油氣滲流力學(xué)

內(nèi)容概要

　　《石油高等院校特色教材：油氣滲流力學(xué)（英文版）》為《油氣滲流力學(xué)》的英文版，由李璗、陳軍斌編寫。全書從驅(qū)動(dòng)力和驅(qū)動(dòng)方式出發(fā)，在對(duì)達(dá)西定律分析的基礎(chǔ)上，遵循由淺入深的認(rèn)識(shí)規(guī)律，詳細(xì)介紹了單相不可壓縮液體的穩(wěn)定滲流理論、剛性水壓驅(qū)動(dòng)下的油井干擾理論、微可壓縮流體的不穩(wěn)定滲流理論、天然氣的滲流規(guī)律、水驅(qū)油理論、油氣兩相滲流理論、流體在雙重介質(zhì)中的滲流理論、非牛頓液體滲流理論等?！　　妒透叩仍盒Ｌ厣滩模河蜌鉂B流力學(xué)（英文版）》可作為石油工程、石油地質(zhì)、地下水工程、油田化學(xué)等專業(yè)本科生教材，也可作為相關(guān)專業(yè)研究生的參考書，還可供從事油氣田勘探與開發(fā)的科研技術(shù)人員參考。

書籍目錄

Chapter 1 Basic law of percolation 1.1 Static state in reservoirs 1.2 Driving forces and driving mode in reservoir 1.3 Darcy's law 1.4 The limitations of Darcy' s law and non-Darcy percolation Exercises Chapter 2 Steady state percolation of single-phase incompressible fluid 2.1 Three basic forms of percolation 2.2 Planar one-dimensional steady state percolation of single-phase incompressible fluid. 2.3 Planar radial fluid flow of single-phase incompressible fluid 2.4 Imperfect well 2.5 Systematic well testing( Step rate testing) 2.6 Differential equation of single-phase fluid percolation Exercises Chapter 3 Interference theory of wells under rigid water drive 3.1 Phenomenon of interference of wells 3.2 Superposition principle of potential 3.3 Method of mirror 3.4 Application of complex function theory in the planar percolation field Exercises Chapter 4 Unsteady state percolation of slightly compressible fluid 4.1 The physical process of elastic fluid percolation towards wells 4.2 The planar one-dimensional unsteady state percolation in semi-infinite formation 4.3 Pressure transient law of elastic fluid unsteady state percolation towards well bore 4.4 Approximate solution of pressure change of fluid percolation towards well in finite closed elastic formation 4.5 Multi interference of wells of elastic unsteady state percolation 4.6 Unsteady state well testing analysis Exercises Chapter 5 Percolation law of natural gas 5.1 Properties of natural gas and its basic differential equation of percolation 5.2 Steady state percolation of gas 5.3 Unsteady state percolation of gas Exercises Chapter 6 Foundation of water/oil displacement theory 6.1 Piston like displacement of oil by water 6.2 Bottom water coning 6.3 Theoretical foundation of non-piston like displacement of oil by water Exercises Chapter 7 Percolation theory of oil-gas two phases( dissolved gas drive) 7.1 Basic differential equation of oil-gas two-phases percolation 7.2 Oil-gas two-phase steady state percolation 7.3 Unsteady state percolation of gassy fluid Exercises Chapter 8 Flow in dual-media 8.1 Flow characteristics in dual-media 8.2 Basic flow equation of single-phase slightly compressible fluid in dual-media 8.3 Pressure distribution in infinite dual-media 8.4 Oil-water two-phase flow in the dual-media 8.5 Flow of fluid in pure fracture formation Exercises Chapter 9 Percolation of non-Newtonian liquid 9.1 Mechanical behavior and type of non-Newtonian liquid 9.2 Percolation of non-Newtonian power law liquid Exercises Chapter 10 Theory of similarity 10.1 Concept of similarity 10.2 Kinematical and dynamic similarity 10.3 Scaled physical model and law of similarity 10.4 Dimension analysis examples for the known equations of physical system 10.5 Examples of analog 10.6 Partial similarity in the scaling models 10.7 Special aspects of standard fitting of porous medium model Exercises Appendix Appendix A Flow equation in cylindrical coordinate Appendix B To obtain the solution of one-dimensional unsteady state flow by the Laplace transformation Appendix C Calculation procedure of error function eft(x) Appendix D Calculation procedure of exponential integral function -Ei(-x) Appendix E Calculation procedure of function F(x) Appendix F Conversion relationship between the commonly used units in reservoir engineering Appendix G Factor and signs of commonly used prefixes in SI system and imperial system of unit References

章節(jié)摘錄

版權(quán)頁(yè)：   插圖：   If the flow which exists in the bottom water coning is called disturbed movement,the flowwith same production and under same condition withoutbottom water coning is called undisturbed movement,andthe two flow laws will be compared later. Assume the top and bottom of formation areimpermeable,the potential distribution on side face of runder two situations is the same.Because the undisturbedrange is wider than the disturbed range,under the samecondition,the potential of disturbed flow at arbitrary pointin formation is smaller than that of undisturbed flow.Thepotential along the cylinder surface of rw of undisturbedflow is expressed with A'B'C'D',which lies in the rightside of the distributing curve ABCD of the potential ofdisturbed flow as shown in Figure 6-9.Because theproduction of the two is equal,its area should be equal to the area ABCDEA. It can be seen from Figure 6 -9 that the intersection point C'of straight line DC and A'B'C'D'lies below the point C,and the coordinate of point C is coincident with the coning apex.At thismoment,because the flow rate of disturbed flow and undisturbed flow is equal,the area A'B'C'D'EA'should be equal to the area ABCDEA ;that is:the area of belt ABCC'B'A'A should be equal to thearea of triangle C'D'D. If the potential remains unchanged and the production of well increases,then thepotential on the borehole wall must decrease,according to the equilibrium condition of waterconing,the following expression can be obtained: The expression above is the slope of line CD,so before the bottom water breaks through theoil well,the potential of oil-bearing part below well bottom can be expressed with thecurve BC as shown in Figure 6-10(b).On the coning apex,the included angle between tangentof curve BC and vertical line is:/3 is positive.So under this condition,the shape of oil-water interface presents tip end at thelocation of well axis as shown in Figure 6-10(a).Water will break through the oil well quickly.When the flow rate is equal and also the potential,the potential of undisturbed flow alongthe well axis is bigger than that of disturbed flow,which is expressed with the curve B'B"C'D' inFigure 6-10(b) ,which lies in the right side of the curve BC.It can be seen that because the areaof triangle C'D'D should be equal to the area of banded region B'B"C'CB,under any condition,the area of triangle C'D'D should be bigger than that of arch.

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《石油高等院校特色教材:油氣滲流力學(xué)(英文版)》可作為石油工程、石油地質(zhì)、地下水工程、油田化學(xué)等專業(yè)本科生教材，也可作為相關(guān)專業(yè)研究生的參考書，還可供從事油氣田勘探與開發(fā)的科研技術(shù)人員參考。

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