SPE 107981 Estimation of Reserves Using the Reciprocal Rate Method P.D. Reese, SPE, D. Ilk, SPE, and T.A. Blasingame, SPE, Texas A&M U. Copyright 2007, Society of Petroleum Engineers This paper was prepared for presentation at the 2007 SPE Rocky Mountain Oil & Gas Technology Symposium held in Denver, Colorado, U.S.A., 16–18 April 2007. This paper was selected for presentation by an SPE Program Committee following review of information contained in an abstract submitted by the author(s). Contents of the paper, as presented, have not been reviewed by the Society of Petroleum Engineers and are subject to correction by the author(s). The material, as presented, does not necessarily reflect any position of the Society of Petroleum Engineers, its officers, or members. Papers presented at SPE meetings are subject to publication review by Editorial Committees of the Society of Petroleum Engineers. Electronic reproduction, distribution, or storage of any part of this paper for commercial purposes without the written consent of the Society of Petroleum Engineers is prohibited. Permission to reproduce in print is restricted to an abstract of not more than 300 words; illustrations may not be copied. The abstract must contain conspicuous acknowledgment of where and by whom the paper was presented. Write Librarian, SPE, P.O. Box 833836, Richardson, TX 75083-3836, U.S.A., fax 01-972-952-9435. Abstract In this work we develop, validate, and apply the "reciprocal rate method" to estimate oil reserves using only rate-time production data. This approach requires the development of boundary-dominated flow, and can be used to validate reserve extrapolations from numerical/analytical reservoir models. The methodology does presume that flowing well bottomhole pressures are approximately constant — but we will demonstrate that the method is tolerant of substantial changes in the flowing bottomhole pressure. This approach requires a plot of the reciprocal of flowrate (1/q) and the so-called "material balance time" (cumulative production/flowrate or Np/q). The "secret" to this approach is the use of material balance time — this function accounts for most variation in rate/pressure, and permits the extrapolation of the 1/q function. This methodology has been applied for oil and gas wells (including oil wells with high water production) — and in all cases, the reciprocal rate method has proven to be robust and consistent. The primary technical contributions of this work are: ● Direct method to estimate reserves using only rate-time data (time, rate, and cumulative production). ● The reciprocal rate method is based on variable-rate theory, and is more rigorous than Arps approach (exponential or hyperbolic rate relations). Introduction Simply put, the Reciprocal Rate Method is an unsophisticated, yet theoretical approach for estimating reserves. The governing equation is derived in Appendix A — and for convenience is given as the "Arps" form of the result: [Arps (1942)] 1 1 Di ⎡ Np = + ⎢ q qi qi ⎢⎣ q ⎤ ⎥ ............................................................. (1) ⎥⎦ Where the qi and Di parameters can be derived from theory for the black oil case (see Appendix A). For reference, the Arps exponential model is given as: q = qi e− Dit ......................................................................... (2) It is important (perhaps critical) to note that Eq. 1 (and 2) are derived under the assumption that the well is producing at a constant flowing bottomhole pressure, pwf. Our contention is that the Reciprocal Rate Method is robust and will tolerate changes in pwf, particularly smooth changes. We illustrate the robustness of this method using appropriate field examples. For convenience, we write Eq. 1 as a simple straight-line relation with arbitrary coefficients. This form is given as: ⎡ Np 1 =c+m⎢ q ⎢⎣ q ⎤ ⎥ ................................................................. (3) ⎥⎦ Multiplying through Eq. 3 by the flowrate term (q) yields: 1 = c q + m Np .................................................................... (4) At depletion, the flowrate will decrease to zero (i.e., q → 0), and Eq. 4 reduces to the following identity: ( Np ) q →0 ≡ 1 (reserves)................................................... (5) m The procedure for this methodology is as follows: Step 1: Plot 1/q versus Np/q. Step 2: Estimate the slope of the straight-line portion of the data trend, m. As advice, the "later" data should yield the most consistent trend. Step 3: Take the reciprocal of the slope (m) as the estimate of the reserves which will be produced at depletion (boundary-dominated flow regime) for this particular production scenario. As noted above, the single most important constraint is the assumption of the constant flowing bottomhole pressure — however; we will demonstrate the utility of this approach, even in the presence of erratic changes in the flowing bottomhole pressures. Demonstration The purpose of this work is to provide the practicing engineer with a theoretically robust, yet extraordinarily simple methodology to estimate reserves using production performance data (in this case rate-time data only). Having said that, there are limitations — in particular, for gas wells which do not exhibit "liquid" character (exponential rate decline), our success has been variable, and this case remains a work in progress. However; for the case of oil wells we have had considerable (almost universal) success — less-than-desired results for oil cases tend to occur when some portion of the data is corrupted by a substantial "non-ideal" condition (e.g., the continuous 2 P.D. Reese, D. Ilk, and T.A. Blasingame SPE 107981 evolution of formation damage as will be indicated by one of the example cases). In this section we present 3 case histories (all oil wells) where the Reciprocal Rate Method has been successfully applied. These cases are presented in relevant detail below: haps should) provide a simple reservoir signature. One "test" would be to re-plot the data for this case as a log-log reciprocal rate plot. This plot could serve as a diagnostic to confirm that the straight-line observed on the Cartesian plot is actually a relevant (reservoir) response. Example 1: Well NRU 3106 (Texas, USA) In Fig. 3 we present the log-log reciprocal rate plot for this case (Well NRU 3106 (Texas, USA)). We immediately note that, while we might "adjust" the model constant, the translation of the reciprocal model to the log-log plot (straight line trend → power-law trend) confirms the validity of the (Cartesian) reciprocal rate plot. This well is a production well in a low permeability reservoir that is being waterflooded at pressures above the fracture gradient (continuous fracture propagation is likely in the injection wells). The oil and water production profiles for this case are shown in Fig. 1. Reciprocal Rate Method Well NRU 3106 (Texas, USA) — Log-Log Reciprocal Rate Plot Reciprocal Rate Method Well NRU 3106 (Texas, USA) — Production History Plot 0 10 3 Legend: Well NRU 3106 qo Function qw Function qo Exponential Rate Model Reciprocal of Oil Rate, 1/qo,1/STB/Day 2 10 1 10 1 -3 qo = 4.8771x10 exp(-5.61878x10 t), STB/D (Np)max = Reserves = 86,000 STB 4000 3500 3000 2500 2000 1500 1000 500 -1 10 -2 10 -2 -3 10 -4 10 0 10 10 Production Time, Days The Cartesian format plot of 1/q versus Np/q — i.e., the Reciprocal Rate Method plot for this case is shown in Fig. 2. We note an excellent data trend, and we can clearly see that the method will yield relevant results for this case. Reciprocal Rate Method Well NRU 3106 (Texas, USA) — Reciprocal Rate Plot -2 -5 0.10 (Np)max = Reserves = 86,000 STB 0.09 10 3 4 5 10 10 This case considers a production well in a high permeability oil reservoir that is simultaneously experiencing waterflood and water influx. Our rationale in presenting this case is to validate that the proposed reciprocal rate model can be applied to reservoir behavior that is experiencing addition of energy from "outside" of the reservoir. The historical performance data for this case is presented in Fig. 4. Reciprocal Rate Method Well WWL B41 (Louisiana, USA) — Production History Plot 4 0.06 1 10 2 (Np)max = Reserves = 360,000 STB 4000 3500 0 10 In Fig. 2 it is clear that the reciprocal rate method has some merit — from empirical as well as theoretical standpoints. The most common observation is that the 1/q versus Np/q trend is excellent — but why? The most obvious answer is theory — this case considers a black oil that is being repressured by waterflooding, which certainly could (and per- -3 qo = 4.4009x10 exp(-1.22247x10 t), STB/D 3000 Figure 2 — Example 1: Cartesian reciprocal rate plot — Well NRU 3106 (Texas, USA). Excellent match of the data functions for this case. 2 10 2500 Oil Material Balance Time (Np/qo), Days 3 10 2000 9000 8000 7000 5000 4000 3000 2000 0.01 6000 Legend: Well NRU 3106 1/qo Function 1/qo Linear (Np/qo) Model 0.02 500 0.03 Legend: Well WWL B41 qo Function qw Function qo Exponential Rate Model 0 0.04 Oil and Water Rates, qoand qw, STB/D 10 0.05 0 2 Example 2: Well WWL B41 (Louisiana, USA) 0.07 0.00 10 Figure 3 — Example 1: Log-log format reciprocal rate plot — Well NRU 3106 (Texas, USA). Excellent match of data confirms reciprocal rate concept model. 0.08 1000 Reciprocal of Oil Rate, 1/qo,1/STB/Day 0.12 1/qo = 1.9545x10 + 1.15207x10 (Np/qo), 1/STB/D 1 Oil Material Balance Time (Np/qo), Days Figure 1 — Example 1: Oil and water rate history plot — Well NRU 3106 (Texas, USA). 0.11 -5 1/qo = 1.9545x10 + 1.15207x10 (Np/qo), 1/STB/D (Np)max = Reserves = 86,000 STB 1500 0 0 10 Legend: Well NRU 3106 1/qo Function 1/qo Linear (Np/qo) Model 1000 Oil and Water Rates, qoand qw, STB/D 10 Production Time, Days Figure 4 — Example 4: Oil and water rate history plot — Well WWL B41 (Louisiana, USA). The Cartesian format plot of 1/q versus Np/q — i.e., the Estimation of Reserves Using the Reciprocal Rate Method Reciprocal Rate Method Well WWL B41 (Louisiana, USA) — Reciprocal Rate Plot 0.050 Legend: Well WWL B41 1/qo Function 1/qo Linear (Np/qo) Model Reciprocal of Oil Rate, 1/qo,1/STB/Day 0.045 0.040 3 Reciprocal Rate Method SE Asia Oil Well — Production and Pressure History Plot 4 5000 10 Legend: SE Asia Oil Well Oil Flowrate (qo), STB/D Wellbore Flowing Pressure (pwf), psia 4500 4000 3500 3000 3 2500 10 Oil Flowrate 2000 1500 0.035 1000 Wellbore Flowing Pressure 500 0.030 0 225 200 175 150 125 100 75 50 25 0.025 0 2 10 Wellbore Flowing Pressure (pwf), psia Reciprocal Rate Method plot for this case is shown in Fig. 5. This case also provides an extraordinary correlation trend for the 1/q — Np/q data. This performance strongly confirms the reciprocal rate method, and suggests that we should expect the method to work for cases of external reservoir drive energy. Oil Flowrate (qo), STB/D SPE 107981 0.020 Production Time, days 0.015 Figure 7 — Example 3: Oil rate and pressure history plot — Southeast Asia — Oil Well. -3 -6 1/qo = 2.4024x10 + 2.77778x10 (Np/qo), 1/STB/D 0.005 14000 13000 12000 11000 10000 9000 8000 7000 6000 5000 4000 3000 0 1000 2000 (Np)max = Reserves = 360,000 STB 0.000 Oil Material Balance Time (Np/qo), Days Figure 5 — Example 2: Cartesian reciprocal rate plot — Well WWL B41 (Louisiana, USA). Very good correlation of behavior. As in the previous case, we would like to assess the general character of the 1/q versus Np/q concept model. In Fig. 6 we present the log-log reciprocal rate plot for this case (WWL B41 (Louisiana, USA)). We immediately note that, while we might "adjust" the model constant, the translation of the reciprocal model to the log-log plot confirms the validity of the (Cartesian) reciprocal rate plot. Reciprocal Rate Method Well WWL B41 (Louisiana, USA) — Log-Log Reciprocal Rate Plot 0 -3 -6 1/qo = 2.4024x10 + 2.77778x10 (Np/qo), 1/STB/D (Np)max = Reserves = 360,000 STB -1 10 In Fig. 8 we present "Arps" analysis (semilog rate-time plot with the Arps exponential model imposed on the data). Obviously the rate profile mimics the influences of the pressure behavior, except at the latest times, where damage appears to be continuously evolving. Reciprocal Rate Method SE Asia Oil Well — Production History Plot 4 10 Legend: SE Asia Oil Well qo Function qo Exponential Rate Model Change in Reservoir Model (Increasing Damage) 3 10 -3 qo = 1546exp(-3.0x10 t), STB/D (Np)max = Reserves = 515,000 STB (Exponential Trend Not Applicable) 225 200 175 150 125 100 75 50 10 25 2 10 -2 0 Reciprocal of Oil Rate, 1/qo,1/STB/Day 10 From Fig. 7 we note that the late-time rate and pressure are "off-trend," and while we do not know the cause, we do observe a degradation in the rate performance with time (evolving well damage may be the culprit). Oil Flowrate, qo, STB/D 0.010 Production Time, Days Figure 8 — Example 3: Oil rate history plot with exponential rate model imposed — Southeast Asia — Oil Well. -3 10 Legend: Well WWL B41 1/qo Function 1/qo Linear (Np/qo) Model -4 10 0 10 1 10 2 10 3 10 4 10 5 10 Oil Material Balance Time (Np/qo), Days Figure 3 — Example 2: Log-log reciprocal rate plot — Well WWL B41 (Louisiana, USA). Excellent performance of the reciprocal rate concept model. Example 3: Southeast Asia — Oil Well This case is somewhat unique in that the data appear to be relevant (comparison of multiple analyses), but the Arps ratetime relation clearly fails to represent the behavior for this case. The original data for this case are shown in Fig. 7. As noted, the trend shown in Fig. 8 appears to be valid — but this trend is found to be inconsistent with all of the other analyses that have been applied to these data (estimated reserves are almost a factor of 2 too high). In Fig. 9 we present the Cartesian format plot of 1/q versus Np/q (i.e., the Reciprocal Rate Method plot). The obvious features which are not aligned are the early-time (transient) flow data, as well as the "late-time" data which appear to be (strongly) affected by evolving reservoir damage (cause/ mechanism unknown). 4 P.D. Reese, D. Ilk, and T.A. Blasingame reserves for this system based on: Reciprocal Rate Method SE Asia Oil Well — Reciprocal Rate Plot ( Np ) q →0 ≡ Legend: SE Asia Oil Well 1/qo Function 1/qo Linear (Np/qo) Model 0.00150 Change in Reservoir Model (Increasing Damage) 0.00125 0.00100 (Np)max = Reserves = 313,000 STB 0.00075 -4 -6 1/qo = 2.676x10 + 3.1948x10 (Np/qo), 1/STB/D 0.00050 500 450 400 350 300 250 200 150 0 0.00000 100 0.00025 50 Reciprocal of Oil Rate, 1/qo,1/STB/Day 0.00200 0.00175 Oil Material Balance Time (Np/qo), Days Figure 9 — Example 3: Cartesian reciprocal rate plot — Southeast Asia — Oil Well. Good correlation of mid-time behavior (late-time data are affected by increasing damage). The final view of the data is provided by the log-log format reciprocal rate plot (Fig. 10). In this case we find an acceptable match of the late-time data, but clearly the early time data are not well represented by the reciprocal rate model (nor should these data be). The issue for this analysis is that the data for this case have been reviewed and analyzed repeatedly, and were found to be consistent (with the noted exception of the late time damage signature). The issue could be a slight mis-match in the pressure and rate — but again, rigorous, model-based analysis suggests that these data are valid. Reciprocal Rate Method SE Asia Oil Well — Log-Log Reciprocal Rate Plot -1 10 Reciprocal of Oil Rate, 1/qo,1/STB/Day -4 -6 1/qo = 2.676x10 + 3.1948x10 (Np/qo), 1/STB/D (Np)max = Reserves = 313,000 STB -2 10 -3 10 Legend: SE Asia Oil Well 1/qo Function 1/qo Linear (Np/qo) Model 0 1 10 2 10 3 10 4 10 We have provided field demonstrations of this methodology for the following cases: ● Well NRU 3106 (Texas, USA) — The Reciprocal Rate Method has significant value as an example — a black oil system being re-pressured by waterflooding. This is a very common scenario, and we expect this case to become a typical application for this method. ● Well WWL B41 (Louisiana, USA) — An extraordinary correlation trend for the 1/q — Np/q data is observed in this case. The performance of the 1/q — Np/q data confirms the validity of the Reciprocal Rate Method where external reservoir drive energy is present. ● Southeast Asia (Oil Well) — The "early-time" and "late-time" data are not aligned, which we believe prevents the overall success of the Reciprocal Rate Method for this case The issues in this case are not clear but we suspect that the rate and pressure data are affected by an evolving formation damage at late times. Conclusions: 1. The Reciprocal Rate Method is a basic yet theoretical approach for estimating reserves using only rate-time data (time, rate, and cumulative production). The reciprocal rate method is based on variable-rate theory, and is more rigorous than the Arps approach. 2. The Reciprocal Rate Method is assumes a constant flowing bottomhole pressure — but we have shown that the method should tolerate arbitrary changes in pwf — particularly smooth changes. 3. In this work we have validated the applicability of the method using field examples — but we have limited our application to black oil systems for simplicity and clarity. Further development is required for cases of compressible fluids (see Appendices B and C for efforts related to gas wells). 4. The method appears to be particularly robust for cases where external reservoir drive energy is present. Nomenclature -5 10 1 (reserves)................................................... (5) m Recommendations/Comment: Reciprocal Rate Method should be extended/generalized for cases where the flowing fluid is compressible. -4 10 10 SPE 107981 5 10 Oil Material Balance Time (Np/qo), Days Figure 10 — Example 3: Log-log reciprocal rate plot — Southeast Asia — Oil Well. Fair performance of the reciprocal rate concept model (weak transient/ transition behavior). Summary and Conclusions Summary: We provide the systematic development of the Reciprocal Rate Method, which has as a base the following relation: ⎡ Np ⎤ 1 =c+m⎢ ⎥ ................................................................. (3) q ⎣⎢ q ⎦⎥ The slope of the "reciprocal rate" plot yields an estimate of the A = bpss = Bo = Boi = cA = ct = Di = EUR = q = qi = h = k = mmb = N = Np = (Np)q→0= Reservoir drainage area, ft2 Intercept term in Eq. A-1, psi/STB/D Oil formation volume factor, RB/STB Initial oil formation volume factor, RB/STB Reservoir shape factor, dimensionless Total compressibility, psi-1 Coefficient in Eq. A-14, 1/D Estimated ultimate recovery, STB Production rate, STB/D Initial production rate, STB/D Net pay thickness, ft Average reservoir permeability, md Slope term in Eq. A-1, psi/STB Original oil-in-place, STB Cumulative oil production, STB Maximum oil production, STB SPE 107981 p pi pwf rw s t t μo γ = = = = = = = = = Estimation of Reserves Using the Reciprocal Rate Method Average reservoir pressure, psia Initial reservoir pressure, psia Bottomhole flowing pressure, psia Wellbore radius, ft Skin factor, dimensionless Time, days Material balance time (Np/q), days oil viscosity, cp Euler's constant (0.577216 …) References Arps J.J.: "Analysis of Decline Curves," Trans. AIME (1945) 160, 228-247. Blasingame, T.A. and Lee, W.J.: "Variable-Rate Reservoir Limits Testing," paper SPE 15028 presented at the SPE Permian Basin Oil and Gas Recovery Conference, Midland, TX, 13-14 March 1986. Blasingame, T.A. and Rushing, J.A.: "A Production-Based Method for Direct Estimation of Gas-in-Place and Reserves," paper SPE 98042 presented at the 2005 SPE Eastern Regional Meeting held in Morgantown, W.V., 14–16 September 2005. Doublet, L.E., Pande, P.K., McCollum, T.J., and Blasingame, T.A.: "Decline Curve Analysis Using Type Curves — Analysis of Oil Well Production Data Using Material Balance Time: Application to Field Cases," paper SPE 28688 presented at the 1994 Petroleum Conference and Exhibition of Mexico held in Veracruz, MEXICO, 10-13 October 1994. Fetkovich, M.J.: "Decline Curve Analysis Using Type Curves," JPT (March 1980) 1065-1077. Pratikno, H., Rushing, J.A., and Blasingame, T.A.: "Decline Curve Analysis Using Type Curves — Fractured Wells," paper SPE 84287 presented at the SPE annual Technical Conference and Exhibition, Denver, Colorado, 5-8 October 2003. Appendix A: Derivation of the Reciprocal-Rate Method for Estimating Reserves — Oil Case The purpose of this derivation is to provide the rigorous basis for the Reciprocal-Rate Method using a fundamental material balance and the pseudosteady-state flow relation. Starting with the oil material balance relation, we have: Black Oil Material Balance Relation: (p > pb) p = pi − mmb Np ............................................................ (A-1) Where mmb is defined as: mmb = 1 Bo .............................................................. (A-2) Nct Boi We next utilize the pseudosteady-state flow relation (also for a black oil). This relation is given as: Black Oil Pseudosteady-State Flow Relation: (p > pb) p = pwf + bpss q ............................................................. (A-3) Where bpss is defined as: μ B ⎡ 1 ⎡ 4 1 A ⎤ ⎤⎥ ⎥ + s ......................... (A-4) bpss = 141.2 o o ⎢ ln ⎢ kh ⎢ 2 ⎢ eγ CA rw2 ⎥ ⎥ ⎣ ⎦ ⎦ ⎣ Combining Eqs. A-1 and A-3, and solving for (pi-pwf), we obtain the following identity: ( pi − pwf ) = m mb Np + b pss q ......................................... (A-5) 5 Rearranging Eq. A-5 yields the "material balance time" formulation, which is given as: ⎡ Np Δp = b pss + m mb ⎢ q ⎢⎣ q ⎤ ⎥ .................................................. (A-6) ⎥⎦ Where Δp=(pi-pwf). Eq. A-6 is the basis of modern production data analysis — and is known as the "material balance time" formulation. Material balance time is defined as: ⎡ Np ⎤ t =⎢ ⎥ ....................................................................... (A-7) ⎣⎢ q ⎦⎥ A plot of Δp/q versus Np/q yields a straight-line trend where the slope of the line (mmb) is inversely proportional to the inplace fluid volume of the reservoir system. This is an older approach for the analysis of production data [Blasingame and Lee (1986)], but we note that more recent implementations of this approach use the Δp/q and Np/q plotting functions (and auxiliary functions) as diagnostic functions on log-log plots [Doublet et al (1994)]. Returning to Eq. A-7, we would like to assume a constant bottomhole flowing pressure (pwf), which yields a constant pressure drop Δpcon. Dividing through Eq. A-7 by Δpcon yields the following result: ⎡ Np 1 ˆ = b pss + mˆ mb ⎢ q ⎢⎣ q ⎤ ⎥ .................................................... (A-8) ⎥⎦ Where: b pss bˆ pss = ................................................................. (A-9) Δpcon mˆ mb = m mb ............................................................... (A-10) Δpcon As noted, we have assumed a constant pressure drop (Δpcon) to develop Eq. A-8 — however; this result provides the basis for the reciprocal rate method, that can be used to estimate the reserves (NOT in-place fluid volume for a given reservoir system). Multiplying through Eq. A-8 by the flowrate term (q), we have: 1 = bˆ pss q + mˆ mb Np ...................................................... (A-11) As the flowrate decreases to zero (i.e., q → 0), Eq. A-11 reduces to the following identity: ( Np ) q →0 ≡ 1 ........................................................ (A-12) mˆ mb Where the maximum cumulative production (Np)q→0 is typically referred to as the Estimated Ultimate Recovery (EUR) or the reserves of the system (NOT the in-place fluids — but rather, the quantity of fluids that will be produced at infinite producing time, at the current producing condition. Therefore a plot of 1/q versus Np/q yields a straight-line trend where the slope of the line (mˆ mb ) is inversely proportional to the EUR or reserves of the reservoir system. Again we note that a constant bottomhole pressure was assumed, but we will demonstrate that the "reciprocal rate method" is robust and useful method for estimating reserves. As an alternative derivation of this method, one can use the "exponential decline result" derived using the assumption of a constant flowing bottomhole pressure (see Blasingame and 6 P.D. Reese, D. Ilk, and T.A. Blasingame Rushing [Blasingame and Rushing (2005)] for generic detail regarding the derivation of the exponential decline result). Without derivation, the "exponential decline result" is given as: q = qi e − Dit ................................................................... (A-13) Where the following coefficients are given without derivation: m Di = mb .................................................................... (A-14) bpss qi = 1 ( pi − pwf ) ..................................................... (A-15) bpss Integration of Eq. A-13 with respect to time yields: Np = 1 (qi − q) ........................................................... (A-16) Di Solving Eq. A-16 for the flowrate, q, yields: q = qi − Di Np ............................................................... (A-17) Dividing through Eq. A-17 by the flowrate, q, gives us: q 1 = i − Di q ⎡ Np ⎢ ⎢⎣ q ⎤ ⎥ .......................................................... (A-18) ⎥⎦ Dividing through Eq. A-18 by the initial flowrate, qi, we have: 1 1 Di ⎡ Np ⎤ = − ⎢ ⎥ ....................................................... (A-19) qi q qi ⎣⎢ q ⎦⎥ Solving Eq. A-19 for the reciprocal flowrate (1/q) yields: 1 1 Di ⎡ Np ⎤ = + ⎢ ⎥ ........................................................ (A-20) q qi qi ⎣ q ⎦ Recalling our "rigorous result" (Eq. A-8) for comparison: ⎡ Np ⎤ 1 ˆ = b pss + mˆ mb ⎢ ⎥ ..................................................... (A-8) q ⎢⎣ q ⎦⎥ Substituting Eqs. A-9 and A-10 into Eq. A-8, we obtain: b pss 1 m = + mb q Δpcon Δpcon ⎡ Np ⎢ ⎢⎣ q ⎤ ⎥ ............................................. (A-21) ⎥⎦ Rearranging Eq. A-15 yields: bpss bpss 1 = = ............................................. (A-22) qi ( pi − pwf ) Δpcon Combining and solving Eqs. A-14 and A-15 for the quantity (mmb/Δpcon) yields: bpss Di mmb = qi bpss ( pi − pwf ) mmb = ( pi − pwf ) = mmb Δpcon ..................................................................................... (A-23) Substitution of Eqs. A-22 and A-23 into Eq. A-21 gives us: 1 1 Di ⎡ Np = + ⎢ q qi qi ⎢⎣ q ⎤ ⎥ ....................................................... (A-24) ⎥⎦ Where Eqs. A-20 and A-24 are identical — which confirms the "reciprocal rate formulation" from separate (albeit theoreti- SPE 107981 cally tied) results. As a final comment, the Di/qi term is the reciprocal of reserves — that is: Di 1 = ........................................................... (A-25) qi ( Np ) q → 0 Or, in proper form, we have: q ( Np ) q →0 = i ........................................................... (A-26) Di Substituting Eq. A-26 into Eq. A-24 gives us: 1 1 1 = + q qi ( Np ) q → 0 ⎡ Np ⎢ ⎢⎣ q ⎤ ⎥ ........................................... (A-27) ⎥⎦ As was noted earlier in this derivation (i.e., Eq. A-12), as q → 0 we obtain the maximum cumulative production at a particular flow conditions (i.e., (Np)q→0) — where (Np)q→0, is by defini-tion, the reserves. Appendix B: Derivation of the Reciprocal-Rate Method for Estimating Reserves — Gas Case In this Appendix we attempt to rationalize the use of the reciprocal rate concept for the case of a single well in a dry gas reservoir. We begin by recalling the result used by Blasingame and Rushing [Blasingame and Rushing (2005)] for rate-cumulative production (where the well is produced at a constant bottomhole flowing pressure). This result is given as: q g = q gi − Di Gp + 1 Di Gp 2 ........................................... (B-1) 2 G Dividing through Eq. B-1 by the gas flowrate, qg, we have: ⎤ ⎡ ⎡ Gp ⎤ 1 D i q ⎢ Gp ⎥ 1= − Di ⎢ ⎥+ g qg ⎢⎣ q g ⎥⎦ ⎢⎣ q g ⎥⎦ 2 G q gi 2 ............................. (B-2) Dividing through Eq. B-2 by the initial gas flowrate, qgi, yields the following result: D 1 1 = − i q gi q g q gi 2 ⎤ ⎡ ⎡ Gp ⎤ 1 1 D i q ⎢ Gp ⎥ .................. (B-3) ⎥+ ⎢ g ⎢⎣ q g ⎥⎦ ⎢⎣ q g ⎥⎦ 2 G q gi Solving Eq. B-3 for the reciprocal gas flowrate, 1/qg, gives: D 1 1 = + i q g q gi q gi 2 ⎤ ⎡ ⎡ Gp ⎤ 1 1 D i q ⎢ Gp ⎥ .................. (B-4) ⎥− ⎢ g ⎢⎣ q g ⎥⎦ ⎢⎣ q g ⎥⎦ 2 G q gi Recalling the "oil" result, Eq. A-24, we have: 1 1 Di ⎡ Np ⎤ = + ⎢ ⎥ ....................................................... (A-24) q qi qi ⎣⎢ q ⎦⎥ Comparing Eqs. B-4 and A-24, it does not appear that we can obtain a simple extrapolation form for the gas case. We can modify the "reciprocal rate" formulation by moving the reciprocal initial gas flowrate, 1/qgi, to the left-hand-side of Eq. B-4, we obtain: 2 ⎡ Gp ⎤ 1 1 D Gp 1 1 Di − = i − qg ⎢ ⎥ ....................... (B-5) q g q gi q gi q g 2 G q gi ⎢⎣ q g ⎥⎦ Estimation of Reserves Using the Reciprocal Rate Method Appendix C: Estimation of Reservoirs for the Case of a Gas Well Production Data Analysis Plot for East Texas Gas Well "Summary" History Plot — Rate and Pressure Functions Gas Flowrate, qg, MSCF/D 10 5 12000 Legend: East Texas Gas Well qg Production Data pw Production Data (measured surface/converted bottomhole) 10 10000 4 8000 6000 10 3 4000 2000 0 2200 2100 2000 1900 1800 1700 1600 1500 1400 1300 1200 1100 900 1000 800 700 600 500 400 300 200 0 2 100 10 (Computed) Flowing Bottomhole Pressure, pwf, psia In this Appendix we provide the analysis of the gas well case first evaluated by Pratikno et al. [Pratikno et al. (2002)]. In this analysis we consider the behavior of the "East Texas Gas Well" from initial production (July 2001) to present (April 2007) (see Fig. C.1, below). This work is in contrast to previous analyses which only considered the first year of production, but we believe that addressing the entire production history will be more relevant than just the first year — particularly because our present goal is to estimate reserves, not reservoir properties. Production Time, Day Fig. C.1 — Production and pressure history for the "East Texas Gas Well" (Texas, USA). 7000 6500 6000 5500 4500 4000 3500 3000 2500 2000 1500 1000 500 5000 0.0040 0.0035 0.0030 0.0030 0.0025 0.0025 0.0020 0.0020 0.0015 (1/G) = 1/(2.2x10 ) 0.0010 0.0010 6 0.0005 0.0000 7000 6500 6000 5500 5000 4000 3500 3000 2500 4500 G = 2.2x10 MSCF = 2.2 BSCF 0.0005 0.0000 0.0015 6 Approximate Material Balance Time (Gp/qg), Days Fig. C.2 — Cartesian format "Reciprocal Rate" plot for the "East Texas Gas Well" (Texas, USA). To confirm the Cartesian format match, we also present the reciprocal rate plot in log-log format (i.e., log(1/qg) versus log(Gp/qg)) (see Fig. C.3). Although our model match favors the late-time data (this view is exaggerated in the log-log format), we are satisfied that our trend provides a representative estimate of the gas reserves for this case. Production Data Analysis Plot for East Texas Gas Well Reciprocal Rate Plot — Log-Log Format Reciprocal Gas Flowrate (1/qg), 1/MSCFD After somewhat exhaustive efforts with Eq. B-8, it was concluded that this result cannot be formulated as an extrapolation technique to estimate reserves directly. For application of Eq. B-8, the reader is referred to the work by Blasingame and Rushing [Blasingame and Rushing (2005)]. 0.0045 0.0035 1 q gi ⎤ ⎡ Gp ⎤ (1− b) ⎡ q g = q gi ⎢1 − ⎥ ⎢G ≡ ⎥ ........................ (B-8) G ⎦⎥ (1 − b) Di ⎦⎥ ⎣⎢ ⎣⎢ 0.0050 1/qg ≈ intercept + (1/G) Gp/qg 0.0040 2000 The extrapolation of Eq. B-7 for qg→0 will yield a factor of 2 times the reserves (note the 2G term in Eq. B-7). Another formulation which was considered is that of the socalled "hyperbolic" rate decline relation [Arps (1942), Fetkovich (1980)], given in rate-cumulative production form by Blasingame and Rushing [Blasingame and Rushing (2005)]. This result is given as: 0.0045 1500 qg ⎤ 1 D 1 1 Di = i − Gp .................................. (B-7) ⎥ q gi ⎥⎦ Gp q gi 2 G q gi 0.0050 1000 ⎡ ⎢1 − ⎢⎣ Production Data Analysis Plot for East Texas Gas Well Reciprocal Rate Plot — Log-Log Format 0 Eq. B-6 is simply a modified form of the Blasingame and Rushing extrapolation formula. We will provide a demonstration of this relation for a gas reservoir case in as part of the example application given in Appendix C. We will use a slight simplification of Eq. B-6 for our demonstration example in Appendix C — this result is: 0 ⎡ 1 1 ⎤ qg D 1 1 Di = i − − Gp ............................... (B-6) ⎢ ⎥ q q G q gi ⎦⎥ p gi 2 G q gi ⎣⎢ g 7 As with the other cases evaluated in this work, we will use the Cartesian format "reciprocal rate" plot (1/qg versus Gp/qg — and this graph is shown in Fig. C.2. While the model match shown in Fig. C.2 favors the latest production data, this is appropriate as we wish to estimate the reserves at this particular point in time (i.e., the present is the latest time in the well history). 500 Then multiplying through Eq. B-5 by the (qg/Gp) function gives us: Reciprocal Gas Flowrate (1/qg), 1/MSCFD SPE 107981 10 10 10 10 10 -1 -1 10 0 10 1 10 2 10 3 10 4 10 5 10 1/qg ≈ intercept + (1/G) Gp/qg -2 10 -3 10 6 (1/G) = 1/(2.2x10 ) -4 10 -1 -2 -3 -4 6 G = 2.2x10 MSCF = 2.2 BSCF 10 -5 10 -1 0 1 2 3 4 10 10 10 10 10 Approximate Material Balance Time (Gp/qg), Days 10 10 -5 5 Fig. C.3 — "Reciprocal Rate" plot (log-log format ) for the "East Texas Gas Well" (Texas, USA). In Fig. C.4 we present the "Gas Reciprocal Rate" plot, which is derived from Eq. B-7. This plot is simply a variation of the result given by Blasingame and Rushing [Blasingame and Rushing (2005)] for the case of a gas well producing at a constant flowing bottomhole pressure. We also noted that the x-axis intercept is (from Eq. B-7) a factor of 2 times the gas reserves (G). In this case (i.e., Fig. C.4), our results confirm the estimate of 2.2 BSCF for the reserves estimate. While we had hoped to develop a "reciprocal rate" analog for the gas case from Eq. B-4, it simply is not possible to develop 8 P.D. Reese, D. Ilk, and T.A. Blasingame a (direct) reserves extrapolation formula from Eq. B-4. This remains a topic for further investigation. Production Data Analysis Plot for East Texas Gas Well Reciprocal Rate Function Versus Cumulative Gas Production Plot 0.9 qgi = 1650 MSCFD ⎡ qg ⎤ 1 D 1 1 Di = i − Gp ⎥ ⎢1 − ⎣⎢ q gi ⎥⎦ Gp q gi 2 G q gi 0.8 0.7 0.6 0.5 0.4 Intercept: 2G = 4.4 BSCF G = 2.2 BSCF 0.3 0.2 5.00 4.75 4.50 4.25 4.00 3.75 3.50 3.25 3.00 2.75 2.50 2.25 2.00 1.75 1.50 1.25 1.00 0.75 0.00 0.0 0.50 0.1 0.25 Rate-Cumulative Production Function: [1-(qg/qgi)](1/Gp), 1/BSCF 1.0 Cumulative Gas Production, Gp, BSCF Fig. C.4 — "Gas Reciprocal Rate" plot for the "East Texas Gas Well" (Texas, USA). SPE 107981
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