uAbstract

uFigures

uEquations

uTables

uIntroduction

uInflatable Dual Packer

uFocused Sampling

uExample 1 – Focused Probe Sampling

uExample 2 – Dual Packer Sampling

uConclusions

uReferences

uAbstract

uFigures

uEquations

uTables

uIntroduction

uInflatable Dual Packer

uFocused Sampling

uExample 1 – Focused Probe Sampling

uExample 2 – Dual Packer Sampling

uConclusions

uReferences

uAbstract

uFigures

uEquations

uTables

uIntroduction

uInflatable Dual Packer

uFocused Sampling

uExample 1 – Focused Probe Sampling

uExample 2 – Dual Packer Sampling

uConclusions

uReferences

uAbstract

uFigures

uEquations

uTables

uIntroduction

uInflatable Dual Packer

uFocused Sampling

uExample 1 – Focused Probe Sampling

uExample 2 – Dual Packer Sampling

uConclusions

uReferences

uAbstract

uFigures

uEquations

uTables

uIntroduction

uInflatable Dual Packer

uFocused Sampling

uExample 1 – Focused Probe Sampling

uExample 2 – Dual Packer Sampling

uConclusions

uReferences

uAbstract

uFigures

uEquations

uTables

uIntroduction

uInflatable Dual Packer

uFocused Sampling

uExample 1 – Focused Probe Sampling

uExample 2 – Dual Packer Sampling

uConclusions

uReferences

uAbstract

uFigures

uEquations

uTables

uIntroduction

uInflatable Dual Packer

uFocused Sampling

uExample 1 – Focused Probe Sampling

uExample 2 – Dual Packer Sampling

uConclusions

uReferences

uAbstract

uFigures

uEquations

uTables

uIntroduction

uInflatable Dual Packer

uFocused Sampling

uExample 1 – Focused Probe Sampling

uExample 2 – Dual Packer Sampling

uConclusions

uReferences

Equations

Equation 1. Variables affecting drawdown.  Q is flow rate, μ is viscosity,   k is formation permeability and Cpf is the probe geometry factor

Tables

Introduction

The Pinda was deposited in a shallow marine environment and is rich in carbonates and is frequently highly dolomitized. In such complex reservoirs the acquisition of quality formation tester samples is crucial to the reservoir evaluation. In this paper we wish to discuss results from previous attempts in the same area, the subsequent recommendations that were made and their implementation. This discussion is informed by the fact that these are low permeability rocks drilled with oil base mud, containing oils that are very close to saturation pressure. 

The interplay between formation characteristics and tool operation is described by the implementation of Darcy’s law (Moran and Finklea, 1962; Schlumberger, 2006) as seen in Equation 1.

As can be seen the drawdown at the sand face is a function of the mobility (k/μ), the flow rate and the probe size.  Therefore in order to minimize the drawdown and stay above the bubble point it is required to either reduce the flow rate or increase the probe size. However neither of these options is without consequence. When the flow rate is reduced we will reduce the drawdown but the resulting very low flow rates imply it will take much longer to clean up the oil base mud filtrate. Similarly, a larger probe size permits a larger flow rate for a given drawdown but also allows for less sealing area for the packer as the flowing area is increased.  The sealing success rate must be balanced against the requirements for drawdown and flow rate.

The question is then posed: how to design a sampling program that accounts for the bubble point and contamination conditions?  Looking at Equation 1 we see that four variables affect the drawdown.  The formation permeability, k, and the fluid viscosity, μ, are out of our control. We are left to manipulate the geometry of rp (probe radius) by how we interface with the formation, and flow rate, Q by our pump design. Table 1 is a summary of available probes and their geometry

Inflatable Dual Packer

The inflatable dual packer uses two inflatable rubber elements to isolate and communicate with the reservoir.  The spacing between the packer elements is adjustable however the nominal spacing is about 1.0 metre.  Whereas the probes discussed earlier have a flow area that ranges anywhere from 0.15 to about 2 square inches, the dual packer, when inflated in an 8.5 inch borehole will isolate a flow area of about 960 square inches. This obviously leads to a huge reduction in drawdown for a given flowrate and mobility.  We can model the performance of the probes and packers.  The results of this modeling are presented in Table 2 and assume a formation mobility of 50 mD/cp.

As can be seen the inflatable dual packer presents considerable advantage in terms of reduced drawdown, increased flow rate or both.  However, the advantages of the dual packer do not come without consideration.  The dual packer is typically longer on station.  Inflate and deflate times are longer than the set and retract sequences for a single probe.  Additionally, when considering clean-up time, it is now necessary to clean up a cylinder that is 1.0 metre in height as opposed to the cone of fluid associated with a probe type of tool.  This can take quite a bit longer.  Finally, extended on-station times and larger tool diameter often dictate the inflatable dual packer is run drill pipe conveyed instead of on wireline which greatly increases the costs associated with rig time.

Focused Sampling

As the above discussion shows, in lower permeability reservoirs where there is a drawdown constraint due to saturation pressure, we will either be forced to use a dual packer with its attendant considerations or, if we elect to use a probe, forced to pump at very low flow rates.  The low flow rates, however, present a problem for sampling oil in a well drilled with oil base mud: clean-up time will be very long.  We can mitigate this by using a focused probe sampling tool (Weinheber and Vasques, 2006; Dong et al, 2005; Akurt et al, 2006).  Focused sampling has been available for several years now and we describe the basics of operation here.

Consider in Figure 1 a conventional (non-focused) probe. We show in this figure a packer set against the borehole wall (left hand side).  We assume that the near wellbore fluid, in yellow-green, is invaded filtrate and that the far field virgin fluid, in blue, is the desired formation fluid.  After the tool is set and the pretest is complete the pump is started to begin the evacuation of fluid from the formation and into the wellbore.  In the case of a conventional sampling probe the flow regime that exists is similar to the one depicted in the right side of Figure 1. Essentially a cone of clean reservoir fluid is set up surrounded by a shell of filtrate. A number of observations can be made about this fluid flow regime.  Firstly, some amount of pure reservoir fluid can be seen quickly, often within one or two strokes of the pump. However additional clean-up can take considerable time and pumped volumes (Hammond, 1991). Secondly, it is practicably impossible to achieve zero percent contamination. There will always be some amount of filtrate flowing around the outside of the cone. The lowest level of contamination that can be achieved is related to the ratio of vertical to horizontal permeability and to the viscosity contrast between the filtrate and the formation fluid. Extensive sampling experience with probe-type formation testers has shown that near-zero contamination results are only possible in the rare case of sampling very thin beds in high-mobility environments. A real time contamination prediction algorithm based on the optical densities of the sampled fluids has been in widespread use for several years and has proven to be an effective gauge of fluid quality (Smits et al, 1995; Mullins et al, 2000).

Now consider the schematic of the focused sampling probe shown in Figure 2.  Note that there have been two significant changes to the focused probe versus the conventional probe.  Firstly, the probe has been separated into two distinct flow areas. There is a perimeter ring around the outside which we shall call the guard ring or guard side.  In the center there is a flow area which we shall call the sample probe or the sample side. Secondly, there are now two separate flowlines into the tool body.  The tool is equipped with a bypass valve that connects or isolates the guard side from the sample side. When this valve is open or connecting we refer to the flow as “commingled”. When the valve is closed or isolating we refer to the flow as “split”. Additionally, the tool carries two pressure gauges: a quartz gauge on the sample side and a strain gauge on the guard side. When the bypass is open we expect these gauges to be reading the same. When the bypass is closed the difference between strain and quartz is the pressure drop across the inner packer. Now consider the flow regime set up by the focused probe during pumping. Note that the same conical flow regime is assumed.  In this case the filtrate contamination is going to be captured by the outer flow ring and “guarded” away. The clean reservoir fluid is going to be isolated by the center sample probe and will be captured exclusive of the filtrate. Experience has shown that the best results are achieved when drawdown on the guard side (the strain gauge) is higher than the drawdown on the sample side (the quartz gauge). This pressure profile assures that filtrate is guarded away from the sample probe.

Example 1 – Focused Probe Sampling

We look first at the focused sampling station in Figure 3. Note at the beginning that hydrostatic pressure is ~x600 psi.  Two 10 cc pretests are executed and formation pressure is x340 psi. Note that on the first pretest mobility was calculated at 13 mD/cp and on the second pretest mobility was 21 mD/cp. During the pretest and during the initial pumping sequences the inner bypass valve is open, connecting guard with sample. The sample and guard side pressure are hence reading the same. At 1000 s the lower pumpout on the guard side is activated. 

At point ‘B’ at about 2900 s the lower pumpout module is stopped and the upper pumpout is started. The flow rate achieved is a very low 1.1 cc/s and the resultant drawdown is only 80 psi. Note that the inner bypass is still open so guard and sample are still reading the same pressure. This 80 psi translates to a flowing mobility of about 21 mD/cp. At about 7400 s the inner bypass is closed and both pumps are activated. This is the “split flow” mode. Initially the guard side pump is started at 2.3 cc/s and the sample side pump is started at 1 cc/s. Note immediately that the pressure on the sample side starts to fall as drawdown increases. It is interpreted that this is likely due to an increase in sample side viscosity as the lower viscosity filtrate is directed to the guard side and the higher viscosity reservoir oil heads towards the sample side. Eventually the pressure on the sample side falls lower than on the guard side (sample side drawdown is higher). As described earlier this is an undesirable situation. Best results are obtained when the drawdown on the guard exceeds the drawdown on the sample so as to encourage the separation of filtrate from reservoir oil. Therefore at about 9400 s the engineer begins stepped increases in the guard side pump speed in order to increase the guard drawdown. By ~7500 s this is achieved and sampling can commence.

Example 2 – Dual Packer Sampling

Multiple attempts to acquire a water sample in the lower part of the reservoir with a probe only resulted in high drawdown low mobility pretests. It was therefore decided to inflate the dual packer. Figure 4 shows the sequence. At point ‘A’ we see the lower pump being used to inflate the packer. During all of time period ‘A’ we are in pump-in mode to inflate the packers. At point ‘B’ we switch to pump-out mode and begin the drawdown from the formation. After initially running the lower pump at ~450 rpm the pump is slowed to 300 rpm and the flowing pressure stabilizes. The stable Δp is about 700 psi below formation pressure and the flow rate is about 1.8 cc/s.  This corresponds to a mobility of about 0.2 mD/cp. At point ‘C’ the lower pump is turned off and the upper pump is started.  Recall that the upper pump is configured with an extra High Pressure displacement unit (the same as the lower pump) but with a fixed displacement hydraulic pump set at about 0.3 cc/rev. As a result even a relatively high pump speed of 650 rpm results in only a 1.5 cc/s flow rate and slightly less Δp. The points marked with ‘X’ indicate where the sample bottles are filled.  All of the samples obtained were less than 5% OBM filtrate (by volume).

Conclusions

Sampling near saturated oils from low permeability reservoirs in a well drilled with oil base mud can provide a significant challenge for a wireline formation tester. The conflicting requirements of drawdown and rate will pull tool string design in opposite directions. On the one hand we need to minimize flowrate to control the drawdown. On the other we need maximum flow rate to clean-up OBM contamination in a cost efficient manner. In this paper we have shown how to balance this. We implement the industry-unique focused probe toolstring and combine it with hardware options that result in the lowest practical WFT flow rates. Instead of just pumping large volumes to effect OBM clean-up we pump intelligently and focus the flow. So even though flow rates are less than 2 cc/s, the resultant samples are of a quality to perform accurate PVT characterization.

Of course it is acknowledged that there is a lower limit to permeabilities that may be sampled with the probe type tools. To that end an inflatable dual packer is also included in the tool string and successfully deployed to acquire a water sample and confirm the location of the transition zone. For further information see Contreiras et al, 2008.

References

Akurt R., et al; 2006, Focusing on Downhole Fluid Sampling and Analysis, Schlumberger Oilfield Review: Winter 2006, p. 4-19.

Beaiji, T, M. Zeybek, R. Crowell, R. Akkurt, S. Al-Dossari, A. Amin, and S. Crary; 2007, Advanced Formation Testing in OBM Using Focused Fluid Sampling for Producibility Evaluation in Mature Fields: SPE 110511 presented at the 2007 ATCE, Anaheim, California, USA, 11-14 November 2007.

Dong, C., C. Del Campo, R. Vasques, P. Hegeman, and N. Matsumoto, 2005, Formation Testing Innovations for Fluid Sampling: Seventeenth Annual Deep Offshore Technology Conference, Vitoria, Brazil, 8–10 November 2005.

Hammond, P.S., 1991, One- and Two-Phase Flow During Fluid Sampling by a Wireline Tool Transport in Porous Media: in Transport in Porous Media, Springer-Verlag, v. 6, p. 299-330.

Contreiras, K.K., F. Van-Dúnem, P. Weinheber, A. Gisolf, and M. Rueda; 2008, Improved Techniques for Acquiring Pressure and Fluid Data in a Challenging Offshore Carbonate Environment: SPE 115504, SPE ATCE in Denver, CO., 21-24 September, 2008.

Moran, J.H., and E.E. Finklea, 1962, Theoretical Analysis of Pressure Phenomena Associated with the Wireline Formation Tester: SPE Journal of Petroleum Technology, August 1962; SPE 00177.

O'Keefe, M., K.O. Eriksen, S. Williams, D. Stensland, and R. Vasques; 2006, Focused Sampling of Reservoir Fluids Achieves Undetectable Levels of Contamination: SPE paper 101084, SPE APOGC, Adelaide, Australia, 11–13 September 2006.

Schlumberger Educational Services Fundamentals of Formation Testing 2006.

Weinheber, P.J. and R. Vasques, 2006, New Formation Tester Probe Design for Low-Contamination Sampling: Paper RR presented SPWLA Annual Symposium, Veracruz, Mexico, June 4-7, 2006.

Weinheber, P.J., A. Gisolf, R.J. Jackson, and I. De Santo, 2008, Optimizing Hardware Options for Maximum Flexibility and Improved Success in Wireline Formation Testing, Sampling and Downhole Fluid Analysis Operations: SPE 19713 presented SPE 2008 NAICE, Abuja, Nigeria, 4-6 August 2008.

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