The general form of non-linear single-phase pressure diffusion @model with the finite number of wells is given by:
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where
reservoir pressure | time | ||
fluid density | position vector | ||
effective porosity | position vector of the -th source | ||
total compressibility | Dirac delta function | ||
gradient operator | |||
formation permeability to a given fluid | gravity vector | ||
dynamic viscosity of a given fluid | fluid velocity under Darcy flow | ||
sandface flowrates of the -th well | reservoir boundary | ||
reservoir boundary flow condition through the reservoir boundary , which is usually the aquifer or gas cap |
The alternative form is to write down equations and in reservoir volume outside wellbore and match the solution to the fluid flux through the well-reservoir contact:
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where
well-reservoir contact of the -th well | |
normal vector of differential area on the well-reservoir contact, pointing inside wellbore | |
sandface flowrates at the -th well (could be injecting to or producing from the reservoir ) |
Physical models of pressure diffusion can be split into two categories: Newtonian and Rheological (non-Newtonian) based on the fluid stress model.
Mathematical models of pressure diffusion can be split into three categories: Linear, Pseudo-Linear and Non-linear.
These models are built using Numerical, Analytical or Hybrid pressure diffusion solvers.
Many popular 1DR solutions can be approximated by Radial Flow Pressure Diffusion @model which has a big methodological value.
The simplest analytical solutions for pressure diffusion are given by 1DL Linear-Drive Solution (LDS) and 1DR Line Source Solution (LSS).
Physics / Mechanics / Continuum mechanics / Fluid Mechanics / Fluid Dynamics / Pressure Diffusion / Pressure Diffusion @model
[ Aquifer Drive Models ] [ Gas Cap Drive Models ]
[ Linear single-phase pressure diffusion @model ]