[0001] The invention relates to the oil and gas industry and is intended for the treatment
of the well bottom zones of oil and gas wells, for the purpose of increasing their
output. One method of achieving this objective is that of treating the productive
layer with acoustic field energy. To create such a field, two types of emitting systems
are most commonly used, namely the magnetostrictive and the piezoceramic types, the
basic frequency range of which is within the range of 10-25 kHz. Each of said two
types of emitter has its advantages and drawbacks, and their use depends on numerous
factors.
[0002] For emitters (devices) with magnetostrictive transducers, a rod-shaped type of active
element, known as a magnetostrictor, is most frequently used. The main argument in
favour of selecting this rod-shaped transducer is the possibility of producing emitters
with small dimensions. A liquid or a waveguide is used as the passive element for
transferring the energy of the elastic oscillations generated by the active element
(magnetostrictor) into the medium to be treated.
[0003] Devices for acoustic treatment of the well bottom zones of productive layers are
known from the patents
RU 2026970 and
RU 2674165, in which magnetostrictive transducers of the rod-shaped type with electrical windings
on the rods are located in an evacuated chamber. The energy of the elastic oscillations
is transferred to the medium to be treated by creating an oscillatory motion of the
liquid filling the chamber and therefore of the wall of the emitter housing, which
acts as a resonator.
[0004] In some cases, the passive element used for transferring the energy is a waveguide
or an acoustic transformer, in which case, in addition to transferring the energy,
the waveguide has the function of protecting the magnetostrictor from direct contact
with the corrosive downhole medium. This design is used in Patent
RU 2196217.
[0005] The transfer of the magnetostrictor energy also takes place by means of a waveguide
in the patent
RU 2634769, but, by contrast with the previous case, the magnetostrictive rod-shaped transducer
is located in a chamber of the open type, in direct contact with the downhole medium.
[0006] It should be noted that in all the aforementioned devices, rod-shaped magnetostrictive
transducers are used as the acoustic radiation source. The main drawback of such devices
is that the emitting surface of the device has a small area, but the magnetostrictive
transducers themselves radiate much of the energy in the axial direction and only
a small fraction of the energy goes in the radial direction. The task of the proposed
invention is to increase the efficiency of oil recovery. The technical result is an
increase in the radius of effective action of the acoustic emitter on the well bottom
zone of the layer, due to the increased acoustic power of the magnetostrictive transducer
which has a predominantly radial direction of radiation, and also due to the prevention
of corrosive destruction of the emitter and the increase in its efficiency.
[0007] The technical result is achieved because the acoustic emitter comprises a constituent
housing, consisting of two sealed chambers and one chamber that communicates with
the environment via apertures formed in the lower part of the constituent housing.
Sealed electrical lead-ins, for the connection of the excitation windings of the magnetostrictive
transducer, are placed in the cavity of the first sealed chamber (coaxial with the
geophysical head), which is filled with air. According to the invention, an acoustic
magnetostrictive transducer of cylindrical shape, with an electrical winding, is placed
in the second sealed chamber, which is filled with electrically insulating liquid.
A characteristic of the design of the magnetostrictive transducer is that between
the cylindrical core of the magnetostrictive transducer and its winding there are
fitted end pieces made of resilient material, which are used for uniform packing,
to provide a minimum gap between the winding and the cylindrical core itself, and
for fastening the magnetostrictive transducer in the sealed chamber. The sealed chamber
filled with liquid terminates in a bellows which is required for equalizing the pressure
in the sealed chamber of the emitter with the external downhole pressure. The electrically
insulating liquid is poured into the sealed chamber of the emitter through an opening
in the end of the bellows, which is sealed with a plug.
[0008] The mechanical oscillations of the magnetostrictive transducer with the cylindrical
core have a radial direction; that is to say, they are transmitted through the electrically
insulating liquid to the housing of the emitter, acting as a resonator, and from there
to the downhole medium in which the formation of the acoustic field in the well and
the well bottom zone takes place. Individual parts in the emitter housing are made
of non-magnetic materials, enabling electrical losses to be minimized.
[0009] Thus, the minimizing of electrical losses and the good heat dissipation from the
magnetostrictive transducer through the electrically insulating liquid to the walls
of the emitter housing, and through them into the downhole medium, provide stable
thermal conditions for the device, and, together with the isolation of the magnetostrictive
transducer from the corrosive downhole medium, make it possible to increase the operating
reliability and efficiency of the emitter, and consequently the effectiveness of the
acoustic treatment of the layer.
Calculation of the resonance frequency
[0010] Ring-shaped magnetostrictive transducers radiate sound from their inner or outer
surface, depending on the positioning of the screen. In the present case, radiation
takes place into the internal medium with a uniform azimuth characteristic of directionality
in a plane perpendicular to the axis of Fig. 1.
[0011] For a magnetostrictive transducer assembled from thin rings and operating with a
transverse piezoelectric effect, the intrinsic frequency is determined by the equation

where c is the speed of sound in the material from which the core of the ring-shaped
transducer is assembled,
E is Young's modulus, 2.18*1011 Pa
ρ is the density of the material; for Permendur, ρ = 8.15*103 kg/m3
R is the mean radius of the ring,

[0012] Let us calculate the speed of sound in Permendur:

[0013] Then the resonance frequency of the ring-shaped magnetostrictive transducer is:

[0014] Thus, the intrinsic frequency of the downhole acoustic emitter will be:
f
0 = 19500 Hz.
[0015] Other electrical parameters were calculated by the methods set out in [1], [2] and
[3]:
- [1] I.P. Golyamina, "Ul'trazvukovye preobrazovateli", Moscow, 1972, 200 pp;
- [2] A.V. Donskoy and O.K. Keller, "Ul'trazvukovye elektrotekhnologicheskie ustanovki",
Leningrad, Energoizdat, 1982, 208 pp.;
- [3] GOST 27955-88 (IEC 782-84) Preobrazovateli ul'trazvukovye magnitostriktsionnye.
Metody izmereniya kharakteristik.
Fig. 1 shows the direction of the oscillations of the cylindrical (ring-shaped) magnetostrictive
transducer, where R is the external radius of the core, and a is the width of the
ring;
Fig. 2 shows a longitudinal section through the downhole acoustic emitter.
[0016] The acoustic emitter for treating oil and gas wells comprises a constituent housing
1, consisting of a plurality of chambers, namely two sealed chambers 4 and 10 and
one (lower) chamber 2 that communicates with the environment via apertures 3 formed
in the lower part of the acoustic emitter housing. Sealed electrical lead-ins 11 are
brought into the cavity of the sealed chamber 10 (coaxial with the geophysical head
9), which is filled with air, for the connection of the excitation windings of the
magnetostrictive transducer 7.
[0017] According to the invention, in the sealed chamber 4, filled with electrically insulating
liquid, in the vibration zone 5, there is placed a magnetostrictive transducer 7 with
a core of cylindrical shape with an electrical winding, while, between the cylindrical
core of the transducer and its winding there are fitted end pieces 8 made of resilient
material, which are used for uniform packing, for providing a minimum gap between
the winding and the cylindrical core, and for fastening the magnetostrictive transducer
7 in the sealed chamber.
[0018] The components of the acoustic emitter housing 1 are sealed with rubber packing rings
(not shown in the figure), and the parts are secured mechanically with detachable
rubber connectors (not shown in the figure).
[0019] A standard geophysical head 9 is fitted at the upper end of the emitter housing 1
above the sealed chamber 4 with the magnetostrictive transducer 7, for connecting
the downhole acoustic emitter to a supply cable (not shown in the figure), the head
being connected to the electrical windings of the magnetostrictive transducer 7, using
sealed electrical lead-ins 11. The chamber 2, communicating with the downhole medium
through an aperture 3, takes the form of a cylinder terminating in a conical part.
The pressure in the inner sealed chamber 4 of the emitter, filled with electrically
insulating liquid, is equalized with the downhole pressure by means of a bellows 6.
[0020] The device operates in the following manner. An alternating voltage at an operating
frequency corresponding to the resonance frequency of the magnetostrictive transducer
7 is supplied from a surface generator by means of a cable through a standard geophysical
head 9 and sealed electrical lead-ins 11 to the electrical winding of the ring-shaped
magnetostrictive transducer 7 located in the sealed chamber 4. The contacts of the
geophysical head 9 are connected to the sealed electrical lead-ins 11 by means of
conductors (not shown in the figures) passing through the cavity of the sealed chamber
10. At the same time, a magnetic biasing current is supplied from the same generator
to the same electrical winding.
The alternating current flowing through the core winding of the ring-shaped magnetostrictive
transducer 7 creates an alternating electromagnetic field in the core, causing a change
in the dimensions of the core in the form of radial oscillations. These oscillations,
perpendicular to the cylindrical surface of the core, in the form of compression and
expansion waves, are transmitted to the liquid surrounding the core, which in turn
causes oscillations in the walls of the emitter housing 1 (in the vibration zone 5)
and in the surrounding medium. Between the cylindrical core and the winding of the
magnetostrictive transducer 7 there are fitted end pieces 8 made of resilient material,
which are used for uniform packing of the electrical winding, for providing a minimum
gap between the winding and the cylindrical core, for protecting the winding conductor
from wear, and for fastening the magnetostrictive transducer 7.
[0021] Additionally, the electromagnetic field of the electrical winding of the ring-shaped
magnetostrictive transducer 7 generates eddy currents in the walls of the emitter
housing 1 in the vibration zone 5, the walls heating up in these conditions. The downhole
medium, coming into contact with the metal housing 1 of the emitter in the vibration
zone 5, heats up as a result of thermal conductivity. Thus, during the operation of
the downhole acoustic emitter, a simultaneous wave and local heating action takes
place on the downhole medium with sufficient power, which is particularly important
for operation in wells with high-viscosity oil. The equalization of the pressure of
the sealed chamber 4, filled with electrically insulating liquid, with the external
downhole pressure takes place because of the bellows 6 which is positioned in the
chamber 2 and communicates with the downhole medium through the apertures 3.
[0022] By using the aforesaid device at low energy cost it is possible to carry out effective
thermo-acoustic treatment of the well bottom zone with the aim of increasing its production
rate by cleaning the perforations of the downhole equipment and the pores of the collector
to remove mechanical contaminants and gas hydrate and heavy oil deposits. The invention
makes it possible to increase the efficiency of oil recovery, especially in the extraction
of high-viscosity oil.
1. Acoustic emitter for treating oil and gas wells, taking the form of a cylindrical
housing (1), consisting of two sealed chambers (4;10) and one chamber (2) that communicates
with the environment via apertures (3), one first sealed chamber (10) being filled
with air and having sealed electrical lead-ins (11), while the second sealed chamber
(4) is filled with an electrically insulating liquid, characterized in that a magnetostrictive transducer (7), with a cylindrical core with an electrical winding
and end pieces (8) made of resilient material between the cylindrical core and the
electrical winding, is placed in the second sealed chamber (4) filled with electrically
insulating liquid.
2. Acoustic emitter for treating oil and gas wells according to Claim 1, characterized in that the magnetostrictive transducer (7) comprises a core of cylindrical shape, the radial
radiation of which causes an increase in the acoustic power of the radiation and effective
treatment of the downhole medium in the well bottom zone.
3. Acoustic emitter for treating oil and gas wells according to one of Claims 1 or 2,
characterized in that the one chamber (2) that communicates with the environment via apertures (3) is a
lower chamber and the apertures (3) are formed in the lower part of the housing (1).
4. Acoustic emitter for treating oil and gas wells according to one of Claims 1 to 3,
characterized in that the one chamber (2), that communicates with the environment via apertures (3), takes
the form of a cylinder terminating in a conical part.
5. Acoustic emitter for treating oil and gas wells according to one of Claims 1 to 4,
characterized in that the second sealed chamber (4) filled with the electrically insulating liquid terminates
in a bellows (6) which is used for equalizing the pressure in the sealed chamber (4)
of the emitter with the external downhole pressure.
6. Acoustic emitter for treating oil and gas wells according to Claim 5, characterized in that electrically insulating liquid is poured into the second sealed chamber (4) of the
emitter through an opening in the end of the bellows (6), which is sealed with a plug.
7. Acoustic emitter for treating oil and gas wells according to Claim 5 or 6, characterized in that the bellows (6) is positioned in the one chamber (2), that communicates with the
environment via apertures (3).
8. Acoustic emitter for treating oil and gas wells according to one of Claims 1 to 7,
characterized in that a geophysical head (9) is fitted at the upper end of the housing (1) above the second
sealed chamber (4) with the magnetostrictive transducer (7), the geophysical head
(9) being connected to the electrical winding of the magnetostrictive transducer (7),
using said electrical lead-ins (11).
9. Acoustic emitter for treating oil and gas wells according to one of Claims 1 to 8,
characterized in that the first sealed chamber (10), that is filled with air, is coaxially surrounded by
the second sealed chamber (4) filled with the electrically insulating liquid.
10. Acoustic emitter for treating oil and gas wells according to one of Claims 1 to 9,
characterized in that the magnetostrictive transducer (7) is ring-shaped.