恶梦
发表于 2025-3-21 17:02:38
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Permanent
发表于 2025-3-21 21:06:04
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山羊
发表于 2025-3-22 01:40:24
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
发表于 2025-3-22 08:09:12
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
发表于 2025-3-22 10:32:29
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
发表于 2025-3-22 15:29:43
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
发表于 2025-3-22 17:31:26
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
发表于 2025-3-22 22:05:10
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CLEAR
发表于 2025-3-23 02:36:26
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grounded
发表于 2025-3-23 07:29:34
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