3. Results and discussion

Porosity is one of the most common defects in aluminum cast parts caused mostly due to insufficient feeding and hydrogen precipitation during solidification. The amount of dissolved hydrogen in cast Al-Si alloys can be kept very low by degassing the melt. However, shrinkage porosity can still be a problem in the cast parts caused by non-proper feeding ability. Consequently, understanding the feeding behavior of hypoeutectic Al-Si-Cu alloys is an important aspect of sound casting production. In this paper, the impact of various contents of Si and Cu on different feeding regions has been analyzed by applying the TA technique. The main objective of this work was to better understand their impact on the feeding ability of Al-Si-Cu alloys and to quantify each feeding region regarding the characteristic solidification temperatures and/or the corresponding amount of fraction solid precipitated between those temperatures.

Quantification of Feeding Regions of Hypoeutectic Al-(5, 7, 9)Si-(0-4)Cu (wt.%) Alloys Using… DOI: http://dx.doi.org/10.5772/intechopen.90337

### 3.1 Analysis of characteristic solidification temperatures

The results of the cooling curve analysis are summarized in Table 2. The values of characteristic solidification temperatures (Tliq, TDCT, TRigidity and Tsol) have been determined from the cooling curves or their corresponding first derivatives curves. The dendrite coherency [3] and rigidity [12] temperatures have been determined by applying the two thermocouples method (one thermocouple located at the center


Two sets of the characteristic temperatures have been collected for each analyzed alloy (two cooling curves have been collected for each alloy).

#### Table 2.

Characteristic solidification temperatures of Al-(5, 7, 9)Si-(0–4)Cu (wt.%) alloys determined using cooling curve analysis.

5 mm away from the cup inner wall. They recorded temperature during solidification of an investigated alloy (especially between 750 and 400°C temperature range). The National Instrument data acquisition system has been applied to collect temperature-time data. During all trials, the sampling rate was five data per second. The cooling conditions were maintained constant during all experiments, but due to various Si and Cu contents, the solidification rates slightly varied between maximal 0.26°C/s for Al-5Si-4Cu (wt.%) alloy and minimal 0.11°C/s for Al-9Si (wt.%) alloy. The cooling rate has been calculated as the ratio of the temperature difference between Tliq and Tsol to the total solidification time between these two temperatures. Each TA trial was repeated two times. Consequently, a total of 50 cooling

Actual chemical composition (in wt.%) of synthetic Al-Si-Cu alloys.

Alloy Si Cu Al-5Si 4.96 0 Al-5Si-1Cu 5.22 1.12 Al-5Si-2Cu 5.12 1.88 Al-5Si-3Cu 5.08 3.11 Al-5Si-4Cu 5.01 4.30 Al-7Si 6.80 0 Al-7Si-1Cu 7.32 0.89 Al-7Si-2Cu 7.32 2.04 Al-7Si-3Cu 7.32 3.28 Al-7Si-4Cu 7.13 4.30 Al-9Si 8.80 0 Al-9Si-1Cu 8.93 0.92 Al-9Si-2Cu 8.93 2.17 Al-9Si-3Cu 8.82 2.93 Al-9Si-4Cu 8.92 4.02

Porosity is one of the most common defects in aluminum cast parts caused mostly due to insufficient feeding and hydrogen precipitation during solidification. The amount of dissolved hydrogen in cast Al-Si alloys can be kept very low by degassing the melt. However, shrinkage porosity can still be a problem in the cast parts caused by non-proper feeding ability. Consequently, understanding the feeding behavior of hypoeutectic Al-Si-Cu alloys is an important aspect of sound casting production. In this paper, the impact of various contents of Si and Cu on different feeding regions has been analyzed by applying the TA technique. The main objective of this work was to better understand their impact on the feeding ability of Al-Si-Cu alloys and to quantify each feeding region regarding the characteristic solidification temperatures and/or the corresponding amount of fraction solid precipi-

curves were gathered.

Table 1.

Mass Production Processes

3. Results and discussion

tated between those temperatures.

24

(Tc) and second (Tw) placed nearby the inner wall of test cup). Characteristic solidification parameter such as dendrite coherency point (DCP) has determined by identifying the first local minimum on the delta T curve (ΔT ¼ T<sup>w</sup> � Tc) plotted versus time. The dendrite coherency temperature (DCT) has detected by reading the temperature on the cooling curve for the corresponding time related to dendrite coherency point [3]. It has recently been found that the second local minimum on the ΔT versus time curve is related to the TRigidity [12]. The reason that DCP and rigidity occur at these minimums of the ΔT curve is because the heat removal from the solid is faster than from the liquid phase. This is due to the significantly higher thermal conductivity of the solid dendrites by DCP and solid dendrites and eutectic cells by rigidity in comparison to the surrounding liquid metal.

that any increase in the content of Si and Cu significantly depressed the liquidus, dendrite coherency, and rigidity temperatures, while solidus temperature is less prone to their influence. According to the results obtained using the cooling curve analysis, the increase in Si content by one weight percent depresses the Tliq to 8.5°C by the constant content of Cu. The experimental result indicated the stronger impact of Si on the Tliq in comparison with that obtained using the binary Al-Si phase diagram. Calculated from the binary phase diagram, increase of Si content up to eutectic concentration (12.0 wt.%) decreases the Tliq by 83°C (the temperature drops almost linearly from 660 to 577°C), which is approximately a decrease of 7°C per 1 wt.% of Si. One weight percent of Cu by constant content of Si decreases the Tliq by approximately 4.4°C, which is a higher value than expected according to the equilibrium binary Al-Cu phase diagram (3.4°C/1 wt.% of Cu). The most plausible reason for these differences can be found in the fact that in all experiments, a limited range of Si (up to 8.9 wt.%) and Cu (up to 4.3 wt.%) content has been analyzed in comparison with significantly broader concentration ranges (up to 12 wt.% for Si and up to 33 wt.% for Cu) taken from the binary Al-Si and Al-Cu phase diagrams. At the same time, the impact of higher cooling rates during some experiments (0.26°C/s) cannot be disregarded, which certainly depressed the Tliq

DOI: http://dx.doi.org/10.5772/intechopen.90337

Quantification of Feeding Regions of Hypoeutectic Al-(5, 7, 9)Si-(0-4)Cu (wt.%) Alloys Using…

During the solidification of any aluminum hypoeutectic Al-Si-Cu alloys, a dendritic network of primary α-aluminum crystals will be developed. However, as the melt cools, the dendrite tips of the growing crystals begin to impinge upon one another until a coherent dendritic network is formed [4]. The temperature at which the dendrite tips start to touch each other is called dendrite coherency temperature TDCT. This temperature is a very important feature of the solidification process because it marks the moment when the "mass" feeding is transferred to the

interdendritic feeding [33–42]. According to many researchers, casting defects such as macrosegregation, shrinkage porosity and hot tearing begin to develop after the TDCP [33–37]. The solidification conditions, the chemical compositions of alloy and the addition of grain refiners are major factors that have a significant impact on the DCT. Regardless of the applied measurement techniques, it has been verified that faster cooling rate and increase in solute concentration postponed the coherency point for the lower temperature [36, 37, 41]. From Table 2 and Figure 3, it is obvious that the higher Si and Cu contents progressively reduce the DCT. The impact of Si is more significant than that of Cu. For the Cu free alloys, 1 wt.% of Si decreases the DTC to 7.2°C, while by alloys with various content of Cu (from 1 to 4 wt.%) that decrease is slightly higher and is approximately 7.9°C. Each increase in the Cu content by 1 wt.% in analyzed alloys will decrease the DCT to approximately 3.2°C. These results are not unexpected and are consistent with the available literature data [37, 39]. According to literature data, the size of secondary dendrite arms mostly depends on the local cooling rates and the amount of alloying elements present in the melt. The impact of the local cooling rate is very well studied; a higher cooling rate relates to the smaller dendrites and vice versa. The effect of alloying elements on the size of dendrite arm spacing needs to be also considered due to their not even distribution in the liquid and solid phases. Excess amount of solute displaced away from the solidification interface into the melt results in an increase in the volume of solute located between already formed dendrite arms. The resulted constitutional undercooling (supersaturation) is an additional driving force for the growth of the dendrites. In order to accommodate an excess amount of solute elements, the space between primary α-aluminum dendrites must be increased. The higher concentration of alloying elements will reduce the growth of secondary dendrites and postpone their contact-coherency to lower temperature. Based on the

to a lower value.

27

The Tliq specifies the maximal temperature at which the crystal can coexist with the melt in thermodynamic equilibrium. Above the Tliq there is not a single crystal and the melt is liquid and homogeneous. From Table 2 and Figure 3, it is evident

#### Figure 3.

The impact of Si on the characteristic solidification temperature: (a) Al-(5, 7, 9)Si-0Cu (wt%), (b) Al-(5, 7, 9)Si-1Cu, (c) Al-(5, 7, 9)Si-2Cu (wt%), (d) Al-(5, 7 9)Si-3Cu (wt%) and (e) Al-(5, 7, 9)Si-4Cu (wt%) alloys.

Quantification of Feeding Regions of Hypoeutectic Al-(5, 7, 9)Si-(0-4)Cu (wt.%) Alloys Using… DOI: http://dx.doi.org/10.5772/intechopen.90337

that any increase in the content of Si and Cu significantly depressed the liquidus, dendrite coherency, and rigidity temperatures, while solidus temperature is less prone to their influence. According to the results obtained using the cooling curve analysis, the increase in Si content by one weight percent depresses the Tliq to 8.5°C by the constant content of Cu. The experimental result indicated the stronger impact of Si on the Tliq in comparison with that obtained using the binary Al-Si phase diagram. Calculated from the binary phase diagram, increase of Si content up to eutectic concentration (12.0 wt.%) decreases the Tliq by 83°C (the temperature drops almost linearly from 660 to 577°C), which is approximately a decrease of 7°C per 1 wt.% of Si. One weight percent of Cu by constant content of Si decreases the Tliq by approximately 4.4°C, which is a higher value than expected according to the equilibrium binary Al-Cu phase diagram (3.4°C/1 wt.% of Cu). The most plausible reason for these differences can be found in the fact that in all experiments, a limited range of Si (up to 8.9 wt.%) and Cu (up to 4.3 wt.%) content has been analyzed in comparison with significantly broader concentration ranges (up to 12 wt.% for Si and up to 33 wt.% for Cu) taken from the binary Al-Si and Al-Cu phase diagrams. At the same time, the impact of higher cooling rates during some experiments (0.26°C/s) cannot be disregarded, which certainly depressed the Tliq to a lower value.

During the solidification of any aluminum hypoeutectic Al-Si-Cu alloys, a dendritic network of primary α-aluminum crystals will be developed. However, as the melt cools, the dendrite tips of the growing crystals begin to impinge upon one another until a coherent dendritic network is formed [4]. The temperature at which the dendrite tips start to touch each other is called dendrite coherency temperature TDCT. This temperature is a very important feature of the solidification process because it marks the moment when the "mass" feeding is transferred to the interdendritic feeding [33–42]. According to many researchers, casting defects such as macrosegregation, shrinkage porosity and hot tearing begin to develop after the TDCP [33–37]. The solidification conditions, the chemical compositions of alloy and the addition of grain refiners are major factors that have a significant impact on the DCT. Regardless of the applied measurement techniques, it has been verified that faster cooling rate and increase in solute concentration postponed the coherency point for the lower temperature [36, 37, 41]. From Table 2 and Figure 3, it is obvious that the higher Si and Cu contents progressively reduce the DCT. The impact of Si is more significant than that of Cu. For the Cu free alloys, 1 wt.% of Si decreases the DTC to 7.2°C, while by alloys with various content of Cu (from 1 to 4 wt.%) that decrease is slightly higher and is approximately 7.9°C. Each increase in the Cu content by 1 wt.% in analyzed alloys will decrease the DCT to approximately 3.2°C. These results are not unexpected and are consistent with the available literature data [37, 39]. According to literature data, the size of secondary dendrite arms mostly depends on the local cooling rates and the amount of alloying elements present in the melt. The impact of the local cooling rate is very well studied; a higher cooling rate relates to the smaller dendrites and vice versa. The effect of alloying elements on the size of dendrite arm spacing needs to be also considered due to their not even distribution in the liquid and solid phases. Excess amount of solute displaced away from the solidification interface into the melt results in an increase in the volume of solute located between already formed dendrite arms. The resulted constitutional undercooling (supersaturation) is an additional driving force for the growth of the dendrites. In order to accommodate an excess amount of solute elements, the space between primary α-aluminum dendrites must be increased. The higher concentration of alloying elements will reduce the growth of secondary dendrites and postpone their contact-coherency to lower temperature. Based on the

(Tc) and second (Tw) placed nearby the inner wall of test cup). Characteristic solidification parameter such as dendrite coherency point (DCP) has determined by identifying the first local minimum on the delta T curve (ΔT ¼ T<sup>w</sup> � Tc) plotted versus time. The dendrite coherency temperature (DCT) has detected by reading the temperature on the cooling curve for the corresponding time related to dendrite coherency point [3]. It has recently been found that the second local minimum on the ΔT versus time curve is related to the TRigidity [12]. The reason that DCP and rigidity occur at these minimums of the ΔT curve is because the heat removal from the solid is faster than from the liquid phase. This is due to the significantly higher thermal conductivity of the solid dendrites by DCP and solid dendrites and eutectic

The Tliq specifies the maximal temperature at which the crystal can coexist with the melt in thermodynamic equilibrium. Above the Tliq there is not a single crystal and the melt is liquid and homogeneous. From Table 2 and Figure 3, it is evident

The impact of Si on the characteristic solidification temperature: (a) Al-(5, 7, 9)Si-0Cu (wt%), (b) Al-(5, 7, 9)Si-1Cu, (c) Al-(5, 7, 9)Si-2Cu (wt%), (d) Al-(5, 7 9)Si-3Cu (wt%) and (e) Al-(5, 7, 9)Si-4Cu (wt%)

cells by rigidity in comparison to the surrounding liquid metal.

Mass Production Processes

Figure 3.

alloys.

26

previously mentioned, it could be assumed that elements with a lower solubility in the aluminum melt are more effective in reducing the size of secondary dendrite arm spacing (SDAS). Therefore, the effect of the same content of Cu (max. solubility in Al is 5.7 wt.%) is significantly lower than the effect of the same amount of Si (max. solubility in Al is 1.6 wt.%).

volume fraction of phases formed prior to quenching in a set of melt specimens obtained between the Tliq and Tsol. This technique requires the use of small samples that have rapid cooling rates in order to preserve the structure present at a given temperature. Small test samples and rapid cooling rates minimize structural transformation during quenching and thus maximize the accuracy of this measurement procedure. Another approach for determining fraction solid makes use of the TA technique [3, 4, 17, 25, 26, 28–30, 43–52]. The amount of heat evolved from a solidifying test sample can be calculated as the integrated area between the first derivative curve and the zero line. The amount of heat is proportional to the fraction solid. Differential thermal analysis (DTA) and differential scanning calorimetry (DTC) have also been used for the determination of solid fraction. However, these techniques are not suitable for industrial applications because they require complicated and expensive instrumentation as well as rigid and precise test procedures that are only possible in a laboratory environment. The literature also suggests a number of models for the calculation of fraction solid (more details can be find in Table 3). Most of them are based on parameters derived from the fundamental analysis of the solidification process for simple alloy systems. Due to the highly complex nature of alloy solidification, many questionable assumptions

Quantification of Feeding Regions of Hypoeutectic Al-(5, 7, 9)Si-(0-4)Cu (wt.%) Alloys Using…

The TA technique has been applied in this work to calculate the distribution of fraction solid between the Tliq and Tsol during solidification of investigated alloys.

> LEVER RULE [30}

GRAIN NUCLEATION [32, 37]

HEAT BALANCE [9, 10, 35, 37]

LINEAR [30] Latent heat is assumed to vary

simplicity.

mushy zone.

SCHEIL'S [30] In this model, it is assumed that

spherical.

(zc).

linearly between liquidus and solidus temperatures. This model has no theoretical basis but is frequently used due to its

Solidification in this model is assumed to progress very slowly and the solid and liquid phases coexist in equilibrium in the

no solute diffusion occurs in the solid phase and also that the liquid is perfectly homogeneous.

The calculation of fraction solid is based on the grain nucleation law and on the assumption that the shape of the grains is

Fraction solid can be calculated by determining the cumulative area between the first derivative of the cooling curve (cc), and the "zero" cooling curve (hypothetical cooling curve without phase transformations)

(see Table 3, comments) have been made in these models.

1. <sup>f</sup><sup>s</sup> <sup>¼</sup> <sup>T</sup>liq�<sup>T</sup> Tliq�Tsol

2. <sup>f</sup><sup>s</sup> <sup>¼</sup> <sup>1</sup> 1�k Tliq�T Tm�T <sup>k</sup> <sup>¼</sup> <sup>T</sup>m�Tliq Tm�Tsol

3. TAlSi

5.

Table 3.

29

TAlSi <sup>E</sup>,G ; f<sup>s</sup> ¼ 1

f<sup>s</sup> ¼ Ðt 0

dT

Ðts 0

dt—cooling rate

<sup>E</sup>,G <T <Tliq <sup>f</sup><sup>s</sup> <sup>¼</sup> <sup>1</sup> � <sup>T</sup>m�<sup>T</sup> <sup>T</sup>m�Tliq � � <sup>1</sup> k�1

4. <sup>f</sup><sup>s</sup> <sup>¼</sup> <sup>1</sup> � exp � <sup>4</sup>

Tliq—liquidus temperature, °C Tsol—solidus temperature, °C T—instantaneous temperature, °C

DOI: http://dx.doi.org/10.5772/intechopen.90337

k—distribution coefficient of binary alloys Tm—melting temperature of pure aluminum

<sup>3</sup> <sup>π</sup>R<sup>3</sup><sup>N</sup> � � R—average grain radius, m N—average grain density, m�<sup>3</sup>

> ¼ cp L Ðt 0 dT dt � � CC � dT dt � � ZC h idt

dT ð Þ dt CC� dT ð Þ dt ZC ½ �dt

dT ð Þ dt CC� dT ð Þ dt ZC ½ �dt

cp—specific heat of an alloy L—latent heat of solidification

Review of models for calculation of fraction solid.

No Type of models Method Comments

The rigidity point/temperature indicates the moment during solidification at which the flow of residual melt through interdendritic channels is completely restricted. As Figure 2 shows, the TRigidit<sup>y</sup> has been determined as the second minimum on the ΔT curve (ΔT ¼ Tw � Tc) that are identified in the region of primary precipitation of Al-Si eutectic. Again, the most likely main reason for this difference is due to different thermal conductivity in solid and liquid phases. The rigidity point indicates the moment when the interdendritic feeding is transferred to burst feeding. According to Campbell [11], after the rigidity point, the stress will exceed the network strength and the dendritic network will collapse.

From Table 2 and Figure 3, it is obvious that any changes in the content of Si have no significant impact on the value of TRigidit<sup>y</sup>. Small changes in this temperature (�0.5°C) could be related to the accuracy of applied thermocouples. On the contrary to that, the addition of Cu (up to 4 wt.%) to Al-Si alloys depressed this temperature to approximately 3.2°C per one weight percentage of Cu. It is interesting to note that by a lower content of Si (5 wt.%) the depression is stronger (�4.0° C/1 wt.% Cu) than by alloys with higher Si (9 wt.%) content (2.5°C/1 wt.% of Cu).

Finally, the Tsol identifies the temperature at which the last portion of the liquid has been transformed into a solid. Below this temperature, the given alloy is stable in the solid phase. The results presented in Table 2 and Figure 3 indicate that various Si and Cu contents in investigated alloys have the lowest impact on solidus temperature. The average Tsol determined using cooling curve analysis, for all investigated alloys, was approximately 500°C.

The addition of Si and Cu into aluminum alloys considerably changes the solidification ranges of these alloys (the difference between Tliq and Tsol). The Al-Si alloys free of Cu, as Figure 3 illustrates, solidified in the temperature range between 80 and 50°C depending on the content of Si. The lower Si content corresponds to the wider solidification interval of these alloys and vice versa. Addition of Cu into Al-Si alloys, as Figure 3 shows, significantly increases their solidification intervals. By lowering the contents of Si (e.g., 5 wt.%) and Cu (e.g., 1 wt.%) this interval is approximately 130°C, getting narrower (�90°C) by increasing the contents of Si (e.g., up to 9 wt.%) and Cu (e.g., up to 4 wt.%). It is well known that casting characteristics of Al-Si-Cu alloys are generally influenced upon adding Cu. The Cu precipitate in the eutectic form during the last stage of solidification prolonging solidification interval of those alloys [31]. It is also well known from the foundry practice that alloys with wider solidification intervals are more prone to the formation of shrinkage porosity.

#### 3.2 Fraction solid analysis

The term fraction solid is related to the amount of solid phase(s) formed during melt solidification between liquidus and solidus temperatures, expressed in percentage. Correct information regarding fraction solid is necessary to accomplish computer simulation of casting feed ability as well as to characterize the solidification process and make a prediction concerning the casting structure.

Various methods for determining the fraction solid of casting alloys are presented in the literature [30–38]. The most commonly used technique employs quantitative metallography. The image analysis system is used to measure the

## Quantification of Feeding Regions of Hypoeutectic Al-(5, 7, 9)Si-(0-4)Cu (wt.%) Alloys Using… DOI: http://dx.doi.org/10.5772/intechopen.90337

volume fraction of phases formed prior to quenching in a set of melt specimens obtained between the Tliq and Tsol. This technique requires the use of small samples that have rapid cooling rates in order to preserve the structure present at a given temperature. Small test samples and rapid cooling rates minimize structural transformation during quenching and thus maximize the accuracy of this measurement procedure. Another approach for determining fraction solid makes use of the TA technique [3, 4, 17, 25, 26, 28–30, 43–52]. The amount of heat evolved from a solidifying test sample can be calculated as the integrated area between the first derivative curve and the zero line. The amount of heat is proportional to the fraction solid. Differential thermal analysis (DTA) and differential scanning calorimetry (DTC) have also been used for the determination of solid fraction. However, these techniques are not suitable for industrial applications because they require complicated and expensive instrumentation as well as rigid and precise test procedures that are only possible in a laboratory environment. The literature also suggests a number of models for the calculation of fraction solid (more details can be find in Table 3). Most of them are based on parameters derived from the fundamental analysis of the solidification process for simple alloy systems. Due to the highly complex nature of alloy solidification, many questionable assumptions (see Table 3, comments) have been made in these models.

The TA technique has been applied in this work to calculate the distribution of fraction solid between the Tliq and Tsol during solidification of investigated alloys.


Table 3. Review of models for calculation of fraction solid.

previously mentioned, it could be assumed that elements with a lower solubility in the aluminum melt are more effective in reducing the size of secondary dendrite arm spacing (SDAS). Therefore, the effect of the same content of Cu (max. solubility in Al is 5.7 wt.%) is significantly lower than the effect of the same amount of Si

The rigidity point/temperature indicates the moment during solidification at which the flow of residual melt through interdendritic channels is completely restricted. As Figure 2 shows, the TRigidit<sup>y</sup> has been determined as the second minimum on the ΔT curve (ΔT ¼ Tw � Tc) that are identified in the region of primary precipitation of Al-Si eutectic. Again, the most likely main reason for this difference is due to different thermal conductivity in solid and liquid phases. The rigidity point indicates the moment when the interdendritic feeding is transferred to burst feeding. According to Campbell [11], after the rigidity point, the stress will

From Table 2 and Figure 3, it is obvious that any changes in the content of Si have no significant impact on the value of TRigidit<sup>y</sup>. Small changes in this temperature (�0.5°C) could be related to the accuracy of applied thermocouples. On the contrary to that, the addition of Cu (up to 4 wt.%) to Al-Si alloys depressed this temperature to approximately 3.2°C per one weight percentage of Cu. It is interesting to note that by a lower content of Si (5 wt.%) the depression is stronger (�4.0° C/1 wt.% Cu) than by alloys with higher Si (9 wt.%) content (2.5°C/1 wt.% of Cu). Finally, the Tsol identifies the temperature at which the last portion of the liquid has been transformed into a solid. Below this temperature, the given alloy is stable in the solid phase. The results presented in Table 2 and Figure 3 indicate that various Si and Cu contents in investigated alloys have the lowest impact on solidus temperature. The average Tsol determined using cooling curve analysis, for all

The addition of Si and Cu into aluminum alloys considerably changes the solidification ranges of these alloys (the difference between Tliq and Tsol). The Al-Si alloys free of Cu, as Figure 3 illustrates, solidified in the temperature range between 80 and 50°C depending on the content of Si. The lower Si content corresponds to the wider solidification interval of these alloys and vice versa. Addition of Cu into Al-Si alloys, as Figure 3 shows, significantly increases their solidification intervals. By lowering the contents of Si (e.g., 5 wt.%) and Cu (e.g., 1 wt.%) this interval is approximately 130°C, getting narrower (�90°C) by increasing the contents of Si (e.g., up to 9 wt.%) and Cu (e.g., up to 4 wt.%). It is well known that casting characteristics of Al-Si-Cu alloys are generally influenced upon adding Cu. The Cu precipitate in the eutectic form during the last stage of solidification prolonging solidification interval of those alloys [31]. It is also well known from the foundry practice that alloys with wider solidification intervals are more prone to the forma-

The term fraction solid is related to the amount of solid phase(s) formed during melt solidification between liquidus and solidus temperatures, expressed in percentage. Correct information regarding fraction solid is necessary to accomplish computer simulation of casting feed ability as well as to characterize the solidifica-

tion process and make a prediction concerning the casting structure.

Various methods for determining the fraction solid of casting alloys are presented in the literature [30–38]. The most commonly used technique employs quantitative metallography. The image analysis system is used to measure the

exceed the network strength and the dendritic network will collapse.

(max. solubility in Al is 1.6 wt.%).

Mass Production Processes

investigated alloys, was approximately 500°C.

tion of shrinkage porosity.

3.2 Fraction solid analysis

28

There are two known methods in the literature, Newtonian [29, 30, 52] and Fourier, [29, 30, 52] that have been successfully used to calculate fraction solid distribution using cooling curve analysis. In order to be capable of applying both methods, it is necessary to define the so-called baseline [29, 30, 52]. The baseline denotes the first derivative curve of the investigated alloy, assuming that melt during solidification process does not undergo any phase transformation. Therefore, it is to expect that base and first derivative curves are overlapping each other in the areas before liquidus (single liquid phase) and after solidus (single solid phase) temperatures. In this paper only the Newtonian method has been applied for calculating the base line using cooling curve analysis.

Table 4 and Figure 4 summarize the impact of various content of Si and Cu on the distribution of fraction solid at characteristic solidification temperatures (Tliq, TDCT, TRigidity and Tsol). For Cu free Al-Si alloys, as Table 4 and Figure 4 shows, an increase in the content of Si from 5 up to 9 wt.% lowering the amount of fraction solid at DCT for 50%, while the amount of fraction solid at TRigidity is only for 5% lower by higher silicon content. Addition of Cu into Al-Si alloys drastically changes the distribution of the fraction solid at characteristic solidification temperatures. By increasing the content of Cu from 1 up to 4 wt.%, the fraction solid at TRigidity decreased independently from the Si content to approximately 30% (from almost 90 to approximately 60%). At the same time, the addition of Cu does not have such a significant impact on the amount of fraction solid precipitated at the DCP. At lower content of Si, this impact is much stronger (fraction solid by adding Cu decreased to almost 10%), while by a higher content of Si, the impact is negligible (about 1%). According to Table 4 and Figure 4, it appears that the alloy with a shorter solidification range (e.g., Al-9Si-4Cu (wt.%)) achieves both Dendrite Coherency and Rigidity points at a lower fraction solid (12% and 56%, respectively) compared to the alloy with wider freezing range (e.g., Al-5Si-1Cu (wt.%)) and consequently higher fraction solid values for these two points ( 24% and 84%, respectively).

From Figure 4, it is obvious that with the Cu free Al-Si alloys, the interdendritic feeding region is dominantly independent of the content of Si in the investigated alloy. Increase in the Si content from 5 to 9 wt.% decreased the amount of fraction solid at the DCT from approximately 27% up to 13%. For the same increase of the Si content, the amount of fraction solid which precipitated at Rigidity point decreased from 94% to 89.5%. This means that around 70% of fraction solid precipitated during solidification between Dendrite Coherency and Rigidity temperatures. At the same time, an increase in the content of silicon from 5 to 9 wt.% decreases the amount of fraction solid by almost 50%, which precipitated between Tliq and TDCT. The burst feeding region is getting slightly wider by adding Si into aluminum alloys. Addition of Cu into these Al-Si hypoeutectic alloys considerably changes the distribution of the fraction solid among feeding regions. The Cu significantly increases the presence of the burst feeding. With Al-5Si-5Cu (wt.%) alloy, the amount of fraction solid formed between Rigidity and Solidus temperatures was about 15%, while at Al-9Si-4Cu (wt.%) that amount was above 40%.

Simultaneously, the amount of fraction solid formed between TDCP and TRigidity was noticeably reduced from 60% by Al-5Si-1Cu (wt.%) alloy up to 44% by Al-9Si-4Cu (wt.%) alloy. Generally, it can be noticed that the higher content of Cu significantly increases the existence of the burst feeding region, decreases the domain of interdendritic region and slightly reduces the mass feeding region. It is evident from Figure 3 that the various Si content significantly depressed the DCT, while its impact on TRigidity could be neglected. Higher Si content decreased the solidification interval (Tliq Tsol) of those alloys, changing also their solidification mode. It is

evident that the alloying element may change feeding ranges ability by shifting the alloy characteristic solidification temperatures. This may cause either a widening or narrowing of the corresponding feeding ranges of the alloy. The Cu has an impact on both dendrite coherency and TRigidity, as shown in Table 2, by depressing them to lower values. It is also well known that copper increases the solidification interval of Al-Si alloys. It can be seen from Figure 4 that increase in the content of Si

Characteristic fraction solid values of Al-(5, 7, 9)Si-(0–4)Cu (wt.%) alloys determined using cooling curve

Fraction solid values for the characteristic solidification temperatures have been collected for each analyzed alloy.

Alloy F<sup>s</sup> at

DOI: http://dx.doi.org/10.5772/intechopen.90337

Al-5Si-1Cu 26.0 85.7

Al-5Si-2Cu 24.0 79.7

Al-5Si-3Cu 19.3 73.7

Al-5Si-4Cu 15.4 65.3

Al-7Si 17.8 91.9

Al-7Si-1Cu 16.7 76.4

Al-7Si-2Cu 14.7 65.6

Al-7Si-3Cu 14.5 61.8

Al-7Si-4Cu 13.9 56.4

Al-9Si 14.1 89.1

Al-9Si-1Cu 12.2 73.1

Al-9Si-2Cu 12.3 65.8

Al-9Si-3Cu 13.3 61.3

Al-9Si-4Cu 12.6 56.0

Table 4.

analysis.

31

Al-5Si 0 27.5 95.2 100

Quantification of Feeding Regions of Hypoeutectic Al-(5, 7, 9)Si-(0-4)Cu (wt.%) Alloys Using…

Tliq TDCP TRigidity Tsol

24.6 93.1

23.2 82.5

21.3 76.7

17.6 74.7

16.5 68.7

17.5 91.2

18.7 78.2

14.5 66.7

15.8 65.5

14.1 55.4

12.3 90.2

13.1 77.8

12.8 63.1

13.8 60.1

12.3 57.1


Quantification of Feeding Regions of Hypoeutectic Al-(5, 7, 9)Si-(0-4)Cu (wt.%) Alloys Using… DOI: http://dx.doi.org/10.5772/intechopen.90337

Fraction solid values for the characteristic solidification temperatures have been collected for each analyzed alloy.

#### Table 4.

There are two known methods in the literature, Newtonian [29, 30, 52] and Fourier, [29, 30, 52] that have been successfully used to calculate fraction solid distribution using cooling curve analysis. In order to be capable of applying both methods, it is necessary to define the so-called baseline [29, 30, 52]. The baseline denotes the first derivative curve of the investigated alloy, assuming that melt during solidification process does not undergo any phase transformation. Therefore, it is to expect that base and first derivative curves are overlapping each other in the areas before liquidus (single liquid phase) and after solidus (single solid phase) temperatures. In this paper only the Newtonian method has been applied for calculating the base line

Table 4 and Figure 4 summarize the impact of various content of Si and Cu on the distribution of fraction solid at characteristic solidification temperatures (Tliq, TDCT, TRigidity and Tsol). For Cu free Al-Si alloys, as Table 4 and Figure 4 shows, an increase in the content of Si from 5 up to 9 wt.% lowering the amount of fraction solid at DCT for 50%, while the amount of fraction solid at TRigidity is only for 5% lower by higher silicon content. Addition of Cu into Al-Si alloys drastically changes the distribution of the fraction solid at characteristic solidification temperatures. By increasing the content of Cu from 1 up to 4 wt.%, the fraction solid at TRigidity decreased independently from the Si content to approximately 30% (from almost 90 to approximately 60%). At the same time, the addition of Cu does not have such a significant impact on the amount of fraction solid precipitated at the DCP. At lower content of Si, this impact is much stronger (fraction solid by adding Cu decreased to almost 10%), while by a higher content of Si, the impact is negligible (about 1%). According to Table 4 and Figure 4, it appears that the alloy with a shorter solidification range (e.g., Al-9Si-4Cu (wt.%)) achieves both Dendrite Coherency and Rigidity points at a lower fraction solid (12% and 56%, respectively) compared to the alloy with wider freezing range (e.g., Al-5Si-1Cu (wt.%)) and consequently higher fraction solid values for these two points ( 24% and 84%,

From Figure 4, it is obvious that with the Cu free Al-Si alloys, the interdendritic feeding region is dominantly independent of the content of Si in the investigated alloy. Increase in the Si content from 5 to 9 wt.% decreased the amount of fraction solid at the DCT from approximately 27% up to 13%. For the same increase of the Si content, the amount of fraction solid which precipitated at Rigidity point decreased from 94% to 89.5%. This means that around 70% of fraction solid precipitated during solidification between Dendrite Coherency and Rigidity temperatures. At the same time, an increase in the content of silicon from 5 to 9 wt.% decreases the amount of fraction solid by almost 50%, which precipitated between Tliq and TDCT. The burst feeding region is getting slightly wider by adding Si into aluminum alloys. Addition of Cu into these Al-Si hypoeutectic alloys considerably changes the distribution of the fraction solid among feeding regions. The Cu significantly increases the presence of the burst feeding. With Al-5Si-5Cu (wt.%) alloy, the amount of fraction solid formed between Rigidity and Solidus temperatures was about 15%,

Simultaneously, the amount of fraction solid formed between TDCP and TRigidity was noticeably reduced from 60% by Al-5Si-1Cu (wt.%) alloy up to 44% by Al-9Si-4Cu (wt.%) alloy. Generally, it can be noticed that the higher content of Cu significantly increases the existence of the burst feeding region, decreases the domain of interdendritic region and slightly reduces the mass feeding region. It is evident from Figure 3 that the various Si content significantly depressed the DCT, while its impact on TRigidity could be neglected. Higher Si content decreased the solidification interval (Tliq Tsol) of those alloys, changing also their solidification mode. It is

while at Al-9Si-4Cu (wt.%) that amount was above 40%.

using cooling curve analysis.

Mass Production Processes

respectively).

30

Characteristic fraction solid values of Al-(5, 7, 9)Si-(0–4)Cu (wt.%) alloys determined using cooling curve analysis.

evident that the alloying element may change feeding ranges ability by shifting the alloy characteristic solidification temperatures. This may cause either a widening or narrowing of the corresponding feeding ranges of the alloy. The Cu has an impact on both dendrite coherency and TRigidity, as shown in Table 2, by depressing them to lower values. It is also well known that copper increases the solidification interval of Al-Si alloys. It can be seen from Figure 4 that increase in the content of Si

all five feeding regions proposed by Campbell can be accurately quantified by either the temperature or corresponding fraction solid precipitated at those temperatures.

Quantification of Feeding Regions of Hypoeutectic Al-(5, 7, 9)Si-(0-4)Cu (wt.%) Alloys Using…

In the available literature, information related to a quantitative description of the five feeding mechanisms proposed by Campbell is limited. In this paper, the impact of the main alloying elements Si and Cu on different feeding regions of hypoeutectic Al-Si-Cu cast alloys has been studied using the TA technique. It has been shown that both elements have a significant impact on the characteristic solidification temperatures as well as on the amount of fraction solid precipitated at given temperatures. This work has also shown that TA is a valuable tool widely used in aluminum foundries that can collect numerous parameters (characteristic solidification temperatures, fraction solid distribution and others), which are beneficial for a better understanding of the solidification path of hypoeutectic Al-Si-Cu alloys. Applying TA technique as presented in this paper, it is now possible to describe each feeding region quantitatively through a temperature difference related to the total solidification interval or through a different amount of fraction solid that precipitated in each region. It can be assumed that calculated fraction solid at the DCT and fraction solid at TRigidity together with corresponding characteristic solidification temperatures are useful parameters for performing computer simulations of casting feed ability and for the characterization of the solidification process of

Publication of the manuscript is funded by the Lola Institute Ltd. (www.li.rs).

All authors declare that they have no conflict of interest in this research.

, Mile B. Djurdjevic<sup>1</sup> and Srećko Manasijević<sup>2</sup>

© 2019 The Author(s). Licensee IntechOpen. This chapter is distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/ by/3.0), which permits unrestricted use, distribution, and reproduction in any medium,

\*

4. Conclusion

DOI: http://dx.doi.org/10.5772/intechopen.90337

cast Al-Si-Cu alloys.

Acknowledgements

Conflict of interest

Author details

Gerhard Huber<sup>1</sup>

33

1 Nemak Linz GmbH, Linz, Austria

2 Lola Institute Ltd, Belgrade, Serbia

provided the original work is properly cited.

\*Address all correspondence to: srecko.manasijevic@li.rs

#### Figure 4.

The impact of Si on the fraction solid: (a) Al-(5, 7, 9)Si-0Cu (wt%), (b) Al-(5, 7, 9)Si-1Cu (wt%), (c) Al-(5, 7, 9)Si-2Cu (wt%), (d) Al-(5, 7, 9)Si-3Cu (wt%) and (e) Al-(5, 7, 9)Si-4Cu (wt%) alloys at the characteristic solidification temperatures.

(from 5 to 9 wt.%) and Cu (from 0 to 4 wt.%) significantly dropped down the amount of fraction solid at TRigidity, while the amount of fraction solid at DCT is slightly reduced. Besides chemical compositions, it is well known that other parameters have also been identified to affect the feeding capability of aluminum alloys [35–43]. Among these are melt superheat, temperature gradients during solidification, the influence of chemical composition, eutectic modification, grain refinement and hydrogen solubility. All these factors need to be taken into consideration in order to be able to properly answer which feeding region is more significant for the formation of cast defects. The correct answer could only be achieved if additional experimental techniques were introduced, such as the Tatur test sample, the measurement of the collecting temperature and the Hubler test sample, in addition to the thermal analysis. This paper has shown that applying cooling curve analysis to

all five feeding regions proposed by Campbell can be accurately quantified by either the temperature or corresponding fraction solid precipitated at those temperatures.
