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Sprueing of wax patterns and some notes on the metaHurgy of the process

Much time and attention has been spent in considerations of how toenhance the quality and reliability of the casting process, but very little regard has been paid to the process of solidification of the alloys used which is absolutely crucial for the final quality.

Melting is an extremely traumatic condition for any metallic alloy and, to restore its original, pre-melt, condition, it is essential that, during solidifaction, it recreates its original crystalline structure. A brief explanation here may be of interest.

A typical gold alloy is composed of many billions of atoms of gold, silver, copper and other consitutants. When the alloy is a solid, all of these atoms are bonded together in a fied relationship, but not stationary.

If imaginary lines are drawn joining the centres of each atom, regular geometrical shapes are the result; this is known as the crystalline structure. One can imagine this in

casting ? good or bad ? depend exclusively on the subsequent solidification, which can broadly be compared to the freezing of water.

Solidification, or freezing, starts from the walls of the container and progresses towards the centre. At a certain point in this process it is thus possible to identify a solid phase, a liquid phase and a viscous phase. Impurities in particle form tend to be progressively pushed towards the section which solidifies last.

As the melt cools, solidification develops throughout the liquid mass as groupings of crystals in three dimensions, propagating in fir?tree

and the waxes should be checked to ensure that they are free of these surface inclusions. When using vacuum injection

nhance the quality and reliability the form of adjacent cubes with an f the casting process, but very atom at each comer (figs. 20 & 21).

ttle regard has been paid to the As previously stated, the atoms are rocess of solidification of the not stationary but in a permanent

Iloys used which is absolutely state of balanced oscillation, the rucial for the final quality. amplitude of which is elated to the elting is an extremely traumatic kinetic energy of the component ondition for any metallic alloy and, atoms and determines the hardness
o restore its original, pre?melt, con? of the alloy. This oscillation exists ition, it is essential that, during even at O’C and diminishes down to
olidification, it recreates its original absolute zero at ?273’C. With a rise stalline structure. A brief expla? in temperature, this oscillation
ation here may be of interest. increases in amplitude, the crystal typical gold alloy is composed line structure dilates, and the metal
f many billions of atoms of gold, thus expands. When this amplitude silver, copper and other constitu? exceeds a certain level, the atomic
nts. When the alloy is a solid, all bonds are ruptured and the crystal if these atoms are bonded together line structure breaks down (fig. 22);
n a fixed relationship, but not the alloy then becomes a liquid.

tationary.

page 23

The metallurgical properties of the forms known as "dendrites" (after the acient Greek word for tree). Those that grow in a direction opposite to the diffusion of heat are known as "columnar dendrites" and when growth is irregular and disorderly are known as "equiaxial dendrites".

Figures 23 and 24 depict the external face of the alloy in solid black, the solidifying sections in small squares and the still liquid section in white.

As the dendrites grow they broaden and form a myriad of microscopic islets which, upon solidification, weld together forming a granular structure which may be clearly observed under a microscope. Each granule represents a section of the alloy which has solidified crystallising in a given direction.

The left?hand section of figure 25 depicts an equiaxial dendrite; the right?hand section depicts a columnar dendrite. Figure 26 shows a typical microscopic view of metallic granular configuration.

If cooling of the metal after casting does not occur in a well?defined direction, irregular faults will inevitably occur in the component.

We will now examine this process on the microscopic (as opposed to atomic) level.

The black portion of figure 26 shows the growth of dendrites forming the grain structure. Very small inclusions or impurities are about to be trapped and the empty spaces will become typical voids or porosity.

The crosshatched area depicts the

section which is still liquid. If contamination of the melt has occurred during the melting/casting process by foreign bodies, oxides or gaseous inclusions, these will remain trapped between the grains at point of solidification and degrade the metallurgical characteristics of the component that has been thus badly cast These contaminants will nersist

through any subsequent remelting of the material.

To summarise, good solidification depends on these factors:

1) Heat diffusion

2) Contamination during melting/ casting

3) Formation of the various phases

4) The number of initial nuclei of crystallisation

5) The type of dendritic growth (columnar and equiaxial).

From the preceding, it is quite easy to understand the types of factors that may produce porosity in castings. The causes, excepting contamination (which may be eliminated by taking care not to introduce impurities) are exclusively to do with the manner of cooling and solidification. Therefore, conditions must be established to ensure that:

A ? The component is continuously as c anges in qui to so

B ? Solidification takes place uniformly and gradually.

To ensure that the first condition is met, it is always necessary to provide a "thermal reservoir" capable of supplying, without interruption, molten metal during all the progressive contractions of the solidifying component. One may think in terms of a metal feed tank in the centre sprue (in the case of "tree" sprueing) or within the base in the case of "button" sprucing (fig. 27).

Immense importance attaches to the dimensional relationships of the

centre sprue or base and the individual sprues or runners connecting them to the patterns.

The fact that must be borne in mind is that the metal within the feeder system remains liquid longer than that in the patterns. It is interesting to consider here the case of dental lost?wax castings where porosity is absolutely inadmissable due to possibilites of ingress of bacteria and other micro?organisms.

Figure 28 shows the size of the feeder system provided for casting relatively small toothshaped patterns. It is necessary to remember that the vast majority of alloys melt and sol? idify over a range of temperatures. Diagrams in figure 29 show the cooling curves of some gold/silver (Au?Ag) alloys indicating the respective "heatsoaking interval". Point "S" indicates the start of sol idification while point "F" marks completion of solidification. Fine gold and fine silver solidify at a precise temperature, whereas their

various alloys solidify within a ?ange of temperatures known as the ’heatsoaking interval" or "melting .?ange". The contraction from liquid o solid is represented in figure 30 xhich also depicts the progressive eduction of the mass during tem)erature variation.

1 . By contraction at liquidus (from )oint "D" to point "C" we mean the eduction of the metal mass when )assing from casting temperature to ?netting temperature. Casting tem)efuture is always higher thari melting emperature otherwise the molten rietal will not have sufficient fluidity o fully occupy the mould.

rhere can be a difference between hese temperatures of 50’C ? 150’C lependent upon the type of alloy ind the type of item to be cast.

2 . Heatsoaking contraction (point ’C" to "B") takes place during the nterval from casting temperature to netting temperature. This phase indergoes the greatest mass reducion and thus requires the maximum ittention.

3. Contraction in the solid state point "B" to point "A") takes place vhen the solidified mass cools town to ambient temperature from olidification temperature "B".

rhese contraction processes may ause voids in the cast patterns inown as "shrinkage porosity" vhen these are relatively massive nd "microporosity" when small ind dotlike. Diffuse microporosity mmediately sub?surface are prouced by inclusions of air or gas enerated by investment and trapped hiring solidification. More attention o this phenomenon will be given iarther on. The contraction process as such a strong bearing on the ultinate quality of the castings that we fraw attention to the following dia,rarns:

Figure 31 shows the manner in which shrinkage porosity forms after mass contraction if the solidifying casting is starved of farther molten metal.

Figure 32 shows the solidification process within a correctly fed mould. The sprueing system allows adequate feeding during solidification and no porosity results in the cast item.

If the sprue size is not adequate to permit continuous feeding until solidification is complete, the results may be as depicted in figure 33.

Another factor of equal importance to the size of the sprue is its location

on the cast pattern. As a general rule, the sprue should be attached to the most massive part of the pat

tem and provision be made for a reservoir of molten metal to feed thin, remote, sections (fig. 34).

If these thin, remote, sections are adequately fed with molten metal, porosity will not be experienced (fig. 35).

The foregoing section concerning sprueing principles and techniques is of importance with regard to metal feeding. We shall now examine how to achieve uniform cooling of the casting, from the exterior to the interior.

A ? The central stem of the "Tree" at the centre of the flask is the principal thermal reservoir and its size must, thus, be proportional to the

weight and size of the patterns. Some practitioners in this field assert that a tapered form is the most appropriate in order to avoid excessive recycling of precious metal with consequent "losses". Also, hot metal inevitably reached the top of the "tree" first and, thus, the lower part, where the metal arrives at a slightly lower temperature, requires the larger cross?section.

36 ? Incorrect sprucing
3 7 & 38 ? Correct sprueing
39 ? Incorrect sprueing
40 ? Correct sprucing
41 ? Sprue systems joined to central "tree
(left?hand: correct, right?hand: incorrect)

B ? It is important that all of the pattems in a given flask are of a similar size, mass and cross?section.

 

C ? Patterns should be attached to the central stem in a clean, fidy and regular fashion.

D ? The overall diameter of the

assembled "tree" must be in relation to the internal diameter of the flask. Ideally, there should be a clearance of 10? 15 mm between the outermost patterns and the inside of the flask.

E ? Flask temperature at the moment of casting must be determined by pattern profile.

F ? It is desirable that cooling of the molten metal should take place from one side only of the flask, developing in one direction. Our vacuum system built in to the casting arm is of value here, creating suction at the opposite end of the flask to that at which the metal is injected, not only satisfying the foregoing condition, but also removing harmful gases generated by the metal impacting the investment. This point will be dealt with in more detail later.

Figure 43 depicts the result of progressive cooling without the harniful phenomena described earlier. It must be home in mind that all of the phases described in this sectionoccur in a very brief interval of time and are influenced by metal temperature, alloy composition, flask temperature, profile of the casting patterns and ? above all ? the method of casting employed.