This patent generally relates to subterranean wellbores. More particularly, this patent relates to drilling mud and a method and apparatus for minimizing or eliminating the need for casing the wellbore.
Conventionally, when a wellbore is created, a number of casings are installed in the wellbore to prevent collapse of the wellbore wall and to prevent undesired outflow of drilling fluid into the formation or inflow of fluid from the formation into the wellbore. The wellbore is typically drilled in intervals whereby a casing (such as, steel pipe), which is to be installed in a lower wellbore interval, is lowered through a previously installed casing of an upper wellbore interval. As a consequence of this procedure, the casing of the lower interval is of smaller diameter than the casing of the upper interval. Therefore, the casings are in a nested arrangement with casing diameters decreasing in the downward direction. Cement annuli are typically provided between the outer surfaces of the casings and the wellbore wall to seal the casings from the wellbore wall and prevent flow from lower intervals from going between the wellbore wall and back side of the casings.
In most wells, the most critical role of the casing/cementing system is to increase the minimum fracture gradient to enable continued drilling. Generally, when drilling a well, the pore pressure gradient (PPG) and the fracture pressure gradient (FG) increase with the true vertical depth (TVD) of the well. Typically for each drilling interval, a mud density (mud weight or MW) is used that is greater than the pore pressure gradient, but less than the fracture pressure gradient.
As the well is deepened, the mud weight is increased to maintain a safe margin above the pore pressure gradient. If the mud weight were to fall below the pore pressure gradient, the well may take a kick. A kick is an influx of formation fluid into the wellbore. Kicks can result in dangerous situations and extra well costs to regain control of the well. If the mud weight is increased too much, the mud weight will exceed the fracture pressure gradient at the top of the drilling interval (usually this is the location with the smallest fracture pressure gradient). This normally leads to lost returns. Typically, lost returns occur when the drilling fluid flows into a fracture (or other opening) in the formation. Lost returns results in large volumes of mud loss, which is costly in terms of fluid replacement and operational time to treat and replace lost returns. Lost returns also lower the bottom hole pressure of the wellbore, which can lead to a kick. Additionally, lost returns results in the cuttings not being removed from the wellbore. The cuttings may then accumulate around the drill string causing the drill string to become stuck. A stuck drill pipe is a difficult and costly problem that often results in abandoning the interval or the entire well.
To prevent the above situation from occurring, conventional practice typically involves running and cementing a steel casing string in the well. The casing and cement serve to block the pathway for the mud pressure to be applied to the earth above the depth of the casing shoe. This allows the mud weight to be increased so that the next drilling interval can be drilled. This process is generally repeated using decreasing bit and casing sizes until the well reaches the planned depth. The process of tripping, running casing, and cementing may account for as much as 25 to 65 percent of the time required for drilling a well. Tripping is the process of pulling the drill pipe or running the drill pipe into the well. Because well costs are primarily driven by the required rig time to construct the well, these processes may increase the cost of drilling the well. Furthermore, with the conventional steel casing tapered-hole-drilling process, the final hole size that is achieved may not be useable or optimal and the casing and cement operations substantially increase well costs.
As a consequence of this nested arrangement, relatively large wellbore diameters are required in the upper part of the wellbore. Such large wellbore diameters involve increased costs due to the time to drill the holes, the time to install all of the casings, costs of casing, and drilling fluid consumption. Moreover, increased drilling rig time and costs are involved due to required tripping drill pipe out, cement pumping, cement hardening, required equipment changes due to variations in hole diameters drilled in the course of the well, tripping drill pipe in, and the large volume of cuttings drilled and removed.
For exploration wells, the reduction in hole size with increasing depth may result in not reaching the planned target depth or not reaching the planned target depth with enough hole size to run logging tools to fully evaluate the formation. Typically, at least a 0.1524 meter (6-inch) open hole is needed to fully evaluate the formation. For some wells, the need to set casing to accommodate pore pressure/fracture gradient concerns results in running out of hole size. For development wells, the telescopic nature of the well reduces the final hole size in the reservoir. This reduction in the contact size of the well with the reservoir may reduce the production rate of the well, thereby, reducing the well's performance. Generally, a larger hole size in the reservoir increases the well's production rate for a given drawdown. Drawdown is the difference between the fluid pressure in the reservoir and inside the well.
Current technologies used to address the problems discussed above, especially in deepwater wells, include the use of a dual (or multiple) gradient drilling system. For example, U.S. Pat. No. 4,099,583 discloses a dual gradient drilling system. In this method, a lighter fluid is injected into the mud return annulus (typically in the riser) or other pathway to reduce the mud density from the injection point upwards. This helps tailor the mud pressure gradient profile to closer match the desired pressure gradient profile that is between the pore pressure gradient and fracture gradient profiles. Multiple gradient drilling systems may reduce the required number of casing strings by possibly one or two. However, these systems are mechanically complex, are very costly to implement, create operational concerns (for example, for well control), and still result in a tapered wellbore.
U.S. Pat. No. 6,530,437 and U.S. Pat. No. 6,588,501 disclose a multi-gradient drilling method and an apparatus for reduction of hydrostatic pressure in sub sea risers. For example, in Mauer et al., rigid hollow spheres are injected into the flowing mud at discrete locations in the riser and in the borehole below the mud line. This permits stepwise reduction in the effective mud density above the point of injection. Furthermore, this approach can in principle be used to stepwise change the mud density in the return annulus in such a way as to keep the mud weight between the pore pressure gradient and the fracture gradient.
To accomplish this, multiple injection points at different vertical positions within the annulus would be needed. The vertical position of these injection points would also need to be adjusted to accommodate unanticipated deviations in the pore pressure and fracture gradients. This stepwise reduction in mud density can at best only reduce the number of intermediate casing strings required by the number of injection points added. These systems, like conventional multi-gradient systems, are mechanically complex, are very costly to implement and create operational concerns (for example, for well control).
A series of U.S. patents assigned to Actisystems of Edmond OK disclose the addition of various fluid aphrons to drilling mud formulations. See, for example, U.S. Pat. No. 6,422,326, U.S. Pat. No. 6,156,708, U.S. Pat. Nos. 5,910,467 and 5,881,826. The fluid aphrons reduce the density of the mud and reduce the lost circulation potential of the mud. Liquid aphrons are oil in water emulsions with a high oil/water volume ratio and are 5-20 microns in size. A small volume of this emulsion is dispersed into the drilling mud to form colloidal liquid aphrons (CLA). In this way a very large interfacial area is created without large power input. Colloidal gas aphrons (CGA) are microbubbles 10-100 microns in diameter coated with multiple layers of surfactant and created by shearing the liquid above some critical shear rate. The use of gas aphrons does not provide the desired object compression that reduces the number of required intermediate casing strings.
Another technology used to address some of problems discussed above is the use of solid expandable liners (SELs). An example of a solid expandable liner is disclosed in U.S. Pat. No. 6,497,289. Solid expandable liners are special tubular systems that are run into a well and expanded. The expansion allows the open hole to be lined using a string that has a larger interior diameter than would otherwise be available with a conventional liner. The solid expandable liner system allows a larger bit and/or additional casing strings to be run in the well. In development wells, this can facilitate penetrating the reservoir with a larger wellbore size. For exploration wells, having one or two additional liners may enable the well to reach a planned target with a useable wellbore size. While some aspects of a solid expandable liner may be beneficial, it has several drawbacks. These include time and cost, connections, hole quality requirements, tapering, and cementing. However, a solid expandable liner cannot reduce the number of required casing strings.
Accordingly, there is a need for improved drilling mud to minimize or eliminate the need to install casings or linings inside a wellbore that addresses the above-mentioned drawbacks of current casing techniques. This invention satisfies that need.
One embodiment of the invention is a variable density drilling mud. The drilling mud comprises compressible particulate material in the drilling mud wherein the density of the drilling mud changes in response to pressure changes.
A second embodiment is also disclosed. This embodiment is a method for varying drilling mud density. The method comprises estimating the pore pressure and fracture gradient, and choosing a drilling mud with compressible material wherein the effective mud weight of the drilling mud remains between the pore pressure and the fracture gradient in at least one interval of a wellbore.
A third embodiment is also disclosed. This embodiment is an apparatus for drilling a wellbore. The apparatus comprises a drill string with a bottom hole assembly and a drill bit on the bottom hole assembly, and means to pump variable density mud into the wellbore to maintain the mud pressure in the wellbore between the pore pressure gradient and the fracture gradient. In one embodiment, the means to pump the variable density drilling mud is a mud pump that pumps the mud down the drill string through the drill bit and back up the annulus between the drillstring and the wellbore.
In the following detailed description and example, the invention will be described in connection with its preferred embodiments. However, to the extent that the following description is specific to a particular embodiment or a particular use of the invention, this is intended to be illustrative only. Accordingly, the invention is not limited to the specific embodiments described below, but rather, the invention includes all alternatives, modifications, and equivalents falling within the true scope of the appended claims.
We have discovered that we can tailor the drilling mud density with depth so that the effective mud weight remains between the pore pressure and the fracture gradient at all depths. We have further discovered that the required variation in mud density can be achieved with the addition of particulate component whose density is substantially different from that of the remaining fluid and whose volume (and therefore density) changes in response to pressure. The particulate components may include various shapes, such as spheres, cubes, pyramids, oblate or prolate spheroids, cylinders, pillows and/or other shapes or structures. Further, the particulate components may be compressible hollow objects, which are filled with pressurized gas, or even compressible solid materials or objects, as described further below.
One embodiment is a method for varying the density of drilling mud in a wellbore at a chosen location. As shown in
In one embodiment, the variable density drilling mud comprises particulate materials such as, compressible (or collapsible) hollow objects. More preferably, the compressible hollow objects would have a relatively small diameter and be gas pressurized, (for example, spheres, oblate or prolate spheroids, cylinders, pillows or any other suitable shape). The material would be chosen to achieve a favorable compression in response to pressure changes. Examples of suitable materials include but are not limited to polymer, polymer composites, metals, metal alloys, and/or polymer or polymer composite laminates with metals or metal alloys.
Preferably, only one drilling mud design would be necessary. In this scenario the particulate material would be tailored to provide a drilling mud density change at depth that would permit one drilling mud design to maintain a drilling mud pressure between the pore pressure gradient and fracture gradient throughout the wellbore. If the drilling mud design cannot maintain a mud pressure between the pore pressure gradient and fracture pressure gradient, additional casing may be added as necessary. Preferably, the particulate material in the variable density drilling mud is chosen to have a favorable density change at depth wherein the drilling mud pressure is maintained between the pore pressure gradient and the fracture pressure gradient with the least number of casings
The initial internal pressure of the hollow object may be selected based on the depth at which a transition in the compressibility is desired. At depths in the mud column for which the pressure is below the initial internal pressure, the mechanical properties of the shell material, such as Young's Modulus, and the differential pressure across the shell control the volume change of the objects. At depths for which the pressure in the mud column is above the initial internal pressure, the volume change of the hollow objects gradually becomes dominated by the compressibility of the gas if the differential pressure across the wall exceeds the collapse pressure of the hollow objects.
The compression of these hollow objects results in a different gradient of mud density above and below the depth defined by the initial internal pressure of the hollow objects. Mixing objects of different initial internal pressure and changing the volume fraction and distribution of initial pressures as the depth of the well increases can achieve the desired result of maintaining the mud pressure between the required bounds.
The hollow objects may be partially filled with a liquid, mixtures of condensable and non-condensable gases, or any combination thereof. Addition of a condensable gas or liquids allows additional flexibility in tailoring the variation of mud density with depth. For instance, at the temperature and pressure of the gas/liquid phase boundary the condensable gas liquefies with an increase in density and a corresponding decrease in volume. The decrease in internal volume of the object will result in a step increase in effective mud density at the depth and temperature corresponding to the phase transition. An additional potential benefit of using a gas mixture containing a condensable gas is the finite internal volume occupied by the condensed gas at depths greater than that at which it condenses. Because the compressibility of liquids is generally lower than that of the non-condensable gas, the liquid volume can be used to set an upper limit on the deformation experienced by the wall of the hollow object. This may assist in controlling the fatigue life of the flexible objects as they cycle between the bottom of the hole and the surface.
Confining the volume change to a large number of small diameter objects mixed into the remaining mud fluid allows tailoring of the initial size and shape of the objects, to achieve the desired rheology of the composite mud system. Both the gel point of the mud and the variation of the mud viscosity with shear rate are altered by the addition of a large volume fraction of the proposed compressible objects to the mud. The initial properties of the fluid phase are preferably chosen such that the resulting composite mud gel point is sufficient to suspend the rock cuttings in the annulus during normal operations, including non-circulating operations. Furthermore, the viscosity of the composite mud satisfies pumpability requirements without developing unacceptable dynamic pressure gradients in the annulus. This is facilitated by the fact that both the gel point alteration and the modification of the composite mud viscosity with shear rate exhibit similar functionality for compressible object volume fraction loading of up to 45 percent.
In the case of a spherical hollow shell, the tensile strength of the materials required is defined by the relationship:
T=(pr)/2 h. (1)
Wherein:
T is the tensile strength,
p is the internal pressure,
r is the radius of the sphere, and
h is the wall thickness of the spherical shell.
For a sphere of diameter 1.0 mm (millimeter) with an internal pressure of 13.8 Mpa (mega pascals) (2000 psig (pounds per square inch gauge)) and a wall thickness of 0.125 mm, the yield strength of the material required would be T=27.6 Mpa (40,000 psi). Many common materials have a yield strength that meets or exceeds the required level.
A greater potential issue is the effective lifetime of the pressurized spheres due to gas leakage through the wall. In the case of the crystalline polymer PEEK the gas permeation rate for oxygen for a differential pressure of 1 Bar is approximately 852.5 cm3/day m2(centimeter3/day/meter2) for a 100 micron thick wall at 25° C. (Celsius). The initial volume of gas in a 1-mm internal diameter sphere at 136 atmospheres is only 0.071 cm3 at standard temperatures and pressure (STP). The leak rate for such a sphere is then approximately 0.0152 cm3/hr (centimeter3/hour) and the sphere would lose approximately 2.95 Mpa (428 psi) of the initial 13.8 Mpa (2000 psi) charge in one hour and would have a useful lifetime of less than one hour. Therefore, it may be advantageous to reduce the gas permeation rate if a polymer shell is to be useful for the purpose of this invention.
We have devised several options to reduce the permeation rate and to create a material with a substantially low permeability. The spheres can be made larger with thicker walls than the current example. For example, at a given h/r ratio, the lifetime will increase as the square of the sphere radius. The spheres can be filled with gases with large molecular volumes, such as SF6 (sulfur hexa-flouride) that possess intrinsically low diffusion rates. SF6 has a diffusion constant approximately 100 smaller than CO2 (carbon-dioxide) in polymer membranes. The wall of a polymer sphere could be filled with particulate such as exfoliated clay particles to act as barriers to gas permeation.
Alternatively, the walls of the hollow objects may be made of metals, laminates of polymer and thin metal films, or any other material with sufficient tensile strength and suitably low gas permeability. In the case of metal films and metal/polymer laminates, literature data suggests that both the strength and permeability of many common metals and polymer/metal laminates are more than adequate to satisfy both the strength and permeability requirements for the proposed application.
In one embodiment, it is envisioned that the compressible solid objects are continuously re-circulated with the flowing mud. In this embodiment, the compressible objects may be passed directly through the mud pumps at the surface down the drill string, through the drill bit and back up the annulus between the drill string and the wellbore. If necessary, an additional separation step may be performed at the surface to separate the compressible objects from the cuttings and reconstitute the composite mud prior to re-injection. The large density difference between the compressible objects and the cuttings may greatly facilitate any separation that is required.
In an embodiment the re-injection of the objects would occur down stream of the mud pumps. Methods for continuously injecting rigid spheres into a flowing mud stream and for separation of rigid spheres from the mud have already been disclosed in the patent literature. See for example, U.S. Pat. Nos. 6,530,437 and 6,588,501.
Similarly, if it is undesirable to pass the compressible objects through the high shear jets at the drill bit, the compressible objects can be shunted around the bit. One method to accomplish this would be to use a downhole centrifugal separator just above the BHA (Bottom Hole Assembly) in the drill string with a side injection port just above the BHA to shunt the spheres into the return annulus bypassing the high shear zone at the cutting face.
Other anticipated and unanticipated benefits may result from the addition of flexible pressurized hollow objects to the mud composition. For example, addition of these objects may reduce friction between the rotating drill string and the wall. The relevant prior art includes for example, U.S. Pat. No. 4,123,367. In this patent, a method for reducing drag and torque on a rotary drill string by the addition of minute spherical solid glass beads to the mud is disclosed.
The addition of flexible pressurized hollow objects to the mud composition may also in part mitigate lost returns. In a lost returns situation, the partially compressed hollow objects re-circulating with the mud will enter the fault along with the mud flow. As they enter the formation fault, the objects are expected to expand as they move from the higher-pressure wellbore into the lower-pressure of the formation fault. We expect the objects will become lodged in the fault helping to seal the formation. The flexibility of the objects is also expected to assist in formation of a more effective seal. Relevant prior art includes for example, U.S. Pat. No. 4,836,940. This patent discloses the addition of a pelletized composition comprising a water insoluble, water absorbent polymer and bentonite. In this concept, the pellets enter the formation fault where they become trapped. The trapped pellets slowly absorb water swelling and sealing the formation.
An example of the application of this concept to hypothetical deep water well drilled to a final depth of 22,000 feet is illustrated below.
In the example illustrated in
The first drilling mud 24 composition allows the wellbore to be drilled from the surface casing 23 to the intermediate casing 21. The second drilling mud 25 composition allows the wellbore to be drilled to the target depth 29 without any additional casing. This planning diagram, without the variable density drilling mud would require 6 intermediate casings 31. Reducing the additional casings after the surface casing form 6 to 1 reduces well costs.
There are several benefits that may be associated with the application of the present techniques. First, the embodiments of the present techniques provide a method of changing the architecture of a well. That is, the present technique eliminates the plateau time associated with setting certain casing strings because the particulate material in the variable density drilling mud reduces the number of changes in the casing strings. Accordingly, the use of variable density drilling mud may allow drilling activities to reach reservoirs at greater depths by overcoming the limitations and restrictions imposed by conventional drilling operations, as noted above. Second, the embodiments of the present techniques reduce the costs associated with accessing reservoirs. In particular, the reduction in the size and cost of the drilling vessel and pumps required because the size of the wellbore may be substantially reduced. Further, the variable density drilling mud may reduce the material costs, such as drill bits, risers, casing, cement and mud. As such, the use of the variable density drilling mud with the particulate materials in a well may reduce the costs associated with accessing a reserve and provide justification to access certain reservoirs.
In another embodiment, the particulate materials, which include the compressible (i.e. collapsible or deformable) hollow particles, may be made of shape memory alloys (SMAs). As described in greater detail in
To begin, the shape memory alloys rely upon pressure (i.e. applied stress load to the shape memory alloy) and temperature to determine the phase of the shape memory alloy. These phases include an austenite phase and a martensite phase. As shown in
Because the temperatures influence the phase of the shape memory alloy, adjustments in the stress or pressure with respect to the temperature may define various phase regions for the shape memory alloy. That is, the phase of the shape memory alloy depends on the previous phase along with the pressure and temperature to determine the phase region. In these different regions, the shape memory alloy has different behavioral characteristics, such as superelasticity, which may also be referred to as pseudoelasticity. The superelastic characteristic is observed along an isothermal superelastic loading path 402 and a non-isothermal superelastic loading path 404. On the isothermal superelastic loading path 402, the temperature remains constant as the stress is increased (i.e. loaded) and decreased (i.e. unloaded). On the non-isothermal loading path 404, the temperature increases as the stress increases, which may be representative of loading the compressible hollow shape memory alloy particles inside a wellbore. That is, the non-isothermal loading path 404 represents the stress and temperature experienced by shape memory alloys as the depth in the wellbore increases.
Accordingly, these different phase regions of the shape memory alloys may be best understood with reference to the paths 402 and 404. With each of the paths 402 and 404, the shape memory alloy is in the austenite phase when the temperature and stress are below the martenstic start line 406. Between the martenstic start line 406 and the martenstic finish line 408, the shape memory alloy is in an austenitic-to-martenstic transformation region. Above the martenstic finish line 408, the shape memory alloy is in the martensite phase. As such, any additional loading of pressure or stress maintains the shape memory alloy in this region. Alternatively, as the loading is decreased, the shape memory alloy remains in the martensite phase as long as the shape memory alloy is above the austenitic start line 410. Between the austenitic start line 410 and the austenitic finish line 412, the shape memory alloy is in the martenstic-to-austenitic transformation region. Then, below the austenitic finish line 412, the shape memory alloy is in the austenite phase. The transformation of the shape memory alloy is further described in
During the loading process, the shape memory alloy behaves in an elastic manner, as shown in the austenite elastic line 502. When a first stress level or collapse threshold is reached, as shown by first point 504, the transformation stage begins. The first collapse threshold may be a point along the martenstic start line 406 of
During the unloading process, the shape memory alloy again behaves in an elastic manner that is consistent with the martensite phase, as shown in the martensite elastic line 508. When a second stress level or collapse threshold is reached, as shown by third point 510, the reverse transformation stage begins for the conversion from martensite-to-austenite phase. The transformation phase may again be entered by unloading the stress on the shape memory alloy, as shown by second transformation line 512. As the stress on the shape memory alloy is reduced, the shape memory alloy may reform into its previous structure. Then, the transformation to the austenite phase is complete at the fourth point 513. When the shape memory alloy has transformed into the austenite phase, as shown by the austenite elastic line 502, the shape memory alloy behaves in an elastic manner of the austenite phase. The transformation of the shape memory alloy is further described
To begin, an austenite shape memory alloy particle 602 may have the structure of a sphere, as one example. As the austenite shape memory alloy particle 602 is transported down within the wellbore, and the pressure external to the austenite shape memory alloy 602 increases, as shown by the line 604. Accordingly, as the pressure and stress exceed the stress or collapse threshold, such as the first point 504 of
Once the martensitic shape memory alloy particle 606 is directed to move up the wellbore, the martensitic shape memory alloy particle 606 may retain its shape until the martensitic shape memory alloy particle 606 reaches a point where the surrounding hydrostatic pressure and temperature is less than the collapse or stress threshold, such as the third point 510 of
To provide the target response, as shown in diagram 700 of
For example, a shape memory alloy may also be utilized to vary the density of the drilling mud. Beneficially, with a shape memory alloy, the structure of the shape memory alloy particle may be varied and recovered based on the hydrostatic pressure and temperature within the wellbore, as shown by shape memory alloy responses 710a and 710b. This flexibility in the structure reduces the dependence on pressurized gas inside the shape memory alloy particle and expansion is achieved based on the shape recovery of the shape memory alloy particle. As a result, the effective weight of the drilling mud is adjusted based on the temperature and the pressure within the wellbore.
Further, as shown in diagram 702 of
Beneficially, the use of these shape memory alloy particles may provide more resiliency than other types of materials. The shape memory alloy particles may be more resistant to damage than polymer particles because metals are generally stronger than polymers. As a result, the shape memory alloy particles may be separated from the drilling mud at the surface and reused in an efficient manner.
Furthermore, the shape memory alloys provide additional flexibility in varying the density of the drilling mud. For instance, the shape memory alloys may be designed for specific applications by adjusting the transformation temperatures of the alloy, shape of the particles, and/or wall thickness based upon the anticipated downhole pressures and temperatures. This flexibility provides additional mechanisms for changing the architecture of a well, as noted above. It should also be noted that the hollow particles may be deformable to adjust between an initial and a deformed shape, which may also increase the density of the drilling mud.
Moreover, in an alternative embodiment, the variable density drilling mud may include particulate materials that are compressible (or collapsible) solid materials or objects. These compressible solid objects may function similar to the compressible hollow objects and have similar shapes, such as spheres, oblate or prolate spheroids, cylinders, pillows or any other suitable shape, for example. Again, the material utilized in these solid objects may be selected to achieve a specific compression in response to pressure changes, as discussed above. Beneficially, these particulate materials may be utilized to reach greater depths because the architecture of the casing strings may change and may justify the access to other resources, as noted above.
While the present techniques of the invention may be susceptible to various modifications and alternative forms, the exemplary embodiments discussed above have been shown by way of example. However, it should again be understood that the invention is not intended to be limited to the particular embodiments disclosed herein. Indeed, the present techniques of the invention are to cover all modifications, equivalents, and alternatives falling within the spirit and scope of the invention as defined by the following appended claims.
This application claims priority to U.S. Application No. 60/580,523 filed Jun. 17, 2004.
Number | Date | Country | |
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60580523 | Jun 2004 | US |
Number | Date | Country | |
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Parent | PCT/US05/20320 | Jun 2005 | US |
Child | 11441698 | May 2006 | US |