Shot Peening Processes to obtain Nanocrystalline surfaces in metal alloys:


 

  H. Bai et alii, Frattura ed Integrità Strutturale, 56 (2021) 16-45; DOI: 10.3221/IGF-ESIS.56.02                                                                        

 

16 

 

 

 
 
 
  
Experimental investigation of cracking behaviors of ductile and 
brittle rock-like materials 
 
 
Hao Bai, Wei Du* 
Sichuan Expressway Construction & Development Group Co., LTD, Chengdu, China 
secdcbh@126.com 
582126107@qq.com 
 

Yundong Shou*, Lichuan Chen 
National Breeding Base of Technology and Innovation Platform for Automatic-monitoring of Geologic Hazards (Chongqing 
Engineering Research Center of Automatic Monitoring for Geological Hazards), Chongqing, China 
Wuhan University, China 
shouyundong@whu.edu.cn, https://orcid.org/0000-0001-7424-4006 
chen_lichuan@163.com 
 

Filippo Berto 
Norwegian University of Science and Technology, Norway 
filippo.berto@ntnu.no 
 

 
ABSTRACT. The cracking characteristics of ductile rocks were studied by 
similar materials with sand, barite, epoxide resin, polyamide, silicone rubber 
and alcohol, while the cracking characteristics of brittle rocks were 
investigated by similar material with sand, barite, rosin and alcohol. In this 
paper, to enhance the application range of the rock-like materials in the field 
of geotechnical engineering model tests, the values of the elastic modulus and 
the compressive strength of the artificial rock-like materials are changed in a 
wide range by adjusting the amount of cementitious materials (epoxide resin, 
polyamide, rosin, etc). The elastic modulus, compressive strength and cracking 
characteristics were obtained from the complete axial stress–strain curves of 
the specimens made of similar materials, which were cast using the different 
mixture ratios. These experimental data can provide quantitative investigation 
on mixture ratios of similar materials of rocks to model the geotechnical 
engineering. Furthermore, the effect of mixture ratios on mechanical 
properties and crack propagation pattern of specimens were also investigated 
by the specimens with pre-existing flaws under uniaxial compressive tests.  
  
KEYWORDS. Rock-like materials; Material composition; Ductility; Brittleness; 
Crack evolution. 
 

 

 
 

Citation: Bai, H., Du, W., Berto, F., 
Experimental investigation of cracking 
behaviors of ductile and brittle rock-like 
materials, Frattura ed Integrità Strutturale, 56 
(2021) 16-45. 
 
Received: 02.01.2021  
Accepted: 17.01.2021  
Published: 01.04.2021  
 
Copyright: © 2021 This is an open access 
article under the terms of the CC-BY 4.0, 
which permits unrestricted use, distribution, 
and reproduction in any medium, provided the 
original author and source are credited. 

 

https://youtu.be/PKi-k_hsMbg


 

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INTRODUCTION 
 

he similar simulation test in rocks on the basis of the similarity theory of modeling test is an explorative method to 
study the mechanical properties of geotechnical materials. The mechanical phenomena and the stress-strain variation 
characteristics of prototype are analyzed through the observation of stress and strain on similar models casted by 

using single or multiple materials, which provides a more reasonable scientific basis for the design of the geotechnical 
engineering and the selection of the construction scheme. 
In similar model experimental studies, the ratio of similar materials and the casting method of test models have a great 
influence on the physical and mechanical properties of the material, which plays a decisive role in the success of similar 
simulation tests. For a long period of time, the geotechnical similar simulation test has been an important means of solving 
complex engineering problems. It can not only study the normal stress state of engineering, but also acquire the ultimate 
load and failure modes of engineering. Meanwhile, compared with the numerical calculation, the results given by similar 
simulation tests are more intuitive and can give people a deeper impression, and are widely used in geotechnical engineering 
research. 
The cracking mechanisms of rocks have been studied experimentally on rock-like materials or rock materials, and rock-like 
materials are widely used because the flaws are easy to be fabricated. The first experimental study on rock-like specimens 
that contained flaws under uniaxial compression condition was conducted by Brace and Bombolakis [1]. Since then, many 
studies have examined the fracture processes of pre-cracked rock-like materials subjected to compression. Experimental 
studies have been performed on many different types of rock-like materials, including glass [2,3], Columbia Resin [4], 
polymethyl methacrylate [5,6], cement mortar [7], sandstone-like composite material [8-11], and gypsum [12-18]. To 
investigate the initiation, propagation, and coalescence of cracks in real rock materials, some experiments and numerical 
simulation on rock such as granite [19-21], marble [17-18,22] and mudstone [23] have also been conducted. Zhou et al. [24] 
and Bi et al. [25] proposed General Particle Dynamics to simulate the crack initiation, growth and coalescence in rock or 
rock-like materials. Wang et al. [26-27] developed the conjugated bond-based peridynamics to investigate the cracking 
behaviors in rock or rock-like materials. Zhou et al. [28-29] established micromechanics-based model to study the damage 
mechanism of rocks. Zhou et al.[30] investigated the initiation, growth and coalescence of 3D crack in rock-like rocks. the 
cracking behaviors in rock or rock-like materials. Zhou et al. [30] and Zhang et al. [31-34] studied progressive failure of 
brittle rocks with non-isometric flaws. Such rock-like materials and real rock materials have not only common characteristics 
for crack evolution, but also differences caused by the material properties, loading methods, and specimen geometry [35-
36]. 
Moreover, since rock is a very complex and anisotropic material whose mechanical properties vary widely, ranging from 
hard rock with very high mechanical properties to soft rock with very low mechanical properties [30-36]. However, there is 
scarce study on the cracking behaviors and mechanical properties of ductile and brittle rock-like materials. 
To simulate different kinds of rock with a wide range of intensity variation, a new type of rock-like material with wide-
ranging and stable mechanical properties must be developed. In this paper, the certain raw materials were selected according 
to the mechanical properties of ductile and brittle rocks and the mechanical laws of ductile and brittle rock-like materials 
were obtained by experimental analysis of materials with different ratios, which provides a reference for the ratio of rock-
like materials in experiments. In addition, two rock-like materials were applied to crack propagation experiment, and the 
influence rules of different ratios of rock-like materials on crack propagation modes and mechanical properties of the 
specimens were obtained. 

 
 
EXPERIMENTAL STUDIES 
 
Specimen preparation 

he composition of the raw materials used to make similar models can be basically divided into three categories 
according to their use: the first one is filling material acted as the skeleton, the second one is cementing material that 
plays a role in bonding, and the third one is auxiliary admixture served as regulation of physical and mechanical 

properties. In similar simulation experiments, in order to make the similar model satisfy requirements of the volumetric 
weight similarity ratio, it is more common to use barite, gypsum, sand, iron powder as the filling material. There are also 
many cementitious materials commonly used as bonding materials like gypsum, white latex, epoxide resin, polyamide, 
cement, rosin, etc. At the same time, for the purpose of adjusting the physical and mechanical properties of rock-like 
materials to better simulate the actual rock, it is essential to add additional auxiliary agents, such as silicone rubber, lime, 

T 

T 



 

  H. Bai et alii, Frattura ed Integrità Strutturale, 56 (2021) 16-45; DOI: 10.3221/IGF-ESIS.56.02                                                                        

 

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neoprene, glycerin (humectant), borax (retarder) mica powder, softwood chips, etc. Furthermore, to make rock-like materials 
isotropic and homogeneous after hardening molding, it is also necessary to incorporate a certain amount of organic solvent, 
including frequently-used gasoline, engine oil, alcohol, etc. And its purpose is to dissolve organic substances such as silicone 
rubber, so that the components can be more uniformly mixed.  
In this paper, the experiment was designed to prepare rock-like materials which could simulate ductile and brittle rocks. 
Initially some raw materials are selected as rock-like materials. After that tentative raw materials are added for trial matching. 
Eventually, the preparative rock-like materials are tested in uniaxial compression in order to figure out whether the full 
stress-strain curve of the rock-like materials is similar to the corresponding curve of actual rocks.  
When simulating the raw material composition of ductile rock-like materials, it was finally decided to use sand and barite 
as filling materials. Moreover, epoxide resin and polyamide were used as cementitious materials, silicone rubber and rosin 
were used as auxiliary adjusting agents, and alcohol was used as organic solvent. The force-displacement curve of whole 
process in uniaxial compression test for ductile rock-like material is shown in Fig. 1. With regard to brittle rock-like 
materials, sand and barite were used as filling materials, rosin was used as cementitious material, silicone rubber, epoxide 
resin and polyamide were used as auxiliary adjusting agents, and alcohol was used as organic solvent. Fig. 1 and Fig. 2 are 
the force-displacement curve of whole process in uniaxial compression test for ductile and brittle rock-like materials, 
respectively. 
 

 
Figure 1: Force-displacement curve of the uniaxial compression UCS test for ductile rock-like materials. 

 

 
Figure 2: Force-displacement curve of UCS test for brittle rock-like materials. 

  



 

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To obtain the experimental phenomena and make data reliable, two specimens for each ratio of materials were made and 
relevant test data was processed averagely. The ratio relationship of raw material is shown in Tabs. 1 and 2. 
 

Number Raw materials Weight ratio 
Percentage of variable 

components 

A1 Sand, barite, epoxy, polyamide and alcohol 500:300:4:4:40 59% (sand) 

A2 Sand, barite, epoxy, polyamide and alcohol 600:300:4:4:40 63.3% (sand) 

A3 Sand, barite, epoxy, polyamide and alcohol 700:300:4:4:40 66.8% (sand) 

A4 Sand, barite, epoxy, polyamide and alcohol 800:300:4:4:40 69.7% (sand) 

B1 Sand, barite, epoxy, polyamide and alcohol 500:300:4:4:40 35.4% (barite) 

B2 Sand, barite, epoxy, polyamide and alcohol 500:350:4:4:40 39% (barite) 

B3 Sand, barite, epoxy, polyamide and alcohol 500:400:4:4:40 42.7% (barite) 

B4 Sand, barite, epoxy, polyamide and alcohol 500:450:4:4:40 45.1% (barite) 

C1 Sand, barite, epoxy, polyamide and alcohol 500:300:4:4:40 0.9% (epoxy and polyamide) 

C2 Sand, barite, epoxy, polyamide and alcohol 500:300:6:6:40 1.4% (epoxy and polyamide) 

C3 Sand, barite, epoxy, polyamide and alcohol 500:300:8:8:40 1.9%(epoxy and polyamide) 

C4 Sand, barite, epoxy, polyamide and alcohol 500:300:10:10:40 2.3%(epoxy and polyamide) 

D1 Sand, barite, epoxy, polyamide and alcohol 500:300:4:4:40 0% (silicone rubber) 

D2 
Sand, barite, epoxy, polyamide, alcohol and silicone 

rubber 
500:300:4:4:40:5 0.6% (silicone rubber) 

D3 
Sand, barite, epoxy, polyamide, alcohol and silicone 

rubber 
500:300:4:4:40:10 1.2% (silicone rubber) 

D4 
Sand, barite, epoxy, polyamide, alcohol and silicone 

rubber 
500:300:4:4:40:15 1.7% (silicone rubber) 

E1 Sand, barite, epoxy, polyamide and alcohol 500:300:4:4:40 0% (rosin) 

E2 Sand, barite, epoxy, polyamide, alcohol and rosin 500:300:4:4:40:2 0.2% (rosin) 

E3 Sand, barite, epoxy, polyamide, alcohol and rosin 500:300:4:4:40:4 0.5% (rosin) 

E4 Sand, barite, epoxy, polyamide, alcohol and rosin 500:300:4:4:40:6 0.7% (rosin) 

F1 
Sand, barite, epoxy, polyamide, alcohol and silicone 

rubber 
500:300:4:4:40:5 0% (rosin) 

F2 
Sand, barite, epoxy, polyamide, alcohol silicone 

rubber and rosin 
500:300:4:4:40:5:2 0.2% (rosin) 

F3 
Sand, barite, epoxy, polyamide, alcohol silicone 

rubber and rosin 
500:300:4:4:40:5:4 0.5% (rosin) 

F4 
Sand, barite, epoxy, polyamide, alcohol silicone 

rubber and rosin 
500:300:4:4:40:5:6 0.7% (rosin) 

 

Table 1: The raw materials and ratio of ductile rock-like materials. 
 

In the process of fabricating specimens, the raw materials were first weighed according to the ratio of each rock-like 
materials. At the same time, the mold was cleaned and assembled, and the inner surface of the mold was coated with an 
appropriate amount of lubricating oil so that the mold could be removed later. Subsequently the sand and barite powder 
were mixed evenly, and the rosin powder or the epoxide resin-polyamide was dissolved in alcohol to form an alcohol 
solution (which was thoroughly stirred and slightly heated with hot water to accelerate dissolution), then the alcohol solution 
was then added evenly to the already mixed mixture. Since silicone rubber was not easily dissolved in alcohol, it could only 
be slowly dispersed in the agitated material during agitation. Finally, the mixture was poured into the mold and tamped (the 
hammer was stopped when there was no obvious sinking during the hammering process). The specimens after pouring 
molding is shown in Fig. 3. 



 

  H. Bai et alii, Frattura ed Integrità Strutturale, 56 (2021) 16-45; DOI: 10.3221/IGF-ESIS.56.02                                                                        

 

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Number Raw materials Weight ratio 
Percentage of variable 

components 

A1' Sand, barite, rosin and alcohol 200:200:5:15 47.6% (sand) 

A2' Sand, barite, rosin and alcohol 250:200:5:15 53.2% (sand) 

A3' Sand, barite, rosin and alcohol 300:200:5:15 57.7% (sand) 

A4' Sand, barite, rosin and alcohol 350:200:5:15 61.4% (sand) 

B1' Sand, barite, rosin and alcohol 200:200:5:15 47.6% (barite) 

B2' Sand, barite, rosin and alcohol 200:250:5:15 53.2% (barite) 

B3' Sand, barite, rosin and alcohol 200:300:5:15 57.7% (barite) 

B4' Sand, barite, rosin and alcohol 200:350:5:15 61.4% (barite) 

C1' Sand, barite, rosin and alcohol 200:200:5:15 1.2% (rosin) 

C2' Sand, barite, rosin and alcohol 200:200:7:15 1.7% (rosin) 

C3' Sand, barite, rosin and alcohol 200:200:9:15 2.1% (rosin) 

C4' Sand, barite, rosin and alcohol 200:200:11:15 2.6% (rosin) 

D1' Sand, barite, rosin and alcohol 200:200:5:15 0% (epoxy and polyamide) 

D2' Sand, barite, rosin, alcohol, epoxy and polyamide 200:200:5:15:1:1 0.47% (epoxy and polyamide) 

D3' Sand, barite, rosin, alcohol, epoxy and polyamide 200:200:5:15:2:2 0.94% (epoxy and polyamide) 

D4' Sand, barite, rosin, alcohol, epoxy and polyamide 200:200:5:15:3:3 1.4% (epoxy and polyamide) 

E1' Sand, barite, rosin and alcohol 200:200:5:15 0% (silicone rubber) 

E2' Sand, barite, rosin, alcohol and silicone rubber 200:200:5:15:2 0.47% (silicone rubber) 

E3' Sand, barite, rosin, alcohol and silicone rubber 200:200:5:15:4 0.94% (silicone rubber) 

E4' Sand, barite, rosin, alcohol and silicone rubber 200:200:5:15:6 1.4% (silicone rubber) 

 

Table 2: The raw materials and proportion of brittle rock-like material. 

 

 

 

Figure 3: Prepared specimens. 



 

                                                                        H. Bai et alii, Frattura ed Integrità Strutturale, 56 (2021) 16-45; DOI: 10.3221/IGF-ESIS.56.02 

 

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Testing System 
In this paper, an electronic universal testing machine was used to carry out the uniaxial compression test of specimens. The 
test machine has two loading modes (load control and displacement control) which can automatically collect data throughout 
the test. In order to prevent the damage of the test machine caused by the sudden destruction of specimen and to ensure 
integrity of the stress-strain curve obtained by experiments, the loading mode of displacement control was selected in the 
experiments. The device used for testing the fracture toughness of rock-like materials consists of a loading device (electronic 
universal testing machine) and a bracket device (for supporting cylindrical specimens to meet the three-point bending 
loading requirements). 
In the process of processing the specimen, 1 mm wide crack was first machined on the specimen, then the crack tip was 
ground with a diamond wire saw to a diameter of 0.5 mm. In the test, the crack length is 10 mm (generally, the ratio of the 
crack length to the specimen diameter is 0.15 to 0.5), and the crack tip angle is 30° (the crack tip angle is generally required 
to be small enough to produce a relatively strong I-type stress filed), the ratio of span to diameter is 1.5 (the ratio of span 
and diameter of the specimen is relatively small when the material strength is low, generally 1.5 to 4). After the specimen 
was processed, the specimen was placed in the exact position of the test holder and was tested under loading by the electronic 
universal testing machine. During the loading process, the crack propagation and failure modes of the specimen were 
observed and recorded, and finally the maximum load at the time of crack propagation was recorded. The crack geometry 
and loading diagram of the specimen are shown in Fig. 4. 
 

 

Figure 4: Crack geometry and loading schematic. 
 
 

ANALYSIS OF EXPERIMENT RESULTS 
 

Analysis of experimental results of ductile rock-like materials 
Effect of raw materials on stress-strain curves and brittleness indexes of ductile rock-like materials 

enerally, the complete stress-strain curve of rocks can be used to qualitatively analyze the brittleness of rock. 
Therefore, based on the brittleness index of the full stress-strain curve, another brittleness index, namely “brittle 
modulus”, is obtained. Eqn. (1) is the calculation expression of the brittle modulus. 

 

 

 

−
=

−

0
0

0

c

c

E                                                                                 (1) 

were 

0E is the brittle modulus, 

 c is peak strength,  

 


+
= 10 2

c ,  0 is the strain corresponding to0 , 

c is the strain corresponding to c . 

Fig. 5 and Fig. 6 are respectively diagrams of the stress-strain curves and brittle modulus changes of ductile rock-like 
materials under different raw material ratios. Combining the failure process of the specimen and analyzing the curve change 
in the figure, it can be seen that:  

G 



 

  H. Bai et alii, Frattura ed Integrità Strutturale, 56 (2021) 16-45; DOI: 10.3221/IGF-ESIS.56.02                                                                        

 

22 

 

① when the amount of sand increases, the difference in the damage of the specimen is little. The reason may be that a large 
amount of cementitious material and barite has a certain ductility when the sand content is low, and the shear failure of the 
sand also has a certain ductility when the sand content is high.  

② When the barite content is relatively low, the specimen exhibits a certain ductility, and as the barite content increases, 
the ductility of the specimen is more pronounced. The reason is probably due to the fact that the cementitious materials, 
epoxide resin and polyamide, have a certain ductility, and the barite material itself also has good ductility when it is failed. 
When the barite content is relatively high, the specimen is mainly failed by the shear failure of sand and barite, and the barite 
itself has better ductility when it is failed.  

③ When the content of epoxide resin and polyamide is relatively low, the specimen has a certain ductility, and as the content 
of epoxide resin and polyamide increases, the ductility of the specimen is more obvious. The reason should be that the 
cementitious materials, epoxide resin and polyamide, have good ductility when they are dried and hardened.  

④ When the silicone rubber is not added, the specimen has a certain ductility, and the ductility of the specimen is more 
obvious as the amount of added silicone rubber increases. The reason is that the silicone rubber after coagulation hardening 
has a good ductility, which increases the ductility of the specimen.  

⑤ In the absence of silicone rubber, when the amount of rosin is 0, the specimen exhibits certain ductile failure properties, 
and as the amount of added rosin increases, the specimen no longer has good ductility, but exhibits brittle failure properties. 
The reason should be that the hardened rosin exhibits a distinct brittle character when it is failed, and ultimately changes 

the ductile failure properties of rock-like material itself. ⑥Under the condition of containing silicone rubber, when the 
amount of rosin is 0, the specimen also exhibits certain ductile failure properties, and as the amount of added rosin increases, 
the ductility of the specimen is not severely reduced. But only when the rosin is added in a large amount, the ductility of 
specimen is slightly reduced. The reason should be that rock-like materials added with silicone rubber without rosin have 
good ductility, and the addition of a small amount of rosin is not sufficient to change their ductility. 
It can also be seen from figures that:  

① As the amount of sand decreases, the strain corresponding to the maximum stress tends to increase, which may be related 
to the strain of epoxide resin and polyamide after hardening. With the decrease of sand content, the residual strength of 
rock-like materials tends to increase, which may be due to the high residual strength of both epoxy and polyamide, as well 
as barite. 

② As the barite content increases, there are some differences in the residual strength of rock-like materials. This is most 
likely due to the high residual strength of both epoxy and polyamide, as well as barite.  

③ As the content of epoxide resin and polyamide increases, the strain corresponding to the maximum stress tends to 
increase slightly, because epoxide resin and polyamide will have a larger strain when broken. Moreover, the residual strength 
of the specimen tends to increase when the content of epoxide resin and polyamide is high, because epoxide resin and 
polyamide also have high residual strength.  

④ When the amount of added silicone rubber increases, the residual strength of the specimen slightly decreases, which is 
likely to be related to the high residual strength of the silicone rubber.  

⑤ As the amount of rosin added increases, the strain corresponding to the maximum stress tends to decrease, which may 
be related to the less strain of the rosin. In the absence of silicone rubber, the residual strength of the specimen does not 
change substantially when the amount of added rosin changes. In the case of silicone rubber, the residual strength of the 
specimen slightly changes when the amount of rosin added increases, which may be related to the high residual strength of 
rock-like materials without rosin. 
 

Effect of raw materials on stress-strain curves and brittleness indexes of ductile rock-like materials 
The elastic modulus can be obtained by the stress-strain curve of rock-like material. Fig. 7 shows the relationship between 
the content of each raw material and the elastic modulus. 
It can be clearly seen from the Fig. 7 that the elastic modulus of the ductile rock-like material can be increased by increasing 
the content of epoxide resin and polyamide, and adding an appropriate amount of rosin. The elastic modulus of rock-like 
materials increases when rosin is added, which may have a great relationship with the elastic modulus of rosin. 
In the experiment, when the amount of sand and barite powder in the raw material component cannot be changed, the 
purpose of lowering the elastic modulus of the material can be achieved by adding the auxiliary admixture silicone rubber. 
From the effect of the raw material on the stress-strain curve, it can be known that if the elastic modulus of the ductile rock-
like material is to be enhanced and the ductile rock-like material has a certain brittleness, the epoxide resin and polyamide 
should not be added excessively, but an appropriate amount of the auxiliary regulator rosin should be added. 



 

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23 

 

 
 

0.0 0.2 0.4 0.6 0.8 1.0 1.2 1.4 1.6
0.0

0.2

0.4

0.6

0.8

1.0

1.2

 Sand for 59%

 Sand for 63.3%

 Sand for 66.8%

 Sand for 69.7%

A
x
ia

l 
st

re
ss

 (
M

P
a
)

Axial strain (%)

0.0 0.2 0.4 0.6 0.8 1.0 1.2 1.4 1.6
0.0

0.2

0.4

0.6

0.8

1.0

1.2

 Barite powder for 35.4%

 Barite powder for 39%

 Barite powder for 42.7%

 Barite powder for 45.1%

A
x
ia

l 
st

re
ss

 (
M

P
a
)

Axial strain (%)

 

 

 

0.0 0.2 0.4 0.6 0.8 1.0 1.2 1.4 1.6 1.8 2.0 2.2
0.0

0.2

0.4

0.6

0.8

1.0

1.2

1.4

1.6

1.8

 Epoxy resin-Polyamide for 0.9%

 Epoxy resin-Polyamide for 1.4%

 Epoxy resin-Polyamide for 1.9%

 Epoxy resin-Polyamide for 2.3%

A
x
ia

l 
st

re
ss

 (
M

P
a
)

Axial strain (%)

0.0 0.2 0.4 0.6 0.8 1.0 1.2 1.4 1.6
0.0

0.2

0.4

0.6

0.8

1.0

1.2

 Silicone rubber for 0%

 Silicone rubber for 0.6%

 Silicone rubber for 1.2%

 Silicone rubber for 1.7%

A
x
ia

l 
st

re
ss

 (
M

P
a
)

Axial strain (%)

 

 

 

 

0.0 0.2 0.4 0.6 0.8 1.0 1.2 1.4
0.0

0.3

0.6

0.9

1.2

1.5

1.8

 Rosin for 0%

 Rosin for 0.2%

 Rosin for 0.5%

 Rosin for 0.7%

A
x
ia

l 
st

re
ss

 (
M

P
a
)

Axial strain (%)

0.0 0.2 0.4 0.6 0.8 1.0 1.2 1.4 1.6
0.0

0.2

0.4

0.6

0.8

1.0

1.2

1.4

 Rosin for 0%

 Rosin for 0.2%

 Rosin for 0.5%

 Rosin for 0.7%

A
x
ia

l 
st

re
ss

 (
M

P
a
)

Axial strain (%)

 

 
Figure 5: Stress-strain curve of ductile rock-like materials with different raw material ratios. 



 

  H. Bai et alii, Frattura ed Integrità Strutturale, 56 (2021) 16-45; DOI: 10.3221/IGF-ESIS.56.02                                                                        

 

24 

 

 

 

 

60.0 62.5 65.0 67.5 70.0

72

80

88

96

B
ri

tt
le

 m
o
d
u
lu

s 
(M

P
a
)

Sand content (%)

35.0 37.5 40.0 42.5 45.0
40

48

56

64

72

B
ri

tt
le

 m
o

d
u
lu

s 
(M

P
a
)

Barite content (%)

 

 

 

1.0 1.5 2.0 2.5

50

55

60

65

70

75

B
ri

tt
le

 m
o

d
u

lu
s 

(M
P

a
)

Content of epoxide resin and polyamide (%)

0.0 0.5 1.0 1.5 2.0

20

40

60

80
B

ri
tt

le
 m

o
d
u
lu

s 
(M

P
a
)

Content of silicone rubber (%)

 

 

 

0.0 0.1 0.2 0.3 0.4 0.5 0.6 0.7

80

100

120

140

160

B
ri

tt
le

 m
o

d
u

lu
s 

(M
P

a
)

Rosin content (without silicone rubber) (%)

0.0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8

50

100

150

200

B
ri

tt
le

 m
o

d
u

lu
s 

(M
P

a
)

Rosin content (adding silicone rubber) (%)

 

 

Figure 6: Brittle modulus of ductile rock-like materials with different raw material ratios. 
 



 

                                                                        H. Bai et alii, Frattura ed Integrità Strutturale, 56 (2021) 16-45; DOI: 10.3221/IGF-ESIS.56.02 

 

25 

 

 
 

 

60.0 62.5 65.0 67.5 70.0

120

140

160

180

E
la

st
ic

 m
o
d
u
lu

s 
(M

P
a
)

Sand content (%)

35.0 37.5 40.0 42.5 45.0

100

120

140

160

180

E
la

st
ic

 m
o
d
u
lu

s 
(M

P
a
)

Barite content (%)

 

 

 

1.00 1.25 1.50 1.75 2.00 2.25 2.50

180

190

200

210

E
la

st
ic

 m
o
d
u
lu

s 
(M

P
a
)

Epoxide resin and Polyamide content (%)

0.00 0.25 0.50 0.75 1.00 1.25 1.50 1.75
50

100

150

200
E

la
st

ic
 m

o
d
u
lu

s 
(M

P
a
)

Content of silicone rubber (%)

 

 

 

0.0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8
150

200

250

300

350

E
la

st
ic

 m
o
d
u
lu

s 
(M

P
a
)

Rosin content (without silicone rubber) (%)

0.0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8
120

140

160

180

200

220

E
la

st
ic

 m
o
d
u
lu

s 
(M

P
a
)

Rosin content (adding silicone rubber) (%)

 

 

Figure 7: Relations between raw materials contents and elastic modulus of ductile rock-like materials. 
 
 



 

  H. Bai et alii, Frattura ed Integrità Strutturale, 56 (2021) 16-45; DOI: 10.3221/IGF-ESIS.56.02                                                                        

 

26 

 

 

 

60.0 62.5 65.0 67.5 70.0

0.8

0.9

1.0

1.1

1.2

U
n

ia
x

ia
l 

c
o

m
p

re
ss

iv
e
 s

tr
e
n

g
th

 (
M

P
a
)

Sand content (%)

35.0 37.5 40.0 42.5 45.0
0.85

0.90

0.95

1.00

1.05

1.10

1.15

U
n

ia
x

ia
l 

c
o

m
p

re
ss

iv
e
 s

tr
e
n

g
th

 (
M

P
a
)

Barite content (%)

 

 

 

1.00 1.25 1.50 1.75 2.00 2.25 2.50
1.0

1.1

1.2

1.3

1.4

1.5

1.6

1.7

U
n

ia
x

ia
l 

c
o

m
p

re
ss

iv
e
 s

tr
e
n

g
th

 (
M

P
a
)

Content of epoxide resin and polyamide (%)

0.00 0.25 0.50 0.75 1.00 1.25 1.50 1.75

0.7

0.8

0.9

1.0

1.1
U

n
ia

x
ia

l 
c
o

m
p

re
ss

iv
e
 s

tr
e
n

g
th

 (
M

P
a
)

Content of silicone rubber (%)

 

 

 

0.0 0.1 0.2 0.3 0.4 0.5 0.6 0.7
1.1

1.2

1.3

1.4

1.5

1.6

1.7

1.8

U
n

ia
x

ia
l 

c
o

m
p

re
ss

iv
e
 s

tr
e
n

g
th

 (
M

P
a
)

Rosin content (without silicone rubber) (%)

0.0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8
0.8

0.9

1.0

1.1

1.2

1.3

1.4

1.5

U
n

ia
x

ia
l 

c
o

m
p

re
ss

iv
e
 s

tr
e
n

g
th

 (
M

P
a
)

Rosin content (adding silicone rubber) (%)

 

 

Figure 8: Relationships between raw materials contents and uniaxial compressive strength of ductile rock-like materials. 

 
 



 

                                                                        H. Bai et alii, Frattura ed Integrità Strutturale, 56 (2021) 16-45; DOI: 10.3221/IGF-ESIS.56.02 

 

27 

 

Effect of raw materials on uniaxial compressive strength of ductile rock-like materials 
The uniaxial compressive strength of the rock-like materials, that is, the peak stress on the curve, can be obtained by the 
stress-strain curve. Fig. 8 shows the relation between the content of each raw material and the uniaxial compressive strength. 
It can be clearly seen from Fig. 8 that the uniaxial compressive strength of ductile rock-like materials can be enhanced by 
increasing the content of epoxide resin and polyamide and adding an appropriate amount of the auxiliary regulator rosin. 
To reduce the uniaxial compressive strength of ductile rock-like materials, it is possible to increase the content of sand and 
barite, and to add an appropriate amount of auxiliary regulator silicone rubber. 
In the experiment, when the content of sand and barite powder cannot be changed, the purpose of reducing the uniaxial 
compressive strength of the ductile rock-like material can be achieved by adding the auxiliary admixture silicone rubber. 
From the effect of the raw material on the stress-strain curve, it can be known that if the uniaxial compressive strength of 
the ductile rock-like material is to be enhanced and the ductile rock-like material has a certain brittleness, the epoxide resin 
and polyamide cannot be excessively added, but an appropriate amount of the auxiliary regulator rosin should be added. 

 

Effect of raw materials on fracture toughness of ductile rock-like materials 
Referring to the relevant literature [37], the formula for fracture toughness of rock-like materials is shown in Eqns. 2 and 3. 
 

= − + − +
−

2 3 4

2
[3.75 11.98 24.4( ) 25.69( ) 10.02( ) ]

( )
IC

PS a a a a a
K

D D D DD D a
                               (2) 

 
where P represents the maximum load at the time of loading, S is the span, D denotes the diameter, which is 0.05 m, and a 
is the crack length, which is 0.02 m. 
Substituting a and D into Eqn. 2 yields 
 

= 2675 ( a m )ICK PS P                                            
(3) 

 
By substituting relevant experimental data into Eqn. 3, the fracture toughness of ductile rock-like materials can be obtained. 
The relationship between the fracture toughness and the content of each raw material is shown in Fig. 9. 
It can be clearly seen from Fig. 9 that the fracture toughness of ductile rock-like materials can be enhanced by increasing 
the content of epoxide resin and polyamide and adding an appropriate amount of auxiliary regulator rosin. At the same time, 
it can be seen that for the purpose of improving the fracture toughness of rock-like materials, the addition of silicone rubber 
and rosin is not as good as the case of adding rosin alone. To reduce the fracture toughness of ductile rock-like materials, 
the content of sand and barite can be increased, and an appropriate amount of auxiliary regulator silicone rubber can be 
added. 
In the experiment, when the content of sand and barite powder cannot be changed, the purpose of reducing the fracture 
toughness of the ductile rock-like material can be achieved by adding the auxiliary admixture silicone rubber. From the 
effect of the raw material on the stress-strain curve, it is also known that if the fracture toughness of the ductile rock-like 
material is to be improved and the ductile rock-like material has a certain brittleness, the epoxide resin and polyamide should 
not be excessively added, but an appropriate amount of the auxiliary regulator rosin should be added. 
 

Analysis of experimental results of brittle rock-like materials 
Effect of raw materials on stress-strain curves and brittleness indexes of brittle rock-like materials 
The uniaxial compressive stress-strain curve and brittle modulus of brittle rock-like materials can be obtained by the same 
treatment method. Fig. 10 and Fig. 11 show respectively stress-strain curves and brittle modulus changes for brittle rock-
like materials at different raw material ratios. 
It can be seen from the curves in the figures:  

① When the sand content is relatively low, the specimen exhibits relatively brittle fracture properties, and the brittle fracture 
characteristics of the specimen are no longer obvious as the sand content increases. Because when the sand content is low, 
the damage of the specimen is mainly the brittle failure of the rosin. When the sand content is relatively high, the specimen 
is mainly failed by the shear failure of the sand. In addition, it can be seen that as the sand content increases, the strain 
corresponding to the maximum stress tends to increase.  
 
 
 



 

  H. Bai et alii, Frattura ed Integrità Strutturale, 56 (2021) 16-45; DOI: 10.3221/IGF-ESIS.56.02                                                                        

 

28 

 

 

60 65 70

0.024

0.026

0.028

0.030

0.032
F

ra
c
tu

re
 t

o
u
g

h
n

e
ss

 (
M

P
a
·m

1
/2

)

Sand content (%)

35 40 45

0.026

0.028

0.030

0.032

F
ra

c
tu

re
 t

o
u
g

h
n

e
ss

 (
M

P
a
·m

1
/2

)

Barite content (%)

 

 

 

1.0 1.5 2.0 2.5

0.030

0.035

0.040

0.045

F
ra

c
tu

re
 t

o
u

g
h

n
e
ss

 (
M

P
a
·m

1
/2

)

Content of epoxide resin and polyamide (%)

0.0 0.5 1.0 1.5 2.0

0.026

0.028

0.030

0.032

F
ra

c
tu

re
 t

o
u
g

h
n

e
ss

 (
M

P
a
·m

1
/2

)

Content of silicone rubber (%)

 

 

 

0.0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8
0.030

0.035

0.040

0.045

F
ra

c
tu

re
 t

o
u

g
h

n
e
ss

 (
M

P
a
·m

1
/2
)

Rosin content (without silicone rubber) (%)

0.0 0.1 0.2 0.3 0.4 0.5 0.6 0.7
0.028

0.030

0.032

0.034

0.036

0.038

F
ra

c
tu

re
 t

o
u

g
h

n
e
ss

 (
M

P
a
·m

1
/2
)

Rosin content (adding silicone rubber) (%)

 

 

Figure 9: Relationships between raw materials contents and fracture toughness of ductile rock-like materials. 
 

 

 



 

                                                                        H. Bai et alii, Frattura ed Integrità Strutturale, 56 (2021) 16-45; DOI: 10.3221/IGF-ESIS.56.02 

 

29 

 

 

0.0 0.5 1.0 1.5 2.0
0.0

0.2

0.4

0.6

0.8

1.0

1.2

1.4

 Sand for 47.6%

 Sand for 53.2%

 Sand for 57.7%

 Sand for 61.4%

S
tr

e
ss

 (
M

P
a
)

Strain (%)

0.0 0.5 1.0 1.5 2.0
0.0

0.2

0.4

0.6

0.8

1.0

1.2

1.4

 Barite powder for 47.6%

 Barite powder for 53.2%

 Barite powder for 57.7%

 Barite powder for 61.4%

 

 

S
tr

e
ss

 (
M

P
a
)

Strain (%)

 

 

 

0.0 0.3 0.6 0.9 1.2 1.5
0.0

0.2

0.4

0.6

0.8

1.0

1.2

1.4

1.6

1.8

 Rosin for 1.2%

 Rosin for 1.7%

 Rosin for 2.1%

 Rosin for 2.6%

 

 

S
tr

e
ss

 (
M

P
a
)

Strain (%)

0.0 0.4 0.8 1.2 1.6 2.0
0.0

0.2

0.4

0.6

0.8

1.0

1.2

1.4

1.6

 Epoxy resin-Polyamide for 0%

 Epoxy resin-Polyamide for 0.47%

 Epoxy resin-Polyamide for 0.94%

 Epoxy resin-Polyamide for 1.4%

 

 

S
tr

e
ss

 (
M

P
a
)

Strain (%)

 

 

 

0.0 0.4 0.8 1.2 1.6 2.0
0.0

0.2

0.4

0.6

0.8

1.0

1.2

1.4

 Silicone rubber for 0%

 Silicone rubber for 0.47%

 Silicone rubber for 0.94%

 Silicone rubber for 1.4%

 

 

S
tr

e
ss

 (
M

P
a
)

Strain (%)

 

 

Figure 10: Stress-strain curve of brittle rock-like materials with different raw material ratios. 

 

 



 

  H. Bai et alii, Frattura ed Integrità Strutturale, 56 (2021) 16-45; DOI: 10.3221/IGF-ESIS.56.02                                                                        

 

30 

 

 

45 50 55 60 65

60

80

100

120

140

160
B

ri
tt

le
 m

o
d

u
lu

s 
(M

P
a
)

Sand content (%)

45 50 55 60

40

60

80

100

120

140

160

B
ri

tt
le

 m
o

d
u
lu

s 
(M

P
a
)

Barite content (%)

 

 

 

1.0 1.5 2.0 2.5

150

200

250

300

350

B
ri

tt
le

 m
o
d

u
lu

s 
(M

P
a
)

Rosin content (%)

0.0 0.5 1.0 1.5

60

80

100

120

140

160

B
ri

tt
le

 m
o
d

u
lu

s 
(M

P
a
)

Epoxide resin-polyamide content (%)

 

 

 

0.0 0.5 1.0 1.5

60

80

100

120

140

160

B
ri

tt
le

 m
o
d

u
lu

s 
(M

P
a
)

Silicone rubber content (%)

 

 

Figure 11: Brittle modulus of brittle rock-like materials with different raw material ratios. 

 
 
 



 

                                                                        H. Bai et alii, Frattura ed Integrità Strutturale, 56 (2021) 16-45; DOI: 10.3221/IGF-ESIS.56.02 

 

31 

 

② When the barite content is relatively low, the specimen exhibits relatively obvious brittle fracture properties. With the 
increase of barite content, the brittle fracture characteristics of the specimen are no longer obvious. This is because when 
the barite content is relatively low, the damage of the specimen is mainly the brittle failure of the rosin. When the barite 
content is relatively high, the damage of the specimen is mainly reflected by the shear failure of sand and barite, and the 
barite material itself has relatively good ductility. It can also be found that as the barite content increases, the strain 
corresponding to the maximum stress tends to increase.  

③ When the content of rosin is relatively high, the specimen exhibits obvious brittle fracture properties, and the brittle 
fracture characteristics of the specimen are no longer obvious with the decrease of rosin content. This is also because when 
the rosin content is relatively high, the damage of the specimen is mainly the brittle failure of the rosin. When the content 
of rosin is relatively low, the damage of the specimen is mainly reflected by the shear failure of sand and barite, and the 
barite itself has better ductility. It can be seen that as the amount of added epoxide resin and polyamide increases, the strain 
corresponding to the maximum stress tends to increase, which may be related to the greater strain of epoxide resin and 
polyamide during failure. Moreover, it can also be seen that as the content of epoxide resin and polyamide increases, the 
residual strength of the specimen increases, which may be related to the good ductility of epoxide resin and polyamide.  

④ When rock-like materials do not contain the epoxide resin and polyamide, the specimen exhibits relatively obvious brittle 
fracture properties, and the brittle fracture characteristics of the specimen are no longer obvious as the amount of epoxide 
resin and polyamide added increases. The reason may be that epoxide resin and polyamide have good ductility during failure, 
thereby improving the brittle fracture property of the rosin itself.  

⑤ When the silicone rubber is not added, the specimen exhibits relatively obvious brittle fracture properties. With the 
increase of the silicone rubber content, the brittle fracture characteristics of the specimen are no longer obvious. The reason 
may be that the silicone rubber has good ductility, thereby improving the brittle fracture properties of the rosin itself. It can 
also be seen that as the amount of added silicone rubber increases, the strain corresponding to the maximum stress tends 
to increase, which may be related to the greater strain of the silicone rubber during failure. In addition, it can be seen that 
there is no significant difference in the residual strength of the specimen when the amount of added silicone rubber is 
increased, which may be related to the ductility of the hardened silicone rubber. 

 

Effect of raw materials on elastic modulus of brittle rock-like materials 
Similarly, the relationship between the content of each raw material and the elastic modulus is shown in Fig. 12. It can be 
seen that in order to increase the elastic modulus of brittle rock-like materials, it can only be achieved by increasing the 
content of the rosin in the raw materials. When the rosin content increases, the elastic modulus of rock-like materials 
increases significantly, which may have a great relationship with the elastic modulus of rosin itself. 
In the experiment, when the content of sand and barite powder cannot be changed, the purpose of lowering the elastic 
modulus of the material can be achieved by adding the auxiliary admixture epoxide resin, polyamide, or silicone rubber. It 
can also be seen from Fig. 12 that silicone rubber has a better effect of lowering the elastic modulus of the material relative 
to the epoxide resin and the polyamide. 
 

Effect of raw materials on uniaxial compressive strength of brittle rock-like materials 
The uniaxial compressive strength of brittle rock-like material was obtained by the stress-strain curve, and the relationship 
between the content of each raw material and the uniaxial compressive strength was as shown in Fig. 13. 
It can be clearly seen from the figure that the uniaxial compressive strength of the brittle rock-like material can be enhanced 
by increasing the content of the rosin and adding an appropriate amount of the auxiliary regulator epoxide resin and 
polyamide. To reduce the uniaxial compressive strength of brittle rock-like materials, the content of sand and barite can be 
increased, and an appropriate amount of auxiliary regulator silicone rubber can be added. 
In the experiment, when the content of sand and barite powder cannot be changed, the purpose of reducing the uniaxial 
compressive strength of the brittle rock-like material can be achieved by adding the auxiliary admixture silicone rubber. 
From the effect of the raw material on the stress-strain curve, it can be known that if the uniaxial compressive strength of 
the brittle rock-like material is to be increased and the brittle rock-like material has a certain ductility, the rosin should not 
be added too much, but an appropriate amount of the auxiliary regulator epoxide resin and polyamide should be added. 
 

Effect of raw materials on fracture toughness of brittle rock-like materials 
Similarly, the fracture toughness of the brittle rock-like material can also be obtained by substituting the relevant test data 
into Eqn. 3. The relationship between the fracture toughness and the content of each raw material is shown in Fig. 14. It 
can be clearly seen that in order to improve the fracture toughness of brittle rock-like materials, it is possible to increase the 



 

  H. Bai et alii, Frattura ed Integrità Strutturale, 56 (2021) 16-45; DOI: 10.3221/IGF-ESIS.56.02                                                                        

 

32 

 

content of rosin and add an appropriate amount of auxiliary regulator epoxide resin and polyamide. It has also been found 
that the addition of epoxide resin and polyamide to improve the fracture toughness of rock-like materials is better. To 
reduce the fracture toughness of brittle rock-like materials, the content of sand and barite in the raw materials should be 
increased, and an appropriate amount of auxiliary regulator silicone rubber can be added. 
 

45 50 55 60

140

160

180

200

220

E
la

st
ic

 m
o
d

u
lu

s 
(M

P
a
)

Sand content (%)

45 50 55 60

140

160

180

200

220

E
la

st
ic

 m
o
d

u
lu

s 
(M

P
a
)

Barite content (%)

 

 

 

1.0 1.5 2.0 2.5

200

250

300

350

400

E
la

st
ic

 m
o

d
u

lu
s 

(M
P

a
)

Rosin content (%)

0.0 0.5 1.0 1.5

160

170

180

190

200

210

220

E
la

st
ic

 m
o
d

u
lu

s 
(M

P
a
)

Content of epoxide resin and polyamide (%)

 

 

 

0.0 0.5 1.0 1.5

130

140

150

160

170

180

190

200

210

E
la

st
ic

 m
o
d

u
lu

s 
(M

P
a
)

Silicone rubber content (%)

 

 

Figure 12: Relationships between raw materials contents and elastic modulus of brittle rock-like materials. 



 

                                                                        H. Bai et alii, Frattura ed Integrità Strutturale, 56 (2021) 16-45; DOI: 10.3221/IGF-ESIS.56.02 

 

33 

 

 
 

47.5 50.0 52.5 55.0 57.5 60.0 62.5

0.9

1.0

1.1

1.2

U
n
ia

x
ia

l 
c
o
m

p
re

ss
iv

e
 s

tr
e
n
g
th

 (
M

P
a
)

Sand content (%)

45 50 55 60

0.9

1.0

1.1

1.2

U
n

ia
x

ia
l 

c
o

m
p

re
ss

iv
e
 s

tr
e
n

g
th

 (
M

P
a
)

Barite content (%)

 

 

 

1.0 1.5 2.0 2.5

1.1

1.2

1.3

1.4

1.5

1.6

1.7

U
n

ia
x
ia

l 
c
o
m

p
re

ss
iv

e
 s

tr
e
n
g

th
 (

M
P

a
)

Rosin content (%)

0.0 0.5 1.0 1.5

1.15

1.20

1.25

1.30

1.35

1.40

1.45

U
n

ia
x
ia

l 
c
o
m

p
re

ss
iv

e
 s

tr
e
n
g

th
 (

M
P

a
)

Content of epoxide resin and polyamide (%)

 

 

 

0.0 0.5 1.0 1.5

0.9

1.0

1.1

1.2

U
n

ia
x

ia
l 

c
o

m
p

re
ss

iv
e
 s

tr
e
n

g
th

 (
M

P
a
)

Silicone rubber content (%)

 

 

Figure 13: Relationships between raw materials contents and uniaxial compressive strength of brittle rock-like materials. 
 

 

 



 

  H. Bai et alii, Frattura ed Integrità Strutturale, 56 (2021) 16-45; DOI: 10.3221/IGF-ESIS.56.02                                                                        

 

34 

 

 

 

 

45 50 55 60 65

0.026

0.028

0.030

0.032

0.034

F
ra

c
tu

re
 t

o
u

g
h

n
e
ss

(M
P

a
·m

1
/2
)

Sand content (%)

45 50 55 60 65

0.026

0.028

0.030

0.032

0.034

F
ra

c
tu

re
 t

o
u

g
h

n
e
ss

(M
P

a
·m

1
/2
)

Barite content (%)

 

 

 

1.0 1.5 2.0 2.5

0.032

0.034

0.036

0.038

0.040

0.042

F
ra

c
tu

re
 t

o
u

g
h

n
e
ss

(M
P

a
·m

1
/2
)

Rosin content (%)

0.0 0.5 1.0 1.5

0.032

0.034

0.036

0.038

F
ra

c
tu

re
 t

o
u
g

h
n

e
ss

(M
P

a
·m

1
/2
)

Epoxide resin-polyamide content (%)

 

 

 

0.0 0.5 1.0 1.5

0.026

0.028

0.030

0.032

0.034

F
ra

c
tu

re
 t

o
u

g
h

n
e
ss

(M
P

a
·m

1
/2
)

Content of silicone rubber (%)

 

 

Figure 14: Relationships between raw materials contents and fracture toughness of brittle rock-like materials. 



 

                                                                        H. Bai et alii, Frattura ed Integrità Strutturale, 56 (2021) 16-45; DOI: 10.3221/IGF-ESIS.56.02 

 

35 

 

In the experiment, when the content of sand and barite powder cannot be changed, the purpose of reducing the fracture 
toughness of the brittle rock-like material can be achieved by adding the auxiliary admixture silicone rubber. From the effect 
of the raw material on the stress-strain curve, it can be known that if the fracture toughness of the brittle rock-like material 
is to be increased and the brittle rock-like material has a certain ductility, the rosin should not be added too much, but an 
appropriate amount of the auxiliary regulator epoxide resin and polyamide should be added. 
 
 

APPLICATION OF ROCK-LIKE MATERIALS IN CRACK PROPAGATION EXPERIMENTS 
 

Experimental design 
n this experiment, crack propagation studies were carried out on specimens with the same original crack arrangement. 
According to the previous test results, the raw material ratios of the crack propagation experiment was finally 
determined, which was divided into the ratio of ductility group and the ratio of brittleness group, as shown in Tab. 3 

and Tab. 4.  

 

Number Raw materials Ratio Epoxide resin - polyamide content (%) 

G1 Sand, barite, epoxy, polyamide and alcohol 300:300:4:4:40 1.23 

G2 Sand, barite, epoxy, polyamide and alcohol 300:300:6:6:40 1.84 

G3 Sand, barite, epoxy, polyamide and alcohol 300:300:8:8:40 2.47 

G4 Sand, barite, epoxy, polyamide and alcohol 300:300:10:10:40 3.11 

G5 Sand, barite, epoxy, polyamide and alcohol 300:300:12:12:40 3.61 

 

Table 3: Ductility group ratio. 

 

Number Raw materials Ratio Rosin content (%) 

H1 Sand, barite, rosin and alcohol 200:200:5:15 1.19 

H2 Sand, barite, rosin and alcohol 200:200:7:15 1.66 

H3 Sand, barite, rosin and alcohol 200:200:9:15 2.12 

H4 Sand, barite, rosin and alcohol 200:200:11:15 2.58 

H5 Sand, barite, rosin and alcohol 200:200:13:15 3.04 

 

Table 4: Brittleness group ratio. 

 
The initial crack layout of this experiment is shown in Fig. 15 (2a shows the crack length, c shows the crack unconnected 
rate, s indicates the crack pitch, and α indicates the crack inclination angle), and the specimen has a pre-crack opening degree 
of 0.8 mm. The dimension of the specimen are 140mm high, 90mm wide and 40mm thick. In the experiment, the 
geotechnical experimental servo test machine from Chongqing University was used as the experimental device, which can 
control the loading mode by using a computer program and collect test data synchronously. Different ways of loading can 
be performed by setting a computer program, and the loading rate can also be adjusted. 
This experiment was to observe the whole process of cracking of cracked specimens, and the crack initiation, expansion 
and coalescence speed were relatively fast. Therefore, in order to achieve the ideal image acquisition effect, the RDT/16 
high-speed dynamic recording system was applied in the experiment. The loading mode of displacement control was selected 
where the loading rate was 1mm/min, and the shooting speed of the high-speed dynamic recording system during loading 
was 25 images per second. 

I 



 

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36 

 

 

 

Figure 15: Crack layout. 
 

Characteristics of the crack propagation process 
Comparative analysis of crack initiation modes 
Tab. 5 is a comparison table of the crack initiation modes of the ductile group. The content of epoxide resin and polyamide 
is gradually reduced from left to right, that is, the brittleness of the material is gradually increased. 
By comparing and analyzing Tab. 5, it can be seen that as the content of epoxide resin and polyamide decreases gradually, 
the new crack initiation mode gradually changes from the state where the initial wing crack and shear crack coexist to only 
the wing crack. Through the observation of the experimental loading process and the analysis of the experimental data, it is 
found that there is no significant difference in the vertical compression displacement of each specimen when the new crack 
starts to sprout.  
 

G5                               G4                                  G3                               G2                            G1           

     

     

a- wing crack  
b- shear crack 
c- wing crack  
d- shear crack  

a- shear crack 
b- wing crack 
c- wing crack 
d- shear crack 

a- shear crack 
b- shear crack 
c- wing crack 
d- wing crack 

a- wing crack 
b- wing crack 
c- wing crack 
d- wing crack 

a- wing crack 
b- wing crack 
c- wing crack 
d- wing crack 

 

Table 5: Crack initiation mode of the ductile group. 

G5 

G5 

G4 

G4 

G3 

G3 

G2 

G2 

G1 

G1 

20mm 20mm 20mm 20mm 20mm 



 

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37 

 

Tab. 6 is a comparison table of the crack initiation modes of the brittle group. The rosin content increases from left to right, 
that is, the brittleness of the material increases gradually. 
By comparing and analyzing Tab. 6, it can be seen that as the rosin content increases gradually, the new crack initiation 
mode is almost all wing crack. Observing the experimental loading process and analyzing the experimental data, it is found 
that when the new crack begins to sprout, the vertical compression displacement of the specimen with more rosin content 
is smaller. 
 

H1                            H2                              H3                              H4                           H5 

     

     

a- wing crack 
b- wing crack 
c- wing crack 
d- wing crack 

a- wing crack 
b- wing crack 
c- wing crack 
d- wing crack 

a- wing crack 
b- wing crack 
c- wing crack 
d- wing crack 

a- wing crack 
b- wing crack 
c- wing crack 
d- wing crack 

a- wing crack 
b- wing crack 
c- wing crack 
d- wing crack 

 

Table 6: Crack initiation mode of the brittle group. 

 
According to the comprehensive analysis of the two tables, as the brittleness of the material increases gradually, the new 
crack initiation mode of the rock-like material gradually changes from shear crack to wing crack. At the same time, when 
the new crack starts to sprout, the vertical compression displacement of the specimen gradually decreases. 

 
Comparative analysis of crack coalescence failure mode 
Tab. 7 is a comparison table of the crack coalescence failure modes of the ductile group. The content of epoxide resin and 
polyamide gradually reduces from left to right, that is, the brittleness of the material gradually increases. 
By comparing and analyzing Tab. 7, it can be seen that as the content of epoxide resin and polyamide reduces gradually, the 
crack coalescence failure mode gradually changes from the initial composite failure of tensile and shear to the tensile failure. 
Observing the experimental loading process and analyzing the experimental data, it can be found that when the cracks 
coalesce, the vertical compression displacement of the specimen with lower content of epoxide resin and polyamide is 
smaller. 
Tab. 8 is a comparison table of the crack coalescence failure modes of brittle group. The content of rosin is gradually 
increased from left to right, that is, the brittleness of the material is gradually increased. 
By comparing and analyzing Tab. 8, it can be seen that as the content of rosin increases gradually, the crack coalescence 
failure mode is almost all tensile failure. Observing the experimental loading process and analyzing the experimental data, it 
can be found that when the cracks coalesce, the vertical compression displacement of the specimen with more rosin content 
is smaller.  
According to the comprehensive analysis of the two tables, as the brittleness of the material increases gradually, the crack 
coalescence failure mode of the rock-like material gradually changes from the composite failure of tensile and shear to tensile 

H1 

H1 

H2 

H2 

H3 

H3 

H4 

H4 

H5 

H5 

20mm 20mm 20mm 20mm 20mm 



 

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38 

 

failure. At the same time, the vertical compression displacement of the specimen gradually decreases when the cracks 
coalesce. 
 

G5                               G4                               G3                              G2                             G1 

     

composite failure 
of tensile-shear 

composite failure 
of tensile-shear 

composite failure 
of tensile-shear 

composite failure 
of tensile-shear 

tensile failure 

 

Table 7: Sketch of crack coalescence of ductile group. 
 

 

   H1                             H2                              H3                             H4                             H5   

     

Tensile failure Tensile failure Tensile failure Tensile failure Tensile failure 

 

Table 8: Sketch of crack coalescence. 

 
 

Analysis of mechanical properties of rock-like materials 
Analysis of crack initiation stress 
① Crack initiation stress of ductile group 
Crack initiation stress refers to the value of instantaneous stress when the initial crack of the specimen is expanded to form 
a new crack. Under the action of uniaxial compression load, the two initial pre-cracks in the specimen do not necessarily 
produce new cracks at the same time, that is, the initial crack initiation stress of the two initial pre-cracks may be different. 
Comparing the photos taken by the high-speed camera at different times with the stresses and strains recorded by the 
uniaxial compression servo system, then the time, strain and stress of cracking of each initial pre-crack can be determined.  
The crack initiation stress and its average value of the two initial pre-cracks are shown in Tab. 9 and Tab. 10. The relationship 
between the crack initiation stress and the ratio of different raw materials is shown in Fig. 16. 
It is found that each specimen produces new cracks in the experiment. Moreover, it can be found that changing the content 
of epoxide resin-polyamide or rosin, the crack initiation stress of the first crack in the specimen is not significantly different 
from the crack initiation stress of the second crack. The reason may be that the cracking of the first crack causes stress 
redistribution, which in turn causes rapid cracking of the other crack. By comparing and analyzing the crack initiation stress 
of the specimen with different content of epoxide resin-polyamide or rosin, it is found that the initial pre-crack in the 
specimen with less content of epoxide resin-polyamide or rosin is more susceptible to cracking. 
 

G5 G4 G3 G2 G1 

H1 H2 H3 H4 H5 

20mm 20mm 20mm 20mm 20mm 

20mm 20mm 20mm 20mm 20mm 



 

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39 

 

 

Number 
Crack initiation stress of 

crack① 
Crack initiation stress of 

crack② 
Average value of crack 

initiation stress 

G1 0.61 0.71 0.66 

G2 0.78 0.72 0.75 

G3 0.82 0.94 0.88 

G4 1.07 1.11 1.09 

G5 1.38 1.34 1.36 

 

Table 9: Crack initiation stress of ductile group (MPa). 

 

Number 
Crack initiation stress of 

crack① 
Crack initiation stress of 

crack② 
Average value of crack 

initiation stress 

H1 0.63 0.55 0.59 

H2 0.86 0.76 0.81 

H3 0.93 0.97 0.95 

H4 1.11 1.13 1.12 

H5 1.19 1.15 1.17 
 

Table 10: Crack initiation stress of brittle group (MPa). 

 

 

1.0 1.5 2.0 2.5 3.0 3.5 4.0
0.4

0.6

0.8

1.0

1.2

1.4

1.6

 crack①

 crack②

C
ra

c
k

 i
n

it
ia

ti
o

n
 s

tr
e
ss

 (
M

P
a
)

Content of epoxide resin and polyamide (%)

1.0 1.5 2.0 2.5 3.0 3.5
0.4

0.6

0.8

1.0

1.2

1.4

 crack①

 crack②

C
ra

c
k
 i

n
it

ia
ti

o
n
 s

tr
e
ss

 (
M

P
a
)

Rosin content (%)

 

Figure 16: The crack initiation stress of two cracks in specimens. 

 

Analysis of peak strain 
① Peak strain of ductile group 
The peak strain of the specimen with different epoxide resin-polyamide content was obtained by processing the experiment 
data, as shown in Tab. 11. The relationship between the peak strain of the specimen and the content of epoxide resin-
polyamide is shown in Fig. 17. 
It can be seen from the figure that the minimum peak strain of the specimen is 0.80% and the maximum peak strain is 
1.55%. Therefore, it can be considered that the change of the content of epoxide resin-polyamide has a relatively striking 
influence on the peak strain of the specimen. At the same time, with the increase of epoxide resin-polyamide content, the 



 

  H. Bai et alii, Frattura ed Integrità Strutturale, 56 (2021) 16-45; DOI: 10.3221/IGF-ESIS.56.02                                                                        

 

40 

 

peak strain of the specimen shows an increasing trend. Meanwhile the peak strain increases rapidly from the beginning, and 
then increases slowly. 

 

Epoxide resin - polyamide content (%) 1.23 1.84 2.47 3.11 3.61 

Peak strain (%) 0.80 1.04 1.23 1.47 1.55 

 

Table 11: Peak strain of ductile group. 
 

1.0 1.5 2.0 2.5 3.0 3.5 4.0

0.8

1.0

1.2

1.4

1.6

P
e
a
k

 S
tr

a
in

 (
%

)

Content of epoxide resin and polyamide (%)

 

 

Figure 17: The relationship between peak strain and epoxide resin-polyamide content. 
 

② Peak strain of brittle group 
The peak strain of the specimen with different rosin content was obtained by processing the experiment data, as shown in 
Tab. 12. The relationship between the peak strain of the specimen and the rosin content is shown in Fig. 18. 
It can be seen from the figure that the minimum peak strain of the specimen is 0.41% and the maximum peak strain is 
0.70%. Therefore, it can be considered that the change of the rosin content has modest influence on the peak strain of the 
specimen but is not very obvious. At the same time, with the rosin content increases, the peak strain of the specimen shows 
a decreasing trend, and the strain decreases rapidly from the start and then decreases slowly. 
 

Rosin content (%) 1.19 1.65 2.13 2.56 3.05 

Peak strain (%) 0.70 0.64 0.51 0.44 0.41 

 

Table 12: Peak strain of brittle group. 
 

1.0 1.5 2.0 2.5 3.0

0.4

0.5

0.6

0.7

P
e
a
k
 S

tr
a
in

 (
%

)

Epoxide resin-polyamide content (%)

 

 

Figure 18: The relationship between peak strain and rosin content. 



 

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41 

 

By comparing the peak strains of the ductile group and the brittle group,  it can be known that the content of the 
cementitious material has a certain influence on the peak strain of the material. Moreover, with the brittleness of the material 
increases, the peak strain of the material gradually decreases. 
 

Analysis of crack connection mode and connection stress  
Tab. 13 is a table of crack connection modes of ductile group. The epoxide resin-polyamide content gradually reduces from 
left to right, that is, the brittleness of the material gradually increases. By analyzing Tab. 13, it shows that as the epoxide 
resin-polyamide content decreases gradually, the crack connection mode has no obvious regularity, and the wing crack 
connection is the main connection mode. At the same time, it can be found that as the epoxide resin-polyamide content 
reduces, and correspondingly the crack connection stress gradually reduces.  
 

  G5                               G4                            G3                               G2                            G1 

     

     

Initial crack ① is 
connected to wing 

crack “c”. 

Wing crack “b” is 
connected to wing 

crack “c”. 

Shear crack “b” is 
connected to wing 

crack “c”. 

Wing crack “b” is 
connected to initial 

crack ②. 

Wing crack “b” is 
connected to wing 

crack “c”. 

Connection stress 
is 1.54 MPa 

Connection stress 
is 1.30 MPa 

Connection stress 
is 1.05 MPa 

Connection stress 
is 0.89 MPa 

Connection stress 
is 0.74 MPa 

 

Table 13: Crack connection mode of ductile group. 

 
Tab. 14 is a table of crack connection modes of brittle group. The rosin content gradually increases from left to right, that 
is, the brittleness of the material gradually increases. Through the analysis of Tab. 14, it indicates that as the rosin content 
increases gradually, the crack connection mode has no obvious regularity, and the wing crack connection is the main 
connection mode. At the same time, it can be found that as the rosin content increases, the crack connection stress gradually 
increases accordingly. 
In order to compare the relative magnitude relationship between crack initiation stress, connection stress and peak intensity, 
a comparative analysis of the three is performed, as shown in Fig. 19. It can be found that as the epoxide resin-polyamide 
content increases gradually, that is, the ductility of the material gradually increases, the crack connection stress gradually 
approaches the peak strength. At the same time, as the rosin content increases gradually, that is, the brittleness of the material 
increases gradually, the crack connection stress gradually approaches the initiation stress. 
Future developments will be addressed to improve the mechanical strength in case of more complex geometrical 
discontinuities [38-39]. A specific focus on the cyclic behavior will be addressed to improve the total final fatigue life at 
room [40-42] and high temperature [43] as made for traditional materials. This will allow to improve locally the strength to 
counterbalance local geometrical effects that can occur in a real 3D component [44-49]. 
 

G5 G4 G3 G2 G1 

G5 G4 G3 G2 G1 

20mm 20mm 20mm 20mm 20mm 



 

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42 

 

H1                            H2                               H3                               H4                              H5 

     

     

Wing crack “b” is 
connected to wing 
crack “c”. 

Wing crack “b” is 
connected to wing 
crack “c”. 

Wing crack “b” is 
connected to initial 

crack ②. 

Wing crack “b” is 
connected to wing 
crack “c”. 

Wing crack “b” is 
connected to wing 
crack “c”. 

Connection stress 
is 0.73 MPa 

Connection stress 
is 0.90 MPa 

Connection stress 
is 1.06 MPa 

Connection stress 
is 1.17 MPa 

Connection stress 
is 1.22 MPa 

 

Table 14: Crack connection mode of brittle group. 
 

 

1.0 1.5 2.0 2.5 3.0 3.5 4.0
0.6

0.8

1.0

1.2

1.4

1.6

S
tr

e
ss

 (
M

P
a
)

Epoxide resin-polyamide content (%)

 Peak intensity

 Crack connection stress

 Crack initiation stress

1.0 1.5 2.0 2.5 3.0

0.6

0.8

1.0

1.2

1.4

S
tr

e
ss

 (
M

P
a
)

Rosin content (%)

 Peak intensity

 Crack connection stress

 Crack initiation stress

 

 

Figure 19: The relationship between peak intensity, connection stress and initiation stress. 

 
 
CONCLUSIONS 
 

ased on the mechanical properties of ductile and brittle rocks, certain raw materials were selected and the mechanical 
laws of ductile and brittle rock-like materials were obtained. And two rock-like materials were applied to the 
experiment of crack propagation. The main conclusions can be summarized as follows: 

For the simulation of ductile rock-like materials, sand and barite powder as filler materials, epoxide resin and polyamide as 
cementitious materials, and alcohol as organic solvent can be chosen. When the content of the cementitious material 
increases, the uniaxial compressive strength and fracture toughness of the ductile rock-like material significantly improve, 

B 

H1 H2 H3 H4 H5 

H1 H2 H3 H4 H5 

20mm 20mm 20mm 20mm 20mm 



 

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43 

 

and the change of elastic modulus is not obvious. When the content of other raw materials cannot be changed, the addition 
of auxiliary material silicone rubber is mainly to reduce the elastic modulus and strength of this ductile rock-like material, 
and the addition of rosin is mainly to improve the elastic modulus and brittleness of ductile rock-like materials. Similarly, 
using sand and barite powder as a filling material, rosin as a cementitious material, and alcohol as an organic solvent brittle 
rock-like materials can be better simulated. When the content of the cementitious material increases, the elastic modulus 
and the uniaxial compressive strength of brittle rock-like materials significantly improve, and the fracture toughness even 
improves more obviously. When the content of other raw materials cannot be changed, the auxiliary materials epoxide resin 
and polyamide are mainly added to make the brittle rock-like materials have certain ductility, and the addition of silicone 
rubber is mainly to reduce the elastic modulus and brittleness of brittle rock-like materials. 
Through the crack propagation model experiment of rock-like materials, it is found that as the brittleness of the material 
increases, the new crack initiation mode of the rock-like material gradually changes from shear crack to wing crack, and the 
vertical compression displacement of the specimen will gradually decrease when the new crack starts to sprout. When the 
cracks coalesce, the wing crack connection is the main connection mode, and the vertical compression displacement of the 
specimen with low content of epoxide resin and polyamide in the ductile group or high content of rosin in the brittle group 
is smaller. It can be also known that the damage of the ductile group specimen is mainly based on the tensile-shear composite 
failure mode, while the damage of the brittle group specimen is mostly the tensile failure mode. Moreover, for the specimens 
of ductile group, as the content of epoxide resin and polyamide increases gradually, the crack connection stress increases 
and gradually approaches the peak strength. For the specimens of brittle group, as the rosin content increases gradually, the 
crack connection stress increases but gradually approaches the initiation stress. 

 
 
ACKNOWLEDGEMENTS 
 

he work is supported by the National Natural Science Foundation of China (Nos. 41807251, 52027814, 51809198, 51839009 and 
51679017), Fundamental Research Funds for the Central Universities (No. 2042018kf0008). 
 

 
 

REFERENCES 
 

[1] Brace, W.F. and Bombolakis, E.G. (1963). A note on brittle crack growth in compression, J. Geophys. Res., 68(12), pp.  
3709–3713. DOI: 10.1029/JZ068i012p03709. 

[2] Hoek, E. and Bieniawski, Z.T. (1965). Brittle fracture propagation in rock under compression, Int. J. Fract., 1(3), pp. 
137–155. DOI: 10.1007/BF00186851. 

[3] Bieniawski, Z.T. (1967). Mechanism of brittle fracture of rock, part II—experimental studies, Int. J. Rock Mech. Min. 
Sci., 4(4), pp. 407–423. DOI: 10.1016/0148-9062(67)90031-9. 

[4] Horii, H. and Nemat-Nasser, S. (1985). Compression-induced microcrack growth in brittle solids: axial splitting and 
shear failure, J. Geophys. Res., 90(B4), pp. 3105–3125. DOI: 10.1029/JB090iB04p03105. 

[5] Petit, J. and  Barquins, M. (1988). Can natural faults propagate under mode II conditions, Tectonics, 7(6), pp. 1243–
1256. DOI: 10.1029/TC007i006p01243. 

[6] Chaker, C. and  Barquins, M. (2015). Sliding effect on branch crack, Phys. Chem. Earth, 21(4), pp. 319–323. DOI: 
10.1016/S0079-1946(97)00055-4. 

[7] Cao, P., Liu, T., Pu, C. and Lin, H. (2015). Crack propagation and coalescence of brittle rock-like specimens with pre-
existing cracks in compression, Eng. Geol., 187, pp. 113–121. DOI: 10.1016/j.enggeo.2014.12.010. 

[8] Wong, R.H.C. and Chau, K.T. (1998). Crack coalescence in a rock-like material containing two cracks, Int. J. Rock 
Mech. Min. Sci., 35(2), pp. 147–164. DOI: 10.1016/S0148-9062(97)00303-3. 

[9] Wong, R.H.C., Chau, K.T., Tang, C.A. and Lin, P. (2001). Analysis of crack coalescence in rock-like materials containing 
three flaws—part I: experimental approach, Int. J. Rock Mech. Min. Sci., 38(7), pp. 909–924.  
DOI: 10.1016/S1365-1609(01)00064-8. 

[10] Zhou, X.P., Cheng, H. and Feng, Y.F. (2014). An experimental study of crack coalescence behaviour in rock-like 
materials containing multiple flaws under uniaxial compression, Rock Mechanics Rock Engineering, 47, pp. 1961–1986. 
DOI: 10.1007/s00603-013-0511-7. 

[11] Cheng, H., Zhou, X.P., Zhu, J. and Qian, Q.H. (2016). The effects of crack openings on crack initiation, propagation 
and coalescence behavior in rock-like materials under uniaxial compression, Rock Mechanics Rock Engineering, 49, pp. 
3481–3494. DOI: 10.1007/s00603-016-0998-9. 

T 



 

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44 

 

[12] Reyes, O. and  Einstein, H.H. (1991). Failure mechanisms of fractured rock: A fracture coalescence model, Proc. seventh 
Int. Congr. Rock Mech., 1, pp. 333–340. 

[13] Shen, B., Stephansson, O., Einstein, H.H. and Ghahreman, B. (1995). Coalescence of fractures under shear stress 
experiments, J. Geophys. Res. 100(B4), pp. 5975–5990. DOI: 10.1029/95JB00040. 

[14] Bobet, A. and Einstein, H.H. (1998). Fracture coalescence in rock-type materials under uniaxial and biaxial compression, 
Int. J. Rock Mech. Min. Sci., 35(7), pp. 863–888. DOI: 10.1016/S0148-9062(98)00005-9. 

[15] Sagong, M. and Bobet, A. (2002). Coalescence of multiple flaws in a rock-model material in uniaxial compression, Int. 
J. Rock Mech. Min. Sci., 39(2), pp. 229–241. DOI: 10.1016/S1365-1609(02)00027-8. 

[16] Wong, L.N.Y. and Einstein, H.H. (2006). Fracturing behavior of prismatic specimens containing single flaws, 
Proceedings of the 41st US symposium on rock mechanics, June. Colorado. USA. 

[17] Wong, L.N.Y. and Einstein, H.H. (2009). Crack coalescence in molded gypsum and Carrara marble: part 1. Macroscopic 
observations and interpretation, Rock Mech. Rock Eng., 42, pp. 475–511. DOI: 10.1007/s00603-008-0003-3. 

[18] Wong, L.N.Y. and Einstein, H.H. (2009). Crack coalescence in molded gypsum and Carrara marble: part 2. Microscopic 
observations and interpretation, Rock Mech. Rock Eng., 42, pp. 513–545. DOI: 10.1007/s00603-008-0002-4. 

[19] Basu, A., Mishra, D.A. and Roychowdhury, K. (2013). Rock failure modes under uniaxial compression, Brazilian, and 
point load tests, Bull. Eng. Geol. Environ., 72, pp. 457–475. DOI: 10.1007/s10064-013-0505-4. 

[20] Liang, C.Y. Zhang, Q.B., Li, X. and Xin, P. (2016). The effect of specimen shape and strain rate on uniaxial compressive 
behavior of rock material, Bull. Eng. Geol. Environ., 75, pp. 1669–1681. DOI: 10.1007/s10064-015-0811-0. 

[21] Zhao, F. and He, M.C. (2017). Size effects on granite behavior under unloading rockburst test, Bull. Eng. Geol. 
Environ., 76, pp. 1183–1197. DOI: 10.1007/s10064-016-0903-5. 

[22] Zou, C. and Wong, L.N.Y. (2014). Experimental studies on cracking processes and failure in marble under dynamic 
loading, Eng. Geol., 173, pp. 19–31. DOI: 10.1016/j.enggeo.2014.02.003. 

[23] Hu, M., Liu, Y.X., Ren, J.B., Wu, R. and Zhang, Y. (2019). Laboratory test on crack development in mudstone under 
the action of dry-wet cycles, Bull. Eng. Geol. Environ., 78, pp. 543–556. DOI: 10.1007/s10064-017-1080-x. 

[24] Zhou, X.P., Bi, J. and Qian, Q.H. (2015). Numerical Simulation of Crack Growth and Coalescence in Rock-Like 
Materials Containing Multiple Pre-existing Flaws, Rock Mechanics and Rock Engineering, 48(3), pp. 1097-1114.  
DOI: 10.1007/s00603-014-0627-4. 

[25] Bi, J., Zhou, X.P. and Qian, Q.H. (2016). The 3D Numerical Simulation for the Propagation Process of Multiple Pre-
existing Flaws in Rock-Like Materials Subjected to Biaxial Compressive Loads, Rock Mechanics and Rock Engineering,  
49(5), pp. 1611-1627. DOI: 10.1007/s00603-015-0867-y. 

[26] Wang, Y.T., Zhou, X.P., Wang, Y. and Shou, Y.D. (2018). A 3-D conjugated bond-pair-based peridynamic formulation 
for initiation and propagation of cracks in brittle solids, International Journal of Solids and Structures, 134, pp. 89-115. 
DOI: 10.1016/j.ijsolstr.2017.10.022. 

[27] Wang, Y.T., Zhou, X.P. and Shou, Y.D. (2017). The modeling of crack propagation and coalescence in rocks under 
uniaxial compression using the novel conjugated bond-based peridynamics, International Journal of Mechanical 
Sciences, 128, pp. 614-643. DOI: 10.1016/j.ijmecsci.2017.05.019. 

[28] Zhou, X.P. and Yang, H.Q. (2008). Micromechanical modeling of dynamic compressive responses of mesoscopic 
heterogenous brittle rock, Theoretical and Applied Fracture Mechanics, 48(1), pp. 1-20.  
DOI: 10.1016/j.tafmec.2007.04.008. 

[29] Zhou, X.P., Zhang, Y.X., Ha, Q.L. and Zhu, K.S. (2008). Micromechanical Modelling of the Complete Stress-Strain 
Relationship for Crack Weakened Rock Subjected to Compressive Loading, Rock Mechanics and Rock Engineering,  
41(5), pp. 747-769. DOI: 10.1007/s00603-007-0130-2. 

[30] Zhou, X.P., Zhang, J.Z. and Wong, L.N.Y. (2018). Experimental Study on the Growth, Coalescence and Wrapping 
Behaviors of 3D Cross-Embedded Flaws Under Uniaxial Compression, Rock Mechanics and Rock Engineering, 51(5), 
pp. 1379-1400. DOI:10.1007/s00603-018-1406-4. 

[31] Zhou, X.P., Zhang, J.Z. Qian, Q.H. and Niu, Y. (2019). Experimental investigation of progressive cracking processes 
in granite under uniaxial loading using digital imaging and AE techniques, Journal of Structural Geology, 126, pp. 129-
145. DOI: 10.1016/j.jsg.2019.06.003. 

[32] Zhang, J.Z., Zhou, X.P., Zhou, L.S. and Berto, F. (2019). Progressive failure of brittle rocks with non-isometric flaws: 
Insights from acousto-optic-mechanical (AOM) data, Fatigue & Fracture of Engineering Materials & Structures, 42(8), 
pp. 1787-1802. DOI: 10.1111/ffe.13019. 

[33] Zhang, J.Z. and Zhou, X.P. (2020). Forecasting Catastrophic Rupture in Brittle Rocks Using Precursory AE Time Series, 
Journal of Geophysical Research-Solid Earth, 125(8), e2019JB019276. DOI: 10.1029/2019JB019276. 



 

                                                                        H. Bai et alii, Frattura ed Integrità Strutturale, 56 (2021) 16-45; DOI: 10.3221/IGF-ESIS.56.02 

 

45 

 

[34] Zhang, J.Z. and Zhou. X.P. (2020). AE event rate characteristics of flawed granite: from damage stress to ultimate 
failure, Geophysical Journal International, 222(2), pp. 795-814. DOI: 10.1093/gji/ggaa207. 

[35] Zhou, X.P., Wang, Y.T., Zhang, J.Z. and Liu. F.N. (2019). Fracturing Behavior Study of Three-Flawed Specimens by 
Uniaxial Compression and 3D Digital Image Correlation: Sensitivity to Brittleness, Rock Mechanics and Rock 
Engineering, 52(3), pp. 691-718. DOI: 10.1007/s00603-018-1600-4. 

[36] Zhou, X.P., Lian, Y.J., Wong, L.N.Y. and Berto, F. (2018). Understanding the fracture behavior of brittle and ductile 
multi-flawed rocks by uniaxial loading by digital image correlation, Engineering Fracture Mechanics, 199, pp. 438-460. 
DOI: 10.1016/j.engfracmech.2018.06.007. 

[37] Kjellman, W. (1936). Report on an apparatus for con-summate investigation of the mechanical properties of soils, 
Proceedings of the 1st ICSMFE, pp. 16–20.  

[38] Ayatollahi, M.R., Rashidi Moghaddam, M.,   Razavi, S.M.J., Berto, F. (2016). Geometry effects on fracture trajectory of 
PMMA samples under pure mode-I loading, Engineering Fracture Mechanics, 163, pp. 449–461.  

DOI: 10.1016/j.engfracmech.2016.05.014. 
[39] Torabi, A.R., Campagnolo, A., Berto, F.  (2015). Local strain energy density to predict mode II brittle fracture in 

Brazilian disk specimens weakened by V-notches with end holes Materials and Design, 69, pp. 22–29.  

DOI: 10.1016/j.matdes.2014.12.037. 
[40] Zhu, S-P., Yu, Z-Y, Correia, J., De Jesus, A.,  Berto, F. (2018). Evaluation and comparison of critical plane criteria for 

multiaxial fatigue analysis of ductile and brittle materials, International Journal of Fatigue, 112, pp. 279-288,  

DOI: 10.1016/j.ijfatigue.2018.03.028. 
[41] Correia, J., Apetre, N., Arcari, A., De Jesus, A., Muñiz-Calvente, M., Calçada, R., Berto, F., Fernández-Canteli, A. (2017).  

Generalized probabilistic model allowing for various fatigue damage variables, International Journal of Fatigue 100,  pp. 
187-194. DOI: 10.1016/j.ijfatigue.2017.03.031. 

[42] Ferro, P., Lazzarin, P., Berto, F. (2012). Fatigue properties of ductile cast iron containing chunky graphite, Materials 
Science and Engineering A, 554, pp. 122–128. DOI: 10.1016/j.msea.2012.06.024. 

[43] Berto, F., Gallo, P., Lazzarin, P. (2014). High temperature fatigue tests of un-notched and notched specimens made of 
40CrMoV13.9 steel. Materials and Design, 63(1), pp. 609–619. DOI: 10.1016/j.matdes.2014.06.048. 

[44] Berto, F., Lazzarin, P., Wang, C.H. (2004). Three-dimensional linear elastic distributions of stress and strain energy 
density ahead of V-shaped notches in plates of arbitrary thickness. Int. J. Fracture, 127(3), pp. 265–282.  

DOI: 10.1023/B:FRAC.0000036846.23180.4d. 
[45] Berto, F., Lazzarin, P., Kotousov, A. (2011). On higher order terms and out-of-plane singular mode. Mechanics of 

Materials, 43(6), pp. 332–341.  DOI: 10.1016/j.mechmat.2011.03.004. 
[46] Berto, F., Lazzarin, P. (2013). Multiparametric full-field representations of the in-plane stress fields ahead of cracked 

components under mixed mode loading, International Journal of Fatigue, 46, pp. 16–26.  

DOI: 10.1016/j.ijfatigue.2011.12.004. 

[47] Wu, W., Hu, W., Qian, G., Liao, H., Xu, X., Berto, F. (2019). Mechanical design and multifunctional applications of 
chiral mechanical metamaterials: A review, Materials and Design, 180, 107950. DOI: 10.1016/j.matdes.2019.107950 

[48] F. Berto, E. Barati. Fracture assessment of U-notches under three point bending by means of local energy density. 
Materials & Design 32 (2011), 822-830. DOI: 10.1016/j.matdes.2010.07.017. 

[49] S.M.J. Razavi, P. Ferro, F. Berto, J. Torgersen. Fatigue strength of blunt V-notched specimens produced by selective 
laser melting of Ti-6Al-4V. Theoretical and Applied Fracture Mechanics 97 (2018) 376-384.  
DOI: 10.1016/j.tafmec.2017.06.021.