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Water and gas coning

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Coning is a production problem in which gas cap gas or bottomwater infiltrates the perforation zone in the near-wellbore area and reduces oil production. Gas coning is distinctly different from, and should not be confused with, free-gas production caused by a naturally expanding gas cap. Likewise, water coning should not be confused with water production caused by a rising water/oil contact (WOC) from water influx. Coning is a rate-sensitive phenomenon generally associated with high producing rates. Strictly a near-wellbore phenomenon, it only develops once the pressure forces drawing fluids toward the wellbore overcome the natural buoyancy forces that segregate gas and water from oil.

Basis of terminology

The term coning is used because, in a vertical well, the shape of the interface when a well is producing the second fluid resembles an upright or inverted cone (Fig. 1). Important examples of coning include:

  • Production of water in an oil well with bottomwater drive
  • Production of gas in an oil well overlain by a gas cap
  • Production of bottom water in a gas well

In a horizontal well, the cone becomes more of a crest (Fig. 2), but the phenomenon is still customarily called coning. In a given reservoir, the amount of undesired second fluid a horizontal well produces is usually less than for a vertical well under comparable conditions. This is a major motivation for drilling horizontal wells, for example, in thin oil columns underlain by water.

Impact of coning

Coning is a problem because the second phase must be handled at the surface in addition to the desired hydrocarbon phase, and the production rate of the hydrocarbon flow is usually dramatically reduced after the cone breaks through into the producing well. Produced water must also be disposed of. Gas produced from coning in an oil well may have a market, but also may not. In any event, production of gas in an oil well after the cone breaks through can rapidly deplete reservoir pressure and, for that reason, may force shut in of the oil well.

Several strategies may apply to wells with a potential to cone. One is to try to predict the rate at which a well will cone and produce at a lower rate as long as possible. Or, optimal economics may result by producing at a much higher rate, causing the well to cone, but increasing the cumulative hydrocarbon volume produced (and present value) at any future date. A horizontal well may be preferred to a vertical well.

Predicting coning

Most prediction methods for coning predict a "critical rate" at which a stable cone can exist from the fluid contact to the nearest perforations. The theory is that, at rates below the critical rate, the cone will not reach the perforations and the well will produce the desired single phase. At rates equal to or greater than the critical rate, the second fluid will eventually be produced and will increase in amount with time. However, these theories based on critical rates do not predict when breakthrough will occur nor do they predict water/oil ratio or gas/oil ratio (GOR) after breakthrough. Other theories predict these time behaviors, but their accuracy is limited because of simplifying assumptions.

The calculated critical rate is valid only for a certain fixed distance between the fluid contact and the perforations. With time, that distance usually decreases (for example, bottom water will usually tend to rise toward the perforations). Thus, the critical rate will tend to decrease with time, and the economics of a well with a tendency to cone will continue to deteriorate with time.

Whether a cone will move toward perforations depends on the relative significance of viscous and gravitational forces near a well. The pressure drawdown at the perforations tends to cause the undesired fluid to move toward the perforations. Gravitational forces tend to cause the undesired fluid to stay away from the perforations. Coning occurs when viscous forces dominate.

The variables that could affect coning are:

  • Density differences between water and oil, gas and oil, or gas and water (gravitational forces)
  • Fluid viscosities and relative permeabilities
  • Vertical and horizontal permeabilities
  • Distances from contacts to perforations.

Coning tendency turns out to be quite dependent on some of these variables and insensitive to others.

A number of prediction methods have been published. There is no guarantee of great accuracy when using any of these methods because they all contain significant simplifying assumptions. In particular, areal and vertical variations in vertical permeability (because of flow barriers of varying extent) can cause the prediction methods to differ significantly from what actually happens in the field. Accordingly, the prediction methods are best used for quick approximations, screening, and comparison of alternatives. Reservoir simulations, based on accurate reservoir characterization, will ultimately be required.

The coning prediction method proposed by Chaperon[1] is of particular interest because of the variables it includes and because variations of the method are applicable to gas and water coning in both vertical and horizontal wells. For vertical wells, the Chaperon method calculates the critical rate for coning from the expression

RTENOTITLE....................(1) Chaperon paper uses "h", not "hc"





and hc = distance from perforations to fluid contact, ft. For horizontal wells, the critical rate is given by






Example: Determining the critical production rate for both horizontal and vertical well alternatives

Consider a square, 160-acre drilling unit in an oil reservoir overlain by a gas cap. To determine the critical production rate (at or above which coning is likely to occur) for both horizontal and vertical well alternatives, assume the following well and formation properties: kh = 80 md, aH = 2,640 ft, μo = 0.5 md, ρo = 0.8 g/cm3, ρg = 0.3 g/cm3 (~.0008 g/cm^3?? - a gas density cannot be .3 g/cm^3), Lw = 1,500 ft, h = 90 ft, Bo = 1.2 RB/STB, rw = 0.33 ft, distance from top of perforations in vertical well to GOC = 80 ft, and distance from horizontal well to GOC = 80 ft. Consider two cases: Isotropic Reservoir A, where kv = kh = 80 md, and Anisotropic Reservoir B, where kv = 8 md and kh = 80 md.

Solutions. Isotropic Reservoir A (kv = kh = 80 md). For a horizontal well,







For a vertical well, note that RTENOTITLE = 1,489 ft.






Anisotropic Reservoir B (kv = 8 md and kh = 80 md). For a horizontal well,


For a vertical well,


Conclusions from example

The important conclusions and lessons from this example are:

  • Vertical permeability has only a modest influence on critical coning rate, at least for this situation.
  • The advantage of a horizontal well over a vertical well is substantial for both isotropic and anisotropic reservoirs in this situation.
  • The same sorts of calculations could be made for an oil well coning water or a gas well coning water.
  • These calculations give us no information on time at which the cone will break through to the producing well nor on GOR and oil production rate following breakthrough.

While these types of simple calculations can provide some insight on the potential for coning, a finely grided simulator model could be used to more effectively predict coning behavior including timing and the benefits of a horizontal well over a vertical one.

Coning strategies

Under ideal conditions in which no coning exists, flow is principally horizontal and mainly oil is produced. Fig. 3 illustrates a producing well with no coning. When coning exists, however, the overlying gas is drawn downward or bottomwater is drawn upward and into the oil column. Coning trades oil production for gas or water production. Fig. 4 illustrates a producing well subject to gas and water coning.

Two strategies commonly are used to minimize coning. One approach is partial perforation or penetration. In this approach, only a limited portion of the pay thickness is perforated. If gas coning is anticipated, the pay thickness near the GOC is not perforated. If water coning is anticipated, the pay thickness near the WOC is not perforated. In instances in which severe coning is expected, only a small portion of the pay thickness may be perforated. The variables in Fig. 5 define the length of the perforation interval, b, and its position within the pay thickness, h. The distance Lg is the distance between the top of the pay and the uppermost perforation, and the distance Lw is the distance between the bottom of the pay and the lowest perforation. The quotient b/h is the partial perforation fraction. Although this strategy will reduce and can eliminate coning problems, it suffers an obvious drawback; namely, it temporarily reduces oil production in the hope of eventually avoiding coning.

A second remedial strategy is based on the observation that there is a critical producing rate below which the cone stabilizes and will not reach the perforations. This critical rate is a function of the perforation length. As the perforation length increases, the critical producing rate decreases. Often, the critical producing rate is much less than the possible producing rate. This difference creates an operational decision:

  • Produce at a rate greater than the critical and eventually risk coning
  • Produce at a rate less than the critical and temporarily sacrifice oil production

If the critical rate is less than the minimum economic rate, then the operator has no choice but to produce above the critical rate or abandon the well.

To combat coning, a hybrid strategy is often used whereby a combination of partial perforation and a reduced producing rate is used. One especially unattractive consequence of gas coning is that it prematurely depletes the gas-cap gas and diminishes the gas-cap producing mechanism. Fortunately, gas coning is not as problematic as water coning because the density difference between oil and gas is greater than the difference between water and oil. This density difference through gravity segregation helps mitigate coning.

To develop an effective remedial strategy against coning, certain theoretical aspects regarding coning must be understood. Mathematically, coning is a challenging problem because of its complexity. To develop tractable analytical solutions, tenuous assumptions must be invoked. These assumptions limit the practical applicability of these solutions. The most reliable way to study coning is with a specially designed finite-difference simulator. [2][3][4] Nevertheless, certain analytical solutions and empirical correlations can be helpful and serve as a preliminary guide.

Muskat and Wyckoff [5] and Chaney et al.[6] were among the first to contribute substantively to this problem. Since their efforts, several other authors have contributed to the body of literature. [7][8][9][10][11][12][13][14] Many of these works have led to similar correlations. Wheatley[13] presented a comparison of some popular correlations. As a representative sample, the correlations of Schols[12] and Chierici et al.[7] are presented here. Both works apply to both water and gas coning. Both efforts also use the following equation to compute the critical producing rate:



  • Δρ = density difference (g/cm3)
  • Bo = average oil formation volume factor (FVF)
  • μo = average oil viscosity (cp)
  • ko = oil permeability (md)
  • qDc = dimensionless critical producing rate
  • h = pay thickness (ft)
  • qc is given in STB/D

The oil permeability, ko, is the product of the horizontal permeability and the oil relative permeability. The dimensionless critical rate, qDc, is specified by correlation.

Schols’ correlation

Schols’ correlation[12] is based on a numerical simulation study. The dimensionless critical producing rate is



  • b is the length of the perforation interval
  • re is the drainage radius.

This correlation applies to both water and gas coning; however, it directly applies only to cases in which water or gas coning exist separately. In other words, it does not directly apply to cases in which water and gas coning act simultaneously. The correlation can be used to predict the critical rate for a pre-existing completion or to predict the optimum perforation length for a future completion. In this latter application, the optimum perforation length is defined as the length at which the critical and theoretical producing rates are equal. The theoretical producing rate of a partially penetrating well is computed in this section. Example 1 illustrates the former application while Example 2 illustrates the latter application.

Chierici et al. correlation

The correlation by Chierici et al.[7] was based on a potentiometric study. This was one of the most sophisticated correlations. It allows the vertical permeability to differ from the horizontal permeability. This can be an important factor because coning vanishes as the vertical permeability approaches zero. This correlation also treats the problem of simultaneous gas/water coning. This is important in situations in which a gas cap and bottomwater coexist.

The correlation of Chierici et al. was specified in terms of a series of charts. The charts used the following nomenclature. The dimensionless critical rate is denoted as ψ (previously defined as qDc) and the following dimensionless variables are defined as




and RTENOTITLE....................(13) (original paper uses "h" not "b")

The dimensionless critical rate, ψ, is a function of rDe, ε, and δ. Figs. 6 through 12 show the charts. Each chart corresponds to a different value of rDe. Specific charts exist for rDe = 5, 10, 20, 30, 40, 60, and 80.

The chats are used differently depending on whether they are used to compute the critical rates or optimize the perforation length. The problem of optimizing the perforation length for simultaneous gas and water coning is more complicated than separate water or gas coning. The charts simplify the problem; however, the solution procedure depends on the application.

Calculating critical rates

For a pre-existing perforation length, b, the critical rates are computed with the following procedure:

  1. Compute δg, δw, ε, and rDe with Eqs. 10 through 13.
  2. Locate the correct chart or charts, depending on the value of rDe. Interpolation between two charts may be required.
  3. Compute ψg from the charts based on rDe, ε, and δg; then, compute ψw from the charts based on rDe, ε, and δw.
  4. Compute the critical rates to avoid water and gas coning with Eq. 8.

This procedure ignores the curves labeled Δρogρwo. The calculation procedure is simplified if only bottomwater or a gas cap exists. If no bottomwater exists, then the calculation of ψw and δw can be ignored. Conversely, if no gas cap exists, then the calculation of ψg and δg can be ignored. Example 1 illustrates an application.

Calculating optimum perforation length

For a bottomwater, gas-cap reservoir, the procedure to calculate the optimum perforation (length and position) uses the curves labeled Δρogρwo and is as follows:

  1. Compute rDe with Eq. 13. Also, compute Δρogρwo.
  2. Assume a value of ε.
  3. Compute ψ and δ with the charts. These values correspond to ψg and δg.
  4. Compute Lg = g and Lw = h(1 – ε) – Lg.
  5. Compute the critical rate from Eq. 8. Only one critical rate is needed because the procedure assumes equal critical rates for gas and water coning.
  6. Return to Step 2. Assume a new value of ε, and repeat the calculation until an adequate range of ε is covered.
  7. Compute the theoretical producing rate of a partially penetrating well as a function of ε with Eq. 14. (See partially penetrating wells below).
  8. Plot the critical and theoretical producing rates as a function of ε . The value of ε at which the critical and producing rates intersect yields the optimal perforation interval.

This procedure is simplified if only a gas cap or bottomwater exists. The same procedure applies except Δρogρwo is not calculated and δg = 1 – ε (if there is no bottomwater and only gas coning is a problem) or δw = 1 – ε (if there is no gas cap and only water coning is a problem). ψ is computed for a range of ε until an optimal value of ε is identified. Example 2 illustrates this procedure for a gas cap reservoir. Example 3 illustrates an application for a gas cap, bottomwater reservoir.

Partially penetrating wells

The theoretical producing rate of a partially penetrating well is needed to compute the optimum perforation length. Partially penetrating wells are wells that do not fully penetrate or are not fully perforated throughout the pay thickness. If vertical permeability exists, these wells will produce fluids from above and below the perforations. Fig. 13 illustrates fluid delivery into a partially penetrating producing well. Under these circumstances, fluid flow is obviously not strictly horizontal. The producing rate in partially penetrating wells with nonzero vertical permeability is greater than the rate with no vertical permeability.

Partially penetrating wells commonly are used to minimize coning. The critical rate gives a producing rate below which no coning will occur. Often, however, the critical flow rate is much less than maximum possible flow rate. To judge the difference, estimates for the flow rate of a partially penetrating well are needed. Several authors have offered analytical expressions to estimate the flow rate. [15][16][17] Most efforts yield estimates within a few percent of one another. The Kozeny expression, [17] for example, is



  • kH = horizontal permeability
  • kv = vertical permeability
  • pe = pressure at drainage radius
  • pw = wellbore pressure
  • s = skin factor, q = oil producing rate, and the argument of the cosine assumes radians

This equation assumes units of md, ft, psi, cp, and STB/D. This equation also assumes steady-state flow in a circular drainage area, where re and rw are the drainage and wellbore radii, respectively. Eq. 14 gives the Kozeny equation in SI units.

Variables affecting coning

The ratio of qc/q is a measure of the tendency not to cone. As q c increases or q decreases, the likeliness to avoid increases. According to Eqs. 8 and 14, the ratio qc/q is proportional to


This expression shows that the likeliness to control coning increases as the penetration interval b decreases. Eq. 15 also shows that the likeliness to control coning increases as the pay thickness increases, density difference increases, well spacing increases, and perforation length decreases. Horizontal permeability does not affect the likelihood of success. This expression also suggests that controlling coning in a thin reservoir may be difficult.

Additional measures to control coning

Other techniques have been applied to control coning. These include:

  • Placing an artificial barrier above or below the pay to suppress vertical flow[18]
  • Injecting oil to control gas coning[19]
  • Use of horizontal wells

Barriers composed of cement and high-molecular-weight polymers have been tried. Another, although expensive, technique is to drill additional wells and produce them at the critical rate.

Example 1: Computing critical rate to prevent coning

Compute the critical rate (STB/D) for a well in a gas-cap reservoir with the following characteristics:

  • kH = 60 md
  • kv = 39 md
  • h = 150 ft
  • re = 933 ft (80-acre well spacing)
  • rw = 0.5 ft
  • Bo = 1.25 RB/STB
  • μo = 1.11 cp
  • ρo = 0.714 g/cm3
  • ρg = 0.098 g/cm3

The well is completed in only the lower 60 ft of the pay thickness.

Schols’ correlation

With Eq. 9, compute qDc. This yields


The critical rate is then computed with Eq. 8, which yields


Chierici et al. correlation

First, evaluate:

  • Lg = 90 ft
  • δg = 90/150 = 0.60
  • ε = 60/150 = 0.40
  • rDe = 5.01.

With the chart for rDe = 5, obtain ψ = 0.120. Evaluating Eq. 8 yields


Example 2: Computing optimum perforation length to prevent coning

For an uncompleted well in the gas-cap reservoir in Example 1, compute the optimum perforation length at a reservoir pressure of 1,800 psia. Assume a wellbore pressure of 1,500 psia and a skin factor of 10.

Schols’ correlation

Compute the dimensionless critical rate and critical rate as a function of b/h. Table 1 summarizes the results for b/h = 0 to 1.

Next, estimate the theoretical producing rate for a partially penetrating well. With Eq. 15 for b = 60 ft yields


Table 1 summarizes the results at other values of b. The rate varies from 0 to 808 STB/D, depending on the length of the perforation interval. The optimum perforation length corresponds to the value of b at which the critical and theoretical producing rates are equal. Fig. 14 shows a plot of q and qc vs. b/h. The curves intersect at approximately b/h = 0.15. This corresponds to:

  • b = 22.5 ft
  • Lg = 127.5 ft
  • q = 187 STB/D

In conclusion, only the lower 22.5 ft of the pay thickness should be perforated to avoid gas coning.

Chierici et al. correlation

First, compute δg = 1– b/h for a range of b/h. Next, compute rDe. From Example 1, rDe = 5. With the appropriate chart, compute ψ for the range of b/h. The charts use b/h as ε. Then compute the critical rate with Eq. 8. Table 2 summarizes the results. Fig. 14 plots qc vs. b/h.

The optimal perforation length corresponds to the value of b/h at which the critical and producing rates are equal. This approximately occurs for b/h = 0.25. This corresponds to:

  • b = 37.5 ft
  • Lg = 112.5 ft
  • q = 275 STB/D

In conclusion, only the lower 37.5 ft of the pay should be perforated. The method of Chierici et al. yields a wider perforation interval than the method of Schols (37.5 vs. 22.5 ft). The Chierici et al. method is consistently more liberal than Schols’ method.

Example 3: Optimum perforation length to prevent coning in a bottom water gas cap reservoir

Assume the gas cap reservoir in Examples 1 and 2 is underlain by water. The water density is 1.092 g/cm3. Compute the optimum perforation length and position of the perforation interval with the Chierici et al. correlation.

Solution. First, compute Δρogρwo. This yields (0.741 – 0.098)/(1.092 – 0.741) = 1.83. Next, determine δg and ψ from the charts for a range of ε. If ε = 0.40, for example, use the chart corresponding to rDe = 5 to determine that δg = 0.24 and ψ = 0.040. Table 3 summarizes the results for a range of ε values from 0.05 to 0.40. Next, compute the critical rate for each value of ψ with Eq. 8. Finally, compute the theoretical producing rate with Eq. 15.

An examination of Table 3 shows that the critical and producing rates are equal at ε = b/h = 0.075. This value of b/h corresponds to Lg = (0.385) (150) = 57.8 ft, b = (0.075) (150) = 11.3 ft, and Lw = 150 – 57.8 – 11.3 = 81 ft. In conclusion, the well should be perforated with an 11.3-ft interval located 57.8 ft below the GOC and 81 ft above the WOC.


aH = total width of reservoir perpendicular to the wellbore, ft
Bo = oil formation volume factor, RB/Mscf
h = net formation thickness, ft
kh = horizontal permeability, md
Lw = completed length of horizontal well, ft
re = external drainage radius, ft
ρ = density, lbm/ft3 or g/cm3
μo = oil viscosity, cp
μw = water viscosity, cp


  1. Chaperon, I. 1986. Theoretical Study of Coning Toward Horizontal and Vertical Wells in Anisotropic Formations: Subcritical and Critical Rates. Presented at the SPE Annual Technical Conference and Exhibition, New Orleans, 5–8 October. SPE-15377-MS.
  2. Fetkovich, M.J., Reese, D.E., and Whitson, C.H. 1998. Application of a General Material Balance for High-Pressure Gas Reservoirs (includes associated paper 51360). SPE J. 3 (1): 3-13. SPE-22921-PA.
  3. Letkeman, J.P. and Ridings, R.L. 1970. A Numerical Coning Model. SPE J. 10 (4): 418-424. SPE-2812-PA.
  4. MacDonald, R.C. 1970. Methods for Numerical Simulation of Water and Gas Coning. SPE J. 10 (4): 425-436. SPE-2796-PA.
  5. Muskat, M. and Wyckoff, R.D. 1935. An Approximate Theory of Water-Coning in Oil Production. Trans., AIME 114: 144.
  6. Chaney, P.E. et al. 1956. How to Perforate Your Well to Prevent Oil and Gas Coning. Oil & Gas J. (7 May): 108.
  7. 7.00 7.01 7.02 7.03 7.04 7.05 7.06 7.07 7.08 7.09 7.10 Chierici, G.L., Ciucci, G.M., and Pizzi, G. 1964. A Systematic Study of Gas and Water Coning By Potentiometric Models. J Pet Technol 16 (8): 923–929. SPE-871-PA.
  8. Bournazel, C. and Jeanson, B. 1971. Fast Water-Coning Evaluation Method. Presented at the Fall Meeting of the Society of Petroleum Engineers of AIME, New Orleans, 3-6 October. SPE 3628.
  9. Høyland, L.A., Papatzacos, P., and Skaeveland, S.M. 1989. Critical Rate for Water Coning: Correlation and Analytical Solution. SPE Res Eng 4 (4): 495–502. SPE-15855-PA.
  10. Kuo, M.C.T. 1983. A Simplified Method for Water Coning Predictions. Presented at the SPE Annual Technical Conference and Exhibition, San Francisco, California, 5–8 October. SPE-12067-MS.
  11. Meyer, H.I. and Garder, A.O. 1954. Mechanics of Two Immiscible Fluids in Porous Media. J. of Applied Physics 25 (11): 1400.
  12. 12.0 12.1 12.2 Schols, R.S. 1972. An Empirical Formula for the Critical Oil Rate. Erdöl Erdgas, Zeitschrift (January): 6–11. Cite error: Invalid <ref> tag; name "r12" defined multiple times with different content Cite error: Invalid <ref> tag; name "r12" defined multiple times with different content
  13. 13.0 13.1 Sobocinski, D.P. and Cornelius, A.J. 1965. A Correlation for Predicting Water Coning Time. J Pet Technol 17 (5): 594-600. SPE-894-PA.
  14. Wheatley, M.J. 1985. An Approximate Theory of Oil/Water Coning. Presented at the SPE Annual Technical Conference and Exhibition, Las Vegas, Nevada, USA, 22-26 September. SPE 14210.
  15. Muskat, M. 1949. Physical Principles of Oil Production. New York City: McGraw-Hill Book Co. Inc.
  16. 16.0 16.1 Saidikowski, R.M. 1979. Numerical Simulations of the Combined Effects of Wellbore Damage and Partial Penetration. Presented at the SPE Annual Technical Conference and Exhibition, Las Vegas, Nevada, 23–26 September. SPE-8204-MS.
  17. 17.0 17.1 Chierici, G.L., Ciucci, G.M., and Pizzi, G. 1964. A Systematic Study of Gas and Water Coning By Potentiometric Models. J Pet Technol 16 (8): 923–929. SPE-871-PA.
  18. Howard, G.C. and Fast, C.R. 1950. Squeeze Cementing Operations. Trans., AIME 189: 53.
  19. Richardson, J.G. and Blackwell, R.J. 1971. Use of Simple Mathematical Models for Predicting Reservoir Behavior. J Pet Technol 23 (9): 1145-1154. SPE-2928-PA.

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See also

Oil fluid characteristics

Oil fluid properties

Primary drive mechanisms

Fluid flow through permeable media