BACKGROUND OF THE INVENTION
Field of the Invention
[0001] The present invention is directed to a multiple stage turbine for use as a downhole
motor on a drilling string, and more particularly, to a multiple stage turbine downhole
motor which is driven by the drag or shear stress force alone or in combination with
the dynamic or impulse force of the fluid flowing through the turbine.
Description of the Prior Art
[0002] Prior art downhole motors for use on drilling strings convert the kinetic energy
of a mass of a fluid against the face surface of turbine blades into power for turning
a drill string and thereby a drill bit attached to the bottom of the drill string.
The turbines rely solely on the dynamic or impulse force. Prior art downhole motors
of this type are generally required to be relatively long in order to have sufficient
turbine blade surface area for generating enough power to turn the bit at the proper
speed with sufficient torque. However, because the downhole motor itself is quite
long, it is difficult for the drill string to move through curves and thus it is much
more difficult to control the direction of drilling.
[0003] Another disadvantage of the dynamic force type downhole motors, is that maximum power
and efficiency occur at rather high rotational speeds; higher than the range of operational
speed for most mechanical drill bits, like tricone bits. The reason for this characteristic
is that the functions of power and efficiency, in terms of the velocity of the flow
is proportional to the square of the velocity. The function is a parabola in which
the apex is approximately midway between zero and runaway or no load speed.
[0004] Still another disadvantage of prior art downhole turbine motors is that the turbine
blades are internal with respect to the drilling shaft. In order to drive the turbine,
fluid must flow through the internal structure of the drill string and can cause damage
to the bearings, seals and other internal parts of the downhole motor.
SUMMARY OF THE INVENTION
[0005] A helical multiple impulse hydraulic downhole motor is described in my prior U. S.
patent application Serial No. 045,822, filed May 4, 1987, now abandoned. This application
is incorporated herein by reference.
[0006] It is the primary object of the present invention to provide a multiple stage turbine
which operates by using the shear force of the fluid on the edges of the blades of
the turbine either alone or in combination with the impulse force of the fluid on
the surface of the blades.
[0007] It is another object of the present invention to provide a downhole motor for use
in turning a drilling string, and thereby a drill bit on the end of the drill string,
which operates at a relatively slow speed of 300 - 500 rpm and produces high torque,
with no torque on the pipe of the drill string itself.
[0008] It is another object of the present invention to provide a multiple stage turbine
in which the rotor having the turbine blades, is external to the drilling shaft and
thus the moving parts are external to the drilling shaft. Further, because the blades
are attached to an external movable part, the generated forces are farther away from
the axis of the turbine, giving more leverage and hence more torque.
[0009] The present invention is directed to a multistage turbine for driving a downhole
motor, which is driven by the flow of a fluid therethrough. The turbine comprises
a housing with a plurality of rims and a shaft positioned in the housing, the housing
and rims rotating about the longitudinal axis thereof. A plurality of turbine stages
are mounted on the housing for rotation therewith, each turbine stage including a
rim coaxial with the shaft and a plurality of turbine blades fixed to each rim. A
plurality of flow directing stators are positioned between adjacent turbine stages,
each of the stators having a wall portion and diverter portion, wherein the wall portions
are perpendicular to the axis of the shaft and the diverter portions are at an angle
of less than 90° with respect to the axis of the shaft. At least three of the turbine
blades and the diverter portions form a seal for preventing the flow from passing
therebetween, such that flow through a turbine stage is perpendicular to the axis
of the shaft in the space between adjacent wall portions and wherein the diverter
portions are positioned with respect to said wall means for diverting flow from the
turbine stage to an adjacent turbine stage.
[0010] The turbine blades are positioned between adjacent stators such that flow between
the wall portion of adjacent stators contacts the edges of the turbine blades, thereby
imparting a drag force on the turbine blades and flow through adjacent diverter portions
impinges upon the face surface of the turbine blades, thereby imparting a dynamic
force on the turbine blades, whereby the turbine blades are rotated by the combination
of the drag forces and dynamic forces thereon.
BRIEF DESCRIPTION OF THE DRAWINGS
[0011] Figure 1 is a sectional view of a downhole motor of the present invention.
[0012] Figure 1a is an expanded view of a portion of Figure 1.
[0013] Figure 1b is a sectional view through Section 1b-1b in Figures 1 and 1a.
[0014] Figure 2 is a perspective view of the flow through a turbine of the present invention.
[0015] Figures 3a and 3b are diagrams for analyzing the flow and forces in a turbine of
the present invention.
[0016] Figure 4 is a partial sectional view of a turbine of a first embodiment of the present
invention.
[0017] Figure 5 is a perspective view of a rotor stage of the present invention.
[0018] Figure 6 is a front view of the rotor stage of Figure 5.
[0019] Figure 7 is a perspective view of a stator of the first embodiment of the present
invention.
[0020] Figure 8 is a perspective view of an alternate embodiment of a stator of the present
invention.
[0021] Figure 9 is a partial layout illustrating the flow of fluid through a first embodiment
of the turbine of the present invention.
[0022] Figure 10 is a partial layout illustrating the flow of fluid through a second embodiment
of the turbine of the present invention.
[0023] Figure 11 is a partial sectional view of a turbine of a second embodiment of the
present invention.
[0024] Figure 12 is a perspective view of the stator of the second embodiment of the present
invention.
[0025] Figure 13 is a front view of the stator of Figure 12.
[0026] Figure 14 is a bottom view of the stator of Figure 12.
[0027] Figure 15 is a partial layout illustrating the flow of fluid through a third embodiment
of the turbine of the present invention.
[0028] Figure 16 is a partial layout illustrating the flow of fluid through a fourth embodiment
of the turbine of the present invention.
[0029] Figure 17a is a partial sectional view of a fifth embodiment of the turbine of the
present invention.
[0030] Figure 17b is a partial sectional view of Section 17A-17A' of Figure 17a.
[0031] Figure 17c is a sectional view of Section 17B-17B' of Figure 17b.
[0032] Figure 17d is a perspective view of the turbine rotor of the fifth embodiment of
the present invention.
[0033] Figures 18a and 18b are partial layouts illustrating the intermediate seal for the
drag and dynamic embodiment of the present invention.
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS
[0034] The present invention is directed to a multiple stage turbine which comprises a plurality
of single stages, each of which operates on the principle of the shear stress of fluid
flowing in passages or spaces in the stage against the edges of the turbine blades
which generate drag forces either alone or in combination with impulse forces of the
fluid against the surface of the blades. The volume of flow is not a factor as to
the drag force or the shear forces on the edges of the turbine blades. The power produced
by the drag force is a function of the relative velocity and drag surface, the drag
surface being the edges of the turbine blades, and not the surface or face of the
blade itself. The use of the drag force results in a higher torque then a conventional
turbine rotor of the same dimensions. This enables the motor of the present invention
to generate sufficient torque using less stages, which in turn enables it to be shorter
in length than a conventional turbine motor.
[0035] Figure 1 is an elevational view of a downhole motor 1 which comprises an outer casing
3 and an inner shaft 5. The motor further includes a bearing assembly 7 and a turbine
assembly 9 having a plurality of stages, each stage having a stator and rotor assembly.
Each stator assembly comprises a plurality of flow directing stators 11 and each rotor
assembly comprises a plurality of turbine blades 13 which are fixed to a rotor rim
15.
[0036] A plurality of turbine rotors 13 are pre-loaded and held together by means of nuts
28 and 29 located at the ends of the downhole motor. A drill bit (not shown) may be
connected to nut 28. These nuts also hold the bearing assembly 7 in place. The bearings
7 may be tapered journal bearings or other types of bearings such as ball bearings.
If necessary, nuts for holding the assembly together can be used as intermediate portions
of the motor. Block 31 provides separation between the bearing assembly 7 and the
turbine assembly 9 and forms a seal therebetween. Block 31 can also be used to house
a pressure compensator for the bearing lubrication system, should such pressure compensation
be necessary.
[0037] Referring to Figures 1, 1a and 1b, fluid, the flow of which is illustrated by arrows
F1 - F7, flows through the downhole motor 1 as shown. Flow starts at F1 - F3 axially
through the center of shaft 5, between F3 and F4, the fluid flows through a plurality
of slots 33 in the shaft 5. Between F4 and F5, the fluid flows through the turbine
assembly 9, rotating the turbine blades 13 and the outer casing 3. End piece 28 is
screw-threaded into outer casing 3 and tightened against blades 13 to thereby cause
the blade 13 to rotate with the outer casing 3. At F5 - F6, the fluid then flows out
of the turbine assembly 9 and into the shaft 5 through additional slots 35, which
are the same as slots 33, and then exits from the downhole motor into the bore hole.
As can be seen, the turbine assembly is mounted on the outside of the shaft 5, thus,
the moving parts are external to the drill shaft.
[0038] Figure 2 shows the flat helical flow path through a turbine assembly 9. The turbine
assembly is mounted on a shaft 5. The turbine assembly includes a plurality of flow
directing stators 11 fixed to the shaft 5, with a plurality of turbine blades 13 being
fixed to the corresponding rotor rim 15 being positioned to rotate between adjacent
stators 11 (See Figure 1). A seal is formed between flow directing portions 19b and
19a and the turbine blades 13 so that the flow F is circular in the channel or space
formed between adjacent stators 11 and then flows through the channel or space between
the flow diverters 17a and 17b and 19a and 19b into an adjacent turbine stage between
the next adjacent stators 11. Thus as can be seen, the flow follows a flat circular
path through almost an entire 360° and then a somewhat helical path diagonally downward
into the next turbine stage. The drag forces and impulse forces applied to the turbine
blades by the flow through the turbine will depend upon the configuration of the turbine
blades 13 and the stators 11 as will be explained in more detail below.
[0039] The turbine of the present invention is driven by the shear stress or drag force
in combination with the dynamic or impulse force of the fluid flowing through the
turbine. The drag force is generated by the flow of fluid against the edges of the
turbine blades. The dynamic force is generated by the impact of the flow against the
surface of the face of the turbine blades as its flows through the rotor blades at
the entrance and the outlet of each turbine stage.
[0040] The total force acting on the rotor is:
where:
- Fdr =
- shear force or drag force
- Fdy =
- impulse or dynamic force
The drag force is as follows:
where:
- γ =
- specific weight of the fluid (Kgf/m³).
- λdr =
- drag coefficient (dimensionless) from rotor blades and channels geometrical configuration.
- C =
- mean velocity of the flow through the drag channels (m/sec).
- u =
- peripheral velocity of the rotor (m/sec).
- adr =
- drag area upon which the shear stress acts (m²).
[0041] The dynamic force can be calculated with reference to Figure 3a which is a section
of the rotor blades, transverse to the axis of rotation wherein:
- u =
- tangential velocity of the rotor (m/sec).
- w₁ =
- relative velocity of the flow (m/sec).
- β₁ =
- angle of w₁ with the direction u (degrees).
- C₁ =
- absolute velocity, vectorial addition of of u and w₁.
- α₁ =
- angle of C, with the direction of u.
- wx1 =
- component of w₁ in the direction of movement u.
[0042] The subscript "1" corresponds to the inlet of the flow for every change of direction
through the blade assembly.
[0043] The subscripts "2" are used to denote the corresponding values of the flow at the
outlet of every change of direction, generating a hydraulic impulse.
[0044] In order to deduce or obtain the equation for the dynamic force, referring to Figure
3b, shows the composition of the triangles of velocities at the inlet and outlet of
the flow at every impulse or change of direction.
[0045] According to Newton's Second Law:
wherein:
w
x1 and w
x2 are the components of the relative velocities in the direction of the movement.
Then:
and
wherein:
- m =
- number of changes of direction or impulses in each stage.
[0046] Referring to Figures 4 - 6, it can be seen that the blades 13 are fixed to rotor
rims 15. Although only four blades are shown, the remaining blades are positioned
around the entire rim 15. When a plurality of rotor assemblies are used as shown in
Figure 1, the rim 15 can have a width equal to the width of the turbine blades 13
and a spacer 15' can be positioned adjacent to the rim 15. Alternatively, the rim
15 can be made wider than the blade 13 so that the spacer 15' is an integral portion
thereof. Figure 6 is an elevation view taken in plane 6-6 of Figure 5 showing the
orientation of blades 13 with respect to rim 15 and the center of rim 15. Although
the blades 13 are shown in a V-shape cross-section, other cross-sections can be used
such as a rounded V, offcenter V, a combination of round and offcentered Vs, etc.
[0047] Figure 7 is a perspective view of a flow directing stator 11. Stator 11 has wall
portions 25 and flow diverting portions 17a and 17b and 19a and 19b. Flow diverting
portions 17a and 19a form seals with adjacent turbine blades 13, as shown in Figure
2. Although the seal is not a perfect seal since it is necessary for the turbine blades
to rotate, the seal substantially stops the flow of fluid thereby maintaining the
proper flow path through the turbine assembly as will be described below. The stator
11 further comprises a hub 21 having a keyway 23 for receiving the key 6 when the
stator is mounted on the shaft 5. The stator assembly further includes a wall portion
25 integrally formed with the flow directing portions. As shown in Figure 4, a space
27 is formed between wall portion 25 and spacer 15'. The space 27 is made very small
so that the flow of fluid through the space is negligible, but the space is sufficient
to permit the rotation of rotor 13 with respect to stator 11.
[0048] Figure 8 is an alternative embodiment of the stator 11 in which the hub 21 has a
reduced diameter portion 21a. The length or angle of the reduced portion will depend
upon the particular flow characteristics but generally will be less than 90°. The
purpose of the reduced hub radius is to allow the fluid to flow under the blades 13c,
thereby eliminating the impulse forces on blades 13c and to quickly equalize the flow
on both sides of the blades 13d. If desired, the sharp corners between surfaces 17a
and 17b, and 19a and 19b can be rounded in order to smooth the flow and reduce turbulence.
[0049] Figure 9 is a partial layout illustrating the flow of fluid through two blade assemblies
13 in a first embodiment of the turbine of the present invention. The arrows F show
the flow and the arrows D and I illustrate the drag and dynamic forces on the turbine
blades 13. Starting from the right, the flow F causes a drag force D on the edges
of the turbine blades 13. When the flow reaches surface 17b, it is diverted downward
as shown, striking the blades 13a and applying a dynamic force I to the blades 13a.
Flow then continues through flow diverters 19a and 19b into the adjacent stage of
turbine blades and again dynamic forces I are applied to blades 13a. Flow then continues
towards the left where only drag forces are applied to the edges of the blades 13.
[0050] Figure 10 is a partial layout illustrating the flow of fluid through a second embodiment
of the turbine of the present invention in which three impulses are produced in each
stage. The arrows F show the flow and the arrows D and I illustrate the drag and dynamic
on the turbine blades 13. Starting from the right, the flow F causes a drag force
D on only one edge of the turbine blades 13. In the embodiment of Figure 8, the turbine
blades are configured so that the drag force is on both edges of the blades. When
the flow reaches surface 17b it is diverted downward, as shown, striking the blades
13a and applying a dynamic force I to the blades 13a. The flow then continues through
flow diverters 19a and 19b into the adjacent stage of turbine blades 13 and again
dynamic forces are applied to blades 13a.
[0051] In the embodiment of Figure 10, there are three changes of direction so three impulses
are generated in every stage. In the equation (3), in this case the value of parameters
"m" would be three.
[0052] Figures 11 - 15 illustrate a third embodiment of the turbine of the present invention.
In Figure 11, flow directing stators 111 include diverter portions 117a, and 117b
and 119a and 119b and wall portions 125. The turbine blade stages 113 are the same
as those described in the embodiment of Figures 4 - 6.
[0053] Figure 12 is a perspective view of the flow directing stator 111. The stator 111
comprises a hub 121 with a keyway 123 and a wall portion 125. The wall portion 125
has a plurality of sections 125a - 125k (not shown in Figure 12) which can be seen
in Figure 13 which is a full layout of a plurality of flow directing stators and turbine
blade stages. Figure 13 is an elevational view in plane 13-13 of Figure 12, and Figure
14 is a side view of Figure 13 in plane 14-14. The surfaces of diverter portions 117
and wall portions 125 in the corresponding Figures 11 - 15, have been designated by
letters A - G.
[0054] The flow through the turbine in the embodiment of Figures 11 - 15 is illustrated
by the arrows F in Figure 15. This flow causes impulse forces on the outer halves
113a of the turbine blades 113. The inner halves 113b of the turbine blades 113 do
not have any significant forces acting thereon, but rather, act with corresponding
diverter wall portions 125a, 125e and 125i to form a substantial seal therebetween.
The seals ensure that the flow is as indicated by arrows F, rather than through the
space between the turbine blades and the wall portions 125a, 125e and 125i. The impulse
forces on the turbine blades 113a are the same impulse forces described above with
respect to the embodiment of Figures 4 - 9. As can be seen however, in this embodiment
there are no substantial drag forces on the turbine blades. The lack of substantial
drag forces occurs because centrifugal force on the flow moves the fluid towards the
outside against wall portions 125c, 125k and 125g which are away from the edges of
the turbine blades. This embodiment is the limit for the dynamic force, because "m"
has been increased to provide the maximum dynamic force.
[0055] Figure 16 shows a fourth embodiment of the turbine of the present invention. In this
embodiment, the blades 213 are alternately attached to the outside rotor rim (not
shown). A sealing wall members form a seal with one side of blades 213, and the other
side of blades 213 form a seal with stator 211. Flow is in one direction around the
annular space and is almost 360° at which point it flows through the outlet into the
next stage. The sinuous path of the flow F produces drag forces D on the tips or edges
of the blades 213 and additionally produces impulses I on the surfaces of the blades.
The drag and dynamic forces can be calculated in accordance with the equations set
forth above. However, since the path is not very well defined, the equations have
to be effected by coefficients determined experimentally.
[0056] Instead of blades, planar or rounded bodies can be used and attached to the rotor
rim to eliminate eddy currents and turbulence and to enhance impulses on the slanted
surfaces to produce the desired number of smooth changes of direction along the annular
channels.
[0057] Figures 17a - 17d illustrate a fifth embodiment of the turbine of the present invention.
In this embodiment, the turbine is substantially a pure drag turbine which is simple,
versatile, has high torque and a comparatively high efficiency. Additional turbine
blades can be added to produce additional forces either drag forces or dynamic forces
to modify the performance of the turbine, if desired.
[0058] Referring to Figures 17a - 17d, the flow indicated the arrow F, flows through the
turbine with the intermediate seal 315 at the diagonal entrance of the next stage.
The turbine has blades 313 which contact seals 315. The seal 317a and the diagonal
diverter divert the flow through opening 317 in the wall of stator 311. The flow channel
is cylindrical and covers almost 360° and is coaxial and parallel with the cylindrical
space covered by the rotor and its blades. In other words, the flow is cylindrical
and intermediate between the edges of the blades and the internal hub, as shown in
Figure 17c.
[0059] The blade length, thickness, angle of inclination, as well as separation between
blades, can be varied. All of these variables affect the drag coefficient λdr and
thus the ultimate drag force, velocity and efficiency.
[0060] The drag action in this embodiment of the present invention is generally better than
in the other embodiments of the present invention.
[0061] In the fifth embodiment, since the flow through the channels is cylindrical and parallel
to the rotor and blades, the blades do not cross or deviate from the direction of
the flow, to produce an impulse, except in the change of stages. The change of direction
of the flow from one stage to the next is produced by the seal and stator and hence
friction loss, and correspondingly hydraulic head loss are small.
[0062] The following is an explanation of the manner in which the intermediate seals operate
in the present invention. Considering one stage of the turbine with the drag and dynamic
actions, such as in Figure 18a and 18b, which shows schematically a section of the
channel with seven changes of direction. The rotor is shown divided in two portions;
one is the seal portion in the change of stage, and the other is the complement portion
for the rest of the rotor.
[0063] The equilibrium equations for each one of the those portions are:

P₁ and P₇ are the pressures at the inlet and outlet of the stage, and Ap is the area
of the blades on which the pressures act.

The total force acting on the rotor will be:
Thus, the forces coming from pressure acting on the section cancel each other.
[0064] Although the present invention is shown as a turbine, the principles of the invention
can also be used for a pump, blower or compressor.
[0065] The present invention may be embodied in other specific forms without departing from
the spirit or essential characteristics thereof. The presently disclosed embodiments
are therefore to be considered in all respects as illustrative and not restrictive,
the scope of the invention being indicated by the appended claims, rather than the
foregoing description, and all changes which come within the meaning and range of
equivalency of the claims are, therefore, to be embraced therein.
1. A turbine for driving a downhole motor, said turbine being driven by the flow of a
fluid therethrough said turbine comprising:
(a) a housing;
(b) a shaft positioned in said housing, said shaft rotating about the longitudinal
axis thereof;
(c) a rotor assembly having a plurality of turbine stages mounted on said shaft for
rotation therewith, each turbine stage including a rim means coaxial with said shaft
and a plurality of turbine blades fixed to said rim means; and
(d) a stator assembly having a plurality of flow directing stator means, each of said
stator means being positioned between adjacent turbine stages, each of said stator
means having a wall means and diverter means, wherein said wall means are perpendicular
to the axis of said shaft and said diverter means are at an angle of less than 90°
with respect to the axis of said shaft, wherein at least one of said turbine blades
and said diverter means form a seal for preventing the flow from passing therebetween,
such that flow through a turbine stage is perpendicular to the axis of said shaft
in the space between adjacent wall means and wherein said diverter means are positioned
with respect to said wall means for diverting flow from the turbine stage to an adjacent
turbine stage.
2. A turbine as set forth in Claim 1, wherein said turbine blades are positioned between
adjacent stator means such that the flow between the wall means of the adjacent stator
means contacts the edges of said turbine blades thereby imparting a drag force on
said turbine blades whereby said turbine is rotated.
3. A turbine as set forth in Claim 1, wherein said turbine blades are positioned between
adjacent stator means such that flow between adjacent diverter means impinges upon
the face surface of said turbine blades thereby imparting a dynamic force on said
turbine blades whereby said turbine is rotated.
4. A turbine as set forth in Claim 1, wherein said turbine blades are positioned between
adjacent stator means such that flow between the wall means of adjacent stator means
contacts the edges of said turbine blades, thereby imparting a drag force on said
turbine blades and flow through adjacent diverter means impinges upon the face surface
of said turbine blades, thereby imparting a dynamic force on said turbine blades,
whereby said turbine blades are rotated by the combination of the drag forces and
dynamic forces thereon.
5. A turbine as set forth in any one of Claim 1, 2 or 4, wherein each of said wall means
are planar in single plane perpendicular to the axis of said shaft.
6. A turbine as set forth in any one of Claims 1, 2 and 4, wherein said turbine blades
are mounted on said rim such that the flow through a turbine stage contacts at least
one the side edges of said turbine blades.
7. A turbine as set forth in Claim 6, wherein said turbine blades are mounted on said
rim such that the flow through a turbine stage contacts both side edges of said turbine
blades.
8. A turbine as set forth in any one of Claims 1, 2 and 4, wherein said turbine blades
are mounted on said rim such that the flow through a turbine stage contacts the front
edges of said turbine blades.
9. A turbine as set forth in any one of Claims 1 - 4, wherein each of said wall means
comprises:
(a) a plurality of planar first sections perpendicular to the axis of said shaft,
wherein at least one of said planar first sections is not coplanar with at least another
of said planar first sections; and
(b) a plurality of planar second sections positioned between and interconnecting said
planar firs sections.
10. A turbine as set forth in any one of Claims 1, 2 and 4, further including center seal
means for forming a seal with a side edge of at least two of said turbine blades,
wherein when the seal is formed, the other side edge of said at least one turbine
blades forms the seal with said stator means.
11. A turbine as set forth in Claim 1, wherein said at least one turbine blade which forms
a seal with said diverter means is at least three turbine blades.