Numerical Simulation of Rock Uniaxial Compressive Strength and Deformation Failure Law under Different Size Conditions

Rock engineering occupies an important position in the 21st century. In the face of rock engineering disasters, we are only looking for the essential problems through experiments on rocks, but rock experiments cannot be realized in large numbers, so the article uses numerical simulation software RFP...

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Main Authors: Zhichao Tian, Chunan Tang, Hao Li, Hui Xing, Xiangda Ning
Format: Article
Language:English
Published: Wiley 2021-01-01
Series:Advances in Civil Engineering
Online Access:http://dx.doi.org/10.1155/2021/6643884
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author Zhichao Tian
Chunan Tang
Hao Li
Hui Xing
Xiangda Ning
author_facet Zhichao Tian
Chunan Tang
Hao Li
Hui Xing
Xiangda Ning
author_sort Zhichao Tian
collection DOAJ
description Rock engineering occupies an important position in the 21st century. In the face of rock engineering disasters, we are only looking for the essential problems through experiments on rocks, but rock experiments cannot be realized in large numbers, so the article uses numerical simulation software RFPA (Realistic Failure Process Analysis) 2D Basic to simulate rock under different size conditions numerically. In this paper, a rock model with a diameter of 50 mm is used for simulation research. Meanwhile, five calculation models of height-to-diameter ratios of 1.0, 1.5, 2.0, 2.5, and 3 are used. Through simulation calculation, we find that the rock model failure is more than complicated when the value of the height-to-diameter ratio is exceedingly low (1), but as the height-to-diameter ratio increases, the failure mode will become simpler. The stress-concentrated failure will be in the form of axial failure. When the height-to-diameter ratio increases (1.5–2), other damage cracks appear on the basis of axial cleavage failure. As the height-to-diameter ratio continues to increase (about 2.5), only shear failure occurs. When the height-to-diameter ratio reaches a relatively high level (3), there will be both axial rip and other damage. When the height-to-diameter ratio is oversize, there will be both axial rip failure and end damage.
format Article
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institution Kabale University
issn 1687-8086
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language English
publishDate 2021-01-01
publisher Wiley
record_format Article
series Advances in Civil Engineering
spelling doaj-art-8a171f3a76604094be19f890f810562d2025-02-03T06:43:27ZengWileyAdvances in Civil Engineering1687-80861687-80942021-01-01202110.1155/2021/66438846643884Numerical Simulation of Rock Uniaxial Compressive Strength and Deformation Failure Law under Different Size ConditionsZhichao Tian0Chunan Tang1Hao Li2Hui Xing3Xiangda Ning4School of Resources and Civil Engineering, Northeastern University, Shenyang, Liaoning 110819, ChinaSchool of Resources and Civil Engineering, Northeastern University, Shenyang, Liaoning 110819, ChinaSchool of Civil Engineering, Inner Mongolia University of Science and Technology, Baotou, Mongolia 014010, ChinaInstitute of Mining Research, Inner Mongolia University of Science and Technology, Baotou, Mongolia 014010, ChinaSchool of Civil Engineering, Inner Mongolia University of Science and Technology, Baotou, Mongolia 014010, ChinaRock engineering occupies an important position in the 21st century. In the face of rock engineering disasters, we are only looking for the essential problems through experiments on rocks, but rock experiments cannot be realized in large numbers, so the article uses numerical simulation software RFPA (Realistic Failure Process Analysis) 2D Basic to simulate rock under different size conditions numerically. In this paper, a rock model with a diameter of 50 mm is used for simulation research. Meanwhile, five calculation models of height-to-diameter ratios of 1.0, 1.5, 2.0, 2.5, and 3 are used. Through simulation calculation, we find that the rock model failure is more than complicated when the value of the height-to-diameter ratio is exceedingly low (1), but as the height-to-diameter ratio increases, the failure mode will become simpler. The stress-concentrated failure will be in the form of axial failure. When the height-to-diameter ratio increases (1.5–2), other damage cracks appear on the basis of axial cleavage failure. As the height-to-diameter ratio continues to increase (about 2.5), only shear failure occurs. When the height-to-diameter ratio reaches a relatively high level (3), there will be both axial rip and other damage. When the height-to-diameter ratio is oversize, there will be both axial rip failure and end damage.http://dx.doi.org/10.1155/2021/6643884
spellingShingle Zhichao Tian
Chunan Tang
Hao Li
Hui Xing
Xiangda Ning
Numerical Simulation of Rock Uniaxial Compressive Strength and Deformation Failure Law under Different Size Conditions
Advances in Civil Engineering
title Numerical Simulation of Rock Uniaxial Compressive Strength and Deformation Failure Law under Different Size Conditions
title_full Numerical Simulation of Rock Uniaxial Compressive Strength and Deformation Failure Law under Different Size Conditions
title_fullStr Numerical Simulation of Rock Uniaxial Compressive Strength and Deformation Failure Law under Different Size Conditions
title_full_unstemmed Numerical Simulation of Rock Uniaxial Compressive Strength and Deformation Failure Law under Different Size Conditions
title_short Numerical Simulation of Rock Uniaxial Compressive Strength and Deformation Failure Law under Different Size Conditions
title_sort numerical simulation of rock uniaxial compressive strength and deformation failure law under different size conditions
url http://dx.doi.org/10.1155/2021/6643884
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AT chunantang numericalsimulationofrockuniaxialcompressivestrengthanddeformationfailurelawunderdifferentsizeconditions
AT haoli numericalsimulationofrockuniaxialcompressivestrengthanddeformationfailurelawunderdifferentsizeconditions
AT huixing numericalsimulationofrockuniaxialcompressivestrengthanddeformationfailurelawunderdifferentsizeconditions
AT xiangdaning numericalsimulationofrockuniaxialcompressivestrengthanddeformationfailurelawunderdifferentsizeconditions