dc.creator | Gutierrez, Julieta | |
dc.creator | Serebrinsky, Santiago Ariel | |
dc.date.accessioned | 2022-08-19T19:26:25Z | |
dc.date.accessioned | 2022-10-15T06:37:00Z | |
dc.date.available | 2022-08-19T19:26:25Z | |
dc.date.available | 2022-10-15T06:37:00Z | |
dc.date.created | 2022-08-19T19:26:25Z | |
dc.date.issued | 2021-09 | |
dc.identifier | Gutierrez, Julieta; Serebrinsky, Santiago Ariel; Propagation regimes, transition times, and approximate universality in 2D hydraulic fracture propagation with fluid lag; Elsevier Science; Engineering Fracture Mechanics; 254; 107905; 9-2021; 1-11 | |
dc.identifier | 0013-7944 | |
dc.identifier | http://hdl.handle.net/11336/166143 | |
dc.identifier | CONICET Digital | |
dc.identifier | CONICET | |
dc.identifier.uri | https://repositorioslatinoamericanos.uchile.cl/handle/2250/4356064 | |
dc.description.abstract | During its lifetime, a hydraulic fracture is known to traverse a trajectory in a region of a parametric space of non-dimensional evolutionary parameters. The topology of this diagram depends upon the phenomena considered. For the specific case of a 2D-plane strain fracture propagating in an elastic solid on a straight path normal to the minimum compressive stress, with a constant rate of injection of an incompressible newtonian fluid, and without leak-off, the diagram is a triangle whose vertices are typically called O, M, and K. The non-dimensional parameters are the toughness K and remote stress T (monotonically increasing with time). At each point in the trajectory P(t)=(K,T)(t), the configuration of the fracture is essentially described by several non-dimensional variables, in this case the opening Ω0 and pressure Π0 at the inlet, and the length γ. When fluid lag is considered, as in this case, a fourth variable (e.g., the fluid fraction ξf) can be appended to build the descriptive set F0={Ω0,Π0,γ,ξf}. Various propagation regimes are observed across the MKO triangle. As the main results, we: (1) provide specific, K-dependent transition times among the propagation regimes; and (2) found that the transient evolutions of all propagating cracks with moderate values of the non-dimensional toughness (K≳0.3), from the OK edge to the MK edge, are contained in a thin bundle about a universal curve in the F0-space. This result can be applied, e.g., to readily setup approximate initial conditions for more detailed hydraulic fracture propagation simulations. In addition, we developed a four-parameter family of parametrizations of the MKO triangle suitable for plotting trajectories and other loci on the triangle. | |
dc.language | eng | |
dc.publisher | Elsevier Science | |
dc.relation | info:eu-repo/semantics/altIdentifier/url/https://www.sciencedirect.com/science/article/pii/S0013794421003337 | |
dc.relation | info:eu-repo/semantics/altIdentifier/doi/http://dx.doi.org/10.1016/j.engfracmech.2021.107905 | |
dc.rights | https://creativecommons.org/licenses/by-nc-nd/2.5/ar/ | |
dc.rights | info:eu-repo/semantics/restrictedAccess | |
dc.subject | FLUID LAG | |
dc.subject | HYDRAULIC FRACTURE | |
dc.subject | TWO DIMENSIONAL | |
dc.title | Propagation regimes, transition times, and approximate universality in 2D hydraulic fracture propagation with fluid lag | |
dc.type | info:eu-repo/semantics/article | |
dc.type | info:ar-repo/semantics/artículo | |
dc.type | info:eu-repo/semantics/publishedVersion | |