Energy absorption characteristics of cementsoil under confining pressure based on SHPB test
Changhui Gao^{1} , Qinyong Ma^{2}
^{1, 2}School of Civil Engineering and Architecture, Anhui University of Science and Technology, Huainan, 232001, P. R. China
^{2}Engineering Research Center of Underground Mine Construction, Ministry of Education, Anhui University of Science and Technology, Huainan, 232001, P. R. China
^{1, 2}Corresponding authors
Journal of Vibroengineering, Vol. 19, Issue 8, 2017, p. 61986207.
https://doi.org/10.21595/jve.2017.18562
Received 30 April 2017; received in revised form 14 July 2017; accepted 23 July 2017; published 31 December 2017
Cementsoil has been widely used for engineering application. However, no attention has been paid to the energy absorption characteristics of cementsoil under impact loading. In this paper, a series of split Hopkinson pressure bar (SHPB) tests have been conducted to explore the energy absorption characteristics of cementsoil, and the effects of confining pressure (from 0 to 2.0 MPa) and strain rate (from 130 to 172 s^{1}) on the absorbed energy and the energy absorbency rate are investigated. The results show that the energy evolution of cementsoil under confining pressure is found to be similar at different strain rate. Both the absorbed energy and the energy absorbency rate are influenced by the confining pressure. Moreover, both the absorbed energy and the energy absorbency rate increase at first and then remain stable at a certain value with the increase of confining pressure. In addition, the absorbed energy linearly increases with the incident energy increasing, and a similar tendency is found between the absorbed energy and the strain rate, yet no obvious effect on the energy absorbency rate by the strain rate. Moreover, the energy mechanism of cementsoil is explained from the perspective of failure modes of cementsoil specimen.
Keywords: cementsoil, absorbed energy, energy absorbency rate, confining pressure, strain rate, SHPB.
1. Introduction
The stabilization of soil with Portland cement has been successfully used for improving geotechnical performance in applications such as deep excavation, pavement base layers, slop protection and underground construction works, and so on [13], which presents great economic and environmental benefits. Stabilization in this way improves the strength and durability of soil, reduces noise and dust in the work environment, also, improves soil workability. Moreover, many researches have been done for the strength [4, 5], permeability [6, 7], erosion resistance [8, 9] of cementsoil. Those published works, however, were focused only on properties of cementsoil under static loads, no attention has been paid to the dynamic properties of cementsoil.
The study on dynamic properties of cementsoil has significant relation to the engineering applications. According to the literature [10], cementsoil is often used for rapid construction of airstrip base. When the airplane comes down to the ground at 240 km/h, a strong impact will be produced on cementsoil base. In addition, present foundation treated by cementsoil, adjacent to mechanical excavation or blasting construction, always involves cementsoil responses to impact loading. Of course, earthquake loading is subjected to construction made of cementsoil now and then. Besides, dynamic load is impacted on the foundation cementsoil, in essence, which is the embodiment of dynamic property of cementsoil under confining pressure. Thus, understanding the dynamic behavior of cementsoil under confining pressure is significant to dynamic analysis and design of foundation.
According to the laws of thermodynamics, energy conversion is the basis rule of physical processes of materials. For many materials such as rock [11, 12], concrete [13, 14], porous materials [15, 16], and other materials [1719], the essence of their damage and failure is the germination, extension, aggregation and connection of internal microcracks result in the deformation and failure under the driving of energy [20]. Energy plays an important role in deformation and failure of materials. Therefore, research of the energy absorption characteristics of cementsoil under impact loading is of great significance to evaluate the mechanism of energy evolution and antiimpact ability, which is of certain theoretical significance and practical value.
In this paper, a series of SHPB tests are carried out to investigate the energy absorption characteristics of the cementsoil under five kinds of confining pressures (0, 0.5, 1.0, 1.5 and 2.0 MPa), and the impact pressures are from 3.0 to 4.5 MPa (corresponding to different strain rates). The effect of confining pressure and strain rate on the energy absorption characteristics of the cementsoil, including the absorbed energy, the incident energy, and the energy absorbency rate, are evaluated in this work.
2. Experimental program and energy calculation
2.1. Effectiveness analysis of test data
The Ø50 mm split Hopkinson pressure bar (SHPB) apparatus is adopted in the present work, and due to relatively low wave impedance of cementsoil, the semiconductor strain gauge is pasted on the transmitted bar to record the weak signal of transmitted wave. Confining pressure device is shown in Fig. 1.
Fig. 1. Confining pressure device
In order to clarify the effectiveness of test data, the propagation theory of onedimensional wave and uniform stress hypothesis need to be satisfied. To solve the problem of uniform stress in SHPB tests, some measures were taken and original waveform collected in SHPB test is shown in Fig. 2. As clear in Fig. 2, the halfsine wave pattern loading is achieved and the waveform is smooth. It also can be found that the time of the rising edge of incident pulse is about 0.14 ms, and the time of duration is about 0.4 ms. So, the number of transmissionreflection cycles (${c}_{tf}$) for stress pulse in cementsoil specimen can be calculated by the following Eq. (1) as:
where ${t}_{r}$ is the time of the rising edge of incident pulse (about 0.14 ms), ${t}_{tf}$ is the time of one transmissionreflection cycle for stress pulse in cementsoil specimen.
And, ${t}_{tf}$ can be expressed as:
where $h$ is the length of specimen (0.025 m), $v$ is the propagation velocity of stress pulse in cementsoil (about 1450 m/s), so the ${t}_{tf}$ is 0.0345 ms.
Finally, ${c}_{tf}$ can be obtained by calculation as:
Thus, there is enough time to achieve uniform stress state for cementsoil specimen.
Fig. 2. Original waveform (${C}_{p}=$ 2.0 MPa, ${I}_{p}=$ 0.3 MPa). ${C}_{p}$ – confining pressure; ${I}_{p}$ – impact loading pressure (below)
The theory of onedimensional wave requires $\lambda =ct>5d$[21], where $\lambda $ is the width of incident stress pules, $c$ is Pwave velocity (5190 m/s), $t$ is the propagation time of stress pulse (0.04 ms), $d$ is the diameter of specimen (0.05 m). It can be obtained by calculation as:
Therefore, the theory of onedimensional wave can be clarified.
2.2. Materials
The silty clay tested in this investigation was obtained from foundation and its physical properties and grain size distribution are shown in Table 1 and Table 2, respectively. Ordinary Portland cement (P·O 42.5) was used as the binding agent in this work. Distilled water was used for specimen preparation.
Table 1. Basic physical properties of silty clay
Liquid limit (%)

Plasticity limit (%)

Plasticity index

Optimum moisture content (%)

Maximum dry density (g·cm^{3})

35.40

23.82

11.58

22.40

1.69

Table 2. The grain size distribution of silty clay
Grain size (mm)

Content (%)

Grain size (mm)

Content (%)

$d\le $0.005

19.54

0.005$d\le $0.075

40.23

0.075$d\le $ 0.25

12.70

0.25$d\le $0.5

16.05

0.5$d\le $ 1

9.08

1$d\le $2

2.40

2.3. Methods of energy calculation
Absorbed energy (${W}_{S}$), which is the capacity to absorb energy of stress wave for cementsoil per unit volume, can be expressed as follow:
where ${W}_{I}$, ${W}_{R}$ and ${W}_{T}$ are_{}the energy of incident wave, reflected wave and transmitted wave, respectively, they can be calculated through Eq. (6):
where $E$, $C$, and $A$ are the Young’s modulus, Pwave velocity and the crosssectional area, respectively; ${\epsilon}_{I}\left(t\right)$, ${\epsilon}_{R}\left(t\right)$ and ${\epsilon}_{T}\left(t\right)$ are the strain of incident wave, reflected wave, and transmitted wave, respectively; $t$ is the duration time of elastic wave.
3. Results and discussion
3.1. Relationship between the absorbed energy and the incident energy
Through Eq. (5) and (6), the representative energytime curve of cementsoil is obtained and shown in Fig. 3. In the initial loading, the incident energy increase rapidly with the propagation of stress wave, but the absorbed energy of cementsoil has a slight increase with the extension of stress wave. That is because most of incident energy is reflected back into incident bar, some is absorbed by cementsoil specimen, and only a small percentage of incident energy is transferred to transmitted bar [22]. It also can be seen that the time duration of the stress wave is about 0.35 ms, and the values of incident energy and absorbed energy maintain stable after reaching a certain time about 0.275 ms, which means the failure of cementsoil specimen.
Fig. 4 shows the relationship between the incident energy and the absorbed energy of cementsoil in SHPB test. From Fig. 4, the absorbed energy of cementsoil under different confining pressure increase with the increase of incident energy, and there is a good liner relationship between the incident energy and absorbed energy, which can be expressed as Eq. (7):
where ${W}_{s}$ and ${W}_{I}$ are the absorbed energy and incident energy, respectively; $a$ and $b$ are the parameters of fitting equation. The values of $a$, $b$ and ${R}^{2}$ are listed in Table 3 (for the range of incident energy is from 50 to 120 J).
Fig. 3. Energytime curve of the cementsoil (${C}_{p}=$2.0 MPa, ${I}_{p}=$0.3 MPa)
Fig. 4. Relationship between the incident energy and the absorbed energy
3.2. Absorbed energy of cementsoil
The absorbed energy under different confining pressure have been calculated and the relationship between the absorbed energy and confining pressure is shown in Fig. 5. It can be observed that absorbed energy is sensitive to the value of confining pressure, and the relationship between absorbed energy and confining pressure is also influenced by the change of strain rate.
Table 3. Values of $a$, $b$ and correlation coefficient ${R}^{2}$
Confining pressure (MPa)

$a$

$b$

${R}^{2}$

0

–2.33

0.10

0.94

0.5

–2.55

0.11

0.93

1.0

1.35

0.12

0.91

1.5

2.14

0.11

0.81

2.0

–2.94

0.16

0.96

As clear in Fig. 5, the absorbed energy increases firstly and then remains stable at a certain value with the increase of the confining pressure, which the turning point is 1.0 MPa of the confining pressure. For example, at the strain rate of 152 s^{1}, the absorbed energy increase from 4.51 to 9.83 J with the confining pressures increasing from 0 to 1.0 MPa, after that, there is a relatively steady trend for the value of absorbed energy when the confining pressure is more than 1.0 MPa. In addition, the cementsoil specimens have fairly great improvement in the value of absorbed energy under confining pressure compared with that of uniaxial condition (${C}_{p}=$0 MPa). It can be observed that the absorbed energy increase from 5.56 to 12.87 J with the confining pressures increasing from 0 to 1.0 MPa at strain rate of 160 s^{1}, which causes an increase of 131.47 %.
The scatter diagram between absorbed energy and strain rate is shown in Fig. 6. All of groups show a similar trend that with the increase of strain rate, absorbed energy of cementsoil specimen increases. After data fitting, the relationship between the absorbed energy and strain rate can be assumed to be liner, and which can be expressed as Eq. (8):
where ${W}_{s}$ is the absorbed energy of cementsoil specimen, $\alpha $ and $\beta $ are the parameters of fitting equation. The values of $\alpha $, $\beta $ and ${R}^{2}$ are listed in Table 4 (for the range of strain rate is from 130 to 180 s^{1}). Most of the values of ${R}^{2}$^{}of fitting curves are more than 0.90, that is to say, Eq. (8) can well be described the strain rate sensitivity of the absorbed energy of cementsoil.
Fig. 5. Absorbed energy versus confining pressure
Fig. 6. Absorbed energy versus strain rate
Table 4. Values of $\alpha $, $\beta $ and correlation coefficient ${R}^{2}$
Confining pressure (MPa)

$\alpha $

$\beta $

${R}^{2}$

0

–18.74

0.15

0.99

0.5

–9.62

0.11

0.91

1.0

–8.48

0.13

0.80

1.5

–5.47

0.11

0.89

2.0

–11.85

0.15

0.92

3.3. Energy absorbency rate of cementsoil
In order to measure the absorption efficiency of cementsoil under confining pressure, the energy absorbency rate $\eta $ can be defined by Eq. (9):
where ${W}_{s}$ and ${W}_{I}$ are the absorbed energy and the incident energy, respectively.
Fig. 7 shows the comparison of the energy absorbency rate of cementsoil with different confining pressure and strain rate. It is can be seen that the confining pressure has an effect on the average value of energy absorbency rate. From Fig. 7(a), compared with uniaxial condition, the energy absorbency rate of cementsoil specimen has a significantly increase under confining pressure, but it shows no remarkable change when the value of confining pressure is from 1.0 to 2.0 MPa, which settles around a range of values about 12.0 %14.0 %. By examining Fig. 7(b), there is no obvious regularity between the energy absorbency rate and strain rate.
Fig. 7. Relationship among the confining pressure, strain rate and the energy absorbency rate
a)
b)
3.4. Discussion of energy mechanism for cementsoil
Test results both in this paper and of other studies [2325] conclude that both the absorbed energy and the energy absorbency rate of the materials are influenced by the confining pressure. As for cementsoil tested in this work, its absorbed energy increases firstly and then decreases with the increase of the value of confining pressure, and so does the energy absorbency rate. The effect mechanism of confining pressure on energy absorption characteristics of cementsoil can be expressed as follow:
The critical state confining pressure, which is varies for different kinds of material, has been proposed in the previous literatures [26, 27]. There has a difference in the state of low confining pressure and high confining pressure for rock and soil as well as cementsoil. Specifically, both the absorbed energy and the energy absorbency rate of cementsoil increase with the increase of confining pressure when the values of confining pressure is lower than the critical state confining pressure, while the confining pressure show a negative effect on energy absorption when it is over the critical state confining pressure. In this paper, for cementsoil under confining pressure, a value of critical state confining pressure, about 1.0 MPa, is founded. Both the absorbed energy and the energy absorbency rate increase with the increase of confining pressure from 0 to 1.0 MPa, and then remain stable at a certain value with further increase of confining pressure. Such a similar result was presented by Jin [28]. Analyzing the causes, the counterforce during the lateral deformation of specimen under impact load increases with the value of confining pressure increasing, and then it is difficult for cracks inside of specimen to extend so that the absorbed energy of specimen keeps steady gradually [29]. On a macro level, the result of this behavior shows a smaller energy absorbency rate for cementsoil.
Compared with the uniaxial condition, the values of absorbed energy and the energy absorbency rate of cementsoil under confining pressure have a significant increase. Due to the energy absorption characteristics are closely related to the failure mode of specimen, so it can be explained through Fig. 8 and Fig. 9 that show the failure modes of cementsoil under different stress state. The cementsoil specimen under uniaxial state is broken into fragments, however, a better integrity for specimen is maintained under confining pressure state. Previous research showed that the initiation and propagation of fracture crack and deformation of specimen are limited under confining pressure state [30], so if the cementsoil specimen want to reach its failure state, more energy should be absorbed. That is to say, the confining pressure strengthens the capacity of energy absorption for cementsoil [31]. Thus, the absorbed energy and the energy absorbency rate increase naturally.
Fig. 8. Failure modes of cementsoil under confining pressure
a)${C}_{p}=$ 0.5 MPa, strain rate 130 s^{1}
b)${C}_{p}=$ 1.5 MPa, strain rate 152 s^{1}
Fig. 9. Failure modes of cementsoil under uniaxial condition
a) strain rate 152 s^{1}
b) strain rate 160 s^{1}
c) strain rate 172 s^{1}
d) strain rate 180 s^{1}
Many researches [17, 32] including this work show that the absorbed energy of cementsoil specimen is also related to the strain rate. In other words, the higher the strain rate, the more energy is absorbed for specimen. The strain rate effect on the absorbed energy of cementsoil is simply summarized in this paper.
In general, the value of strain rate has a positive correlation with impact loading pressure, so the higher the strain rate, the higher the impact loading pressure, which also means that incident energy increases gradually. Combining with the analysis in Section 3.1 and it can be found that the more energy is absorbed by cementsoil specimen with the increase of incident energy.
Mechanism of the strain rate effects on the energy absorption of cementsoil can also be explained through the failure modes of cementsoil specimen. As shown in Fig. 9, with the increasing of strain rate, the grain size of fragments becomes smaller and the number of fragments increases, which means the higher the damage degree of cementsoil specimen. From the perspective of microcracks and energy absorption of materials [33], the expansion of internal microcrack and the generation of new fracture surface of cementsoil is a process of absorbing energy for cementsoil. The more serious the damage degree of cementsoil specimen is, the more energy of specimen is absorbed.
4. Conclusions
The energy absorption characteristics of cementsoil under confining pressure were studied for the first time. Based on SHPB test, the effects of confining pressure (from 0 to 2.0 MPa) and strain rate (from 130 to 172 s^{1}) on the absorbed energy and the energy absorbency rate are investigated. The absorbed energy and the energy absorbency rate of cementsoil are shown to be significantly affected by the value of confining pressure. Both the absorbed energy and the energy absorbency rate increase at first and then remain stable at a certain value with the increase of the value of confining pressure. The maximum value of the absorbed energy and the energy absorbency rate appear on the confining pressure of 1.0 MPa. The absorbed energy of cementsoil is sensitive to the strain rate, but the relationship between the energy absorbency rate and strain rate is not obvious. The more energy of cementsoil specimen is absorbed, the more serious the damage degree of specimen is. In addition, the values of absorbed energy and the energy absorbency rate of cementsoil under confining pressure have a significant increase compared with the uniaxial condition. There is a liner relationship between the absorbed energy and incident energy for cementsoil, and a similar tendency is also found between the absorbed energy and the strain rate.
Acknowledgements
Thanks to the Engineering Research Center of Underground Mine Construction, Ministry of Education and the Anhui University of Science and Technology, for providing the experiment conditions.
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