• Corpus ID: 248811333

Three-dimensional buoyant hydraulic fracture growth: constant release from a point source

@inproceedings{Mori2022ThreedimensionalBH,
  title={Three-dimensional buoyant hydraulic fracture growth: constant release from a point source},
  author={A. Mori and B. Lecampion Geo-Energy Laboratory - Gaznat Chair on Geo-Energy and Ecole polytechnique f'ed'erale de Lausanne and Switzerland.},
  year={2022}
}

• A. Mori, B. L. G. L. -. G. C. O. Geo-Energy, +1 author Switzerland.
• Published 16 May 2022
• Physics

Hydraulic fractures propagating at depth are subjected to buoyant forces caused by the density contrast between fluid and solid. This paper is concerned with the analysis of the transition from an initially radial towards an elongated buoyant growth – a critical topic for the understanding of vertical hydraulic fractures extent in the upper earth crust. Using fully coupled numerical simulations and scaling arguments, we show that a single dimensionless number governs buoyant hydraulic fracture growth: the dimensionless viscosity of a radial hydraulic fracture at the time when buoyancy becomes of order one. It quantifies if the transition to buoyancy occurs when the growth of the radial hydraulic fracture is either still in the regime dominated by viscous flow dissipation or already in the regime where fracture energy dissipation dominates. A family of fracture shapes emerge at late time from finger-like (toughness regime) to inverted elongated cudgel-like (viscous regime). 3D toughness dominated buoyant fractures exhibit a finger-like shape with a constant volume toughness dominated head and a viscous tail having a constant uniform horizontal breadth: there is no further horizontal growth past the onset of buoyancy. However, if the transition to buoyancy occurs while in the viscosity dominated regime, both vertical and horizontal growths continue matching scaling arguments. As soon as the fracture toughness is not strictly zero, horizontal growth stops when the dimensionless horizontal toughness becomes of order one. The horizontal breadth follows the predicted scaling.