Use of Fly Ash Layer as a Barrier to Prevent Contamination of Rainwater by Contact with Hg-Contaminated Debris
Abstract
:1. Introduction
2. Site Description and Rainwater Contamination
2.1. Abandoned Mercury Mining Facilities
2.2. Precipitation and Evapotranspiration in the Study Area
2.3. Rainwater Contamination
3. Materials and Methods
3.1. Water Balance
3.2. Tests’ Description
3.2.1. Laboratory Tests
3.2.2. Full-Scale Tests in the Abandoned Mine Facilities
- Summary of precipitation, temperature, etc., hour by hour.
- Summary of precipitations, temperatures, etc., of the previous days.
4. Results
4.1. Results of the Tests in the Contaminated Debris Treatment Cell
4.1.1. Results of the Monitoring of Ash Wetness for Three Months
4.1.2. Effect of the Thickness of the Ash Layer
- The ash layer must be thick enough so that the recharge does not reach the maximum recharge, which is the limit for start infiltration.
- The recharge, at the end of a hydrological year, must be zero or have the same value as at the beginning of this year.
4.2. Analysis of Other Areas with Different Climatology
4.2.1. Selection of the Mining Areas
- There has been metal mining in the past and there may be abandoned waste dumps that need to be restored.
- There could be future mining projects driven by the existence of strategic raw materials.
- They are less than 500 km from a thermal power plant (in operation or closed) with an ash dump.
- They have different climatic conditions from each other, with the evapotranspiration to precipitation ratio ET0/P varying between 0.5 and 3.0.
4.2.2. Analysis of Three Representative Cases
4.2.3. Criterion to Determine the Ash Layer Thickness for Minimum Infiltration
- For ET0/P ≥ 1, ash can be used as a barrier layer, achieving zero infiltration or waterproofing if the ash layer is thick enough; for values of ET0/P ≈ 1, thicknesses of h = 50–60 cm will be necessary, which are drastically reduced to h = 10–15 cm when ET0/P ≥ 2. This ensures that water will not pass through the ash layer because it has sufficient maximum recharge to absorb excess water during rainy seasons. Theoretically, the ash layer could replace a layer of clay or a layer of clay plus a HDPE sheet.
- For ET0/P < 1, the ash layer can no longer be considered impermeable. With values of ET0/P ≈ 0.7, a layer of 40–50 cm can be used to stop more than 80% of rainwater. However, a HDPE waterproofing sheet may be required. With ET0/P ≈ 0.5 values, the worst conditions, it does not make sense for the ash layer to be very thick because it becomes totally saturated and does not have time to dry; however, the ash layer can still be useful since a thickness of only 10–15 cm allows less than 50% of the rainwater to pass through.
5. Discussion and Conclusions
- The effect is permanent over time as it is based on a physical barrier effect.
- The contamination reduction is independent of the initial concentration.
- The contamination reduction is for any PTE (Hg, Pb, Zn, etc.).
- Not trying to achieve absolute waterproofing based only on a very low hydraulic conductivity.
- Using by-products such as fly ash, with sufficiently low hydraulic conductivity and sufficiently high porosity, with sufficient recharge capacity to facilitate evapotranspiration and reduce water infiltration as far as possible.
- Prevent the rainwater from being contaminated is always a good result and, even if 100% waterproofing is not achieved, it can be a successful result in many cases.
- Reducing the volume of contaminated water results in economic savings because treatments for eliminating PTEs of the contaminated water are usually expensive.
- The leachate contamination reduction, due to the dilution in the water of the rivers, greatly reduces the extent of contamination so that the maximum concentration levels are closer to the source of contamination.
- The recharge is sufficiently large to absorb the maximum difference between precipitation and evapotranspiration.
- Infiltration is theoretically null or as little as possible.
- The recharge balances evapotranspiration in the dry season, ensuring that the planted species always have moisture.
Author Contributions
Funding
Data Availability Statement
Acknowledgments
Conflicts of Interest
Appendix A. Model of the Water Balance
Appendix A.1. Infiltration and Evaporation Models
Appendix A.1.1. Infiltration and Evaporation Analytical Models
Appendix A.1.2. Empirical Evapotranspiration Models
Appendix A.2. Water Balance
Appendix A.2.1. Hypothesis and Basic Formulae
- The test is performed in a treatment cell with a waterproofing sheet on the walls and floor; therefore, water can only enter the cell from the top surface. The capillary rise and deep percolation components are null.
- Water can only exit the cell either by evaporating or through a drain that exists in the slag layer just below the ash; there are no plants and then there is no transpiration, and no drainage was observed.
- The only water supply from outside the cell is rainwater; there is no irrigation.
- The treatment cell is horizontal, so there is no horizontal water flow; water can only ascend/descend or evaporate.
- It is tested on an ash layer of thickness h; for it to become saturated with rainfall, a small area of ash layer is prepared by reducing its thickness to h = 10 cm.
- The rainwater evaporates or passes into the ashes, increasing their humidity. As long as a maximum degree of humidity is not reached, the water not evaporated remains retained in the ash layer.
- The water begins to infiltrate into the lower layer of slag as soon as the ashes are saturated with water, acting as a drainage layer.
- There are no plants, so there is no elimination of water by transpiration; it is only by direct evaporation.
- Capillarity does not enter directly into the calculations.
- It is assumed that the behavior described by the model is valid for an ash layer up to h ≈ 50–60 cm.
- (1)
- In the first scenario, precipitation of the analyzed day is less than potential evapotranspiration (Pi ≤ ETPi), but there is sufficient water recharge for all that evapotranspiration to occur (Pi + Ri-1 ≥ ETPi). Actual evapotranspiration, ETRi, will be equal to potential evapotranspiration, ETPi, since there is enough water. Recharge is increased by precipitation, but decreased by evapotranspiration (Equations (A1)–(A4)).
- (2)
- Scenario typical of very dry periods. Precipitation is less than potential evapotranspiration (Pi ≤ ETPi) and there is not enough recharge to produce all that possible evapotranspiration (Pi + Ri-1 < ETPi). The actual evapotranspiration ETRi will equal rainfall and whatever water remains in the recharge. Recharge is increased by precipitation, but recharge is depleted due to evaporation being so intense (Equations (A5)–(A8)).
- (3)
- The third scenario is typical of humid periods, in which precipitation is higher than evapotranspiration (Pi > ETPi), leading to increased recharge, but without reaching the state of soil saturation and without reaching the maximum moisture that the soil can store (Ri ≤ Rmax). The part of rainfall that does not evaporate increases soil water recharge (Equations (A9)–(A12)) is as follows:
- (4)
- The fourth scenario occurs in rainy periods (Pi > ETPi). After several days of rainfall, the maximum recharge (Ri > Rmax) is reached and water begins to percolate or infiltrate to the lower layers (Ii > 0). However, the precipitation intensity does not reach a minimum value (Pi ≤ PN) for runoff to occur (Equations (A13)–(A18)).
- (5)
- The fifth scenario occurs in times of continuous rainfall (Pi > ETPi), with days of very heavy rainfall, above a minimum value (Pi > PN), which causes runoff (Ei > 0), because the 1 h rainwater flow (I1) is greater than the maximum possible infiltration through the water-saturated ash (I1 > Imax) (Equations (A19)–(A26)).
Appendix A.2.2. Precipitation and Evapotranspiration
Appendix A.2.3. Maximum Water Recharge
Appendix A.2.4. Maximum Water Infiltration
- The piezometric level h is equal to the thickness of the ash layer, since the rainfall is not considered to accumulate on the ash and the bottom layer is a draining layer.
- Since the flow is vertical, the distance to be traveled by the water is equal to the thickness of the ash layer x = h.
Appendix A.2.5. Runoff Condition
26 February 2024 | P24max (mm/day) | 45.80 |
I24 (mm/h) | 1.91 | |
20 May 2024 | P1max (mm/h) | 25.60 |
I1 (mm/h) | 25.60 | |
20 May 2024 | P6max (mm/6 h) | 37.00 |
I6 (mm/h) | 6.17 | |
n24-1 | 0.82 | |
n24-6 | 0.85 | |
n6-1 | 0.79 | |
n | 0.82 |
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Solid Sample | As (g/kg) | Hg (g/kg) | Leachate Sample | As (mg/L) | Hg (μg/L) |
---|---|---|---|---|---|
1 | 84.28 | 14.64 | 1 | 94.44 | 40.69 |
2 | 254.07 | 41.50 | 2 | 83.87 | 31.49 |
3 | 46.18 | 6.35 | 3 | 203.33 | 14.94 |
4 | 54.80 | 34.69 | 4 | 160.98 | 14.34 |
5 | 44.42 | 7.49 | 5 | 137.82 | 10.14 |
6 | 44.12 | 22.19 | 6 | 188.63 | 8.47 |
7 | 29.64 | 19.05 | 7 | 246.11 | 8.03 |
8 | 603.34 | 25.29 | 8 | 820.38 | 12.88 |
9 | 210.00 | 16.00 | 9 | 732.89 | 12.24 |
10 | 48.00 | 0.53 | 10 | 571.92 | 16.05 |
11 | 98.59 | 1.45 | 11 | 332.06 | 12.51 |
N | 11 | 11 | N | 11 | 11 |
Min | 29.64 | 0.53 | Min | 83.87 | 8.03 |
Max | 603.34 | 41.50 | Max | 820.38 | 40.69 |
Average | 136.13 | 17.20 | Average | 324.77 | 16.53 |
SD | 172.07 | 13.17 | SD | 261.85 | 10.20 |
SiO2 (wt%) | 61.7 | Hg (mg/kg) | 34,691 |
Fe2O3 (wt%) | 7.1 | As (mg/kg) | 54,801 |
MgO (wt%) | - | Zn (mg/kg) | 0.03 |
K2O (wt%) | 0.8 | Cu (mg/kg) | 420 |
Al2O3 (wt%) | 7.1 | Cr (mg/kg) | 920 |
CaO (wt%) | 3.9 | Pb (mg/kg) | 3400 |
SO3 (wt%) | 7.2 | Ni (mg/kg) | 0.02 |
TiO2 (wt%) | 0.55 | Cd (mg/kg) | 0.01 |
MnO (wt%) | 0.02 | pH | 5.1 |
SiO2 (wt%) | 56.5 | Hg (mg/kg) | 2 |
Fe2O3 (wt%) | 9.5 | As (mg/kg) | 59 |
MgO (wt%) | 0.9 | Zn (mg/kg) | 90 |
K2O (wt%) | 2.61 | Cu (mg/kg) | 57 |
Al2O3 (wt%) | 23.9 | Cr (mg/kg) | 83.6 |
CaO (wt%) | 3.4 | Pb (mg/kg) | 16 |
SO3 (wt%) | 2.04 | Ni (mg/kg) | 65.4 |
TiO2 (wt%) | 0.85 | Cd (mg/kg) | 1.84 |
MnO (wt%) | - | pH | 10.9 |
Parameter | Value | Standard |
---|---|---|
Bulk density (g/cm3) | 0.96 | [35] |
Actual particle density (g/cm3) | 2.38 | [36] |
Moisture content of the ash in stockpile (% by weight) | 1.24 | [37] |
Porosity (% by volume) | 58.8 | [35] |
Hydraulic conductivity (m/s) | 2.83 × 10−6 | [38] |
Zone | Mineral | Location | Province | Power Plant | Distance |
---|---|---|---|---|---|
1 | Mercury | Mieres | Asturias | Soto de Ribera (2) | 15 km |
2 | Zinc | Torrelavega | Cantabria | Aboño (1) | 162 km |
3 | Wolframio | Santa Comba | La Coruña | Meirama (3) | 40 km |
4 | Copper | Santiago de Compostela | La Coruña | Meirama (3) | 55 km |
5 | Tin, Wolframio | Beariz | Orense | Compostilla (4) | 157 km |
6 | Iron | Villablino | León | Compostilla (4) | 62 km |
7 | Lead | Santa Engracia | La Rioja | Pasajes (5) | 190 km |
8 | Uranium | Ciudad Rodrigo | Salamanca | Puertollano (6) | 481 km |
9 | Iron | Alquife | Granada | Carboneras (7) | 149 km |
10 | Mercury | Almadén | Ciudad Real | Puertollano (6) | 91 km |
11 | Arsenic | Bellmunt del Priorat | Tarragona | Cercs (8) Escatrón (9) | 211 km 123 km |
12 | Copper, Silver | Riotinto | Huelva | Los Barrios (10) | 258 km |
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Rodríguez, R.; Bascompta, M.; García-Ordiales, E.; Ayala, J. Use of Fly Ash Layer as a Barrier to Prevent Contamination of Rainwater by Contact with Hg-Contaminated Debris. Environments 2025, 12, 107. https://doi.org/10.3390/environments12040107
Rodríguez R, Bascompta M, García-Ordiales E, Ayala J. Use of Fly Ash Layer as a Barrier to Prevent Contamination of Rainwater by Contact with Hg-Contaminated Debris. Environments. 2025; 12(4):107. https://doi.org/10.3390/environments12040107
Chicago/Turabian StyleRodríguez, Rafael, Marc Bascompta, Efrén García-Ordiales, and Julia Ayala. 2025. "Use of Fly Ash Layer as a Barrier to Prevent Contamination of Rainwater by Contact with Hg-Contaminated Debris" Environments 12, no. 4: 107. https://doi.org/10.3390/environments12040107
APA StyleRodríguez, R., Bascompta, M., García-Ordiales, E., & Ayala, J. (2025). Use of Fly Ash Layer as a Barrier to Prevent Contamination of Rainwater by Contact with Hg-Contaminated Debris. Environments, 12(4), 107. https://doi.org/10.3390/environments12040107