Next Article in Journal
Self-Healing Concrete Using Rubber Particles to Immobilize Bacterial Spores
Next Article in Special Issue
Methods to Characterize Effective Thermal Conductivity, Diffusivity and Thermal Response in Different Classes of Composite Phase Change Materials
Previous Article in Journal
Induction of Osteogenic Differentiation of Mesenchymal Stem Cells by Bioceramic Root Repair Material
Previous Article in Special Issue
Alkali-Activated Cements for TES Materials in Buildings’ Envelops Formulated With Glass Cullet Recycling Waste and Microencapsulated Phase Change Materials
 
 
Search for Articles:
Title / Keyword
Author / Affiliation / Email
Journal
Article Type
 
 
Advanced Search
 
Section
Special Issue
Volume
Issue
Number
Page
 
Journals
Materials
Volume 12
Issue 14
10.3390/ma12142312
materials-logo
Submit to this Journal Review for this Journal Propose a Special Issue
► Article Menu

Article Menu

share Share announcement Help format_quote Cite question_answer Discuss in SciProfiles thumb_up
...
Endorse textsms
...
Comment
first_page
settings
Order Article Reprints
Font Type:
Arial Georgia Verdana
Font Size:
Aa Aa Aa
Line Spacing:
Column Width:
Background:
Article

The Use of Eutectic Fe-Si-B Alloy as a Phase Change Material in Thermal Energy Storage Systems

by
Jianmeng Jiao
1,*,
Bettina Grorud
1,
Caroline Sindland
1,
Jafar Safarian
1,
Kai Tang
2,
Kathrine Sellevoll
1 and
Merete Tangstad
1
1
Department of Materials Science and Engineering, Norwegian University of Science and Technology (NTNU), N-7491 Trondheim, Norway
2
SINTEF Materials and Chemistry, N-7491 Trondheim, Norway
*
Author to whom correspondence should be addressed.
Materials 2019, 12(14), 2312; https://doi.org/10.3390/ma12142312
Submission received: 6 June 2019 / Revised: 9 July 2019 / Accepted: 17 July 2019 / Published: 19 July 2019
(This article belongs to the Special Issue Phase Change Materials for Thermal Energy Storage)
Browse Figures
Versions Notes

Abstract

:
Fe-26.38Si-9.35B eutectic alloy is proposed as a phase change material (PCM) as it exhibits high latent heat, high thermal conductivity, moderate melting point, and low cost. For successful implementation of it in the latent heat thermal energy storage (LHTES) systems, we investigate the use of graphite as a refractory material that withstands long-term melting/solidification in contact with the Fe-26.38Si-9.35B alloy. The PCM has been thermally cycled up to 1–4 times below and above its melting point at the temperature interval of 20 °C or 100 °C. It is observed that this eutectic alloy shows good thermal stability over a small temperature range of 1057–1257 °C. Some SiC and B4C solid precipitation will be formed at the top of the alloy. However, it does not seem to increase with time. The graphite crucible as a refractory material will produce a protective layer of SiC and B4C that will hinder the interaction between the PCM and the crucible. The small volume change during solidification will not break the graphite crucible during cycling. The chemical wear or dissolution of the crucible is negligible. It demonstrates the viability of Fe-26.38Si-9.35B alloy as a heat storage material in this type of container.

1. Introduction

The consumption of various forms of energy has increased over the past few decades, which leads to continuous growth in greenhouse gas emissions. With a rise in fuel prices, there has recently been a keen interest in producing and storing energies [1]. The pursuit for storage materials has led to a class of materials called phase change materials (PCMs), in which heat storage is carried out due to the fusion of latent heat or other phase changes. PCMs are chosen to undergo solid-liquid, solid-gas, liquid-gas, and solid-solid phase transformations, and typically most PCMs operate between solid-liquid phase transformation in thermal engineering applications, which is known as melting-solidification cycle [2]. The use of PCM storing energy can overcome the mismatch between the power supply and power demand [3].
Due to the advantages offered by latent heat thermal energy storage (LHTES), numerous low-temperature applications have been applied by the low-temperature PCMs [4]. However, most of the low-temperature PCMs have low thermal conductivity, chemical instability, and degradation after multiple thermal cycles. Hence, these disadvantages limit their application in thermal energy systems (TES) [5].
High-temperature PCMs based on eutectic metal alloys have, therefore, lately received considerable attention in the use of thermionic photovoltaic converter in the thermal energy storage systems due to their high thermal conductivity and good stabilities [6]. Khare et al. [7] found that metals such as aluminum, magnesium, silicon, and zinc, were useful for high-temperature heat storage in the temperature range of 400–700 °C. Particularly the alloys 88Al-12Si [8,9,10,11,12] and 60Al-34Mg-6Zn [13,14,15,16] were identified to have superior properties for PCMs. However, the maximum operating temperature is still below 1000 °C.
To develop a new generation material with ultra-high temperature energy storage beyond 1000 °C, Matthew (2015) [17] tried to use pure silicon as a PCM to develop a solar thermal propulsion system for micro-satellites. However, as the volume expansion of silicon was approximately 10%, it led to the PCM container breakage during solidification [18]. To decrease the pure silicon volume expansion, Datas et al. (2016) [19] proposed a novel PCM, silicon (Si)-boron (B) alloy based on the contraction of the silicon lattice on an alloy with boron [20]. Comparing with the regular PCMs, silicon and boron possess higher latent heat [21] and higher thermal conductivity. As a target high-temperature PCM, Si-B alloy has a desirable latent heat to affect the energy density and a moderate melting point at the eutectic point [19]. However, a strong penetration into the graphite crucible was observed by Homa et al. [22] as well as our unpublished experimental results [23]. The volume expansion of the Si-3.25B (mass %) alloy did not decrease much compared with the pure silicon. It is decided to develop a ternary X-Si-B alloy, aiming to minimize the interaction of the molten alloy with graphite container and to decrease the volume expansion of Si-B alloy upon solidification. Simultaneously, the latent heat of fusion should not drop dramatically. In this regard, iron was chosen as a third element to add to Si-B alloy for the first time to generate a eutectic Fe-Si-B alloy as a new PCM. Using FactSage commercial FTlite database, the chemical composition of the eutectic Fe-Si-B alloy was confirmed to consist of 64.27 mass % iron, 26.38 mass % silicon, and 9.35 mass % boron (Fe-26.38Si-9.35B) and it had a high latent heat at the melting temperature of 1157 °C. The thermal conductivity of the Fe-26.38Si-9.35B alloy was estimated by assuming the ideal mixture of pure elements of silicon [24], iron [25], and boron [26], as shown in Table 1. The estimated results showed that the increase in temperature resulted in a decrease in thermal diffusivity. The minimum thermal conductivity value being 30.6 W/(m∙K) at 1100 °C exhibits a high thermal conductivity.
Isotropic graphite crucible is chosen as the potential PCM container for the Fe-26.38Si-9.35B alloy. This is a graphite material with isotropic structure and properties created through the cold isostatic press of micro particles. Isotropic graphite in the same direction has constant properties making it is ease of machining. The carbon atoms in the planes are covalently bonded in the graphite and it makes the material electrically conductive. Moreover, long time use is possible even at high temperatures exceeding 2000 °C in an inert atmosphere. With the exception of some strong oxidizers, it is chemically stable. Furthermore, its low thermal expansion and high thermal conductivity coefficients give it good thermal shock resistance. This study aimed to investigate the possibility to use the new Fe-26.38Si-9.35B PCM in graphite containers. Therefore, the phase formation of Fe-26.38Si-9.35B alloy, the interlayer between Fe-26.38Si-9.35B alloy and graphite crucible, the wettability behavior on graphite substrate and the penetration depth of Fe-26.38Si-9.35B alloy to graphite crucible after thermal cycling were researched systematically by experiments and phase equilibrium calculation. The obtained results established reliable data on thermophysical properties of Fe-26.38Si-9.35B alloy in both solid and liquid states around the melting point. It provides a technological basis for future implementing the PCM into reality in the LHTES application.

2. Thermodynamic Properties of Fe-Si-B System

Thermodynamic calculations were carried out in order to determine the Fe-Si-B eutectic composition and its melting temperature. Furthermore, its phase formation in the cooling path and fusion latent heat were also predicted using FactSage software version 7.2 (Montreal, Canada and Aachen, Germany). Thermodynamic data were taken from the FTlite database.
The Fe-Si-B ternary system has three sub-binary systems, Fe-Si, Fe-B, and Si-B. The Fe-Si sub-binary system has five silicides. Fe2Si, FeSi, and Fe3Si7 are silicides with a small homogeneity range melting congruently. On the other hand, Fe3Si2 and FeSi2 silicides are involved only in solid state reactions. Fe3Si7 is a low-temperature form of the FeSi2 phase [27]. The Fe-B sub-binary system has two intermediate phases, Fe2B and FeB, and the latter melts congruently and has a narrow homogeneity range [28]. In addition, the Si-B sub-binary system has three intermediate phases: SiB3 a solid solution with a homogeneity range of 50.6–56.5 mass % boron, SiB6 stoichiometric compound, and SiBn an extended solid solution between 82.6 and 91.9 mass % boron, respectively [20].
Figure 1 illustrates the liquidus projection of the ternary Fe-Si-B system calculated by FactSage based on FTlite commercial database. The colored lines correspond to the isothermal curves. The nominal chemical composition of the eutectic Fe-26.38Si-9.35B alloy is presented at the red point, a eutectic reaction occurs when the temperature of the molten alloy decreases to 1157 °C, liquid → FeSi + FeB + SiB6.
For illustrating the phase formation of the solidification process, the cooling path of the Fe-26.38Si-9.35B alloy from 1450 °C to 600 °C is shown in Figure 2. It is seen from the figure that three compounds, 70.9 mass% in FeSi, 20.4 mass% in FeB, and 8.7 mass% in SiB6 are formed when the temperature is below 1157 °C.
The latent heat of fusion of Fe-26.38Si-9.35B eutectic alloy was calculated by the FTlite database of FactSage 7.2. Figure 3a shows the relationship between the melting temperature and their latent heat for all the possible PCMs candidates. The red circle represents the latent heat of Fe-26.38Si-9.35B alloy. Comparing with all other possible candidates, the new Fe-Si-B alloy has a high latent heat (1250 kWh/m3) and moderate melting temperature (1157 °C). Additionally, silicon (second most abundant element on Earth) and iron (fourth most abundant element on Earth) are abundant and have low costs (silicon—1.7 $/kg) [19]. Furthermore, it shows a high thermal conductivity (Figure 3b).

3. Experimental Procedure and Materials

The objective of this work was to investigate the phase formation in the Fe-26.38Si-9.35B alloy, the penetration depth of the molten Fe-26.38Si-9.35B alloy into graphite crucible after thermal cycling experiments, and the wettability behavior of Fe-26.38Si-9.35B particle on graphite substrate. This part describes the preparation method of master alloys, the graphite tube resistance furnace, the sessile drop furnace, and the characterization methods according to the research topic.

3.1. Materials

In this study, commercial pure solar grade silicon in granule form from fluidized bed reactor (FBR) process, boron powder (99.9 mass %), and iron powder (99 mass %) are chosen as the raw materials. The impurities in boron powder analyzed by inductively coupled plasma-mass spectrometer (ICP-MS) are summarized in Table 2. It is seen from Table 2 that iron is the main impurity in boron powder, other contaminants are less than 51 ppm mass and their influence on the Fe-Si-B alloy is negligible.
Two different crucibles of graphite and alumina (Al2O3) were used for the experiments. A dense graphite crucible with an outer diameter of 22 mm and 15 mm inner diameter was machined from a block of isostatically pressed graphite and further used for thermal cycle experiments in a resistance furnace. Al2O3 crucible was used to make a Fe-26.38Si-9.35B master alloy. The properties of the graphite and Al2O3 crucibles are summarized in Table 3. Especially, the function of the thermal conductivity coefficient of the used graphite crucible with temperature is shown in Figure 4.
The eutectic Fe-26.38Si-9.35B master alloy was prepared as follows. The iron, silicon, and boron particles were weighed in an amount of 150 g and layered by descending melting temperature, then melted in the Al2O3 crucible in an induction furnace under argon. The Al2O3 crucible was placed inside a larger graphite crucible. The raw materials were melted through heating to 1700 °C, holding it for 1 h at this temperature for complete melting and homogenization. The solidified master alloy was then taken from the Al2O3 crucible and crushed in a mortar into pieces. The chemical composition of the eutectic Fe-26.38Si-9.35B master alloy was analyzed by ICP-MS. Both the detected and normalized content of silicon, iron, boron, aluminum, and manganese, in addition to the nominal composition of the alloy calculated by FactSage, are given in Table 4. Two master alloys were made in Al2O3 crucible, so we labeled them as Fe-Si-B-1, and Fe-Si-B-2. It is seen from Table 4 that the impurity contents of the aluminum and manganese are low. The Fe-Si-B-2 master alloy is closer to the nominal composition compared with the Fe-Si-B-1.

3.2. Thermal Cycle Experiments of Fe-26.38Si-9.35B PCM

The thermal cycle experiment was carried out using 6–12 g of the Fe-26.38Si-9.35B master alloy in a graphite crucible in a vertical graphite tube furnace. The heat is supplied by resistive heating, in which the passage of an electric current through a graphite element produces heat. Two different types of thermocouples, B-type in the side and C-type in the top, were used to measure the furnace temperature. The thermocouples were calibrated by melting pure copper. Meanwhile, the thermogradient in the graphite tube furnace is regularly checked before the experiment and the temperature variation within the sample is less than 2 °C. This deviation is within the accuracy level for the thermocouple. The schematic of the furnace is shown in Figure 5.
To investigate the thermal cycle behavior of the Fe-26.38Si-9.35B PCM, we exposed the alloy to its melting point, re-melted and solidified in 1-4 thermal cycles at the temperature interval of 1157 ± 20 °C and 1157 ± 100 °C in argon atmosphere. Figure 6 presents one of the applied temperature profiles; the furnace was heated to 1450 °C, then it was held for 1 h at 1450 °C for homogenization. After that, the thermal cycle at 1157 ± 100 °C was initiated with a holding time of 10 min at the top and bottom of each interval.

3.3. Wetting Experiment

The wetting experiment was conducted by a sessile drop method on graphite substrate in a dedicated resistance furnace. A small piece of Fe-26.38Si-9.35B master alloy was chosen and placed on the graphite substrate. Heating was performed in a vacuum of 10−1 mbar up to 1100 °C in 4 min. Next, the alloy was heated to 1450 °C with a rate of 20 °C/min and, finally, it was cooled down to room temperature with a natural cooling rate. The temperature profile is presented in Figure 7.

3.4. Structural Characterization

The solidified alloy in the graphite crucible was cut with a diamond cut-off wheel. Then, the metallographic preparation was performed by a stepwise electronically controlled grinding and polishing machine. The Fe-26.38Si-9.35B sample and crucible after being mounted, ground, and polished are shown in Figure 8. It is observed that the sample and graphite crucible is easily separated.
The microstructures were studied by electron probe micro-analyzer (EPMA) (JEOL JXA 8500F, Germany) and scanning electron microscope (SEM) (Zeiss Supra, 55 VP, Germany). The SEM was supplied with secondary electron (SE) contrast and backscattered electron (BSE) detector at an acceleration voltage of 15 or 20 kV and a working distance of 10 mm. The inner surface of the crucible was analyzed through optical microscopy (OM) (Leica MEF4M, Germany), and images were taken from three positions at the left wall, the left corner, and the bottom of the sample, as seen in Figure 8b. Moreover, the industrial computed tomography (CT) (XT H 225 ST, Nikon, Japan) scanning technique was also used to produce 2D cross-sectional images of the alloy to qualify the densification of the solidified alloy. The chemical composition of the formed phase was determined by wavelength dispersive X-ray spectroscopy (WDS) technique. Phase analysis was also performed using an X-ray diffractometer (XRD) (Bruker D8 A25 DaVinci, Germany) with Cu Kα radiation, 35–105 deg diffraction angle, 0.013 deg step size. The diffraction peak patterns were analyzed using DIF-FRAC.EVA software (Bruker AXS GmbH, Karlsruhe, Germany) and the JCPSD-database PDF-4 + 2018 RDB.

4. Results and Discussion

4.1. Phase Formation in the Fe-26.38Si-9.35B Alloy

The formed phases are detected in the Fe-26.38Si-9.35B alloys after 1–4 melting/solidification process, which contains FeSi, FeB, SiB6, SiC, B4C, and FeSiB3. Figure 9a–c present the distribution of elements measured by EPMA for the Fe-26.38Si-9.35B alloy at top, center, and bottom three different positions, in which the alloys have be subjected to two thermal cycles at 1157 ± 20 °C It is apparent from Figure 9a–c that FeSi phase is determined as the metal matrix, and FeSiB3 is identified as a new phase by WDS analysis (Table 5). The most interesting aspect of this figure is that FeSi and FeB phases can only be distinguished in the element distribution pictures, instead of BSE pictures. Furthermore, the top position of the sample (Figure 9a) shows that some SiC particles exist in the alloy and the SiC particles are decorated with B4C phases. In the bulk of the sample (Figure 9b) the SiC and B4C phases are not detected. Hence, five phases are present at the top position of the metal, four phases in the bulk of the alloy, and six phases in the bottom area towards the graphite crucible.
A continuous SiC and B4C layer was generated between the Fe-26.38Si-9.35B alloy and graphite crucible. A typical EPMA image on the interface between graphite crucible and Fe-Si-B alloy after four thermal cycles at 1157 ± 100 °C is shown in Figure 10. Combined with Figure 9c, we know that two continuous barrier layers, a thicker outer layer of SiC and a thinner B4C inner layer, are formed at the interface between the PCM alloy and graphite crucible.
All phases in the samples after thermal cycles were analyzed by WDS in EPMA, and each phase was measured at least twenty points in the samples, the chemical component of FeSi, FeSiB3, FeB, and SiB6 are summarized in Table 5.
Figure 11 presents the isothermal cross-section of Fe-Si-B ternary system within 50–100 mass % iron at the temperature range of 1137–1450 °C. The two black points represent the chemical composition of the two master alloys produced and analyzed by ICP-MS, used in the thermal cycle experiments and measurements of thermophysical properties. It is seen from Figure 11 that they are both in the liquid area at 1250–1450 °C, and then transferred to the liquid + SiB6 phase area when the temperature decreases to 1177 °C, and through further cooling, they should reach the FeB + FeSi + SiB6 phase region at 1137 °C. The thermal cycle experiment performed at the temperature range of 1137–1177 °C has a phase composition between liquid + SiB6 and FeB + FeSi + SiB6 phase area. The solidification and melting process is undertaken between the liquid phase and FeB + FeSi + SiB6 phases area when the temperature interval is changed between 1057 °C and 1257 °C.
Compared with the experimental results, FeSi, FeB, and SiB6 are expected from the calculated diagram. It is seen from Table 5 that ~11 at% boron was dissolved to the FeSi phase and formed an interstitial solution, which was verified by the XRD results, where the offset of the FeSi peak towards left (Figure 12b). Simultaneously, only small traces of silicon (0.23 at %) was detected in the FeB phases.
FeSiB3 is not expected from the calculated phase diagram. The measured average chemical composition of the new phase FeSiB3 was 22.0 at % Fe, 20.6 at% Si, and 57.3 at %. Neamţu et al. [32] documented that only Fe3Si and Fe2B phases existed in the Fe-11.6Si-1.1B amorphous powder after heated up to 900 °C in the DSC furnace. Moreover, Tong et al. [33] prepared the nanocrystalline FeBSi alloy specimens in a vacuum furnace by heating the amorphous FeBSi ribbons, and α-Fe(Si) solid solution and Fe2B phases were confirmed by XRD analysis. They also did not detect any ternary Fe-Si-B compounds. At present, FeSiB3 is assumed to be a new observed phase, which is different with the other three ternary compounds Fe5Si2B, Fe4.7SiB2, and Fe2Si0.4B0.6 described by Aronsson [34]. Further investigation should be performed to confirm the FeSiB3 lattice structure.
The produced Fe-26.38Si-9.35B eutectic alloy was melted in graphite crucible and, hence, the carbon would be dissolved into the melts. The dissolved carbon will change the composition of the alloy. To investigate the influence of carbon on the phase formation in Fe-26.38Si-9.35B alloy, the liquidus projection in the Fe-Si-9B-C (mass %) alloy was calculated using the SINTEF database [35], as shown in Figure 13.
The primary crystallized phases are SiC, B4C, FeB, and graphite. SiC and graphite phases are stable at the high-temperature and higher carbon range, whereas, B4C and FeB phases are stable at the low-temperature and at lower carbon range. When the molten Fe-Si-B alloy equilibrates with graphite crucible, the carbon solubility increases with increasing temperature at a constant iron content or with the increase of iron content at a constant temperature. The grey dashed line represents the constant iron content of 64.2 mass %, which shows that SiC coexists with Fe-26.38Si-9.35B melts at temperatures above 1600 °C. However, it reacts with boron to form B4C when the temperature decreases to the B4C phase area. The maximum operating temperature of the present work is 1450 °C, which is lower than 1600 °C. Hence, the molten Fe-26.38Si-9.35B alloy should be equilibrated with B4C. This is confirmed by the experimental results, i.e., the formation of B4C layer at the interface (Figure 10).
According to Figure 13, the carbon solubility in the Fe-26.38Si-9.35B alloy is at the range of 0.1–0.3 mass % at the temperature range of 1500–1600 °C, which means that carbon dissolved into the melts is low. As the temperature decreases during cooling, the dissolved carbon is precipitated to SiC particle. With the decreasing temperature, B4C will precipitate at 1396 °C [36]. However, these phases are only found at the top position of the alloy. They are not detected in the bulk of the sample. According to the calculation s by FactSage, the density of the molten Fe-26.38Si-9.35B alloy, B4C, and SiC is 4.3836 g/mL, 2.52 g/mL, and 3.217g/mL, respectively. This means that B4C and SiC particles will float to the top of the molten Fe-Si-B alloy in the melting/solidification process due to their lower density.

4.2. Effect of Thermal Cycling

The stability of the phases under solid-liquid cycles near the melting point in a PCM is crucial to obtain a long lifecycle. Therefore, thermal cycle experiments were performed to identify the stability of the observed phases in the Fe-Si-B alloy inside the graphite crucible during solidification and melting process, where the thermal cycle and the temperature range was designed as 1–4 times at 1157 ± 20 °C and 1157 ± 100 °C. The morphologies of the samples in the bulk of the samples after the thermal cycle experiments are shown in BSE images in Figure 14a–e. By comparison, the BSE images show that the structures in the Fe-26.38Si-9.35B alloys after thermal cycle experiments are similar, which are consisted of FeSi, FeB, FeSiB3, and SiB6.
The samples after thermal cycle experiments were also analyzed by XRD and are shown in Figure 12. It is seen from the figure that the FeSi, FeB, and B4C phases were verified by XRD. However, the SiC and SiB6 phases were not detected. The FeSiB3 phase was not found in the XRD database (PDF-4 + 2018 RDB). The five XRD spectrums represent five different thermal cycle conditions, which are similar. It substantiates the phase stability in the Fe-26.38Si-9.35B alloy after 1–4 thermal cycles during melting/solidification process.
The penetration depth of the alloy into the graphite crucible after thermal cycle experiments was measured at the bottom, center, and side positions of the crucible by optical microscopy and is presented in Figure 15. The crucibles experienced little penetration from the molten Fe-26.38Si-9.35B alloy. The penetration depth in these samples was measured at higher magnifications. It is found that they are to be 60–180 µm at the bottom, 40–120 µm at the corner, and 40–100 µm at the wall. The similar measurements were conducted from the Si-3.25B/graphite system. The median penetration depth was found to be 1150 µm at the bottom, 1150 µm at the corner, and 830 µm at the wall [23]. It indicates that the penetration depth of the molten Fe-26.38Si-9.35B into the graphite crucible is negligible compared with molten Si-3.25B alloy. Therefore, the graphite material can be used for long-term thermal cycles without breakage.

4.3. Wettability of Graphite Substrate by the Molten Fe-26.38Si-9.35B

The Fe-26.38Si-9.35B alloys could easily be detached from the crucibles after thermal cycle experiments or during the cutting process. To explain this phenomenon, an investigation of the wettability property of the Fe-26.38Si-9.35B alloy on graphite substrate is done on graphite substrate. It is beneficial to obtain a proper view of the crucible material. The images of the sample taken during the wetting test are presented in Figure 16.
Figure 16 shows that the Fe-26.38Si-9.35B particle started to melt at about 1220 °C, which is shown as the white dotted circles in the Figure. This is somewhat higher than the calculated eutectic temperature from the FactSage calculation of 1157 °C. It may be caused by the oxide layer existed at the surface of the Fe-26.38Si-9.35B particle. The complete melting of the alloy on the graphite substrate was observed at 1234 °C. The final contact angle decreased to 31° at 1450 °C, showing high wettability with graphite materials.
Cao er al. [37] measured the contact angles of Fe-5.3Si-3B alloy on SiC substrate under vacuum. The contact angle of 100° on SiC substrate at 1150–1360 °C had a considerable difference with our experimental result of 31° on graphite at 1450 °C. It is known that the wetting angle of pure iron on graphite exhibited good wetting at 1300–1500 °C, with 0–66° under different atmospheres [38,39,40,41]. However, it increased from less than 90° to around 140° when carbon content increased in the melt [39]. In the study performed by Rubio et al. [42], the Fe-14.1Si alloy was found to be much lower, reaching 38° at 1550 °C, which had a similar angle with our experimental result.
The wetting tests show that the eutectic Fe-26.38Si-9.35B alloy displays good wetting behavior on the graphite substrate, which will make the Fe-26.38Si-9.35B alloy adhering to the graphite instead of detaching. Therefore, the detaching phenomenon in the experiments may be caused by other unknown reasons and it will be further investigated. Though the wettability towards the transformed C-crucible is high, it was still penetrating the crucible less than Si-B alloys, which had been observed by our work in the lab [23]. The melting point was observed around 1220 °C, which was higher than the theoretical melting point of 1157 °C.

4.4. Pore Formation in the Solidified Fe-26.38Si-9.35B Alloy

There are plenty of pores at the top and center positions of the Fe-26.38Si-9.35B ingot after melting/solidification process. The Fe-26.38Si-9.35B PCM alloy after four times thermal cycles at 1157 ± 100 °C in graphite crucible was used to perform a non-destructive analysis by computed tomography (CT) at the scanning rotation range of 0–360°. Four different angle positions of the sample are presented in Figure 17. Compared with the cross-section of the PCM alloy after the CT scan in Figure 18, it is seen that the solidified sample is not dense at the top and center positions of the sample as the small pores exist inside the sample. The PCM alloy close to the wall and bottom of the graphite crucible is however dense. Meanwhile, a crack line was observed at the bottom between the PCM alloy and graphite crucible, and this attests that the PCM alloy had a volume shrinkage during solidification process.
The pores inside the Fe-26.38Si-9.35B alloy might arise from two causes [43]: (a) Shrinkage during solidification, and (b) exsolution of dissolved gases. The volume change of the Fe-26.38Si-9.35B alloy is calculated by FactSage software package and its commercial databases, as shown in Figure 19. It is obvious that the alloy volume decreases with the decrease of temperature. Notably, there is an evident volume shrinkage in the freezing point.
In the solidification process, the molten alloy close to the wall and bottom of the graphite is first solidified. The center part is finally solidified, which could not obtain enough molten alloy to supplement because of shrinkage. Hence, the pores are concentrated in the final solidification position. At the same time, the solubility of gas in the liquid state is normally higher than in the solid state [44]. Therefore, the gas precipitation may occur during solidification process due to the segregation of the gas elements. Examples of this is dissolved carbon and dissolved oxygen producing CO gas.
The pores in the Fe-26.38Si-9.35B alloy will destroy the metal continuity and decrease its corrosion resistance [45]. However, it can be controlled by reducing the dissolved gases content and decreasing the freezing rate [43]. In the TES, the optimal heat extraction would be from the bottom of the crucible. Thus, the pores will not affect the use of Fe-26.38Si-9.35B alloy as a PCM.

5. Conclusions

This work was conducted to investigate the application of Fe-26.38Si-9.35B eutectic alloy at 1157 ± 20 and 1157 ± 100 °C for 1–4 thermal cycles in the graphite crucible for a PCM material and the corresponding container development. The stability of the alloy and its interaction with the graphite container were theoretically and experimentally studied. The samples were investigated by EPMA-WDS, SEM-EDS, CT scan, XRD, and OM. The main conclusions are summarized as follow:
  • The fusion enthalpy of the eutectic Fe-26.38Si-9.35B alloy is calculated to be 1250 kWh/m3. This value is higher than other possible PCMs candidates in the literature.
  • Six different phases are found in the PCM alloy after solidification. FeSi, FeB, SiB6, and FeSiB3 are the main phases appeared in the sample. SiC and B4C particles are located at the edge of the treated alloy in graphite crucible. The new ternary phase, FeSiB3, is identified by wavelength dispersive X-ray spectroscopy analysis.
  • Under conditions of this study, the penetration of molten PCM alloy into the graphite crucible is negligible and the alloy has no degradation effect on graphite container.
  • Wetting experiment shows that the molten PCM alloy wets well with graphite substrate, for the low contact angle of 31°.The shrinkage of the Fe-26.38Si-9.35B alloy creates small amounts of pores at the top and center position of the solidified sample. No expansion upon solidification is promising for further use of this PCM alloy.
  • Further study will focus on investigating the stability of Fe-26.38Si-9.35B alloy in other refractory materials (e.g. Si3N4, BN, and Al2O3) in the melting/solidification process. Other investigations, such as the fusion enthalpy of the Fe-26.38Si-9.35B alloy and the confirmation of the new FeSiB3 phase will be considered in subsequent works.

Author Contributions

Conceptualization: M.T. and J.S.; methodology: M.T.; software: K.T. and J.J.; validation: M.T., J.S., and J.J.; formal analysis: J.J., C.S., B.G., and K.S.; investigation: J.J. C.S., B.G., and K.S; resources: J.J. and M.T.; writing—J.J.; writing—review and editing: J.S., K.T., and M.T.; visualization: J.J.; supervision: M.T. and J.S.; project administration: M.T.; funding acquisition: M.T.

Funding

The project AMADEUS has received funds from the European Union’s Horizon 2020 research and innovation program, FET-OPEN action, under grant agreement 737054. The sole responsibility for the content of this publication lies with the authors. It does not necessarily reflect the opinion of the European Union. Neither the REA nor the European Commission are responsible for any use that may be made of the information contained therein.

Conflicts of Interest

The authors declare no conflict of interest.

References

  1. Kenisarin, M.M. High-temperature phase change materials for thermal energy storage. Renew. Sustain. Energy Rev. 2010, 14, 955–970. [Google Scholar] [CrossRef]
  2. Kumar, N.; Banerjee, D. Phase Change Materials. In Handbook of Thermal Science and Engineering; Springer International Publishing: Cham, Switzerland, 2018; pp. 2213–2275. ISBN 978-3-319-26695-4. [Google Scholar]
  3. Fernández, A.I.; Barreneche, C.; Belusko, M.; Segarra, M.; Bruno, F.; Cabeza, L.F. Considerations for the use of metal alloys as phase change materials for high temperature applications. Sol. Energy Mater. Sol. Cells 2017, 171, 275–281. [Google Scholar] [CrossRef] [Green Version]
  4. Liu, M.; Saman, W.; Bruno, F. Review on storage materials and thermal performance enhancement techniques for high temperature phase change thermal storage systems. Renew. Sustain. Energy Rev. 2012, 16, 2118–2132. [Google Scholar] [CrossRef]
  5. Kenisarin, M.; Mahkamov, K. Solar energy storage using phase change materials. Renew. Sustain. Energy Rev. 2007, 11, 1913–1965. [Google Scholar] [CrossRef]
  6. Magomedov, A.M. Netraditsionnye Istochniki Energii (Non-Traditional Sources of Energy); AOZT “Pamiatniki Otechestva”: Moscow, Russia, 1996. [Google Scholar]
  7. Khare, S.; Dell’Amico, M.; Knight, C.; McGarry, S. Selection of materials for high temperature sensible energy storage. Sol. Energy Mater. Sol. Cells 2013, 115, 114–122. [Google Scholar] [CrossRef]
  8. Kotzé, J.P.; von Backström, T.W.; Erens, P.J. Simulation and Testing of a Latent Heat Thermal Energy Storage Unit with Metallic Phase Change Material. Energy Procedia 2014, 49, 860–869. [Google Scholar] [CrossRef] [Green Version]
  9. He, Q.; Zhang, W. A study on latent heat storage exchangers with the high-temperature phase-change material. Int. J. Energy Res. 2001, 25, 331–341. [Google Scholar] [CrossRef]
  10. Akiyama, T.Y. Ashizawa, J.Y. Storage and release of heat in a single spherical capsule containing phase change material of high melting point. Heat Transf. Jpn. Res. 1992, 21, 199–217. [Google Scholar]
  11. Li, F.; Hu, Y.J.; Zhang, R.Y. The Influence of Heating-Cooling Cycles on the Thermal Storage Performances of Al-17 Wt.% Si Alloy. Adv. Mater. Res. 2011, 239–242, 2248–2251. [Google Scholar] [CrossRef]
  12. Kotzé, J.P.; von Backström, T.W.; Erens, P.J. High Temperature Thermal Energy Storage Utilizing Metallic Phase Change Materials and Metallic Heat Transfer Fluids. J. Sol. Energy Eng. 2013, 135, 035001. [Google Scholar] [CrossRef] [Green Version]
  13. Khare, S.; Dell’Amico, M.; Knight, C.; McGarry, S. Selection of materials for high temperature latent heat energy storage. Sol. Energy Mater. Sol. Cells 2012, 107, 20–27. [Google Scholar] [CrossRef]
  14. Cárdenas, B.; León, N. High temperature latent heat thermal energy storage: Phase change materials, design considerations and performance enhancement techniques. Renew. Sustain. Energy Rev. 2013, 27, 724–737. [Google Scholar] [CrossRef]
  15. Farkas, D.; Birchenall, C.E. New eutectic alloys and their heats of transformation. Metall. Trans. A 1985, 16, 323–328. [Google Scholar] [CrossRef]
  16. Gasanaliev, A.M.; Gamataeva, B.Y. Heat-accumulating properties of melts. Russ. Chem. Rev. 2000, 69, 179–186. [Google Scholar] [CrossRef]
  17. Gilpin, M.R. High Temperature Latent Heat Thermal Energy Storage to Augment Solar Thermal Propulsion for Microsatellites. Ph.D. Thesis, Viterbi School of Engineering, Los Angeles, CA, USA, April 2015. [Google Scholar]
  18. Rhim, W.K.; Ohsaka, K. Thermophysical properties measurement of molten silicon by high-temperature electrostatic levitator: Density, volume expansion, specific heat capacity, emissivity, surface tension and viscosity. J. Cryst. Growth 2000, 208, 313–321. [Google Scholar] [CrossRef]
  19. Datas, A.; Ramos, A.; Martí, A.; del Cañizo, C.; Luque, A. Ultra high temperature latent heat energy storage and thermophotovoltaic energy conversion. Energy 2016, 107, 542–549. [Google Scholar] [CrossRef] [Green Version]
  20. Olesinski, R.W.; Abbaschian, G.J. The B-Si (Boron-Silicon) system. Bull. Alloy Phase Diagr. 1984, 5, 478–484. [Google Scholar] [CrossRef]
  21. Zaitsev, A.I.; Kodentsov, A.A. Thermodynamic properties and phase equilibria in the Si-B system. J. Phase Equilibria. 2001, 22, 126–135. [Google Scholar] [CrossRef]
  22. Homa, M.; Sobczak, N.; Hodor, K.; Gezgin, S. Simultaneous TGA-DTA thermal analysis of Si-30B alloy. In Proceedings of the 73th Word Foundry Congress, Krakow, Poland, 23–27 September 2018. [Google Scholar]
  23. Grorud, B. Interaction of Eutectic Fe-Si-B Alloy with Graphite Crucibles. Master’s Thesis, NTNU, Trondheim, Norway, June 2018. [Google Scholar]
  24. Shanks, H.R.; Maycock, P.D.; Sidles, P.H.; Danielson, G.C. Thermal conductivity of silicon from 300 to 1400 K. Phys. Rev. 1963, 130, 1743–1748. [Google Scholar] [CrossRef]
  25. Powell, R.W. Further measurements of the thermal and electrical conductivity of iron at high temperatures. Proc. Phys. Soc. 1939, 51, 407–418. [Google Scholar] [CrossRef]
  26. Slack, G.A.; Oliver, D.W.; Horn, F.H. Thermal conductivity of boron and some boron compounds. Phys. Rev. B 1971, 4, 1714–1720. [Google Scholar] [CrossRef]
  27. Poletti, M.G.; Battezzati, L. Assessment of the ternary Fe-Si-B phase diagram. Calphad Comput. Coupling Phase Diagr. Thermochem. 2013, 43, 40–47. [Google Scholar] [CrossRef]
  28. Lacaze, J.; Sundman, B. An assessment of the Fe-C-Si system. Metall. Trans. A 1991, 22, 2211–2223. [Google Scholar] [CrossRef]
  29. Ho, C.Y.; Powell, R.W.; Liley, P.E. Thermal Conductivity of the Elements. J. Phys. Chem. Ref. Data 1972, 1, 279–421. [Google Scholar] [CrossRef] [Green Version]
  30. Zalba, B.; Marı́n, J.M.; Cabeza, L.F.; Mehling, H. Review on thermal energy storage with phase change: materials, heat transfer analysis and applications. Appl. Therm. Eng. 2003, 23, 251–283. [Google Scholar] [CrossRef]
  31. Bjørnstad, E.L.; Tranell, G. Mass Transfer of Al and Ca Between Silicon and Synthetic SiO2-CaO-Al2O3 Slags. In Materials Processing Fundamentals; Allanore, A., Lambotte, G., Lee, J., Eds.; Springer: Boston, MA, USA, 2017; pp. 85–96. [Google Scholar] [CrossRef]
  32. Neamţu, B.V.; Marinca, T.F.; Chicinaş, I.; Isnard, O.; Popa, F.; Păşcuţă, P. Preparation and soft magnetic properties of spark plasma sintered compacts based on Fe–Si–B glassy powder. J. Alloys Compd. 2014, 600, 1–7. [Google Scholar] [CrossRef]
  33. Tong, H.Y.; Wang, J.T.; Ding, B.Z.; Jiang, H.G.; Lu, K. The structure and properties of nanocrystalline Fe78B13Si9 alloy. J. Non. Cryst. Solids 1992, 150, 444–447. [Google Scholar] [CrossRef]
  34. Aronsson, B.; Engström, I. X-Ray Investigations on M-Si-B Systems (M = Mn, Fe, Co). II. Some Features of the Fe-Si-B and Mn-Si-B Systems. Acta Chem. Scand. 1960, 14, 1403–1413. [Google Scholar] [CrossRef]
  35. Tang, K.; Oslash, E.J.; Tranell, G.; Tangstad, M. A Thermochemical Database for the Solar Cell Silicon Materials. Mater. Trans. 2009, 50, 1978–1984. [Google Scholar] [CrossRef] [Green Version]
  36. Seifert, H.J.; Peng, J.; Golczewski, J.; Aldinger, F. Phase equilibria of precursor-derived Si-(B-)C-N ceramics. Appl. Organomet. Chem. 2001, 15, 794–808. [Google Scholar] [CrossRef]
  37. Gao, H.; Dong, B.S.; Zhong, J.; Li, Z.Z.; Xu, M.; Zhou, S.X. The influence of substrate and atmosphere on the properties of FeSiB(Cu,Nb) alloy melts. Sci. China Technol. Sci. 2016, 59, 1892–1898. [Google Scholar] [CrossRef]
  38. Humenik, M.; Kingery, W. Metal-Ceramic Interactions: III, Surface Tension and Wettability of Metal-Ceramic Systems. J. Am. Ceram. Soc. 1954, 37, 18–23. [Google Scholar] [CrossRef]
  39. Sun, H.; Mori, K.; Sahajwalla, V.; Pehlke, R.D. Carbon Solution in Liquid Iron and Iron Alloys. High Temp. Mater. Process. 1998, 17, 257–270. [Google Scholar] [CrossRef]
  40. Wu, C.; Sahajwalla, V. Influence of melt carbon and sulfur on the wetting of solid graphite by Fe-C-S melts. Metall. Mater. Trans. B 1998, 29, 471–477. [Google Scholar] [CrossRef]
  41. Zhao, L.; Sahajwalla, V. Interfacial phenomena during wetting of graphite/alumina mixtures by liquid iron. ISIJ Int. 2003, 43, 1–6. [Google Scholar] [CrossRef]
  42. Rubio, P.J.Y.; Hong, L.; Saha-Chaudhury, N.; Bush, R.; Sahajwalla, V. Dynamic Wetting of Graphite and SiC by Ferrosilicon Alloys and Silicon at 1550 C. ISIJ Int. 2006, 46, 1570–1576. [Google Scholar] [CrossRef]
  43. Coble, R.L.; Flemings, M.C. On the removal of pores from castings by sintering. Metall. Trans. 1971, 2, 409–415. [Google Scholar] [CrossRef]
  44. Brinkman, J.A. On the mechanism of pore formation during diffusion. Acta Metall. 1955, 3, 606–607. [Google Scholar] [CrossRef]
  45. Hashim, J.; Looney, L.; Hashmi, M.S.J. Metal matrix composites: production by the stir casting method. J. Mater. Process. Technol. 1999, 92–93, 1–7. [Google Scholar] [CrossRef]
Materials 12 02312 g001 550
Figure 1. Projection of Fe-Si-B system, where red point represents the Fe-26.38Si-9.35B eutectic alloy (FTlite database).
Figure 1. Projection of Fe-Si-B system, where red point represents the Fe-26.38Si-9.35B eutectic alloy (FTlite database).
Materials 12 02312 g001
Materials 12 02312 g002 550
Figure 2. Cooling path of the Fe-26.38Si-9.35B alloy calculated by FactSage.
Figure 2. Cooling path of the Fe-26.38Si-9.35B alloy calculated by FactSage.
Materials 12 02312 g002
Materials 12 02312 g003 550
Figure 3. (a) Latent heat of fusion of different materials as a function of the melting temperature [19], (b) Thermal conductivity of different types of PCMs [29,30].
Figure 3. (a) Latent heat of fusion of different materials as a function of the melting temperature [19], (b) Thermal conductivity of different types of PCMs [29,30].
Materials 12 02312 g003
Materials 12 02312 g004 550
Figure 4. Thermal conductivity coefficient of the used graphite crucible vs. temperature.
Figure 4. Thermal conductivity coefficient of the used graphite crucible vs. temperature.
Materials 12 02312 g004
Materials 12 02312 g005 550
Figure 5. Schematic of the resistance vertical graphite tube furnace [31].
Figure 5. Schematic of the resistance vertical graphite tube furnace [31].
Materials 12 02312 g005
Materials 12 02312 g006 550
Figure 6. A graphic representation of the typical thermal cycle experiment.
Figure 6. A graphic representation of the typical thermal cycle experiment.
Materials 12 02312 g006
Materials 12 02312 g007 550
Figure 7. The temperature profile of the Fe-26.38Si-9.35B sample on the graphite substrate in the wetting test.
Figure 7. The temperature profile of the Fe-26.38Si-9.35B sample on the graphite substrate in the wetting test.
Materials 12 02312 g007
Materials 12 02312 g008 550
Figure 8. Graphite crucible and Fe-Si-B sample after being mounted, ground, and polished. (a) the Fe-26.38Si-9.35B alloy after thermal cycle experiment, (b) the graphite crucible after thermal cycle experiment, the red rectangles represent the positions that are analyzed by optical microscopy.
Figure 8. Graphite crucible and Fe-Si-B sample after being mounted, ground, and polished. (a) the Fe-26.38Si-9.35B alloy after thermal cycle experiment, (b) the graphite crucible after thermal cycle experiment, the red rectangles represent the positions that are analyzed by optical microscopy.
Materials 12 02312 g008
Materials 12 02312 g009 550
Figure 9. EPMA images of Fe-26.38Si-9.35B alloy after two times melting/solidification cycles at 1157 ± 20 °C: (a) at the top, (b) at the center, and (c) at the bottom.
Figure 9. EPMA images of Fe-26.38Si-9.35B alloy after two times melting/solidification cycles at 1157 ± 20 °C: (a) at the top, (b) at the center, and (c) at the bottom.
Materials 12 02312 g009
Materials 12 02312 g010 550
Figure 10. The distribution of phases at the interface between Fe-26.38Si-9.35B alloy and the graphite crucible after four thermal cycles at 1157 ± 100 °C.
Figure 10. The distribution of phases at the interface between Fe-26.38Si-9.35B alloy and the graphite crucible after four thermal cycles at 1157 ± 100 °C.
Materials 12 02312 g010
Materials 12 02312 g011 550
Figure 11. Isothermal cross-section of the ternary Fe-Si-B system at the iron range 50–100 mass % calculated by FactSage at temperatures of (a) 1450 °C, (b) 1250 °C, (c) 1177 °C, and (d) 1137 °C.
Figure 11. Isothermal cross-section of the ternary Fe-Si-B system at the iron range 50–100 mass % calculated by FactSage at temperatures of (a) 1450 °C, (b) 1250 °C, (c) 1177 °C, and (d) 1137 °C.
Materials 12 02312 g011
Materials 12 02312 g012 550
Figure 12. (a) XRD patterns of Fe-26.38Si-9.35B alloys with different temperature intervals and thermal cycles. (b) An expanded view of the FeSi XRD spectra at the scan range of 35–55°, showing a clear peak shift towards left.
Figure 12. (a) XRD patterns of Fe-26.38Si-9.35B alloys with different temperature intervals and thermal cycles. (b) An expanded view of the FeSi XRD spectra at the scan range of 35–55°, showing a clear peak shift towards left.
Materials 12 02312 g012
Materials 12 02312 g013 550
Figure 13. Liquidus projection of Fe-Si-9mass %B-C phase diagram.
Figure 13. Liquidus projection of Fe-Si-9mass %B-C phase diagram.
Materials 12 02312 g013
Materials 12 02312 g014 550
Figure 14. Backscattered electron images at different thermal cycles in the center position of the samples. (a) 1 cycle at 1157 ± 20 °C, (b) 1 cycle at 1157 ± 100 °C, (c) 2 cycles at 1157 ± 20 °C, (d) 3 cycles at 1157 ± 100 °C, (e) 4 cycles at 1157 ± 100 °C.
Figure 14. Backscattered electron images at different thermal cycles in the center position of the samples. (a) 1 cycle at 1157 ± 20 °C, (b) 1 cycle at 1157 ± 100 °C, (c) 2 cycles at 1157 ± 20 °C, (d) 3 cycles at 1157 ± 100 °C, (e) 4 cycles at 1157 ± 100 °C.
Materials 12 02312 g014
Materials 12 02312 g015 550
Figure 15. Images of the contact area of the alloy and the graphite crucible at (a,d,g) bottom of the crucible, (b,e,h) left wall of the crucible, and (c,f,i) left corner of the crucible.
Figure 15. Images of the contact area of the alloy and the graphite crucible at (a,d,g) bottom of the crucible, (b,e,h) left wall of the crucible, and (c,f,i) left corner of the crucible.
Materials 12 02312 g015
Materials 12 02312 g016 550
Figure 16. Images of Fe-26.38Si-9.35B droplets on the graphite substrate under vacuum in the sessile drop wettability test.
Figure 16. Images of Fe-26.38Si-9.35B droplets on the graphite substrate under vacuum in the sessile drop wettability test.
Materials 12 02312 g016
Materials 12 02312 g017 550
Figure 17. 2D-CT images of graphite crucible with solidified Fe-26.38Si-9.35B alloy at different angle position. (a) front view, (b) right side view, (c) rear view, and (d) left side view.
Figure 17. 2D-CT images of graphite crucible with solidified Fe-26.38Si-9.35B alloy at different angle position. (a) front view, (b) right side view, (c) rear view, and (d) left side view.
Materials 12 02312 g017
Materials 12 02312 g018 550
Figure 18. Photo of cross-sectioned graphite crucible with solidified Fe-26.38Si-9.35B alloy.
Figure 18. Photo of cross-sectioned graphite crucible with solidified Fe-26.38Si-9.35B alloy.
Materials 12 02312 g018
Materials 12 02312 g019 550
Figure 19. Calculated volume evolution of Fe-26.38Si-9.35B alloy with the decrease of temperature from 1450 °C to 600 °C.
Figure 19. Calculated volume evolution of Fe-26.38Si-9.35B alloy with the decrease of temperature from 1450 °C to 600 °C.
Materials 12 02312 g019
Table
Table 1. The thermal conductivity of the pure metal and its relative eutectic alloys.
Table 1. The thermal conductivity of the pure metal and its relative eutectic alloys.
MetalThermal Conductivity, λ (W/(m∙K))
30 °C100 °C300 °C500 °C700 °C900 °C1100 °C
Si[24]142.297.457.74029.828.928.7
Fe[25]71.765.452.841.935.534.735.6
B[26]26––––––
Fe-26Si-9B8164.947.337.131.330.330.6
Table
Table 2. The certified impurities in boron powder (ppm mass).
Table 2. The certified impurities in boron powder (ppm mass).
SampleBoron
Fe211
Cr11
Si16
Al51
Zr29
Mn1
Table
Table 3. The physical properties of the graphite and alumina crucibles.
Table 3. The physical properties of the graphite and alumina crucibles.
CruciblePropertyValueUnit
GraphiteBulk1.9mg/m3
Cumulative pore volume0.052m3/g
Open porosity10vol %
Radius of average open pores1.4µm
Thermal conductivity140W/(m∙K)
Al2O3Purity99.8%
Operating temperature range<1750°C
PermeabilityGas tight-
Water absorptionNone-
Table
Table 4. Chemical composition of the master alloy analyzed by ICP-MS (mass %).
Table 4. Chemical composition of the master alloy analyzed by ICP-MS (mass %).
Sample SiFeBAlMn
Fe-Si-B-1Detected26.6856.478.110.0670.21
Normalized29.1561.698.860.0730.23
Fe-Si-B-2Detected27.8766.459.540.180.23
Normalized26.7363.729.150.170.22
Nominal composition26.3864.279.35
Table
Table 5. Fe, Si, and B contents in FeSi, FeSiB3, FeB, and SiB6 phases measured with WDS (at %).
Table 5. Fe, Si, and B contents in FeSi, FeSiB3, FeB, and SiB6 phases measured with WDS (at %).
PhaseFeStd. Dev.SiStd. Dev.BStd. Dev.
FeSi45.5±1.243.2±1.111.3±1.7
FeSiB322.0±1.020.6±1.457.3±0.4
FeB47.7±0.90.23±0.952.0±0.1
SiB60.31± 0.110.6± 0.289.3± 0.2

Share and Cite

MDPI and ACS Style

Jiao, J.; Grorud, B.; Sindland, C.; Safarian, J.; Tang, K.; Sellevoll, K.; Tangstad, M. The Use of Eutectic Fe-Si-B Alloy as a Phase Change Material in Thermal Energy Storage Systems. Materials 2019, 12, 2312. https://doi.org/10.3390/ma12142312

AMA Style

Jiao J, Grorud B, Sindland C, Safarian J, Tang K, Sellevoll K, Tangstad M. The Use of Eutectic Fe-Si-B Alloy as a Phase Change Material in Thermal Energy Storage Systems. Materials. 2019; 12(14):2312. https://doi.org/10.3390/ma12142312

Chicago/Turabian Style

Jiao, Jianmeng, Bettina Grorud, Caroline Sindland, Jafar Safarian, Kai Tang, Kathrine Sellevoll, and Merete Tangstad. 2019. "The Use of Eutectic Fe-Si-B Alloy as a Phase Change Material in Thermal Energy Storage Systems" Materials 12, no. 14: 2312. https://doi.org/10.3390/ma12142312

Note that from the first issue of 2016, this journal uses article numbers instead of page numbers. See further details here.

Article Metrics

Back to TopTop