Study on the Microscale Mechanisms of Multi-Source Solid Waste Synergy in Enhancing Physicochemical Properties of Red Mud-Based Backfill Materials
Abstract
:1. Introduction
2. Materials and Methods
2.1. Materials
2.2. Experimental Procedure
2.3. Experimental Methods
2.3.1. Uniaxial Compressive Strength Test
2.3.2. Microstructure Characterization
2.3.3. Environmental Performance Test
3. Results and Discussion
3.1. Physicochemical Performance Analysis
3.1.1. Compressive Strength Analysis
3.1.2. Energy Evolution Patterns
- (1)
- Initial damage stage (OA). The dissipated energy increases nonlinearly with deformation, primarily due to the closure of micropores and internal friction within the specimen. Both the input energy and elastic energy also increase with deformation, but the elastic energy remains lower than the dissipated energy during this stage. As the micropores close, the growth rate of the elastic strain energy begins to accelerate. The specimen transitions into the stable damage stage when the elastic strain energy equals the dissipated energy (after the intersection point of the curves). Therefore, the point where the dissipated energy equals the elastic energy can be regarded as the boundary between the initial damage stage and the stable damage stage.
- (2)
- Stable damage stage (AB). After the intersection point of the dissipated energy and elastic strain energy curves, the specimen enters the stable damage stage. During this stage, as the micropores are further compacted and internal friction continues, the dissipated energy curve increases approximately linearly. Both the total energy and elastic strain energy increase at the same rate, with their growth rates exceeding that of the dissipated energy. This stage is primarily characterized by the accumulation of elastic strain energy.
- (3)
- Stationary damage stage (BC). As the micropores become fully compacted, the specimen enters the stationary damage stage. During this stage, the dissipated energy remains nearly constant, and its evolution curve appears approximately horizontal. At this point, the micropores in the rock sample are completely closed, and almost no new dissipated energy is generated. As a result, the slope of the dissipated energy evolution curve is minimal (close to zero). Meanwhile, both the total energy and elastic energy continue to increase at an accelerated rate as the rock sample is further compacted, with their growth trends remaining consistent. In this stage, the energy input into the rock sample is primarily converted into elastic energy.
- (4)
- Accelerated damage stage (CD). As the deformation of the fractured rock sample increases, internal cracks begin to propagate and new cracks form, leading to the dissipation of the elastic strain energy stored in the rock sample. During this stage, the growth rate of the dissipated energy gradually increases (indicated by the rising slope of the dissipated energy evolution curve), while the growth rate of the elastic strain energy gradually decreases (indicated by the declining slope of the elastic strain energy evolution curve). As the specimen reaches its maximum compressive strength, the total input energy essentially peaks, and the elastic strain energy stored in the rock sample reaches its limit. At this point, the damage evolution of the fractured rock mass enters the failure stage.
- (5)
- Damage failure stage (DE). After the rock sample reaches its peak strength, the damage evolution of the specimen enters the damage failure stage. During this stage, the dissipated energy evolution curve exhibits a sharp and sudden increase, while the elastic strain energy evolution curve shows a sharp and sudden decrease, and the total energy remains essentially constant. The further propagation and interconnection of cracks in the fractured rock mass cause the specimen to ultimately lose its load-bearing capacity. The elastic strain energy accumulated in the rock sample is rapidly released in the form of dissipated energy, resulting in a sharp increase in the dissipated energy curve and a sharp decrease in the elastic strain energy curve [48].
3.2. Microstructure Analysis
3.2.1. Analysis of Hydration Product Phases
3.2.2. Chemical Bond Analysis of Hydration Products
3.2.3. Pore Structure Analysis
3.2.4. Micro Morphology Analysis
3.3. Economic and Environmental Impacts
3.4. Mechanism Analysis
4. Conclusions
- (1)
- RFDC6 exhibits excellent mechanical properties at different curing ages. The compressive strength of the material increases by 80.0% from 3 days to 28 days. Particularly at the 28-day curing age, due to the high integrity of the specimen and fewer microcracks, it demonstrates higher rigidity and can more effectively absorb and dissipate energy during the damage process. Its compressive strength is significantly higher than that of other systems. RFCC6 performs well in early strength improvement, but the compressive strength of the material only increases by 18.0% from 3 days to 28 days. At the 28-day curing age, its compressive strength improvement is limited, primarily enhancing the elastic properties of the material, which helps maintain the integrity of the filling structure and prevent structural collapse due to local overload. RFSC6 shows lower mechanical properties than the RFC reference system at different curing ages. Although the compressive strength of the material increases by 36.7% from 3 days to 28 days, at the 28-day curing age, its input energy, elastic energy, and dissipated energy are generally low. The insufficient energy absorption and load-bearing capacity, along with the lower overall structural integrity, result in less ideal mechanical performance.
- (2)
- Through microscopic analysis, it can be observed that the main hydration products of red mud-based filling materials include C(-A)-S-H gel and ettringite. These products interweave and adsorb to form a dense structural network, which is the primary factor contributing to the improvement in the material’s mechanical properties. In the RFDC6 system, the synergistic effect of SO42− promotes the generation of more C(-A)-S-H gel and ettringite, filling the internal pore structure of the material and enhancing its density. This transforms larger pores into smaller gel pores, making the pore structure more complete and more conducive to improving compressive strength. In the RFCC6 system, the increase in OH− concentration promotes the early formation of C(-A)-S-H gel. This gel fills the pores, converting larger pores into larger capillary pores. However, due to the limited solid phase content, the material’s density does not significantly improve, but the substantial gel content significantly enhances the material’s elastic properties. In the RFSC6 system, there is a considerable amount of unreacted raw materials. Carbonate precipitates are formed due to the carbon capture capability of steel slag, and there are gaps between the unreacted raw materials and the hydration products. The internal structure of the material is relatively fragmented, lacking a complete load-bearing structure, which results in a decline in various properties.
- (3)
- By testing the leachate of materials from each system, it can be observed that the heavy metal ion concentrations in the leachate of red mud-based filling materials all comply with the limits specified in the “GB 8978-1996 Integrated Wastewater Discharge Standard”. The synergistic effects of desulfurized gypsum, carbide slag, and steel slag with red mud effectively immobilize heavy metal ions in red mud-based filling materials, demonstrating excellent environmental performance.
Author Contributions
Funding
Institutional Review Board Statement
Informed Consent Statement
Data Availability Statement
Conflicts of Interest
References
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Components (Wt%) | Fe2O3 | Al2O3 | SiO2 | Na2O | TiO2 | CaO | SO3 | P2O5 | K2O |
---|---|---|---|---|---|---|---|---|---|
RM | 49.84 | 19.33 | 12.20 | 8.53 | 7.93 | 0.87 | 0.55 | 0.19 | 0.16 |
FA | 8.60 | 28.15 | 38.79 | 0.24 | 1.84 | 17.16 | 3.02 | 1.06 | 1.14 |
DG | 0.00 | 0.03 | 0.04 | 0.06 | 0.00 | 49.19 | 50.64 | 0.00 | 0.00 |
CS | 1.45 | 3.93 | 3.53 | 0.00 | 0.00 | 88.75 | 1.51 | 0.83 | 0.00 |
SS | 31.83 | 6.23 | 21.20 | 3.26 | 1.79 | 25.66 | 3.68 | 2.13 | 4.22 |
PC | 3.35 | 4.22 | 16.15 | 0.21 | 0.42 | 68.77 | 3.41 | 0.08 | 0.67 |
Sample | RM | FA | DG | CS | SS | PC |
---|---|---|---|---|---|---|
RFC | 70 | 20 | - | - | - | 10 |
RFDC4 | 67.2 | 19.2 | 4 | - | - | 9.6 |
RFDC6 | 65.8 | 18.8 | 6 | - | - | 9.4 |
RFDC8 | 64.4 | 18.4 | 8 | - | - | 9.2 |
RFCC4 | 67.2 | 19.2 | - | 4 | - | 9.6 |
RFCC6 | 65.8 | 18.8 | - | 6 | - | 9.4 |
RFCC8 | 64.4 | 18.4 | - | 8 | - | 9.2 |
RFSC4 | 67.2 | 19.2 | - | - | 4 | 9.6 |
RFSC6 | 65.8 | 18.8 | - | - | 6 | 9.4 |
RFSC8 | 64.4 | 18.4 | - | - | 8 | 9.2 |
Sample | Compressive Strength/MPa | |||||
---|---|---|---|---|---|---|
3 d | Rangeability/% | 7 d | Rangeability/% | 28 d | Rangeability/% | |
RFC | 2.65 | - | 2.73 | - | 3.72 | - |
RFDC4 | 3.76 | 41.9% | 4.66 | 70.7% | 6.82 | 83.3% |
RFDC6 | 4.09 | 54.3% | 6.36 | 133.0% | 7.36 | 97.8% |
RFDC8 | 3.48 | 31.3% | 4.38 | 60.4% | 5.62 | 51.1% |
RFCC4 | 2.56 | −3.4% | 2.98 | 9.2% | 3.14 | −15.6% |
RFCC6 | 3.66 | 38.11% | 4.00 | 46.5% | 4.32 | 16.1% |
RFCC8 | 3.07 | 15.85% | 3.24 | 18.7% | 3.63 | −2.4% |
RFSC4 | 2.33 | −12.1% | 2.52 | −7.7% | 3.26 | −12.4% |
RFSC6 | 2.45 | −7.5% | 2.67 | −2.19% | 3.35 | −9.9% |
RFSC8 | 1.81 | −31.7% | 2.36 | −13.6% | 3.10 | −16.7% |
Sample | RFC | RFDC6 | RFCC6 | RFSC6 |
---|---|---|---|---|
Specific surface area (m2/g) | 21.8451 | 23.8856 | 21.6598 | 21.9245 |
Total pore volume (cm3/g) | 0.099563 | 0.125435 | 0.119396 | 0.111114 |
Average pore size (nm) | 17.5122 | 18.6526 | 19.6011 | 19.4901 |
Sample | Leaching Ion (mg/L) | ||||||
---|---|---|---|---|---|---|---|
As | Pb | Cd | Cr | Cu | Mn | Hg | |
RFC | 0.0173 | 0.0066 | <0.0012 | 0.0817 | 0.069.0 | <0.0036 | 0.0005 |
RFDC6 | 0.0162 | <0.0042 | <0.0012 | 0.0691 | 0.022.6 | <0.0036 | 0.0002 |
RFCC6 | 0.0157 | <0.0042 | <0.0012 | 0.0591 | 0.037.9 | <0.0036 | 0.0003 |
RFSC6 | 0.0169 | 0.0057 | <0.0012 | 0.0535 | 0.010.2 | <0.0036 | 0.0001 |
GB8978-1996 limits | 0.5 | 0.1 | 1.5 | 1.0 | 2.0 | 0.5 | 0.05 |
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Huang, J.; Yan, G.; Kong, S.; Bai, X.; Zhang, J.; Ge, Z. Study on the Microscale Mechanisms of Multi-Source Solid Waste Synergy in Enhancing Physicochemical Properties of Red Mud-Based Backfill Materials. Materials 2025, 18, 1822. https://doi.org/10.3390/ma18081822
Huang J, Yan G, Kong S, Bai X, Zhang J, Ge Z. Study on the Microscale Mechanisms of Multi-Source Solid Waste Synergy in Enhancing Physicochemical Properties of Red Mud-Based Backfill Materials. Materials. 2025; 18(8):1822. https://doi.org/10.3390/ma18081822
Chicago/Turabian StyleHuang, Jinjing, Guochao Yan, Shaoqi Kong, Xuyang Bai, Jiawei Zhang, and Zhiguo Ge. 2025. "Study on the Microscale Mechanisms of Multi-Source Solid Waste Synergy in Enhancing Physicochemical Properties of Red Mud-Based Backfill Materials" Materials 18, no. 8: 1822. https://doi.org/10.3390/ma18081822
APA StyleHuang, J., Yan, G., Kong, S., Bai, X., Zhang, J., & Ge, Z. (2025). Study on the Microscale Mechanisms of Multi-Source Solid Waste Synergy in Enhancing Physicochemical Properties of Red Mud-Based Backfill Materials. Materials, 18(8), 1822. https://doi.org/10.3390/ma18081822