# Effect of Wetting-Drying Cycles on Mechanical Behaviour and Electrical Resistivity of Unsaturated Subgrade Soil

Authors: Zhi Hu; Kai Peng; Lihua Li; Qiang Ma; Henglin Xiao; Zhichao Li; Pinbo Ai
Journal: Advances in Civil Engineering
 (2019)

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## Abstract

Compacted soil is widely used in road and railway subgrade, while alternation of seasons can cause fluctuations in moisture content of soil (i.e., wetting-drying cycles) and influence the performance of soil. In order to research the effect of wetting-drying cycles on mechanical behaviour and electrical resistivity of compacted unsaturated subgrade soil, wetting-drying tests considering different number and cyclic amplitude were conducted on compacted unsaturated clay specimens, and the electrical resistivity and unconfined compressive strength of soil were measured in this study. The AC (alternative current) two-electrode method was applied in the resistivity measurement. The experimental results show that increasing number and cyclic amplitude of wetting-drying cycles can both reduce the strength and electrical resistivity of the compacted unsaturated specimens. After 3-4 wetting-drying cycles, the strength and electrical resistivity tend to be constant value. The change of pore structure can be the key factor leading to the reduction of electrical resistivity of soil subjected to wetting-drying cycles and consequently causing the decrease of soil strength in the present study. Thus, the electrical resistivity can be adopted to indirectly assess the mechanical behaviour of unsaturated compacted soil after wetting-drying cycles.


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## Body

## 1. Introduction

Compacted soil is extensively applied as filling materials in ground treatment of buildings, retaining walls, dams, and especially in road/railway subgrade. Most of the subgrade soil is located in relatively shallow depth, so it can be vulnerable to wetting-drying cycles due to variations of meteorological and hydrological conditions especially in humid subtropical regions [1, 2]. A large number of studies have been conducted on the effect of wetting-drying cycles on properties of compacted soil. Most are focused on the mechanical and deformation behaviours [3–7]. It has been discovered that soil strength may decrease after a certain number of wetting-drying cycles. Chen et al. [8] recently investigated the impact of wetting-drying cycles on the shear strength of an unsaturated compacted soil by controlling suction. However, results show that the shear strength has a slight increase after five cycles, which is explained as the densification effect of wetting-drying cycles on soil. For unsaturated soil, suction is an important factor influencing the soil properties. Wetting-drying cycles can be treated as an alternative loading on the soil in form of suction along with the change of moisture content. So, the soil-water characteristic or hydromechanical behaviour is also studied [1, 9, 10]. The initial condition and suction path can affect the properties of soil subjected to cyclic wetting-dryings. Moreover, some investigations have been conducted on the soil structure [11] and microscale behaviour [12].As an important behaviour of soil, strength for different wetting-drying cycles can hardly be tested and obtained on a single specimen. Because uncovered damage occurs when loading on soil exceeds its strength, further wetting-drying test cannot be carried out on it. Thus, testing of soil strength is performed on different specimens, and this inevitably reduces the reliability of results. To make up for this, methods and indexes of nondestructive testing can be applied to reveal the evolution of soil behaviour synchronously during wetting-drying cycles, including CT (computed tomography) [13], electrical resistivity/conductivity, ultrasonic velocity [14], surface morphology [15], NMR (nuclear magnetic resonance) [16], etc.Taking advantage of convenient operation and relative low cost, electrical resistivity is largely used to study the soil behaviour [17–21]. The electrical resistivity of unsaturated soil is primarily determined by material composition, structures, and characteristics of pore fluid in soil [22, 23]. In the process of wetting-drying cycles, electrical resistivity of soil can change apparently, while the change trend and the mechanism are in dispute. The DC (direct current) two-electrode method was applied to investigate the electrical behaviour of clay, and results show a rise in electrical resistivity with increasing number of wetting-drying cycles [24, 25]. Recently, Huang et al. [26] reported that the shear strength has a significant drop after wetting-drying paths while the changes of electrical resistivity are not keeping in a consistent trend. In addition, few studies on the effect of cyclic amplitude and the evolution of electrical resistivity during wetting-drying cycles have been reported. Thus, further studies on the electrical properties of compacted unsaturated soil with wetting-drying cycles are needed.In this paper, the mechanical behaviour and electrical resistivity of compacted unsaturated clay under wetting-drying cycles are studied. The AC (alternative current) two-electrode method was adopted to measure the electrical resistivity of soil, and unconfined compression tests were conducted for each wetting-drying cycle. Then, the effect of number and cyclic amplitude of wetting-drying cycles on soil strength and electrical resistivity is investigated. Finally, the relationship between soil strength and electrical resistivity is discussed.


## 2. Experimental Program

### 2.1. Tested Material and Specimen Preparation

The soil used in the tests was clay collected from a site in Wuhan, China. The impurities and rocks in soil were firstly removed. Then, the soil samples were sieved through a 2 mm sieve and air-dried. The basic material properties of the soil were investigated in laboratory as listed in Table1. The clay was classified as clay of low plasticity (CL) according to the Unified Soil Classification System (USCS).Table 1
Basic material properties of the tested clay.
Property
Value
Grain composition (%)
>0.075 mm
16.1
0.075 to 0.05 mm
4.8
0.05 to 0.01 mm
36.3
0.01 to 0.005 mm
8.4
0.005 to 0.002 mm
9.4
<0.002 mm
20.2
Specific gravity,Gs
2.76
Liquid limit, LL (%)
37.0
Plastic limit, PL (%)
20.0
Plastic index, PI (%)
17.0
Maximum dry density,ρdmax (g/cm3)
1.98
Optimum moisture content, OMC (%)
16.0
Saturated moisture content (%)
25.5For cyclic wetting-drying tests, the air-dried soil samples were wetted to optimum moisture content (i.e., MC = 16%). After reaching the design moisture content, the wet soil samples were kept in a sealed plastic bag for at least 24 hours. Then cylindrical specimens (38 mm in diameter and 76 mm high) were prepared referring to the procedures of tamping method described in ASTM standard D5311. Five layers were used in the compaction, and the height was used to determine the degree of compaction for each layer. A top cap was placed on the last layer, and continuous compression on the top cap was applied until the desired dry density was obtained. In this study, the dry density of specimens was controlled asρd = 1.84 g/cm3, which corresponds to degree of compaction K = 0.93, the compaction criteria of heavy-haul railway subgrade (Chinese code of design of heavy-haul railway, TB 10625-2017). Then, all specimens were wrapped with plastic films and cured in a desiccator for 24 hours, to accelerate uniform distribution of moisture in the specimens. In order to study the effects of dry density and moisture content on the electrical resistivity, specimens with various dry densities (1.68 g/cm3, 1.78 g/cm3, 1.84 g/cm3, and 1.88 g/cm3) and moisture contents (10%, 12%, 14%, 16%, 18%, and 20%) were prepared. The same procedure of preparation and processing was applied as described above. Here, the dry density ρd = 1.68 g/cm3, 1.78 g/cm3, 1.84 g/cm3, and 1.88 g/cm3 corresponds to degree of compaction K = 0.85, 0.90, 0.93, and 0.95, respectively.


### 2.2. Test Equipment and Procedures

#### 2.2.1. Cyclic Wetting-Dying Test

Cyclic wetting-drying tests were performed following the procedures in the authors’ previous study [27]. Specimens were wetted by a spray bottle and dried by air. The moisture content of the specimens was controlled by controlling the mass of the specimen. Initial moisture content and initial mass of specimen can be measured first, and equation (1) was applied to control the target mass of the specimen:(1)m1=w11+w0m0,where m0 and m1 are initial mass and target mass of specimen and w0 and w1 represent initial and target moisture content of the specimen.For compacted subgrade, the soil is typically compacted at optimum moisture content (OMC). After several alternations of seasons, the moisture content in subgrade soil may increase slightly to a so-called equilibrium moisture content (EMC) [28]. Moreover, concerning long-term service of road or railroad, the moisture content of subgrade soil shows periodic fluctuation around the equilibrium moisture content. Based on the phenomenon, the wetting-drying path in the present study was designed as illustrated in Figure 1. The specimens were prepared at OMC as described above firstly and then wetted to EMC to start the wetting-drying cycles. When reaching the desired number of wetting-drying, the moisture content of specimens was kept at EMC for further testing. The EMC was set as 17% in the test, and the cyclic amplitude of wetting-drying was considered as EMC ± 1%, EMC ± 3%, and EMC ± 5%. Since many studies [10, 15, 29, 30] have reported that the influence of wetting-drying cycles on the properties of soil is limited after 4 to 6 cycles, the maximum number of wetting-dryings was selected as five cycles in this study. After each wetting-drying cycle, the dimensions of the specimen should be measured to calculate volumetric strain of specimens. A vernier caliper with an accuracy of 0.01 mm was applied to measure diameters and height of the specimen. To calculate the volumetric strain, the volume change of the specimen compared with initial volume was divided by initial volume. Moreover, unconfined compression tests should be conducted on each layer.Figure 1
Wetting-drying path.


#### 2.2.2. Electrical Resistivity Measurement

For laboratory electrical resistivity measurement of soil, the four-electrode method and two-electrode method can be used [24, 31]. The devices of two-electrode method are simple, while contact resistance between electrode and soil is usually large especially at low moisture content. The contact resistance can be neglected when using four-electrode method, but soil specimen could be disturbed by the insertion of two measuring electrodes. Since soil strength should be obtained after wetting-drying cycles, the two-electrode method was selected in this study to keep the integrality of specimens. Moreover, an alternative current (AC) supply was used rather than direct current (DC) supply, to avoid polarization of soil and electrode. The schematic of electrical resistivity measurement is shown in Figure 2. Note that Hc and Lc represent high and low currents and Hp and Lp represent high and low potentials. For the sake of reducing contact resistance, a fixed-weight block was applied on the top platen during the measurement. The weight of block can be adjusted for different experimental conditions. Within an independent study or a set of tests, the weight should be fixed to ensure comparability of data.Figure 2
Schematic of electrical resistivity measurement.A LCR digital bridge (TH2817A, Tonghui Electronic Co., Ltd) was adopted to measure the electrical resistance of soil specimens, as shown in Figure3. Meanwhile, the diameter (D) and length of specimen (L) were measured carefully to calculate the electrical resistivity of specimen applying the following equation:(2)ρ=RAL,where ρ is electrical resistivity, R is electrical resistance, A is the cross section area calculated by the diameter D of specimen, and L is the length of the specimen.Figure 3
The digital bridge (Tonghui, TH2817A).When using AC power supply, the AC frequency has a dramatic effect on the electrical resistivity of soil. The electrical resistivity of three specimens with different moisture contents (MC = 12%, 17%, and 22%) is presented in Figure4, considering a sequence of current frequencies (100 Hz, 500 Hz, 1 kHz, 5 kHz, 10 kHz, 20 kHz, and 50 kHz). It can be seen that the electrical resistivity decreases sharply when the current frequency varies from 100 Hz to 1 kHz. When the current frequency exceeds 10 kHz, the measured electrical resistivity tends to be constant. Besides, the data volatility is gradually reduced as the current frequency increases. It can be also observed from the figure that the specimen with low moisture content is more sensitive to current frequency. Rinaldi and Cuestas [32] have reported that electrode polarization occurs below 2 kHz or 3 kHz and double layer relaxation appears beyond 100 kHz. The conductivity of soil exhibits almost constant behaviour between the above mentioned frequencies, namely, ohmic conduction. In order to avoid electrode polarization and improve data stability, current frequency was chosen as 50 kHz in this study, and the measuring voltage was fixed at default value of the equipment, i.e., 1 V.Figure 4
Variations of electrical resistivity with different current frequencies.It is known that the electrical resistance is very sensitive to temperature; thus, a temperature correction of electrical resistivity is necessary. For this purpose, three specimens were used to record the electrical resistivity at different temperatures. Results are shown in Figure5. By applying the temperature correction equation as shown in equation (3), the relationship between electrical resistivity at any temperature and electrical resistivity at 25°C can be calculated [24]:(3)ρ25=ρT1+αT−25,where ρ25 is electrical resistivity at 25°C, ρT is electrical resistivity at temperature T, T is the test temperature, and α is the empirical correction coefficient.Figure 5
Temperature correction curves for electrical resistivity.One can obtain the average correction coefficientα = 0.0205°C−1. Temperatures during measurement are all recorded to convert the electrical resistivity into values at temperature T = 25°C. The electrical resistivity of specimens was measured at each wetting-drying cycle and before the unconfined compression test.


#### 2.2.3. Unconfined Compression Test

After the specimens underwent cyclic wetting-drying, unconfined compression tests were conducted on these specimens. The test procedures were following the method described in ASTM standard D2166/D2166M. A strain-controlled compression apparatus was used as shown in Figure6. The strain rate was controlled at 2%/min. Note that for unsaturated clay, matric suction can be a significant influencing factor on soil strength. In this study, with careful preparation of specimens, the differences of initial dry unit weight and initial moisture content were very small between each specimen. As known, matric suction is determined by degree of saturation at a constant dry unit weight. Here, the specimens have nearly the same dry unit weight and degree of saturation, so we consider the initial matric suctions of specimens are the same.Figure 6
The compression apparatus for unconfined compression tests.


## 2.1. Tested Material and Specimen Preparation

The soil used in the tests was clay collected from a site in Wuhan, China. The impurities and rocks in soil were firstly removed. Then, the soil samples were sieved through a 2 mm sieve and air-dried. The basic material properties of the soil were investigated in laboratory as listed in Table1. The clay was classified as clay of low plasticity (CL) according to the Unified Soil Classification System (USCS).Table 1
Basic material properties of the tested clay.
Property
Value
Grain composition (%)
>0.075 mm
16.1
0.075 to 0.05 mm
4.8
0.05 to 0.01 mm
36.3
0.01 to 0.005 mm
8.4
0.005 to 0.002 mm
9.4
<0.002 mm
20.2
Specific gravity,Gs
2.76
Liquid limit, LL (%)
37.0
Plastic limit, PL (%)
20.0
Plastic index, PI (%)
17.0
Maximum dry density,ρdmax (g/cm3)
1.98
Optimum moisture content, OMC (%)
16.0
Saturated moisture content (%)
25.5For cyclic wetting-drying tests, the air-dried soil samples were wetted to optimum moisture content (i.e., MC = 16%). After reaching the design moisture content, the wet soil samples were kept in a sealed plastic bag for at least 24 hours. Then cylindrical specimens (38 mm in diameter and 76 mm high) were prepared referring to the procedures of tamping method described in ASTM standard D5311. Five layers were used in the compaction, and the height was used to determine the degree of compaction for each layer. A top cap was placed on the last layer, and continuous compression on the top cap was applied until the desired dry density was obtained. In this study, the dry density of specimens was controlled asρd = 1.84 g/cm3, which corresponds to degree of compaction K = 0.93, the compaction criteria of heavy-haul railway subgrade (Chinese code of design of heavy-haul railway, TB 10625-2017). Then, all specimens were wrapped with plastic films and cured in a desiccator for 24 hours, to accelerate uniform distribution of moisture in the specimens. In order to study the effects of dry density and moisture content on the electrical resistivity, specimens with various dry densities (1.68 g/cm3, 1.78 g/cm3, 1.84 g/cm3, and 1.88 g/cm3) and moisture contents (10%, 12%, 14%, 16%, 18%, and 20%) were prepared. The same procedure of preparation and processing was applied as described above. Here, the dry density ρd = 1.68 g/cm3, 1.78 g/cm3, 1.84 g/cm3, and 1.88 g/cm3 corresponds to degree of compaction K = 0.85, 0.90, 0.93, and 0.95, respectively.


## 2.2. Test Equipment and Procedures

### 2.2.1. Cyclic Wetting-Dying Test

Cyclic wetting-drying tests were performed following the procedures in the authors’ previous study [27]. Specimens were wetted by a spray bottle and dried by air. The moisture content of the specimens was controlled by controlling the mass of the specimen. Initial moisture content and initial mass of specimen can be measured first, and equation (1) was applied to control the target mass of the specimen:(1)m1=w11+w0m0,where m0 and m1 are initial mass and target mass of specimen and w0 and w1 represent initial and target moisture content of the specimen.For compacted subgrade, the soil is typically compacted at optimum moisture content (OMC). After several alternations of seasons, the moisture content in subgrade soil may increase slightly to a so-called equilibrium moisture content (EMC) [28]. Moreover, concerning long-term service of road or railroad, the moisture content of subgrade soil shows periodic fluctuation around the equilibrium moisture content. Based on the phenomenon, the wetting-drying path in the present study was designed as illustrated in Figure 1. The specimens were prepared at OMC as described above firstly and then wetted to EMC to start the wetting-drying cycles. When reaching the desired number of wetting-drying, the moisture content of specimens was kept at EMC for further testing. The EMC was set as 17% in the test, and the cyclic amplitude of wetting-drying was considered as EMC ± 1%, EMC ± 3%, and EMC ± 5%. Since many studies [10, 15, 29, 30] have reported that the influence of wetting-drying cycles on the properties of soil is limited after 4 to 6 cycles, the maximum number of wetting-dryings was selected as five cycles in this study. After each wetting-drying cycle, the dimensions of the specimen should be measured to calculate volumetric strain of specimens. A vernier caliper with an accuracy of 0.01 mm was applied to measure diameters and height of the specimen. To calculate the volumetric strain, the volume change of the specimen compared with initial volume was divided by initial volume. Moreover, unconfined compression tests should be conducted on each layer.Figure 1
Wetting-drying path.


### 2.2.2. Electrical Resistivity Measurement

For laboratory electrical resistivity measurement of soil, the four-electrode method and two-electrode method can be used [24, 31]. The devices of two-electrode method are simple, while contact resistance between electrode and soil is usually large especially at low moisture content. The contact resistance can be neglected when using four-electrode method, but soil specimen could be disturbed by the insertion of two measuring electrodes. Since soil strength should be obtained after wetting-drying cycles, the two-electrode method was selected in this study to keep the integrality of specimens. Moreover, an alternative current (AC) supply was used rather than direct current (DC) supply, to avoid polarization of soil and electrode. The schematic of electrical resistivity measurement is shown in Figure 2. Note that Hc and Lc represent high and low currents and Hp and Lp represent high and low potentials. For the sake of reducing contact resistance, a fixed-weight block was applied on the top platen during the measurement. The weight of block can be adjusted for different experimental conditions. Within an independent study or a set of tests, the weight should be fixed to ensure comparability of data.Figure 2
Schematic of electrical resistivity measurement.A LCR digital bridge (TH2817A, Tonghui Electronic Co., Ltd) was adopted to measure the electrical resistance of soil specimens, as shown in Figure3. Meanwhile, the diameter (D) and length of specimen (L) were measured carefully to calculate the electrical resistivity of specimen applying the following equation:(2)ρ=RAL,where ρ is electrical resistivity, R is electrical resistance, A is the cross section area calculated by the diameter D of specimen, and L is the length of the specimen.Figure 3
The digital bridge (Tonghui, TH2817A).When using AC power supply, the AC frequency has a dramatic effect on the electrical resistivity of soil. The electrical resistivity of three specimens with different moisture contents (MC = 12%, 17%, and 22%) is presented in Figure4, considering a sequence of current frequencies (100 Hz, 500 Hz, 1 kHz, 5 kHz, 10 kHz, 20 kHz, and 50 kHz). It can be seen that the electrical resistivity decreases sharply when the current frequency varies from 100 Hz to 1 kHz. When the current frequency exceeds 10 kHz, the measured electrical resistivity tends to be constant. Besides, the data volatility is gradually reduced as the current frequency increases. It can be also observed from the figure that the specimen with low moisture content is more sensitive to current frequency. Rinaldi and Cuestas [32] have reported that electrode polarization occurs below 2 kHz or 3 kHz and double layer relaxation appears beyond 100 kHz. The conductivity of soil exhibits almost constant behaviour between the above mentioned frequencies, namely, ohmic conduction. In order to avoid electrode polarization and improve data stability, current frequency was chosen as 50 kHz in this study, and the measuring voltage was fixed at default value of the equipment, i.e., 1 V.Figure 4
Variations of electrical resistivity with different current frequencies.It is known that the electrical resistance is very sensitive to temperature; thus, a temperature correction of electrical resistivity is necessary. For this purpose, three specimens were used to record the electrical resistivity at different temperatures. Results are shown in Figure5. By applying the temperature correction equation as shown in equation (3), the relationship between electrical resistivity at any temperature and electrical resistivity at 25°C can be calculated [24]:(3)ρ25=ρT1+αT−25,where ρ25 is electrical resistivity at 25°C, ρT is electrical resistivity at temperature T, T is the test temperature, and α is the empirical correction coefficient.Figure 5
Temperature correction curves for electrical resistivity.One can obtain the average correction coefficientα = 0.0205°C−1. Temperatures during measurement are all recorded to convert the electrical resistivity into values at temperature T = 25°C. The electrical resistivity of specimens was measured at each wetting-drying cycle and before the unconfined compression test.


### 2.2.3. Unconfined Compression Test

After the specimens underwent cyclic wetting-drying, unconfined compression tests were conducted on these specimens. The test procedures were following the method described in ASTM standard D2166/D2166M. A strain-controlled compression apparatus was used as shown in Figure6. The strain rate was controlled at 2%/min. Note that for unsaturated clay, matric suction can be a significant influencing factor on soil strength. In this study, with careful preparation of specimens, the differences of initial dry unit weight and initial moisture content were very small between each specimen. As known, matric suction is determined by degree of saturation at a constant dry unit weight. Here, the specimens have nearly the same dry unit weight and degree of saturation, so we consider the initial matric suctions of specimens are the same.Figure 6
The compression apparatus for unconfined compression tests.


## 2.2.1. Cyclic Wetting-Dying Test

Cyclic wetting-drying tests were performed following the procedures in the authors’ previous study [27]. Specimens were wetted by a spray bottle and dried by air. The moisture content of the specimens was controlled by controlling the mass of the specimen. Initial moisture content and initial mass of specimen can be measured first, and equation (1) was applied to control the target mass of the specimen:(1)m1=w11+w0m0,where m0 and m1 are initial mass and target mass of specimen and w0 and w1 represent initial and target moisture content of the specimen.For compacted subgrade, the soil is typically compacted at optimum moisture content (OMC). After several alternations of seasons, the moisture content in subgrade soil may increase slightly to a so-called equilibrium moisture content (EMC) [28]. Moreover, concerning long-term service of road or railroad, the moisture content of subgrade soil shows periodic fluctuation around the equilibrium moisture content. Based on the phenomenon, the wetting-drying path in the present study was designed as illustrated in Figure 1. The specimens were prepared at OMC as described above firstly and then wetted to EMC to start the wetting-drying cycles. When reaching the desired number of wetting-drying, the moisture content of specimens was kept at EMC for further testing. The EMC was set as 17% in the test, and the cyclic amplitude of wetting-drying was considered as EMC ± 1%, EMC ± 3%, and EMC ± 5%. Since many studies [10, 15, 29, 30] have reported that the influence of wetting-drying cycles on the properties of soil is limited after 4 to 6 cycles, the maximum number of wetting-dryings was selected as five cycles in this study. After each wetting-drying cycle, the dimensions of the specimen should be measured to calculate volumetric strain of specimens. A vernier caliper with an accuracy of 0.01 mm was applied to measure diameters and height of the specimen. To calculate the volumetric strain, the volume change of the specimen compared with initial volume was divided by initial volume. Moreover, unconfined compression tests should be conducted on each layer.Figure 1
Wetting-drying path.


## 2.2.2. Electrical Resistivity Measurement

For laboratory electrical resistivity measurement of soil, the four-electrode method and two-electrode method can be used [24, 31]. The devices of two-electrode method are simple, while contact resistance between electrode and soil is usually large especially at low moisture content. The contact resistance can be neglected when using four-electrode method, but soil specimen could be disturbed by the insertion of two measuring electrodes. Since soil strength should be obtained after wetting-drying cycles, the two-electrode method was selected in this study to keep the integrality of specimens. Moreover, an alternative current (AC) supply was used rather than direct current (DC) supply, to avoid polarization of soil and electrode. The schematic of electrical resistivity measurement is shown in Figure 2. Note that Hc and Lc represent high and low currents and Hp and Lp represent high and low potentials. For the sake of reducing contact resistance, a fixed-weight block was applied on the top platen during the measurement. The weight of block can be adjusted for different experimental conditions. Within an independent study or a set of tests, the weight should be fixed to ensure comparability of data.Figure 2
Schematic of electrical resistivity measurement.A LCR digital bridge (TH2817A, Tonghui Electronic Co., Ltd) was adopted to measure the electrical resistance of soil specimens, as shown in Figure3. Meanwhile, the diameter (D) and length of specimen (L) were measured carefully to calculate the electrical resistivity of specimen applying the following equation:(2)ρ=RAL,where ρ is electrical resistivity, R is electrical resistance, A is the cross section area calculated by the diameter D of specimen, and L is the length of the specimen.Figure 3
The digital bridge (Tonghui, TH2817A).When using AC power supply, the AC frequency has a dramatic effect on the electrical resistivity of soil. The electrical resistivity of three specimens with different moisture contents (MC = 12%, 17%, and 22%) is presented in Figure4, considering a sequence of current frequencies (100 Hz, 500 Hz, 1 kHz, 5 kHz, 10 kHz, 20 kHz, and 50 kHz). It can be seen that the electrical resistivity decreases sharply when the current frequency varies from 100 Hz to 1 kHz. When the current frequency exceeds 10 kHz, the measured electrical resistivity tends to be constant. Besides, the data volatility is gradually reduced as the current frequency increases. It can be also observed from the figure that the specimen with low moisture content is more sensitive to current frequency. Rinaldi and Cuestas [32] have reported that electrode polarization occurs below 2 kHz or 3 kHz and double layer relaxation appears beyond 100 kHz. The conductivity of soil exhibits almost constant behaviour between the above mentioned frequencies, namely, ohmic conduction. In order to avoid electrode polarization and improve data stability, current frequency was chosen as 50 kHz in this study, and the measuring voltage was fixed at default value of the equipment, i.e., 1 V.Figure 4
Variations of electrical resistivity with different current frequencies.It is known that the electrical resistance is very sensitive to temperature; thus, a temperature correction of electrical resistivity is necessary. For this purpose, three specimens were used to record the electrical resistivity at different temperatures. Results are shown in Figure5. By applying the temperature correction equation as shown in equation (3), the relationship between electrical resistivity at any temperature and electrical resistivity at 25°C can be calculated [24]:(3)ρ25=ρT1+αT−25,where ρ25 is electrical resistivity at 25°C, ρT is electrical resistivity at temperature T, T is the test temperature, and α is the empirical correction coefficient.Figure 5
Temperature correction curves for electrical resistivity.One can obtain the average correction coefficientα = 0.0205°C−1. Temperatures during measurement are all recorded to convert the electrical resistivity into values at temperature T = 25°C. The electrical resistivity of specimens was measured at each wetting-drying cycle and before the unconfined compression test.


## 2.2.3. Unconfined Compression Test

After the specimens underwent cyclic wetting-drying, unconfined compression tests were conducted on these specimens. The test procedures were following the method described in ASTM standard D2166/D2166M. A strain-controlled compression apparatus was used as shown in Figure6. The strain rate was controlled at 2%/min. Note that for unsaturated clay, matric suction can be a significant influencing factor on soil strength. In this study, with careful preparation of specimens, the differences of initial dry unit weight and initial moisture content were very small between each specimen. As known, matric suction is determined by degree of saturation at a constant dry unit weight. Here, the specimens have nearly the same dry unit weight and degree of saturation, so we consider the initial matric suctions of specimens are the same.Figure 6
The compression apparatus for unconfined compression tests.


## 3. Results and Discussions

### 3.1. Effect of Dry Density and Moisture Content on Soil Electrical Resistivity

The electrical resistivity of compacted clay with different dry densities and moisture contents is presented in Figure7. As shown in the figure, the electrical resistivity of soil with the same dry density is obviously decreased when the moisture content increases. Also, for soil specimens with the same moisture content, higher dry density can cause smaller electrical resistivity. These results are in accordance with previous studies [25] as presented in Figure 7, and it can be proved that the testing method of soil electrical resistivity in this study is reliable. Figure 8 presents the variation of electrical resistivity with degree of saturation. It can be seen that the electrical resistivity decreases as the degree of saturation increases.Figure 7
Variations of electrical resistivity with moisture content and degree of compaction.Figure 8
Variations of electrical resistivity with degree of saturation.


### 3.2. Effect of Wetting-Drying Cycles on Soil Strength

Before the unconfined compression tests, the moisture content of specimens was controlled the same, i.e., MC = EMC. The actual degree of saturation (Sr) data of specimens used in unconfined compression tests are presented in Table 2. It can be seen that Sr falls in the range of 84.4% to 86.7% for different specimens. It is known that the suction of soil changes slightly due to variations of degree of saturation in high moisture content conditions [33]; thus, it can be assumed that differences of suction between specimens were very limited, and the effect of suction on soil strength can be neglected at equilibrium moisture content.Table 2
Actual degree of saturation of specimens at EMC.
Number of wetting-drying cycles
Degree of saturation,Sr (%)
EMC ± 1%
EMC ± 3%
EMC ± 5%
1
84.8
86.4
84.4
2
86.0
86.6
86.0
3
86.8
85.7
85.1
4
86.6
85.1
84.9
5
85.3
85.9
84.4The effect of number and cyclic amplitude of wetting-drying cycles on unconfined compressive strength (UCS) of soil is shown in Figure9. It can be seen that the soil strength reduces with larger number of wetting-drying, and after 3-4 cycles, the soil strength tends to be constant. Additionally, greater reduction in soil strength can be observed with larger cyclic amplitude of wetting-drying. After the 5th wetting-drying cycles, the soil strength can be decreased by 19%, 20%, and 56% compared to that of noncycle specimen for cyclic amplitude of EMC ± 1%, EMC ± 3%, and EMC ± 5%, respectively.Figure 9
Effect of wetting-drying cycles on unconfined compressive strength of soil.Furthermore, typical photos of specimens after failure undergoing five cycles are presented in Figure10. With larger cyclic amplitude of wetting-drying, more cracks can be found on the surface of specimen after failure and the width of cracks increases apparently. From the point of view of damage mechanics, the growth and development of macrocracks are related to properties of microcracks and material structure change [34]. For unsaturated clay, cracks occur when the tensile stress induced by the developed suction exceeds the tensile strength of the specimen during drying path. Some cracks can be repaired in wetting path. However, irreversible soil structure change can result in accumulation of cracks after wetting-drying cycles [15]. Larger suction range suggests more crack accumulation. Thus, it can be deduced that more microcracks are caused by wetting-drying cycles with larger cyclic amplitude. If the degradation of soil strength is treated as a result of soil damage, the process of soil damage can be the evolution of microcracks and soil structure. It can be also suggested that large fluctuation of soil moisture content could generate significant decline of soil strength. Thus, waterproof and drainage facilities in compacted soil structures appear very important, and more attentions should be paid on the design and construction of hydraulic buffer or hydraulic barrier to reduce fluctuation of moisture content in soil.Figure 10
Photos of specimens after failure undergoing five wetting-drying cycles: (a) cyclic amplitude EMC ± 1%; (b) cyclic amplitude EMC ± 3%; (c) cyclic amplitude EMC ± 5%.
(a)
(b)
(c)


### 3.3. Effect of Cyclic Wetting-Drying on Soil Electrical Resistivity

The influences of cyclic wetting-dryings on soil electrical resistivity are presented in Figures11 and 12. Here, soil moisture content of specimens at the start point is EMC = 17%. It can be seen from Figure 11 that in each cycle, the soil electrical resistivity firstly decreases, then increases to a peak value, and finally drops to around the initial value. The variations of electrical resistivity are in negative correlation with moisture content. In addition, the soil electrical resistivity shows a fluctuant downward trend with more wetting-drying cycles. Moreover, the higher fluctuation of electrical resistivity can be recognized on specimens subjected to larger cyclic amplitude. It can be also observed that electrical resistivity at maximum moisture content shows a declining trend within the first three wetting-drying cycles. After the 3rd cycle, the electrical resistivity at maximum moisture content becomes stable, while the impact of wetting-drying cycles on the electrical resistivity at minimum moisture content is very small.Figure 11
Evolutions of soil electrical resistivity with wetting-drying cycles.Figure 12
Variations of final electrical resistivity with wetting-drying cycles.For better comparison of electrical resistivity for each wetting-drying cycle, electrical resistivity at moisture content 17% (i.e., the end point) for each cycle is plotted in Figure12. Overall, the electrical resistivity of soil decreases rapidly at the first three cycles and becomes a constant value after 3-4 cycles except the cyclic amplitude EMC ± 5%. The increase of cyclic amplitude contributes to the reduction of electrical resistivity, especially after three wetting-drying cycles. It can be suggested from the above results that the electrical resistivity of compacted soil can be greatly reduced by wetting-drying cycles.Figures13 and 14 illustrate variations of void ratio and degree of saturation during wetting-drying cycles. In the figures, numbers of wetting-drying cycle and the approximate equilibrium position are indicated. From Figure 13, it can be found that as the number of wetting-drying cycle increases, electrical resistivity shows hysteresis loop against void ratio. For the case of EMC ± 5%, the size of hysteresis loop reduces obviously with a movement to the negative axis of the coordinate. Moreover, the first wetting-drying cycle has the major impact on the size reduction of hysteresis loop, and the effect of the rest four cycles is relatively small. This phenomenon is possibly due to that the evolution of soil structure tends to be stable. When cyclic amplitude of wetting-drying reduces from EMC ± 5% to EMC ± 1%, the hysteresis loop gradually shrinks and disappears. It can be deduced that the cyclic amplitude has great influence on the wetting-drying effect.Figure 13
Relationship between void ratio and electrical resistivity during wetting-drying cycles.Figure 14
Relationship between degree of saturation and electrical resistivity during wetting-drying cycles.For degree of saturation, similar hysteresis phenomenon can be observed from Figure14. While the size of hysteresis loop nearly remains the same, the position continuously moves towards low electricity resistivity position. This can be related to the hysteresis effect of water retention characteristics of clay. It can be also obtained that at the equilibrium position, the influences of wetting-drying cycles on void ratio and degree of saturation are tiny.In this study, all compacted soil specimens are unsaturated during the whole test procedures. The resistivity of unsaturated soil is dominated by porosity, pore structure, degree of saturation, properties of pore fluid, diffuse double layer of clay, temperature, and other factors [22, 23]. For specimens with moisture content of 17% undergoing different wetting-drying cycles, the changes of degree of saturation and pore fluid can be neglected. Besides, the effect of temperature on electrical resistivity can be ignored due to the temperature correction.Consequently, the evolution of volumetric strain and apparent density of specimens with wetting-drying cycles are plotted in Figures15 and 16, respectively. It can be observed from Figure 15 that the volumetric strain of specimens EMC ± 5% and EMC ± 3% shows slight swelling, while specimen EMC ± 1% can be considered slightly shrinking. Larger cyclic amplitude of wetting-drying allows the clay larger suction range history. More aggregates and micropores were generated during the wetting-drying cycle, which causes the slight swelling. But overall, volumetric strain and the change of density of specimens are very small. In other words, the influence of porosity change on electrical resistivity is very limited for each end of wetting-drying cycle. This is in accordance with results shown in Figure 13.Figure 15
Variations of volumetric strain with wetting-drying cycles.Figure 16
Variations of rate of apparent density change with wetting-drying cycles.Based on electrical model for unsaturated soil proposed by Rhoades et al. [35], there are three electrical conductance elements in unsaturated soil, namely, solid element, liquid element, and solid-liquid series-coupled element, as shown in Figure 17. The contribution of solid element is limited as a result of very low conductivity of clay mineral [22]. The liquid element can be also divided into water in diffuse double layer and water in pores or free water. The effect of diffuse double layer mainly depends on characteristics of bulk solution in soil and proportion of clay particle [36]. By ignoring the solution of clay particle, the concentration of bulk solution in soil may keep constant as the same moisture content at the end of each wetting-drying cycle. In addition, proportion of clay particle can be treated a constant value without any pressure on soil. So, it can be deduced that the diffuse double layer would appear to have relatively little role to play on electrical resistivity. As known that the conductivity of pore fluid is far larger than soil particle, the increase of fluid element can reduce the electrical resistivity. In other words, it can be achieved mainly by improving the connectivity of pore fluid. Under the premise of constant moisture content, volume, and porosity, the variation of pore structure may improve the connectivity of pore fluid. Hence, the pore structure can be the most likely factor affecting the electrical resistivity during wetting-drying cycles. Bodner et al. [11] have reported that cyclic wetting-drying can decrease the pore range and increase pore size, where the properties of tested soil are similar to this study. Moreover, Ma et al. [37] also found that proportion of large-sized pores is increased after wetting-drying cycles for Quaternary red clay. As discussed above, surface cracks can be observed on the specimens after failure shown in Figure 10, and similar deduction can be obtained that wetting-drying cycles can produce more macropores or cracks in clay due to increasing large-sized pores. Increasing large size pores and decreasing small size pores may lead to pore fluid transporting from small pores to large pores. Here, it can be also deduced that the proportion of fluid element is increased under the condition of constant porosity. Thus, the electrical resistivity of soil reduces as shown in Figure 12. It should be noted that larger cyclic amplitude of wetting-drying has greater impact on the pore structure of soil and consequently causes more reduction in electrical resistivity.Figure 17
Schematic illustration of three electrical conductance elements in unsaturated soil: (a) solid-liquid series-coupled element, (b) liquid element, and (c) solid element.


### 3.4. Relationship between Soil Strength and Electrical Resistivity

The relationship between electrical resistivity and unconfined compressive strength of soil is presented in Figure18. The unconfined compressive strength shows a linear growth with the increasing electrical resistivity for constant cyclic amplitude of wetting-drying cycles. In the last section, it has been discussed that the reduction of electrical resistivity of soil reveals an irreversible structure change in soil dominated by development of large pores. However, this process also promotes transfixion of more macrocracks and weakens the continuity of soil skeleton, leading to poor mechanical behaviour of soil. Thus, it can be suggested that electrical resistivity is suitable to indirectly reveal the mechanical behaviour of compacted unsaturated soil under cyclic wetting-drying in this study.Figure 18
Relationship between electrical resistivity and unconfined compressive strength.


## 3.1. Effect of Dry Density and Moisture Content on Soil Electrical Resistivity

The electrical resistivity of compacted clay with different dry densities and moisture contents is presented in Figure7. As shown in the figure, the electrical resistivity of soil with the same dry density is obviously decreased when the moisture content increases. Also, for soil specimens with the same moisture content, higher dry density can cause smaller electrical resistivity. These results are in accordance with previous studies [25] as presented in Figure 7, and it can be proved that the testing method of soil electrical resistivity in this study is reliable. Figure 8 presents the variation of electrical resistivity with degree of saturation. It can be seen that the electrical resistivity decreases as the degree of saturation increases.Figure 7
Variations of electrical resistivity with moisture content and degree of compaction.Figure 8
Variations of electrical resistivity with degree of saturation.


## 3.2. Effect of Wetting-Drying Cycles on Soil Strength

Before the unconfined compression tests, the moisture content of specimens was controlled the same, i.e., MC = EMC. The actual degree of saturation (Sr) data of specimens used in unconfined compression tests are presented in Table 2. It can be seen that Sr falls in the range of 84.4% to 86.7% for different specimens. It is known that the suction of soil changes slightly due to variations of degree of saturation in high moisture content conditions [33]; thus, it can be assumed that differences of suction between specimens were very limited, and the effect of suction on soil strength can be neglected at equilibrium moisture content.Table 2
Actual degree of saturation of specimens at EMC.
Number of wetting-drying cycles
Degree of saturation,Sr (%)
EMC ± 1%
EMC ± 3%
EMC ± 5%
1
84.8
86.4
84.4
2
86.0
86.6
86.0
3
86.8
85.7
85.1
4
86.6
85.1
84.9
5
85.3
85.9
84.4The effect of number and cyclic amplitude of wetting-drying cycles on unconfined compressive strength (UCS) of soil is shown in Figure9. It can be seen that the soil strength reduces with larger number of wetting-drying, and after 3-4 cycles, the soil strength tends to be constant. Additionally, greater reduction in soil strength can be observed with larger cyclic amplitude of wetting-drying. After the 5th wetting-drying cycles, the soil strength can be decreased by 19%, 20%, and 56% compared to that of noncycle specimen for cyclic amplitude of EMC ± 1%, EMC ± 3%, and EMC ± 5%, respectively.Figure 9
Effect of wetting-drying cycles on unconfined compressive strength of soil.Furthermore, typical photos of specimens after failure undergoing five cycles are presented in Figure10. With larger cyclic amplitude of wetting-drying, more cracks can be found on the surface of specimen after failure and the width of cracks increases apparently. From the point of view of damage mechanics, the growth and development of macrocracks are related to properties of microcracks and material structure change [34]. For unsaturated clay, cracks occur when the tensile stress induced by the developed suction exceeds the tensile strength of the specimen during drying path. Some cracks can be repaired in wetting path. However, irreversible soil structure change can result in accumulation of cracks after wetting-drying cycles [15]. Larger suction range suggests more crack accumulation. Thus, it can be deduced that more microcracks are caused by wetting-drying cycles with larger cyclic amplitude. If the degradation of soil strength is treated as a result of soil damage, the process of soil damage can be the evolution of microcracks and soil structure. It can be also suggested that large fluctuation of soil moisture content could generate significant decline of soil strength. Thus, waterproof and drainage facilities in compacted soil structures appear very important, and more attentions should be paid on the design and construction of hydraulic buffer or hydraulic barrier to reduce fluctuation of moisture content in soil.Figure 10
Photos of specimens after failure undergoing five wetting-drying cycles: (a) cyclic amplitude EMC ± 1%; (b) cyclic amplitude EMC ± 3%; (c) cyclic amplitude EMC ± 5%.
(a)
(b)
(c)


## 3.3. Effect of Cyclic Wetting-Drying on Soil Electrical Resistivity

The influences of cyclic wetting-dryings on soil electrical resistivity are presented in Figures11 and 12. Here, soil moisture content of specimens at the start point is EMC = 17%. It can be seen from Figure 11 that in each cycle, the soil electrical resistivity firstly decreases, then increases to a peak value, and finally drops to around the initial value. The variations of electrical resistivity are in negative correlation with moisture content. In addition, the soil electrical resistivity shows a fluctuant downward trend with more wetting-drying cycles. Moreover, the higher fluctuation of electrical resistivity can be recognized on specimens subjected to larger cyclic amplitude. It can be also observed that electrical resistivity at maximum moisture content shows a declining trend within the first three wetting-drying cycles. After the 3rd cycle, the electrical resistivity at maximum moisture content becomes stable, while the impact of wetting-drying cycles on the electrical resistivity at minimum moisture content is very small.Figure 11
Evolutions of soil electrical resistivity with wetting-drying cycles.Figure 12
Variations of final electrical resistivity with wetting-drying cycles.For better comparison of electrical resistivity for each wetting-drying cycle, electrical resistivity at moisture content 17% (i.e., the end point) for each cycle is plotted in Figure12. Overall, the electrical resistivity of soil decreases rapidly at the first three cycles and becomes a constant value after 3-4 cycles except the cyclic amplitude EMC ± 5%. The increase of cyclic amplitude contributes to the reduction of electrical resistivity, especially after three wetting-drying cycles. It can be suggested from the above results that the electrical resistivity of compacted soil can be greatly reduced by wetting-drying cycles.Figures13 and 14 illustrate variations of void ratio and degree of saturation during wetting-drying cycles. In the figures, numbers of wetting-drying cycle and the approximate equilibrium position are indicated. From Figure 13, it can be found that as the number of wetting-drying cycle increases, electrical resistivity shows hysteresis loop against void ratio. For the case of EMC ± 5%, the size of hysteresis loop reduces obviously with a movement to the negative axis of the coordinate. Moreover, the first wetting-drying cycle has the major impact on the size reduction of hysteresis loop, and the effect of the rest four cycles is relatively small. This phenomenon is possibly due to that the evolution of soil structure tends to be stable. When cyclic amplitude of wetting-drying reduces from EMC ± 5% to EMC ± 1%, the hysteresis loop gradually shrinks and disappears. It can be deduced that the cyclic amplitude has great influence on the wetting-drying effect.Figure 13
Relationship between void ratio and electrical resistivity during wetting-drying cycles.Figure 14
Relationship between degree of saturation and electrical resistivity during wetting-drying cycles.For degree of saturation, similar hysteresis phenomenon can be observed from Figure14. While the size of hysteresis loop nearly remains the same, the position continuously moves towards low electricity resistivity position. This can be related to the hysteresis effect of water retention characteristics of clay. It can be also obtained that at the equilibrium position, the influences of wetting-drying cycles on void ratio and degree of saturation are tiny.In this study, all compacted soil specimens are unsaturated during the whole test procedures. The resistivity of unsaturated soil is dominated by porosity, pore structure, degree of saturation, properties of pore fluid, diffuse double layer of clay, temperature, and other factors [22, 23]. For specimens with moisture content of 17% undergoing different wetting-drying cycles, the changes of degree of saturation and pore fluid can be neglected. Besides, the effect of temperature on electrical resistivity can be ignored due to the temperature correction.Consequently, the evolution of volumetric strain and apparent density of specimens with wetting-drying cycles are plotted in Figures15 and 16, respectively. It can be observed from Figure 15 that the volumetric strain of specimens EMC ± 5% and EMC ± 3% shows slight swelling, while specimen EMC ± 1% can be considered slightly shrinking. Larger cyclic amplitude of wetting-drying allows the clay larger suction range history. More aggregates and micropores were generated during the wetting-drying cycle, which causes the slight swelling. But overall, volumetric strain and the change of density of specimens are very small. In other words, the influence of porosity change on electrical resistivity is very limited for each end of wetting-drying cycle. This is in accordance with results shown in Figure 13.Figure 15
Variations of volumetric strain with wetting-drying cycles.Figure 16
Variations of rate of apparent density change with wetting-drying cycles.Based on electrical model for unsaturated soil proposed by Rhoades et al. [35], there are three electrical conductance elements in unsaturated soil, namely, solid element, liquid element, and solid-liquid series-coupled element, as shown in Figure 17. The contribution of solid element is limited as a result of very low conductivity of clay mineral [22]. The liquid element can be also divided into water in diffuse double layer and water in pores or free water. The effect of diffuse double layer mainly depends on characteristics of bulk solution in soil and proportion of clay particle [36]. By ignoring the solution of clay particle, the concentration of bulk solution in soil may keep constant as the same moisture content at the end of each wetting-drying cycle. In addition, proportion of clay particle can be treated a constant value without any pressure on soil. So, it can be deduced that the diffuse double layer would appear to have relatively little role to play on electrical resistivity. As known that the conductivity of pore fluid is far larger than soil particle, the increase of fluid element can reduce the electrical resistivity. In other words, it can be achieved mainly by improving the connectivity of pore fluid. Under the premise of constant moisture content, volume, and porosity, the variation of pore structure may improve the connectivity of pore fluid. Hence, the pore structure can be the most likely factor affecting the electrical resistivity during wetting-drying cycles. Bodner et al. [11] have reported that cyclic wetting-drying can decrease the pore range and increase pore size, where the properties of tested soil are similar to this study. Moreover, Ma et al. [37] also found that proportion of large-sized pores is increased after wetting-drying cycles for Quaternary red clay. As discussed above, surface cracks can be observed on the specimens after failure shown in Figure 10, and similar deduction can be obtained that wetting-drying cycles can produce more macropores or cracks in clay due to increasing large-sized pores. Increasing large size pores and decreasing small size pores may lead to pore fluid transporting from small pores to large pores. Here, it can be also deduced that the proportion of fluid element is increased under the condition of constant porosity. Thus, the electrical resistivity of soil reduces as shown in Figure 12. It should be noted that larger cyclic amplitude of wetting-drying has greater impact on the pore structure of soil and consequently causes more reduction in electrical resistivity.Figure 17
Schematic illustration of three electrical conductance elements in unsaturated soil: (a) solid-liquid series-coupled element, (b) liquid element, and (c) solid element.


## 3.4. Relationship between Soil Strength and Electrical Resistivity

The relationship between electrical resistivity and unconfined compressive strength of soil is presented in Figure18. The unconfined compressive strength shows a linear growth with the increasing electrical resistivity for constant cyclic amplitude of wetting-drying cycles. In the last section, it has been discussed that the reduction of electrical resistivity of soil reveals an irreversible structure change in soil dominated by development of large pores. However, this process also promotes transfixion of more macrocracks and weakens the continuity of soil skeleton, leading to poor mechanical behaviour of soil. Thus, it can be suggested that electrical resistivity is suitable to indirectly reveal the mechanical behaviour of compacted unsaturated soil under cyclic wetting-drying in this study.Figure 18
Relationship between electrical resistivity and unconfined compressive strength.


## 4. Conclusion

An investigation of the effects of wetting-drying cycles on electrical resistivity and unconfined compressive strength of unsaturated compacted subgrade soil has been carried out. The AC two-electrode method was adopted for measuring the electrical resistivity of soil. The influences of number and cyclic amplitude of wetting-drying were both investigated in this study. From this study, it can be concluded as follows:(1)
The electrical resistivity of soil decreases with increasing moisture content at constant dry density and increasing dry density at constant moisture content.(2)
The soil strength reduces with larger number of wetting-drying, and after 3-4 cycles, the soil strength tends to be constant. Larger cyclic amplitude of wetting-drying results in more surface cracks after failure and significant decline of soil strength.(3)
The electrical resistivity shows a fluctuant downward trend with increasing number of wetting-drying cycles. Moreover, higher fluctuation of electrical resistivity is caused for specimens subjected to larger cyclic amplitude.(4)
The electrical resistivity decreases rapidly at the first three cycles and becomes a constant value after 3-4 cycles except the cyclic amplitude EMC ± 5%. The increase of cyclic amplitude contributes to the reduction of electrical resistivity, especially after three wetting-drying cycles.(5)
The void ratio and degree of saturation of specimen show a hysteresis loop against electrical resistivity with increasing number of wetting-drying cycle. The hysteresis effect can be reduced when cyclic amplitude of wetting-drying decreases from EMC ± 5% to EMC ± 1%.(6)
The influence of porosity change on electrical resistivity is very limited for each end of wetting-drying cycle. The change of pore structure of soil during wetting-drying cycles has an effect on the electrical resistivity.(7)
The unconfined compressive strength shows a linear growth with the increasing electrical resistivity for a constant cyclic amplitude of wetting-drying cycles. Electrical resistivity is suitable to indirectly reveal the mechanical behaviour of compacted unsaturated soil under cyclic wetting-drying.



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*Source: 3465327-2019-06-16.xml*