Effect of topography on the motion parameters and deposition characteristics of deflection-type rock avalanches using the discrete element method
Abstract In this study, the deflection-type rock avalanches, a typical moving form of landslide in mountainous regions, were selected as the research object. Basing on the analysis of topography features of this type of rock avalanche, the discrete element method (DEM) was used to simulate the mass...
Ausführliche Beschreibung
Autor*in: |
Hailong, Yang [verfasserIn] Xiangjun, Pei [verfasserIn] Xiaoyi, Fan [verfasserIn] |
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Format: |
E-Artikel |
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Sprache: |
Englisch |
Erschienen: |
2020 |
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Schlagwörter: |
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Übergeordnetes Werk: |
Enthalten in: Arabian journal of geosciences - Berlin : Springer, 2008, 13(2020), 18 vom: 07. Sept. |
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Übergeordnetes Werk: |
volume:13 ; year:2020 ; number:18 ; day:07 ; month:09 |
Links: |
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DOI / URN: |
10.1007/s12517-020-05913-7 |
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Katalog-ID: |
SPR040897702 |
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520 | |a Abstract In this study, the deflection-type rock avalanches, a typical moving form of landslide in mountainous regions, were selected as the research object. Basing on the analysis of topography features of this type of rock avalanche, the discrete element method (DEM) was used to simulate the mass movement process of rock avalanche under different combinations of topographic factors for analyzing the effect of topography on rock avalanche. Sensitivity analysis for topography shows that the travel distance and the velocity difference are confined by the restraint of slope-toe and deflection effects. The slope inclination of deposition area and flow area are the most significant factors for the travel distance and velocity difference, respectively. In addition, a multivariate regression model was proposed to describe the relationship between motion parameters and main topographic factors. Regarding to the velocity distribution of granular particles inside granular body, the relationship between velocities of granular particles and deposit thickness follows a power law distribution under the different deposit width and length, but there are significant differences in power exponents. As for the granular particle distribution inside a deposit body, there is an obvious inverse-grading structure of granular particles inside the deposit body due to the separation of granular particles in their movement. | ||
650 | 4 | |a Deflection-type |7 (dpeaa)DE-He213 | |
650 | 4 | |a Rock avalanches |7 (dpeaa)DE-He213 | |
650 | 4 | |a Topographic factors |7 (dpeaa)DE-He213 | |
650 | 4 | |a Sensitivity analysis |7 (dpeaa)DE-He213 | |
650 | 4 | |a Motion parameters |7 (dpeaa)DE-He213 | |
650 | 4 | |a Particle distribution |7 (dpeaa)DE-He213 | |
700 | 1 | |a Xiangjun, Pei |e verfasserin |4 aut | |
700 | 1 | |a Xiaoyi, Fan |e verfasserin |4 aut | |
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10.1007/s12517-020-05913-7 doi (DE-627)SPR040897702 (SPR)s12517-020-05913-7-e DE-627 ger DE-627 rakwb eng 550 ASE Hailong, Yang verfasserin aut Effect of topography on the motion parameters and deposition characteristics of deflection-type rock avalanches using the discrete element method 2020 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract In this study, the deflection-type rock avalanches, a typical moving form of landslide in mountainous regions, were selected as the research object. Basing on the analysis of topography features of this type of rock avalanche, the discrete element method (DEM) was used to simulate the mass movement process of rock avalanche under different combinations of topographic factors for analyzing the effect of topography on rock avalanche. Sensitivity analysis for topography shows that the travel distance and the velocity difference are confined by the restraint of slope-toe and deflection effects. The slope inclination of deposition area and flow area are the most significant factors for the travel distance and velocity difference, respectively. In addition, a multivariate regression model was proposed to describe the relationship between motion parameters and main topographic factors. Regarding to the velocity distribution of granular particles inside granular body, the relationship between velocities of granular particles and deposit thickness follows a power law distribution under the different deposit width and length, but there are significant differences in power exponents. As for the granular particle distribution inside a deposit body, there is an obvious inverse-grading structure of granular particles inside the deposit body due to the separation of granular particles in their movement. Deflection-type (dpeaa)DE-He213 Rock avalanches (dpeaa)DE-He213 Topographic factors (dpeaa)DE-He213 Sensitivity analysis (dpeaa)DE-He213 Motion parameters (dpeaa)DE-He213 Particle distribution (dpeaa)DE-He213 Xiangjun, Pei verfasserin aut Xiaoyi, Fan verfasserin aut Enthalten in Arabian journal of geosciences Berlin : Springer, 2008 13(2020), 18 vom: 07. Sept. (DE-627)572421877 (DE-600)2438771-X 1866-7538 nnns volume:13 year:2020 number:18 day:07 month:09 https://dx.doi.org/10.1007/s12517-020-05913-7 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_381 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 13 2020 18 07 09 |
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10.1007/s12517-020-05913-7 doi (DE-627)SPR040897702 (SPR)s12517-020-05913-7-e DE-627 ger DE-627 rakwb eng 550 ASE Hailong, Yang verfasserin aut Effect of topography on the motion parameters and deposition characteristics of deflection-type rock avalanches using the discrete element method 2020 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract In this study, the deflection-type rock avalanches, a typical moving form of landslide in mountainous regions, were selected as the research object. Basing on the analysis of topography features of this type of rock avalanche, the discrete element method (DEM) was used to simulate the mass movement process of rock avalanche under different combinations of topographic factors for analyzing the effect of topography on rock avalanche. Sensitivity analysis for topography shows that the travel distance and the velocity difference are confined by the restraint of slope-toe and deflection effects. The slope inclination of deposition area and flow area are the most significant factors for the travel distance and velocity difference, respectively. In addition, a multivariate regression model was proposed to describe the relationship between motion parameters and main topographic factors. Regarding to the velocity distribution of granular particles inside granular body, the relationship between velocities of granular particles and deposit thickness follows a power law distribution under the different deposit width and length, but there are significant differences in power exponents. As for the granular particle distribution inside a deposit body, there is an obvious inverse-grading structure of granular particles inside the deposit body due to the separation of granular particles in their movement. Deflection-type (dpeaa)DE-He213 Rock avalanches (dpeaa)DE-He213 Topographic factors (dpeaa)DE-He213 Sensitivity analysis (dpeaa)DE-He213 Motion parameters (dpeaa)DE-He213 Particle distribution (dpeaa)DE-He213 Xiangjun, Pei verfasserin aut Xiaoyi, Fan verfasserin aut Enthalten in Arabian journal of geosciences Berlin : Springer, 2008 13(2020), 18 vom: 07. Sept. (DE-627)572421877 (DE-600)2438771-X 1866-7538 nnns volume:13 year:2020 number:18 day:07 month:09 https://dx.doi.org/10.1007/s12517-020-05913-7 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_381 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 13 2020 18 07 09 |
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10.1007/s12517-020-05913-7 doi (DE-627)SPR040897702 (SPR)s12517-020-05913-7-e DE-627 ger DE-627 rakwb eng 550 ASE Hailong, Yang verfasserin aut Effect of topography on the motion parameters and deposition characteristics of deflection-type rock avalanches using the discrete element method 2020 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract In this study, the deflection-type rock avalanches, a typical moving form of landslide in mountainous regions, were selected as the research object. Basing on the analysis of topography features of this type of rock avalanche, the discrete element method (DEM) was used to simulate the mass movement process of rock avalanche under different combinations of topographic factors for analyzing the effect of topography on rock avalanche. Sensitivity analysis for topography shows that the travel distance and the velocity difference are confined by the restraint of slope-toe and deflection effects. The slope inclination of deposition area and flow area are the most significant factors for the travel distance and velocity difference, respectively. In addition, a multivariate regression model was proposed to describe the relationship between motion parameters and main topographic factors. Regarding to the velocity distribution of granular particles inside granular body, the relationship between velocities of granular particles and deposit thickness follows a power law distribution under the different deposit width and length, but there are significant differences in power exponents. As for the granular particle distribution inside a deposit body, there is an obvious inverse-grading structure of granular particles inside the deposit body due to the separation of granular particles in their movement. Deflection-type (dpeaa)DE-He213 Rock avalanches (dpeaa)DE-He213 Topographic factors (dpeaa)DE-He213 Sensitivity analysis (dpeaa)DE-He213 Motion parameters (dpeaa)DE-He213 Particle distribution (dpeaa)DE-He213 Xiangjun, Pei verfasserin aut Xiaoyi, Fan verfasserin aut Enthalten in Arabian journal of geosciences Berlin : Springer, 2008 13(2020), 18 vom: 07. Sept. (DE-627)572421877 (DE-600)2438771-X 1866-7538 nnns volume:13 year:2020 number:18 day:07 month:09 https://dx.doi.org/10.1007/s12517-020-05913-7 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_381 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 13 2020 18 07 09 |
allfieldsGer |
10.1007/s12517-020-05913-7 doi (DE-627)SPR040897702 (SPR)s12517-020-05913-7-e DE-627 ger DE-627 rakwb eng 550 ASE Hailong, Yang verfasserin aut Effect of topography on the motion parameters and deposition characteristics of deflection-type rock avalanches using the discrete element method 2020 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract In this study, the deflection-type rock avalanches, a typical moving form of landslide in mountainous regions, were selected as the research object. Basing on the analysis of topography features of this type of rock avalanche, the discrete element method (DEM) was used to simulate the mass movement process of rock avalanche under different combinations of topographic factors for analyzing the effect of topography on rock avalanche. Sensitivity analysis for topography shows that the travel distance and the velocity difference are confined by the restraint of slope-toe and deflection effects. The slope inclination of deposition area and flow area are the most significant factors for the travel distance and velocity difference, respectively. In addition, a multivariate regression model was proposed to describe the relationship between motion parameters and main topographic factors. Regarding to the velocity distribution of granular particles inside granular body, the relationship between velocities of granular particles and deposit thickness follows a power law distribution under the different deposit width and length, but there are significant differences in power exponents. As for the granular particle distribution inside a deposit body, there is an obvious inverse-grading structure of granular particles inside the deposit body due to the separation of granular particles in their movement. Deflection-type (dpeaa)DE-He213 Rock avalanches (dpeaa)DE-He213 Topographic factors (dpeaa)DE-He213 Sensitivity analysis (dpeaa)DE-He213 Motion parameters (dpeaa)DE-He213 Particle distribution (dpeaa)DE-He213 Xiangjun, Pei verfasserin aut Xiaoyi, Fan verfasserin aut Enthalten in Arabian journal of geosciences Berlin : Springer, 2008 13(2020), 18 vom: 07. Sept. (DE-627)572421877 (DE-600)2438771-X 1866-7538 nnns volume:13 year:2020 number:18 day:07 month:09 https://dx.doi.org/10.1007/s12517-020-05913-7 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_381 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 13 2020 18 07 09 |
allfieldsSound |
10.1007/s12517-020-05913-7 doi (DE-627)SPR040897702 (SPR)s12517-020-05913-7-e DE-627 ger DE-627 rakwb eng 550 ASE Hailong, Yang verfasserin aut Effect of topography on the motion parameters and deposition characteristics of deflection-type rock avalanches using the discrete element method 2020 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract In this study, the deflection-type rock avalanches, a typical moving form of landslide in mountainous regions, were selected as the research object. Basing on the analysis of topography features of this type of rock avalanche, the discrete element method (DEM) was used to simulate the mass movement process of rock avalanche under different combinations of topographic factors for analyzing the effect of topography on rock avalanche. Sensitivity analysis for topography shows that the travel distance and the velocity difference are confined by the restraint of slope-toe and deflection effects. The slope inclination of deposition area and flow area are the most significant factors for the travel distance and velocity difference, respectively. In addition, a multivariate regression model was proposed to describe the relationship between motion parameters and main topographic factors. Regarding to the velocity distribution of granular particles inside granular body, the relationship between velocities of granular particles and deposit thickness follows a power law distribution under the different deposit width and length, but there are significant differences in power exponents. As for the granular particle distribution inside a deposit body, there is an obvious inverse-grading structure of granular particles inside the deposit body due to the separation of granular particles in their movement. Deflection-type (dpeaa)DE-He213 Rock avalanches (dpeaa)DE-He213 Topographic factors (dpeaa)DE-He213 Sensitivity analysis (dpeaa)DE-He213 Motion parameters (dpeaa)DE-He213 Particle distribution (dpeaa)DE-He213 Xiangjun, Pei verfasserin aut Xiaoyi, Fan verfasserin aut Enthalten in Arabian journal of geosciences Berlin : Springer, 2008 13(2020), 18 vom: 07. Sept. (DE-627)572421877 (DE-600)2438771-X 1866-7538 nnns volume:13 year:2020 number:18 day:07 month:09 https://dx.doi.org/10.1007/s12517-020-05913-7 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_381 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 13 2020 18 07 09 |
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Arabian journal of geosciences |
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Hailong, Yang @@aut@@ Xiangjun, Pei @@aut@@ Xiaoyi, Fan @@aut@@ |
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|
author |
Hailong, Yang |
spellingShingle |
Hailong, Yang ddc 550 misc Deflection-type misc Rock avalanches misc Topographic factors misc Sensitivity analysis misc Motion parameters misc Particle distribution Effect of topography on the motion parameters and deposition characteristics of deflection-type rock avalanches using the discrete element method |
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550 ASE Effect of topography on the motion parameters and deposition characteristics of deflection-type rock avalanches using the discrete element method Deflection-type (dpeaa)DE-He213 Rock avalanches (dpeaa)DE-He213 Topographic factors (dpeaa)DE-He213 Sensitivity analysis (dpeaa)DE-He213 Motion parameters (dpeaa)DE-He213 Particle distribution (dpeaa)DE-He213 |
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ddc 550 misc Deflection-type misc Rock avalanches misc Topographic factors misc Sensitivity analysis misc Motion parameters misc Particle distribution |
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ddc 550 misc Deflection-type misc Rock avalanches misc Topographic factors misc Sensitivity analysis misc Motion parameters misc Particle distribution |
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ddc 550 misc Deflection-type misc Rock avalanches misc Topographic factors misc Sensitivity analysis misc Motion parameters misc Particle distribution |
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Arabian journal of geosciences |
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title |
Effect of topography on the motion parameters and deposition characteristics of deflection-type rock avalanches using the discrete element method |
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(DE-627)SPR040897702 (SPR)s12517-020-05913-7-e |
title_full |
Effect of topography on the motion parameters and deposition characteristics of deflection-type rock avalanches using the discrete element method |
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Hailong, Yang |
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Arabian journal of geosciences |
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Arabian journal of geosciences |
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Hailong, Yang Xiangjun, Pei Xiaoyi, Fan |
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Hailong, Yang |
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10.1007/s12517-020-05913-7 |
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550 |
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verfasserin |
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effect of topography on the motion parameters and deposition characteristics of deflection-type rock avalanches using the discrete element method |
title_auth |
Effect of topography on the motion parameters and deposition characteristics of deflection-type rock avalanches using the discrete element method |
abstract |
Abstract In this study, the deflection-type rock avalanches, a typical moving form of landslide in mountainous regions, were selected as the research object. Basing on the analysis of topography features of this type of rock avalanche, the discrete element method (DEM) was used to simulate the mass movement process of rock avalanche under different combinations of topographic factors for analyzing the effect of topography on rock avalanche. Sensitivity analysis for topography shows that the travel distance and the velocity difference are confined by the restraint of slope-toe and deflection effects. The slope inclination of deposition area and flow area are the most significant factors for the travel distance and velocity difference, respectively. In addition, a multivariate regression model was proposed to describe the relationship between motion parameters and main topographic factors. Regarding to the velocity distribution of granular particles inside granular body, the relationship between velocities of granular particles and deposit thickness follows a power law distribution under the different deposit width and length, but there are significant differences in power exponents. As for the granular particle distribution inside a deposit body, there is an obvious inverse-grading structure of granular particles inside the deposit body due to the separation of granular particles in their movement. |
abstractGer |
Abstract In this study, the deflection-type rock avalanches, a typical moving form of landslide in mountainous regions, were selected as the research object. Basing on the analysis of topography features of this type of rock avalanche, the discrete element method (DEM) was used to simulate the mass movement process of rock avalanche under different combinations of topographic factors for analyzing the effect of topography on rock avalanche. Sensitivity analysis for topography shows that the travel distance and the velocity difference are confined by the restraint of slope-toe and deflection effects. The slope inclination of deposition area and flow area are the most significant factors for the travel distance and velocity difference, respectively. In addition, a multivariate regression model was proposed to describe the relationship between motion parameters and main topographic factors. Regarding to the velocity distribution of granular particles inside granular body, the relationship between velocities of granular particles and deposit thickness follows a power law distribution under the different deposit width and length, but there are significant differences in power exponents. As for the granular particle distribution inside a deposit body, there is an obvious inverse-grading structure of granular particles inside the deposit body due to the separation of granular particles in their movement. |
abstract_unstemmed |
Abstract In this study, the deflection-type rock avalanches, a typical moving form of landslide in mountainous regions, were selected as the research object. Basing on the analysis of topography features of this type of rock avalanche, the discrete element method (DEM) was used to simulate the mass movement process of rock avalanche under different combinations of topographic factors for analyzing the effect of topography on rock avalanche. Sensitivity analysis for topography shows that the travel distance and the velocity difference are confined by the restraint of slope-toe and deflection effects. The slope inclination of deposition area and flow area are the most significant factors for the travel distance and velocity difference, respectively. In addition, a multivariate regression model was proposed to describe the relationship between motion parameters and main topographic factors. Regarding to the velocity distribution of granular particles inside granular body, the relationship between velocities of granular particles and deposit thickness follows a power law distribution under the different deposit width and length, but there are significant differences in power exponents. As for the granular particle distribution inside a deposit body, there is an obvious inverse-grading structure of granular particles inside the deposit body due to the separation of granular particles in their movement. |
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container_issue |
18 |
title_short |
Effect of topography on the motion parameters and deposition characteristics of deflection-type rock avalanches using the discrete element method |
url |
https://dx.doi.org/10.1007/s12517-020-05913-7 |
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Xiangjun, Pei Xiaoyi, Fan |
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Xiangjun, Pei Xiaoyi, Fan |
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10.1007/s12517-020-05913-7 |
up_date |
2024-07-03T18:57:31.410Z |
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|
score |
7.397662 |