It is widely accepted in the oil and gas industry that viscosity is the single most important transport property for subsurface simulations, well design, and pipeline and process simulations. As crude oil viscosity varies with temperature, pressure, and composition, there are many existing models for estimating crude oil viscosity. Unfortunately, some of these models require difficult-to-obtain measurements. Another issue is that many models are not reliable over the desired range of temperature, pressure, and compositions. In particular, high-pressure high-temperature (HPHT) conditions are problematic.
Accordingly, there are disclosed in the drawings and the following description robust viscosity estimation methods and systems. In the drawings:
It should be understood, however, that the specific embodiments given in the drawings and detailed description do not limit the disclosure. On the contrary, they provide the foundation for one of ordinary skill to discern the alternative forms, equivalents, and modifications that are encompassed together with one or more of the given embodiments in the scope of the appended claims.
Disclosed herein are methods and systems for robust estimation of crude oil viscosity. In an example method, a relative density value (e.g., API gravity) of crude oil is first obtained. The relative density value may be obtained, for example, from previous and/or ongoing measurements of crude oil at any point in a pre-production environment, production system, or post-production system. Using the obtained relative density value, an effective molecular weight of the crude oil is determined. For example, a curve that correlates API gravity with effective molecular weight may be used to determine the effective molecular weight. Further, the effective molecular weight may be modified by applying a Watson characterization adjustment, a gas content adjustment, and/or a relative pressure adjustment. For example, an effective molecular weight determined using the relative density value and a Watson characterization factor (if available) is suitable for calculating a deal oil viscosity. Meanwhile, an effective molecular weight (with or without Watson characterization adjustment) with gas content adjustment is suitable for calculating a saturated oil viscosity. Further, an effective molecular weight (with or without Watson characterization adjustment) with a gas content adjustment and a relative pressure adjustment is suitable for calculating an under-saturated oil viscosity. The disclosed viscosity model calculates crude oil viscosity as a function of the effective molecular weight (or modified variations), temperature, and pressure. In some cases, crude oil viscosity is calculated by scaling a crude oil viscosity value corresponding to an effective molecular weight with gas content adjustment for a gas/oil ratio at bubble point pressure. The calculated crude oil viscosity may be used in fluid flow simulations used for pre-production, production, and/or post-production operations. For example, well completion operations, production settings, and/or enhanced oil recovery settings may be based at least in part on crude oil viscosities calculated using the disclosed viscosity model.
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In at least some embodiments, the computer system 20 uses a calculated crude oil viscosity to perform fluid flow simulations related to pre-production, production, and/or post-production operations. Further, the computer system 20 may use the calculated crude oil viscosity and/or simulation results to direct well completion operations, production settings (e.g., gas lift), and/or enhanced oil recovery settings.
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The viscosity model 128 enables calculation of crude oil viscosity for HPHT conditions that are becoming more common (e.g., offshore deep-water wells and unconventional oil wells such as steam-assisted gravity drain wells). In at least some embodiments, the viscosity model 128 covers all kinds of crude oils ranging from gas condensate, volatile oil, black oil, heavy oil to oil-sand bitumen.
In an example embodiment, the viscosity model 128 is based on a model introduced by Yarranton et al., which relies on gas-chromatography (GC) to predict crude oil viscosity. See Yarranton et al., Cold, Hot, or Dilute: Modeling the Viscosity of Heavy Oil for In Situ Processes, GeoConvention 2013: Integration. In the Yarranton model, viscosity is estimated as:
μ=μ0[1+α(T)ΔP], (1)
where α(T)=(0.008+0.00006MW)(1−0.0033ΔT), and where μo is the oil viscosity at atmospheric pressure and temperature T.
In at least some embodiments, μo is calculated using the following equations:
log[log(μ0+1)]=A−B log(T), (2)
A=k
1(1−exp(−k2MW)+k3MW, (3)
B=k
4(1−exp(−k5MW), (4)
where MW is the molecular weight of crude oil, and k1 to k5 are predetermined constants. As an example, suitable values for k1 to k5 are: k1=9.77; k2=0.01; k3=0.00028; k4=3.71; and k5=0.015.
In at least some embodiments, the value for MW in equations 1, 3, and 4 corresponds to an effective molecular weight (MWEFF) determined by correlating the relative density of crude oil with molecular weight (i.e., GC or other expensive analysis is not needed). One example relative density is referred to as American Petroleum Institute (API) gravity, and in at least some embodiments, the effective molecular weight used in equations 1 to 4 is determined as:
MWEFF=k6+k7γAPI−(k8−k9γAPI)ln(γAPI), (5)
where γAPI is an API gravity value for the crude oil, and k6 to k9 are predetermined constants. As an example, suitable values for k6 to k9 are: k6=1006.7; k7=0.38; k8=222.6; and k9=0.237.
In addition to the performance comparison of Table 1,
A Watson characterization factor or K-factor is a systematic way of classifying a crude oil according to its paraffinic, naphthenic, intermediate or aromatic nature. 12.5 or higher indicate a crude oil of predominantly paraffinic constituents, while 10 or lower indicate a crude of more aromatic nature. Paraffinic (linear) hydrocarbon molecules are subject to more inter-molecular interactions and are consequently more viscous. Incorporation of the Watson characterization factor (Kw) into viscosity models has been shown to improve estimation accuracy. See e.g., Bergman et al., A Consistent and Accurate Deal-Oil-Viscosity Method, SPE Reservoir Evaluation & Engineering, vol. 12, issue 6, pages 815-840 (2009). In at least some embodiments, the viscosity model 128 provides an option of using Kw, if available. For example, the viscosity model 128 may employ an adjustment of effective MW (ΔMWEFF) that includes the effect of Kw is given as:
ΔMWEFF=k10Kw−k11, (6)
where k10 and k11 are predetermined constants. As an example, suitable values for k10 and k11 are: k10=584.41×γAPI−0.655 and k11=6545.26×γAPI−0.632. The performance of the viscosity model 128 with and without the Kw effect is given in Table 2.
In addition to the performance comparison of Table 2,
The viscosity model 128 also may account for the effect of solution gas (i.e., a saturated or live oil scenario). This is done by calculating an effective molecular weight with gas content adjustment determined using available oil field data (e.g., gas gravity, gas/oil ratio, oil API gravity). For example, an effective molecular weight with gas content adjustment (MWEFF,GCA) may be calculated as:
MWEFF,GCA=MWEFF×x0+MWgas×(1−x0)×n, (7)
where MWEFF is calculated from equation 5, x0 is the deal oil molar fraction in the gas saturated oil, MWgas is the gas molecular weight, and n is the non-ideality factor to account for the mixing effect of gas and deal oil. If x0 is expressed in terms of solution gas/oil ratio (Rs) and gas gravity (γg), an effective molecular weight with gas content adjustment (MWEFF,GCA) may be calculated as:
where MWEFF is calculated from equation 5, ρ0 is a density value of the crude oil (e.g., ρ0=141.5/(131.5+oil API gravity) g/cm3), n is a non-ideality factor (e.g., obtained from a regression process), Rs is a gas/oil ratio at bubble point pressure, ρair is a density value of air at standard condition (e.g., 0.001225 g/cm3), γg is a density value of gas, and MWair is a molecular weight value of air (e.g., 29 g/mol).
Accordingly, in at least some embodiments, the viscosity model 128 may estimate viscosity for a saturated crude oil scenario using equation 1-5 and 8 and available crude oil measurements. More specifically, the MW value for equations 1, 3, and 4 may correspond to a MWEFF,GCA value determined using equation 8 for a gas/oil ratio at bubble point pressure. In equation 8, the MWEFF value is calculated using equation 5 (correlating a molecular weight with available relative density measurements). Further, the MWEFF value used for equation 8 may be adjusted using equation 6 (a Watson characterization adjustment).
The viscosity model 128 also may account for HPHT scenarios, where crude oil is often under-saturated. In at least some embodiments, the viscosity model 128 calculates viscosity for an under-saturated crude oil scenario as:
μ=μobexp[k12×(P−Pb)/γAPI], (9)
where μob is a crude oil viscosity value corresponding to an effective molecular weight with gas content adjustment for a gas/oil ratio at bubble point pressure, k12 is a predetermined constant, P is a measured pressure of the crude oil, Pb is a bubble point pressure of the crude oil, and γAPI is an API gravity value for the crude oil. As an example, a suitable value for k12 is k12=0.0015 (e.g., determined from a regression process). In at least some embodiments, μob is calculated using equations 1-5 and 8 (i.e., μob is the calculated saturated oil viscosity). Accordingly, equation 9 operates to scale the saturated oil viscosity calculated using equations 1-5 and 8 based on a relative pressure adjustment (P−Pb) that identifies how close to bubble point pressure the crude oil is at.
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At various times during the drilling process, the drill string 32 shown in
The wireline logging string 56 includes logging tool(s) 59 and a logging tool 58 with sensor(s) 38 and optional source(s) 37 to obtain measurements. The logging tool 58 may also include electronics for data storage, communication, etc. The measurements obtained by sensor(s) 38 are conveyed to earth's surface and/or are stored by the logging tool 58. As previously noted, such measurements as a function of position or time may be analyzed to determine formation properties, fluid properties, and/or fluid flow properties as described herein. At earth's surface, a surface interface 14 receives the measurements via the cable 15B or other telemetry, and conveys the measurements to computer system 20, or another computer system, for analysis including calculating viscosity estimates using viscosity model 128.
Measurement data is periodically sampled and collected from the production well of
In at least some embodiments, the various sensors of the production well of
In at least some embodiments, additional measurement data may be collected using a production logging tool, which may be lowered by a cable into production tubing 72. In other illustrative embodiments, production tubing 72 is first removed, and the production logging tool is then lowered into casing 66. In other alternative embodiments, coil tubing may be used to lower and raise a production logging tool. Such production logging tools may be pushed down either the production tubing 72 or the casing 66 with the production tubing 72 removed. The additional measurement data obtained from such production logging tools can be used to supplement other downhole sensors. The additional measurement data may be communicated to computer system 20, or another computer system, during the logging process, or alternatively may be retrieved after the tool assembly is removed from the downhole environment.
Returning to
The viscosity model 128 described herein can be understood to be a universal model. In other words, viscosity model 128 is both a compositional model and an extended black oil model. With the viscosity model 128, oil composition data and/or oil field property data (e.g., API gravity, gas/oil ratio, etc.) can be used to calculate oil viscosity. Unlike many other models that were developed using oil data for a particular geological region (e.g., Middle East or Gulf of Mexico), the viscosity model 128 was developed using data from worldwide oils. Accordingly, implementation and maintenance of the viscosity model 128 should be simplified compared to model developed using a narrower set of oil data. The viscosity model 128 is the first known attempt to use effective molecular weight tuned by solution gas/oil ratio and gas gravity data to model saturated oil viscosity. This tuning provides greater simplicity and potentially higher accuracy compared to other models. Further, the viscosity model 128 is the first known attempt to extend a black oil viscosity model into HPHT conditions. The accuracy of viscosity model 128 can be significantly improved by tuning with only one measured viscosity value (see e.g.,
Embodiments disclosed herein include:
A: A method that comprises obtaining a relative density value of crude oil, and determining an effective molecular weight of the crude oil based on the relative density value. The method also comprises calculating a crude oil viscosity value as a function of the effective molecular weight. The method also comprises storing or displaying the crude oil viscosity value.
B. A system that comprises a memory unit that stores a relative density value of crude oil, and at least one processing unit that determines an effective molecular weight of crude oil based on the relative density value. The at least one processing unit calculates a crude oil viscosity value as a function of the effective molecular weight.
Each of the embodiments, A and B, may have one or more of the following additional elements in any combination. Element 1: the effective molecular weight (MWEFF) is determined using: MWEFF=k6+k7γAPI−(k8−k9γAPI)ln(γAPI), where γAPI is an API gravity value for the crude oil, and k6 to k9 are predetermined constants. Element 2: determining the effective molecular weight comprises applying a Watson characterization adjustment. Element 3: the Watson characterization adjustment is represented as: ΔMWEFF=k10Kw−k11, where ΔMWEFF is a change in the effective molecular weight, Kw is a Watson characterization factor, and k10 and k11 are predetermined constants. Element 4: determining the effective molecular weight comprises applying a gas content adjustment. Element 5: the effective molecular weight with gas content adjustment (MWEFF,GCA) is represented as:
where MWEFF is an effective molecular weight value based on the obtained relative density of the crude oil, ρ0 is a density value of the crude oil, n is a non-ideality factor, Rs is a gas/oil ratio at bubble point pressure, ρair is a density value of air, γg is a density value of gas, and MWair is a molecular weight value of air. Element 6: determining the effective molecular weight comprises applying a gas content adjustment and a relative pressure adjustment. Element 7: the relative pressure adjustment is based on a comparison of a measured pressure of the crude oil with a bubble point pressure of the crude oil. Element 8: the crude oil viscosity value (μ) is calculated as: =μobexp[k12×(P−Pb)/γAPI], where μob is a crude oil viscosity value corresponding to an effective molecular weight with gas content adjustment for a gas/oil ratio at bubble point pressure, k12 is a predetermined constant, P is a measured pressure of the crude oil, Pb is a bubble point pressure of the crude oil, and γAPI is an API gravity value for the crude oil. Element 9: obtaining the relative density value comprises collecting measurements from sensors in a borehole, and deriving an API gravity value for the crude oil based on the collected measurements. Element 10: determining if the crude oil is saturated and applying a gas content adjustment to the effective molecular weight of the crude oil in response to a determination that the crude oil is saturated; and determining if the crude oil is under-saturated and applying a gas content adjustment and a relative pressure adjustment to the effective molecular weight of the crude oil in response to a determination that the crude oil is under-saturated. Element 11: the crude oil viscosity value is calculated by scaling an initial viscosity value (μ0) represented as: log[log(μ0+1)]=A−B log(T), where A=k1(1−exp(−k2MW)+k3MW and B=k4(1−exp(−k5MW), and where MW is a molecular weight of crude oil, and k1 to k5 are predetermined constants.
Element 12: the at least one processing unit determines the effective molecular weight using: MWEFF=k6+k7γAPI−(k8−k9γAPI)ln(γAPI), where MWEFF is the effective molecular weight, γAPI is an API gravity value for the crude oil, and k6 to k9 are predetermined constants. Element 13: the at least one processing unit determines the effective molecular weight by applying a Watson characterization adjustment. Element 14: the at least one processing unit determines the effective molecular weight by applying at least one of a gas content adjustment and a relative pressure adjustment. Element 15: the at least one processing unit calculates the crude oil viscosity value by scaling an initial crude oil viscosity value corresponding to an effective molecular weight with gas content adjustment for a gas/oil ratio at bubble point pressure. Element 16: the at least one processing unit calculates the crude oil viscosity value by scaling a bubble-point crude oil viscosity value based on the effective molecular weight, temperature, and pressure. Element 17: further comprising sensors in a borehole to collect crude oil measurements, wherein the crude oil measurements are used to derive the relative density value of the crude oil. Element 18: the at least one processing unit performs a simulation of fluid movement based at least in part on the calculated crude oil viscosity value. Element 19: the at least one processing unit directs operations of a well completion unit or production unit based at least in part on the calculated crude oil viscosity value.
Numerous variations and modifications will become apparent to those skilled in the art once the above disclosure is fully appreciated. The ensuing claims are intended to cover such variations where applicable.
Filing Document | Filing Date | Country | Kind |
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PCT/US2014/039410 | 5/23/2014 | WO | 00 |