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Article

Application of Cold Sintering Process for Stabilizing Heavy Metals in Municipal Solid Waste Incineration Fly Ash

Department of Resources Engineering, National Cheng Kung University, Tainan 70101, Taiwan
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Author to whom correspondence should be addressed.
Sustainability 2023, 15(19), 14110; https://doi.org/10.3390/su151914110
Submission received: 30 July 2023 / Revised: 16 September 2023 / Accepted: 18 September 2023 / Published: 23 September 2023
(This article belongs to the Section Pollution Prevention, Mitigation and Sustainability)

Abstract

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Municipal solid waste incineration fly ash (MSWI FA) consists predominantly of compounds comprising elements such as calcium, aluminum, silicon, sodium, and others. Additionally, it encompasses a complex mixture of heavy metals, chlorides, sulfates, organic pollutants, and other constituents. The effective and economically viable treatment of MSWI FA poses a formidable challenge for resource cycling at the current stage. In this research report, we adopt a novel low-temperature sintering method called the “Cold Sintering Process” (CSP) as a means to immobilize heavy metals within the fly ash. By utilizing a Taguchi orthogonal array method, we will adjust five control factors in the CSP, including sintering temperature, uniaxial pressure, sintering time, initial water addition, and sodium carbonate dosage. The leaching of cadmium from the fly ash, as measured by the Toxicity Characteristic Leaching Procedure (TCLP), will serve as the quality indicator of products. Through the application of CSP, MSWI FA was transformed into structurally stable ceramic blocks, and the heavy metals within the blocks were effectively immobilized. The results of the experiments showed that MSWI FA under the conditions of a temperature of 300 °C, uniaxial pressure of 312 MPa, sintering time in 60 min, 25 wt% water addition, and 9 wt% Na2CO3 addition could effectively reduce the leaching of cadmium by 77.71%, lead by 21.14%, zinc by 42.37%, and chromium by 99.99%, as compared to the original MSWI FA TCLP results. The X-ray Diffraction (XRD) results indicate that during the CSP, fly ash forms phases such as calcium silicate, rankinite, hydrogrossular, anorthite, and marilite. These phase transformations are considered beneficial for preventing the leaching of internal heavy metals. Scanning Electron Microscopy-Energy Dispersive X-ray Spectroscopy (SEM-EDS) results reveal that CSP is advantageous for compacting the overall structure, and EDS results further demonstrate that some of the Pb and Zn are carried out from the interior of the blocks, with uneven distribution on the surface of fly ash particles. The aforementioned experimental results serve as preliminary indications of CSP’s capability to stabilize detrimental components within high-purity fly ash. Future research endeavors may entail the refinement of material proportions, modification of experimental parameters, and other methodologies, thus facilitating potential scalability to industrial applications. Such developments align with the overarching goal of resource utilization.

1. Introduction

Incineration is currently considered one of the effective approaches for urban waste management [1]. By subjecting municipal solid waste (MSW) to the incineration process, a substantial reduction in volume and the recovery of energy for electricity generation can be achieved [2], thereby addressing various challenges associated with waste landfilling. Following incineration, the overall waste volume is reduced by 85% to 90%, with a corresponding decrease in mass ranging from 60% to 90% [3]. Additionally, the process generates approximately 15% to 20% of bottom ash (BA) and 3% to 5% of fly ash (FA) [4]. The subsequent management and resource circulation of fly ash residues are a significant concern to be addressed. The main constituents of municipal solid waste incineration fly ash (MSWI FA) are compounds composed of Ca, Si, Al, Cl, Na, K, S, Fe, Mg, and P, among others. Trace elements (<1%) include heavy metal compounds such as Pb, Zn, Cd, Cu, Hg, Cr, Ni, As, and others [3]. The particles of fly ash exhibit irregular shapes, with sizes predominantly ranging from <10 μm to 50 μm [5]. The source of heavy metals in fly ash is the waste itself, and they become associated with the fly ash during the incineration process through the following mechanisms: (1) Volatile forms of heavy metal compounds are released during combustion. (2) These volatiles undergo chemical reactions and become enriched on the surface of the fly ash. (3) The flue gas, along with the particles, enters the air pollution control system. (4) The particles are captured by the air pollution control system [3,5,6,7].
In recent years, research on fly ash treatment can be broadly categorized into three aspects: thermal treatment [8,9], stabilization/solidification (S/S) [10,11], and chemical separation [5,12,13,14]. Thermal treatment and S/S primarily aim to promote overall structural stability through the generation of secondary phases or physical encapsulation, thereby reducing the mobility of internal contaminants [10,15]. Chemical separation, on the other hand, focuses on the separation of target elements using hydrometallurgy techniques [16,17,18]. In 2016, Randall and his research team introduced a novel sintering technique called the Cold Sintering Process (CSP) [19]. This technique requires a temperature below 350 °C, along with the application of uniaxial pressure and pre-wetting of raw powders. Remarkably, within a span of 2 h, highly dense ceramic blocks can be obtained through this method [20,21,22,23]. From the standpoint of incineration fly ash treatment technology, CSP embodies characteristics found in both S/S and thermal treatment techniques (such as sintering and hydrothermal methods). Its ability to operate at lower temperatures and shorter reaction times positions CSP as a promising method for fly ash treatment within the academic and scientific community. However, most studies have focused on utilizing CSP to enhance the electrical properties of ceramic materials by modifying experimental parameters such as sintering time, uniaxial stress, sintering time, and liquid additives [24,25,26]. In this research, our team aims to apply the CSP technique to treat MSWI FA. Through the examination of the stability and immobilization capacity of heavy metal elements in the incineration fly ash after the CSP treatment, this assessment aims to determine the potential for further resource recycling applications of CSP in the future.
Initially, the FA powder undergoes pre-treatment through drying, ball milling, and sieving. Subsequently, the fly ash powder is subjected to CSP experiments based on a Taguchi orthogonal array (L16(45)), where it is sintered into ceramic blocks. The TCLP test is conducted for 18 h to evaluate the leaching of cadmium metal in the products. The leaching amount of cadmium metal in the TCLP test serves as the basis for adjusting the control factor parameters to determine the optimal combination for immobilizing heavy metals within the fly ash. Additionally, XRD and SEM-EDS analysis are employed to further investigate the solidification mechanism.
The primary objective of our study is to utilize CSP as a means to create a novel, high-density material that is environmentally benign. In addition to facilitating the recycling of incineration fly ash, we seek to expand the application of CSP to the treatment of diverse waste materials. This endeavor aligns with our broader commitment to advancing environmental sustainability in the academic sphere.

2. Materials and Methods

2.1. MSWI Fly Ash

The MSWI fly ash utilized in this research was sourced from an incineration facility located in southern Taiwan. To ensure sample homogeneity, grab samples were collected from the bag filter and subsequently mixed in a laboratory micro-blender for 30 s. The coning and quartering method was employed to reduce the sample weight to 2 kg while maintaining representativeness. Subsequently, the fly ash samples were sieved, and the fraction with a diameter smaller than 0.59 mm was collected for use in the subsequent experimental procedures. Preliminary analysis of the fly ash was conducted using XRF (NEX CG, Electron Optics Laboratory, Rigaku, Tokyo, Japan) to determine the elemental composition within the ash. Simultaneously, three sets of fly ash samples, each weighing 0.4 g, were subjected to complete digestion using aqua regia under the conditions of L/S ratio of 50, temperature of 200 °C, and a dwell time of 120 min. Following digestion, the resulting solution was analyzed for its elemental composition using flame atomic absorption spectroscopy (AANALYST-100, Mineral Processing Lab, PerkinElmer, Waltham, MA, USA). The XRF analyses and aqua regia digestion experiments data were combined to determine the relative weight percentages of elements within the fly ash. This combined analysis enabled us to ascertain the respective contributions of each element in the fly ash composition. The crystalline phase composition of fly ash samples were determined using XRD (D8 Advance, ES NCKU, BRUKER, Mannheim, Germany). XRD experiments were conducted using a copper target material with a diffraction angle range of 2-theta = 10–70 degrees. The step size for data collection was 0.03 degrees, and the scanning rate was set at 2 degrees per minute. Surface morphology and initial particle size analysis of the fly ash samples were analysed using SEM (SU-1510 & SU-5000, Core Facility of NCKU, Hitachi, Tokyo, Japan) after Au coating. Moreover, the SEM observations were complemented by laser particle size analysis (BT-9300, Mineral Processing Lab, Bettersize, Dandong, China) to obtain a comprehensive characterization of the particle size distribution of the fly ash samples.

2.2. CSP Pre-Treatment

The main purpose of the CSP pretreatment is to eliminate impurities and oversized aggregates from the fly ash samples, while simultaneously reducing the particle size and narrowing the overall particle size distribution. This pre-treatment process is crucial for facilitating the densification process during the CSP, enabling effective compaction, and enhancing the overall performance of the material. The pretreatment procedure began with the placement of the fly ash in an oven at 70 °C for 24 h, aiming to remove any residual moisture present in the samples. Subsequently, a 24 h ball milling process was applied to reduce its particle size. The milling container used has a volume of 250 cm3, a diameter of 6.2 cm, and contains grinding balls with a diameter of 1 cm and a density of 6 g/cm3. The density of the fly ash was measured using the pycnometer method, with an average value of 2.5 g/cm3 obtained from five measurements. The total weight of the grinding balls is 450 g with a filling ratio of 0.5, while the total weight of the fly ash is 75 g with a filling ratio of 0.2. The rotation speed during milling is 158 revolutions per minute (rpm). To eliminate oversized impurities and agglomerates, the pretreated fly ash was subjected to sieving using 10-mesh (about 1700 microns) and 150-mesh (about 106 microns) screens. These meticulous pretreatment steps were implemented to ensure the effective removal of excess moisture, achieving finer particle size, and eliminating larger impurities and agglomerates from the fly ash samples, ultimately enhancing the quality and suitability of the material for subsequent processing.

2.3. Cold Sintering Process

In this study, we selected five control factors based on relevant literature that may affect the quality of CSP. These factors include A: Sintering temperature, B: Magnitude of uniaxial pressure, C: Sintering time, D: Initial water addition, and E: Fly ash and sodium carbonate addition. The CSP experiments were conducted by gradually heating at a rate of 10 °C per minute while keeping all other factors constant. Before conducting the CSP experiments, the pre-treated fly ash and sodium carbonate were meticulously blended according to the prescribed experimental proportions. The resulting powder mixture was then uniformly wetted with the addition of water and vigorously stirred to achieve homogeneity. The specific procedure for the preparation is illustrated in Figure 1. The prepared CSP slurry obtained from pretreatment was poured into a mold shown in Figure 2b, which has an inner diameter of 2 cm.
The CSP equipment used in this study was custom-designed and assembled, as shown in Figure 2. The mold had an inner diameter of 20 mm and could withstand a maximum uniaxial pressure of 15 tons. The mold heater was capable of ramping up the temperature at a rate of 10 °C per minute and heating up to a maximum temperature of 320 °C.
The CSP can be divided into two stages: stage 1 and stage 2. In stage 1, only uniaxial pressure is applied. At this stage, the uniaxial pressure promotes the reactions between the fly ash particles and the pre-added water. Some substances in the fly ash, such as soluble salts and certain heavy metals were transfered to the liquid phase during this stage. The dissolution of fly ash particles in terms of quantity significantly affects the densification of the subsequent CSP product. Additionally, under the influence of uniaxial pressure, some fly ash particles undergo plastic deformation, and the bulk density of fly ash particles increases compared to the condition that no uniaxial pressure is applied. Upon reaching the specified pressure, stage 2, also known as the heating stage, commences. In this stage, the interplay of temperature, pressure, and water induces the release of more constituents from the fly ash particles into the water. As the temperature surpasses the boiling point of water, evaporation occurs. The originally dissolved substances in the water become supersaturated, precipitating onto the surface of primary fly ash particles and forming a secondary phase. This dissolution–precipitation reaction continues to take place iteratively during stage 2. Finally, with the combined effect of temperature and pressure, all solvents evaporate, resulting in the formation of densely consolidated fly ash blocks.

2.4. Taguchi Method Parameter Optimization

In the absence of sufficient data in the existing literature on CSP for fly ash, we relied on the technical specifications and operating conditions mentioned in the current CSP literature [24,25,26]. Additionally, we take into account similar stabilization techniques applied to fly ash to date, such as Hydrothermal Reaction Sintering [27,28], Cold Sintering [29,30], Hydrothermal Hot Pressing [24,31], and Reactive Hydrothermal Liquid-Phase Densification [32]. Based on those pieces of information, we selected five key control factors and their corresponding levels that have the most significant impact on heavy metal immobilization in CSP for fly ash. To explore the effects of each factor on heavy metal immobilization, we employed the Taguchi method [33], which allowed us to predict the optimal experimental conditions. By combining the knowledge from the existing CSP literature and analogous techniques, we aimed to bridge the knowledge gap and establish a framework for applying CSP on fly ash, specifically focusing on its ability to immobilize heavy metals.
In this study, the L16(45) orthogonal array was employed as the experimental basis for discussing the results of the CSP experiments. The control factors investigated include A: Sintering temperature, B: Uniaxial pressure, C: Sintering time, D: Water addition, and E: Sodium carbonate addition. Each control factor consists of four levels, as shown in Table 1 and Table 2.
The selection of temperature, uniaxial stress, and sintering time was determined with reference to the current literature review on CSP [24,25,26]. In the existing CSP research, several materials are identical to incineration fly ash, and they have achieved relative densities exceeding 80% through the CSP. Previous research has indicated that in the Al2O3-NaCl system, CSP conducted at 120 °C, under a uniaxial pressure of 200 MPa, and with the addition of 4 wt% water, results in the formation of Al2O3-Nacl blocks with a relative density of 96% in just 50 min [34,35]. When combined with temperatures ranging from 80 to 140 °C, uniaxial pressure between 100 and 500 MPa, and 11 wt% water, CSP generates blocks with relative densities exceeding 87% within 10 to 90 min [36]. For CaCO3 (vaterite), it has been observed that by subjecting it to a uniaxial pressure of 280 MPa at room temperature in the presence of 20 wt% water and paraffin oil, CaCO3 blocks with relative densities of 82% and 64% can be achieved in only 30 min [37,38]. For SiO2, previous research has demonstrated that by employing a 20 wt% solution of 5M NaOH under 270 °C and 430 MPa uniaxial pressure, SiO2 blocks with a relative density of 98% can be achieved within 60 min [39]. By reviewing the CSP literature that shares similar compositions with fly ash, we have selected three control factors, namely temperature, uniaxial pressure, and sintering time, along with their respective levels. Regarding solvent addition, our preference is to use water as the primary solvent. Given the complex composition of fly ash, it is challenging to rely on the dissolution characteristics of a single material as a reference. Therefore, we have initiated preliminary tests using water. CSP exhibits a reaction environment akin to the hydrothermal method from the initial temperature ramp-up phase until complete internal moisture evaporation. The significant divergence lies in CSP’s heightened focus on the role of uniaxial mechanical pressure in densification. Some studies, supported by experimentation and simulations, have demonstrated the efficacy of Na2CO3 in conjunction with the hydrothermal method for inhibiting the leaching of internal heavy metals. Consequently, this study incorporates Na2CO3 as an auxiliary additive [40].
After undergoing CSP, the fly ash is transformed into a solidified form. To effectively describe the leaching behavior of heavy metals in fly ash CSP blocks, it is necessary to select one specific heavy metal as the leaching indicator. Common heavy metals found in fly ash, such as Zn, Pb, Hg, Cu, Cr, Cd, and Ni, are all viable choices. Among these heavy metals, Cd [5] and Pb [41] are considered the least stable and are more susceptible to contaminating groundwater. However, due to the amphoteric property, Pb undergoes dissolution–precipitation–secondary-phase formation processes during CSP, which can introduce larger uncertainties and errors for leaching results. Therefore, Cd was ultimately selected as the quality characteristic for the Taguchi experimental design in order to assess the leaching behavior of heavy metals in fly ash CSP blocks. To analyze the data, several techniques were employed, such as calculating the signal-to-noise (S/N) ratio, determining the factor effects, plotting factor effect charts, and adjusting the factor levels to maximize the S/N ratio. Through these approaches, an empirical model was established, and the optimal theoretical experimental parameters for enhancing the heavy metal immobilization capacity during the CSP were determined. Additionally, validation experiments were conducted to compare the calculated values with the actual experimental results and explore the potential reasons for any discrepancies observed.

3. Results and Discussion

3.1. Characteristics of Fly Ashes

The fly ash used in this study, derived from municipal solid waste (MSW), was obtained from the Chengxi Incineration Plant situated in Tainan, Taiwan. The initial phase of the experimental investigation involved a comprehensive analysis aimed at determining the intrinsic properties of the fly ash. Utilizing the XRF technique, an elemental analysis was performed, and the obtained results are presented in Table 3. Subsequently, aqua regia digestion was conducted on the fly ash, followed by elemental analysis using Atomic Absorption Spectrometry (AAS). Table 4 provides an overview of the relative proportions of different elements identified in the fly ash. Table 3 and Table 4 reveal that the dominant constituents of the fly ash are calcium, sodium, and potassium, whereas the contents of heavy metals, such as zinc, lead, copper, chromium, and cadmium, are comparatively lower. Despite the relatively low concentrations of heavy metals in the fly ash, their potential for leaching remains a significant environmental concern.
The XRD analysis conducted on the fly ash sample at room temperature, as illustrated in Figure 1, revealed the predominant crystalline phases present in the fly ash. Figure 3 displays the XRD results of the fly ash. These include NaCl (Halite, PDF#05-0628), SiO2 (Quartz, PDF#46-1045), CaCO3 (Calcite, PDF#05-0586), CaSO4 (Anhydrite, PDF#37-1496), and KCl (Sylvite, PDF#41-1476). Based on the X-ray diffraction (XRD) results, it can be observed that the fly ash used in this study exhibits minimal differences compared to fly ash generated from general municipal waste incineration.
SEM images at different magnifications, as illustrated in Figure 4a,b, depict the surface morphology of fly ash particles in their original state. Figure 4a displays the SEM image of the fly ash sample at 800 times magnification, revealing that conglomerates of larger fly ash particles are composed of numerous smaller particles with sizes ranging approximately in the tens of micrometers. These larger particles exhibit a multi-layered structure and indication of agglomerates rather than individual primary particles. The loose stacking of these large particles suggests a lack of strong bonding between them. The irregular surface topography of these particles results from their formation through the gradual aggregation of acidic high-temperature flue gas (containing heavy metals, organic compounds, etc.) generated during waste incineration and the introduction of alkaline agents in the gas treatment system.
Increasing the SEM magnification to 8000 times in Figure 4b allows for clear visibility of the smaller fly ash particles on the surface of the larger particles. These smaller particles exhibit sizes ranging from approximately 1 to 10 μm and possess a more angular and disordered shape. Previous studies have reported a typical particle size range of 10–50 μm for fly ash, although larger fly ash particles up to 300 μm in size have been observed. The results of laser particle size analysis conducted on the fly ash samples are presented in Figure 5. The D50 value, representing the median particle size, is determined to be 8.24 μm. The particle size distribution of the fly ash sample ranges from approximately 0.67 μm to 34.57 μm, as depicted in the graph. These findings were aligned with the observations from the SEM analysis in Figure 2, providing further evidence of a diverse range of particle sizes present in the fly ash sample.

3.2. Cold Sintering Process Pre-Treatment

In order to enhance the energy efficiency of cold sintering and promote the uniformity of fly ash, a pre-processing step was employed in this study. The fly ash powder underwent a series of treatments, including a 24 h drying process, a 24 h ball milling process, and a two-stage sieving process using 50-mesh and 150-mesh screens. The pre-treated fly ash samples were then subjected to laser particle size analysis and SEM analysis.
Oversized fly ash particles require more energy for densification during the sintering process. Conversely, undersized fly ash particles are prone to move into the gaps between molds during cold sintering, leading to a shortened mold lifespan. SEM images in Figure 6a,b at a magnification of 10,000 times and 30,000 times demonstrate well-defined grain morphology and grain boundaries in the pre-treatment fly ash samples. Notably, the grain edges appear smoother and exhibit reduced angularity compared to the fly ash samples without pre-processing. The sequential treatments of drying, ball milling, and sieving have effectively refined the particle size distribution of the fly ash, resulting in smaller and more uniform particles. The results of SEM analysis further verify the improved surface characteristics of the pre-treated fly ash, suggesting its potential for enhanced performance in various applications. The optimized particle size distribution and refined morphology attained through the pre-processing steps offer promising prospects for the utilization of fly ash in diverse fields.
In cases where the particle size distribution curve exhibits a bimodal distribution, smaller particles can fill the voids between larger particles, facilitating subsequent densification processes. The particle size distribution analysis, as presented in Figure 7, indicates a notable reduction in the D50 value from 8.24 μm to 4.31 μm after the pre-processing steps, representing a decrease of 47.7% in size. Moreover, the particle size distribution range narrowed from 0.67–34.57 μm in the original fly ash sample to 0.31–16.25 μm after the pre-processing.

3.3. Taguchi Experiment and Optimization of Cold Sintering Process

In this study, we employed an L16(45) Taguchi orthogonal array to investigate the effects of five control factors, namely sintering temperature, uniaxial pressure, sintering time, water additives, and sodium carbonate additives, on the immobilization of heavy metals during the CSP. The objective was to determine the optimal conditions for the effective immobilization of heavy metals in the CSP. Table 1 presents the L16(45) Taguchi orthogonal array used in the experimental design, while Table 2 displays the levels of the control factors within the orthogonal array.
The complete results of the L16(45) orthogonal array experiment are revealed in Table 5. The first column, labeled EXP., represents the experiment numbers, comprising 16 sets of different combinations of factor levels. Cd(1), Cd(2), and Cd(3) represent the cadmium concentrations (mg/L) measured in the TCLP solution after the fly ash underwent CSP at specific control factor conditions. The number in parentheses denotes the replicate experiment serial number. The concentration of cadmium in the solution indicates the extent of cadmium leaching and serves as an indicator of the effectiveness of heavy metal immobilization. The Cd AVE. represents the arithmetic average among Cd(1), Cd(2), and Cd(3), and it will be utilized in the subsequent calculations of the factor response table/graph. The symbol Sn represents the standard deviation of Cd(1), Cd(2), Cd(3), and Cd AVE., which is calculated using Equation (1). In this equation, yi represents the quality characteristic, y ¯ represents the average value of the quality characteristic, and n represents the number of individual elements. Unlike the typical formula for standard deviation calculation, Equation (1) uses n as the denominator instead of the more common n − 1. Under this condition, the sample standard deviation tends to be equal to the population standard deviation. However, regardless of the specific calculation method, the standard deviation represents the degree of dispersion of n data points.
S n = i = 1 n ( y i y ¯ ) n
In the Taguchi method, the S/N ratio serves as a quality index, where a higher S/N ratio indicates better quality. In this study, the objective is to minimize the leaching of heavy metals during the TCLP testing, thus adopting the “smaller the better” characteristic for ideal functionality. The S/N ratio calculation for the “smaller the better” characteristic is expressed by Equation (2), where y ¯ represents the mean value and Sn represents the standard deviation.
S / N = 10   l o g ( y ¯ 2 + S n 2 )
Table 6 is the factor response table of the orthogonal array experiment, while Figure 8 displays the factor response graph. The values in Table 6 represent the S/N ratio contributions of each control factor at different levels, calculated based on the data from Table 1 and Table 5. By recording the S/N ratio contributions of each control factor at different levels, the S/N ratio factor response graph can be plotted. Additionally, by subtracting the maximum and minimum values of the S/N ratio contributions for each control factor at different levels, the range values in Table 6 were obtained. These range values indicate the ranking of the impact of each control factor on the S/N ratio.
Results in Table 6 and Figure 8 indicate the ranking of the impact of control factors on the S/N ratio from highest to lowest as follows: sintering temperature, Na2CO3 additives, water additives, sintering time, and uniaxial pressure. Table 7 presents the variability analysis of the experimental results from Table 5.
Table 7 obtained by using analysis of variance (ANOVA) and SS (Sum of Squares) represents the sum of squared differences between each variation vector and the mean. The Total Sum of Squares (SST) is defined as follows:
S S T o t = i = 1 n j = 1 r y i j 2 ( n × r × y ¯ 2 ) = S U M S Q y i j y ¯
where n is the number of columns in the orthogonal array and r is the number of experimental replications. The sum of squares for the factor effects (SSA) can be expressed as:
S S A = n × r L A k = 1 L A ( y A k y ¯ ) 2 = n × r × V A R P ( y A 1 ¯ + y A 2 ¯ + + y L A ¯ )
where LA is the levels of control factor. The sum of squares for error (SSe) can be expressed as:
S S e = i = 1 n S i 2 × ( r 1 )
The definition of degrees of freedom (DOF) is that for a set of x samples, when x independent pieces of information can be provided, DOF = x − 1. The total degrees of freedom (DOFT) can be expressed as:
D O F T o t = n × r 1
The degrees of freedom for factor A (DOFA) can be expressed as:
D O F A = L A 1
The degrees of freedom for error (DOFe) can be expressed as:
D O F e = n × ( r 1 )
Variance is defined as the SS divided by the DOF. Taking the square root of this value yields the standard deviation. The relationship between these three measures can be summarized as follows:
V A R = S S D O F = S 2
When the number of sample approaches infinity, the F-value tends to approach 1. In finite samples, a larger F-value indicates that the numerator and denominator come from a smaller probability space within the sample, indicating a stronger impact of the factor effect. In practice, the F-value can be calculated as:
F = m S Z 2 S y 2 = ( S S A D O F A ) / V T o t
The denominator ( S y 2 ) represents the total variance (VT = ST2) calculated from the original sample. The numerator ( S Z 2 ) is the variance estimated from the “sample means” and multiplied by the factor m, obtained from the unaveraged original sample variance. By calculating the magnitude of the F-value, we can make preliminary judgments about the size of the effect of the factor. Furthermore, using a probability function, we can calculate the probability of obtaining an F-value greater than the observed F-value. The calculation can be achieved as follows:
P r o b a b i l i t y = F D I S T ( F ,   D O F Z ,   D O F y )
DOFz represents the degrees of freedom for the numerator in the F-value calculation. It is equal to the total number of sample (n) divided by the factor m, minus 1. DOFy represents the degrees of freedom for the denominator in the F-value calculation.
Its purpose is to validate the correctness of the ranking of control factor impacts in the S/N factor response table/graph and to examine the significance of control factors in immobilizing heavy metals (whether they have a significant impact or not). The results of the variability analysis in Table 7 confirm that the ranking of control factor impacts in Table 6 and Figure 8 is correct. Furthermore, by maximizing the S/N ratio, the optimal conditions for fly ash CSP in immobilizing heavy metals can be predicted as follows: sintering temperature: level 4 (300 °C); uniaxial pressure: level 2 (10 tons); sintering time: level 2 (60 min); water additives: level 4 (25 wt%); Na2CO3 additives: level 4 (9 wt%). Additionally, an additive model can be utilized to calculate the S/N ratio and theoretical values of the quality characteristic for the optimal CSP conditions. A comparison can then be made between the calculated values and the actual experimental data.
After identifying the optimal conditions for CSP in immobilizing heavy metals using the Taguchi method, it is necessary to conduct confirmation experiments. These experiments involve comparing the actual experimental values obtained under the optimal CSP conditions with the theoretical values calculated using the additive model. This comparison aims to assess the accuracy and reliability of the empirical model in predicting the response variable. Table 8 presents a comparison between the additive model calculated values and the average experimental values obtained from triple replications under the optimal CSP conditions for both the quality characteristic and the S/N ratio. In terms of the quality characteristic, which represents the cadmium leaching concentration of the CSP-treated fly ash blocks after 18 h of TCLP testing, there is a difference of 0.085 mg/L between the experimental values and the additive model calculated values. For the S/N ratio, there is a difference of 0.615 dB. The slight differences between the additive model theoretical values and the experimental values can be attributed to several possible reasons identified by our team. Firstly, it is possible that certain control factors with significant effects were overlooked during the initial selection process. For example, the inclusion of more effective solid additives or solution additives that facilitate the CSP might have improved the results. Secondly, there may be interactions among the existing control factors that were not accounted for, leading to deviations in the predictions of the empirical model. Finally, there could be noise factors present in the experimental conditions of the existing control factors that cannot be ignored, contributing to the observed discrepancies.
Based on the results from the factor response graphs/tables and the variance analysis, it can be observed that under the current selection of control factors and their respective levels, the optimal CSP conditions (sintering temperature: 300 °C; uniaxial pressure: 10 tons; sintering time: 60 min; water additives: 25 wt%; Na2CO3 additives: 9 wt%) still demonstrate a relatively good effect in immobilizing cadmium. Additionally, within a certain range, the empirical model can be used to make predictions for the response variable with reasonable accuracy.
Triple replicate cold sintering experiments were conducted using the optimal CSP conditions for fly ash, and the resulting sintered blocks were subjected to TCLP testing, along with the original fly ash sample. The results are shown in Table 9. In this study, cadmium was used as an indicator for the leaching concentration of heavy metals. The results indicate that under the optimal CSP conditions, there was a significant reduction in the leaching concentrations of cadmium (77.71%), lead (21.14%), zinc (42.37%), and chromium (99.99%) compared to the original fly ash sample. It is noteworthy that lead, zinc, and chromium, despite being heavy metals, exhibited different outcomes under the same solidification conditions. Based on the compositional analysis results in Table 3 and Table 4, it can be inferred that the high initial content of lead and zinc in the fly ash compared to cadmium and chromium may have exceeded the solidification limits of CSP, or there might have been certain factors during the CSP that hindered the effective solidification of lead and zinc.

3.4. Analysis of Properties and Solidification Mechanism of Fly Ash CSP Blocks

The fly ash ceramic blocks were prepared under the optimal conditions of CSP at a temperature of 300 °C, a uniaxial pressure of 10T, sintering time 60 min, water additives of 25 wt%, and a sodium carbonate (Na2CO3) addition of 9 wt% are shown in Figure 9, along with the XRD analysis results of the fly ash sample. The main phases identified in the fly ash include halite (NaCl, PDF#05-0628), quartz (SiO2, PDF#46-1045), calcite (CaCO3, PDF#05-0586), anhydrite (CaSO4, PDF#37-1496), gypsum (CaSO4·2H2O, PDF#33-0311), and sylvite (KCl, PDF#41-1476). During the CSP, where multiple factors such as temperature, pressure, time, and liquid composition are simultaneously involved, the peak intensities of NaCl and KCl gradually decrease, while new phases such as calcium silicate (Ca2SiO4, PDF#31-0302), rankinite (Ca3Si2O7, PDF#22-0539), hydrogrossular (Ca3Al2(SiO4)2(OH)2, PDF#420570), anorthite (Ca(Al2Si2O8), PDF#86-1716), and marilite ((Na,Ca)2(Si,Al)6(O,OH)12(Cl,CO3)0.5, PDF#31-1279) begin to appear. Based on the formation of secondary phases observed in Figure 9 and the effectiveness of heavy metal immobilization of fly ash under the optimal CSP conditions shown in Table 9, it can be inferred that the secondary phases generated during the CSP have the ability to inhibit the leaching of internal heavy metals during the TCLP test to some extent.
Under the combined influence of temperature, pressure, time, liquid composition, and sodium carbonate addition, the overall structure during the CSP exhibits a high level of densification. Figure 10a illustrates the sintered blocks of fly ash under the optimal CSP conditions, as observed by SEM at a magnification of 10,000 times. Compared to the untreated fly ash sample in Figure 6, the overall structure shows a significant improvement in bulk density, with some small pores visible on the surface connecting to the interior. From a CSP perspective, these small pores are likely remnants of water evaporating from the blocks at temperatures above the boiling point during the CSP. In Figure 11a at the top left corner, it is evident that the fly ash ceramic blocks produced under the optimal CSP conditions display sharp fracture surfaces with distinct angular features. This indicates that the crystals produced possess specific growth directions during the crystallization process, indirectly supporting the presence of secondary phases observed in the XRD results. Figure 11b reveals the intertwined growth patterns within the internal structure of the fly ash after undergoing the optimal CSP conditions. This suggests that when the fly ash sample is mixed with sodium carbonate and water, and subjected to the entire CSP, reactions such as dissolution, precipitation, and the formation of new secondary phases occur between the fly ash particles. As a result, a dense and mutually enclosed structure is formed.
The SEM images captured in Figure 12 clearly reveal the presence of cavities at the bottom center of the image, which are formed when water escapes from the fly ash ceramic blocks under high temperatures and pressures. Upon examining the distribution of various elements on the surface of the blocks, it is evident that the concentrations of zinc and lead are relatively non-uniform, with significantly higher concentrations observed in the vicinity of the cavities at the bottom of the image. This suggests that during the CSP, a portion of the lead and cadmium present in the fly ash dissolves in the added water. As the water gradually leaves the fly ash blocks under high temperature and pressure, these elements are transported to the surface of the blocks, resulting in poor solidification efficiency.
This phenomenon may be attributed to the fact that both zinc and lead are amphoteric metals. When the fly ash initially combines with water, the resulting solution exhibits strong alkalinity with a pH above 10. Consequently, lead, zinc, and other soluble substances are leached out together.
Figure 13 depicts the elemental distribution of zinc (Zn), lead (Pb), cadmium (Cd), and chromium (Cr) in the cross-section of the fly ash ceramic blocks under the optimal CSP conditions, as measured by EDS. In Figure 13, the SEM image, the distribution of zinc, lead, cadmium, and chromium elements appears to be more uniform compared to the surface of the blocks.
Based on the comprehensive analysis of XRD, SEM, and EDS results, the mechanism of internal heavy metal immobilization in fly ash through the CSP is illustrated in Figure 14. Prior to the CSP initiation, when pre-processed, fly ash is mixed with sodium carbonate, water, and other additives (Figure 1); certain substances on the surface of fly ash particles dissolve into the water, including some heavy metals. As CSP progresses, uniaxial stress is applied to the entire system, causing the fly ash particles to undergo mutual compression and plastic deformation, resulting in densification of the overall structure. Simultaneously, compared to the non-pressurized state, more surface substances of the fly ash particles dissolve. As the temperature increases, along with the applied uniaxial stress, more surface substances of the fly ash particles transfer to the liquid phase (resembling a pressurized leaching effect), where water plays a crucial role in mass transfer. As the temperature rises above the boiling point of water, water gradually evaporates from the interior of the blocks, leading to an increase in pH and the migration of some heavy metals from the interior to the surface of the blocks. Substances originally dissolved in the water (including heavy metals and soluble salts) become supersaturated due to water evaporation and precipitate between the fly ash particles. Simultaneously, under the influence of thermal and mechanical energy, phase transformations occur at the grain boundaries of the fly ash particles, resulting in the formation of stable secondary phases that encapsulate the precipitated heavy metals at the grain boundaries, thus reducing the leaching of heavy metals in the TCLP test. However, heavy metals carried to the surface of the blocks during the evaporation process are less effectively encapsulated by the newly formed secondary phases (such as lead and zinc) compared to those within the blocks, resulting in lower immobilization effectiveness.
In recent years, there has been a considerable body of literature reviewing the treatment methods and solidification mechanisms for MSWI fly ash [42,43,44]. These studies provide valuable insights into the potential application of CSP in fly ash treatment. Regarding thermal treatment, some literature has indicated that fly ash vitrification entails processes such as dehydration (100–200 °C), polymorphic transition (480–670 °C), and fusion (1100–1250 °C) [45]. The XRD results from our study (Figure 9) demonstrate that CSP results in the formation of numerous secondary phases in fly ash. This suggests that CSP can achieve similar effects to traditional thermal treatment but with lower energy consumption.
Whether fly ash can reach the vitrification stage during thermal treatment depends on its composition (or additives). Alkaline oxides (e.g., MgO, CaO) and acidic oxides (e.g., SiO2, P2O5) can affect the melting temperature. In future fly ash CSP research, it may be beneficial to consider adding alkaline oxides as flux agents in the formulation to enhance solidification. Additionally, during the vitrification process, internal substances in fly ash can enter pre-existing crystalline phases or substitute atoms in the lattice [46,47]. The XRD pattern in Figure 9, showing marilite ((Na,Ca)2(Si,Al)6(O,OH)12(Cl,CO3)0.5), is an example of atomic substitution, indicating that this solidification mechanism is operational in CSP.
Moreover, the existing literature suggests that environments with elevated chloride content may facilitate the formation of chloride compounds, posing challenges for the stabilization of Cd, Pb, and Zn through thermal treatment techniques [48,49]. The EDS results align with this observation, with Pb and Zn signals on the surface of fly ash blocks showing more pronounced irregularities compared to the cross-sectional analysis. It is postulated that the high concentration of chloride ions within the fly ash leads to the formation of chloride compounds, which are subsequently transported to the exterior during the CSP through water evaporation. Future scholarly investigations in CSP may benefit from preliminary measures to eliminate chloride ions from the fly ash interior, ultimately enhancing the efficacy of the solidification process.

4. Conclusions

This study employed CSP to effectively immobilize heavy metals present in fly ash by incorporating them into the subsequently formed secondary phases, such as calcium silicate, rankinite, hydrogrossular, anorthite, and marilite. The CSP technique resulted in a significant reduction in the leaching concentrations of cadmium, lead, zinc, and chromium in fly ash by 77.71%, 21.14%, 42.37%, and 99.99%, respectively, thereby ensuring compliance with the TCLP regulatory limits.
To determine the optimal CSP conditions for minimizing the leaching of heavy metals, the Taguchi method was employed. The identified optimal conditions included a temperature of 300 °C, pressure of 10T (312 MPa), time of 60 min, liquid ratio of 25 wt%, and sodium carbonate content of 9 wt%. These conditions facilitated effective heavy metal immobilization, particularly for cadmium and lead. Furthermore, the experimental model developed using the L16(45) orthogonal array was validated, revealing good predictability for cadmium leaching but some discrepancy for lead leaching. SEM-EDS analysis of the surface of CSP-treated fly ash blocks exhibited irregular particle morphology with distinct angular structures. Pore features were observed on the block surface, attributed to the evaporation of water during the CSP. EDS analysis indicated significantly higher concentrations of lead and zinc in the vicinity of these pores, while no notable differences were observed for cadmium and chromium. The internal structure of the blocks displayed a spotted pattern, demonstrating a uniform distribution of elements.
At present, the application of CSP in fly ash treatment is still in its nascent stages. However, the results of this study underscore the promising potential of CSP technology in this context. CSP exhibits the advantages of low energy consumption and short processing times, allowing it to achieve outcomes akin to traditional thermal treatment methods. Future research avenues may explore the incorporation of alkaline oxides to further enhance vitrification during the CSP. The elevated concentration of chloride ions in fly ash poses challenges for the stabilization of heavy metals such as Cd, Pb, and Zn, suggesting the introduction of dechlorination steps before CSP.
In summation, CSP technology represents a novel pathway for ceramic materials and, if effectively leveraged for its unique attributes, holds significant promise for the future of waste materials like fly ash within the domain of resource recycling.

Author Contributions

Conceptualization, S.-K.L. and Z.-E.W.; methodology, Z.-E.W. and Y.-H.S.; scrub data and maintain research data, Z.-E.W. and S.-K.L.; Formal analysis, Y.-H.S. and Z.-E.W.; Supervision, Y.-H.S.; Validation, Z.-E.W. and S.-K.L.; Visualization, Z.-E.W. and Y.-H.S.; Writing—original draft, Z.-E.W. and S.-K.L.; Writing—review & editing, Y.-H.S. All authors have read and agreed to the published version of the manuscript.

Funding

This research received no external funding.

Institutional Review Board Statement

Not applicable.

Informed Consent Statement

Not applicable.

Data Availability Statement

No new data were created.

Acknowledgments

We express our gratitude to Che-Hao Lin and the research team members from the College of Intelligent Semiconductor and Sustainable Manufacturing at National Cheng Kung University for their valuable assistance in SEM imaging. We also extend our thanks to Yu-Hsien Lee and the research team members from the Institute of Resource Engineering at National Cheng Kung University, as well as the Department of Earth Sciences, for their kind support in XRD analysis.

Conflicts of Interest

The authors declare no conflict of interest.

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Figure 1. Steps for fly ash CSP material preparation.
Figure 1. Steps for fly ash CSP material preparation.
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Figure 2. CSP experimental setup: (a) Overall view of the CSP equipment. (b) Customized mold used for CSP. (c) Mold heater.
Figure 2. CSP experimental setup: (a) Overall view of the CSP equipment. (b) Customized mold used for CSP. (c) Mold heater.
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Figure 3. XRD analysis of MSWI fly ash sample.
Figure 3. XRD analysis of MSWI fly ash sample.
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Figure 4. SEM secondary electron images of MSWI fly ash samples (a) 800× (b) 8000×.
Figure 4. SEM secondary electron images of MSWI fly ash samples (a) 800× (b) 8000×.
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Figure 5. Laser particle size analysis of fly ash samples.
Figure 5. Laser particle size analysis of fly ash samples.
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Figure 6. SEM secondary electron images of MSWI fly ash samples after the CSP pre-treatment (a) 10,000× (b) 30,000×.
Figure 6. SEM secondary electron images of MSWI fly ash samples after the CSP pre-treatment (a) 10,000× (b) 30,000×.
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Figure 7. Laser particle size analysis results of pre-treated samples.
Figure 7. Laser particle size analysis results of pre-treated samples.
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Figure 8. S/N ratio factor response graphic.
Figure 8. S/N ratio factor response graphic.
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Figure 9. XRD diffraction results of fly ash sample and fly ash under the optimal CSP conditions.
Figure 9. XRD diffraction results of fly ash sample and fly ash under the optimal CSP conditions.
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Figure 10. SEM secondary electron images of fly ash blocks surface under the optimal CSP condition (a) 10,000× (b) 50,000×.
Figure 10. SEM secondary electron images of fly ash blocks surface under the optimal CSP condition (a) 10,000× (b) 50,000×.
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Figure 11. SEM secondary electron images of fly ash bulk cross-section under the optimal CSP condition (a) 4500× (b) 50,000×.
Figure 11. SEM secondary electron images of fly ash bulk cross-section under the optimal CSP condition (a) 4500× (b) 50,000×.
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Figure 12. EDS analysis result of fly ash bulk surface under the optimal CSP condition.
Figure 12. EDS analysis result of fly ash bulk surface under the optimal CSP condition.
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Figure 13. EDS analysis result of fly ash bulk cross-section under the optimal CSP condition.
Figure 13. EDS analysis result of fly ash bulk cross-section under the optimal CSP condition.
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Figure 14. The schematic diagram illustrates the mechanism and process of heavy metal immobilization in fly ash through the CSP.
Figure 14. The schematic diagram illustrates the mechanism and process of heavy metal immobilization in fly ash through the CSP.
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Table 1. L16(45) Four-level orthogonal array.
Table 1. L16(45) Four-level orthogonal array.
ABCDE
EXP.Sintering TemperatureUniaxial PressureSintering TimeWater AdditivesNa2CO3
Additives
111111
212222
313333
414444
521234
622143
723312
824421
931342
1032431
1133124
1234213
1341423
1442314
1543241
1644132
Table 2. Different levels of control factors in the L16(45) orthogonal array.
Table 2. Different levels of control factors in the L16(45) orthogonal array.
Sintering TemperatureUniaxial PressureSintering TimeWater AdditivesNa2CO3
Additives
Level 1150 °C7.5 T (234 MPa)30 min10 wt%3 wt%
Level 2200 °C10 T (312 MPa)60 min15 wt%5 wt%
Level 3250 °C12.5 T (390 MPa)90 min20 wt%7 wt%
Level 4300 °C15 T (468 MPa)120 min25 wt%9 wt%
Table 3. MSWI fly ash XRF composition analysis results.
Table 3. MSWI fly ash XRF composition analysis results.
ElementsCaNaKZnPbCuCrCd
wt%58.3921.3510.716.232.590.510.150.06
Table 4. Analysis results of fly ash digestion in aqua regia solution.
Table 4. Analysis results of fly ash digestion in aqua regia solution.
ElementsCaNaKZnPbCuCrCd
AAS value
(mg/L)
2925.9581052.503539.745275.27101.95220.0759.6143.597
Ratio between elements (wt%)59.37%21.35%10.95%5.59%2.07%0.41%0.20%0.07%
Table 5. Experimental results of FA CSP using L16(45) orthogonal array.
Table 5. Experimental results of FA CSP using L16(45) orthogonal array.
EXP.Cd(1)Cd(2)Cd(3)Cd AVE.SnS/N Ratio
11.7931.8591.8921.8480.050−5.337
21.5951.6171.541.5840.040−3.998
31.5951.3641.3751.4440.130−3.231
41.2761.2541.1661.2320.058−1.822
51.0561.0781.0561.0630.013−0.534
61.1991.1881.2431.210.029−1.658
71.541.6831.4631.5620.112−3.896
81.5511.6391.8811.6900.171−4.604
91.2321.11.2981.210.101−1.686
101.2981.3971.2981.3310.057−2.492
111.0561.0121.1221.0630.055−0.545
121.0781.1551.0561.0960.052−0.809
131.0231.0780.9021.0010.090−0.044
140.8141.0450.8140.8910.1330.906
151.0451.0450.7920.9610.1460.249
161.0781.0230.9021.0010.090−0.044
AVE.1.2620.083−1.846
Cd(1), Cd(2), Cd(3), Cd AVE. are quality characteristic, unit: mg/L. Sn is the standard deviation.
Table 6. S/N ratio factor response table.
Table 6. S/N ratio factor response table.
CdSintering TemperatureUniaxial PressureSintering TimeWater AdditivesNa2CO3
Additives
Level 1−3.597−1.900−1.896−2.284−3.046
Level 2−2.673−1.810−1.273−2.298−2.406
Level 3−1.383−1.856−1.976−1.575−1.435
Level 40.267−1.819−2.240−1.229−0.499
Range3.8640.0900.9671.0692.547
Rank15432
Unit of S/N ratio: dB.
Table 7. Analysis of variance results for L16(45) orthogonal array experiment.
Table 7. Analysis of variance results for L16(45) orthogonal array experiment.
FACTORSSDOFVarFProbabilityConfidence LevelRank/Significant *?
sintering temperature2.17530.7258.5380.152%99.85%1/Y
uniaxial pressure0.00630.0020.02399.522%0.48%5/N
sintering time0.12730.0420.50068.807%31.19%4/N
water additives0.32930.1101.29331.305%68.70%3/N
Na2CO3 additives1.07430.3584.2152.383%97.62%2/Y
Error0.283320.0089* At least 97% confidence
TOTAL3.992470.085S = 0.094
Table 8. Comparison of quality characteristics, S/N ratio calculated values, and experimental values for the optimal CSP conditions.
Table 8. Comparison of quality characteristics, S/N ratio calculated values, and experimental values for the optimal CSP conditions.
CdAdditive Model Calculation ValueExperimental Values
quality characteristic (mg/L)0.6870.772
S/N ratio (dB)2.8422.227
Table 9. Comparison of TCLP results of CSP optimal conditions and FA sample.
Table 9. Comparison of TCLP results of CSP optimal conditions and FA sample.
CdPbZnCr
FA sample3.2392.66331.9150.589
CSP optimal condition0.7722.10018.3920.000
Percentage Increase/Decrease−77.71%−21.14%−42.37%−99.99%
Unit: mg/L.
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Liao, S.-K.; Wu, Z.-E.; Shen, Y.-H. Application of Cold Sintering Process for Stabilizing Heavy Metals in Municipal Solid Waste Incineration Fly Ash. Sustainability 2023, 15, 14110. https://doi.org/10.3390/su151914110

AMA Style

Liao S-K, Wu Z-E, Shen Y-H. Application of Cold Sintering Process for Stabilizing Heavy Metals in Municipal Solid Waste Incineration Fly Ash. Sustainability. 2023; 15(19):14110. https://doi.org/10.3390/su151914110

Chicago/Turabian Style

Liao, Shih-Kai, Zhong-En Wu, and Yun-Hwei Shen. 2023. "Application of Cold Sintering Process for Stabilizing Heavy Metals in Municipal Solid Waste Incineration Fly Ash" Sustainability 15, no. 19: 14110. https://doi.org/10.3390/su151914110

APA Style

Liao, S.-K., Wu, Z.-E., & Shen, Y.-H. (2023). Application of Cold Sintering Process for Stabilizing Heavy Metals in Municipal Solid Waste Incineration Fly Ash. Sustainability, 15(19), 14110. https://doi.org/10.3390/su151914110

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