3.2. FIFC Landslide Early Warning Model
What follows is a brief introduction of failure index fragility curve. On the basis of the fragility curve theory, it is an improved version of the fragility curve. First proposed by the United Nations ISDR, the concept of vulnerability [
19] attributes disaster losses to hazard factors, exposure, and vulnerability. With the first application to the assessment of flood disasters, the vulnerability curve was then introduced to the evaluation of geological hazards, for example, earthquakes, typhoons, mud-rock flow, and landslides, among others [
20,
21,
22]. As a measurement to the extent of damage to the hazard-affected body, vulnerability, as the key to disaster damage estimation and risk assessment, functions as a link between disaster-causing factors and hazard. Expressed with the relationship curve or equation between disaster (h) and damage (d), i.e., V = f (h, d), it is alternatively known as vulnerability curve or damage/loss curve. It is employed to measure the correlation between the intensity of different disasters and their corresponding losses (rates) [
23].
In the landslide early warning model for ion-adsorption rare earth slopes, the safety factor value represents the degree of potential disasters; the water level height is employed to represent the main disaster-causing factors. Some other elements, for instance, slope height, slope angle, cohesion, and internal friction angle, should also be taken into consideration. The correlation among these factors can be described with Equation (7). Before drawing the failure index vulnerability curve, we need to standardize the values of safety factors and water level heights (0–1).
and
stand for water level index and safety factor index after standardization. Equations (8) and (9) show the conversion process. The changing water levels under different working conditions, including slope height, toe of side slope, cohesion, and internal friction angle, lead to the variation in slope safety factor. The scenario of these variations is numerically simulated. The failure index vulnerability curve is drawn on the basis of the collected data.
Figure 3 is a schematic diagram of the vulnerability curve under a particular working condition:
is the maximum water level line before solution injection (). is the corresponding when the slope safety factor . is the critical water level index (the corresponding when ). Wimin is the minimum water level index (the corresponding water level index when and ).
Figure 3 is the schematic diagram of vulnerability curve under a specific working condition. In accordance with the actual circumstances of rare earth mines, similar vulnerability curves can be established in this way. In practical applications, we can calculate the corresponding water level index (
) with the set formula by reading the slope water level. The matching safety factor index (
) defines the corresponding early warning risk. These operations are achieved by the embedded programs in the landslide early warning system.
3.4. Selection of Landslide-Induced Factors
As previously mentioned, we take diverse elements into consideration when developing early warning system for landslide risks. These elements include water level, slope height, slope angle, cohesion, and internal friction angle. The altitudes for most ion-adsorption rare earth slopes in South China are lower than 500 m above sea level, with a slope height of 20–50 m and slope angle of 30~50°. The research of Wu Changfu [
25] shows that slope height has little effect on slope stability. Therefore, the effect of slope height on its stability can be excluded. In the following, we are going to discuss the effects of slope angle, cohesion, and internal friction angle on the slope stability.
The value ranges for the three factors (slope angle, cohesion, and internal friction angle) were determined on the basis of the actual circumstances of ion-adsorption rare earth slopes in southern China (
Table 1). We then conducted comparative tests with these parameters, including: slope angles of 35°, 40°, and 45°; cohesive forces of 4 kPa, 11 kPa, and 18 kPa; internal friction angles of 27°, 29°, and 31°.
While establishing the geometric model for sensitivity analysis, we shall as far as possible, exclude the interference of irrelevant factors. These include the thickness of each layer of rare earth ore, including topsoil layer, complete- weathering layer 1, complete-weathering layer 2, semi-weathered layer, and bedrock. The thickness of each layer in this modeling was designated as follows: the thickness ratio of topsoil, complete-weathering layer 1, complete-weathering layer 2, semi-weathered layer, and bedrock was 2:8:8:6:11; the slope height was set to be 35 m. The cohesion density, cohesion force, and internal friction angle of topsoil layer were designated to be 13.6 kN/m
3, 5 kPa, and 30°, respectively; the density of complete-weathered layer was 11.8 kN/m
3; the cohesion force and internal friction angle of complete-weathered layer 1 were set to be 18 kPa and 31°, respectively; the density, cohesion, and internal friction angle of semi-weathered layer were set to be 10 kN/m
3, 3 kPa, and 35°, respectively; the bedrock density, cohesion, and internal friction angle were set to be 24 kN/m
3, 2 kPa, and 65°, respectively. It should be noted that the parameters in
Table 1 only affect those of complete-weathering layer 2, i.e., the part of the complete-weathering layer below the phreatic line. The specific comparison test groups are shown in
Table 2.
On the basis of the experimental groups in
Table 2, we established the corresponding numerical model for GeoStudio 2012 sensitivity analysis. The safety factors with the most dangerous landslide surface were calculated for each group. At first, the safety factors for three internal friction angle values were worked out with a slope angle of 40°, and a cohesion of 11 kPa. Then, the safety factors for three cohesion values were calculated with a slope angle of 40°, and an internal friction angle of 11 kPa. In the same way, the safety factors at different slope angles were calculated. The results are shown in
Figure 6 and
Table 3.
Figure 6a–g respectively correspond to the calculation results of groups 1–7.
Then, we draw the sensitivity analysis curves upon normalizing all parameters to be within 0~1. For example, “0” demonstrates that c is 0 kPa, and “1” shows that c is 18 kPa. On the basis of the numerical simulation results, the sensitivity curves under different slope angles (
), cohesion forces (c), and internal friction angles (
) are drawn in a graph (
Figure 7).
The hierarchical effects of slope angle, cohesion, and internal friction angle on the sensitivity of slope stability are described as: slope angle > cohesion > internal friction angle. That said, the influence of slope angle is the most significant, followed by cohesion. In comparison with slope angle and cohesion, internal friction angle has little effect on the slope stability. The reason for this can be accounted in the following: the ion-adsorption rare earth ore is a mixture of sand soil and 20% fine-grained clay soil. The internal friction angle is mainly controlled by the gradation of soil. Mainly demonstrated on the rare earth fine particles, the erosion effect of leaching solution on the large particles is extremely small. In general, in situ leaching has slight effect on the overall gradation. In the final analysis, the influences of internal friction angle variations on soil mass strength and slope stability are smaller than those of the other two factors during the leaching process of rare earth ore.
In accordance with the above analysis, we consider the effects of slope stability caused by the variation in internal friction angles as a secondary factor when establishing a landslide early warning model. In this research, the effect of internal friction angle changes on the slope stability is excluded.