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NANO-FINISHING TECHNIQUES

Sunil Jha and V.K. Jain
Department of Mechanical Engineering
Indian Institute of Technology Kanpur - 208016, INDIA

Source of information: http://web.iitd.ac.in/~suniljha/nanofinishing.pdf


1 Magnetic Abrasive Finishing (MAF)

      Magnetic abrasives are emerging as important finishing methods for metals and ceramics. Magnetic Abrasive Finishing is one such unconventional finishing process developed recently to produce efficiently and economically good quality finish on the internal and external surfaces of tubes as well as flat surfaces made of magnetic or non-magnetic materials. In this process, usually ferromagnetic particles are sintered with fine abrasive particles (Al2O3, SiC, CBN or diamond) and such particles are called ferromagnetic abrasive particles (or magnetic abrasive particles). However, homogeneously mixed loose ferromagnetic and abrasive particles are also used in certain applications. Fig. 1 shows a Plane MAF process in which finishing action is generated by the application of magnetic field across the gap between workpiece surface and rotating electromagnet pole. The enlarged view of finishing zone in Fig. 4 shows the forces acting on the work surface to remove material in the form of chips. Force due to magnetic field is responsible for normal force causing abrasive penetration inside the workpiece while rotation of the magnetic abrasive brush (i.e. North pole) results in material removal in the form of chips.
      The magnetic abrasive grains are combined to each other magnetically between magnetic poles along a line of magnetic force, forming a flexible magnetic abrasive brush. MAF uses this magnetic abrasive brush for surface and edge finishing. The magnetic field retains the powder in the gap, and acts as a binder causing the powder to be pressed against the surface to be finished [1]. 3D minute and intricately curved shape can also be finished along its uneven surface. Controlling the exciting current of the magnetic coil precisely controls the machining force of the magnetic abrasives on the work piece [2].

Plane Magnetic abrasive finishing
Fig. 1 - Plane Magnetic abrasive finishing

      Since the magnitude of machining force caused by the magnetic field is very low but controllable, a mirror like surface finish (Ra value in the range of nano-meter) is obtained. In MAF, mirror finishing is realized and burrs are removed without lowering the accuracy of the shape. These fine finishing technologies using magnetic abrasives have a wide range of applications. The surface finishing, deburring and precision rounding off the workpiece can be done simultaneously. MAF can be used to perform operations as polishing and removal of thin oxide films from high speed rotating shafts. Shinmura [3] have applied MAF to the internal surface of work pieces such as vacuum tubes and sanitary tubes.
      Fig. 2 shows the magnetic abrasive jet finishing of internal surface of a hollow cylindrical workpiece. It's a variant of MAF process in which working fluid mixed with magnetic abrasives is jetted into the internal surface of the tube, with magnetic poles being provided on the external surface of the tube [4]. The magnetic abrasives in the jet mixed with fluid are moved to the internal surface by magnetic force, where the magnetic abrasives finish the internal surface effectively and precisely.

Magnetic abrasive jet finishing
Fig. 2 - Magnetic abrasive jet finishing

      Fig. 3 shows a schematic of a typical MAF process in which the workpiece to be machined is located between two magnetic poles. The gap between the workpiece and the pole is filled with a magnetic abrasive powder. The magnetic abrasive grains are linked to each other magnetically between the north and south magnetic poles along the lines of magnetic force, forming a flexible 2-5 mm long magnetic brush. MAF uses this magnetic abrasive brush for surface and edge finishing. The magnetic field retains the powder in gaps, and acts as a binder causing the powder to be pressed against the surface to be finished [5]. A rotary motion is provided to cylindrical workpiece, such as ceramic bearing rollers between magnetic poles. Also axial vibratory motion is introduced in the magnetic field by the oscillating motion of magnetic poles to accomplish surface and edge finishing at faster rate and better quality.
      The process is highly efficient and the removal rate and finishing rate depends on the workpiece circumferential speed, magnetic flux density, working clearance, workpiece materials, and size, type and volume fraction of abrasives. The exciting current of the magnetic coil precisely controls the machining force transferred through magnetic abrasives on the work piece.

Magnetic Abrasive Finishing of cylindrical surface
Fig. 3 -Magnetic Abrasive Finishing of cylindrical surface

      Since the magnitude of machining force caused by the magnetic field is very low, a mirror like surface finish (Ra value in the range of nano-meter) can be obtained. Results were reported in the literature of finishing stainless steel rollers using MAF to obtain final Ra of 7.6 nm from an initial Ra of 0.22 µm in 30 seconds [6].

2 Magnetorheological Finishing (MRF)

      Traditional methods of finishing high precision lenses, ceramics and semiconductor wafers are very expensive and labor intensive. The primary obstacle in manufacturing high precision lenses is that lenses are usually made of brittle materials such as glass, which tends to crack while it is machined. Even a single microscopic crack can drastically hinder a lens's performance, making it completely ineffective for its intended application. Every device that uses either lasers or fiber optics requires at least one high precision lens, increasing its demand higher than ever.
      Lens manufacturing can be classified into two main processes: grinding and finishing. Grinding gets the lens close to the desired size, while finishing removes the cracks and tiny surface imperfections that the grinding process either overlooked or created. The lens manufacturer generally uses its in-house opticians for the finishing process, which makes it an arduous, labor-intensive process. Perhaps the biggest disadvantage to manual grinding and finishing is that it is nondeterministic. To overcome these difficulties, Center for Optics Manufacturing (COM) in Rochester, N.Y. has developed a technology to automate the lens finishing process known as Magnetorheological Finishing (MRF) [7].
      The MRF process relies on a unique "smart fluid", known as Magnetorheological (MR) fluid. MR-Fluids are suspensions of micron sized magnetizable particles such as carbonyl iron, dispersed in a non-magnetic carrier medium like silicone oil, mineral oil or water. In the absence of a magnetic field, an ideal MR-fluid exhibits Newtonian behaviour. On the application of an external magnetic field to a MR-suspension, a phenomenon known as Magnetorheological effect, shown in Fig.4, is observed. Fig. 4a shows the random distribution of the particles in the absence of external magnetic field; In Fig. 4b, particles magnetize and form columns when external magnetic field is applied. The particles acquire dipole moments proportional to magnetic field strength and when the dipolar interaction between particles exceeds their thermal energy, the particles aggregate into chains of dipoles aligned in the field direction. Because energy is required to deform and rupture the chains, this micro-structural transition is responsible for the onset of a large "controllable" finite yield stress [8]. Fig. 4c shows an increasing resistance to an applied shear strain, γ due to this yield stress. When the field is removed, the particles return to their random state and the fluid again exhibits its original Newtonian behaviour.

Magnetorheological effect
Fig. 4 - Magnetorheological effect, (a) MRP-fluid at no magnetic field, (b) at magnetic field strength H, and (c) At magnetic field H & applied shear strain γ

      Rheologically, the behaviour of MR-fluid in presence of magnetic field is described by Bingham Plastic model [9]:


where τ is the fluid shear stress, τ0 is magnetic field induced yield shear stress, η is dynamic viscosity of MR-fluid and γ’ is Shear rate [s-1].
      The dynamic viscosity is mostly determined by the base fluid. The field induced shear stress τ0 depends on the magnetic field strength, H. The strength of the fluid (i.e. the value of static yield shear stress) increases as the applied magnetic field increases. However, this increase is non-linear since the particles are ferromagnetic and magnetizations in different parts of the particles occur nonuniformly [10]. MR-fluids exhibit dynamic field strength of 50-100 kPa for applied magnetic fields of 150-250 kA/m (~2-3 kOe) [11]. The ultimate strength of MR-fluid is limited by magnetic saturation.
      The ability of electrically manipulating the rheological properties of MR-fluid attracts attention from wide range of industries and numerous applications are explored [12]. These applications are use of MR-fluid in shock absorbers and damping devices, clutch, brakes, actuators, and artificial joints. The magnetic field applied to the fluid creates a temporary finishing surface, which can be controlled in real time by varying the field's strength and direction. The standard MR fluid composition is effective for finishing optical glasses, glass ceramics, plastics and some non-magnetic metals [13].
       In the Magnetorheological finishing process as shown in Fig. 5, a convex, flat, or concave workpiece is positioned above a reference surface. A MR fluid ribbon is deposited on the rotating wheel rim, Fig. 6. By applying magnetic field in the gap, the stiffened region forms a transient work zone or finishing spot. Surface smoothing, removal of sub-surface damage, and figure correction are accomplished by rotating the lens on a spindle at a constant speed while sweeping the lens about its radius of curvature through the stiffened finishing zone [14]. Material removal takes place through the shear stress created as the magnetorheological polishing ribbon is dragged into the converging gap between the part and carrier surface. The zone of contact is restricted to a spot, which conforms perfectly to the local topography of the part. Deterministic finishing of flats, spheres, and aspheres can be accomplished by mounting the part on rotating spindle and sweeping it through the spot under computer control, such that dwell time determines the amount of material removal.

Magnetorheological finishing process
Fig. 5 - Magnetorheological finishing process

A Vertical MRF Machine
Fig. 6 - A Vertical MRF Machine [14]

      The MR-polishing fluid lap has following merits over traditional lap:
      1. Its compliance is adjustable through the magnetic field.
      2. It carries heat and debris away from the polishing zone.
      3. It does not load up as in grinding wheel.
      4. It is flexible and adapts the shape of the part of the workpiece which is in its contact.
      The computer controlled Magnetorheological finishing process has demonstrated the ability to produce the surface accuracy of order 10-100 nm peak to valley by overcoming many fundamental limitations inherent to traditional finishing techniques [7].These unique characteristics made Magnetorheological Finishing as the most efficient and able process for high precision finishing of optics. MRF makes finishing of free form shapes possible for first time.
      Applications that use high precision lenses include medical equipment such as endoscopes, collision-avoidance devices for the transportation industry, scientific testing devices and military's night vision equipment like infrared binoculars. Missiles are equipped with a wide variety of high precision lenses for navigation, target location, and other functions. The nano diamond doped MR fluid removes edge chips, cracks, and scratches in sapphire bend bars.

References

  1. Kremen. G.Z. (1994), «Machining time estimation for magnetic abrasive processes.» International Journal of Production Research, vol. 32, No. 12, 2817 - 2825.
  2. Jain, V. K.; Kumar, P.; Behera,P. K. ; and Jayswal, S.C. (2001), «Effect of working gap and circumferential speed on the performance of magnetic abrasive finishing process», Wear, 250, pp. 384 - 390.
  3. Shinmura. T. (1987), «Study on magnetic abrasive finishing - characteristics of finished surface.» Journal of Japan Society of Precision Engineering, 53,11, 1791 - 1793.
  4. Kim. J.D. (1997), «Development of a magnetic abrasive jet machining system for internal polishing of circular tubes.» Journal of material processing technology, 71,384 - 393.
  5. Kremen G.Z., Machining time estimation for magnetic abrasive processes, International Journal of Production Research, vol. 32, No. 12, 2817 - 2825, 1994.
  6. Fox, M; Agrawal, K; Shinmura, T; Komanduri, R «Magnetic Abrasive Finishing of Rollers», Annals of CIRP, Vol. 43/1, 1994.
  7. Kordonski W.I., Magnetorheological finishing, International Journal of modern physics B, vol. 10, Nos. 23&24, 2837 - 2849, 1996.
  8. Furst E. M. and Gast A.P., Micromechanics of Magnetorheological Suspensions, Physical Review E, Vol. 61, No. 6, 6732 - 6739, 2000.
  9. Kordonski W., Gordokin S., and Zhuravski N., Static Yield Stress in Magnetorheological Fluid, Int. J. of Modern Physics B, Vol. 15, Nos. 6 & 7, 1078 - 1084, 2001.
  10. Ginder J. M. and Davis L. C., Shear Stresses in Magnetorheological Fluids: Role of Magnetic Saturation, Appl. Phys. Letter, 65 (26), 3410 - 3412, 1994.
  11. Carlson J. D., Catanzarite D. M. and Clair K. A. St., Commercial Magnetorheological Fluid Devices, Int. J. of Modern Physics B, Vol. 10, Nos. 23 & 24, 2857-2865, 1996.
  12. Klingenberg D. J., Magnetorheology: Applications and Challenges, AIChE Journal, Vol. 47, N0. 2, 246 - 249, 2001.
  13. Lambropoulo S. J., Yang F., and Jacob S.D., Optical fabrication and testing, Technical digest series (Optical Society of America, Washington DC), vol. 7, 150 - 153, 1996.
  14. COM, Magnetorheological finishing, Article by Center for Optics Manufacturing,1998.


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