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- W2897906084 abstract "Abstract The single-phase, multidimensional flow equation for a reservoir block was derived in Chapter 2 . In Chapter 3 , this flow equation was rewritten using CVFD terminology for a reservoir block identified by engineering notation or block order. Chapters 4 and 5 presented the treatment of blocks that fall on reservoir boundaries using fictitious wells. In Chapter 6 , the wellblock production rate equation was derived for various well operating conditions. In this chapter, the single-phase, multidimensional flow equation that incorporates the wellblock production rate and boundary conditions is presented for various fluids, including incompressible, slightly compressible, and compressible fluids. These fluids differ from each other by the pressure dependence of their densities, formation volume factors (FVFs), and viscosities. The presentation includes the flow equation for an incompressible system (rock and fluid) and the explicit, implicit, and Crank-Nicolson equations for slightly compressible and compressible fluids. The flow equations for block-centered grids and point-distributed grids have the same general form. The differences between the two grid systems lie in the construction of the grid, the treatment of boundary conditions, and the treatment of the wellblock production rate as was discussed in Chapters 4-6 Chapter 4 Chapter 5 Chapter 6 . The presentation in this chapter uses CVFD terminology to express the flow equation in a multidimensional domain." @default.
- W2897906084 created "2018-10-26" @default.
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- W2897906084 date "2020-01-01" @default.
- W2897906084 modified "2023-09-23" @default.
- W2897906084 title "Single-phase flow equation for various fluids" @default.
- W2897906084 doi "https://doi.org/10.1016/b978-0-12-819150-7.00007-4" @default.
- W2897906084 hasPublicationYear "2020" @default.
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