precise
• Useful with a variety of
  materials: metals,
  composites, plastics,
  and ceramics
• Smooth, clean cuts
• Faster process
• Decreased heat-
  affected zone


                         ME 338: Manufacturing Processes II
                       Instructor: Ramesh Singh; Notes: Profs.   48
                                 Singh/Melkote/Colton
Schematic of LBM Device




          ME 338: Manufacturing Processes II
        Instructor: Ramesh Singh; Notes: Profs.   49
                  Singh/Melkote/Colton
Laser Setup
• Laser Processing Center
   – 100 W SPI single mode fiber laser (Power and frequency modulated)
   – Optics for variable intensity distribution and spot size
   – 3 axis (Z decoupled) translational stages and controls




                                                   “Method and device for generating laser
   – Provides uniform/Gaussian intensity            beam of variable intensity distribution
   – 7 µm -900 µm spot size possible                      and variable spot size”,
   – Hardening/Cladding/Texturing/Brazing              Indian Patent Application No.
                                                              442/MUM/2011.
                              Machine Tools Laboratory
                               Micromachining Cell
LBM (Cont.)
• Important physical parameters in LBM
   – Reflectivity
   – Thermal conductivity of workpiece surface
   – Specific heat and latent heats of melting and evaporation
• The lower these quantities, the more efficient the
  process.

• The cutting depth t:            t = P / vd
                     P is the power input, v is the cutting speed,
                     and d is the laser-beam-spot diameter.



                             ME 338: Manufacturing Processes II
                           Instructor: Ramesh Singh; Notes: Profs.   51
                                     Singh/Melkote/Colton
Heat Source Modeling
• Solution for stationary point using Green’s Theorem:
     The differential equation for the conduction of heat in a
     stationary medium assuming no convection or radiation, is

      This is satisfied by the solution for infinite body,
                                      δq                           ( x − x ') 2 + ( y − y ') 2 + ( z − z ') 2
      dT '( x, y, z, t ) =                            3
                                                          ex p [ −                                            ]
                                                                                  4 a ( t − t ')
                             ρ C (4 π a ( t − t '))   2


      sem i − in f in ite
                                      2δ q                         ( x − x ') 2 + ( y − y ') 2 + ( z − z ') 2
      dT '( x, y, z, t ) =                            3
                                                          ex p [ −                                            ]
                                                                                  4 a ( t − t ')
                             ρ C (4 π a ( t − t '))   2


      δq = instantaneous heat generated, C = sp. heat capacity, α =
      diffusivity, ρ = Density, t = time, K = thermal conductivity.
      gives the temperature increment at position (x, y, z) and time
      t due to an instantaneous heat source δq applied at position
      (x’, y’, z’) and time t’. ME 338: Manufacturing Processes II
                                       Instructor: Ramesh Singh; Notes: Profs.                                52
                                                 Singh/Melkote/Colton
Moving point heat source in semi-infinite body




In moving coordinate system:
                                         2δ q                           ( X − x ') 2 + (Y − y ') 2 + ( Z − z ') 2
         dT '( x, y, z, t ) =                               3
                                                                exp [ −                                           ]
                                                                                       4 a ( t − t ')
                                ρ C (4 π a ( t − t '))      2


In fixed coordinate system:
                                        2δ q                         ( x − vt '− x ') 2 + ( y − y ') 2 + ( z − z ') 2
        dT '( x, y, z, t ) =                            3
                                                            ex p [ −                                                  ]
                                                                                       4 a ( t − t ')
                               ρ C (4 π a ( t − t '))   2


            Note that δ q = Pdt '                ME 338: Manufacturing Processes II
                                               Instructor: Ramesh Singh; Notes: Profs.                                53
                                                         Singh/Melkote/Colton
Moving point heat source:
Consider point heat source P heat units per unit time moving with velocity v on semi-
infinite body from time t’= 0 to t’= t. During a very short time heat released at the
surface is dQ = Pdt’. This will result in infinitesimal rise in temperature at point (x, y, z)
at time t given by,

                        t '= t
                                        2 Pdt '                        ( x − vt '− x ') 2 + ( y − y ') 2 + ( z − z ') 2
 dT '( x, y, z, t ) =    ∫
                        t '= 0
                                                          3
                                                              ex p [ −
                                                                                         4 a ( t − t ')
                                                                                                                        ]
                                 ρ C (4 π a ( t − t '))   2



The total rise in of the temperature can be obtained by
integrating from t’=0 to t’= t
Gaussian Circular
     • Gaussian beam distribution
                               2P                  2( x '2 + y '2 )
             I ( x ', y ') =         2
                                         exp[−                  2
                                                                           ]
                               πσ                         σ

     • Gaussian circular heat source
                                             2dt '                                               ( X − x ') 2 + (Y − y ') 2 + ( Z − z ') 2
     dT '( X , Y , Z , t ) =                                    3
                                                                     I ( x ', y ')dx ' dy 'exp[−                                           ]
                                                                                                               4a(t − t ')
                                   ρ C (4π a(t − t '))          2

                                             ∞    ∞
                2dt '                2P                               2( x '2 + y '2 )                   ( X − x ')2 + (Y − y ')2 + ( Z − z ')2
dT ' =                         3
                                    πσ   2   ∫ ∫
                                             −∞   −∞
                                                       exp[−
                                                                            σ2
                                                                                         ]dx ' dy 'exp[−
                                                                                                                      4a(t − t ')
                                                                                                                                                ]
         ρ C (4π a(t − t '))   2


     In fixed coordinate sytem
                                                       t '= t
                             4P                              dt '(t − t ') −0.5      2(( x − vt ') 2 + y 2 )    z2
               T − T0 =
                        ρ C π 4 aπ                       ∫0 σ 2 + 8a (t − t ') exp[ − σ 2 + 8a (t − t ') − 4 a (t − t ') ]
                                                       t '=

                                                                      ME 338: Manufacturing Processes II
                                                                    Instructor: Ramesh Singh; Notes: Profs.                            55
                                                                              Singh/Melkote/Colton
Uniform Circular/Rectangular
• Circular
                         t                σ
                2P              dt '                    (( x − vt ') − x ') 2
 T − T0 =
            8 π 2σ 2 K   ∫
                         0
                             ( t − t ')   ∫
                                          −σ
                                               ex p [ −
                                                            4 a ( t − t ')
                                                                              ]d x ' ×

           y − σ 2 − x '2            y + σ 2 − x '2
 [ − erf (                 ) + erf (                 )]
            2 a ( t − t ')            2 a ( t − t ')

• Rectangular
                             2δ q d t '                             z2
    T − T0 =                                        3
                                                        exp[−                ]
                                                              4 a ( t − t ')
                4 b l ρ C ( 4 π a ( t − t ') )      2

    l                                              b
             ( ( x − v t ') − x ') 2                    ( y − y ') 2
    ∫l
    −
       exp[−
                  4 a ( t − t ')
                                     ]d x ' ∫ e x p [ −
                                           −b
                                                        4 a ( t − t ')
                                                                       ]d y '



                                        ME 338: Manufacturing Processes II
                                      Instructor: Ramesh Singh; Notes: Profs.            56
                                                Singh/Melkote/Colton
LBM Capability
• MRR
  – Cutting speed can be as high as 4 m/min.
  – Typical material removal rate is 5 mm3/min.


• Dimensional Tolerance
  – Typical ranges from ±0.015 - ±0.125 mm


• Surface Finish
  – Ra varies between 0.4 – 6.3 µm.

                       ME 338: Manufacturing Processes II
                     Instructor: Ramesh Singh; Notes: Profs.   57
                               Singh/Melkote/Colton
LBM (Cont.)
• Process Variations

   – Laser beam machines can be used for cutting, surface hardening,
     welding, drilling, blanking, engraving and trimming.

   – Types of lasers used: pulsed and CW CO2, Nd:YAG, Nd:glass,
     ruby and excimer.

   – High-pressure gas streams are used to enhance the process by
     aiding the exothermic reaction process, to cool and blow away the
     vaporized or molten material and slag.




                            ME 338: Manufacturing Processes II
                          Instructor: Ramesh Singh; Notes: Profs.   58
                                    Singh/Melkote/Colton
LBM (Cont.)
• Applications
   –   Multiple holes in very thin and thick materials
   –   Non-standard shaped holes and slots
   –   Prototype parts
   –   Trimming, scribing and engraving of hard materials
   –   Small diameter lubrication holes

• Limitations
   – Localized thermal stresses, heat affected zones, recast layer and
     thermal distribution in thin parts
   – Difficulty of material processing depends on how close materials
     boiling and melting points are
   – Hole wall geometry can be irregular
   – The cutting of flammable materials is usually inert gas assisted


                              ME 338: Manufacturing Processes II
                            Instructor: Ramesh Singh; Notes: Profs.   59
                                      Singh/Melkote/Colton
Electron-Beam Machining (EBM)
    How it Works
•   A stream of electrons is started by
    a voltage differential at the
    cathode. The concave shape of
    the cathode grid concentrates the
    stream through the anode.
•   The anode applies a potential field
    that accelerates the electrons.
•   The electron stream is then forced
    through a valve in the electron
    beam machine.
•   The beam is focused onto the
    surface of the work material,
    heating, melting, and vaporizing
    the material.




                                         ME 338: Manufacturing Processes II
                                       Instructor: Ramesh Singh; Notes: Profs.   60
                                                 Singh/Melkote/Colton
EBM (Cont.)
The entire process occurs in a vacuum chamber because a collision
between an electron and an air molecule causes the electrons to veer
off course. LBM doesn’t need vacuum because the size and mass of a
photon is numerous times smaller than the size of an electron.




                            ME 338: Manufacturing Processes II
                          Instructor: Ramesh Singh; Notes: Profs.      61
                                    Singh/Melkote/Colton
EBM Characteristics
• Mechanics of material removal – melting, vaporization
• Medium – vacuum
• Tool – beam of electrons moving at very high velocity
• Maximum MRR = 10 mm3/min
• Specific power consumption = 450 W/mm3/min
• Critical parameters – accelerating voltage, beam
  diameter, work speed, melting temperature
• Materials application – all materials
• Shape application – drilling fine holes, cutting contours in
  sheets, cutting narrow slots
• Limitations – very high specific energy consumption,
  necessity of vacuum, expensive machine

                          ME 338: Manufacturing Processes II
                        Instructor: Ramesh Singh; Notes: Profs.   62
                                  Singh/Melkote/Colton
Comparative Performance




          ME 338: Manufacturing Processes II
        Instructor: Ramesh Singh; Notes: Profs.   63
                  Singh/Melkote/Colton
Focused Ion Beam Technologies
• Ga+ ion beam raster over the
  surface similar to SEM
• Milling of small holes and
  modifications in the structures
  can be done
• Most instruments combine
  nowadays a SEM and FIB for
  imaging with high resolution,
  and accurate control of the
  progress of the milling
• Process is performed in
  vacuum


                            ME 338: Manufacturing Processes II
                          Instructor: Ramesh Singh; Notes: Profs.   64
                                    Singh/Melkote/Colton
Mechanism




Rate of etch depth
                     Where, Y is sputter yield of surface atoms per
                     incoming ion, using a probe of current I is given by
                     A is the etched area, ρ is the density of target
                     material, M is atomic mass of target material and
                     e is charge
                         ME 338: Manufacturing Processes II
                       Instructor: Ramesh Singh; Notes: Profs.     65
                                 Singh/Melkote/Colton
Dual Beam System




       ME 338: Manufacturing Processes II
     Instructor: Ramesh Singh; Notes: Profs.   66
               Singh/Melkote/Colton
ME 338: Manufacturing Processes II
Instructor: Ramesh Singh; Notes: Profs.   67
          Singh/Melkote/Colton
Focused Ion Beam Technologies
• FIB finds application in:
   – Ablation of hard materials:
     diamond, WC
   – Polishing of single crystals
   – Deposition
   – Site-specific analysis
   – FIB lithography
   – TEM samples


• Capital investment ~ 5 Crore




                              ME 338: Manufacturing Processes II
                            Instructor: Ramesh Singh; Notes: Profs.   68
                                      Singh/Melkote/Colton
Process Capabilities of FIB
•   Deposition
•   Etching
•   Low material removal
•   Very high cost
•   Nanometric imaging resolution
•   Can process conducting and non conducting materials




                         ME 338: Manufacturing Processes II
                       Instructor: Ramesh Singh; Notes: Profs.   69
                                 Singh/Melkote/Colton
Summary
• Process description and capability
  –   Ultrasonic Machining (USM)
  –   Water-Jet Machining & Abrasive-Jet Machining
  –   Chemical Machining
  –   Electrochemical Machining (ECM)
  –   Electrical-Discharge Machining (EDM)
• High-Energy-Beam Machining
  – Laser-beam machining (LBM)
  – Electron-beam machining (EBM)
  – Focused Ion Beam (FIB)


                        ME 338: Manufacturing Processes II
                      Instructor: Ramesh Singh; Notes: Profs.   70
                                Singh/Melkote/Colton

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Non trad

  • 1. Non-Traditional Machining ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 1 Singh/Melkote/Colton
  • 2. Introduction • Machining is a broad term to describe removal of material from a workpiece. • Machining categories: – Cutting involves single-point or multipoint cutting tools, each with a clearly defined geometry. – Abrasive processes, such as grinding. – Nontraditional machining, utilizing electrical, chemical, and optical sources of energy. ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 2 Singh/Melkote/Colton
  • 3. Nontraditional Machining • Ultrasonic Machining (USM) • Water-Jet Machining & Abrasive-Jet Machining • Chemical Machining • Electrochemical Machining (ECM) • Electrical-Discharge Machining (EDM) • High-Energy-Beam Machining – Laser-beam machining (LBM) – Electron-beam machining (EBM) ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 3 Singh/Melkote/Colton
  • 4. Traditional vs. Nontraditional • Primary source of energy – Traditional: mechanical. – Nontraditional: electrical, chemical, optical • Primary method of material removal – Traditional: shearing – Nontraditional: does not use shearing (e.g., abrasive water jet cutting uses erosion) Water jet machining Grinding 2D cutting process ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 4 Singh/Melkote/Colton
  • 5. Why Nontraditional Machining? • Situations where traditional machining processes are unsatisfactory or uneconomical: – Workpiece material is too hard, strong, or tough. – Workpiece is too flexible to resist cutting forces or too difficult to clamp. – Part shape is very complex with internal or external profiles or small holes. – Requirements for surface finish and tolerances are very high. – Temperature rise or residual stresses are undesirable or unacceptable. ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 5 Singh/Melkote/Colton
  • 6. Ultrasonic Machining (USM) • Process description – The tool, which is negative of the workpiece, is vibrated at low amplitude (0.013 to 0.08 mm) and high frequency (about 20 kHz) in an abrasive grit slurry at the workpiece surface. – The slurry also carries away the debris from the cutting area. – The tool is gradually moved down maintaining a constant gap of approximately 0.1 mm between the tool and workpiece surface. ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 6 Singh/Melkote/Colton
  • 7. USM (Cont.) • Cracks are generated due to the high stresses produced by particles striking a surface. • The time of contact between the particle and the surface is given by: 1/ 5 5r  c 0  t0 ≈   (10 − 100 µ s ) Force of a particle on surface: c0  v  F = d (mv) / dt r: radius of a spherical particle c0: workpiece elastic wave velocity = E / ρ Average force of a particle striking the surface: v: velocity of particle striking surface Fave = 2mv / t 0 ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 7 Singh/Melkote/Colton
  • 8. USM (Cont.) • Example: Explain what change, if any, takes place in the magnitude of the impact force of a particle in ultrasonic machining as the temperature of the workpiece is increased. Solution: Here, m and v are constant. 1/ 5 5r  c 0  1 1 t0 =   ⇒ t0 ∝ ∝ c0  v  c04 / 5 E 2/5 When temperature increases, E decreases and t0 increases. Hence, F decreases. ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 8 Singh/Melkote/Colton
  • 9. USM (Cont.) Assuming hemispherical brittle fracture 3 2π  D  V=   3 2 D ≈ 2 dh 2π V= (dh) 3 / 2 3 MRR = ηV Z f where V = volume removed by a single grain f = frequency of operation Z = number of particles impacting per cycle η = efficiency ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 9 Singh/Melkote/Colton
  • 10. USM (Cont.) • Applications – USM is best suited for hard, brittle materials, such as ceramics, carbides, glass, precious stones, and hardened steels. (Why?) • Capability – With fine abrasives, tolerance of 0.0125 mm or better can be held. Ra varies between 0.2 – 1.6 µm. • Pros & Cons: – Pros: precise machining of brittle materials; makes tiny holes (0.3 mm); does not produce electric, thermal, chemical damage because it removes material mechanically. – Cons: low material removal rate (typically 0.8 cm3/min); tool wears rapidly; machining area and depth are limited. ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 10 Singh/Melkote/Colton
  • 11. USM Parts Ceramic ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 11 Singh/Melkote/Colton
  • 12. Water-Jet Machining (WJM) also called hydrodynamic machining WJM is a form of micro erosion. It The extreme pressure of the accelerated works by forcing a large volume of water particles contacts a small area of the water through a small orifice in the workpiece and acts like a saw and cuts a nozzle. narrow groove in the material. http://www.flowcorp.com/waterjet-resources.cfm?id=360 ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 12 Singh/Melkote/Colton
  • 13. WJM (Cont.) • Pros: no need for predrilled holes, no heat, no workpiece deflection (hence suitable for flexible materials), minimal burr, environmentally friendly. • Cons: limited to material with naturally occurring small cracks or softer material. • Applications: – Mostly used to cut lower strength materials such as wood, plastics, rubber, paper, leather, composite, etc. – Food preparation – Good for materials that cannot withstand high temperatures of other methods for stress distortion or metallurgical reasons. ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 13 Singh/Melkote/Colton
  • 14. WJM Examples PWB (printed wire board) ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 14 Singh/Melkote/Colton
  • 15. Abrasive Water-Jet Machining (AWJM) The water jet contains abrasive particles such as silicon carbide, thus increasing MRR. Metallic materials can be cut. Particularly suitable for heat-sensitive materials. ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 15 Singh/Melkote/Colton
  • 16. AWJM Parts Bullet Proof Glass Part Steel rack (75 mm thick) Ceramic Part Source: http://www.waterjets.org/ ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 16 Singh/Melkote/Colton
  • 17. Abrasive-Jet Machining (AJM) A high-velocity jet of dry air, The gas supply pressure is on nitrogen, or carbon dioxide the order of 850 kPa (125 psi) containing abrasive particles is and the jet velocity can be as aimed at the workpiece surface high as 300 m/s and is under controlled conditions. controlled by a valve. ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 17 Singh/Melkote/Colton
  • 18. AJM Process Capability • Material removal – Typical cutting speeds vary between 25 -125 mm/min • Dimensional Tolerances – Typical range ±2 - ±5 µm • Surface Finish – Typical Ra values vary from 0.3 - 2.3 µm ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 18 Singh/Melkote/Colton
  • 19. AJM Applications & Limitations • Applications – Can cut traditionally hard to cut materials, e.g., composites, ceramics, glass – Good for materials that cannot stand high temperatures • Limitations – Expensive process – Flaring can become large – Not suitable for mass production because of high maintenance requirements ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 19 Singh/Melkote/Colton
  • 20. Chemical Machining (CM) • Chemical machining, basically an etching process, is the oldest nontraditional machining process. • Material is removed from a surface by chemical dissolution using chemical reagents, or etchants, such as acids and alkaline solutions. • The workpiece is immersed in a bath containing an etchant. The area that are not required to be etched are masked with “cut and peel” tapes, paints, or polymeric materials. • In chemical milling, shallow cavities are produced on plates, sheets, forgings, and extrusions for overall reduction of weight (e.g., in aerospace industry). Depths of removal can be as much as 12 mm. ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 20 Singh/Melkote/Colton
  • 21. CM (Cont.) • Chemical blanking is used to produce features which penetrate through the material via chemical dissolution. The metal that is to be blanked is – thoroughly cleaned with solvents. – coated and the image of the part is imprinted. – soaked in a solvent that removes the coating, except in the protected areas. – spray etched to dissolve the unprotected areas and leave the finished part. ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 21 Singh/Melkote/Colton
  • 22. CM (Cont.) • Typical applications – Chemical blanking: burr-free etching of printed-circuit boards (PCB), decorative panels, thin sheet-metal stampings, and the production of complex or small shapes. – Chemical milling: weight reduction of space launch vehicles. Pros: low setup, maintenance, and tooling costs; small, delicate parts can be machined; suitable for low production runs on intricate designs. Cons: slow (0.025-0.1 mm/min); surface defects; chemicals can be extremely dangerous to health. ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 22 Singh/Melkote/Colton
  • 23. Electrochemical Machining (ECM) • Process description: – In ECM, a dc voltage (10-25 v) is applied across the gap between a pre-shaped cathode tool and an anode workpiece. The workpiece is dissolved by an electrochemical reaction to the shape of the tool. – The electrolyte flows at high speed (10-60 m/s) through the gap (0.1-0.6 mm) to dissipate heat and wash away the dissolved metal. ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 23 Singh/Melkote/Colton
  • 24. ECM (Cont.) • The material removal rate by ECM is given by: MRR = C I η where, MRR=mm3/min, I=current in amperes, η=current efficiency, which typically ranges from 90-100%, C is a material constant in mm3/A·min. Feed rate (mm/min): f = MRR / A0 Assuming a cavity with uniform cross-sectional area A0 ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 24 Singh/Melkote/Colton
  • 25. ECM (Cont.) • Pros: high shape complexity possible, high MRR possible, high- strength materials, mirror surface finish possible. • Cons: workpiece must be electrically conductive; very high tooling (dedicated) and equipment costs; high power consumption. • Applications: complex cavities in high-strength materials, esp. in aerospace industry for mass production of turbine blades. ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 25 Singh/Melkote/Colton
  • 26. EDM-History ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 26 Singh/Melkote/Colton
  • 27. Electrical Discharge Machining (EDM) EDM is a thermal erosion process whereby material is melted and vaporized from an electrically conducive workpiece immersed in a liquid dielectric with a series of spark discharges between the tool electrode and the workpiece created by a power supply. EDM is one of the most accurate while quite affordable mfg process. ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 27 Singh/Melkote/Colton
  • 28. EDM (Cont.) The EDM system consists of a shaped tool or wire electrode, and the part. The part is connected to a power supply to create a potential difference between the workpiece and the tool. When the potential difference is sufficiently high, a transient spark The dielectric fluid 1) acts as an discharges through the insulator until the potential is fluid, removing a very small sufficiently high, 2) acts as a amount of metal from the flushing medium, and 3) provides workpiece. a cooling medium. ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 28 Singh/Melkote/Colton
  • 29. Process-Basics ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 29 Singh/Melkote/Colton
  • 30. EDM (Cont.) MRR is basically a function of the current and the melting point of the workpiece material. An approximate empirical relationship is: 4 −1.23 MRR=mm3/min MRR = 4 × 10 I T w I=current in amperes Tw=melting point of workpiece (ºC) Wear rate of electrode: Wt = 11× 10 3 I Tt −2.38 Wear ratio of workpiece to electrode: Wt=mm3/min Tt=melting point of electrode material (ºC) R = 2.25 Tr−2.3 Tr=ratio of workpiece to electrode melting points (ºC) ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 30 Singh/Melkote/Colton
  • 31. MRR - EDM Metal removal is function of pulse energy • Experimental Approach and frequency: h = K1Wn TOOL (-) D= K2Wn where W = Pulse energy, J DC VOLTAGE h = height of crater, mm D = diameter of crater, mm K1, K2 = constants depending h on electrode materials D and dielectric n = constant depending on WORKPIECE work tool combination (+) The crater volume from geometry, π 3  Scheme of Crater Formation Vc = h D 2 + h 2  6 4  MRR = Vc f η π 3 2 2 3n where f = frequency of operation and η = efficiency Vc = K1  K 2 + K1 W 6 4  ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 31 Singh/Melkote/Colton
  • 32. Volume of the crater ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 32 Singh/Melkote/Colton
  • 33. EDM Process Capability • MRR – Range from 2 to 400 mm3/min. High rates produce rough finish, having a molten and recast structure with poor surface integrity and low fatigue properties. • Dimensional Tolerances – Function of the material being processed – Typically between ±0.005 - ±0.125 mm • Surface Finish – Depends on current density and material being machined – Ra varies from 0.05 – 12.5 µm – New techniques use an oscillating electrode, providing very fine surface finishes. ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 33 Singh/Melkote/Colton
  • 34. EDM Applications Widely used in aerospace, moldmaking, and die casting to produce die cavities, small deep holes, narrow slots, turbine blades, and intricate shapes. Cavities produced by EDM Stepped cavities ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 34 Singh/Melkote/Colton
  • 35. EDM Limitations • Limitations – A hard skin, or recast layer is produced which may be undesirable in some cases. – Beneath the recast layer is a heat affected zone which may be softer than parent material. – Finishing cuts are needed at low MRR. – Produces slightly tapered holes, specially if blind. ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 35 Singh/Melkote/Colton
  • 36. Wire EDM A wire travels along a prescribed path, cutting the workpiece, with the discharge sparks acting like cutting teeth. ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 36 Singh/Melkote/Colton
  • 37. Wire EDM (Cont.) MRR in Wire EDM MRR = V f h b where, b = d w + 2s MRR = mm3/min Vf = feed rate of wire into the workpiece in mm/min h = workpiece thickness or dw = wire diameter in mm height in mm s = gap between wire and workpiece in mm ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 37 Singh/Melkote/Colton
  • 38. Wire EDM Parts ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 38 Singh/Melkote/Colton
  • 39. Example • Example: You have to machine the following part from a 85mmx75mmx20mm steel block. You have to choose between EDM and Conventional machining. Your objective is to minimize the cutting power required, which process will you choose? 12.5 Assumptions: – EDM process: 40 • Wire diameter: dw=0.2 mm • Gap: s=0.1 mm – Conventional machining: 10 • Negative of the part has to be 12.5 removed 12.5 20 20 20 12.5 ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 39 Singh/Melkote/Colton
  • 40. Example Solution: - EDM process VEDM = lc*(dw+2s)*t = 1440 mm3 - Conventional machining VM= Vtotal – Vpart = 99500 mm3 - Power comparison u M VM u EDM VEDM We will choose machining if ≤ tM t EDM let’s assume tEDM=αtM u EDM VEDM then machining if α ≤ u M VM ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 40 Singh/Melkote/Colton
  • 41. Reverse micro-EDM • Fabrication of high aspect ratio micro-electrode arrays • Potential application in machining hole arrays via micro- EDM/ECM ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 41 Singh/Melkote/Colton
  • 42. Arrays Fabricated via R µ-EDM @IITB 6x6 array 4x4 array ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 42 Singh/Melkote/Colton
  • 43. Experimental Setup ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 43 Singh/Melkote/Colton
  • 44. Fabricated Texture ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 44 Singh/Melkote/Colton
  • 45. High-Energy-Beam Machining • Laser-Beam Machining (LBM) • Electron-Beam Machining (EBM) • Focused Ion-Beam Machining ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 45 Singh/Melkote/Colton
  • 46. Laser-Beam Machining (LBM) • Laser Concept – Add energy to make electrons “jump” to higher energy orbit – Electron “relaxes” and moves to equilibrium at ground-state energy level – Emits a photon in this process (key laser component) – Two mirrors reflect the photons back and forth and “excite” more electrons – One mirror is partially reflective to allow some light to pass through: creates narrow laser beam ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 46 Singh/Melkote/Colton
  • 47. LBM (Cont.) Excited State Electron Ground State Photon Nucleus Orbits Electron is Electron relaxes energized to the to ground state excited state and photon is produced Photon Emission Model ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 47 Singh/Melkote/Colton
  • 48. LBM (Cont.) • More precise • Useful with a variety of materials: metals, composites, plastics, and ceramics • Smooth, clean cuts • Faster process • Decreased heat- affected zone ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 48 Singh/Melkote/Colton
  • 49. Schematic of LBM Device ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 49 Singh/Melkote/Colton
  • 50. Laser Setup • Laser Processing Center – 100 W SPI single mode fiber laser (Power and frequency modulated) – Optics for variable intensity distribution and spot size – 3 axis (Z decoupled) translational stages and controls “Method and device for generating laser – Provides uniform/Gaussian intensity beam of variable intensity distribution – 7 µm -900 µm spot size possible and variable spot size”, – Hardening/Cladding/Texturing/Brazing Indian Patent Application No. 442/MUM/2011. Machine Tools Laboratory Micromachining Cell
  • 51. LBM (Cont.) • Important physical parameters in LBM – Reflectivity – Thermal conductivity of workpiece surface – Specific heat and latent heats of melting and evaporation • The lower these quantities, the more efficient the process. • The cutting depth t: t = P / vd P is the power input, v is the cutting speed, and d is the laser-beam-spot diameter. ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 51 Singh/Melkote/Colton
  • 52. Heat Source Modeling • Solution for stationary point using Green’s Theorem: The differential equation for the conduction of heat in a stationary medium assuming no convection or radiation, is This is satisfied by the solution for infinite body, δq ( x − x ') 2 + ( y − y ') 2 + ( z − z ') 2 dT '( x, y, z, t ) = 3 ex p [ − ] 4 a ( t − t ') ρ C (4 π a ( t − t ')) 2 sem i − in f in ite 2δ q ( x − x ') 2 + ( y − y ') 2 + ( z − z ') 2 dT '( x, y, z, t ) = 3 ex p [ − ] 4 a ( t − t ') ρ C (4 π a ( t − t ')) 2 δq = instantaneous heat generated, C = sp. heat capacity, α = diffusivity, ρ = Density, t = time, K = thermal conductivity. gives the temperature increment at position (x, y, z) and time t due to an instantaneous heat source δq applied at position (x’, y’, z’) and time t’. ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 52 Singh/Melkote/Colton
  • 53. Moving point heat source in semi-infinite body In moving coordinate system: 2δ q ( X − x ') 2 + (Y − y ') 2 + ( Z − z ') 2 dT '( x, y, z, t ) = 3 exp [ − ] 4 a ( t − t ') ρ C (4 π a ( t − t ')) 2 In fixed coordinate system: 2δ q ( x − vt '− x ') 2 + ( y − y ') 2 + ( z − z ') 2 dT '( x, y, z, t ) = 3 ex p [ − ] 4 a ( t − t ') ρ C (4 π a ( t − t ')) 2 Note that δ q = Pdt ' ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 53 Singh/Melkote/Colton
  • 54. Moving point heat source: Consider point heat source P heat units per unit time moving with velocity v on semi- infinite body from time t’= 0 to t’= t. During a very short time heat released at the surface is dQ = Pdt’. This will result in infinitesimal rise in temperature at point (x, y, z) at time t given by, t '= t 2 Pdt ' ( x − vt '− x ') 2 + ( y − y ') 2 + ( z − z ') 2 dT '( x, y, z, t ) = ∫ t '= 0 3 ex p [ − 4 a ( t − t ') ] ρ C (4 π a ( t − t ')) 2 The total rise in of the temperature can be obtained by integrating from t’=0 to t’= t
  • 55. Gaussian Circular • Gaussian beam distribution 2P 2( x '2 + y '2 ) I ( x ', y ') = 2 exp[− 2 ] πσ σ • Gaussian circular heat source 2dt ' ( X − x ') 2 + (Y − y ') 2 + ( Z − z ') 2 dT '( X , Y , Z , t ) = 3 I ( x ', y ')dx ' dy 'exp[− ] 4a(t − t ') ρ C (4π a(t − t ')) 2 ∞ ∞ 2dt ' 2P 2( x '2 + y '2 ) ( X − x ')2 + (Y − y ')2 + ( Z − z ')2 dT ' = 3 πσ 2 ∫ ∫ −∞ −∞ exp[− σ2 ]dx ' dy 'exp[− 4a(t − t ') ] ρ C (4π a(t − t ')) 2 In fixed coordinate sytem t '= t 4P dt '(t − t ') −0.5 2(( x − vt ') 2 + y 2 ) z2 T − T0 = ρ C π 4 aπ ∫0 σ 2 + 8a (t − t ') exp[ − σ 2 + 8a (t − t ') − 4 a (t − t ') ] t '= ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 55 Singh/Melkote/Colton
  • 56. Uniform Circular/Rectangular • Circular t σ 2P dt ' (( x − vt ') − x ') 2 T − T0 = 8 π 2σ 2 K ∫ 0 ( t − t ') ∫ −σ ex p [ − 4 a ( t − t ') ]d x ' × y − σ 2 − x '2 y + σ 2 − x '2 [ − erf ( ) + erf ( )] 2 a ( t − t ') 2 a ( t − t ') • Rectangular 2δ q d t ' z2 T − T0 = 3 exp[− ] 4 a ( t − t ') 4 b l ρ C ( 4 π a ( t − t ') ) 2 l b ( ( x − v t ') − x ') 2 ( y − y ') 2 ∫l − exp[− 4 a ( t − t ') ]d x ' ∫ e x p [ − −b 4 a ( t − t ') ]d y ' ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 56 Singh/Melkote/Colton
  • 57. LBM Capability • MRR – Cutting speed can be as high as 4 m/min. – Typical material removal rate is 5 mm3/min. • Dimensional Tolerance – Typical ranges from ±0.015 - ±0.125 mm • Surface Finish – Ra varies between 0.4 – 6.3 µm. ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 57 Singh/Melkote/Colton
  • 58. LBM (Cont.) • Process Variations – Laser beam machines can be used for cutting, surface hardening, welding, drilling, blanking, engraving and trimming. – Types of lasers used: pulsed and CW CO2, Nd:YAG, Nd:glass, ruby and excimer. – High-pressure gas streams are used to enhance the process by aiding the exothermic reaction process, to cool and blow away the vaporized or molten material and slag. ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 58 Singh/Melkote/Colton
  • 59. LBM (Cont.) • Applications – Multiple holes in very thin and thick materials – Non-standard shaped holes and slots – Prototype parts – Trimming, scribing and engraving of hard materials – Small diameter lubrication holes • Limitations – Localized thermal stresses, heat affected zones, recast layer and thermal distribution in thin parts – Difficulty of material processing depends on how close materials boiling and melting points are – Hole wall geometry can be irregular – The cutting of flammable materials is usually inert gas assisted ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 59 Singh/Melkote/Colton
  • 60. Electron-Beam Machining (EBM) How it Works • A stream of electrons is started by a voltage differential at the cathode. The concave shape of the cathode grid concentrates the stream through the anode. • The anode applies a potential field that accelerates the electrons. • The electron stream is then forced through a valve in the electron beam machine. • The beam is focused onto the surface of the work material, heating, melting, and vaporizing the material. ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 60 Singh/Melkote/Colton
  • 61. EBM (Cont.) The entire process occurs in a vacuum chamber because a collision between an electron and an air molecule causes the electrons to veer off course. LBM doesn’t need vacuum because the size and mass of a photon is numerous times smaller than the size of an electron. ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 61 Singh/Melkote/Colton
  • 62. EBM Characteristics • Mechanics of material removal – melting, vaporization • Medium – vacuum • Tool – beam of electrons moving at very high velocity • Maximum MRR = 10 mm3/min • Specific power consumption = 450 W/mm3/min • Critical parameters – accelerating voltage, beam diameter, work speed, melting temperature • Materials application – all materials • Shape application – drilling fine holes, cutting contours in sheets, cutting narrow slots • Limitations – very high specific energy consumption, necessity of vacuum, expensive machine ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 62 Singh/Melkote/Colton
  • 63. Comparative Performance ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 63 Singh/Melkote/Colton
  • 64. Focused Ion Beam Technologies • Ga+ ion beam raster over the surface similar to SEM • Milling of small holes and modifications in the structures can be done • Most instruments combine nowadays a SEM and FIB for imaging with high resolution, and accurate control of the progress of the milling • Process is performed in vacuum ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 64 Singh/Melkote/Colton
  • 65. Mechanism Rate of etch depth Where, Y is sputter yield of surface atoms per incoming ion, using a probe of current I is given by A is the etched area, ρ is the density of target material, M is atomic mass of target material and e is charge ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 65 Singh/Melkote/Colton
  • 66. Dual Beam System ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 66 Singh/Melkote/Colton
  • 67. ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 67 Singh/Melkote/Colton
  • 68. Focused Ion Beam Technologies • FIB finds application in: – Ablation of hard materials: diamond, WC – Polishing of single crystals – Deposition – Site-specific analysis – FIB lithography – TEM samples • Capital investment ~ 5 Crore ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 68 Singh/Melkote/Colton
  • 69. Process Capabilities of FIB • Deposition • Etching • Low material removal • Very high cost • Nanometric imaging resolution • Can process conducting and non conducting materials ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 69 Singh/Melkote/Colton
  • 70. Summary • Process description and capability – Ultrasonic Machining (USM) – Water-Jet Machining & Abrasive-Jet Machining – Chemical Machining – Electrochemical Machining (ECM) – Electrical-Discharge Machining (EDM) • High-Energy-Beam Machining – Laser-beam machining (LBM) – Electron-beam machining (EBM) – Focused Ion Beam (FIB) ME 338: Manufacturing Processes II Instructor: Ramesh Singh; Notes: Profs. 70 Singh/Melkote/Colton