Quan Wang , Hao Yu , Egor Dontsov , YiLun Zhong , XiuYuan Chen , HengAn Wu
{"title":"层状岩层水力压裂的统一时空标度规律","authors":"Quan Wang , Hao Yu , Egor Dontsov , YiLun Zhong , XiuYuan Chen , HengAn Wu","doi":"10.1016/j.jmps.2025.106367","DOIUrl":null,"url":null,"abstract":"<div><div>This work presents a unified scaling law for a plane strain hydraulic fracture propagation in layered rocks, where fracturing behavior is influenced by both layer thickness and property contrasts across interfaces, leading to non-self-similar propagation over time. The singular integral balance equation is derived by introducing a kernel function that accounts for the varying elastic modulus and a modified load term that incorporates in-situ stress. The layered distribution of elastic modulus and fracture energy is considered using dynamic tip asymptotics. The governing equations and boundary conditions are then made dimensionless by new characteristic scales of fracture opening, fluid pressure, and fracture length, which are proposed to depict the spatial relationship between the interface and fracture. Solutions are obtained through a decoupled approach to match the fracture morphology and tip boundary conditions. This model captures a novel time-sensitive propagation mode of a hydraulic fracture, that can be dominated by toughness in the tip region and viscosity dissipation at the interface region, especially in multilayer rocks. Consequently, the temporal scale of injection time and the spatial scale of layer thickness are integrated into the characteristic scales. A scaling law is thus proposed to fully consider the variations of elastic modulus, fracture energy, fluid injection rate, injection time, and layer thickness on propagation behavior. The law spans the temporal-spatial parameter space within a general framework that quantifies the evolution of viscosity dissipation induced by interfaces, summarizing four specific cases: the homogeneous model, single-interface model, multi-layer model, and homogenized model. The proposed law provides a universal measure for modeling hydraulic fracturing of layered heterogeneous rocks with arbitrary thickness and propagation stage.</div></div>","PeriodicalId":17331,"journal":{"name":"Journal of The Mechanics and Physics of Solids","volume":"206 ","pages":"Article 106367"},"PeriodicalIF":6.0000,"publicationDate":"2025-09-13","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"A unified temporal-spatial scaling law for hydraulic fracturing in layered rock formations\",\"authors\":\"Quan Wang , Hao Yu , Egor Dontsov , YiLun Zhong , XiuYuan Chen , HengAn Wu\",\"doi\":\"10.1016/j.jmps.2025.106367\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><div>This work presents a unified scaling law for a plane strain hydraulic fracture propagation in layered rocks, where fracturing behavior is influenced by both layer thickness and property contrasts across interfaces, leading to non-self-similar propagation over time. The singular integral balance equation is derived by introducing a kernel function that accounts for the varying elastic modulus and a modified load term that incorporates in-situ stress. The layered distribution of elastic modulus and fracture energy is considered using dynamic tip asymptotics. The governing equations and boundary conditions are then made dimensionless by new characteristic scales of fracture opening, fluid pressure, and fracture length, which are proposed to depict the spatial relationship between the interface and fracture. Solutions are obtained through a decoupled approach to match the fracture morphology and tip boundary conditions. This model captures a novel time-sensitive propagation mode of a hydraulic fracture, that can be dominated by toughness in the tip region and viscosity dissipation at the interface region, especially in multilayer rocks. Consequently, the temporal scale of injection time and the spatial scale of layer thickness are integrated into the characteristic scales. A scaling law is thus proposed to fully consider the variations of elastic modulus, fracture energy, fluid injection rate, injection time, and layer thickness on propagation behavior. The law spans the temporal-spatial parameter space within a general framework that quantifies the evolution of viscosity dissipation induced by interfaces, summarizing four specific cases: the homogeneous model, single-interface model, multi-layer model, and homogenized model. The proposed law provides a universal measure for modeling hydraulic fracturing of layered heterogeneous rocks with arbitrary thickness and propagation stage.</div></div>\",\"PeriodicalId\":17331,\"journal\":{\"name\":\"Journal of The Mechanics and Physics of Solids\",\"volume\":\"206 \",\"pages\":\"Article 106367\"},\"PeriodicalIF\":6.0000,\"publicationDate\":\"2025-09-13\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Journal of The Mechanics and Physics of Solids\",\"FirstCategoryId\":\"5\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/S0022509625003412\",\"RegionNum\":2,\"RegionCategory\":\"工程技术\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"MATERIALS SCIENCE, MULTIDISCIPLINARY\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of The Mechanics and Physics of Solids","FirstCategoryId":"5","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0022509625003412","RegionNum":2,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"MATERIALS SCIENCE, MULTIDISCIPLINARY","Score":null,"Total":0}
A unified temporal-spatial scaling law for hydraulic fracturing in layered rock formations
This work presents a unified scaling law for a plane strain hydraulic fracture propagation in layered rocks, where fracturing behavior is influenced by both layer thickness and property contrasts across interfaces, leading to non-self-similar propagation over time. The singular integral balance equation is derived by introducing a kernel function that accounts for the varying elastic modulus and a modified load term that incorporates in-situ stress. The layered distribution of elastic modulus and fracture energy is considered using dynamic tip asymptotics. The governing equations and boundary conditions are then made dimensionless by new characteristic scales of fracture opening, fluid pressure, and fracture length, which are proposed to depict the spatial relationship between the interface and fracture. Solutions are obtained through a decoupled approach to match the fracture morphology and tip boundary conditions. This model captures a novel time-sensitive propagation mode of a hydraulic fracture, that can be dominated by toughness in the tip region and viscosity dissipation at the interface region, especially in multilayer rocks. Consequently, the temporal scale of injection time and the spatial scale of layer thickness are integrated into the characteristic scales. A scaling law is thus proposed to fully consider the variations of elastic modulus, fracture energy, fluid injection rate, injection time, and layer thickness on propagation behavior. The law spans the temporal-spatial parameter space within a general framework that quantifies the evolution of viscosity dissipation induced by interfaces, summarizing four specific cases: the homogeneous model, single-interface model, multi-layer model, and homogenized model. The proposed law provides a universal measure for modeling hydraulic fracturing of layered heterogeneous rocks with arbitrary thickness and propagation stage.
期刊介绍:
The aim of Journal of The Mechanics and Physics of Solids is to publish research of the highest quality and of lasting significance on the mechanics of solids. The scope is broad, from fundamental concepts in mechanics to the analysis of novel phenomena and applications. Solids are interpreted broadly to include both hard and soft materials as well as natural and synthetic structures. The approach can be theoretical, experimental or computational.This research activity sits within engineering science and the allied areas of applied mathematics, materials science, bio-mechanics, applied physics, and geophysics.
The Journal was founded in 1952 by Rodney Hill, who was its Editor-in-Chief until 1968. The topics of interest to the Journal evolve with developments in the subject but its basic ethos remains the same: to publish research of the highest quality relating to the mechanics of solids. Thus, emphasis is placed on the development of fundamental concepts of mechanics and novel applications of these concepts based on theoretical, experimental or computational approaches, drawing upon the various branches of engineering science and the allied areas within applied mathematics, materials science, structural engineering, applied physics, and geophysics.
The main purpose of the Journal is to foster scientific understanding of the processes of deformation and mechanical failure of all solid materials, both technological and natural, and the connections between these processes and their underlying physical mechanisms. In this sense, the content of the Journal should reflect the current state of the discipline in analysis, experimental observation, and numerical simulation. In the interest of achieving this goal, authors are encouraged to consider the significance of their contributions for the field of mechanics and the implications of their results, in addition to describing the details of their work.