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Gold Science and Technology ›› 2023, Vol. 31 ›› Issue (5): 752-762.doi: 10.11872/j.issn.1005-2518.2023.05.036

• Mining Technology and Mine Management • Previous Articles     Next Articles

Study on the Effect of Thermal Shock on Dynamic Fracture Behavior of Granite

Weihua WANG(),Kai LI(),Ruixin HUANG   

  1. School of Resources and Safety Engineering,Central South University,Changsha 410083,Hunan,China
  • Received:2023-03-03 Revised:2023-04-06 Online:2023-10-31 Published:2023-11-21
  • Contact: Kai LI E-mail:50973993@qq.com;LK15200721534@163.com

Abstract:

In engineering operations such as geothermal development and utilization in high-temperature rock formations,underground coal gasification,multiple oil extractions,underground disposal of high-level radioactive waste,and protection and restoration of important buildings after fires,rocks often experience thermal shock due to drastic temperature changes.Thermal shock refers to the phenomenon where an object undergoes a large amount of heat exchange in a short time due to rapid heating or cooling,resulting in the generation of thermal shock stress within the object.To investigate the impact of thermal shock on the dynamic fracture behavior of high-temperature granite,the granite was heated to three different temperature levels of 100,300,600 ℃,followed by cooling using three different methods of furnace cooling,air cooling,and water cooling to provide different cooling rates,resulting in varying degrees of thermal shock within the granite samples.The notched semi-circular bend (NSCB) specimens of the granite samples subjected to thermal shock treatment were tested using a split Hopkinson pressure bar (SHPB) system for dynamic fracture behavior.The fracture pattern of the specimens was recorded using a high-speed camera.The results show that with the increase in specimen temperature and cooling rate,the dry density and longitudinal wave velocity of the specimens decrease significantly,and the porosity increase.Under thermal shock,the dynamic fracture toughness value of the specimens decreased significantly.At the same loading rate level,the dynamic fracture toughness value of the water-cooled specimens is lower than that of the air-cooled specimens,indicating that the crack propagation resistance of rock materials decrease when subjected to dynamic impact.Furthermore,at loading rates higher than 130 GPa·m0.5/s,the effect of thermal shock on fracture toughness is more pronounced.By analyzing the relationship between dynamic fracture toughness and loading rate,a power law function with a good fitting degree is obtained,revealing the impact of thermal shock on dynamic fracture toughness.Therefore,this study provides valuable reference for the stability of rock formations in cooling treatment projects involving high-temperature rocks,contributing to the design and management of engineering operations such as geothermal development and utilization,underground coal gasification,multiple oil extractions,underground disposal of high-level radioactive waste,and protection and restoration of important buildings after fires.

Key words: thermal shock, granite, mode I dynamic fracture toughness, NSCB, cooling method, fracture patterns, SHPB system

CLC Number: 

  • TD315

Fig.1

Schematic diagram of the NSCB specimen"

Fig.2

Temperature change curves of thermal treatments"

Fig.3

Split Hopkinson pressure bar(SHPB) system"

Table 1

Main parameters of the SHPB system"

参数数值参数数值
杆径/mm50弹性模量/GPa240
入射杆长度/mm2 000泊松比0.28
吸收杆长度/mm500纵波波速/(m·s-15 400
投射杆长度/mm1 500杆密度/(kg·m-37 800

Fig.4

Dynamic forces on both ends of the NSCB specimen"

Fig.5

Time-history curve of dynamic SIF"

Fig.6

Untreated specimens and specimens treated with thermal shock"

Table 2

Averaged dry density of NSCB specimens"

温度

/℃

炉内冷却空气冷却水冷却
ρsσρaσρwσ
1003.1850.00243.1810.00253.1740.0020
3003.1630.00463.1610.00533.1490.0018
6003.1250.00183.1140.00123.1010.0050

Fig.7

Dry density of the NSCB specimens"

Table 3

Averaged P-wave velocity of NSCB specimens"

温度

/℃

炉内冷却空气冷却水冷却
VsσVaσVwσ
1003 333.4318.143 356.3145.053 167.2565.46
3002 793.4256.802 618.8151.702 493.0157.04
6001 395.5717.661 338.2842.941 278.827.08

Fig.8

P-wave velocity of the NSCB specimens"

Table 4

Average porosity of NSCB specimens"

温度/℃炉内冷却空气冷却水冷却
PsσPaσPwσ
1001.340.041.370.131.890.19
3001.470.081.520.241.920.08
6001.890.081.660.082.230.16

Fig.9

Porosity of the NSCB specimens"

Fig.10

Relationship between dynamic fracture toughness and loading rate of NSCB specimens at three kinds of temperature"

Table 5

Parameters of dynamic fracture toughness and loading rate fitting function"

冷却方式温度/℃abR2
未处理250.3690.6280.969

炉内冷却

1000.2590.9820.964
3000.4630.5150.932
6000.1820.7010.886

空气冷却

1000.4850.9410.977
3000.1290.7590.949
6000.4540.4790.827

水冷却

1000.2700.6360.883
3000.2650.6130.908
6000.1230.7130.971

Table 6

Average cooling rate during air cooling and water cooling"

温度/℃空气冷却速率/(℃·min-1水冷却速率/(℃·min-1
1003.46975.00
30011.591137.50
60022.577143.75

Fig.11

Two typical failure modes in dynamic NSCB tests"

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