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Directional Solidification and Phase Stabilization

Directional Solidification and Phase Stabilization


Source: Sina Shahbazmohamadi and Peiman Shahbeigi-Roodposhti-Roodposhti, School of Engineering, University of Connecticut, Storrs, CT

Directional solidification zone melting is a metallurgical process in which a narrow region of a crystal (usually in the form of bar) is melted. The furnace moves along the rod shape sample, meaning that the molten zone is moved along the crystal and the molten zone is moved from one end of the bar to the other. This mechanism is widely used in alloys, however solute atoms tend to segregate to the melt. In this type of alloy, the impurities also concentrate in the melt, and move to one end of the sample along with the moving molten zone. Therefore, zone melting is used most extensively for commercial material refining. Fig. 1. shows how the high-impurity molten-zone moves from one side of the bar to the other. The vertical axis is the impurity concentration and the horizontal axis is the sample length. Due to the tendency for impurities to segregate to the molten region, its concentration in the melt is higher than in the solid. Therefore, as the molten materials travel to the end of bar, the impurity will be transported to the end of bar and leave the high purity solid material behind it.

Figure 1
Figure 1: Schematic of the composition change during zone melting directional solidification.

In this study, a zone melting directional solidification apparatus will be employed to synthesize stable structures of Pb-Cd alloys.


In addition to material refining, zone melting directional solidification is capable of developing stable microstructures. However, having a diffusion process in the liquid (close to the solid liquid interface) may cause mixing and a convection current in the melt, leading to unstable microstructure formation. Stable phase development is particularly important in peritectic reactions.

Fig. 2 shows a schematic of a peritectic reaction in a phase diagram. As it has been demonstrated in Fig. 2, a peritectic reaction is a solidification reaction in which a solid phase (e.g. α) and liquid phase (L) will together form a second solid phase (β) as it is cooled (L +α β).The arrow in the figure shows the cooling process and how phases form.

Figure 2
Figure 2: Schematic of peritectic reaction in a phase diagram.

Banding (Fig. 3), is a common structure in directionally solidified peritectic alloys at relatively lower growth rates resulting from oscillatory modes of convection in the liquid. The liquid, close to the growing interface, is undercooled with respect to the other phase. Therefore, the primary phase cannot reach steady state, while the second phase nucleates and grows ahead of the primary phase. In a similar way, the primary phase prevents the second phase from reaching steady state by nucleating during the transient growth regime of the second phase leads toalternate bands of α and β phases, formed nearly parallel to the planner interface in the peritectic system. Banding structures have been observed in many peritectic systems including Fe-Ni, Sn-Cd, Zn-Cu, Sb-Sn, and Pb-Bi. The width of individual layer, space between them and their stability are highly influenced by growth velocity and nucleation temperature. In addition, composition ranges and convection in the liquid can alter the layer structure.

Figure 3
Figure 3: Schematic of banded structure (white: α, black: ß, G.D.: Growth Direction).

In this study, we aim to employ the zone-melting directional solidification furnace with a mechanism to avoid the influence of convection. The furnace (Fig. 4.) has been designed and developed here at UConn. The process of solidification is in vertical direction. Therefore, if the solute has more density, it migrates bellow the melt. Then, a chill zone right after the furnace freezes the melted materials before they have enough time for convection/mixing. Therefore, this technique is limited to alloys with relatively heavy solute.

Alloys from Pb-Cd, Pb-Bi or Sn-Cd system should be directionally solidified at different thermal gradient and velocity in order to establish the growth conditions for mentioned systems in which diffusion in the solid phases is relatively slow. All samples should be made from pure metals (initial purity more than 99.99%).

Figure 4
Figure 4: Zone melting-freezing directional solidification furnace, developed at UConn.

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  1. Insert a 100 µm chromel-alumel thermocouple (in a 0.1 cm double bore mullite protection tube) in an 8 mm outside diameter Pyrex tube. The tube length should be around 30 cm. The thermocouple tip should be coated with a boron nitride slurry.
  2. Form rods of the desired composition by first melting the alloy in a crucible, and drawing the molten alloy into the Pyrex tube by means of a partial vacuum. For this, use a bulb attached to the end of the Pyrex tube to suck the melt into the tube.
  3. Place the sample in the vertical resistance zone melting and freezing apparatus (Fig. 4). The distance between the heating element and the following chill is set at 0.5 cm.
  4. Run the furnace to move vertically from bottom to top. At least three directional zone melting freezing pass is suggested.
  5. Remove the sample from the Pyrex tube (break the tube) and polish it for microstructure characterizations. For polishing, use the three-step SiC papers (600, 800 and 1200) followed by three steps of Alumina/colloidal silica abrasive particles (3µm, 1µm and 0.05 µm).
  6. Analyze the microstructures using optical microscopy.

Zone melting directional solidification is a metallurgical method employed to prepare stable phases in solid materials. During the solidification process, a melted alloy cools into various phases that form the solid. Using a directional solidification furnace, the process of phase formation and stabilization inside a solid material, is well controlled. This video will illustrate the principles of directional solidification and show how to apply them in the laboratory setting, to develop stable microstructures in a solid sample.

To begin, let us have a closer look at the process of solidification itself, which involves the cooling of a liquid. As the temperature decreases, particles of the liquid move slower and start to nucleate, to form what is called "the solid phase." This principle is illustrated in a phase diagram that shows the different phases of the material as the temperature varies. In the vicinity of the solid-liquid interphase, the process of particle diffusion in the liquid occurs. This may cause mixing, and a convection current in the melt, leading to the formation of unstable microstructures. The alloy in this video is formed of two types of solid phases: an alpha phase, and a beta phase. In the particular case of a peritectic reaction, a solid phase alpha interacts with a liquid, to form a second solid-phase beta. At low growth rate, alternating bands of alpha and beta phases form.

This is called the "banding process." The banding structure is the result of the oscillatory modes of convection inside the liquid. The composition range, the convection in the liquid, the nucleation temperature, and the growth velocity will dictate the characteristics of the banding results. These are defined by the width of the individual bands, the space between them, and their stability. Using a zone melting-freezing furnace in a vertical direction, is a neat way to control the solidification process. In this experiment, a solid is moved to the furnace where a liquid is prepared, then it is transferred immediately to a cooling zone that freezes the melted material. This transition can be performed rapidly enough to avoid the convection inside the liquid phase. The thermal gradient between the hot and cold zones and the velocity can be easily adjusted to control the growth conditions of the solid phases. We will now see how these principles apply in an experiment using a zone-melting directional solidification furnace.

First, take a 30cm long Pyrex tube, having an 8mm outside diameter. Choose a 100-micron Chromel Alumel thermocouple, covered in a 0.1cm double-bore mullite protection tube and having its tip coated with a boron-nitride slurry. Then carefully insert the thermocouple in the Pyrex tube. Next, weigh the alloy samples and place them in a crucible. Leave the crucible inside a furnace until the alloy is melted. Attache a bulb to the end of the Pyrex tube, then use the bulb to apply suction and draw the melt into the glass tube. The rode formed inside the tube will be used in our next experiment.

Place the sample inside the custom-built apparatus specifically designed and developed for vertical solidification. This setup consists of a furnace sandwiched between two cooling systems. The distance between the heating element and the following Cho Zone is set at 0.5cm. Connect the thermocouple to the data acquisition module and then connect this module to the computer. From the bottom to top, proceed to a vertical run of the furnace. Record the run time and determine the velocity of the furnace movement along the Pyrex tube. Determine the thermal gradient by taking the difference between the temperature of the melted alloy inside the furnace, and the temperature in the chill zone.

First, break the glass tube to remove this sample. Use the band saw to cut the sample into the desired length, and then mount the sample using epoxy resin. Proceed to polishing the sample in the following steps. First, use a silicon-carbide paper of grade 600, then polish with a silicon-carbide paper of grade 800, and finally of grade 1200. Now use Alumina Abrasive Particles to finish the polishing. Use, in order, 3-micron, 1-micron, and 0.05-micron size particles. The sample is now ready to be analyzed by imaging its microstructures. Using an optical microscope, images of a lead-55 cadmium alloy sample are obtained in longitudinal and transversal axes. Microstructures are revealed, which originate from directional zone melting solidification.

Let's now take a look at the images obtained. Longitudinal and transverse micrographs of lead-55 cadmium alloy sample show composite-like microstructures develop during zone-melting directional solidification. These microstructures depend on the thermal gradient and velocity ratio. First, from a measurement at low ratio, one sees branched dendrites, and cells of alpha phase, in the matrix of beta phase. Second, at moderate ratio, aligned, stable, unbranched microstructures of alpha phase in matrix of beta phase are developed.

The zone melting freezing directional solidification furnace is a powerful tool to control the development of stable microstructures in materials for various applications. In this metallurgical process, the furnace moves along the rod-shaped sample and melts a narrow region of the solid. Since the impurities tend to segregate inside the melt, they are moved to one end of the sample, along with the moving molten zone. Thus, the zone melting freezing directional solidification furnace is routinely used in commercial alloy refining. The solar panels technology also takes advantage of alloys with stable solid phases. In fact, high quality semi-conductors are essential to ensure longer bulk lifetime and increase the efficiency of solar cells.

You've just watched JoVE's introduction to directional solidification and phase stability. You should now understand how microstructure development in materials is controlled with a directional solidification furnace, based on the zone melting and freezing principal. Thanks for watching.

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Figs. 5 and 6 show the microstructures developed from directional zone melting solidification of Pb-55Cd alloy revealed by optical microscope, at two different G/V ratios (G: thermal gradient, V: velocity of the furnace movement along the Pyrex tube).

At low ratio (G/V=1.03×106 (oC.Sec/Cm2)) the microstructure consisted of branched dendrites of α phase in the matrix of ß phase. At moderate G/V ratio (G/V=1.55×106 (oC.Sec/Cm2) however, aligned stable microstructures (unbranched dendrites or cells) of α phase in matrix of ß phase are developed.

Figure 5
Figure 5: Longitudinal (left) and transverse (right) micrographs of Pb-55Cd alloy, taken at low ratio G/V=1.03×106 (oC.Sec/Cm2), showing how the stable microstructures develop during zone melting directional solidification.

Figure 6
Figure 6: Longitudinal micrograph of Pb-55Cd alloy, taken at moderate ratio G/V=1.55×106 (oC.Sec/Cm2), and showing how the aligned stable microstructures develop during zone melting directional solidification.

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Applications and Summary

This experiment demonstrates to employ a specific type of zone melting freezing directional solidification furnace to develop stable microstructures. Unlike the two phase unstable microstructure that is not in equilibrium at room temperature and the structure degrade over a period of months by diffusion at room temperature, the single phase structure obtained in sample grown does not undergo any change.

Sample with stable phases, developed by mentioned furnace may have wide applications in various industries including biosensors and semiconductors in which alloys with stable phases are necessary to avoid degradation during long time application. Moreover, the furnace may be employed at researches aimed to find the influence of convection on stable and metastable phase's formations.

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Directional Solidification Phase Stabilization Metallurgical Method Solidification Process Melted Alloy Directional Solidification Furnace Phase Formation Stabilization Solid Material Microstructures Cooling Of A Liquid Nucleation Solid Phase Phase Diagram Particle Diffusion Convection Current Stable Microstructures Alpha Phase Beta Phase Peritectic Reaction Banding Pro

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