Titlebook: Applied Hydrodynamics in Petroleum Exploration; Eric C. Dahlberg Book 1995Latest edition Springer-Verlag New York, Inc. 1995 Engineering G

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Permanent

山羊

Potential Energy Variation in Fluids,sed up (converted to .) as the spring expands back to its original, presqueezed length. Potential energy is thus energy made by storing up the results of some active work. One does work in winding up tighter and tighter the spring inside a small toy car. When the car is released on the floor, the st

净礼

Rock, Pore Space, and Fluid Systems,nment in terms of single bodies of homogeneous fluid. It is not really this way in a rock, however, since any single fluid mass is essentially interspersed within a network of intergranular pore spaces, throats, fracture openings, etc. As long as the fluids are in complete communication, the princip

IOTA

Nonnormal Formation Pressures, down to the depth of the measurement is termed ., even though for the conditions at hand it may be completely normal. The standard is assumed to be the local hydrostatic gradient from the surface, and this gradient is termed .. The relationships for different pressures measured beneath the surface

表状态

Pressure Variation with Depth,om simple graphical plots of formation pressure against the depths (or elevation) at which they are measured. There are essentially three exploration problem areas in which such P—D plots are applied: the first concerns the prediction of pay thickness (i.e., placing oil-water, gas-water, and gas-oil

指令

Potentiometric Maps and Subsurface Water Flow,ion water within a particular aquifer or subsurface reservoir. The elevation of the surface at any point on it reflects (but does not exactly equal) the height to which a column of water would rise above a reference datum within a vertical tube (ignoring capillarity). This is an approximation of the

拖债

CLEAR

grounded

Entrapment Potential Maps,cannot escape in any direction. One classification scheme, devised by Meissner (1984) and illustrated in Figure 11.1, proposes a three end-member system constituting a triangle. The three end-members in the scheme occupy positions at its apices: . (lower left), . (lower right), and . (top center). S