US2021270124A1PendingUtilityA1

Method for distinguishing authenticity of high-pressure physical property parameters of oil reservoirs

Assignee: YANGZHOU JIANGSU OILFIELD RUIDA PETROLEUM ENGINEERING TECH DEVELOPMENT CO LTDPriority: Jan 30, 2019Filed: Aug 8, 2019Published: Sep 2, 2021
Est. expiryJan 30, 2039(~12.5 yrs left)· nominal 20-yr term from priority
Inventors:Haijin Zheng
E21B 49/00E21B 47/009E21B 47/047E21B 49/0875
27
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Claims

Abstract

A method for distinguishing an authenticity of high-pressure physical property parameters of oil reservoirs is provided. The method includes: collecting the high-pressure physical property parameters, screening a standard well, calculating a pump efficiency by means of formulas, then calculating an absolute value Δ=|ηtheory−ηreality| of each group of absolute errors, and taking a smallest absolute value Δmin of the absolute error. wherein Δmin≤ε, ε is a set accuracy, generally, 0≤ε≤0.02, and the high-pressure physical property parameters corresponding to a group of the theoretical pump efficiency ηtheory and the real pump efficiency ηreality are real high-pressure physical property parameters of an oil reservoir to be distinguished. The method provides a fast, simple and practical means for distinguishing correct high-pressure physical property parameters. The method is applicable to an oil well in a certain zone of an oil reservoir to be determined.

Claims

exact text as granted — not AI-modified
What is claimed is: 
     
         1 . A method for distinguishing an authenticity of high-pressure physical property parameters of an oil reservoir, comprising the following steps:
 1) collecting the high-pressure physical property parameters: collecting the high-pressure physical property parameters of a sampled well of the oil reservoir to be distinguished, wherein the high-pressure physical property parameters comprise a gas-oil ratio GOR, a solubility coefficient α, a saturation pressure P b , a formation crude oil density ρ o , and a formation crude oil viscosity μ o ;   2) screening a standard well: determining the standard well from multiple oil wells continuously exploited in a same block and a same zone as the sampled well, wherein an indicator diagram of the standard well reflects a pump of the standard well does not leak and a tubing string of the standard well does not leak, and meanwhile, the standard well has a lowest water content, a highest liquid yield and a largest submergence in the multiple oil wells;   3) calculating a pump efficiency: substituting each group of the high-pressure physical property parameters collected in step 1) and related data of the standard well screened in step 2) into the following formula, and calculating a theoretical pump efficiency η theory  and a real pump efficiency η reality  of the standard well:   
       
         
           
             
               
                 η 
                 theory 
               
               = 
               
                 
                   
                     
                       S 
                       - 
                       λ 
                     
                     S 
                   
                   ⁢ 
                   β 
                 
                 - 
                 
                   
                     Q 
                     leak 
                   
                   
                     Q 
                     theory 
                   
                 
               
             
           
         
         
           
             
               λ 
               = 
               
                 
                   
                     π 
                     ⁢ 
                     
                         
                     
                     ⁢ 
                     
                       D 
                       2 
                     
                     ⁢ 
                     ρ 
                     ⁢ 
                     
                         
                     
                     ⁢ 
                     gh 
                   
                   
                     4 
                     ⁢ 
                     
                         
                     
                     ⁢ 
                     E 
                   
                 
                 ⁢ 
                 
                   ( 
                   
                     
                       
                         L 
                         1 
                       
                       
                         f 
                         1 
                       
                     
                     + 
                     
                       
                         L 
                         2 
                       
                       
                         f 
                         2 
                       
                     
                     + 
                     … 
                     + 
                     
                       
                         L 
                         n 
                       
                       
                         f 
                         n 
                       
                     
                     + 
                     
                       
                         L 
                         p 
                       
                       
                         f 
                         t 
                       
                     
                   
                   ) 
                 
               
             
           
         
         
           
             
               β 
               = 
               
                 1 
                 
                   1 
                   + 
                   
                     
                       
                         ( 
                         
                           GOR 
                           - 
                           
                             α 
                             ⁢ 
                             
                                 
                             
                             ⁢ 
                             
                               P 
                               s 
                             
                           
                         
                         ) 
                       
                       ⁢ 
                       
                         ( 
                         
                           1 
                           - 
                           
                             f 
                             w 
                           
                         
                         ) 
                       
                     
                     
                       ( 
                       
                         
                           10 
                           ⁢ 
                           
                               
                           
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                             P 
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                         + 
                         1 
                       
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         when P s ≥P b , making P s =P b , wherein if an oil pipe is anchored, L p /f t  is not comprised in λ;
   η reality   =Q   reality   /Q   theory *100%;
 
     Q   theory   =πD   2   ρgSN/ 4; 
     Q   leak   =πDρgδ   3   h /(12 L   p /μ);
 
   ρ=(1− f   w )*ρ o   +f   w *ρ w ;
 
     h=h   dynamic +1000*( p   oil   −p   casing )* g/ρ;    
     P   s   =p   casing +( h   setting   −h   dynamic )*ρ o   *g/ 1000;
 
   μ= f   w +(1− f   w )*μ o ;
 
 
         wherein 
         Q reality  represents a real output of an oil well of the multiple oil wells; 
         Q theory  represents a theoretical displacement of the oil well of the multiple oil wells; 
         Q leak  represents a pump leakage; 
         the GOR represents the gas-oil ratio and a unit of the GOR is m 3 /m 3 ; α represents the solubility coefficient and a unit of the solubility coefficient is m 3 /(m 3 ·Mpa); P b  represents the saturation pressure and a unit of the saturation pressure is Mpa; ρ o  represents the formation crude oil density and a unit of the formation crude oil density is t/m 3 ; μ o  represents the formation crude oil viscosity and a unit of the formation crude oil viscosity is Pa·S; 
         λ represents a stroke loss of the standard well and a unit of the stroke loss is m; β represents a gas influence coefficient of the standard well, wherein the gas influence coefficient is dimensionless; ρ represents a mixed liquid density of the standard well and a unit of the mixed liquid density is t/m 3 ; h represents a pump lift of the standard well and a unit of the pump lift is m; P s  represents a submergence pressure of the standard well and a unit of the submergence pressure is Mpa; μ represents a hydrodynamic viscosity of the standard well and a unit of the hydrodynamic viscosity is Pa·S; f w  represents a rate of a water content of a pumped liquid in the standard well; h dynamic  represents a dynamic liquid level depth of the standard well and a unit of the dynamic liquid level depth is m; D represents a pump diameter of the standard well and a unit of the pump diameter is m; h setting  represents a pump setting depth of the standard well and a unit of the pump setting depth is m; p oil  represents a wellhead oil pressure of the standard well and a unit of the wellhead oil pressure is Mpa; P casing  represents a casing pressure of the standard well and a unit of the casing pressure is Mpa; S represents a stroke length of the standard well and a unit of the stroke length is m; N represents a stroke frequency of the standard well and a unit of the stroke frequency is 1/min; L 1 , L 2  and L n  respectively represent a length of a first-level rod, a length of a second-level rod and a length of an n-level rod of the standard well and a unit of the length is m; f 1 , f 2  and f n  respectively represent a cross-sectional area of a first-level rod, a cross-sectional area of a second-level rod and a cross-sectional area of an n-level rod of the standard well and a unit of the cross-sectional area is m 2 ; L p  represents a pump depth of the standard well and a unit of the pump depth is m; f t  represents a cross-sectional area of a metal part of the oil pipe of the standard well and a unit of the cross-sectional area is m 2 ; E represents an elastic modulus of a steel of a pumping rod in the standard well, and E is 2.1*10 7  N/cm 2 ; g represents a gravity acceleration of the standard well and a unit of the gravity acceleration is m/s 2 ; δ represents an annular gap between a pump plunger and a pump cylinder of the standard well and a unit of the annular gap is m; L pl  represents a length of the pump plunger of the standard well and a unit of the length of the pump plunger is m; and ρ w  represents a water density of the standard well and a unit of the water density is t/m 3 ; and 
         4) screening results: after the pump efficiency is calculated in the step 3), for the standard well screened in step 2) and the each group of the high-pressure physical property parameters collected in step 1), obtaining a group of the theoretical pump efficiency η theory  and the real pump efficiency η reality , and for each group of the theoretical pump efficiency η theory  and the real pump efficiency η reality , calculating an absolute value Δ=|η theory −η reality | of an absolute error, and taking a smallest absolute value Δ min  of the absolute error:
   Δ min =|η theory −η reality |;
 
 
         wherein if Δ min  meets a condition: Δ min ≤ε, wherein ε is a set accuracy, and 0≤ε≤0.02, 
         the high-pressure physical property parameters corresponding to the group of the theoretical pump efficiency η theory  and the real pump efficiency η reality , comprising the gas-oil ratio GOR, the solubility coefficient α, the saturation pressure P b , the formation crude oil density ρ o , and the formation crude oil viscosity μ o , are real high-pressure physical property parameters of the oil reservoir to be distinguished.

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