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Review Article

Processing and properties of macroporous silicon carbide ceramics: A review

Peer review under responsibility of The Ceramic Society of Japan and the Korean Ceramic Society.

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Pages 220-242
Received 17 May 2013
Accepted 10 Jul 2013
Published online: 18 Apr 2018

Abstract

Macroporous silicon carbide is widely used in various industrial applications including filtration for gas and water, absorption, catalyst supports, concentrated solar power, thermoelectric conversion, etc. During the past several years, many researchers have found diverse routes to fabricate macroporous SiC with porosity ranging from 9% to 95%. This review presents a detailed discussion on processing techniques such as partial sintering, replica, sacrificial template, direct foaming, and bonding techniques, as well as the mechanical and thermal properties of macroporous SiC ceramics fabricated using these methods. The full potential of these materials can only be achieved when properties are tailored for a specific application, whereas the control over these properties is highly dependent on the processing route. From the collected data, we have found that the porosity ranges from 9% to 91% with flexural strength of 1–205 MPa, compressive strength of 1–600 MPa, fracture toughness of 0.3–4.3 MPa m1/2, and thermal conductivity of 2–82 W/(m·K). This review will enlighten future investigations on processing of porous SiC and its usage in various applications.

1 Introduction

Porous silicon carbide (SiC) ceramics have been a focus of interesting research in the field of porous materials. Porous SiC ceramics are essential in a variety of industries due to their unique combination of properties such as excellent mechanical strength, good chemical resistance, high thermal conductivity, low thermal expansion coefficient, and high thermal shock resistance. These properties cannot be achieved from their conventional dense counterparts. Porous SiC ceramics are hence an ideal candidate for grinding materials, filters, catalytic supports, separation membranes, acoustic and thermal insulators, high-temperature structural materials, kiln furniture, thermoelectric energy conversion, and reinforcement of composites [1[2]18]. Many industries have exploited porous SiC in water filtration, porous burners, diesel particulate filters with honeycomb structures, metal matrix composites, polymer matrix composites, high-temperature/high-voltage semiconductor electronics, vacuum chucks, membranes, hot gas filters, and molten metal filters [19[20]27].

The processing methods used for the preparation of porous ceramics such as foams, honeycomb structures, interconnected rods, and hollow spheres were reviewed by Colombo [28[29]30]. The application of porous ceramics in a variety of fields has also been described in a recent book edited by Scheffler and Colombo [31]. The processing-microstructure-property relations for each of the main processing routes have been reviewed by Studart et al. [32]. Processing of ceramics components with hierarchical porosity was reviewed by Colombo et al. [33]. The processing methods used for the preparation of polysiloxane-derived porous ceramics were recently reviewed by Kumar and Kim [34]. Ohji and Fukushima reviewed more recent progress in processing and applications of macroporous ceramics [35]. They also suggested some issues to be resolved to further mine the potential of porous ceramics and to expand their applicability. While these valuable studies contain extensive information on the processing and applications of porous ceramics, only two short reviews on porous SiC ceramics are available [36,37] and an extensive review focused on macroporous SiC ceramics has not been made yet.

Extensive efforts have been devoted to controlling the sizes, amounts, shapes, locations, and connectivity of distributed pores, and this has resulted in improved and unique properties and functions of porous SiC ceramics [32,34,35,38[39]40]. The pore characteristics are commonly divided into pore morphology, porosity, and pore size. Amongst them, the pore morphology is also divided into open and closed pores. Open pores are distinguished into penetrating pores where fluid can penetrate and non-penetrating pores referred to as closed pores. Open pores are very important for separation-filtration and closed pores are beneficial for light-weight materials and heat insulating materials [41]. The pore size of macroporous SiC ceramics is an important property for filters to allow easy fluid flow [42]. The distribution of the size and shape of the pore space in porous ceramics is directly related to desired functions in particular applications. With the growing prevalence of porous SiC ceramics in industrial applications, a number of technologies have been developed to fabricate control their pore characteristics and to identify pore-related properties. This research has led to a deeper understanding of the relationship between various pore-related properties. For example, an increase in porosity generally results in decreased flexural strength [34,43[44]45]. Moreover, macroporous SiC ceramics with smaller pores generally have better flexural strength than ceramics with larger pores at an equivalent porosity [46]. Apart from mechanical properties, other properties such as thermal conductivity, electrical conductivity, thermal shock resistance, and gas permeability are influenced by the range of porosity. The gas permeability is relatively dependent on open porosity. The permeability decreases with a decrease in open porosity and is also slightly influenced by closed porosity [47]. Since pores retain air, the thermal conductivity is generally decreased with increased porosity [48].

From previous works, it is clear that the properties of macroporous SiC ceramics are strongly dependent on their porosity and microstructure. In turn, the porosity and microstructure of macroporous SiC ceramics are strongly dependent on their processing methods. The need to establish uniformity of cell size, shape, and volume in order to achieve superior part properties in specific applications has been strongly emphasized in various studies [34,49,50]. Thus, a better understanding of the processing methods and the property–porosity relations in macroporous SiC ceramics would be beneficial for achieving further progress in this field.

Because of the large number of articles in the field, this review mainly focuses on the processing and properties of macroporous SiC ceramics whose pore size is larger than 50 nm. Different processing routes for macroporous SiC ceramics have been developed for specific applications to satisfy the associated requirements for porosity, pore size, and degree of interconnectivity. The processes can be divided into five categories: (i) partial sintering, (ii) replica, (iii) sacrificial template, (iv) direct foaming, and (v) bonding techniques, as schematically illustrated in Fig. 1. It is also worth noting that even though we gathered many examples and classified them into five categories to illustrate some of the processing routes suggested thus far, a number of other approaches can be found in recent literature using similar concepts to those outlined here. The processing features of each technique are discussed and compared with regards to the versatility and ease of fabrication, as well as their influence on the microstructure, porosity, and properties of the macroporous SiC ceramics. Property–porosity relations including flexural strength–porosity, compressive strength–porosity, fracture toughness–porosity, and thermal conductivity–porosity relations are discussed in this paper. Finally, we suggest some remaining issues that should be addressed for future advances in this field.

Fig. 1 Schematic of processing methods: (a) partial sintering, (b) replica, (c) sacrificial template, (d) direct foaming, and (e) bonding techniques.

2 Processing routes

A wide range of processing routes have been proposed for the production of porous SiC ceramics, employing various raw materials from nature or artificial materials, leading to a variety of microstructure and pore morphologies. Each fabrication method is best suited for producing a specific range of pore sizes, pore size distribution, and overall amount of porosity [13]. This article intends to overview the main processing methods as well as the most recent improvements, advancement, and novel approaches that have been developed for macroporous SiC ceramics. The fabrication processes that have been discussed in this review article are (1) partial sintering, (2) replica method, (3) sacrificial template, (4) direct foaming, and (5) bonding technique. The basic principles of these methods are schematically presented in Fig. 1 and a list of macroporous SiC ceramics produced with these methods is given in Tables 15. The essential features of each of these routes are systematically discussed and compared in terms of the microstructural and pore characteristics of the macroporous SiC ceramics. More importantly, the influence of each processing technique on microstructure and mechanical properties of the macroporous SiC ceramics is critically discussed.

2.1 Partial sintering

Partial sintering is the simplest, frequently used and most conventional method to fabricate porous SiC ceramics. Particles of powder compact are bonded by partial sintering due to surface diffusion, evaporation–condensation, recrystallization or a solution–reprecipitation process. We can see a homogeneous pore structure when sintering is terminated before fully densified (Fig. 1(a)). Full densification is often retarded or prohibited by reducing the sintering potential. Reduced sintering potential is achieved by low sintering temperature, a constrained network of coarse powders, sintering without additives, and recrystallization. Pore size and porosity are controlled by the size of starting powders and degree of partial sintering. Generally, the powder has to be two to five times larger than the pore size required [35]. It has been previously postulated that the elastic modulus is directly dependent on the neck radius to particle radius ratio and such neck formation allows the elastic behavior to be directly related to the sintering kinetics. Examples of partial sintering method reported in the previous studies are shown in Table 1.

Table 1 Examples of partial sintering method reported in the literature.

Lin and Tsai [51] processed macroporous SiC ceramics by slip casting of submicron SiC powder-alumina additive mixtures and sintering at 1450–1800 °C. By varying both sintering temperature and alumina content (3–8 wt%), both porosity and pore size have been tailored within a range of 29–39% and 0.10–2.33 μm, respectively. Suwanmethanond et al. [5] processed porous SiC ceramics by pressureless sintering of SiC powder compacts with various additives including Al2O3, B4C, phenol resin, and carbon black. Fukushima et al. [14,52] also processed porous SiC ceramics by cold isostatic pressing (CIP) of submicron β-SiC powder and alumina additive mixtures and subsequent sintering at 1500–1800 °C. By varying sintering temperature, CIP pressure, and alumina additive, both the microstructure and pore size have been tailored. The pore size and particle size of the porous SiC membrane is found to be increased when there is no addition of alumina. By an addition of 4% alumina, it showed the retention of small pore sizes and fine particles. This was mainly due to the formation of SiO2–Al2O3 liquid phase from a thin SiO2 layer that exists on the surface of SiC particles and alumina. Treatment with higher CIP pressure reduced the pore size of the porous SiC ceramics effectively. Fukushima and coworkers [53] prepared porous SiC membrane supports which are sintered at 1500–1800 °C by using different additive contents and weight ratios of Al2O3/Y2O3. For the membrane support with 1 wt% additives, the pore size and grain size increased with increasing sintering temperature. However, the linear shrinkage and porosity did not change during heating because grain growth took place through surface diffusion and evaporation–condensation, resulting in an increase of pore size without shrinkage. Eom et al. [54] processed porous SiC ceramics from a carbon-filled polysiloxane without any templates by carbothermal reduction and subsequent liquid-phase sintering with Al2O3–Y2O3 as an additive and the obtained porosity ranged from 39% to 54% and pore size ranged from 0.003 to 30 μm. The grain morphology of the SiC grains transformed from equiaxed to platelet grains with increasing sintering temperature as a result of the β → α phase transformation of SiC and subsequent grain growth. Zhao and his colleagues [55] processed porous SiC ceramics by pressureless sintering silicon-resin coated SiC powder compacts containing Al2O3–SiO2–Y2O3 additives at 1350–1750 °C. The obtained porosity was in the range of 66–70%.

Ihle and his colleagues [56,194,195] have intensively studied the structure and phase formation of porous liquid-phase sintered SiC (LPS-SiC) containing Y2O3 and Al2O3 additives. Thermodynamic calculations and sintering experiments revealed that silicides or carbides can be formed in addition to stable oxides. The main parameters controlling the formation of the different reaction products are free carbon content, the oxygen activity, and the sintering temperature. They suggested that decomposition of oxide additives can be effectively suppressed and stable porous LPS-SiC can be produced by using CO containing atmospheres. Owens and Ruppel [62] fabricated porous SiC ceramics by forming SiC powder mixtures with a multimodal distribution of SiC particles and subsequent sintering. Kim et al. [44] processed porous SiC ceramics by adding large (65 μm) SiC particles or SiC whiskers into submicron SiC particles to restrain the densification. Yttrium aluminum garnet (Y3Al5O12, YAG) was added as a sintering additive. By controlling the content of large SiC whiskers or particles and the applied pressure during sintering, porous SiC ceramics with porosity ranging from 0.3% to 39% were fabricated. Fukushima et al. [63] added nano-sized SiC powder into submicron-sized SiC powder and sintered the formed body prepared from the powder mixtures at 1500–1800 °C. A higher CIP pressure treatment was effective in reducing pore size. The pore size and grain size increased with increasing sintering temperature. Enlarged neck regions were observed, due to the enhanced mass transfer from the nano-sized particles to the neck area. The increased neck area improved the compressive strength. Jang et al. [65,66] fabricated porous SiC ceramics using a submicron-sized and micron-sized SiC powder mixture without sintering additives by vacuum sintering at 1700–2000 °C. The obtained porosity was in the range of 30–40% and the average grain size increased with increasing sintering temperature. Kawamura et al. [67] processed porous SiC ceramics by synthesizing SiC from pelletized powder mixtures of Si and fullerene or Si and amorphous carbon at a temperature as low as 1000 K in sodium vapor. The obtained porosity was in a range of 66–71%. Hotta et al. [60] processed porous SiC ceramics with 1 wt% Al2O3 or 1 wt% AlN–Y2O3 additives by spark plasma sintering. A flexural strength of 95 MPa at 42% porosity was obtained in the porous ceramics and the obtained porosity was in a range of 32–39%. Zhou et al. [61] fabricated porous SiC tubes by extrusion forming and partial sintering methods. The tubes sintered at 1800–1900 °C had porosities of 40–46% and pore sizes of 0.19–1.70 μm.

Liu et al. [68] fabricated wood-like porous SiC ceramics without a template via high temperature recrystallization process by mimicking the formation mechanism of cellular structure of woods. The decomposition of SiC produces the gas mixture of Si, Si2C and SiC2 above 1800 °C. The possible reactions are given as follows:(1) SiC(s)Si(g)+C(s)(1) (2) 2SiC(s)Si(g)+SiC2(g)(2) (3) Si(g)+SiC(s)Si2C(g)(3)

The Si-carrying gas species play a role as a transport medium for carbon and SiC. The directional flow of gas mixture in porous green body induces the surface ablation, rearrangement, and recrystallization of SiC grains, which leads to the formation of the aligned columnar fibrous SiC crystals and tubular pores in the axial direction. Representative morphologies of wood-like porous SiC ceramics are shown in Fig. 2 [68]. The pressure and concentration gradients are two driving forces for the transport of the produced gases. The orientation degree of SiC crystals and the pores in the axial direction strongly depend on the temperature and pressure so that it increases with increasing temperature while it decreases with increasing furnace pressure. The obtained porosity was in range of 53–61% and it increased with increasing the sintering temperature within a range of 1950–2300 °C.

Fig. 2 Typical morphologies of wood-like porous SiC ceramic fabricated by partial sintering: (a) the radial section surface and (b) the axial section surface [68].

Reproduced with the permission of Elsevier.

Kim et al. [69] processed porous SiC ceramics with interconnected huge plate-like grains via recrystallization from oxidized β-SiC powder with 1 wt% B4C. β-SiC powders were oxidized at 650 °C for 2 h to remove the free carbon present in it. When β → α phase transformation occurred at 2100 °C, rapid grain growth of α-SiC consumed the unstable β-SiC matrix resulting in an interconnected network structure with huge plate like grains. Both the oxidation of β-SiC powder and the addition of B4C are essential for rapid grain growth via a gas phase reaction, such as an evaporation–condensation reaction. Typical microstructure of porous SiC ceramics with interconnected huge plate-like grains is shown in Fig. 3 [69]. The porosity and mean pore size of the porous SiC ceramics were 47% and 6–7 μm, respectively.

Fig. 3 Typical microstructure of porous SiC ceramics with interconnected huge plate-like grains produced by partial sintering method [69].

Reproduced with the permission of Elsevier.

In summary, partial sintering is the simplest and easiest way to fabricate porous SiC ceramics with porosity ranging below 65% and with pore size ranging from 0.1 to 10 μm. In this technique, particles of a SiC powder compact are bonded by partial sintering due to surface diffusion, evaporation–condensation, recrystallization or a solution–reprecipitation process. Full densification is retarded or prohibited by reducing the sintering potential. Reduced sintering potential is achieved by low sintering temperature, a constrained network of coarse powders, sintering without additives, and recrystallization. A very homogeneous pore structure with narrow pore size distribution has been successfully prepared through recrystallization process. One of the advantages of this method in the processing of porous SiC ceramics is an easiness of dimensional control, owing to the occurrence of grain growth without any shrinkage and densification, which can be obtained due to the strong covalent bonding characteristic of SiC.

2.2 Replica method

The replica method is based on the copy of the original foams concerning its pore shape and strut structure. Three different techniques were suggested to produce macroporous SiC ceramics: (1) impregnation of polymer foams with SiC suspension or precursor solution, (2) chemical vapor deposition (CVD) of SiC on polymeric foams, and (3) infiltration of natural wood-derived or artificial carbon foams with Si sources. Macroporous SiC ceramics with open cells of high volume porosity and with cell sizes ranging from 100 μm to millimeters are frequently fabricated by the replica method. Examples of replica method reported in the literature are shown in Table 2. The original invention of using a sponge as a template was from Schwartzwalder and Somers [196]. In early 1960s, they used a polymeric sponge to prepare ceramic cellular structure of various pore sizes, porosities, and chemical compositions. Since then the sponge replica technique has become the most popular method to produce macroporous ceramics with high porosity and open cells. The most frequently used synthetic template is polymeric sponge such as polyurethane (PU) [197[198]203]. The method is being widely used to produce filters or light weight structures in various applications. Porosity range of more than 90% can be produced using this method. SiC filter for molten metals is a typical example produced through the replica technique.

Table 2 Examples of replica method reported in the literature.

The first method based on impregnation of polymer foams with a SiC suspension or precursor solution involves (i) impregnating the porous or cellular structure with SiC suspension or precursor solution, (ii) removing the excess suspension by passing through rollers or centrifuges, (iii) drying the SiC or precursor coated polymer sponge, (iv) heat treatment through careful heating to remove the polymer sponge by decomposition, and (v) densification of the SiC coating by sintering in an appropriate temperature [70[71]73,79,80]. The impregnation of a cellular structure with a SiC suspension or precursor solution produces macroporous SiC ceramics which exhibit facsimile morphology of original porous material. Reticulated porous SiC ceramics processed by the above method contains triangular pores inside struts after the organic sponge is burned out, making them sensitive to structural stresses and limiting their structural applications. Zhu et al. [74] developed a recoating method to improve mechanical strength of the reticulated porous SiC ceramics. In the method, the coating process is composed of two stages. In the first stage, a thicker slurry is used to coat the sponge preform uniformly. The green body is preheated to produce a reticulated preform with sufficient handling strength after the sponge has been burned out. In the second stage, the preform is recoated by a thinner slurry using centrifugal method. By this method mechanical strength of the reticulated porous SiC ceramics has been improved significantly. The authors also suggested that the flexural strength of reticulated porous SiC ceramics improved remarkably as the solid content of SiC slurries increased [70,71].

Mouazer and coworkers [72] fabricated porous SiC ceramics using SiC powder, B4C–graphite as a sintering aid, gelatin as a gelling agent, and polyurethane foam as a template for replica technique. In the study, pores of polyurethane foam were filled with aqueous slurry of ceramic powders with appropriate amount of gelling, anti-foaming and dispersing agents. The sponge is compressed to ensure that it is completely filled with slurry and rolled on to remove excess of slurry. The porous SiC foams with a porosity ranging from 78% to 88% were obtained after drying, calcination, and sintering at 2120 °C for 1 h in argon. Boron-doped SiC has a good electrical conductivity and making it suitable for electrically conductive foam. Yao et al. [75] processed reticulated porous SiC ceramics with polyurethane sponges by using MgO–Al2O3–SiO2 additives at 1000–1450 °C. The sintering additives are employed from alumina, kaolin and talc powders. By adding the sintering additives, the authors could lower the optimum sintering temperature to 1300 °C, which was at least 100 °C lower than that with Al2O3–SiO2 additives. Soy et al. [76] fabricated reticulated porous SiC ceramics using a ceramic slurry consisting of SiC powders and bentonite (montmorillonite). Bentonite was used as both a binder for ceramic slurry at room temperature and a sintering additive at elevated temperatures. Increasing bentonite content from 1 wt% to 10 wt% decreased the porosity from 86% to 84% and increased mechanical strength.

Due to the covalent nature of Si–C bonds, porous SiC ceramics normally needed to be sintered at high temperatures or/and with the addition of sintering additives, which have limited the application of porous SiC ceramics. New processing routes that overcome these problems are the preceramic polymer processes, during which the polymer precursors convert into ceramic materials. This process has an advantage of requiring usually low temperature of 1000–1200 °C [72]. Some examples of the processing route using precursor solutions are described here. Bao et al. [79] processed reticulated SiC ceramics using polysilane polymeric precursors. Polyurethane foams were immersed in polysilane precursor solutions and these were heated in nitrogen at 900–1300 °C. The SiC foams produced in this manner showed well-defined open-cell structures and the struts were free of voids. Nangrejo and Edirisinghe [80] used two types of polymeric precursors for SiC and dichloromethane as a solvent for processing reticulated SiC ceramics. PU foams were soaked in precursor solutions and subsequently pyrolyzed in nitrogen to produce SiC foams. It was possible to control the sintering shrinkage by varying the concentration of polymeric precursor and/or second phase fillers [204,205]. A representative microstructure of the reticulated SiC ceramics fabricated from SiC slurry consisted of well-defined open-cell structures as shown in Fig. 4(a) [73]. Vogt et al. [21] processed macroporous SiC foams by dipping PU foams several times into the polysiloxane (MK polymer) precursor slurry. After first coating cycle, the PU foam was decomposed, leaving hollow struts inside the ceramic structure, and simultaneously polysiloxane was pyrolyzed. Highly porous SiC ceramics with porosities higher than 96% were obtained by the process and the struts were polycrystalline and contain voids which were formed after removal of the unreacted carbon. The polysiloxane-derived phase acts as an additional binding phase at elevated temperatures and allows an appropriate handling for reinfiltration of the foam structures before nitridation at 1400 °C or recrystallization at 1850 °C [82]. Aoki and McEnaney [110] developed a modified replication method for producing SiC foams by (i) coating of polymer foams with phenolic resin, (ii) carbonization of the resin by pyrolysis, (iii) reaction of the resin-derived carbon foam with Si vapor at high temperatures and (iv) removal of the unreacted carbon by oxidation at 800 °C.

Fig. 4 Typical microstructures of macroporous SiC ceramics produced via the replica technique: (a) SiC foams produced by impregnation of polyurethane sponges with SiC slurry [73], (b) SiC foams produced by CVD process [85], (c) SiC foams produced by infiltration of wood-derived carbon foams with Si vapor [88] and (d) SiC foams produced by infiltration of wood-derived carbon foams with Si vapor [111].

The second method based on CVD of SiC involves CVD coating of SiC on polyurethane foams. Duocell® SiC foams (Oakland, California) are produced by this method. The cellular materials presented an open cell microstructure consisting of interconnected SiC struts which defined polyhedral cells with 12–14 faces (Fig. 4(b)) [85].

The third method based on the infiltration of natural wood-derived carbon foams with Si sources involves (i) pyrolysis of woods for making carbon foams and (ii) infiltration of the carbon foams with gaseous or liquid Si, SiO2, or TEOS to form SiC or Si-SiC ceramics [8,38,39,48,71,82[83]106]. Ota and coworkers [82] were probably first team to use wood as a natural template to produce cellular ceramics with alkoxide solutions via sol–gel chemistry. Based on this work, Greil and coworkers [39,83[84]88] processed cellular SiC ceramics with anisotropic pore structures by infiltration of liquid Si into carbonized wood and subsequent reaction to SiC. The procedure was to heat the wood in non-oxidizing atmosphere at temperatures between 800 and 1800 °C which resulted in decomposition of the polyaromatic constituents to form carbon preforms. The biological carbon preforms were used as templates for infiltration with gaseous or liquid Si to form cellular SiC and Si/SiC ceramics. Depending on the initial cellular microstructure of the various kinds of wood, SiC ceramics of different anisotropic pore structures in the form of pseudomorphs of the original wood were obtained [83]. According to Greil’ data [86], the porosities ranging from 32% to 91% were obtained depending on the wood. Maximum diameters for the tracheal cells were in the range of 50 μm for pine up to 350 μm for oak. The anisotropic nature of cellular SiC ceramics produced using wood as template might be advantageous in applications that require open and highly oriented porous structures, such as in catalytic supports and in the filtration of hot gases [86]. Lopez-Alvarez and coworkers [106] used juncus maritimus which is also known as sea rush as a template to fabricate porous SiC scaffolds. Sea rush is thermally decomposed and subsequently infiltrated by molten Si in order to fabricate 3D porous SiC scaffolds that preserve the original microstructure of the plant. The average pore diameter and porosity of the SiC scaffolds were 12 μm and 48%, respectively. Qian et al. [107] processed porous SiC ceramics by carbothermal reduction of charcoal–SiO2 composites in argon atmosphere, which was fabricated by infiltrating silica sol into porous wood-derived carbon foams. Many other researchers [89,91,93,94,96,99,100,104,108,109] processed porous SiC ceramics with a variety of wood-derived templates, but their strategies are basically same with Greil’ approach. Typical microstructure of SiC foams produced by infiltration of wood-derived carbon foams with Si vapor is shown in Fig. 4(c) [88].

Herzog et al. [97] developed modified wood-based process by using wood-based fiberboards as a template for overcoming the inhomogeneity problem that hinders the use of natural bulk wood as a template for SiC components. In the process, wood-based fiberboards were prepared by pressing technique and the boards were transformed into carbon foams by pyrolysis. The carbonized wood-based material was infiltrated with SiO2 sol and transformed into porous SiC by the carbothermal reduction process. The obtained structural properties of the materials were isotropic and porosities were in the range of 55–74%. Qian et al. [92] processed macroporous SiC ceramics by (i) pressing phenol resin impregnated wood powders, (ii) pyrolysis, (iii) infiltration of Si at 1450–1600 °C, and (iv) removal of residual Si at 1700 °C. Pore structure of the obtained materials was homogeneous and porosities were ranged between 65% and 75%.

The artificial carbon foams for processing porous SiC ceramics by replication method involve resin-derived carbon foams [110], paper-derived carbon foams [111], and mesophase pitch [112,116]. SiC foams were produced by siliciding the carbon foams with Si vapor sources, such as Si3N4, vapor or liquid Si, and CH3SiCl3. A typical microstructure of the porous SiC ceramics fabricated from artificial carbon foams is shown in Fig. 4(d) [111]. Xue and Wang [113] processed porous SiC ceramics from cotton and phenol resin-derived carbon foams by liquid Si infiltration. The obtained porosity was in range of 10–35%. Cho et al. [114] fabricated porous SiC ceramics by dip-coating porous reaction-bonded SiC supports with slurries consisting of fine SiC powders and phenol resin and by slicing the coated layer with liquid Si. By the process, porous SiC ceramics with multi-layered pore structure were produced for hot gas filter applications. Shimada and his colleagues [115] processed porous SiC ceramics from a clutch lining waste-derived carbon foams and Si sources such as tetraethoxysilane and SiO by reacting them at 1500–1600 °C. The obtained porosity was about 80%.

In summary, the replica method is the most appropriate technique to produce open-cell SiC ceramics with pore sizes ranging from 10 μm to 5 mm at porosity levels between 60% and 95%. The adhesion of an impregnating suspension on a polymeric sponge is the most crucial step in the polymer replica technique. While this technique benefits from its overall simplicity, the mechanical strength and reliability of porous structures produced with this method can be substantially degraded by the formation of hollow struts and cracked struts during pyrolysis of the polymer sponge [32]. Wood-derived carbon foams have also been used as templates to produce porous SiC ceramics. Wood-derived porous SiC ceramics have an anisotropic pore structure, resulting in anisotropic properties. The several steps required to convert the wood structures into macroporous SiC ceramics might excessively increase the cost of the product [32]. Based on various processing parameters in replica method, the available data indicate a minimum flexural strength of 0.7 MPa with 86% porosity [70] and a maximum flexural strength of 205 MPa with 9% porosity [113] for the porous SiC ceramics.

2.3 Sacrificial template method

The sacrificial template method is one of the techniques to fabricate porous SiC ceramics by mixing appropriate amounts of sacrificial template as a pore forming agent with SiC powders or SiC precursors, forming a biphasic composite using the template-SiC powder or precursor mixtures, and removing the template before or during sintering process to create pores (Fig. 1(c)) [31,43,46,50,117,136]. This method leads to porous materials displaying a negative replica of the original sacrificial template, as opposed to the positive morphology obtained from the replica technique [32]. The way that the sacrificial template is extracted from the biphasic composites depends primarily on the type of pore former employed. A wide variety of sacrificial materials have been used as templates, including synthetic and natural organics, liquids, salts, metals, and ceramics. Table 3 illustrates some examples of possible sacrificial templates. Synthetic and natural organics are often extracted through decomposition by applying thermal treatments at temperatures between 200 and 1000 °C [43,45[46]47,118[119]124,134,135]. Liquids are often extracted through freeze drying or sublimation after freezing [137[138]139]. Carbon and SiO2 templates are removed by oxidation [117,141[142]143] and chemical leaching [117,146], respectively. Salts are often extracted by leaching using water [140].

Table 3 Examples of sacrificial template method reported in the literature.

Polymer microbeads and microspheres have been frequently employed for sacrificial template method. For example, Kim and his colleagues [43,46,47,118] fabricated porous SiC ceramics by (i) mixing SiC powders, sintering additives, and polymer microbeads, (ii) forming by dry pressing, (iii) subsequent heat-treatments for decomposing the templates, and (iv) sintering the formed body. By controlling the microbead content and sintering temperature, it was possible to achieve tailored porosity ranging from 16% to 69% [43]. Eom et al. [47] processed porous SiC ceramics with various microstructures by controlling α/β ratio in the starting SiC powders. A typical microstructure obtained from 1% α-SiC and 99% β-SiC powders is shown in Fig. 5(a) [47]. Polymer precursors and artificial templates have also been used for producing porous SiC ceramics via sacrificial template method. Kim and his colleagues [45,119[120]123,125[123]128] developed a new processing method for fabricating macroporous SiC ceramics from carbon-filled polysiloxane by carbothermal reduction and subsequent sintering process. The strategy adopted for making porous SiC ceramics involves the following: (i) fabricating a formed body from a mixture of polysiloxane, carbon source such as phenol resin or carbon black, SiC powder as an optional inert filler, sacrificial templates, and sintering additives; (ii) pyrolysis of polymeric materials; (iii) synthesizing SiC by carbothermal reduction; and (iv) sintering the materials. The sacrificial templates used were polymer microbeads, hollow microspheres or expandable microspheres. In the process, SiC can be synthesized from the polysiloxane, if an additional carbon source is added and the mixture is heated at higher temperatures (>1400 °C) [119,206]. By controlling the template, inert filler, additive contents, and sintering temperature, it was possible to adjust the porosity so that it ranged from 40% to 95%. Kotani et al. [131] fabricated porous SiC ceramics using allylhydrido-polycarbosilane as a SiC precursor and polymer microbead as a template. The final product was formed without critical crack initiation and it was possible only, when the polymer was sufficiently contained to make a strong skeletal structure. Eom et al. [124] and Kumar et al. [133] fabricated highly porous SiC ceramics using poly(ether-co-octane) and hollow microsphere with more than 78% of porosity. Jin and Kim [50] processed highly porous SiC ceramics by pyrolyzing a cross-linked body consisting of polycarbosilane (PCS) and polymer microbeads at 1100–1400 °C in an argon atmosphere. By controlling the microbead content and pyrolysis temperature, it was possible to achieve tailored porosity ranging from 56% to 88% [50]. A typical microstructure obtained by the process is shown in Fig. 5(b) [50].

Fig. 5 Typical microstructures of macroporous SiC ceramics produced via the sacrificial template technique: (a) SiC foams produced using polymer microbead as a template and β-SiC powders [47], (b) SiC foam obtained using polymer microbead as a template and polycarbosilane as a SiC precursor [50], and (c) SiC foams produced by gelation-freezing method parallel to the freezing direction [137] and (d) perpendicular to the freezing direction [137].

(a), (c) and (d) are reproduced with the permission of Elsevier and (b) is reproduced with the permission of Springer.

Eom et al. [47,207,208] suggested three different strategies for controlling microstructure of porous SiC ceramics: (1) control of post annealing temperature, (2) control of additive content, and (3) control of initial α-SiC content in the starting powder. In the first strategy, the grain size increased with an increase of the annealing time and the morphology of SiC grains changed from equiaxed to cube after an annealing at 1750 °C and to hexagonal platelets after an annealing at 1950 °C [207]. In the second strategy, a toughened strut microstructure was obtained in porous SiC ceramics by the carbothermal reduction of polysiloxane-derived SiOC containing hollow microspheres, followed by sintering with Al2O3–Y2O3–CaO, as a result of enhanced grain growth due to the bimodal distribution of SiC, low viscosity of the liquid phase, and the β → α phase transformation of SiC. In the last strategy, by adjusting the initial α-SiC content in the processing of porous SiC ceramics, the grain morphology can be controlled from equiaxed to large platelet grains. A microstructure consisting of large platelet α-SiC grains were obtained from β powder or a mixture of α/β powders containing small (≤10%) amounts of α powders by sintering at 1950 °C for 4 h. Song et al. [132] fabricated porous SiC by a novel processing route with a duplex pore structure which is developed by using a polysiloxane, carbon black, SiC, Al2O3, Y2O3, and two kinds of pore former (expandable microspheres and PMMA spheres). It is fabricated by carbothermal reduction of a polysiloxane-derived SiOC and a subsequent sintering process. Two kinds of pore formers, expandable microspheres and PMMA spheres, were added simultaneously to create a duplex pore structure with high permeability. The duplex pore structure consists of large pores derived from the expandable microspheres and small windows in the struts that were replicated from the PMMA spheres. The presence of these small windows in the strut area improved the permeability of the porous ceramics.

Eom et al. [209] investigated the effect of forming methods and fabricated porous SiC from blends of carbon-filled polysiloxane. They used three different plastic forming methods like compression molding, injection molding and extrusion method. Each method gave different microstructures and porosities. The compression molding process led to more homogenous microstructure and lower porosity (72%) than the other forming methods. The extrusion and injection molding methods resulted in the production of porous SiC ceramics with 84% and 74% of porosities, respectively. Additive composition also found to result in different porosities and microstructures [129,130]. The obtained porosity of porous SiC ceramics fabricated from polysiloxane-derived SiOC by carbothermal reduction and subsequent sintering ranged from 56% to 72% after sintering at 1750 °C, depending on the additive composition.

Natural organics such as wax, dextrin, yeast, and agar were also used as templates for producing SiC foams. Roy et al. [134] processed porous SiC ceramics using SiC powder and wax as a template. Ying et al. [135] and Chi et al. [136] used dextrin and yeast as a template, respectively, to fabricate porous SiC ceramics. Yeast belongs to microorganism and is mainly composed of C, H, O, N, P and S elements. The surface of yeast has many pores with a porosity of 29.7%, which was measured from mercury porosimetry. Therefore, some slurry is adsorbed on the surface of yeast. Yeast completes its pyrolysis at higher temperature than general pore former, which relieves the closing of pores without deleterious residual and reaction with the green body. The sintering behavior of porous SiC ceramics showed a great difference with the change in content of sintering aid (Al2O3) and the optimal content of Al2O3. In addition, the sintering temperature and hold time had great influence on sintering properties of porous SiC ceramics [136]. Glycerol was adopted as stabilizing agent to decrease the sedimentation of the raw materials during processing. Glycerol has a high viscosity of 1499 mPa s and can bind SiC particles in the pores on the surface of the yeast.

Fukushima and his coworkers [137] produced porous SiC by a gelation-freezing method. In the method, raw powder was firstly dispersed into water (which acts as a pore former) with a gelation agent. After gelation, the wet gel is immersed into cold ethanol to form ice crystals. A vacuum freeze drier is used to dry the frozen gel, so that the ice is sublimated without shrinkage of green body and then sintered to obtain porous SiC ceramics. Using the gelation-freezing technique SiC foams with high porosity (∼87%) and unidirectional oriented micrometer-sized cylindrical pores were prepared [32,137]. Typical microstructures of SiC foams produced by the gelation-freezing method are shown in Fig. 5(c) and (d) [137]. Yoon et al. [138,139] processed porous SiC ceramics from PCS/camphene solution by a freezing method. In the technique, camphene is used as a pore former. The solution prepared at 60 °C was cast into a mold at a temperature ranging from 20 to −196 °C. It results in a bi-continuous structure with regularly patterned interconnection. After the freeze casting solidification, camphene grows dendritically toward the center of the cast body. Pore size decreases by lowering freezing temperature. The sample even frozen at liquid nitrogen shows a highly porous structure, implying the effectual growth of camphene dendrites during freezing. After the removal of the frozen camphene network by sublimation, the samples showed highly porous structure. Pyrolysis of porous PCS object at 1400 °C for 1 h in argon atmosphere produced porous SiC ceramics with oriented porosity. Fitzgerald et al. [140] used sodium chloride compact for producing fine open-cell SiC foams. In this process, PCS is first pressure infiltrated into a porous sodium chloride compact, having a controlled particle size and density. The salt is subsequently leached away using water; the resulting PCS foam is cured by heating in air; and finally pyrolyzed into a SiC ceramic. Homogeneous open-cell SiC foams were produced with controlled cell sizes varying roughly between 10 and 100 μm and controlled relative densities. Wang et al. [117] used carbon fiber, carbon nanotube, and nylon filter as templates and polymethylsilane as a precursor for SiC. Template derived porous SiC plates, SiC nano-net, fiber-inverse and bead-inverse porous SiC ceramics were prepared from polymethylsilane as a SiC precursor and the above templates. The fabrication procedure involves the infiltration of the templates with appropriate concentration of the polymethylsilane, curing of the precursor, precursor pyrolysis and subsequent template removal by oxidation or chemical leaching. Park and his coworkers [142] processed porous SiC ceramics by hot-pressing a SiC nano powder-carbon nano powder-sintering additive mixture and subsequent oxidation at 700 °C in air. By adjusting the carbon content it was possible to control the porosity within a range of 30–50%. Bereciartu et al. [144] fabricated porous SiC with different pore size distributions using mesocarbon microbeads as a sacrificial template from with/without using Y2O3 and Al2O3 as sintering additives. Different sizes of SiC and carbon powders are used to investigate their effect on porosity and mechanical properties. The experimental result shows that the usage of nanometric sized SiC and C powders resulted with the porous SiC ceramics with higher porosity than micrometer sized powders. Yamane et al. [145] fabricated porous SiC from Si powder and carbon black at 900 °C for 24 h in Na vapor. They used grains of Si powder as a source of Si and template for pore forming. The porosity of porous SiC ceramic was around 55–59%. Sung et al. [147] processed macroporous SiC with a highly ordered pore array by infiltrating polymethylsilane solution into a colloidal silica template, pyrolysis of polymethylsilane, and subsequent silica template leaching using HF solution.

In summary, the sacrificial template method is the most appropriate technique to tailor the porosity, pore size distribution, and pore morphology of the final porous SiC ceramics through appropriate choice of the sacrificial template, because pore size, pore shape, and porosity are controlled by the size, shape, and content of the template used. The pore size and porosity attained in this method ranged from 1 to 700 μm and from 15% to 95%, respectively, depending on the template content and processing conditions. The replica method generally produces open-cell macroporous structure, whereas the sacrificial template method is preferred to produce micro or macrocellular structures with interconnected porosity [34,121]. A gelation-freezing process using water as a fugitive template can produce SiC foams with excellent compressive strength (17 MPa) at high porosity (∼86%) because of the formation of unidirectional oriented micrometer-sized cylindrical pores [137].

2.4 Direct foaming method

Direct foaming usually generates bubbles inside ceramic slurries containing SiC powders or inside polymeric precursor solutions to create SiC foams. In this technique, ceramic or precursor suspension is foamed with blowing agents to create stabilized foam, dried and subsequently sintered to obtain macroporous SiC ceramics (Fig. 1(d)). The blowing agents can be volatile liquids, gas evolving solids, or gases that can be evolved in situ by chemical reactions or can be added to the liquid mixture by mechanical stirring or bubbling (gas injection). Nucleation and growth of the gas bubbles inside the precursor liquids or ceramic slurries are influenced by the presence of suspended particles and the viscosity of the slurries. The blowing agents are classified into physical and chemical blowing agents. Chemical blowing agent produces gaseous products by a chemical reaction whereas the physical blowing agent does not accompany chemical reactions and the bubble/foam-making process is reversible. Table 4 illustrates some examples of possible blowing agents for producing porous SiC ceramics by direct foaming technique.

Table 4 Examples of direct foaming method reported in the literature.

Several routes have been developed in last decades to prepare porous SiC ceramics using direct foaming method. Porous SiC ceramics can be produced by using thermosetting properties of Si-based polymers in combination with in situ blowing agents, either in the presence of surfactants [42,148] or by applying the pressure-drop technique [151,152] or by applying steam chest molding [154]. Mouazer et al. [42] introduced foaming-gel casting process with surfactants (Triton X-114 and Tergitol TMN-10) as a blowing agent for the production of porous SiC ceramics. They investigated the effect of the amount of agar (gelling agent) on the final porosity of the ceramic foams. The porosity increased with a decrease in the amount of agar. The suspension viscosity affects the foam volume and consequently the final density of the samples. By changing the agar concentration, it was possible to fabricate SiC foams with a wide range of porosity from 78% to 88% without cracks. Fukushima and Colombo [148] fabricated porous SiC foams from direct blowing of PCS with a chemical blowing agent (azodicarbonamide). This process was simple and efficient to produce porous SiC foams with tailored pore architecture and porosity. Porosity ranging from 59% to 85%, and cell size ranged from 416 to 1455 μm was obtained from this method. A typical microstructure of SiC foams produced by the direct blowing of PCS is shown in Fig. 6(a) [148]. Bao et al. [149] processed SiC foams by using volatiles, as a pore former, which were generated by the decomposition of the polymeric precursors. It was possible to control the porosity of the SiC ceramics by controlling the gas evaporation by tailoring the composition and structure of the polymeric precursors. Good shape retention was obtained in the polysilane precursors with higher functionalities and pyrolytic yields between 50 and 60 wt%. Qiu et al. [150] processed SiC foams with nano-sized grains by combustion synthesis of gel-cast Si/C foam containing n-octylamnie as a blowing agent. The as-synthesized SiC foam has a high porosity in the range of 70–90%.

Kim et al. [151] introduced a new route in direct foaming to fabricate porous SiC from preceramic precursors using CO2 as a blowing agent. The subsequent steps involves: (i) saturation of preceramic polymers using gaseous, liquid, or supercritical CO2, (ii) nucleation and growth of a large number of bubbles using thermodynamic instability via a rapid pressure drop and/or heating, and (iii) transforming the microcellular preceramic polymers into microcellular ceramics by pyrolysis and (optional) subsequent sintering [151[152]153,210]. The experimental result reveals that if the microcellular structures are preserved during the transformation of the preceramic to ceramic, porous ceramics with an extremely fine and homogeneous cell structure could be fabricated. Microcellular SiC ceramics having cell density above 109 cells/cm3 and cell size below 10 μm were fabricated using PCS and/or polysiloxane precursors [151]. The same group also introduced a new processing route in direct foaming by applying steam chest molding [154]. The fabrication process involved the following steps: (i) blending a mixture of polysiloxane, carbon, hollow microspheres, and sintering additives, (ii) steam chest molding of the mixture, (iii) transforming the polysiloxane by pyrolysis into silicon oxycarbide, and (iv) fabricating SiC foams by carbothermal reduction of silicon oxycarbide and subsequent sintering. Porosity of the foams could be controlled by controlling the initial packing density in the steam chest molding step. A representative microstructure of SiC foams produced by the steam chest molding is shown in Fig. 6(b) [154]. It shows a uniform cellular structure with open-cells.

Fig. 6 Typical microstructures of macroporous SiC ceramics produced via the direct foaming technique using (a) azodicabonamide as a chemical blowing agent [148] and (b) water vapor as a physical blowing agent [154].

(a) is reproduced with the permission of Elsevier and (b) is reproduced with the permission of John Wiley and Sons.

In summary, the direct foaming technique is an easy and fast way to prepare both open and closed-cell structures with a wide range of pore size and porosity, up to 95% [32,34,35]. The structures have well interconnected porosity with unique permeability that allows finer adjustment of fluid transport within the structure [34,211]. The total porosity of directly foamed ceramics is proportional to the amount of gas incorporated into the suspension or liquid medium during the foaming process. The main advantage of this method is the possibility of producing dense ceramic struts and defect-free struts, providing a stronger foam in comparison with the replica method. One drawback of this method is the difficulty in producing a material with a narrow pore size distribution [28,32,151]. As long as PCS or polysiloxane is used as a precursor to SiC, the preceramic polymers should be blown first before cross-linking. Otherwise, direct foaming of the preceramics polymers would be difficult in the processing of porous SiC ceramics via direct foaming.

2.5 Bonding technique

Porous SiC ceramics can be produced mainly by partial sintering [212], replica [213,214], sacrificial template [215], and direct foaming [66,216] methods. Different processing routes for porous SiC ceramics have been developed for specific applications to satisfy the associated requirements of porosity, pore size, and degree of interconnectivity. However, all the above methods require high temperatures of ≥1500 °C for the processing if SiC powder is used as a starting material because of its strong covalent bonding characteristic. Thus, one of the key issues in the processing of porous SiC ceramics is how to produce porous SiC ceramics at relatively low temperatures. One way to lower the processing temperature is to use preceramic polymers as a precursor for SiC. Another way to lower the processing temperature of porous SiC ceramics is the use of bonding materials. The in situ reaction bonding process can realize the low-temperature fabrication of porous SiC ceramics (Fig. 1(e)) [155,156]. Alkali, cordierite (2MgO·2Al2O3·5SiO2), mullite (3Al2O3·2SiO2), silica (SiO2), Si, SiC, silicon nitride (Si3N4), silicon oxycarbide (SiOC), and frit phases were investigated as bonding materials for porous SiC ceramics. Porous SiC ceramics containing a bonding phase and moderate porosity possess a unique set of characteristics, such as high thermal shock resistance, chemical stability, high specific strength, and cost-effectiveness. Table 5 illustrates some examples of possible bonding materials for producing porous SiC ceramics by the bonding technique.

Table 5 Examples of bonding technique reported in the literature.

2.5.1 Porous mullite-bonded silicon carbide

It has been reported that the oxidation resistance of recrystallized SiC was improved by the incorporation of a mullite coating on the SiC [217]. Similarly, the corrosion resistance of SiC in contact with coal slag was improved by introducing a chemically vapor-deposited mullite coating on the SiC [218]. Ando et al. [219] reported that mullite-SiC composites have the ability to heal semicircular cracks having diameters of up to 200 μm. A new approach that has received much attention is the incorporation of mullite as a bonding phase in SiC. Silicon carbide has good hardness, strength, and wear resistance, whereas mullite (3Al2O3·2SiO2) has good oxidation resistance and high temperature stability. Furthermore, mullite has good chemical compatibility with SiC, and both materials have similar thermal expansion properties [220]. Thus, the combination of mullite and SiC to form mullite-bonded SiC is an attractive approach and the porous ceramics are expected to exhibit better properties than porous mullite or porous SiC for some applications in oxidizing atmosphere.

Porous mullite-bonded SiC ceramics are fabricated from SiC, Al sources such as Al, AlN, Al2O3, and Al(OH)3, and templates using an in situ bonding technique [156[157]168,221]. It has been reported that the oxidation-derived SiO2 and Al sources react in situ to fabricate porous mullite (3Al2O3·2SiO2)-bonded SiC ceramics at 1400–1550 °C in air [156,157,159,162,165]. Meanwhile, the templates are decomposed or burned out, leaving pores inside the materials. She et al. [156] firstly developed a unique technique to produce mullite-bonded porous SiC ceramics by an in situ oxidation bonding technique. The surface of SiC particles is oxidized to form SiO2 with high reaction activity and the oxidation-derived SiO2 can easily react with the added Al2O3 and form a mullite to bond SiC particles at 1400–1500 °C in air. Ding and coworkers [158] processed porous mullite-bonded SiC by the same technique, in situ oxidation bonding technique with an addition of Y2O3. The addition of Y2O3 enhanced neck formation (bonding part between SiC particles), resulted in improved mechanical properties. They suggested reaction steps involved in the formation of porous mullite-bonded SiC ceramics:(4) SiC+2O2SiO2(amorphous)+CO2(4) (5) AmorphousSiO2Cristobalite(5) (6) 3Al2O3+2SiO23Al2O3.2SiO2(mullite)(6) The formation of mullite phase in between SiC grains can be explained on the basis of in situ reactions. SiC was oxidized to amorphous silica that further crystallized to form cristobalite during sintering at higher temperatures in air. The obtained cristobalite reacts with alumina upon higher temperatures (beyond 1400 °C) to form mullite [155,158,160].

Liu et al. [161] investigated the effect of preheat-treated aluminosilicate (PHAS) addition on the mullitization process and pore structure in the processing of porous mullite-bonded SiC by in situ bonding technique. The addition of 5 wt% PHAS into SiC–Al2O3–graphite batches promoted the mullitization process and the process was almost completed at 1450 °C and resulted in the enhancement of neck growth. The open porosity was reduced by the addition of PHAS, whereas the average pore size from the burnout of graphite was enlarged by the addition of PHAS. Kumar et al. [164,166] processed porous mullite-bonded SiC ceramics with four different Al sources (Al/AlN/Al2O3/Al(OH)3) at 1450–1550 °C for 1–6 h duration in air. They suggested Al2O3 formation reactions from various Al sources as follows:(7) 2Al+1.5O2Al2O3(7) (8) 2AlN+1.5O2Al2O3+N2(8) (9) 2Al(OH)3Al2O3+3H2O(9) The oxidation derived cristobalite reacts with Al2O3 or Al source-derived Al2O3 upon increasing the temperature (beyond 1400 °C) to form mullite according to Eq. (6) [158]. The mullite-silica grains were well connected and strongly adhered with large SiC grains in porous mullite-bonded SiC ceramics by using Al2O3, whereas poor adhesion and weak bonding was found from usage of AlN. The minimum porosity of 17% and maximum porosity of 42% were obtained for the samples prepared with Al2O3 and AlN, respectively, when sintered at 1550 °C for 6 h and 1450 °C for 1 h, respectively [164].

Choi et al. [163,165] fabricated porous mullite-bonded SiC ceramics at temperatures ranging from 1350 to 1450 °C for 2 h using SiC, Al2O3, alkaline-earth metal oxides, and polymer microbeads. The addition of alkaline-earth metal oxides was beneficial for lowering the mullitization temperature from 1450–1550 °C to 1350–1450 °C and for the formation of dense strut, which should lead to the improved mechanical strength. Dey et al. [221] processed porous mullite-bonded SiC ceramics by infiltrating a SiC–Al2O3 powder compact with a liquid precursor of SiO2 and subsequent heat treatment at 1500 °C. The bond phase was composed of needle-shaped mullite which was grown from a siliceous melt formed during the heat-treatment. The obtained porosity was 30% and the pore size was ranged from 2 to 15 μm with an average pore size of 5 μm. Kayal et al. [167,168] fabricated porous mullite-bonded SiC ceramics by infiltrating SiC-petroleum coke powder compacts with a liquid precursor of mullite and subsequent sintering at 1300–1500 °C for 4 h in air. The porous mullite bonded SiC ceramic was composed of SiC, mullite, and cristobalite. The porosity could be varied in the range of 31–49%, depending on the amounts of infiltrate and the petroleum coke powder, and the average pore diameter (∼8 μm) was almost independent of porosity.

Processing of porous mullite-bonded SiC is one of the low-temperature processing technique for porous SiC ceramics and the processing temperature was in the range of 1300–1550 °C in air. A typical microstructure of the porous mullite-bonded SiC is shown in Fig. 7(a) [159]. The obtained porosity was in the range of 17–55%, depending on the template content, composition of Al source, and sintering temperature.

Fig. 7 Typical microstructures of macroporous SiC ceramics produced via the bonding technique: (a) mullite-bonded SiC foam [159], (b) silica-bonded SiC foam [223], (c) self-bonded SiC foam, and (d) SiOC-bonded SiC foam [190]. (a) and (b) are reproduced with permission of Elsevier. (d) is reproduced with permission from the Springer.

2.5.2 Porous silica-bonded silicon carbide ceramics

She et al. [169,222] firstly developed a simple oxidation-bonding technique to fabricate porous SiO2-bonded SiC ceramics. The strategy of the method was to heat the SiC powder compacts in air so that SiC particles are bonded to each other by oxidation-derived amorphous SiO2 glass and/or cristobalite. A typical microstructure of the porous silica-bonded SiC ceramics is shown in Fig. 7(b) [223]. The obtained porosity was in the range of 28–40%, depending on the particle size of SiC powder and the sintering temperature. The porosity decreased with increasing the temperature in the range of 1100–1400 °C and it decreased with increasing the particle size of SiC powder. The same research group [223] could adjust the porosity and the pore size of porous SiO2-bonded SiC ceramics by controlling the graphite content and by controlling the size of graphite particles and/or SiC powders. The average pore diameter obtained was ranged from 3.4 to 7.6 μm, depending on the graphite particle size and the porosity obtained ranged from 32% to 50%. Chun and Kim [170] processed porous SiO2-bonded SiC ceramics with spherical pores by sintering SiC-polymer microbead compacts at 1300–1400 °C in air. By controlling the microbead content and the sintering temperature, it was possible to adjust the porosity in the range of 19–77%. Dey and coworkers [171] processed porous silica-bonded SiC ceramics by an infiltration technique. SiC powder compacts were infiltrated with liquid precursors which produced SiO2 during pyrolysis at 1300 °C in air. The infiltration of the liquid precursor into SiC powder compacts occurred in two steps: (i) an initial rapid infiltration of the precursor governed by capillary pressure and (ii) a slow impregnation via diffusion. The infiltrated silica acts as a bond between SiC particles. The extent of infiltrated SiO2 was found to be dependent on the number of infiltration passes. The obtained porosity was in the range of 26–36%.

2.5.3 Porous self-bonded silicon carbide

The microstructure of porous self-bonded SiC (SBSC) ceramics consists of SiC crystallites bonded with synthesized SiC [173]. A typical microstructure of the porous self-bonded SiC ceramics is shown in Fig. 7(c). The SBSC has a great potential for usage in gas filter applications because of its excellent refractoriness, good heat resistance, and cost effectiveness. SBSC is fabricated from SiC and SiC precursor (PCS) by pyrolysis [172] or from refractory-grade SiC, Si, and carbon by a reaction sintering process [173[174]177]. Zhu et al. [172] fabricated SBSC by using PCS and SiC powders. During heat treatment PCS experiences an organic to inorganic transformation forming SiC and the formed SiC acts as a bonding phase between SiC particles at a temperature as low as 1100 °C. Higher content of PCS gives lower porosity with higher frexural strength. Kennedy et al. [173] prepared porous SBSC from SiC, Si, and C powders and investigated the role of Al and B additives on porosity of porous SBSC. They fabricated four different samples of porous SBSC with different additive compositions to investigate the properties: no additive, 2 wt% B, 2 wt% Al, and 1 wt% Al + 1 wt% B. Generally, it was found that the additive increased the degree of necking while at the same time reducing the porosity by a small amount (2–3%). The same group investigated the effect of SiC particle size on porosity of porous SBSC ceramics. The incorporation of 0.7 μm SiC particles into the ceramic material containing 25 μm SiC particles reduced the porosity from 52% to 46% [177]. Lim et al. [174,175] investigated the effect of Si:C ratio on porosity of porous SBSC ceramics. The porosity of porous SBSC ceramics could be controlled in the range of 36% to 43% by adjusting the Si:C ratio and sintering temperature between 1750 °C and 1850 °C. A maximal porosity of 43% was obtained when the Si:C ratio was 2:1 regardless of the sintering temperature. Kumar et al. [176] investigated the influence of submicron SiC particle addition (0–80 wt%) on porosity of porous SBSC ceramics. The result illustrates that 40 wt% addition of submicron SiC particles increases the packing efficiency and decreased porosity. The obtained porosity was in the range of 40–46%.

2.5.4 Porous silicon nitride-bonded silicon carbide

Porous Si3N4-bonded SiC ceramics are produced by nitridation of the foamed compacts containing SiC and Si powders at 1250–1450 °C in a nitrogen atmosphere [178[179]181]. Nitriding Si to form Si3N4 as a bonding phase at relatively low temperatures has been much interest due to its low production cost [178,180]. However, slow nitridation process, requiring 10 h to days is one the most critical issues in the mass production of dense compacts. In contrast, porous Si3N4-bonded SiC ceramics can be processed within 6 h when some additives are added. Zhang [179] investigated the effect of Al2O3–Y2O3 additives on the microstructure of porous Si3N4-bonded SiC ceramics. The microstructure of ceramic foams containing no additives contained α-Si3N4 whiskers as the main nitride phase and led to a loose microstructure. In contrast, the microstructure of ceramic foams containing Al2O3–Y2O3 additives contained a large amount of β-Si3N4 as well as α-Si3N4 and Si2N2O phases which were bonded by a glassy phase produced between the surface silica on the SiC particles and additives. Choi et al. [180] investigated the effect of starting SiC particle size on nitridation rate and the results showed that the specimen prepared from smaller SiC particles showed higher nitridation rate after nitridation at 1450 °C and resulted in smaller pore size. The obtained porosity was in the range of 32–35%, depending on the size of starting SiC particles and nitridation time. Gain et al. [181] processed porous Si3N4-bonded SiC ceramics from SiC, Si, Al2O3–Y2O3 additives, and ethylene vinyl as a pore former by nitridation of the extruded green body at 1400 °C in a flowing N2 and 10% H2 gas mixture. The porous ceramics contained SiC, α-Si3N4, β-Si3N4, and few Fe phases, and the pore size of the porous ceramics was 260 μm after second extrusion passes and 35 μm after third extrusion passes.

2.5.5 Porous alkali-bonded silicon carbide

Porous alkali-bonded SiC ceramics were fabricated using a geopolymer as a bonding phase [182]. The geopolymer was prepared from metakaolin, as an aluminosilicate raw powder, and KOH/K2SiO3 aqueous solution. The bonding phase is formed from metakaolin in the presence of alkali solution. Metakaolin in alkaline conditions dissolved and reprecipitated to form geopolymeric nano-particles that act as a bonding phase to bind SiC particles together. The obtained porosity was in the range of 78–87%.

2.5.6 Porous cordierite-bonded SiC ceramics

It is known that cordierite (2MgO·2Al2O3·5SiO2) has a low coefficient of thermal expansion [183,184,224] and it can be synthesized at low temperatures [183,225,226]. Thus, cordierite is chosen as a bonding phase to fabricate porous SiC ceramics. Liu and coworkers [204,206] prepared cordierite-bonded porous SiC ceramics from α-SiC, α-Al2O3 and MgO using graphite as a pore former via in situ reaction bonding technique in air. Graphite was burned out to produce pores and the surface of SiC was oxidized to SiO2 at high temperatures. With further increasing the temperature, SiO2 reacted with α-Al2O3 and MgO to form cordierite. SiC particles were bonded by the synthesized cordierite and oxidation-derived SiO2. The sintering of porous SiC ceramics is realized by a series of reactions as follows [183]:(10) SiC+2O2SiO2+CO2(10) (11) MgO+Al2O3MgO.Al2O3(spinel)(11) (12) 2MgO+2Al2O3+5SiO22MgO.2Al2O3.5SiO2(cordierite)(12) (13) 2(MgOAl2O3)+5SiO22MgO.2Al2O3.5SiO2(13)

The open porosity decreases with sintering temperature and the amount of Al2O3–MgO additions, but it increases with graphite particle size and content [183]. The same group [184] studied the effect of CeO2 on the processing of cordierite-bonded porous SiC ceramics. It was found that the addition of CeO2 strongly promotes the phase transformation toward cordierite and inhibits the formation of spinel. By adding 2 wt% CeO2, a large amount of cordierite was synthesized and a trace of spinel was found at 1250 °C. The neck growth which is very important in the porous ceramics was enhanced by CeO2 addition. Zhu et al. [185] processed cordierite-bonded porous SiC ceramics in air from SiC, clay, talc, and Al2O3 using graphite as a pore former via in situ reaction bonding technique. Graphite was burned out to produce pores and the surface of SiC was oxidized to SiO2 at high temperatures. With further increasing the temperature, SiO2 reacted with clay, talc, and Al2O3 to synthesize cordierite. SiC particles were bonded by the in situ synthesized cordierite. The obtained porosity ranged from 28% to 60%.

2.5.7 Porous silicon-bonded silicon carbide

Porous Si-bonded SiC ceramics are fabricated by sintering powder compacts containing SiC, Si, B, and C at temperatures ranging from 1600 °C to 1800 °C [186,187]. The main bonding material is Si in the porous ceramics because the amount of carbon added is very small amount (0.2 wt%) and the added carbon reduces thin SiO2 layers on the surface of SiC particles, enhancing the bonding of SiC by Si. The pore size of the porous ceramics increased with increasing the size of Si powders because molten Si is infiltrated into SiC interparticle pores by capillary force and leaving pores in the ceramics. The obtained porosity of the porous Si-bonded SiC ceramics was in the range of 36–55% depending on the sintering temperature and the starting particle size of Si.

2.5.8 Porous silicon oxycarbide-bonded silicon carbide

Polysiloxane-derived SiOC ceramics have many advantages as a bonding phase for SiC: low processing temperature [227[228]230], excellent mechanical strength [231[232]233], excellent thermal shock resistance [234], good thermomechanical stability [235,236], and excellent creep resistance [237], and high ceramic yield among polymer-derived ceramics [238]. Porous SiOC-bonded SiC ceramics are produced from SiC-polysiloxane mixtures at temperatures as low as 700–1000 °C [188[189]191]. A typical microstructure of the porous SiOC-bonded SiC ceramics is shown in Fig. 7(d) [190].

Ma and coworkers [188] introduced polysiloxane as a binder to fabricate porous SiOC-bonded SiC ceramics. During the heat treatment polysiloxane experiences the organic-inorganic transformation by forming SiOC and this acts as a bonding material between SiC particles. The bonding temperature was about 1000 °C. Porosity decreased with an increase of polysiloxane content and increased with an increase of the particle size of SiC. The obtained porosity was in the range of 41–50% depending on the polysiloxane content and the particle size of SiC. Eom et al. [189] and Lim et al. [190] fabricated porous SiOC-bonded SiC ceramics from SiC, polysiloxane, and optional polymer microbead mixtures at temperatures as low as 700–900 °C by a simple pressing and heat-treatment process. During heat treatment the polysiloxane transformed into an amorphous SiOC phase, which acted as a bonding material between SiC particles. The obtained porosity was in the range of 18–56%, depending on the polysiloxane content, sintering temperature, and polymer microbead content. Thunemann and his colleagues [191] processed SiOC-bonded SiC from polymer (polysiloxane and phenol resin)-coated SiC by warm pressing and pyrolysis at 1000 °C. The obtained porosity was in the range of 34–53% depending on the type of resins and the particle size of SiC. Eom et al. [192] processed SiOC-bonded SiC ceramics from SiC-polysiloxane-alkaline earth (AE) alkoxide mixtures by pressing and pyrolysis at 800 °C. The addition of alkaline earth alkoxide made a stronger bonding between SiC and polysiloxane-derived SiOC by forming Si–O–AE bonds. The obtained porosity was in the range of 15–32% depending on the AE content.

2.5.9 Porous frit-bonded silicon carbide

Porous frit-bonded SiC is fabricated from SiC, frit, and polymer or glass microbeads by pressing and heat-treatment at 800 °C in air [193]. During the heat treatment frit transforms to a viscous phase and bond SiC particles together. The obtained porosity was in the range of 46–55% depending on the particle size of SiC and polymer or glass microbead content.

2.5.10 Summary of bonding technique

Bonding techniques generally offer a cheap, low-temperature processing route to prepare macroporous SiC ceramics with porosity ranging from 15% to 60%. The processing temperature was in a range of 800–1550 °C, depending on the composition of the bonding material. Mullite (3Al2O3·2SiO2), silica (SiO2), silicon carbide (SiC), silicon nitride (Si3N4), alkali, cordierite (2MgO·2Al2O3·5SiO2), silicon (Si), silicon oxycarbide (SiOC), and frit phases have been investigated as bonding materials for porous SiC ceramics. Porous SiC ceramics containing a bonding phase and moderate porosity possess a unique set of characteristics, such as high thermal shock resistance, chemical stability, high specific strength, and cost-effectiveness. One exception to the above processing conditions is the porous alkali-bonded SiC ceramics, which use a geopolymer as a bonding phase [182]. Processing of porous alkali-bonded SiC ceramics can be done at room temperature and the obtained porosity was in a range of 78–87%.

3 Mechanical properties

3.1 Room temperature flexural and compressive strengths

Mechanical properties of porous SiC ceramics depend on their porosity, pore size, microstructure of the strut, and compositions of bonding phase and additives [28,46,208]. Each processing method to produce porous SiC is best suited for producing a specific range of porosity, pore size, and microstructure of the strut [28,170,239]. The effects of porosity, pore size, microstructure of the strut, and compositions of bonding phase and additives on flexural and compressive strengths are discussed in this session.

The most influential parameter on the flexural strength of porous SiC ceramics is porosity. The collection of flexural strength data for various porous SiC ceramics produced via different processing strategies is shown as a function of porosity in Fig. 8. The porosity varied from 9% to 91% and the flexural strength varied from 0.7 to 205 MPa. From the plot, the following observations were made: (1) the flexural strength generally decreases with increasing porosity; (2) at a porosity range of 30–50%, the template technique yields porous SiC ceramics with better strength than the bonding technique; and (3) at a porosity range of 50–80%, the replica technique (mostly from wood templates) provides porous SiC ceramics with higher strength than both the partial sintering and the template techniques.

Fig. 8 Flexural strength as a function of porosity of macroporous SiC ceramics produced via different processing strategies. Data points are labeled with the corresponding reference numbers.

In porous SiC ceramics fabricated by partial sintering technique, a maximum flexural strength of 152 MPa at 65% porosity [58] and a minimum flexural strength of 5.2 MPa at 67% porosity [55] were obtained depending on the various processing parameters. Based on various processing parameters in replica technique, a minimum flexural strength of 0.7 MPa at 86% porosity [70] and a maximum flexural strength of 205 MPa at 9% porosity [113] were reported. In porous SiC ceramics processed by the sacrificial template technique, a maximum flexural strength of 170 MPa at 50% porosity [141] and a minimum flexural strength of 2.4 MPa at 77% porosity [45] were obtained. The flexural strength data of porous SiC ceramics processed by the direct foaming were quite limited and a maximum and a minimum strengths were 6.2 MPa at 86% porosity and 2.9 MPa at 88% porosity, respectively [42]. In porous SiC ceramics fabricated by bonding technique, a maximum flexural strength of 185 MPa at 31% porosity [169] and a minimum flexural strength of 3.6 MPa at 82% porosity [55] were obtained depending on both the bonding method and processing parameters.

According to the model proposed by Rice [240], the strength of a porous material is related to its porosity through the expression.(14) σ=σoexp(bP)(14) where σ and σo are strengths of a porous material with porosity P and nonporous material, respectively, and b is a constant that is dependent on pore characteristics. The model does not expect any dependence of strength on pore size, but a variation only with porosity of porous ceramics. However, the pore size affects the flexural strength of porous SiC ceramics. The effect of pore size on flexural strength of porous SiC ceramics has been investigated systematically by Eom and Kim [46]. They fabricated porous SiC ceramics with different pore sizes by using three different sizes of templates. The obtained porosity of the porous SiC ceramics almost did not change with the size of template at the same content of template. Thus, the porous ceramics have almost same porosity at the same content of template, but different pore sizes. Typical flexural strengths of the porous SiC ceramics with 45% porosity were 55 MPa for the porous SiC with a pore size of 7 μm, 47 MPa for the porous SiC with a pore size of 14 μm, and 20 MPa for the porous SiC with a pore size of 31 μm. Thus, the flexural strength of porous SiC ceramics increased with decreasing the pore size at the same porosity. The result proved that the flexural strength of porous SiC ceramics increases with decreasing the pore size, because a decrease in pore size by using a smaller template decreased the critical flaw size of the porous SiC ceramics. Spherical templates with a small diameter would be beneficial for preparing high-strength, porous SiC ceramics.

Effect of microstructure on the flexural strength of porous SiC ceramics has been investigated by Eom et al. [47,118,208] and Kennedy et al. [177]. Eom et al. [47,118] fabricated porous SiC ceramics with various microstructures by adjusting the initial α-SiC content in the starting composition by the template method. When β-SiC powder or a mixture of α/β powders containing a small amount (≤10%) of α-SiC powder was used, the microstructure consisted of large platelet grains (Fig. 5(a)). In contrast, when using α-SiC powder or α/β powders containing a large amount (>10%) of α powders, the microstructure consisted of small equiaxed grains. The microstructural development was insensitive to the additive composition (Al2O3–Y2O3 or Al2O3–Y2O3–CaO) and the additive content (5% or 7%) [47,118]. A maximum strength of 75 MPa was obtained in the porous SiC with a microstructure consisting of equiaxed grains, whereas a minimum strength of 30 MPa was obtained in the porous SiC with a microstructure consisting of large platelet grains [118]. Kennedy et al. [177] fabricated porous self-bonded SiC ceramics with different grain sizes by adjusting the initial SiC particle size. They used three different sizes of micron-size SiC powders (25 μm, 50 μm, 65 μm) and a submicron-size SiC powder (0.7 μm) as a bonding phase. The porous SiC ceramics fabricated from a 25 μm-size powder showed a maximum flexural strength of 35.5 MPa at 46% porosity, indicating that the porous SiC ceramics with smaller grain size is beneficial in improving the flexural strength of porous self-bonded SiC ceramics at the equivalent porosity.

Eom et al. [129,130] investigated the effect of additive composition on flexural strength of porous SiC ceramics, which were processed by the template method. Variation of additives led to different porosities in the range of 56–72% and different flexural strengths in the range of 8 MPa to 122 MPa. However, some specimens showed different flexural strengths at the same porosity. For example, the flexural strength of porous SiC ceramics sintered with 3 wt% Al2O3–2 wt% Y2O3 was 55 MPa at 62% porosity, whereas that of porous SiC ceramics sintered with 3 wt% Al2O3–1 wt% Y2O3–1 wt% CaO was 45 MPa at the same porosity [129]. Choi et al. [163] fabricated porous mullite-bonded SiC ceramics with 4 wt% alkaline earth oxide additives. The addition of alkaline earth oxides was beneficial for lowering the sintering temperature from 1450–1550 °C to 1350–1450 °C and for improving the flexural strength dramatically. The mullite-bonded SiC ceramics sintered with 4 wt% SrO showed a flexural strength of 44 MPa at 46% porosity. In contrast, the flexural strength of the mullite-bonded SiC ceramics sintered with no additives was 6 MPa at 49% porosity. The results suggest that judicious selection of sintering additive composition is an efficient way to improve the mechanical properties of porous SiC ceramics.

Since the bonding technique has a wide variation in flexural strength at the equivalent porosity (Fig. 8), the flexural strength data belong to each bonding material was plotted as a function of porosity in Fig. 9. From the plot, we can find the following observations: (1) at a porosity range of 10–30%, porous SiOC-bonded SiC ceramics showed greater flexural strength than the mullite-bonded, silica-bonded, and cordierite-bonded SiC ceramics; (2) at a porosity range of 30–40%, porous silica-bonded SiC ceramics showed better flexural strength than the other materials; and (3) at a porosity range of 40–50%, porous mullite-bonded SiC ceramics showed better flexural strength than the other materials.

Fig. 9 Flexural strength as a function of porosity of macroporous SiC ceramics produced with different phases. Data points are labeled with the corresponding reference numbers.

The collection of compressive strength data for various porous SiC ceramics produced via different processing strategies is shown as a function of porosity in Fig. 10. The porosity varied from 30% to 90% and the compressive strength varied from 0.8 to 600 MPa. From the compressive strength versus porosity plot, we made the following observations: (1) the compressive strength generally decreases with increasing porosity; (2) at a porosity range of 30–40%, the partial sintering and the sacrificial template methods yield porous SiC ceramics with better strength than the other processing technique; and (3) at a porosity range of 40–55%, the sacrificial template method provides porous SiC ceramics with higher strength than the other methods. In porous SiC ceramics fabricated by partial sintering technique, a maximum compressive strength of 513 MPa with 39% porosity [63] and a minimum compressive strength of 61 MPa with 54% porosity [54] were obtained depending on the processing parameters. Based on various processing parameters in replica technique, a minimum compressive strength of 0.3 MPa with 90% porosity [73] and a maximum compressive strength of 70 MPa with 55% porosity [83] were reported. In porous SiC ceramics processed by sacrificial template technique, a maximum compressive strength of 600 MPa with 30% porosity [46] and a minimum compressive strength of 4.8 MPa with 78% porosity [139]. The compressive strength data of porous SiC ceramics processed by direct foaming were quite limited and a maximum and a minimum strengths were 77 MPa at 59% porosity and 51 MPa at 62% porosity, respectively [154]. In porous SiC ceramics fabricated by the bonding technique, a compressive strength of 200 MPa at 40% porosity in silica-bonded SiC [170] and a compressive strength of 0.9 MPa at 81% porosity [182] in alkali-bonded SiC were reported.

Fig. 10 Compressive strength as a function of porosity of macroporous SiC ceramics produced via different processing strategies. Data points are labeled with the corresponding reference numbers.

From Figs. 810, it is evident that the flexural and compressive strength generally decreases with increasing porosity in porous SiC ceramics. This tendency has also been observed in many other porous ceramics [241[242]244] and can be attributed to the pore coalescence under load at higher porosities. The pore coalescence increases the defect size and reduces the strength [34]. From the model proposed by Rice (Eq. (14)) [240], the value b was reported to be 6 for cubic stacking and 9 for rhombic stacking [245]. The strength data of porous SiC ceramics processed by various methods showed different b values. For example, the reported b values were 3.4 in porous SiC ceramics fabricated by the partial sintering [44], 3.19–3.24 in porous SiC ceramics fabricated by the template method [141,142], 4.36 in porous mullite-bonded SiC [156], 6.54–7.95 in porous silica-bonded SiC ceramics [169,170], 4.8 in porous cordierite-bonded SiC [140], and 6–16 in porous SiOC-bonded SiC [190]. The observed deviation in the b values suggests a more pronounced influence of density on the strength than that predicted by the model [34]. This can probably attributed to the following factors: (1) the model assumed a constant cell size, whereas the distribution of cell sizes are often found in porous SiC ceramics, especially porous ceramics processed by the bonding technique [156,170,185,190]; (2) the presence of both open and closed pores, which should have some effect on the stress distribution near pores [34]; (3) the variation of solid area for each specimen irrespective of the material porosity [190]; and (4) the presence of abnormally large pores or defects in struts, which lead to the unexpectedly low flexural strength [34].

In summary, from a collection of flexural and compressive strength data for various porous SiC ceramics produced via different processing strategies, the following observations were made: (1) both the flexural and compressive strengths generally decrease with increasing porosity; (2) at a specific porosity range, the strength of porous SiC ceramics are strongly dependent on the processing method; (3) an excellent flexural strength of 152 MPa at 65% porosity was obtained in porous SiC ceramics fabricated by the partial sintering technique; and (4) compressive strengths of 513 MPa at 39% porosity and 77 MPa at 59% porosity were reported in porous SiC ceramics processed by partial sintering and by direct foaming, respectively.

3.2 High temperature flexural strength

The collection of flexural strength data at high temperatures for various porous SiC ceramics is shown in Fig. 11. Singh and Salem [105] measured flexural strength of porous biomorphic SiC ceramics fabricated by the replica method at temperatures from RT to 1350 °C. Flexural strengths of SiC ceramics fabricated from maple wood precursors were 344 MPa and 230 MPa at RT and 1350 °C, respectively. In contrast, those of SiC ceramics fabricated from mahogany wood precursors were 144 MPa and 112 MPa at RT and 1350 °C, respectively. The RT-strength retention of maple-based and mahogany-based SiC ceramics was 67% and 78% at 1350 °C, respectively. The flexural strength of porous SiC ceramics, which were fabricated by CVD of SiC onto reticulated carbon skeletons obtained by pyrolysis of polyurethane foams, was 19 MPa at 200 °C and the material maintained its RT-strength up to 1400 °C [81]. The excellent strength retention of the porous CVD-SiC was attributed to its high purity, probably >99.9% pure. The flexural strength values of porous mullite-bonded SiC ceramics with 30% porosity were 47 MPa at RT, 49 MPa at 900 °C, and 58 MPa at 1100 °C [221]. The increase of flexural strength at 1100 °C was due to the crack healing of porous SiC ceramics by oxidation of SiC during flexural strength testing.

Fig. 11 High temperature flexural strength of macroporous SiC ceramics produced via different processing strategies. Data points are labeled with the corresponding reference numbers.

In summary, wood-derived porous SiC ceramics processed by the replica method maintained 67–78% of their room temperature strengths at 1350 °C, whereas porous SiC ceramics fabricated by CVD of SiC on reticulated carbon foams obtained by pyrolysis of polyurethane foams (replica method) maintained their RT-strength up to 1400 °C. The excellent strength retention of the porous CVD-SiC was attributed to its high purity (99.9% pure).

3.3 Fracture toughness

The collection of fracture toughness data for various porous SiC ceramics produced via different processing strategies is shown as a function of porosity in Fig. 12. The porosity varied from 8 to 95% and the fracture toughness varied from 0.2 to 4.3 MPa m1/2. From the fracture toughness versus porosity data for porous SiC ceramics produced via different processing strategies, the following observations were made: (1) the fracture toughness generally decreases with increasing porosity; and (2) at a porosity range of 40–70%, the replica and partial sintering techniques yield porous SiC ceramics with higher toughness than the template method.

Fig. 12 Fracture toughness as a function of porosity of macroporous SiC ceramics produced via different processing strategies. Data points are labeled with the corresponding reference numbers. The fracture toughness values obtained in Refs [37,47,81], Ref [58], and Ref. [64] were measured by a single-edge notched beam, a chevron-notched beam, and an indentation-strength method, respectively.

The obtained fracture toughnesses of porous SiC ceramics processed by partial sintering and by replica methods were 0.9 MPa m1/2 at 64% porosity and 1.4 MPa m1/2 at 50% porosity, respectively [58,64]. In porous SiC ceramics fabricated by the replica method, the fracture toughness ranged from 0.2 MPa m1/2 at 95% porosity [81] to 1.4 MPa m1/2 at 50% porosity [38]. The fracture toughness data of porous SiC ceramics fabricated by template method were quite limited and the toughness values were 0.3–0.4 MPa m1/2 at 57–58% porosity [47]. Comparison of the fracture toughness values obtained in template method with values obtained in the other methods indicates that the toughness values obtained in template method are lower than those of the other methods. A crack-tip blunting mechanism contributes to the toughening of porous ceramics [58]. However, the microstructure of the porous SiC ceramics fabricated by template method by Eom et al. [47] consisted of large platelet grains, as shown in Fig. 5(a). The growth of platelet SiC grains in the porous SiC ceramics formed sharp edges and V-shaped notches at the contacting region of two platelet grains in the pores. The formation of sharp edges and V-shaped notches in the pore surfaces hindered the contribution of the crack blunting mechanism in the porous ceramics, resulting in lower fracture toughness [47]. The above results suggest that the fracture toughness of porous SiC ceramics can be improved by taking advantage of crack blunting mechanism, which can be accomplished by controlling pore morphology and grain arrangement [58].

Generally, the fracture toughness values are dependent on the measurement methods. It should be noted that the fracture toughness values plotted in Fig. 12 were measured in different methods: the data from Refs [38,47,81], Ref. [58], and Ref. [64] were measured by a single-edge notched beam, a chevron-notched beam, and an indentation-strength method, respectively. Thus, it cannot be ruled out that the difference in the toughness values was partially originated from the difference in the measuring method.

4 Thermal conductivity

One of the potential applications of porous SiC ceramics is a receiver material in solar power plants. The receiver material must (1) efficiently absorb the sunlight collected by the whole mirror field, (2) keep low losses, and (3) efficiently transfer the thermal energy to the exchange media [246]. The enhanced absorbance of SiC due to its naturally black color coupled with its high thermal conductivity enables the collection of solar heat and the effective heating of gases inside the porous SiC ceramics [20]. Thus, the effect of porosity on the thermal conductivity of porous SiC ceramics is an interesting issue for the receiver applications. Fig. 13 shows thermal conductivity of porous SiC ceramics processed by various processing methods as a function of porosity. The thermal conductivities of porous SiC ceramics varied from 2 to 82 W/(m·K) when the porosity varied from 30% to 74%. The thermal conductivity of dense SiC ceramics sintered with Y2O3–La2O3 was in a range of 169–206 W/(m·K) [247]. BeO-doped SiC showed a thermal conductivity as high as 250 W/(m·K) [248]. The thermal conductivities of B4C-doped SiC and Al2O3–Y2O3-doped SiC were reported to be 120 W/(m·K) [249] and 70–90 W/(m·K) [250]. Thus, it is clear that the introduction of porosity into SiC ceramics decreases the thermal conductivity of the ceramics. The effect of porosity on the thermal conductivity of ceramics can be expressed by the following equation [251]:(15) κc=κm1+Vd1Vd(15) where κc and κm are the corrected and measured thermal conductivities, respectively, and Vd is the volume fraction of void. The equation suggests that the thermal conductivity generally decreases with increasing porosity. The data shown in Fig. 13 generally follow the tendency, however, some data shows great deviation from the trend. The thermal conductivity of porous SiC ceramics processed by partial sintering ranged from 27 W/(m·K) at 66% porosity [55] to 82 W/(m·K) at 30% porosity [66]. In porous SiC ceramics fabricated by the replica method, it ranged from 11 W/(m·K) at 60% porosity to 41 W/(m·K) at 46% porosity [48]. In porous SiC ceramics processed by the sacrificial template method it ranged from 2 W/(m·K) at 74% porosity to 21 W/(m·K) at 43% porosity [45]. Porous SiC ceramics fabricated by the partial sintering showed higher thermal conductivity than the other materials processed by the sacrificial template and the replica techniques at the equivalent porosity; e.g., 57 W/(m·K) [66] and 42 W/(m·K) [55] of thermal conductivities at 40% and 68% porosity, respectively, for porous SiC ceramics fabricated by the partial sintering, 10 W/(m·K) at 40% porosity [142] for porous SiC ceramics fabricated by the sacrificial template, and 16 W/(m·K) at 68% porosity [48] for porous SiC ceramics fabricated by the replica method. The high thermal conductivity of the porous SiC ceramics fabricated by the partial sintering was not attributed to the difference in the processing method but attributed to the difference in purity. The porous SiC ceramics fabricated by the partial sintering was fabricated without sintering additives [66], but the other materials were processed with some sintering additives, e.g., Al2O3–Y2O3 [45]. The oxide additives have lower thermal conductivity than SiC ceramics. Wood-derived porous SiC ceramics [48] also showed higher thermal conductivity than the other materials at a range of 45–70% porosity. It was also attributed to a higher purity of the wood-derived porous SiC ceramics, compared to the other materials [45,142]. The wood-derived porous SiC ceramics does not contain any other additives except residual Si, whereas the porous SiC ceramics fabricated by the sacrificial templates contained oxide additives [45,142].

Fig. 13 Thermal conductivity as a function of porosity of macroporous SiC ceramics produced via different processing strategies. Data points are labeled with the corresponding reference numbers.

In summary, the thermal conductivity of porous SiC ceramics is strongly dependent on the porosity as well as the purity of strut materials. Porous SiC ceramics fabricated by partial sintering without sintering additives show higher thermal conductivity than other materials processed by sacrificial template and replica techniques at the equivalent porosity. Thermal conductivities of 57 W/(m·K) at 40% porosity [66] and 42 W/(m·K) at 68% porosity [55] were obtained in porous SiC ceramics fabricated by partial sintering.

5 Other properties and applications

Kitaoka et al. [212] investigated thermal cyclic fatigue behavior of commercial porous SiC filters for gas cleaning under simulated reverse cleaning conditions. The substrate of the SiC filters consisted of a multiphase microstructure of SiC grains (about 200 μm) bonded by a clay-based silicate binder and a filtration layer of mullite with a thickness of 100–300 μm. O-ring specimens were thermally shocked by cyclically blowing cold air outward through them while they were exposed to high-temperature flue gas. The calculated values of the tangential tensile stresses induced by the temperature differences between the inner and outer surfaces were found to be largest at the inner surfaces. Failure of porous SiC filters was initiated at the inner subsurface because of the effects of thermal shock. The thermal shock fatigue lifetime increased as thermal stresses decreased. The fatigue parameter for the porous SiC filters was 41.

Fukushima et al. [57] investigated high-temperature water vapor corrosion of porous SiC with and without alumina to examine the corrosion resistance of porous SiC membrane supports for hydrogen production by steam modification of methane. The corrosion test was performed under similar condition as hydrogen production reaction occurred at 600 °C and 1000 °C, 4 atm, and 3/1 = H2O/N2 where nitrogen gas was substituted for methane. In the corrosion test at 600 °C, porous SiC membrane supports without alumina showed better corrosion resistance, i.e., lower weight gain, than porous SiC membrane supports with alumina. In the corrosion test at 1000 °C, the almost complete conversion to silica and the densification due to the viscous flow sintering of silica occurred on both supports. These results suggest that porous SiC membrane supports should not be used at temperatures above or equal to 1000 °C for hydrogen production.

Zhao et al. [55] processed porous SiC through coat mix process with an Al2O3–SiO2–Y2O3 additive. A series of porous SiC ceramics were produced after molding, carbonization, and sintering. The composite additive improves the thermal shock resistance of porous SiC ceramics and makes little effect on thermal expansion coefficient.

Ding et al. [160] processed mullite-bonded porous SiC by an in situ reaction bonding process with α-SiC, Al2O3, and graphite powder at 1300–1500 °C. They also investigated the gas permeability behavior of mullite-bonded porous SiC ceramics. It was found that the sintering temperature and graphite (pore former) addition during the fabrication of the porous ceramics affect the permeability extremely by varying the texture of porous ceramics such as open porosity, pore size distribution, and tortuosity of pore channels. The increased sintering temperature results in a decreased Darcian (viscous) permeability but an increased non-Darcian (inertial) permeability. The addition of graphite improves the Darcian and non-Darcian permeability by enlarging the open porosity and pore size. The increase in amount of graphite powder increases the porosities of porous ceramics [185]. Eom et al. [47] investigated the effect of microstructure on gas permeability of porous SiC ceramics. The specific flow rate of the porous SiC ceramics with 56% porosity and a toughened microstructure consisted of large platelet α-SiC grains (23.3 L/min/cm2) was seven times higher than that of porous SiC ceramics with 58% porosity and an equiaxed microstructure (3.3 L/min/cm2), although the difference in their porosities was small (∼2%). This result suggests that the development of large platelet α-SiC grains plays an important role in improving the specific flow rate of macroporous SiC ceramics. This is also supported in microcellular SiC ceramics with a duplex microstructure [132]. In general, the permeability of macroporous SiC ceramics is dependent on both porosity and microstructural characteristics. However, the development of large platelet SiC grains is very effective in increasing the permeability of macroporous SiC ceramics at an equivalent porosity. Zhou et al. [61] fabricated porous SiC tubes by extrusion forming and partial sintering methods. The gas permeances of the tubes with an average pore size of 0.2 μm and 1.7 μm were at a level of 10−6 mol m−2 s−1 Pa−1 and 10−5 mol m−2 s−1 Pa−1, respectively. The tubes with an average pore size of 0.2 μm underwent limited oxidation and showed increased mechanical strength during the water vapor corrosion test at 800 °C for 100 h. These porous SiC tubes can be a candidate for tubular-type hydrogen separation membranes because of their high gas permeance, good water vapor corrosion resistance, and high strength (radial crushing strengths of 47–110 MPa) [61].

Porous SiC has been exploited in numerous applications as catalyst supports, receivers/collectors of concentrated solar radiation [20], flow channel inserts [144], alkali resistant parts [252], porous burners for heat radiation [21,24,25] and hot-gas or molten metal filters because of its low thermal-expansion coefficient and good thermal-shock resistance as well as excellent mechanical and chemical stability at elevated temperatures. Some of the major applications of porous silicon carbide have been discussed in this paper.

Porous SiC is one of the high temperature thermoelectric materials [49]. When the temperature difference is applied across the two ends of a solid sample, a thermo electromotive force is generated, which is known as the Seebeck effect. By utilizing this phenomenon, conversion of thermal energy to electric energy, namely thermoelectric power generation is possible. In principle, many years of efforts have been made to develop suitable materials for various applications, including space technology, local communications, small batteries, etc. [1,253]. Porous n-type SiC ceramics have found to show high thermoelectric conversion efficiency at 800–100 °C [253]. Electrical conductivity of porous n-type SiC was comparably higher than the reported values of single crystals, while thermal conductivity was kept as low as 1/10 to 1/30 of that for a dense SiC ceramic [254].

Porous SiC is also used for high-power, high-temperature, and high-frequency applications due to its properties like high breakdown electric field, high melting point, and high saturated electron drift velocity. Furthermore, it is a wide band gap semiconductor that has been studied for the fabrication of UV and blue light-emitting sources such as LED's and diode-lasers [255,256]. Porous SiC has superior properties than bulk SiC for semiconductor light sources. The use of porous SiC in the devices like LEDs and Lasers enable them to operate at UV wavelength. The enhanced properties of porous SiC are also been used for photodetectors [257]. Porous SiC was prepared from both n-type and p-type 6 H-SiC wafers with and without UV illumination [2,255]. Porous SiC can be fabricated in a manner which results in a significant portion of nanocrystallite within the material in the sub 10-nm regime. This results in band gap widening and much more efficient luminescence from the material [2,256]. The luminescence intensity is about 100 times stronger than that of crystalline 6H-SiC [2]. When it is passivated; porous SiC exhibits a much brighter blue luminescence than the bulk material, enabling more efficient blue light sources. Porous SiC has also been used as a sacrificial layer for the patterning of bulk SiC. It is an inert material and difficult to etch by conventional methods meanwhile porous SiC can be removed from its bulk substrate by oxidation and other methods. There are two step processes that can be used to pattern bulk SiC, whereby selected areas of the wafer are made porous, and then the porous layer is subsequently removed. The process to form porous SiC exhibits dopant selectivity (one conductivity type become porous while another is unaffected). Thus, using this two-step etching procedure, dopant selective etch-stops may be implemented for SiC multilayer's [256]. Porous SiC can be oxidized at a faster rate than bulk SiC and this property can be utilized to fabricate dielectrically isolated SiC layers and/or selectively introduced thick sections of SiO2 into SiC wafer. Porous SiC is buried under non-porous SiC layer and it can be oxidized completely to fabricate SiC-insulator. This aspect of porous SiC is very useful in the fabrication of high temperature/power/frequency electronic components [256].

Konstantinov et al. [3] investigated the properties of high resistivity porous SiC for SiC power device passivation. They found the presence of a leaky high-resistivity layer in porous SiC which is known to stabilize the breakdown. A similar technique of surface protection by semi-insulating polycrystalline silicon is widely used in Si power device technology [40]. The presence of a high-resistivity layer on the crystal surface of porous SiC prevents the effects of electric spark formation which appear at about 300–500 V. Henceforth, the porous SiC is a potentially useful material for 6H SiC device passivation [3].

A diesel particulate filter (DPF) is necessarily required to meet standards of high filtration efficiency, tolerance at high temperatures during regeneration, low pressure drop, good mechanical strength, and chemical resistance [19,23,258,259]. Porous SiC ceramic is an ideal material for DPFs due to its refractory nature and the ability to control their porous microstructure [23,258]. The filtration efficiency of these filters is strongly linked to the pore size, pore size distribution, porosity, and pore connectivity. SiC DPF with a porosity range of 40–50% can perform superior PM purification rate (>90%). High porosity guarantees high filtration efficiency and low pressure drop but deteriorates mechanical strength [23,258]. However, ceramic filters have been and will continue to be successfully implemented to improve the quality of the air we breathe.

Processing strategies for porous SiC ceramics with hierarchical porosity were suggested by various researchers [83,139,260,261]. The cellular SiC ceramics replicated from woods have a unique hierarchical pore structure because the microstructural features of wood range from millimeter (growth ring structures) via micrometer (tracheidal cell patterns, macro- and microfibril cell wall textures) down to nanometer scale (molecular fiber and membrane structures of cell walls) [83]. Fukushima et al. [260] proposed a novel process for the decoration of commercial SiC foams with Si2N2O ceramic nanowires for filters with high trapping efficiency and low pressure drop. Yoon et al. [139] fabricated highly aligned porous SiC ceramics decorated with SiC nanowires by the unidirectional freeze casting of SiC/camphene slurries with various PCS contents, where the PCS was used as a binder and source for the in situ growth of the SiC nanowires. Vanhaecke et al. [261] processed a hierarchical SiC support, constituted of a network of SiC nanofibers deposited on a SiC foam host. The SiC ceramics with hierarchical porosity could be useful for applications in acoustic and heat insulation structures, filter and catalyst carrier at high temperatures, as thermally and mechanically loaded light weight structures as well as for medical implant structures [83].

Porous SiC ceramics with highly aligned pore structures can be processed by sacrificial template method, especially gelation-freezing methods [137,138], and partial sintering technique [68]. The porous SiC ceramics with oriented porosity can be an ideal candidate for high temperature filters, composites, corrosion-resistant immobilization supports for bioactive substances [68].

6 Summary

In recent decades, tremendous efforts have been devoted to innovative processing of porous SiC ceramics and investigation of properties and their application in suitable fields. Because of the large number of articles in this field, this review mainly focuses on the processing and properties of macroporous SiC ceramics whose pore size is larger than 50 nm. Different processing routes for macroporous SiC ceramics have been developed for specific applications to satisfy the associated requirements for porosity, pore size, degree of interconnectivity, and properties. In this review, the processes are divided into five categories: (i) partial sintering, (ii) replica, (iii) sacrificial template, (iv) direct foaming, and (v) bonding techniques, as schematically illustrated in Fig. 1. These techniques differ greatly in terms of processing features and final properties achieved.

Partial sintering is the simplest and easiest way to fabricate porous SiC ceramics with porosity ranging below 65% and with pore size ranging from 0.1 to 10 μm. In this technique, full densification is retarded or prohibited by reducing the sintering potential. Reduced sintering potential is achieved by low sintering temperature, a constrained network of coarse powders, sintering without additives, and recrystallization. The replica method is the most appropriate technique to produce open-cell SiC ceramics with pore sizes ranging from 10 μm to 5 mm at porosity levels between 60% and 95%. The sacrificial template method is the most appropriate technique to tailor the porosity, pore size distribution, and pore morphology of the final porous SiC ceramics through appropriate choice of the sacrificial template, because pore size, pore shape, and porosity are controlled by the size, shape, and content of the template used. The pore size and porosity attained in this method ranged from 1 to 700 μm and from 15% to 95%, respectively, depending on the template content and processing conditions. The direct foaming technique is an easy and fast way to prepare both open and closed-cell structures with a wide range of pore size and porosity, up to 95% [32]. Bonding techniques generally offer a cheap, low-temperature processing route to prepare macroporous SiC ceramics with porosity ranging from 15% to 60%. The processing temperature was in a range of 800–1550 °C, depending on the composition of the bonding material. Mullite (3Al2O3·2SiO2), SiO2, SiC, Si3N4, alkali, cordierite (2MgO·2Al2O3·5SiO2), Si, silicon oxycarbide (SiOC), and frit phases have been investigated as bonding materials for porous SiC ceramics.

From a collection of mechanical and thermal properties for various porous SiC ceramics produced via different processing strategies, the following features were observed: (1) an excellent flexural strength of 152 MPa at 65% porosity was obtained in porous SiC ceramics fabricated by the partial sintering technique; (2) compressive strengths of 513 MPa at 39% porosity and 77 MPa at 59% porosity were reported in porous SiC ceramics processed by partial sintering and by direct foaming, respectively; (3) wood-derived porous SiC ceramics processed by the replica method maintained 67–78% of their room temperature strengths at 1350 °C, whereas porous SiC ceramics fabricated by CVD of SiC on reticulated carbon foams obtained by pyrolysis of polyurethane foams (replica method) maintained their RT-strength up to 1400 °C; (4) the obtained fracture toughnesses of porous SiC ceramics processed by partial sintering and by replica methods were 0.9 MPa m1/2 at 64% porosity and 1.4 MPa m1/2 at 50% porosity, respectively; and (5) thermal conductivities of 57 W/(m·K) at 40% porosity [66] and 42 W/(m·K) at 68% porosity [55] were obtained in porous SiC ceramics fabricated by partial sintering.

Considering the influence of the processing method on the microstructure, porosity, and properties of porous SiC ceramics, the selection of the processing route for the production of porous SiC ceramics depends primarily on the final properties required for specific application. Future work in this field should be directed toward (1) the development of more cost-effective processing, which can be accomplished by fewer heat-treatments (pyrolysis, calcination, sintering, etc.) of shorter time and lower temperature [35] and by using more cost-effective raw materials; (2) the development of porous SiC ceramics with improved performance required for specific applications, which can be fulfilled by control over the microstructure and composition (additives or bonding phase) of struts; (3) the investigation of suitable methods for specific target applications, focusing on deliberate tuning of processing parameters that control the properties of the final macroporous SiC ceramics [32]; and (4) the coupling of porosity with other functionalities (such as electrical conductivity [262,263], thermal conductivity [264], and/or ferromagnetic properties [265]), which will lead to more versatile applications and to components with an even wider set of properties, for use in advanced applications such as filters for rocket nozzles, heat exchangers for solar concentrated power applications, and pre-heaters for semiconductor processing gases [29].

Acknowledgement

This work was supported by the National Research Foundation of Korea (NRF) grant funded by the Korea government (MSIP) (2012R1A2A2A01004284).

Notes

Peer review under responsibility of The Ceramic Society of Japan and the Korean Ceramic Society.

References

 

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