Stability Conditions in Lignite Open Pits from Romania, Case Study: Oltețu Open Pit
Abstract
:1. Introduction
- The finite element method [21,25,46] is a modern, precise method that can be applied to complex structures. It allows the consideration of hydrological and hydrogeological conditions, the elements of support and improvement of land, and drainage systems. It does not require the imposition of preliminary assumptions, and it provides indications regarding the evolution of the safety factor and deformations during the entire sliding process.
- Methods based on 3D analyses [47,48,49,50] are applied in the case of slopes with complex geometries, variable structure, and partial loading, with a very well-defined breaking mechanism, and assume the addition of the third dimension in the 2D procedures, which leads to an increase in the number of unknowns. Three-dimensional methods are used quite rarely due to the fact that they have limited applicability.
- Different combinations of the above-mentioned methods.
2. Materials and Methods
2.1. Problem Statement
2.2. Field Observations and Laboratory Tests
2.2.1. The Yellow-Brown Clay
- −
- In the case of very low moisture, a gradual discharge of the massif takes place;
- −
- In the case of high moisture, the risk of landslides in which significant volumes of rocks can be entrained increases;
- −
- In the case of difficult conditions, such as a thick yellow-brown clay layer and the unfavorable geometrical elements of the slopes (high slope and large slope angle), the risk of sliding becomes greater, regardless of the moisture of the rocks.
2.2.2. The sandy Marls
2.2.3. The Lignite
- The geometric non-uniformity of the excavation fronts is caused by the morphology of the land, as the excavation process is completed in one step. This way of excavation leads to variations of the geometric elements, both on the width and on the depth (expansion) of the working front.
- Phenomena of fragmentation and detachment of the rocks from the slopes in conditions of low moisture and plastic flow tendencies of the clay from the upper part of the step under conditions of its saturation.
- Local manifestation of instability, affecting the entire height of the step, with variable extent depending on the structure of the massif and the hydro-meteorological conditions.
- Under the conditions of the initial geometry (December 2021) of the excavation fronts, the risk of massive landslides, which would involve large volumes of rocks and affect the safety of machinery and personnel, is relatively low.
- Taking into account the terrain morphology, the difficulties of ensuring a relatively uniform geometry of the excavation fronts will be accentuated with their advance.
- In the areas with increased amplitudes (the western part of the perimeter), taking into account the functional technological parameters of the E-02 excavator (ERC 1400-30/7 type) and possible instability phenomena, the design of appropriate exploitation technologies must be imposed so that the geometry of the slopes ensures their stability.
3. Results and Discussion
3.1. Analysis of the Stability of In Situ Slopes
- Drained slopes, unaffected by external factors (Fs1);
- Undrained slopes, where pore water pressure can induce landslides (Fs2);
- Undrained slopes and under the influence of seismic shocks, caused by the vibrations generated by the excavator and conveyor belts and/or the occurrence of an earthquake (Fs3).
- The stability analyses were performed for the initial conditions of the slopes only in the L1 (December 2021) and L2 (December 2021) sections, using the stratigraphic columns provided by the mining operator, and confirm the situation observed during the field investigations. Thus, in the area of L1 section, for the configuration of the slope from December 2021, instability phenomena of the clay and marl layers were manifested. The stability analysis carried out led to a value of 1.01 for the stability factor under conditions of no external stress on the slope (limit equilibrium state) and to sub-unit values for the case where pore water pressure and/or the effect of vibrations were manifested. The slope in L2 section was stable in December 2021, and the analyses performed indicate a stability reserve of 22% under no external stress, equilibrium limit under the conditions of the manifestation of pore water pressure, and instability under the conditions of the simultaneous effect of water and vibrations (shocks).
- The other sections, namely cross sections P0–P2, P4 and P5, present the hypothetical position of the lateral slopes at the end of the four quarters of 2022 (as they materialize).
- The stability factor depends on the height, inclination, and structure of the slope, a significant influence on the physical state (static and dynamic) coming from the weight of the clay layer in the structure of the slope. As for the sliding surface, in conditions where the thickness of the clay layer on the upper part exceeds 9–10 m, it is transmitted only through this layer and, as a rule, the stability coefficient is sub-unitary, indicating clay instability phenomena. Under the conditions of a clay layer of less thickness, the sliding surface is transmitted either through the layers of clay and sandy marl or through the entire step.
- Stability is ensured for slopes between 18 and 26 m high, and slope angles of up to 60°, in conditions of no external stress. For all other cases, namely the presence of water and seismic shocks (except for the slope in section L2, III quarter), the stability factor is sub-unitary or approaches the equilibrium limit.
3.2. Determination of the Stable Geometry of the Working Front and Lateral Slopes
3.2.1. Stable Geometry of Working Slopes
- −
- H = 25 m;
- −
- α = 52°;
- −
- Yellow-brown clay layer thickness: 9 m;
- −
- Fs1 = 1.05.
3.2.2. Stable Geometry of Lateral Slopes
- −
- H = 26 m;
- −
- α = 55°;
- −
- Yellow-brown clay layer thickness: 7.6 m;
- −
- Fs1 = 1.25.
- −
- Height of sub-steps H = 10 m;
- −
- The height of the sub-step system (upper step) Hgen = 20 m;
- −
- The width of the intermediate berm B = 60 m;
- −
- The width of the safety berm b = 30 m;
- −
- Inclination of sub-steps slopes αind = 45°;
- −
- General inclination of slope αgen = 25°;
- −
- The stability factor for sub-steps Fs1ind = 1.15;
- −
- The stability factor for general slope (sub-step system) Fs1gen = 1.26.
3.3. Recommendations for Ensuring the Stability Reserve
- Framing the excavation fronts in the geometric parameters that ensure the necessary stability reserve, depending on the type and lifetime of the slopes, according to the elements resulting from the determination of the stable geometry.
- Preliminary uncovering (stripping) of areas with pronounced non-uniformity of the land morphology, thus ensuring the geometry of the slopes in conditions of stability.
- Taking into account the tendency of the yellow-brown clay layer to disaggregate and the possibility of plastic failure, manifested by phenomena of “flow” on the slope both in a dry state as well as in the wet state, the maximum thickness in the structure of the excavation steps must be of maximum 10 m.
- A permanent monitoring of the deformation phenomena of the front and lateral slopes (cracks and fissures, subsidence or swelling areas, and other signs that reflect changes in the state of tension in the massif).
- Detailing the geological structure from the advance of the open pit, either by recovering the data of the initial exploration drillings or by executing new drillings that provide more precise information regarding the stratigraphy, tectonics, and hydrogeology of the area.
4. Conclusions
- The lignite layers in the perimeter of the Oltețu quarry are buried in sedimentary formations, being intercalated by clayey and marly rock layers;
- According to the grain size analyses, these rocks contain variable amounts of sand (generally fine sand), dust, and gravel;
- The geometry of the working fronts is uneven, being conditioned by the geomorphology of the region;
- The variation of the physical and mechanical properties of rocks is accentuated and highly influenced by the water content (moisture);
- The mechanical characteristics (cohesion and internal friction angle) decrease with increasing moisture, being dependent on hydro-meteorological conditions;
- The great variety of physical–mechanical characteristics required statistical processing and the selection of values considered representative for the stability analyzes;
- Considering the reduced resistance characteristics and the plastic behavior of the yellow-brown clay, the first layer from the land surface, it can be stated that it determines the occurrence of instability phenomena, such as sliding, disaggregation, dry flow, and plastic failure, regardless of the rock moisture;
- The stratigraphy is variable and not known precisely until the time of excavation (relatively small number of prospecting drillings on the advancement direction).
Author Contributions
Funding
Informed Consent Statement
Conflicts of Interest
References
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Type of Rock | Layer Thickness [m] | Values Determined in the Laboratory LMP GeoLogic Lab. [69] | Values Determined from Documentations [56] | Statistically Determined Values | |||||
---|---|---|---|---|---|---|---|---|---|
w [%] | γnat/γsat [daN/m3] | c [daN/cm2] | φ [°] | c [daN/cm2] | φ [°] | c [daN/cm2] | φ [°] | ||
Yellow-brown clay | 5–15 | 46.15 39.66 | 1845/1920 1782/1825 | 0.23–0.63 0.33 | 0–10 11.18 | 0.22 | 15 | 0.31 | 10 |
Sandy marl | 3–4 | 22.35 16.13 | 1850/1970 1911/2000 | 0.43 1.72 | 32 22.82 | 0.32 | 20.5 | 0.45 | 21 |
Lignite (IInd layer) | 2.6–5.0 | 36.25 | 1180/1300 | 0.7 */1.6 ** | 18 */34 ** | 0.3/1/1.2 | 30/19/38 | 1.1 | 26.5 |
Sandy marl | 0.3–1.5 | 22.35 16.13 | 1850/1970 1911/2000 | 0.43 1.72 | 32 22.82 | 0.32 | 20.5 | 0.45 | 21 |
Lignit (Ist layer) | 2.3–3.2 | 36.25 | 1187 | 0.7 */1.6 ** | 18 */34 ** | 0.3 | 30 | 1.1 | 26.5 |
Sandy marl | - | 22.35 16.13 | 1850/1970 1911/2000 | 0.43 1.72 | 32 22.82 | 0.32 | 20.5 | 0.45 | 21 |
Section | Stage | Height h [m] | Slope Angle α [°] | Thickness of the Yellow-Brown Clay Layer [m] | Stability Factor | Observations on the Transmission Mode of the Potential Slide Surface | ||
---|---|---|---|---|---|---|---|---|
Fs1 | Fs2 | Fs3 | ||||||
L1 | December 2021 | 23 | 65 | 10 | 1.01 | 0.81 | 0.71 | Sliding through layers of clay and very little sandy marl |
I quarter | 28.5 | 56 | 13 | 0.98 | 0.79 | 0.67 | Sliding through layer of clay | |
II quarter | 31.3 | 70 | 14 | 0.74 | 0.59 | 0.53 | Sliding through layers of clay and sandy marl | |
III quarter | 28 | 61 | 9.5 | 1.05 | 0.84 | 0.73 | Sliding through layers of clay and sandy marl | |
L2 | December 2021 | 26 | 47 | 7 | 1.22 | 0.98 | 0.81 | The potential sliding surface is transmitted over the entire height of the step exits in front of the foot of the slope |
I quarter | 21 | 64 | 11 | 0.91 | 0.73 | 0.71 | Sliding through layers of clay and sandy marl | |
II quarter | 20 | 64 | 10 | 1.12 | 0.90 | 0.79 | Sliding through layers of clay and sandy marl | |
III quarter | 18 | 46 | 10 | 1.54 | 1.23 | 1.08 | The potential sliding surface is transmitted over the entire height of the step and exits in front of the foot of the slope | |
P2 | IV quarter | 27 | 69 | 13.5 | 0.80 | 0.64 | 0.56 | Sliding through the clay layer and very little through the sandy marl |
P4 | IV quarter | 22 | 57 | 10 | 1.01 | 0.81 | 0.70 | Sliding through the clay layer, very little through the sandy marl, tangent to the layer no. II of lignite |
Section | Stage | Height h [m] | Slope Angle α [°] | Thickness of the Yellow-Brown Clay Layer [m] | Stability Factor | Observations on the Transmission Mode of the Potential Slide Surface | ||
---|---|---|---|---|---|---|---|---|
Fs1 | Fs2 | Fs3 | ||||||
P5 | I quarter | 40 | 61 | 18 | 0.65 | 0.52 | 0.45 | Sliding through layers of clay and sandy marl |
P1 | II quarter | 41 | 63 | 28 | 0.52 | 0.42 | 0.36 | Sliding through the clay layer and very little through the sandy marl |
P0 | III quarter | 38 | 48 | 25.5 | 0.67 | 0.53 | 0.44 | Sliding through layer of clay |
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Lazar, M.; Faur, F.; Apostu, I.-M. Stability Conditions in Lignite Open Pits from Romania, Case Study: Oltețu Open Pit. Appl. Sci. 2022, 12, 9607. https://doi.org/10.3390/app12199607
Lazar M, Faur F, Apostu I-M. Stability Conditions in Lignite Open Pits from Romania, Case Study: Oltețu Open Pit. Applied Sciences. 2022; 12(19):9607. https://doi.org/10.3390/app12199607
Chicago/Turabian StyleLazar, Maria, Florin Faur, and Izabela-Maria Apostu. 2022. "Stability Conditions in Lignite Open Pits from Romania, Case Study: Oltețu Open Pit" Applied Sciences 12, no. 19: 9607. https://doi.org/10.3390/app12199607
APA StyleLazar, M., Faur, F., & Apostu, I. -M. (2022). Stability Conditions in Lignite Open Pits from Romania, Case Study: Oltețu Open Pit. Applied Sciences, 12(19), 9607. https://doi.org/10.3390/app12199607