{"title":"构造断层动力滑动附近损伤带的发育","authors":"A. M. Budkov, G. G. Kocharyan, Z. Z. Sharafiev","doi":"10.1134/S1069351325700156","DOIUrl":null,"url":null,"abstract":"<p><b>Abstract</b>—The results of 2D-calculations describing the formation of damage zone during the development of dynamic slip along a horizontal tectonic fault are presented. Different sliding behaviors are investigated, namely, the sub-Rayleigh sliding when rupture velocity <i>V</i><sub>r</sub> is no greater than the velocity of the Rayleigh wave in the medium and supershear when <i>V</i><sub>r</sub> is higher than the velocity of shear waves. The contribution of tensile and shear fracture mechanisms to the development of damage zone in the vicinity of a fault at different depths is considered. The degree of changes in the physical and mechanical properties of the rock massif at different distances from the fault is assessed. It is shown that at large depths, lithostatic stresses completely suppress tensile fracture, and rock fails exclusively due to shear deformation. At shallow depths, however, the tensile fracture mechanism becomes predominant. The stress release associated with the formation of tensile cracks sharply reduces the size of the shear fracture zone which is localized only in the immediate vicinity of the rupture plane. The increase in tensile strength leads to the enlargement of the shear fracture zone. The damage zone in supershear ruptures can have a complex, non-simply-connected structure. The change in the velocity of compression waves <i>C</i><sub>p</sub> by more than 15–20% is only observed in the immediate vicinity (within 10–20 m) of the sliding plane. At larger distances, a change in <span>\\(\\frac{{dC}}{C}\\)</span> is at most 10%. At shallow depths, tensile cracks may occur and propagate quite far from the sliding plane.</p>","PeriodicalId":602,"journal":{"name":"Izvestiya, Physics of the Solid Earth","volume":"61 2","pages":"213 - 223"},"PeriodicalIF":1.0000,"publicationDate":"2025-07-23","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Development of a Damage Zone in the Vicinity of a Dynamic Slip on a Tectonic Fault\",\"authors\":\"A. M. Budkov, G. G. Kocharyan, Z. Z. Sharafiev\",\"doi\":\"10.1134/S1069351325700156\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p><b>Abstract</b>—The results of 2D-calculations describing the formation of damage zone during the development of dynamic slip along a horizontal tectonic fault are presented. Different sliding behaviors are investigated, namely, the sub-Rayleigh sliding when rupture velocity <i>V</i><sub>r</sub> is no greater than the velocity of the Rayleigh wave in the medium and supershear when <i>V</i><sub>r</sub> is higher than the velocity of shear waves. The contribution of tensile and shear fracture mechanisms to the development of damage zone in the vicinity of a fault at different depths is considered. The degree of changes in the physical and mechanical properties of the rock massif at different distances from the fault is assessed. It is shown that at large depths, lithostatic stresses completely suppress tensile fracture, and rock fails exclusively due to shear deformation. At shallow depths, however, the tensile fracture mechanism becomes predominant. The stress release associated with the formation of tensile cracks sharply reduces the size of the shear fracture zone which is localized only in the immediate vicinity of the rupture plane. The increase in tensile strength leads to the enlargement of the shear fracture zone. The damage zone in supershear ruptures can have a complex, non-simply-connected structure. The change in the velocity of compression waves <i>C</i><sub>p</sub> by more than 15–20% is only observed in the immediate vicinity (within 10–20 m) of the sliding plane. At larger distances, a change in <span>\\\\(\\\\frac{{dC}}{C}\\\\)</span> is at most 10%. At shallow depths, tensile cracks may occur and propagate quite far from the sliding plane.</p>\",\"PeriodicalId\":602,\"journal\":{\"name\":\"Izvestiya, Physics of the Solid Earth\",\"volume\":\"61 2\",\"pages\":\"213 - 223\"},\"PeriodicalIF\":1.0000,\"publicationDate\":\"2025-07-23\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Izvestiya, Physics of the Solid Earth\",\"FirstCategoryId\":\"89\",\"ListUrlMain\":\"https://link.springer.com/article/10.1134/S1069351325700156\",\"RegionNum\":4,\"RegionCategory\":\"地球科学\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q4\",\"JCRName\":\"GEOCHEMISTRY & GEOPHYSICS\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Izvestiya, Physics of the Solid Earth","FirstCategoryId":"89","ListUrlMain":"https://link.springer.com/article/10.1134/S1069351325700156","RegionNum":4,"RegionCategory":"地球科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q4","JCRName":"GEOCHEMISTRY & GEOPHYSICS","Score":null,"Total":0}
引用次数: 0
摘要
摘要给出了沿水平构造断层动态滑动发育过程中损伤带形成的二维计算结果。研究了不同的滑动行为,即破裂速度Vr不大于介质中瑞利波速度时的亚瑞利滑动和Vr大于横波速度时的超剪切。考虑了断裂附近不同深度的拉伸和剪切断裂机制对损伤带发育的贡献。评估了离断层不同距离处岩体物理力学性质的变化程度。结果表明,在大深度处,静岩应力完全抑制张性破裂,岩石破坏完全由剪切变形引起。然而,在较浅的深度,拉伸断裂机制占主导地位。与拉伸裂纹形成相关的应力释放急剧减小了剪切断裂带的大小,剪切断裂带仅局限于破裂面附近。抗拉强度的增加导致剪切断裂带的扩大。超剪切破裂的破坏区可能具有复杂的非单连通结构。压缩波速度Cp的变化幅度大于15-20% is only observed in the immediate vicinity (within 10–20 m) of the sliding plane. At larger distances, a change in \(\frac{{dC}}{C}\) is at most 10%. At shallow depths, tensile cracks may occur and propagate quite far from the sliding plane.
Development of a Damage Zone in the Vicinity of a Dynamic Slip on a Tectonic Fault
Abstract—The results of 2D-calculations describing the formation of damage zone during the development of dynamic slip along a horizontal tectonic fault are presented. Different sliding behaviors are investigated, namely, the sub-Rayleigh sliding when rupture velocity Vr is no greater than the velocity of the Rayleigh wave in the medium and supershear when Vr is higher than the velocity of shear waves. The contribution of tensile and shear fracture mechanisms to the development of damage zone in the vicinity of a fault at different depths is considered. The degree of changes in the physical and mechanical properties of the rock massif at different distances from the fault is assessed. It is shown that at large depths, lithostatic stresses completely suppress tensile fracture, and rock fails exclusively due to shear deformation. At shallow depths, however, the tensile fracture mechanism becomes predominant. The stress release associated with the formation of tensile cracks sharply reduces the size of the shear fracture zone which is localized only in the immediate vicinity of the rupture plane. The increase in tensile strength leads to the enlargement of the shear fracture zone. The damage zone in supershear ruptures can have a complex, non-simply-connected structure. The change in the velocity of compression waves Cp by more than 15–20% is only observed in the immediate vicinity (within 10–20 m) of the sliding plane. At larger distances, a change in \(\frac{{dC}}{C}\) is at most 10%. At shallow depths, tensile cracks may occur and propagate quite far from the sliding plane.
期刊介绍:
Izvestiya, Physics of the Solid Earth is an international peer reviewed journal that publishes results of original theoretical and experimental research in relevant areas of the physics of the Earth''s interior and applied geophysics. The journal welcomes manuscripts from all countries in the English or Russian language.