Roller cone bits are used in earth drilling applications such as petroleum or mining operations. Roller cone bits include one or more roller cones rotatably mounted to a bit body. These roller cones have a plurality of cutting elements attached thereto that crush, gouge, and scrape rock at the bottom of a hole being drilled. The cutting structure of a roller cone bit includes two or three rotatable roller cones mounted on legs of a bit body. Two cone bits include two legs with journals and roller cones mounted thereon. The two cone bit often suffers from stability issues related to near bit vibrations. Thus, more stable three cone roller bits are often used in commercial applications due to the increased stability.
However, two cone drill bits do pose some advantages over three cone bits. Particularly, two cone drill bits have a higher rate of penetration than three cone bits. Two cone bits may also have larger bearings which results in a longer bearing life. Additionally, two cone drill bits may have better hydraulics than a three cone drill bit due to more room for nozzles allowing for faster cuttings evacuation.
In one aspect, embodiments of the present disclosure include a method including inputting drill bit characteristics into a simulator, wherein drill bit characteristics include a drill bit mass, coordinates of the drill bit center of gravity, or an inertia tensor of the drill bit, aligning the drill bit center of gravity and a vector of the inertia tensor with a bit axis in the simulator, where the bit axis runs longitudinally through the center of the drill bit, determining new drill bit characteristics based on the aligning the center of gravity and the inertia tensor with the bit axis, and producing a drill bit with the new bit characteristics.
In another aspect, embodiments of the present disclosure include a method including assembling a drill bit, inputting drill bit characteristics into a simulator, performing a mass balance with a simulator, determining new drill bit characteristics, modifying the drill bit by adding or removing mass according to the new mass distribution.
In another aspect, embodiments of the present disclosure include a drill bit including a body, two legs mounted to the body, two journals, one of the two journals mounted to each of the two legs, the two journals having a cone separation angle of less than 180 degrees, two roller cones, one of the two roller cones mounted to each of the two journals, where the drill bit has a center of gravity substantially aligned with a bit axis.
In yet another aspect, embodiments of the present disclosure include a method including producing a two cone roller cone drill bit having a cone separation angle of less than 180 degrees, where the producing comprises aligning a center of gravity of the two cone roller cone drill bit with a bit axis.
This summary is provided to introduce a selection of concepts that are further described below in the detailed description. This summary is not intended to identify key or essential features of the claimed subject matter, nor is it intended to be used as an aid in limiting the scope of the claimed subject matter.
In the following detailed description of embodiments, numerous specific details are set forth in order to provide a more thorough understanding. However, it will be apparent to one of ordinary skill in the art that the disclosed subject matter of the application may be practiced without these specific details. In other instances, well-known features have not been described in detail to avoid unnecessarily complicating the description.
Generally, embodiments disclosed herein relate to roller cone drill bits and methods manufacturing roller cone drill bits. In one aspect, embodiments disclosed herein relate to methods of increasing the stability of roller cone drill bits through mass-balancing of the drill bit. In another aspect, embodiments disclosed herein relate to methods of increasing the stability of two cone drill bits.
Referring initially to
Referring to
Turning to
In the embodiment shown in
Once the legs 12 have been machined and assembled with roller cones 16, the legs may be welded or otherwise coupled to a wedge section 10. Referring to
As shown in
Referring back to
As shown in
As mentioned, several of the features present on a drill bit may be used to incorporate additional weight into the drill bit, at different axial and/or radial positions. Incorporation of such features may allow for drill bit balancing to occur. As used herein, the phrase “drill bit balancing” or “balancing operations” may include aligning at least one of a center of gravity of the drill bit or the inertia tensor of the drill bit with the bit axis. In some embodiments, drill bit balancing operations may include aligning both the center of gravity and the inertia tensor with the bit axis.
The inertia tensor describes an amount of torque (τ) to impart rotational an acceleration (dω) to an object. Referring to equation (1), provided below, the inertia tensor (I) may be represented by a 3-by-3 matrix. The inertial value I for an object is proportional to the amount of torque required to produce a specific rotational acceleration. The x-axis, y-axis, and z-axis with respect to a drill bit may be seen in
For an ideal symmetric and balanced object, torque applied along, for example, the x-axis, will result in rotation about the x-axis, torque applied along the y-axis will result in rotation about the y-axis, etc. That is, the inertia tensor for an ideal symmetric and balanced object has nonzero values for the diagonal entries (i.e. Ixx, Iyy, and Izz) of the matrix and zeroes in the non-diagonal entries. However, for an asymmetric object, torque applied along the x-axis may result in rotation along the x-axis as well as the y-axis and z-axis. That is, the inertia tensor may have non-zero values for I throughout the matrix. Given that drill bits are asymmetric objects, the inertial tensor matrix for the drill bit will generally possess non-zero values throughout the matrix. In some embodiments, the drill bit may be balanced, not just by considering the drill bit's center of gravity relative to the pin axis, but also by considering the inertial tensor. Thus, in such a manner, the drill bit may be axially balanced as well as radially balanced.
Referring to
In order to perform the drill bit balancing operations, a drill bit may be modeled using Computer Aided Design (CAD) software, for example, Pro/Engineer, SolidWorks, AutoCAD, Autodesk, or other CAD software known in the art. Drill bit characteristics including, for example, drill bit mass, center of gravity (COG) coordinates of the drill bit, inertia tensor, and bit volume, may be provided by the model. One of ordinary skill in the art will understand that other physical properties of the drill bit may be provided by the model. These drill bit characteristics may then be input into a simulator to perform drill bit balancing operations.
After inputting the drill bit characteristics into a simulator, static balancing operations may be performed. A drill bit is considered statically balanced if the center of gravity of the pin is in line with the pin axis. According to one embodiment of the present disclosure, a drill bit may be statically balanced by changing the number, location and/or size of the stabilizer pads. Referring to
According to another embodiment of the present disclosure, the wedge 10 and/or legs 12 may be designed to be asymmetric about the pin axis 6 to compensate for imbalance introduced by cone separation angles (discussed above with reference to
According to another embodiment of present disclosure, static balancing operations may include simulating to find a static mass value that can be added to the drill bit in order to align the center of gravity of the drill bit with the pin axis. As used herein, the term “static mass” may refer to a mass that is added to the drill bit (such as in the form of the nozzle extender balancers, stabilizer pads, changes to the wedge geometry, etc) to achieve static balancing. One of ordinary skill in the art will understand, after reading the present disclosure, that more than one static mass may be added to the drill bit (in at least one location) in order to align the center of gravity with the pin axis and that the number (or location) of masses added to the drill bit for static balancing operations should not be seen as limiting the scope of the present disclosure.
In addition to the drill bit characteristics, a radial offset, corresponding to an approximate location of the static mass along the x-axis, and a static longitudinal offset, corresponding to an approximate location of the static mass along the y-axis may be determined and input into the simulator. The radial and axial position may be defined as a function of the available space between the cones. One of ordinary skill in the art will understand that the radial offset may alternatively correspond to an approximate location of the static mass along the z-axis depending on the orientation of the drill bit with respect to the coordinate system. In some embodiments, the radial offset alone may be input into the simulator to perform static balancing. Using the mass of the drill bit, the location of the center of gravity of the drill bit, and radial and longitudinal offsets, the static mass characteristics including mass value, COG coordinates may be determined.
Once the static mass characteristics have been calculated, the new statically balanced drill bit characteristics may be determined. The statically balanced drill bit characteristics may include a new mass, the COG coordinates, and the inertia tensor for the statically balanced drill bit. If the static balancing is performed correctly, the COG coordinates for the statically balanced drill bit should have values of about zero corresponding to the x and z coordinates. As used with respect to the x and z coordinates of the COG for the statically balanced drill bit, the phrase “about zero” may refer to a value of within 0.03 in of 0 for bit diameters 3½ ft thru 12¼ in, within 0.05 in of 0 for bit sizes larger than 12¼ in thru 20 in, and within 0.08 of 0 in for bit sizes 20 in and larger, and in some embodiments, may refer to a value of within about 0.03 in of 0 for bit diameters 3½ ft thru 12¼ in, within about 0.05 in of 0 for bit sizes larger than 12¼ in thru 20 in, and within about 0.08 of 0 in for bit sizes 20 in and larger.
Following static balancing operations (or instead of if just dynamic balancing is to be performed), dynamic balancing operations may be performed. Dynamic balancing operations may include adding at least two masses or dynamic masses to the drill bit in order to align the inertia tensor with the pin axis. The pair of dynamic masses may provide a force couple. As used herein, the term “dynamic mass” may refer to a mass that is added to the drill bit to achieve dynamic balancing. One of ordinary skill in the art will understand that more than two dynamic masses may be added to the drill bit in order to align the inertia tensor with the pin axis, and the number of masses added to the drill bit for dynamic balancing operations should not be seen as limiting the scope of the present disclosure.
In order to perform dynamic balancing, a first dynamic longitudinal offset for a first dynamic mass and a second dynamic longitudinal offset for a second dynamic mass may be input into the simulator. Referring to
Referring to
√(Ixy2+Iyz2)Ixy|
An unbalancing factor of less than 0.01 corresponds to a misalignment of 0.5° between 8 and 8′. For smaller drill bits, e.g. less than 12¼ in, an unbalancing factor of less than 0.02 may be acceptable. In the event that the dynamically Ixy, Iyx and Izy, Iyz values are not about zero, the dynamic balancing operations, or alternately, the dynamic and static balancing operations, may be performed again.
Once the balancing operations are completed and a new mass and COG of the dynamically balanced drill bit are determined, a drill bit with a new mass distribution representative of the static mass and dynamic masses may be determined by modeling the dynamically balanced drill bit using CAD software. As used herein, the term “new mass distribution” refers to a drill bit with the drill bit characteristics of the dynamically balanced drill bit. In some embodiments, the static and dynamic masses may be represented in the model by a sphere of steel. As seen in
For an as-manufactured finished drill bit, the mass distribution of the drill bit may be modified by adding or removing mass from the drill bit based on the new mass distribution, which factors in manufacturing tolerances and variations in welding volume. Modifying the mass distribution may not produce a drill bit identical to the dynamically balanced drill bit model, as adding multiple spherical volumes to the surface of the drill bit, as seen in
For a drill bit that has not yet been manufactured, the drill bit may be materially produced as described above. Specifically, materially producing the drill bit includes machining a bit body 7 of the drill bit 5, where the bit body 7 includes at least two legs 12 and a wedge section 10. The wedge section 10 may be machined to include a number of openings 20. Sleeves or nozzle attachments 24 may then be welded or otherwise coupled to the body. The legs 12 of the drill bit may then be machined. One of ordinary skill in the art will understand that the order of machining the bit body and the legs are not intended to limit the scope of the present application. The legs 12 may be machined to include journals disposed thereon. In some embodiments, the journals may be integrally formed with the legs 12. In other embodiments, the journals may be machined separately from the legs 12 and subsequently coupled to the legs 12 using, for example, welds, a braze, rivets, a press fit or any other coupling means known in the art. A roller cone with cutting structures disposed thereon may be mounted on each journal, and retained, for example, by a ball bearing retention system.
After machining the leg sections and mounting the roller cones on the journals, the drill bit may be assembled. Specifically, bit body and legs may be welded together. Once the bit body and the legs have been welded, an upper section 17 of the drill bit may be machined. In some embodiments, the upper section 17 may be a separate component welded to the top of the welded bit body and legs. In other embodiments the upper section may be formed integrally from the welded bit body and legs. The upper section includes a pin end 23. A nozzle balancer 22 may also be welded or otherwise coupled to the bit body. For example, the nozzle balancer may be welded, brazed, or press fit to the bit body. Further, stabilizer pads 18 disposed on the legs and bit body may be machined. The stabilizer pads may define an outer diameter of the drill bit. The stabilizer pads may also include a plurality of inserts installed thereon. The inserts may be welded or press fit to the stabilizer pads. Once the drill bit has been manufactured, the mass distribution of the drill bit may be modified by adding or removing mass from the drill bit.
To demonstrate the effectiveness of the drill bit balancing operations, a drill bit was modeled using Pro/Engineer. Although, one of ordinary skill in the art will understand that other CAD software may be used without departing from the scope of this disclosure. The drill bit characteristics of the modeled drill bit are provided below in Table 1 below. The unbalanced drill bit characteristics (provided in the first section of Table 1 below), including unbalanced inertia tensor matrix, mass, and COG coordinates of the drill bit, were then provided to the simulator as inputs. The angle Z0-X0 and the length of the hypotenuse between those Z0 and X0 were then calculated using expression (2) and Pythagorean's theorem, respectively.
180°+a tan(Z0,X0) (2)
In addition, referring to
Once the inputs were entered into the simulator, the static mass value (shown in Table 2 below) was determined by multiplying the mass of the drill bit (M0) by the Z0-X0 hypotenuse and dividing the product by the radial offset. Next the COG coordinates for the static mass were calculated. Xst was determined by multiplying the radial offset by sine of angle Z0-X0, Yst was determined by adding the longitudinal offset to Y0, and Zst was determined by multiplying the radial offset by sine of angle Z0-X0. The inertia tensor for the static mass was then calculated using equations (3) shown below.
I
xx
=M
st(Yst2+Zst2)
I
yy
=M
st(Xst2+Zst2)
I
zz
=M
st(Xst2+Yst2)
I
xy
=I
yx
=M
st(Xst×Yst)
I
xz
=I
xy
=M
st(Xst×Zst)
I
yz
=I
zy
=M
st(Yst×Zst) (3)
In order to determine the value of the statically balanced drill bit characteristics shown in Table 2, the sum of the corresponding values of mass, COG coordinates, and inertia tensor, were taken. That is, the sum of M0 and Mst was taken to give Mbal-static. Xbal-static, Ybal-static and Zbal-static are given by the equations (4).
X
bal-static=(Mst·Xst+M0·X0)/(M0+Mst)
Y
bal-static=(Mst·Yst+M0·Y0)/(M0+Mst)
Z
bal-static=(Mst·Zst+M0·Z0)/(M0+Mst) (4)
As seen in Table 2, the Xbal-static and the Ybal-static are about zero, as desired. Thus, if the angle Z0-X0 and the length of the hypotenuse between those Z0 and X0 were to be calculated, they would also be about zero. Similar to the mass and COG calculation for the statically balanced drill bit, the inertia tensor matrix for the statically balanced drill bit was produced by the sums of each like element of the static mass inertia tensor matrix and unbalanced inertia tensor matrix.
Next, dynamic balancing operations were performed, the data for which is shown in Table 3 below, to find the phase angle, mass values, and position that will result in about zero values for Ixy and Iyz in the inertia tensor matrix. In the example simulation, a first longitudinal offset of −6 in. for a first dynamic mass and a second longitudinal offset of 4 in. for a second dynamic mass were input into the simulator. An angle Ixy-Iyz for the statically balanced drill bit was determined using expression (2), substituting the statically balanced Ixy and Iyz for z0 and x0, respectively. Next the COG of the first and second dynamic masses were calculated. In order to determine the Xdyn1, the longitudinal distance between the first and second dynamic masses was multiplied by the sine of the angle for the statically balanced drill bit. Zdyn1 was determined by multiplying the longitudinal distance between the first and second dynamic masses by the cosine of angle Ixy-Iyz for the statically balanced drill bit. In this example, Xdyn2 and Zdyn2 were determined by taking the negative of Xdyn1 and Zdyn1.
The first dynamic mass was then calculated by dividing the Ixy value for the statically balanced drill bit by the product of Mbal-static and the longitudinal distance between the first and second dynamic masses. In this example, the value of the first and second dynamic masses are equal. The inertia tensor of the first and second dynamic masses were then found using equations (4) as applied to the Mdyn1 and COG coordinates (Xdyn1, Ydyn1, Zdyn1) and Mdyn2 and COG coordinates (Xdyn2, Ydyn2, Zdyn2), respectively.
In order to determine the value of the dynamically balanced drill bit characteristics of mass, COG coordinates, and inertia tensor, the sum of the corresponding values were taken. That is, the sum of Mdyn1, Mdyn2, and Mbal-static was taken to give Mbal-dyn, Xbal-dyn, Ybal-dyn, and Zbal-dyn were determined by using equations (5). As seen in Table 1, the Ixy/Iyx and Izy/Iyz values are about zero, as desired.
X
bal-dyn=(Mbal-st·Xbal-st+Mdyn1·Xdyn1+Mdyn2·Xdyn2)/(M0+Mdyn1+Mdyn2)
Y
bal-dyn=(Mbal-st·Ybal-st+Mdyn1·Ydyn1+Mdyn2˜Ydyn2)/(M0+Mdyn1+Mdyn2)
Z
bal-dyn=(Mbal-st·Zbal-st+Mdyn1·Zdyn1+Mdyn2˜Zdyn2)/(M0+Mdyn1+Mdyn2) (5)
In one embodiment, a method of balancing a drill bit includes inputting drill bit characteristics into a simulator. The drill bit characteristics may include an intertia tensor, a drill bit mass and coordinate of the drill bit center of gravity. Once the inputs have been provided to the simulator, the coordinates of the center of gravity and the Iy vector of the inertia tensor may be aligned with the pin axis of the drill bit. After aligning the COG coordinates, Iy vector, and pin axis, a new mass distribution of the drill bit may be determined. Determining the new mass distribution of the drill bit may include producing a model of the drill bit. Once the new mass distribution has been determined, a drill bit with the new mass distribution may be materially produced.
In another embodiment, a method of balancing a drill bit may include assembling a drill bit. Characteristics corresponding to the assembled drill bit may then be determined and input into a simulator. Once the inputs have been entered into the simulator, a mass balance may be performed with the simulator. Based on the mass balance a new mass distribution may be determined. Then, the drill bit may be modified by adding or removing mass based on the new mass distribution.
Although the examples of the methods provided herein are directed to the design and manufacture of two cone drill bits, one of ordinary skill in the art would understand that the methods may also be applied to the design and manufacture of three cone drill bits, fixed cutter bits, bi-center bits, hammer bits, hybrid roller cone/fixed cutter bits, or any tool known in the art, including those where asymmetry may cause instability.
Although only a few example embodiments have been described in detail above, those skilled in the art will readily appreciate that many modifications are possible in the example embodiments without materially departing from this invention. Accordingly, such modifications are intended to be included within the scope of this disclosure as defined in the following claims. Moreover, embodiments disclosed herein may be practiced in the absence of any element which is not specifically disclosed.
In the claims, means-plus-function clauses are intended to cover the structures described herein as performing the recited function and not just structural equivalents, but also equivalent structures. Thus, although a nail and a screw may not be structural equivalents in that a nail employs a cylindrical surface to secure wooden parts together, whereas a screw employs a helical surface, in the environment of fastening wooden parts, a nail and a screw may be equivalent structures. It is the express intention of the applicant not to invoke 35 U.S.C. §112, paragraph 6 for any limitations of any of the claims herein, except for those in which the claim expressly uses the words ‘means for’ together with an associated function.
This application claims the benefit to and priority of U.S. Provisional Application 61/891,544 filed on Oct. 16, 2013, the entirety of which is incorporated herein by reference.
Number | Date | Country | |
---|---|---|---|
61891544 | Oct 2013 | US |