Microwave Firing of Ceramics: Developing Homemade Susceptors and Their Practical Applications

Featured Application

Artisanal ceramics firing.

Abstract

This study explores the feasibility of constructing a microwave kiln for artisanal ceramics using accessible materials and homemade susceptors. Two modified microwave ovens (18 L and 50 L) were equipped with insulation and susceptors to achieve temperatures up to 1280 °C. Susceptors were fabricated from silicon carbide (SiC) and magnetite (Fe₃O₄) powders via microwave-assisted reactive sintering. Magnetite-poor susceptors (SiC/Fe₃O₄ > 2 by weight) demonstrated excellent durability, maintaining stable thermal performance over multiple cycles. In contrast, magnetite-rich susceptors (SiC/Fe₃O₄ ∼ 1) exhibited high initial efficiency and the ability to control redox conditions but degraded significantly after 10–15 cycles due to partial melting. The microwave kiln achieved significant time savings, completing the ramp-up of the firing cycles in 1 h, compared to 8–10 h in conventional kilns. Energy consumption per litre was comparable to large electric kilns but significantly lower than small ones. The fired ceramics, including porcelain and earthenware, showed excellent mechanical and aesthetic qualities, with glazes performing well even at lower temperatures than recommended. The study highlights the advantages of microwave heating, such as faster processing, energy efficiency, and the ability to control redox conditions, which mimic traditional gas-fired kilns. The developed susceptors are cost-effective and easy to manufacture, making this approach accessible to craftspeople and amateurs. While magnetite-rich susceptors enable redox control, their limited lifespan requires further optimisation. This work demonstrates the potential of microwave kilns for artisanal ceramics, offering flexibility, efficiency, and quality comparable to traditional methods, with promising applications for unique or small-scale production. Future research should focus on refining susceptors durability and validating redox control effects on ceramic glazes.

1. Introduction

1.1. The Place of Microwave Heating in Ceramic Firing Methods

Since their invention after World War II, microwave heating and cooking have become a universal tool, widely adopted in homes and catering. This led to the mass production of low-cost, easy-to-use domestic appliances [1]. Industrially, the technology is also extensively used for low- and medium-temperature applications like drying and sterilisation [2,3,4].

At higher temperatures, microwave energy has proven effective for tasks such as reducing iron ore [5,6,7]. For sintering ceramic materials and oxides, microwave heating offers clear advantages over traditional methods. It is a well-established fact that it improves diffusion kinetics and densification, allowing these processes to be completed at a much faster rate and at a lower temperature than conventional sintering [8,9,10]. This combination of faster heating and improved densification dramatically divides processing time by one or two orders of magnitude [10,11] and significantly reduces energy consumption [8,9].

Consequently, high-temperature microwave sintering has been developed for manufacturing high-quality technical ceramics [10,11,12] with significant benefit for advanced applications in the medical, space, and military sectors. In the consumer sector, however, high-temperature microwave applications are rare. They are almost exclusively limited to dental applications for producing small prostheses (zirconia) in very small kilns (1/4–1/2 L). For utilitarian or artisanal ceramics, which represent a large market, there is currently no available equipment that uses only microwave energy.

Despite this, a large number of laboratory studies over the last 30 years have demonstrated the clear benefits of microwave heating for both test specimens and standard-sized objects [13,14,15,16,17,18,19,20,21]. Nevertheless, the technologies used for firing utilitarian ceramics remain based on traditional kilns heated by an external source—often powered by fossil fuels. These energy-intensive and time-consuming techniques immobilise equipment and human resources.

This surprising conservatism in heating techniques for artisanal ceramics, especially when faced with the extraordinary potential of microwave technology in terms of energy, time, and quality gains, has been noted by many authors. One interpretation [22] is the difficulty of modelling wave-matter interactions, particularly for large objects. However, experimental and theoretical work from the last ten years has consistently shown that it is possible to successfully manufacture ceramic tableware using microwave heating [16,17,18,19,20,21,23].

1.2. Microwave Heating Principles and Current State of Knowledge

• General Principles

Microwave heating is fundamentally different from traditional heating processes. In conventional methods, an external source (like oil, gas, or electrical resistance) transfers energy to a material primarily through radiation and conduction. In contrast, microwave heating generates heat internally within the material itself. This occurs at an atomic level as microwaves interact with the material’s molecules.

When a material containing polar molecules is exposed to microwave energy, the electromagnetic radiation causes these molecules to rotate, which generates heat. This phenomenon is known as dielectric heating. A polar molecule, such as water, has a distinct positive and negative charge, giving it an electric dipole moment.

• High-Temperature Heating of Ceramics with Microwaves

The interaction of a material with electromagnetic radiation in the microwave range depends on its dielectric properties, specifically the complex dielectric permittivity. The heating of the material, often referred to as dielectric heating or dielectric loss heating, is directly related to the imaginary part of this permittivity, the dielectric loss factor (ϵ′′).

The loss factor ϵ′′ determines the material’s ability to absorb microwave energy and convert it into heat (its susceptibility or coupling). For significant internal heating to occur, the material must be polar (such as water or many oxides), exhibit structural defects, or be sufficiently conductive at the given frequency.

Materials are generally categorised by their behaviour: low-loss materials (or transparent): non-polar or non-conducting materials (like certain polymers or oxides at low temperatures) that allow microwaves to pass through with minimal absorption and heating. Absorbing materials (or susceptors): materials that strongly absorb microwaves and heat up rapidly (they have a high ϵ′′). Reflecting materials: materials (primarily metals and electrical conductors) that reflect the majority of the incident energy.

It is important to note that all materials exhibit some degree of reflection of microwaves at their surface or interface, and the degree of penetration is related to the penetration depth and the material’s impedance. An absorbing material used to initiate the heating process is called a susceptor.

Achieving high-temperature conditions for sintering materials using direct microwave heating presents several challenges. Conventional microwave applicators, often operating at low frequencies (typically 2.45 GHz), often struggle to efficiently couple with many ceramic materials at room temperature. This is because the dielectric loss (ϵ′′) of most ceramics is very low when cold; it only increases significantly above a certain critical temperature (often 400–600 °C). This makes the initial heating (start-up) very difficult.

Moreover, ceramics, with their non-homogeneous properties (such as dielectric permittivity and losses), complicate this interaction. For large ceramic pieces, uneven heating can lead to strong thermal gradients, causing cracking and failure. Additionally, rapid heating can induce thermal stresses, unwanted porosity, and the formation of localised hot spots, which may lead to a catastrophic thermal runaway [24,25].

To overcome these issues, hybrid-heating techniques have been developed. These methods combine direct microwave heating with a secondary heat source, often a susceptor material with high dielectric loss (ϵ′′ high) at low temperatures.

The susceptor absorbs microwave energy from the start and quickly reaches high temperatures, transferring heat to the ceramic sample through conventional mechanisms like radiation. Once the sample reaches its critical temperature, its own dielectric loss increases enough to allow it to begin absorbing microwaves efficiently and heating internally.

This hybrid approach offers a dual heating mechanism: the susceptor heats the material from the surface, while the microwaves heat it from the centre. This results in more uniform heating compared to direct microwave heating, where the centre typically becomes hotter than the surface (thermal runaway). The reduced heat loss from the surface, aided by the susceptor, further contributes to maintaining thermal homogeneity during the process [10,11,22,26]. In practice, this involves placing various forms of susceptors (tubes, plates, rods, etc.) near the piece to be heated [26,27].

• High-Temperature Microwave Kiln Design

Microwave heating cavities are metal enclosures designed to maximise energy transfer efficiency by containing and reflecting microwaves to create standing waves. These cavities can be multi-mode or single-mode, which influences the distribution of the electromagnetic field. Multi-mode cavities, such as those in a standard microwave oven, allow waves to propagate freely throughout a large volume, while single-mode cavities constrain the field, making them more efficient for small samples and precise control.

The electric field distribution within a multi-mode cavity is complex, depending on the material’s geometry, the microwave emission characteristics, and the material’s evolving dielectric properties [25]. Non-uniform field patterns and hot spots caused by a static applicator design can lead to uneven heating and thermal runaway. To improve heating uniformity and efficiency, multi-mode applicators often use mode stirrers—mobile metallic elements that modify the electromagnetic field—and rotating turntables to change the sample’s position within the cavity [28,29].

• Advantages of Microwave Heating

Despite the challenges, a major advantage of microwave heating is the spectacular time savings, which can be 5 to 10 times faster than conventional heating for achieving comparable or even superior product quality [10,14,18,26].

Since the late 1980s, when microwave ovens were first used for ceramics [9], extensive research has demonstrated the benefits of this heating method. The work of Tiago Santos and his colleagues at the University of Aveiro, Portugal, stands out as some of the most successful in manufacturing everyday ceramic objects with microwaves. Their latest article [23] provides a comprehensive review of this research, highlighting the following key benefits:

• Significant reduction in sintering time and energy consumption.
• Lower firing temperatures (50–75 °C lower than traditional methods) to achieve similar results.
• Faster and more uniform densification of materials.
• Comparable or superior mechanical properties of microwave-fired products compared to those fired conventionally.
• Challenges still exist in accurately measuring sintering temperatures, as thermocouples and pyrometers have limitations. However, analysing the final colour of the ceramics, glazes, and decals can serve as a useful tool for assessing and mapping the firing temperature of the finished pieces [23].

1.3. Aim of the Article

The performance of microwave heating, particularly its time-saving benefits for firing traditional ceramic pieces, makes it a compelling option for craftspeople or amateurs producing small quantities or unique pieces. The absence of commercial devices for this purpose makes it tempting to build such a system using readily available materials, especially given how common microwave appliances are.

The purpose of this article is to demonstrate that it is feasible to build and use a controllable and configurable microwave kiln—one with adjustable temperature, heating rates, and duration—for firing traditional artisanal or artistic ceramics. We will show that this can be performed using materials and equipment available from standard retailers. This article will also highlight the great flexibility of microwave heating for artisanal ceramic production, even in a less-than-perfectly configured kiln.

We will tackle the most difficult questions of the development of susceptors that can be made by the craftsperson using mineral powders in their own workshop. The thermal, physical, and mineralogical behaviours of these susceptors will be described in an initial analysis. We will also evaluate their potential impact on the kiln’s oxidation-reduction properties. To illustrate the process, some examples of firing earthenware, porcelain, and enamels will be presented. Finally, we will compare the advantages and disadvantages of this method to a conventional kiln.

2. Materials and Methods

2.1. The Microwave Kilns

Two commercial microwave ovens were modified to serve as ceramic kilns. The first was a small, 18 L, 2.45 GHz multi-mode microwave. It featured a single 800 W magnetron but had no mode stirrer, and its turntable was removed to accommodate insulation. To allow observations and pyrometer measurements, an 18 mm diameter shutter was installed through the door and oven insulation. Although small and prone to hot spots, this oven (Figure 1a) was invaluable for developing solutions for insulation, magnetron cooling, susceptor sintering, and firing procedures.

The second, larger kiln was built from an aged, 50 L, 2.45 GHz multi-mode microwave (from 1997). To increase power and improve field homogeneity, two additional microwave power units separated from their cavity were attached: one on top (from a 1993, 700 W unit with a pyramidal horn) and a third on the left side (from a 2005, 700 W unit). This created a powerful, triple-magnetron setup (Figure 1c). The maximum electrical power is 3.8 kWh, corresponding to approximately 2200 W of microwave emission power. The electrical consumption of microwaves was measured by consumer wattmeters installed on each of the microwaves. The insulation of this large oven was designed to use refractory materials that combine high microwave transparency with low density, such as alumina-based insulating materials, such as the porous alumina blanket, fibre wool, and insulating fibreboard [26]. Following these recommendations, the insulation was installed using a combination of low-density bio-soluble fibre insulation (1400 °C) for the outer layer and JM23 refractory bricks (1300 °C), sliced into 1 cm thick plates for the inner part. A 1 cm thick slice of a JM26 brick (1400 °C) served as the kiln floor. The insulation thickness was adjusted to meet different firing temperatures (8 cm for 1100 °C and 12 cm for 1300 °C), maintaining the microwave cavity wall temperatures around 100 °C and providing a free volume of 6.5 L and 3 L, respectively. The volume could be changed by adding or removing JM23 plates.

To prevent magnetron overheating, both kilns were equipped with external ventilation. The small kiln had a fixed 1.2 m³/min fan, while the large one had an adjustable 0–14 m³/min system to cool the three magnetrons and the cavity walls. The original power and timer controls were kept, allowing for manual and individual operation of each magnetron.

These two ovens were fitted with a type K shielded thermocouple linked to digital thermometers for temperature measurements and recording by a computer. Their intrinsic accuracy conforms to commercial standards. The overall measurement error includes the quality of the signal processing provided by the commercial devices used.

We consistently ensured the continuity and coherence of the measurements, aligning with the expected gradual temperature rise as a function of the electrical power supplied. Any abrupt anomaly in the temperature curve during our experiments corresponded to a confirmed technical fault with the thermocouple (e.g., breakage, melting, or contamination by glass or ceramic), and the data in those instances were systematically excluded from the analysis and the presented figures. Therefore, the data used in the figures are deemed reliable concerning sensor integrity.

The temperatures were also measured by a commercial digital infrared pyrometer either through the shutter of the small microwave or after opening the oven door. The pyrometer has an accuracy of 3% from 800 to 1600 °C and a measuring spot of 12 mm and 19 mm at 20 cm and 30 cm, respectively.

Concerning the safety assessment of this experimental microwave kiln that could be considered rudimentary when compared to industrial standards, we retained and centralised the original safety mechanisms of the domestic microwave oven, particularly the entire door opening safety system (limit switches). Regarding microwave leakage, leaks were meticulously mapped using a professional-grade detector (RS-2G detector) and were systematically eliminated by implementing adequate shielding across all apertures and connections. This ensured a safe working environment during the trials.

Gaseous or nanoparticle emissions were not monitored during firing. Gaseous emissions would join the range of gases and fumes emitted by classic ceramic kilns. They result not only from fuel combustion but also from high-temperature transformations of ceramic bodies and metal oxide-based glazes during firing at temperatures up to 1400 °C. These emissions are a known issue for which professionals recommend specific safety practices, such as the necessity of adequate ventilation. These precautions were taken during these experimental works.

The possible decomposition of Fe₃O₄ into nanoparticles by microwaves, which are specific to this heating method, has been tested. These effects are demonstrated in experiments that treated susceptors composed of 100% Fe₃O₄, with flashes of particles erupting from the susceptor and becoming embedded in the furnace walls. This phenomenon was never observed when the Fe₃O₄ was mixed with other refractory materials (SiC, SiO₂, Al₂O₃) and represented only 20% to 35% of the susceptor composition. This issue is further minimised given that the Fe₃O₄ particles are completely consumed within the initial 10 min of the sintering process.

Remarkably, this rustic, recycled equipment proved highly durable, withstanding over 150 firing cycles up to 1100 °C and beyond, each lasting several hours. Only a single capacitor failure was recorded.

2.2. Susceptors

2.2.1. Susceptor Considerations

The success of hybrid heating largely depends on the susceptor’s design. Susceptors must provide sufficient preheating without excessively shielding the ceramic piece from microwaves. Therefore, their quantity and placement must be carefully chosen to ensure that microwaves can still reach the material [26]. This is particularly important when a susceptor fully surrounds the sample.

To make it easy to adjust the susceptor quantity and placement, we opted to develop solid, wafer, or rod-shaped susceptors that could be placed on the kiln floor or vertically along the walls [27]. While industrial susceptors are typically made from SiC or MoSi₂ rods [26,30], these materials are not commercially available to the public. Instead, we focused on common, low-cost powdered minerals like silicon carbide (SiC), magnetite (Fe₃O₄), and carbon (graphite, coal) [26,30,31].

SiC is an excellent dielectric material for microwave absorption, known for its low density and high thermal and chemical resistance. However, its absorption performance can be highly variable, depending on its crystalline structure (polytype) and morphology [31]. For this reason, SiC often requires modification to enhance its absorption, which can include adding other dielectric or magnetic materials like magnetite or increasing its porosity to promote multiple reflections [31].

Magnetite (Fe₃O₄), a member of the spinel ferrite class, also excels at microwave absorption due to its complex permeability and permittivity. However, for efficient absorption, magnetite is often most effective when it has nano- to submicrometre size [32].

Since a common method for creating a solid from a powder is high-temperature sintering by reactive solid or liquid phase sintering using microwaves [33,34]. The use of additives to achieve reactive sintering makes it possible to avoid the extreme conditions required to sinter silicon carbide [33,34,35]. The additives reduce sintering temperatures and improve densification while also affecting the high-temperature mechanical and thermal properties of SiC ceramics [34]. Thus, we explored this process to manufacture our susceptors. Although iron, introduced in the form of Fe₂O₃, is not known to be an effective additive for sintering silicon carbide with conventional heating [35], we tested a mixture of a powder of submicrometre magnetite and a powder of micrometre SiC. In just 10 min in the microwave, the mixture was fully sintered, exhibiting excellent mechanical properties. Tests showed that the best performance was achieved with 20% to 45% magnetite by weight. Beyond this range, the mixture was susceptible to thermal runaway, which would episodically destroy the sample.

2.2.2. Susceptor Manufacturing: Materials and Procedure

Based on preliminary test results, a series of susceptors were manufactured using silicon carbide (SiC) and magnetite (Fe₃O₄) powders in various compositions and shapes. The SiC powder, a common abrasive material, had grain sizes ranging from 10 to 100 µm (140 to 1000 MESH).

The magnetite powder was sourced from the Hymag’in start-up (Grenoble, France) and was synthesised from metallurgy ferrous scraps [36]. It featured a fine grain size distribution, ranging from nanometric to microscopic (60–3000 nm), with an average size of around 800 nm (Figure 2). Tests confirmed that this nanoscale or submicroscopic size was crucial for effective microwave interaction; coarser, other commercially available magnetites (from a pigment supplier and LKAB) remained inert. To enhance microwave absorption, especially at low temperatures, alumina (Al₂O₃) and silica (SiO₂) sands were added. At room temperatures, these materials are largely transparent to microwaves [26], acting as a porous structure that improves absorption capacity and allows waves to penetrate the susceptor more easily [31]. As temperatures rise, the changing dielectric loss around 800 °C of alumina allows them to increase the susceptor’s overall absorption [9,26,37]. The Fontainebleau silica sand (200 µm) was purchased from a ceramics supplier, and the alumina corundum sand (250 µm) was an air eraser compound. In use, these sands also played the role of a solid matrix during the reactions undergone by the susceptors during the heating cycles. Pure graphite powder was also used in one test.

The powders were mixed with demineralised water and lightly ground by hand in a porcelain mortar. They were then cast into various shapes using silicone moulds or moulds carved from JM26 refractory bricks (Figure 3). For the silicone moulds, 5% clay (fraction < 2 µm from Wyoming bentonite) was added to improve handling after drying. Sintering was performed in the small microwave for shorter susceptors and in the large kiln for longer ones. In total, approximately 50 susceptors were created and tested in over 150 firing experiments. The main types of susceptors manufactured in this study are listed in

Table 1. Main types of susceptors manufactured. * Only SiC is considered to calculate the Si mole fraction; the porosity is calculated as the difference between the volume of the susceptor and that of the mineral constituents.

Type	Name	Weight Gram	Fe3O4 Wt. %	Silica or Alumina Wt. %	SiC Wt. %	Mole % Silicon SiC *	Mole % Iron	Ratio SiC/Fe3O4	Porosity * %
SiC	SiC-3.5	15	0	0	100	100	0		55
MS Fe3O4 + SiC	MS-3.5-22	23	22	0	68	85.7	14.3	3.1	60
	MS-6-25R	15	25	0	75	83.4	16.6	2.6	51
	MS-7-25	20	25	0	75	83.4	16.6	2.6	51
	MS-6-35R	15	35	0	65	78.2	21.8	1.9	55
MSS Fe3O4 + SiC + silica sand	MSS-7-30	20	30	25	35	72	28	1.3	64
	MSS-6-35R	15	35	25	40	65.9	34.1	1.0	55
	MSS-9-35-R	13	35	25	40	65.9	34.1	1.0	55
MAS Fe3O4 + SiC + alumina sand	MAS-7-30	20	30	25	35	72	28	1.3	64
	MAS-9-35-R	13	35	25	40	65.9	34.1	1.0	55

. The magnetite-based susceptors can be classified into two groups: one with a low Fe₃O₄ wt. content (MS type, SiC/Fe₃O₄ ranging from 1.9 to 3.1) and a group with a higher content (MSS and MAS type, SiC/Fe₃O₄ between 1 and 1.3).

2.2.3. Macroscopic Susceptor Characterisation Method

The behaviours of the susceptors were evaluated by visual observation of them in situ during sintering. We used an optical pyrometer to measure the susceptor’s surface temperature and a shielded type K thermocouple to measure the furnace temperature.

To quantify the susceptors’ thermal power, each one was placed in a small, 100 cm³ insulated chamber inside the small microwave’s 800 cm³ kiln. A thermocouple, positioned 0.6 cm above the susceptor’s surface, continuously recorded the furnace temperatures (Figure 3f). The susceptor’s temperature, measured by a pyrometer immediately after heating, was on average 100 °C ± 40 °C (40 samples) higher than the thermocouple reading.

Based on these measurements, the average thermal power (W/gram) of each susceptor was calculated using its maximum temperature, heating time, mass, and the specific heat values of its components (

Table 2. Specific heat value for the considered minerals. Adsorption P: power calculated as P = m × Cp × (Tf-Ti)/Δt with P: power (W), m: mass to be heated (kg), Cp: specific heat (J/kg.K), Ti: initial temperature, Tf: final temperature °C), Δt temperature rise time (s).

	kJ/(kg⋅K)
SiC	0.678
Magnetite	0.653
quartz	0.7
Alumine	0.9

).

2.2.4. Microscopic Susceptor Characterisation Method

The goal of the microscopic study was to understand the evolution of these materials, their influence on the redox conditions, and the temperatures at which transformations occur.

To study the mineral transformations within the susceptors, two types of preparations were made for scanning electron microscopy:

Slices of the main body of the susceptors, which were glued, thinned, and polished on an aluminium support.

Sampling of the melted structures: This included bubbles and films that formed on the susceptor surfaces. The samples are glued onto an aluminium backing for their direct observation.

These observations were complemented by X-ray diffraction (Cu radiation) performed on crushed powder samples with a Rigaku XMAX 2500 rotating anode X-ray diffractometer at Laboratoire de Géologie de l’Ecole Normale Supérieur in Paris (LGENS) and a Siemens D5000 diffractometer at Institut des Sciences de la Terre (ISTerre) in Grenoble.

Scanning electron microscopy (SEM) investigations were conducted on carbon-coated polished sections of susceptors for imaging with backscattered electrons and energy dispersive X-ray spectroscopy (EDXS) mapping. A probe current of 150 pA at 15 kV was used for EDXS mapping that allowed semi-quantitative compositional analysis. Two different SEMs were used: an SEM-FEG TESCAN CLARA (PtME MNHN) and an SEM-FEG Zeiss SIGMA (LG-ENS). The microscope at LGENS had an EBSD (Electron Backscatter Diffraction) Oxford Instruments device for crystallographic determinations.

The ageing of the susceptors was studied by SEM characterisation on samples chosen immediately after sintering, after two heating cycles (recent), and after more than ten heating cycles (aged).

A firing cycle consisted of a temperature increase to a maximum plateau (heating) followed by a cooling phase. The average heating time was about 60 min (with a maximum of 90 min), while cooling took between 2.5 and 4 h (Figure 4).

3. Results

3.1. Macroscopic Evaluation of the Properties of Different Susceptor Formulations

The results are presented in Figure 5, Figure 6 and Figure 7 and

Table 3. Average absorption power (W/gram) for the main batches of susceptors. The values are presented as a function of their cumulative usage time, from their initial sintering up to their final state after firing ceramics. Cumulative usage time is defined as the total heating time, not including cooling periods.

	Type	Batch Susceptor Number	Average Thermal Power W/Gram	Thermal Power Standard Deviation	Average Cumulative Usage Time Minutes	Average Surface T °C
Just sintered	SiC	7	3.10	1.80	7	561
	MS-3.5-22	8	4.71	0.29	7	843
	MS-6-25R	1	4.75		7	850
	MS-6-35R	1	4.94		7	883
	MS-7-25	4	4.56	0.36	11	752
	MSS-7-30 MAS-7-30	4	4.71	0.86	11	823
«recent» Two cycles of heating	SiC	4	1.50	0.64	30	283
	MS-6-25R	1	4.07		30	732
	MS-6-35R	1	3.89		130	702
	MSS-6-35R	1	3.13		130	565
«old» More 10 cycles of heating	MS-3.5-22	7	4.40	0.39	600	790
	MS-7-25	2	3.97	0.002	800	850
	MSS-7-30 MAS-7-30	17	1.37	0.36	1341	261

. After sintering and use, they showed a clear decrease in thermal power over time. Susceptors made of SiC alone degraded the most, while those containing magnetite retained their performance better.

• Silicon Carbide (SiC) Alone

Susceptors made solely of silicon carbide (with grain sizes of 10–60 µm) coupled unevenly with microwaves, leading to inconsistent temperatures both between and within samples (Figure 5).

These susceptors, even with the addition of 10% bentonite, never fully sintered and remained powdery after heating. The best performance was observed with intermediate grain sizes (600 MESH, or 23 µm), with an average absorption power of approximately 3 W/gram during sintering. However, this power rapidly declined to 1.5 W/gram after just 30 min of use (Table 3, Figure 6 and Figure 7). These characteristics did not allow them to be used further.

• Silicon Carbide + Magnetite (MS) with SiC/Fe₃O₄ ratio = 1.9 − 3.1

These susceptors consistently coupled strongly with microwaves, achieving uniform temperatures across and within samples (Figure 5). Sintering temperatures ranged from 800 to 930 °C. The best performance was observed with intermediate grain sizes (220–500 MESH, 63 to 28 µm). Susceptors with 40 wt. % magnetite performed better than those with 22%, particularly in temperature uniformity.

Successful sintering occurred on the very first heating, resulting in robust, shock-resistant susceptors. The average absorption power of these low iron susceptors was remarkably stable, decreasing only slightly from 4.5 W/gram to 4 W/gram over 800 min of use (Table 3, Figure 7). This exceptional heating power allowed the kiln to reach nearly 800 °C in just 420 s, far surpassing the 250 °C achieved with the best SiC-only susceptors (Figure 6). After repeated use, even at temperatures up to 1300 °C, the MS susceptors retained their shape and appearance, though their surface colour shifted to a greyish-red, suggesting the oxidation of black iron oxide (FeO or Fe₃O₄) to reddish hematite (Fe₂O₃) (Figure 8a).

• Silicon Carbide + Magnetite + Silica or alumina (MSS, MAS) with SiC/Fe₃O₄ ratio = 1 − 1.3

These susceptors also coupled strongly with microwaves, reaching sintering temperatures comparable to the formulations having a high SiC content. However, their very high initial absorption power (4.7 W/gram) steadily decreased with use, eventually matching the low performance of SiC-only susceptors (1.4 W/gram) after 1300 min of cumulative heating (Figure 7). This decline in performance was also reflected in their heating power (Figure 6, curves 4-5-6).

After prolonged use, although keeping their shape, their appearance changed, showing increased surface porosity and fusion bubbling. During one firing of porcelain at 1300 °C, a MAS susceptor with alumina sand developed a melted, glassy film on its surface. The colour of these susceptors remained a deep black with a slight sheen, suggesting a more reducing environment that preserved the reduced iron oxides (Figure 8).

• Other Formulations

Two other compositions were tested: one with magnetite and silica sand and another with magnetite, graphite, and SiC. Both initially heated well but could not sustain the high temperatures. The magnetite and silica sample remained powdery, and both samples oxidised, turning red as the magnetite converted to hematite and the graphite burned away. These formulations were not used further.

The simple, accessible manufacturing process developed here successfully produced batches of magnetite-based susceptors of sufficient quality to fire ceramics with apparent temperature homogeneity in a modestly sized kiln (Figure 9). The susceptors less rich in Fe₃O₄ (SiC/Fe₃O₄ ≥ 1.9) showed excellent durability by keeping both their physical and thermal properties after sintering. Despite an apparent decrease in the performance over time and with an alteration of their appearance, the richest in Fe₃O₄ (SiC/Fe₃O₄ = ~1) still demonstrated the ability to quickly rise to high temperatures to achieve porcelain firing.

3.2. Microscopic Susceptor Characterisation

3.2.1. Descriptions of Mineral Transformations in Susceptors

The mineral transformations observed according to the main formulations and according to the cumulative duration of heating, including the first sintering, are presented in

Table 4. Mineralogical transformations of the main types of susceptors, from their sintering process to their transformation during prolonged use in ceramic heating cycles. The data are derived from the compilation of observations and analyses performed using SEM techniques: SE, BSE, EDS, and EBSD imaging and characterisations, as well as powder X-ray diffraction. The symbols (+) and (-) correspond to the apparition or disappearance of a phase. The number of symbols in brackets represents an approximate intensity between 0 and 5 (100%). * (1) and * (2) indicate that the phase is primary (initial) or secondary (subsequent).

		SiC/Fe3O4 > 1.8						SiC/Fe3O4 < 1.3
	Type	MS 22–25				MSS 22	MAS 22	MSS 30–35		MAS 30–35
	Usage Time	7 min	25 min	130 min	>600 min			130 min	>600 min	130 min	>600 min
Mineral Name	T max °C	850	1100	1100	1300	1300	1300	1100	1300	1100	>1300
Moissanite * (1)	SiC	(-)	(--)	(--)	(--)	(---)	(--)	(---)	(----)	(---)	(----)
Magnetite * (1)	Fe3O4	(-----)	(-----)	(-----)	(-----)	(-----)	(-----)	(-----)	(-----)	(-----)	(-----)
Quartz * (1)	SiO2					(-)		(-)	(-)
Alumina * (1)	Al2O3						(-)			(-)	(-)
Iron BCC	Fe	(++)	(++)	(---)	(---)		(+)	(--)	(-----)	(-)	(-----)
Ferrosilicon sum		(+)	(++)	(++)	(-)	(-)	(-)	(++)	(--)	(++)	(--)
Gupeiite	Fe3Si	(+)	(+)							(+)
Xifengite	Fe5Si3		(+)	(+)		(+)	(+)	(+)	(+)		(+)
	Fe11Si5		(+)		(+)		(+)	(+)		(+)
Ferdisilicite	FeSi2		(+)	(+)			(+)
Cristobalite	SiO2	(++)	(++)	(++)	(++)	(++)	(++)	(++)	(++++)	(++)	(+++)
Trydimite	SiO2								(++)		(+)
Magnetite * (2)	Fe3O4		(+)		(+)		(+)	(++)	(++)	(++)	(+++)
Hematite	Fe2O3			(++)	(+++)	(+)		(++)	(+)
Mullite	Al6Si2O13										(+)
Fayalite/forsterite ferroan	Fe2SiO4		(+)				(++)	(++)	(+)	(+)
Hercynite	FeAl2O4						(+)			(+)	(+)
Glass	Fe-Si-O						(+)	(+)	(+)		(++)
	Si-Al-Fe-O										(+)

. The image descriptions and presentation of crystallographic and chemical data for the main mineral transformations and their evolution during the heating cycles from the first sintering step are shown in Figure 10, Figure 11, Figure 12, Figure 13, Figure 14 and Figure 15.

• Sintering: At the microscopic scale, mineral transformations are characterised by a total disappearance of the initial magnetite within the first minutes of sintering, leading to mineral reactions with silicon carbide. During the initial 7 min sintering at 850 °C, magnetite transforms into three distinct phases: (1) iron droplets, 100 to 200 µm in size, typically located within the largest pores; (2) hematite dispersed throughout the matrix; and (3) micrometric granules of ferrosilicon (gupeiite, Fe₃Si) associated with a layer of cristobalite, formed at the periphery of the silicon carbide grains (Figure 10).

Upon continued sintering at 1100 °C for an additional 18 min, these mineral transformations intensify. The iron droplets develop a polycrystalline structure characteristic of body-centred cubic (BCC) iron. Concurrently, the ferrosilicon layers surrounding the initial silicon carbide grains thicken and extend, while the SiC grains themselves decrease in size. A brief SEM image analysis suggests a 40–50% reduction in SiC grain volume, with the average grain size diminishing from an initial 44 µm to 25–30 µm after heating. These granular structures, consisting of a silicon carbide core surrounded by ferrosilicon, are bonded together by cristobalite. This matrix of cristobalite is locally intergrown with ferrous olivines (fayalite) associated with newly formed magnetite (Figure 11 and Figure 12). The SEM-EBSD images and analyses characterise the various iron-silicon phases present in the matrix surrounding the SiC grains (Figure 13) and, at times, within single crystals (Figure 14). In addition to the gupeiite (Fe₃Si) observed after the initial 850 °C sintering, we also identify xifengite (Fe₅Si₃), ferrosilicite (FeSi₂), and an unnamed iron-silicon phase (Fe₁₁Si₅).

EBSD mapping analysis quantifies the total proportion of ferrosilicon in the matrix to around 15,7%. Within the matrix and in the large zoned crystals, the relative proportions of Fe₅Si₃, Fe₃Si, and FeSi₂ are, respectively, 43 and 48%, 39 and 40%, and 18 and 11% (% of identified phases). Other phases identified in the EBSD mapping include SiC (47%), SiO₂ (cristobalite, 24%), Fe₃O₄ (magnetite, 7.3%), and Fe₂SiO₄ (fayalite, 6.1%). The percentage of unindexed points, likely corresponding to porosity, is 53% (Figure 13,

Table 5. Partial quantification of the mineralogical and porosity changes resulting from thermal cycling, comparing a just sintered susceptor (MS22 at 1100 °C, Figure 11) with an aged one (MAS22 reaching 1300 °C, Figure 15).

Type	MS 22		MAS 22
Duration of heating—T°C	28 mn. T° 1100 °C		>600 mn. T°1300 °C
Mineral proportions based on frequency of occurrence in the FeSi group
Location	FeSi mono-crystal zonation %	Matrix %	Matrix %
Xifengite %	48	42.94	46.05
Gupeiite %	40.5	38.83	9.69
Ferdisilicite %	11.5	18.22	32.19
Fe11 Si5 %	n.d.	n.d.	12.07
Mineral composition in number of occurrence in matrix (75 × 75 µm) × 2 150 × 150 µm
Total FeSi %		15.69	6.7
Moissanite 3c or 6H (SiC) %		47.11	47.09
Magnetite (Fe3O4) %		7.29	7.18
Fayalite or Forsterite ferroan (Fe2SiO4) %		6.10	11.61
Cristobalite (SiO2) %		23.81	22.00
Hercynite (FeAl2O4) Fe %			3.73
Porosity (MS22) or porosity + glass (MAS 22) %		52.89	47.95

). This value is comparable to the porosity calculated for samples containing 25% magnetite (Table 1).

• Low Fe₃O₄ content susceptor evolution. During successive heating cycles of ceramics up to 1300 °C, the mineralogy and structure of the magnetite-poor susceptors (SiC/Fe₃O₄ > 2) undergo moderate changes, as does their external appearance, irrespective of the formulation (with or without added quartz or alumina) (Table 4).

In most cases, the iron droplets found within the porous structure are partially or completely replaced by an iron oxide, typically hematite. An exception is observed in MAS-type susceptors, where the iron oxide is magnetite instead. In MS and MSS susceptors, fayalite (Fe₂SiO₄) is locally replaced by pseudomorphs composed of microscopic fibres or particles of hematite embedded in cristobalite. A glass with the composition of fayalite is also observed locally in the highest-temperature samples. Hercynite (FeAl₂O₄) appears in the MAS susceptors, specifically in association with corundum, meaning that alumina grains are involved in mineral reactions.

The data reveal a near halving of total ferrosilicon (from ∼16% to 7% of EBSD identified occurrences), characterised by a sharp drop in gupeiite (Fe₃Si) but a relative rise in ferrosilicite (FeSi₂). Concurrently, the proportion of fayalite increases significantly, from 6% to 12%. Phases such as SiC, magnetite, and cristobalite maintain stable concentrations. The combined porosity and glassy phase—represented by areas without defined EBSD crystal orientation (Figure 15)—shows a modest reduction from 53% to 48% after cycling.

• High Fe₃O₄ content susceptor evolution. As the transformation of their external appearance suggested, the mineralogy of the susceptors with a high Fe₃O₄ content during the heating cycles of the ceramics shows strong modifications.

The replacement of SiC grains by ferrosilicon and cristobalite is more intense. Visually, we can estimate that approximately 75% of the SiC grains have disappeared after the first two heating cycles (Figure 16). During the first two heating cycles at 1100 °C, large areas composed of cristobalite, containing microscopic hematite crystals, envelop and infiltrate the regions where the SiC and ferrosilicon aggregates are still well preserved (Figure 16). However, these structures disappear and were not observed in the aged susceptors. In the following successive heating cycles, the silicon carbide gradually disappears until it is completely gone after 10 to 15 cycles. This is accompanied by a significant development of siliceous phases, most commonly cristobalite and locally tridymite, in the MAS-30 susceptor shown in Figure 8e.

In this series of iron rich susceptors, the amount of metallic phases decreases with time, more intensely in the siliceous MSS susceptors than in the aluminous MAS ones. Iron disappears completely, while the ferrosilicon phases persist as dispersed particles within the matrix, in the form of xifengite (Fe₅Si₃). Ferrosilicates, such as fayalite, present in the initial heating cycles, decrease or disappear in susceptors used at high temperatures, coinciding with the appearance of glassy phases in the susceptor matrix. These Fe-Si-O glasses are sufficiently abundant to exude and flow to the surface of the susceptors, where they recrystallize (Figure 8c–e) as magnetite and cristobalite (Figure 17). In the MAS alumina susceptors, aluminous phases such as hercynite (FeAl₂O₄) crystallise around the corundum grains, while mullite fibres (Al₆Si₂O₁₃) appear within the cristobalite matrix or in a glass of Si-Al-Fe-O composition, which could be the result of the melting of ferrocordierite (Al₄Si₅Fe₂O₆).

The transformations observed in these magnetite-based susceptors appear to be of great diversity and complexity. These transformations are typically seen in steel slags and ferro-silicon furnaces [38]. The mineral assemblages are highly significant indicators of the extreme temperature and redox conditions these objects have undergone and therefore provide crucial insights into the environment within the microwave kiln.

3.2.2. Interpretation of Mineral Transformations: Evaluation of Temperature and Redox Conditions

The most striking observation is the disappearance of magnetite during sintering, with the pseudomorphic replacement of the silicon carbide grain outer rim by ferrosilicon at temperatures between 850 °C and 950 °C. These results are consistent with experiments [39,40] conducted at 800–1100 °C on mixtures of iron and silicon carbide in air or in the presence of argon and hydrogen. In these studies, silicon carbide was shown to decompose with the formation of the more thermodynamically stable ferrosilicon (Fe₃Si) and the precipitation of graphite.

Other experiments [5,6] conducted to investigate the feasibility of producing cast iron from iron oxide and carbon using microwaves as an energy source have shown that pig iron can be obtained in air with yields of approximately 40%.

To understand the behaviour of magnetite alone when exposed to 2.45 GHz microwaves, a simple experiment was conducted by placing a few grams of magnetite powder in a sealed silica tube and heating it in a small microwave oven. Within seconds, the powder reacted, causing a sudden temperature rise and a strong gas emission until the tube exploded. The resulting post-cooling sample (Figure 18) shows a black core containing electrically conductive particles surrounded by a red hematite crown. This suggests a strong reduction in magnetite to iron and reduced oxides with the emission of oxygen gas, i,e, Fe₃O₄ => 3Fe + 2O₂. This oxygen would be responsible for the tube explosion and for the oxidation of the sample’s outer rim during cooling. Another observation made in this study is the constant appearance of a flame above all susceptors containing magnetite and silicon carbide during the first few minutes of sintering, which suggests the emission of a combustible gas (Figure 18).

All these observations, combined with the presented mineralogical data and literature references [5,6,40,41,42], suggest that during sintering, the reaction between magnetite and silicon carbide in the susceptor is as follows:

(R1) 2 SiC + Fe₃O₄ → Fe₃Si(s) + 2 CO(g) + SiO₂(s)

And in air, the hot CO gas burns according to the following:

(R2) 2 CO + O₂ → 2 CO₂

The observed mineral transformations in the susceptors are interpreted through reference to the phase diagrams of the Fe-Si and FeO-SiO₂ systems (Figure 19 and Figure 20) and [41,42,43,44]. Temperature conditions measured during sintering, ranging from 850 °C to 950 °C, are consistent with the formation of BCC iron and gupeiite (Fe₃Si) via solid-state transformations. The subsequent appearance of higher-temperature and more siliceous ferrosilicon compounds, such as xifengite (Fe₅Si₃) and ferdisilicite (FeSi₂), in susceptors heated to around 1100 °C aligns with their stability fields (Figure 19) in a system necessarily very low in oxygen. During successive heating cycles, the disappearance of gupeiite corresponds to the re-equilibration of the system around its average composition (R1, Figure 19). This re-equilibration occurs either by solid-state recrystallization at temperatures below 1210 °C or by fusion-recrystallization at the highest temperatures [41,42]. The preferential nature of the latter mechanism is strongly suggested by the correspondence between the compositions of the ferrosilicon compounds (Fe₁₁Si₅, Fe₅Si₃, and FeSi₂) and the compositions of the two eutectics in the Fe-Si system, centred at 0.3 and 0.7 mole fraction of Si (Figure 19).

The silica phase resulting from reaction (R1) is nearly always cristobalite. Since its stable equilibrium is typically maintained above 1470 °C, its presence in this context necessitates it being considered metastable. In contrast, tridymite, which is stable under the studied temperature range (850 °C to 1300 °C), was identified by X-ray diffraction in only two samples (MAS-30) (Table 4).

Olivines (fayalite) are compatible with temperatures below 1190 °C, which marks their melting temperature (Figure 20) [43,44]. Above this temperature, in the presence of metallic iron and silica, ferrous olivine melts to produce a highly iron-rich ferrosilicate liquid [43]. The degree of melting is composition-dependent: the greater the iron content and the closer the system is to the eutectic composition, the more extensive the melting. Consequently, the most iron-rich susceptors (SiC/Fe₃O₄ = 1, such as MSS and MAS-30–35) can experience up to 60% melting, while samples with the lowest iron content (SiC/Fe₃O₄ = 3, such as MS-22) are only affected to the extent of 23% (Figure 20).

In addition to temperature, the co-existence of olivine minerals, metallic phases (BCC iron, ferrosilicon), and silica dictates extremely low oxygen partial pressures P(O₂), on the order of 10⁻¹²⁻¹⁶ atmospheres below 1300 °C [43]. These highly reducing conditions are consistent with reaction (R1), which involves the decomposition of silicon carbide (SiC) and the production of CO gas. However, maintaining such reducing conditions is challenged by the presence of oxygen in the furnace atmosphere (P(O₂) = 0.21 atm). In susceptors with a lower iron content, where the destabilisation of SiC is less pronounced, or in susceptors not subjected to extensive heating above 1100 °C, the highly reduced zones are interspersed with more oxidised zones. These zones are characterised by the presence of hematite replacing BCC iron or associated with SiO₂ instead of fayalite, which corresponds to P(O₂) values between 10⁻¹⁰ atm at 1100 °C or 10⁻⁶ atm at 1300 °C [43]. These more oxidising conditions significantly shift the system’s melting point to above 1450 °C [43], further limiting the melting potential of these iron-poor susceptors (SiC/Fe₃O₄ > 2), consistent with the visual observation of melting features (Figure 8a).

In contrast, in susceptors with a higher iron content, where the destabilisation of SiC is more advanced and continues with each heating cycle, reducing conditions are maintained at an intermediate level. This leads to the formation of stable magnetite—SiO₂ assemblages under P(O₂) of approximately 10⁻⁸ to 10⁻¹⁰ atm. between 1100 and 1300 °C. Under these conditions, the melting temperatures are between 1250 °C and 1350 °C [43]. This corresponds well to the appearance of fusion structures on the surface of these susceptors heated around and above 1250 °C (Figure 8c–e).

While the MS 22–25 series susceptors (low iron content) correspond well to the requirements for hybrid ceramic heating at temperatures around 1300 °C, the significant melting observed in the high-iron susceptors above 1200 °C is surprising for their intended use in firing ceramics. However, the observation of a recrystallized melt structure composed of magnetite and silica, which indicates very reducing conditions at the surface of the susceptors exposed to the furnace atmosphere, implies that this atmosphere itself was also significantly reduced. The ability to create a reducing atmosphere, low in oxygen, within a ceramic kiln is a crucial feature [46]. This is necessary to achieve specific effects in glazing and is generally achieved by controlling the combustion process in gas-fired kilns. In electric kilns used for ceramics, the atmosphere is typically oxidising.

Table 6. Stoichiometric balance following reactions R1 and R2 of the susceptor sintering reactions and its consequences on solid phase volume reduction and gas emissions as a function of material composition. (a) and (b) Calculation of the total amount of gas generated by a 150 g susceptor assembly in the same furnace over their typical lifespan of approximately ten heating cycles in the furnace.

Susceptor Name	MS-3.5	MS-6-R	MS-7	MSS-6-R	MSS-7	MAS-7
Weight gram	15	15	20	15	20	20
% Fe3O4	22	35	25	35	30	30
% SiC	68	65	65	35	40	40
SiC/Fe3O4 wt. %	3.1	1.9	2.6	1.0	1.3	1.3
Volume cm3	10.0	9.6	10.8	9.6	10.8	10.8
% SiC consumed	11.16	18.57	13.26	34.48	25.86	25.86
Volume Fe3Si cm3	0.39	0.61	0.59	0.61	0.70	0.70
Volume silica cm3	0.21	0.34	0.32	0.34	0.38	0.38
Solid phase volume variation %	−7.4	−12.3	−12.2	−11.4	−14.6	−13.0
Sintering CO volume, litre	0.64	1.01	0.97	1.01	1.16	1.16
Sintering CO2 volume, litre	1.00	1.59	1.52	1.59	1.82	1.82
(a) Max CO volume, litre				29.4	33.6	33.6
(b) Max CO2 volume, litre				46.2	52.8	52.8

presents the physical transformations (changes in solid and gas volumes) observed in the susceptors during sintering, based on their composition. For susceptors with the highest iron content, the analysis also extends to their use in successive heating cycles, which leads to the complete consumption of silicon carbide (SiC). During these cycles, the high-temperature generation of significant volumes of reducing gases (CO and CO₂)—amounting to several litres under standard conditions in each cycle—is notable. Given the furnace volume of 4–6 L, this gas production is sufficient to ensure the furnace atmosphere remains strongly reducing, even throughout the cooling phase.

The use of iron-rich susceptors, which can partially melt at relatively low temperatures (~1200–1260 °C) in reducing conditions [43], potentially allows for control of the redox potential in the furnace, but this approach also limits their lifespan.

3.3. Added Values of the Studied Susceptors

In conclusion, the susceptors studied here, based on a mixture of silicon carbide and magnetite powder, provide a powerful and versatile toolbox for ceramic firing.

The magnetite-poor susceptors (SiC/Fe₃O₄ > 2) demonstrate excellent durability, reproducibility, and thermal efficiency up to at least 1300 °C, positioning them on par with conventionally used susceptors for hybrid microwave heating [26].

Conversely, the magnetite-rich susceptors (SiC/Fe₃O₄∼1) also exhibit excellent initial thermal efficiency but undergo progressive degradation, limiting their lifespan to ten to fifteen heating cycles. However, they offer a unique ability to control the oxygen reduction level within the furnace. The addition of silica or alumina sand, while finally not necessary for microwave absorption, provides, in fact, an effective structural framework, maintaining the susceptor’s integrity during partial melting reactions above 1200 °C.

For these susceptors, the performance degradation threshold could be evaluated by a significant and irreversible increase in the time required to reach the target temperature (e.g., 1200 °C), or by increased thermal heterogeneity observed within the sample. The end-of-life could be decided by a structural failure such as physical cracking, melting, or disintegration rendering the susceptor unusable. A comparative evaluation of the overall performance of the different types of susceptors is shown in

Table 7. Comparison of the performances of the main types of susceptors tested under significant conditions during this work, including two additional experiments conducted around 1500 °C. The temperature for the additional experiments was estimated based on the observation of mineral reactions, specifically the quartz-cristobalite transition and the graphitization of carbon.

	SiC/Fe3O4 > 1.8 Wt. %		SiC/Fe3O4 < 1.3 Wt. %
	MS 22–25		MSS 30–35		MAS 30–35
Max T °C	1500	1300	1150	1300	1150	1300
Heating cycles	2	30	10	15		15
Redox capacities	No	No	Yes	Yes	Yes	Yes
Physical degradations	No	No	No	Yes	No	Yes
Type of degradation				Partial melting		Strong melting
Significant loss of Thermal power	No	No	Yes	Yes	Yes	Yes
End of life reached	No	No	No	Yes	No	Yes

.

Direct comparison of the performance of the manufactured susceptors with commercially or laboratory-used silicon carbide (SiC)-based susceptors is challenging due to the incompleteness of available literature data. While thermal characteristics, such as thermal power, are sometimes addressed, the crucial factor of susceptor durability is rarely reported. Referring to the comprehensive review by Bhattacharya and Basak [26] on susceptor-assisted microwave processing of materials, the thermal performance of MS25-type susceptors appears superior to that of standard SiC susceptors. Specifically, the MS25 material achieved a temperature rise to 1300 °C in 35 min (Figure 21), whereas the SiC material required 60 min ([26], Figure 6). Furthermore, maximum temperatures exceeding 1500 °C were reached in both cases. However, the repeatability of these reported experiments is unknown, and the timeframe of the present work is insufficient to reliably estimate the operational lifespan of our susceptor types. Notably, the literature lacks a description of susceptors that are intentionally used for their redox capacity, a characteristic that appears to be unique to our iron-rich susceptors.

Both types of susceptors are exceptionally easy and quick to fabricate using readily available, low-cost materials. It depends mainly on the price of the submicroscopic magnetite powder, the price of the other components being negligible, which is currently approximately EUR 0.4/g. This means that a 150 g batch of low-iron susceptors, required for ceramic firing in a 6 L kiln, currently costs around EUR 15 with a lifespan of several dozen firing cycles, whereas for those with a higher iron content with redox capacities, the cost will be around EUR 21 for a lifespan of 10 to 15 cycles. This price can be compared to the EUR 2.50 currently charged by ceramicists per firing cycle for the ageing of heating elements in a standard electric kiln.

4. Examples of Application: Ceramic Firing and Glazing

4.1. Ceramic Materials and Firing Procedure

The materials used for the ceramic pieces were all commercial products available in ceramic material stores in France: white and red earthenware clays. These had a recommended firing temperature of 1050 °C for biscuit and 1020–1060 °C for glazing. Porcelain pastes: These had a recommended firing temperature of 950 °C for the degourdi and 1280–1340 °C for vitrification. Professional ceramists made some of the pieces fired.

The distribution and organisation of the pieces in the oven were performed in a way that optimised space for maximum filling. The susceptors were moved to accommodate the free spaces, ensuring they did not touch the susceptors but remained at a distance of 2 to 3 cm (Figure 1b). Mixing ceramics of different compositions in the same load was avoided to achieve the most homogeneous response possible to the microwave interaction.

The heating method relied on the original manual controls of each modified three-magnetron microwave oven. Power adjustment was performed manually by operating the timer, which regulates the on/off cycles of the magnetron. Typically, this provided 7 or 8 power levels. Temperatures were either recorded by a computer or noted manually, and the heating rate was adjusted manually based on these temperature readings.

The firing curves and power settings were different for the initial firing of raw pieces compared to the second firings for glazing or porcelain.

• First Firing (Raw Pieces): A gradual ramp-up was used, varying from 6 to 10 °C/min up to 200 °C. Power was then increased progressively to full capacity around 600 °C following a ramp-up of about 25 °C/min (Figure 4a). In the large microwave system, heating was achieved through a sequential, stepped power-increase protocol involving three magnetrons. Initially, the first magnetron was activated, and its power was increased progressively until the sample temperature reached 200–250 °C. Subsequently, the second magnetron was engaged, and its power was ramped up until the system achieved 400 °C. Finally, the third magnetron was switched on; it typically reached its full power, and thus the overall maximum system power, when the temperature was around 600 °C. This staged activation minimised thermal shock and ensured controlled heating across the temperature range. From this point, heating was performed at full power without regulation until the maximum temperature was reached. A plateau could then be maintained by readjusting the power.
• Second Firing (Glazing/Porcelain): For small pieces in the small microwave, the power was gradually increased up to 150 °C before switching to full power (Figure 21). In the large microwave, with its larger pieces, the power increase was more gradual, reaching full power around 600 °C over 20 min (Figure 4b).

Cooling was performed naturally by opening the microwave door and removing the first layer of insulation from the oven opening.

Susceptors were placed upright against the walls of the kiln. A typical arrangement involved a long susceptor (7–10 cm) in each corner and a small one (4–6 cm) in the middle of the faces. This amounted to 6 to 7 susceptors, with a total weight of 140–170 g, providing a potential thermal power of 500 to 700 W. For the large kiln, which had a raw piece load of 300 to 700 g, the weight of the susceptors represented 25% to 50% of the total load. The choice of susceptors was made on their size and weight to obtain the best possible heat distribution. Homogeneous susceptor formulations were used in the same firing.

4.2. Material Limitations

The initial difficulty lay in accurately interpreting the thermocouple readings. The literature frequently reports significant temperature gradients between the thermocouple measurement and the temperature experienced by the ceramic part (or measured via alternative methods) [16]. To mitigate this disparity and ensure a more accurate reading of the ceramic temperature, the most effective solution was to place the thermocouple directly inside the piece being fired, when possible, or very close if not.

For firings above 1250–1270 °C in the large oven, a second difficulty arose in finding a material that, for iron-rich susceptors, prevents them from coming into contact with the furnace walls. This material must also be transparent to microwaves and chemically inert with respect to the susceptors. Indeed, the liquids resulting from the partial melting of the iron-rich susceptors react with the silica and alumina content of the insulating refractory material, causing localised melting. This fusion behaviour incidentally confirms that the system was under sufficiently reductive conditions to lower the fusion temperature to approximately 1300 °C, a significant reduction compared to the 1380 °C typically observed under atmospheric oxygen pressure for the SiO₂-FeO-Al₂O₃ system [44].

In this case, while the ceramic pieces were successfully fired without defects, the oven’s insulation is thus damaged at these temperatures around 1300 °C (Figure 22).

4.3. Some Achievements of Large Handicraft Pieces

During this exploration of microwave-fired ceramics, many artisanal pieces were successfully made and fired. While small pieces (less than 7–8 cm) were consistently easy to work and fire, the main challenge in artisanal ceramics is producing larger pieces, commonly up to at least 20 cm in their largest dimension. This study testifies that this could be quickly and successfully accomplished in a microwave oven.

Figure 23 shows a selection of relatively large earthenware pieces fired and glazed using this method. In each case, both firings—the first for the raw, unglazed piece and the second for the glazing—were perfectly executed in terms of both physical quality and the expected colours.

4.3.1. Ceramic Quality

As far as can be judged without proper equipment, the quality of the fired pieces to the touch and appearance seems to have excellent mechanical properties. The quality can also be appreciated by the excellent sound of the pieces, earthenware sounding like porcelain, and by visual assessment carried out by professional ceramists (P. Lemaitre and C. Combes). Two X-ray diffractograms (Figure 24) made on porcelain fired at 1230 °C and earthenware fired at 1005 °C show their excellent crystallinity. In the porcelain, the ratio between mullite and quartz is around 50%, and the high proportion of glass corresponds well to the proportions described in the literature for porcelain sintered at 1250 °C in a microwave oven [20]. For earthenware fired at 1005 °C, the absence of hydrated phases and carbonates, along with the presence of diopside, which appears from gehlinite at 1000 °C and forsterite at 1000 °C [47,48], is consistent with these temperatures.

4.3.2. Glazing Quality

Glazing is a critical step for ceramists, and this work confirms that it can be successfully and quickly accomplished in a microwave kiln, as reported in the literature [23]. Aesthetically, the enamelling produced was of very good quality, achieving the expected effects when applied correctly (Figure 23 and Figure 25).

Tests were conducted to compare the temperatures measured by a thermocouple in the kiln with the glaze manufacturer’s recommendations. The results showed that the acceptable temperature range for a glaze could be extended by 50–100 °C towards lower temperatures without significant changes in colour or texture. The extent of this range depends on the specific glaze, with some being more tolerant than others. For example (Figure 25), crystal turquoise: This glaze, with a recommended range of 1020–1060 °C, showed a consistent appearance between 920 °C and 1010 °C and was already vitreous at 840 °C. Panzy: Recommended for 1020–1100 °C, this glaze did not change its appearance between 960 °C and 1050 °C and was vitreous from 880 °C. Coral Red: This glaze performed best within its recommended temperature range. The behaviour of the glazes was found to be consistent across the three different types of earthenware clay used. These findings support the hypothesis that microwave sintering extends the temperature range transformations to lower temperatures [23].

4.3.3. Time and Energy Saving

In traditional ceramic firing, typically used in the craft sector, the ramp-up lasts between 8 and 11 h in a conventional electric kiln, depending on the materials and uses. In industry, ramp-up times are generally shorter, around 3–4 h, using different processes [46].

In contrast, the firing time of ceramics in a microwave kiln is measured in minutes or in seconds, which is a significant advantage. A typical 3.8 kWh microwave kiln, like the one described, consumes an average of 500 Wh/L for firing earthenware in a 6 L volume to 700 Wh/L for firing porcelain in a 4.8 L configuration (Figure 26). These values are very close to those of the microwave developed by T. Santos and colleagues [23], having a power of 6 kWh for 8 L of useful volume. The consumption relative to the volume in an electric conventional kiln decreases with the volume from around 2400 Wh/L in a 10 L kiln to 500 Wh/L in a 1 m³ one for a complete firing cycle (values calculated from public data of kiln manufacturers and ceramists). Relative to the volume, the energy consumption of a microwave ceramic kiln around 500 to 700 Wh/L is thus equivalent to that of a large conventional electric kiln and significantly lower than that of a small one. This efficiency of a small microwave kiln means that a ceramist does not have to wait, sometimes half a month or more, for a large kiln to be full before firing a single piece. This is particularly beneficial for applications such as on-demand production in tourist areas, for apprenticeship programs where a piece can be fired and completed within a day or two, or for firing unique pieces and conducting tests.

5. Discussion

The primary objective of this study—to demonstrate the feasibility of constructing an easily accessible microwave kiln for artisan ceramic firing—was successfully achieved. The resulting kiln, built from readily available components, is suitably sized for craft production, capable of firing and glazing earthenware, stoneware, and porcelain up to 1280 °C with satisfactory results. Its practical utility is underscored by its efficiency: the ability to fire pieces up to 21 × 21 × 12 cm within hours represents a substantial time and convenience advantage over conventional kilns.

We wish to emphasise from the outset that the developed setup, based on a modified domestic microwave oven, is purely experimental (a proof-of-concept) and was designed to validate the feasibility of a controllable, low-cost sintering process. It is not presented as an industrial prototype. The transition to a commercial application indeed requires serious refinement and optimisation by specialists in microwave engineering and industrial safety, particularly concerning the toxic emissions specific to the use of SiC and the potential SiO gas resulting from its decomposition.

Although the current mechanical and electrical setup requires optimisation—specifically through a centralised, automated control system and better-calibrated power regulation—a strong correlation between heating rate and electrical power suggests that precise control could effectively compensate for potential temperature measurement inaccuracies (Figure 26). However, the temperatures derived from the analysis of mineral reactions on the susceptors did not reveal any inconsistencies with the temperatures measured using thermocouples or optical pyrometry with a commercial device.

Beyond the practical construction, a key scientific challenge was the development of an inexpensive, efficient, and durable susceptor for hybrid microwave heating. This challenge led to the investigation of SiC-Fe₃O₄ composite materials. Optimal compositions were identified, leading to two distinct products: a high-durability susceptor (Fe₃O₄ ≤ 25 wt. % of SiC content) comparable in performance to commercial SiC susceptors; and a highest Fe₃O₄ content one (40 to 50 wt. % of Fe₃O₄) with limited durability but unique redox properties.

The intriguing behaviour of the magnetite-rich susceptors, which exhibited evidence of partial fusion, revealed a significant insight into the material’s function. The physicochemical conditions attained within these susceptors mimic those found in industrial processes like steel slag or ferrosilicon production [38] or in environments with a high reducing power, such as those found in the Earth’s mantle or in meteorites [49,50]. These are characterised by extremely low oxygen environments and liquidus temperatures as low as 1200 °C for the iron-rich Fe-Si-Al-O system.

In the susceptors, Fe₃O₄ acts as a “catalyst”, initiating the reactive sintering of SiC due to its strong microwave absorption. During this process, silicon carbide is consumed and replaced by ferrosilicon and silica as carbon burns away. The synergistic combination of dielectric loss (SiC) and magnetic loss (Fe/ferrosilicon), generated by eddy currents within the metallic cores [51,52], maintains the material’s thermal performance.

Incidentally, the partial melting and subsequent expulsion of molten material and gaseous products from the susceptors in high magnetite variants facilitates an interface between the internal susceptor environment and the furnace atmosphere, allowing the furnace to potentially operate under reducing conditions. While this partial melting compromises long-term durability, the resulting reducing environment is a highly desirable asset for specific ceramic glazes and body compositions [46].

Future research must focus on validating this reducing atmosphere for the whole kiln hypothesis through detailed glaze analysis [23,46]. Furthermore, the observation that the Fe₃O₄ additive enables the reactive sintering of SiC at low temperature (850–950 °C) and low pressure (1 bar) to form a silicate binder represents an incidental but highly promising avenue for developing new, low-energy SiC based material manufacturing processes.

6. Conclusions

This work has demonstrated the possibility for a ceramic artisan or amateur to use a microwave oven to fire earthenware and porcelain up to approximately 1280 °C. The system’s operation is similar to that of a conventional microwave.

With ramp-up firing cycles taking only 1 h, the time savings are considerable. Despite a reduced volume, the energy consumption per object is equivalent to that of a large kiln, offering a flexibility previously unknown in ceramics. This allows for the finished object to be obtained soon after its design.

The process is exceptionally efficient, allowing a ceramist to prepare a piece in the morning, fire it before lunch, and remove it after coffee, thereby demonstrating extraordinary ease of use and a significant time-saving advantage over traditional kilns.

The results and difficulties encountered align with those described in the literature, both in terms of the remarkable quality of the finished products and the challenges in understanding the actual temperature conditions they experienced [23]. It is surprising that, despite a lack of precise temperature and power control, the results were consistently excellent. This suggests that the ceramic piece, rather than the kiln, might be controlling the firing process.

The research conducted to create susceptors from readily available materials led to the development of components with unexpected capabilities. Not only do they provide efficient heating, but they also have the capacity to reduce the atmosphere of the kiln. This latter ability, which still needs to be fully demonstrated on a kiln-wide scale, could represent a new advancement for ceramic firing using electricity.