阅读说明：本技术 随钻核磁共振探头天线配置方法、装置、设备及存储介质 (Method, device and equipment for configuring nuclear magnetic resonance probe antenna while drilling and storage medium ) 是由 廖广志 龙志豪 肖立志 孙哲 张文秀 侯学理 李楠 朱万里 于 2021-01-15 设计创作，主要内容包括：本发明实施例提供一种随钻核磁共振探头天线配置方法、装置、设备及存储介质,所述方法包括：采集随钻核磁共振探头的静磁场,根据静磁场确定静磁场对应的目标射频磁场；根据目标射频磁场确定电感值最小时,随钻核磁共振探头天线的天线参数；根据天线参数构建随钻核磁共振探头天线,以使随钻核磁共振探头天线产生最优射频磁场,使随钻核磁共振探头能够根据最优射频磁场激发共振信号,并接收共振信号对应的反馈信号,基于反馈信号获取原状地层信息。本发明实施例能够使设计得到的随钻核磁共振探头天线在实际应用中产生与理论中的目标射频磁场相似的最优射频磁场,进而使随钻核磁共振测井仪可以准确地探测原状地层信息。(The embodiment of the invention provides a method, a device, equipment and a storage medium for configuring a nuclear magnetic resonance probe while drilling antenna, wherein the method comprises the following steps: collecting a static magnetic field of a nuclear magnetic resonance probe while drilling, and determining a target radio frequency magnetic field corresponding to the static magnetic field according to the static magnetic field; when the inductance value is determined to be minimum according to the target radio frequency magnetic field, the antenna parameters of the nuclear magnetic resonance probe antenna while drilling are determined; the nuclear magnetic resonance while drilling probe antenna is constructed according to the antenna parameters, so that the nuclear magnetic resonance while drilling probe antenna generates an optimal radio frequency magnetic field, the nuclear magnetic resonance while drilling probe can excite a resonance signal according to the optimal radio frequency magnetic field, receive a feedback signal corresponding to the resonance signal, and acquire undisturbed formation information based on the feedback signal. According to the embodiment of the invention, the designed nuclear magnetic resonance probe antenna while drilling can generate the optimal radio frequency magnetic field similar to the theoretical target radio frequency magnetic field in practical application, so that the nuclear magnetic resonance logging instrument while drilling can accurately detect the information of an undisturbed formation.)

1. The method for configuring the nuclear magnetic resonance probe while drilling antenna is characterized by being applied to a nuclear magnetic resonance probe while drilling antenna configuration device, wherein the configuration device is used for controlling the nuclear magnetic resonance probe while drilling antenna mounted on the nuclear magnetic resonance probe while drilling to work so that the nuclear magnetic resonance probe while drilling excites resonance signals according to a radio-frequency magnetic field generated by the nuclear magnetic resonance probe while drilling antenna;

the method comprises the following steps:

acquiring a static magnetic field of a nuclear magnetic resonance probe while drilling, and determining a target radio frequency magnetic field corresponding to the static magnetic field according to the static magnetic field;

when the inductance value is determined to be minimum according to the target radio frequency magnetic field, determining antenna parameters of the nuclear magnetic resonance probe antenna while drilling;

and constructing a while-drilling nuclear magnetic resonance probe antenna according to the antenna parameters so that the while-drilling nuclear magnetic resonance probe antenna generates an optimal radio frequency magnetic field, enabling the while-drilling nuclear magnetic resonance probe to excite a resonance signal according to the optimal radio frequency magnetic field, receiving a feedback signal corresponding to the resonance signal, and acquiring undisturbed formation information based on the feedback signal.

2. The method of claim 1, wherein the determining the antenna parameters of the MWD probe antenna with the minimum inductance value according to the target RF magnetic field comprises:

establishing an inductance function according to a target radio frequency magnetic field, and determining a constraint condition of the inductance function on inductance;

and constraining the inductance function by using the constraint condition, and determining the antenna parameters of the MWD probe antenna when the inductance value of the inductance function is minimum.

3. The method of claim 2, wherein the establishing an inductance function according to the target radio frequency magnetic field and determining the constraint condition of the inductance function on the inductance comprises:

constructing a residual constraint term of current density relative to inductance according to a target radio frequency magnetic field, and establishing an inductance function according to the residual constraint term;

and determining the constraint condition of the inductance function on the inductance.

4. The method of claim 2, wherein the constraining the inductance function with the constraint condition to determine the antenna parameters of the MWD probe antenna when the inductance value of the inductance function is minimum comprises:

according to the constraint conditions, performing partial derivative calculation on the inductance function, and determining the optimal regularization parameter of the inductance function;

and determining antenna parameters of the MWD probe antenna according to the optimal regularization parameters and the inductance function.

5. The method according to claim 4, wherein the performing a partial derivative calculation on the inductance function according to the constraint condition to determine an optimal regularization parameter of the inductance function comprises:

judging whether the partial derivative value of the inductance function is equal to a preset threshold value or not according to a preset initial regularization parameter;

if so, the regularization parameter corresponding to the inductance function is the optimal regularization parameter;

and if not, updating the regularization parameter until the partial derivative value of the inductance function is equal to a preset threshold value.

6. The method of claim 5, wherein updating the regularization parameter if the partial derivative of the inductance function is not equal to a predetermined threshold until the partial derivative of the inductance function is equal to the predetermined threshold comprises:

if the partial derivative value of the inductance function is smaller than a preset threshold value, increasing the regularization parameter until the partial derivative value of the inductance function is equal to the preset threshold value;

and if the partial derivative value of the inductance function is larger than a preset threshold value, reducing the regularization parameter until the partial derivative value of the inductance function is equal to the preset threshold value.

7. The method of claim 4, wherein the determining antenna parameters of the MWD probe antenna according to the optimal regularization parameter and the inductance function comprises:

solving the inductance function according to the optimal regularization parameter to determine current density;

and solving the convection function according to the current density to determine the antenna parameters of the MWD probe antenna.

8. An antenna configuration device for a nuclear magnetic resonance while drilling probe is characterized by comprising:

the acquisition module is used for acquiring a static magnetic field of the nuclear magnetic resonance probe while drilling and determining a target radio frequency magnetic field corresponding to the static magnetic field according to the static magnetic field;

the determining module is used for determining antenna parameters of the nuclear magnetic resonance probe while drilling antenna when the inductance value is minimum according to the target radio frequency magnetic field;

and the execution module is used for constructing the while-drilling nuclear magnetic resonance probe antenna according to the antenna parameters so as to enable the while-drilling nuclear magnetic resonance probe antenna to generate an optimal radio frequency magnetic field, enable the while-drilling nuclear magnetic resonance probe to excite a resonance signal according to the optimal radio frequency magnetic field, receive a feedback signal corresponding to the resonance signal and acquire undisturbed formation information based on the feedback signal.

9. An apparatus for configuring an antenna of a nuclear magnetic resonance while drilling probe, comprising: a memory and at least one processor;

the memory stores computer-executable instructions;

the at least one processor executing the computer-executable instructions stored by the memory causes the at least one processor to perform the method of configuring an MWD probe antenna as recited in any one of claims 1-7.

10. A computer-readable storage medium having computer-executable instructions stored thereon which, when executed by a processor, implement the method of any one of claims 1-7.

Technical Field

The invention relates to the technical field of nuclear magnetic resonance logging, in particular to a method, a device, equipment and a storage medium for configuring a nuclear magnetic resonance probe antenna while drilling.

Background

As oil development continues, oil exploration techniques are also becoming increasingly important. In the field of petroleum exploration, while-drilling nuclear magnetic resonance logging is used as a latest development means of nuclear magnetic resonance logging, and more accurate undisturbed formation information and more reliable oil reservoir evaluation parameters can be provided.

In the prior art, the mainstream design method of a probe antenna of a nuclear magnetic resonance logging while drilling tool is a forward design method, namely, electromagnetic simulation software is applied to carry out optimization simulation on structural parameters of the antenna.

However, the above method depends on subjective experience judgment of a designer, which causes a large difference between a radio frequency magnetic field generated by the designed antenna in practical application and a theoretical target radio frequency magnetic field, and further causes that the while-drilling nuclear magnetic resonance logging instrument cannot accurately detect undisturbed formation information and the like.

Disclosure of Invention

The embodiment of the invention provides a method, a device, equipment and a storage medium for configuring an antenna of a nuclear magnetic resonance while drilling probe, which are used for solving the technical problem that a nuclear magnetic resonance while drilling logging instrument cannot accurately detect original formation information due to the fact that a radio-frequency magnetic field generated by the antenna designed in a forward design method is greatly different from a theoretical target radio-frequency magnetic field.

In a first aspect, an embodiment of the present invention provides a method for configuring a nuclear magnetic resonance while drilling probe antenna, where the method for configuring a nuclear magnetic resonance while drilling probe antenna is applied to a nuclear magnetic resonance while drilling probe antenna configuration device, and the configuration device is configured to control a nuclear magnetic resonance while drilling probe antenna installed on a nuclear magnetic resonance while drilling probe to operate, so that the nuclear magnetic resonance while drilling probe excites a resonance signal according to a radio frequency magnetic field generated by the nuclear magnetic resonance while drilling probe antenna, and the method includes:

acquiring a static magnetic field of a nuclear magnetic resonance probe while drilling, and determining a target radio frequency magnetic field corresponding to the static magnetic field according to the static magnetic field;

when the inductance value is determined to be minimum according to the target radio frequency magnetic field, determining antenna parameters of the nuclear magnetic resonance probe antenna while drilling;

and constructing a while-drilling nuclear magnetic resonance probe antenna according to the antenna parameters so that the while-drilling nuclear magnetic resonance probe antenna generates an optimal radio frequency magnetic field, enabling the while-drilling nuclear magnetic resonance probe to excite a resonance signal according to the optimal radio frequency magnetic field, receiving a feedback signal corresponding to the resonance signal, and acquiring undisturbed formation information based on the feedback signal.

In a possible implementation manner, when the inductance value is determined to be minimum according to the target radio frequency magnetic field, the antenna parameters of the nuclear magnetic resonance while drilling probe antenna comprise:

establishing an inductance function according to a target radio frequency magnetic field, and determining a constraint condition of the inductance function on inductance;

and constraining the inductance function by using the constraint condition, and determining the antenna parameters of the MWD probe antenna when the inductance value of the inductance function is minimum.

In a possible implementation, the establishing an inductance function according to a target radio frequency magnetic field and determining a constraint condition of the inductance function on the inductance includes:

constructing a residual constraint term of current density relative to inductance according to a target radio frequency magnetic field, and establishing an inductance function according to the residual constraint term;

and determining the constraint condition of the inductance function on the inductance.

In a possible embodiment, the constraining the inductance function by using the constraint condition to determine the antenna parameters of the mri probe antenna when the inductance value of the inductance function is minimum includes:

according to the constraint conditions, performing partial derivative calculation on the inductance function, and determining the optimal regularization parameter of the inductance function;

and determining antenna parameters of the MWD probe antenna according to the optimal regularization parameters and the inductance function.

In a possible implementation manner, the performing a partial derivative calculation on the inductance function according to the constraint condition to determine an optimal regularization parameter of the inductance function includes:

judging whether the partial derivative value of the inductance function is equal to a preset threshold value or not according to a preset initial regularization parameter;

if so, the regularization parameter corresponding to the inductance function is the optimal regularization parameter;

and if not, updating the regularization parameter until the partial derivative value of the inductance function is equal to a preset threshold value.

In a possible implementation, if the partial derivative value of the inductance function is not equal to the preset threshold, updating the regularization parameter until the partial derivative value of the inductance function is equal to the preset threshold includes:

if the partial derivative value of the inductance function is smaller than a preset threshold value, increasing the regularization parameter until the partial derivative value of the inductance function is equal to the preset threshold value;

and if the partial derivative value of the inductance function is larger than a preset threshold value, reducing the regularization parameter until the partial derivative value of the inductance function is equal to the preset threshold value.

In a possible implementation manner, the determining, according to the optimal regularization parameter and the inductance function, an antenna parameter of the mri probe antenna includes:

solving the inductance function according to the optimal regularization parameter to determine current density;

and solving the convection function according to the current density to determine the antenna parameters of the MWD probe antenna.

In a second aspect, an embodiment of the present invention provides an apparatus for configuring an antenna of a nuclear magnetic resonance while drilling probe, including:

the acquisition module is used for acquiring a static magnetic field of the nuclear magnetic resonance probe while drilling and determining a target radio frequency magnetic field corresponding to the static magnetic field according to the static magnetic field;

the determining module is used for determining antenna parameters of the nuclear magnetic resonance probe while drilling antenna when the inductance value is minimum according to the target radio frequency magnetic field;

and the execution module is used for constructing the while-drilling nuclear magnetic resonance probe antenna according to the antenna parameters so as to enable the while-drilling nuclear magnetic resonance probe antenna to generate an optimal radio frequency magnetic field, enable the while-drilling nuclear magnetic resonance probe to excite a resonance signal according to the optimal radio frequency magnetic field, receive a feedback signal corresponding to the resonance signal and acquire undisturbed formation information based on the feedback signal.

In a third aspect, an embodiment of the present invention provides a device for configuring an antenna of a nuclear magnetic resonance while drilling probe, including: a memory and at least one processor;

the memory stores computer-executable instructions;

the at least one processor executing the computer-executable instructions stored by the memory causes the at least one processor to perform the method for configuring an antenna of a nuclear magnetic resonance while drilling probe according to any one of the first aspect.

In a fourth aspect, the present invention provides a computer-readable storage medium, in which computer-executable instructions are stored, and when a processor executes the computer-executable instructions, the method according to any one of the first aspect is implemented.

According to the configuration method, device, equipment and storage medium of the nuclear magnetic resonance while drilling probe antenna provided by the embodiment of the invention, the nuclear magnetic resonance while drilling probe antenna can generate the optimal radio frequency magnetic field similar to the theoretical target radio frequency magnetic field in practical application by acquiring the static magnetic field of the nuclear magnetic resonance while drilling probe and determining the target radio frequency magnetic field corresponding to the static magnetic field, determining the antenna parameters of the nuclear magnetic resonance while drilling probe antenna when the inductance value is minimum according to the target radio frequency magnetic field and constructing the nuclear magnetic resonance while drilling probe antenna according to the antenna parameters, so that the nuclear magnetic resonance while drilling logging instrument can accurately detect the information of the original stratum.

Drawings

In order to more clearly illustrate the embodiments of the present invention or the technical solutions in the prior art, the drawings needed to be used in the description of the embodiments or the prior art will be briefly introduced below, and it is obvious that the drawings in the following description are some embodiments of the present invention, and for those skilled in the art, other drawings can be obtained according to these drawings without creative efforts.

Fig. 1 is a schematic view of an application scenario provided in an embodiment of the present invention;

FIG. 2 is a schematic flow chart of a method for configuring an antenna of a nuclear magnetic resonance while drilling probe according to an embodiment of the present invention;

FIG. 3 is a schematic diagram of static magnetic field data provided by an embodiment of the present invention;

FIG. 4 is a schematic flow chart illustrating another method for configuring an antenna of an LWD nuclear magnetic resonance probe according to an embodiment of the present invention;

FIG. 5 is a schematic structural diagram of an antenna equivalent model of a nuclear magnetic resonance while drilling probe antenna according to an embodiment of the present invention;

fig. 6 is a schematic structural diagram of an antenna configuration device of a nuclear magnetic resonance while drilling probe according to an embodiment of the present invention;

fig. 7 is a schematic structural diagram of an mri probe antenna configuration device according to an embodiment of the present invention.

Detailed Description

In order to make the objects, technical solutions and advantages of the embodiments of the present invention clearer, the technical solutions in the embodiments of the present invention will be clearly and completely described below with reference to the drawings in the embodiments of the present invention, and it is obvious that the described embodiments are some, but not all, embodiments of the present invention. All other embodiments, which can be derived by a person skilled in the art from the embodiments given herein without making any creative effort, shall fall within the protection scope of the present invention.

In the field of oil exploration, compared with cable nuclear magnetic resonance logging, while-drilling nuclear magnetic resonance logging is used as a latest development means of nuclear magnetic resonance logging, more accurate undisturbed formation information such as porosity, saturation, permeability and the like and more reliable oil reservoir evaluation parameters such as movable hydrocarbon content and the like can be provided. The good detection characteristic and the signal-to-noise ratio have great significance compared with the nuclear magnetic resonance logging while drilling.

At present, the mainstream design method of the nuclear magnetic resonance probe antenna while drilling is a forward design method, namely, electromagnetic simulation software is used for optimizing and simulating the structural parameters of the antenna, but the method depends on subjective experience judgment of designers, so that a radio frequency magnetic field generated by the designed antenna in practical application is greatly different from a theoretical target radio frequency magnetic field, and the nuclear magnetic resonance logging instrument while drilling cannot accurately detect original formation information and the like.

In order to solve the above problems, in this embodiment, a reverse design method is adopted to design and configure the nuclear magnetic resonance while drilling probe antenna, that is, the antenna parameters of the nuclear magnetic resonance while drilling probe antenna are determined according to the target radio frequency magnetic field, so as to construct the nuclear magnetic resonance while drilling probe antenna. The method comprises the steps of determining a target radio-frequency magnetic field corresponding to the acquired static magnetic field of the while-drilling nuclear magnetic resonance probe, determining antenna parameters of the while-drilling nuclear magnetic resonance probe antenna when the inductance value is minimum according to the target radio-frequency magnetic field, and constructing the while-drilling nuclear magnetic resonance probe antenna according to the antenna parameters, so that the obtained while-drilling nuclear magnetic resonance probe antenna can generate an optimal radio-frequency magnetic field similar to the theoretical target radio-frequency magnetic field in practical application, resonance signals excited by the while-drilling nuclear magnetic resonance probe can be maximized, and the while-drilling nuclear magnetic resonance logging instrument can accurately detect undisturbed formation information.

Fig. 1 is a schematic view of an application scenario provided in an embodiment of the present invention. As shown in fig. 1, the mri probe antenna configuration device acquires data related to the mri probe on the mri logging tool, performs correlation operation processing according to the data, and controls the operation of the mri probe antenna installed on the mri probe.

Fig. 2 is a schematic flow chart of a method for configuring an antenna of a nuclear magnetic resonance while drilling probe according to an embodiment of the present invention. The execution main body of the method in the embodiment of the invention can be equipment configured for the nuclear magnetic resonance probe while drilling antenna. As shown in fig. 2, the method in this embodiment may include:

step 201, collecting a static magnetic field of a nuclear magnetic resonance probe while drilling, and determining a target radio frequency magnetic field corresponding to the static magnetic field according to the static magnetic field.

In this embodiment, the static magnetic field of the nuclear magnetic resonance while drilling probe is a magnetic field generated by the permanent magnet of the probe, and the target radio frequency magnetic field is an ideal radio frequency magnetic field to be generated by the nuclear magnetic resonance while drilling probe antenna in theory, and the target radio frequency magnetic field theoretically matches with the static magnetic field generated by the permanent magnet of the probe to generate the largest resonance signal. The static magnetic field of the nuclear magnetic resonance while drilling probe can be acquired by a gauss meter.

Optionally, the step of determining the target radio-frequency magnetic field corresponding to the static magnetic field according to the static magnetic field may be specifically performed by selecting the static magnetic field on a certain plane of the central axis of the logging tool, and determining the target radio-frequency magnetic field corresponding to the static magnetic field based on a target field method according to a nuclear magnetic resonance condition and the like.

FIG. 3 is a schematic diagram of static magnetic field data provided by an embodiment of the present invention. As shown in fig. 3, the abscissa represents the radial distance of the target point from the center axis of the logging while drilling nuclear magnetic resonance tool, and the ordinate represents the static magnetic field intensity, which represents the intensity distribution of the static magnetic field in the radial direction of the center axis of the logging while drilling nuclear magnetic resonance tool. The target point is a point discretely selected according to different distances on a certain ray radiated outwards along the central axis of the logging-while-drilling nuclear magnetic resonance logger in a static magnetic field on a certain plane of the central axis of the logging-while-drilling nuclear magnetic resonance logger.

Specifically, target radio frequency magnetic field data corresponding to the static magnetic field data is determined based on a target field method according to nuclear magnetic resonance conditions, and a target radio frequency magnetic field is determined. The target radio frequency magnetic field can be expressed as a vector, the vector corresponds to the static magnetic field, and the dimension of the vector is the number of the target radio frequency magnetic field data. The nuclear magnetic resonance conditions include: the target radio frequency magnetic field frequency is Larmor frequency corresponding to the static magnetic field intensity corresponding to the target radio frequency magnetic field frequency; the target radio frequency magnetic field direction is orthogonal to the static magnetic field direction. The target field method is an analytical algorithm, and the relationship between the magnetic field and the coil can be deduced through the target field method. The target radio-frequency magnetic field data corresponds to the static magnetic field data, and the more the number of the selected static magnetic field data is, that is, the more the selected target points are, the more the number of the corresponding target radio-frequency magnetic field data is, the higher the accuracy of the target radio-frequency magnetic field is, for example, the number of the selected static magnetic field data may be 600, and if the accuracy of the target radio-frequency magnetic field is to be improved, the number of the selected static magnetic field data needs to be increased.

And step 202, determining antenna parameters of the nuclear magnetic resonance probe while drilling antenna when the inductance value is minimum according to the target radio frequency magnetic field.

In this embodiment, inductance is taken as a constraint parameter, the constraint parameter is related to coil energy storage of the antenna, that is, the constraint parameter is a parameter to be considered in the antenna optimization design, and the coil energy storage of the antenna has a positive correlation with inductance, impedance, and the like of the coil, so that it is known that the constraint parameter may be inductance, impedance, and the like. When the inductance value is the minimum, the corresponding antenna parameters are obtained, and the nuclear magnetic resonance while drilling probe antenna constructed according to the antenna parameters can generate the optimal radio frequency magnetic field similar to the theoretical target radio frequency magnetic field.

Further, the preset antenna model structure is a solenoid type structure, and correspondingly, the antenna parameters are variable parameters, which may include a coil line width, a coil pitch, a solenoid diameter, a coil turn number, and the like of the antenna. And calculating and determining antenna parameters according to the antenna equivalent model.

And 203, constructing a while-drilling nuclear magnetic resonance probe antenna according to the antenna parameters so that the while-drilling nuclear magnetic resonance probe antenna generates an optimal radio frequency magnetic field, enabling the while-drilling nuclear magnetic resonance probe to excite a resonance signal according to the optimal radio frequency magnetic field, receiving a feedback signal corresponding to the resonance signal, and acquiring undisturbed formation information based on the feedback signal.

Specifically, the nuclear magnetic resonance probe while drilling antenna configured according to the obtained antenna parameters can generate an optimal radio frequency magnetic field, and the optimal radio frequency magnetic field can be matched with a static magnetic field generated by the nuclear magnetic resonance probe while drilling to excite a resonance signal. The optimal radio frequency magnetic field is a radio frequency magnetic field which is generated by the nuclear magnetic resonance probe while drilling antenna in practical application and is similar to a theoretical target radio frequency magnetic field.

According to the configuration method of the nuclear magnetic resonance while drilling probe antenna, when the inductance value is determined to be the minimum according to the target radio frequency magnetic field, the antenna parameters of the nuclear magnetic resonance while drilling probe antenna are determined, and the nuclear magnetic resonance while drilling probe antenna is constructed according to the antenna parameters, the nuclear magnetic resonance while drilling probe antenna can be designed to generate the optimal radio frequency magnetic field similar to the theoretical target radio frequency magnetic field in practical application, and the nuclear magnetic resonance while drilling logging instrument can accurately detect the undisturbed formation information.

In order to more accurately determine the antenna parameters of the nuclear magnetic resonance probe while drilling antenna when the inductance value is minimum, the embodiment of the invention further determines the antenna parameters of the nuclear magnetic resonance probe while drilling antenna when the inductance value is minimum by introducing an inductance function and performing partial derivative calculation on the inductance function and determining the optimal regularization parameters.

Fig. 4 is a schematic flow chart of another method for configuring an antenna of a nuclear magnetic resonance while drilling probe according to an embodiment of the present invention. As shown in fig. 4, the method in this embodiment may include:

step 401, collecting a static magnetic field of the nuclear magnetic resonance while drilling probe, and determining a target radio frequency magnetic field corresponding to the static magnetic field according to the static magnetic field.

For a specific implementation process and principle of step 401 in this embodiment, reference may be made to the foregoing embodiments, and details are not described herein.

Step 402, constructing a residual constraint term of current density relative to inductance according to a target radio frequency magnetic field, and establishing an inductance function according to the residual constraint term.

Specifically, based on the target field method, a residual constraint term of the current density with respect to the inductance is constructed, that is, the inductance is expressed by the current density, and the inductance function may include the residual constraint term and a regularization term. The residual constraint term is the magnetic field linearity deviation derived from the target field method.

The inductance function calculation formula is as follows:

in the formula, Mc is the RF magnetic field value calculated by current density, B_zFor a set target radio frequency magnetic field, Mc-B_zFor residual, λ is the regularization parameter, W is the positive definite matrix associated with the current density, and c is the fourier coefficient of the current density expansion. The first term of Φ is the residual constraint term, i.e.For residual constraint terms, the second term is a regularization term, i.e.Is a regularization term. The residual constraint term is l₂Norm, regularization term adopts Tikhonov regularization term.

And 403, determining the constraint condition of the inductance function on the inductance.

In this embodiment, the constraint condition of the inductance function on the inductance is that when the inductance value is minimum, the antenna parameters of the nuclear magnetic resonance while drilling probe antenna are determined.

And 404, performing partial derivative calculation on the inductance function according to the constraint condition, and determining the optimal regularization parameter of the inductance function.

Optionally, the step of performing partial derivative calculation on the inductance function according to the constraint condition to determine an optimal regularization parameter of the inductance function may specifically include: judging whether the partial derivative value of the inductance function is equal to a preset threshold value or not according to a preset initial regularization parameter; if so, the regularization parameter corresponding to the inductance function is the optimal regularization parameter; and if not, updating the regularization parameter until the partial derivative value of the inductance function is equal to a preset threshold value.

In this embodiment, when the inductance value is the minimum, the offset calculation may be performed on the inductance function when the corresponding inductance function takes the minimum value, and the optimal regularization parameter of the inductance function is determined when the inductance function takes the minimum value.

Specifically, the value of the regularization parameter is changed, and when the inductance function takes a minimum value or is close to the minimum value, the regularization parameter corresponding to the inductance function is the optimal regularization parameter, that is, when the partial derivative value of the inductance function is 0 or close to 0, the regularization parameter corresponding to the inductance function is the optimal regularization parameter.

The initial regularization parameters may be preset empirically to reduce the number of iterations. The slope formula of the inductance function changing along with the regularization parameter, namely the partial derivative formula of the inductance function to the Fourier coefficient c of the current density expansion is as follows:

further, in the above-mentioned case,the value of (A) is the partial derivative of the inductance function, willIs compared with a preset threshold value, which may be a value greater than 0 and less than 1, for example, the preset threshold value may be 0.1.

If this time is theIf the value of the threshold is equal to the preset threshold, the regularization parameter corresponding to the inductance function at the moment is taken as the optimal regularization parameter.

If this time is theIf the value of (d) is less than the preset threshold, the regularization parameter is increased, for example, the regularization parameter is multiplied by a multiple greater than 1, where the multiple may be the preset threshold divided by the currentTo the value obtained for the next iteration untilIs equal to a preset threshold.

If this time is theIf the value of (d) is greater than the preset threshold, then the current regularization parameter is decreased, for example, the current regularization parameter is multiplied by a multiple less than 1, which may be the preset threshold divided by the current regularization parameterTo the value obtained for the next iteration untilIs equal to a preset threshold.

And 405, solving the inductance function according to the optimal regularization parameter to determine the current density.

Specifically, the optimal regularization parameter is brought into an inductance function, the inductance function is solved, a Fourier coefficient c of a current density expansion is determined, and then a corresponding current density j is determined according to the Fourier coefficient c of the current density expansion.

The current density j is calculated by the formula:

wherein j is_θ(theta ', z') represents the component of the current density j in the angular direction theta, j_z(θ ', z') represents a component of the current density j in the axial direction z, m, n represent the number of fourier series terms, L represents the height of the coil, and a represents the radius of the cylindrical surface on which the current density j is distributed.

And 406, solving the current function according to the current density, and determining the antenna parameters of the MWD probe antenna.

The direct solution of the current density j is complex, and in order to simplify the calculation process, a current function is introduced and is solved according to the current density j, wherein the current density j is a vector and the current function is a scalar.

The current density j versus the flow function Ψ (θ ', z') can be expressed as:

wherein e is_rIndicating the direction of the vector potential, r' is the position vector from the origin to the corresponding current density location. From equation (5), the component of the current density j in the angular direction θ and the component in the axial direction z can be obtained:

according to the formulas (3) to (7), the formula of the stream function Ψ (θ ', z') is obtained:

solving the flow function Ψ (θ ', z') to obtain a Fourier series expression of the flow function, and further obtaining an isoline path, wherein the isoline path is a winding form of the antenna. And further obtaining an antenna equivalent model, namely an antenna equivalent current loop model, according to the winding form of the antenna, and further calculating according to the antenna equivalent current loop model to obtain antenna parameters.

The above specific implementation manner is the prior art in the field, and the present application does not specifically limit this.

And 407, constructing a while-drilling nuclear magnetic resonance probe antenna according to the antenna parameters so that the while-drilling nuclear magnetic resonance probe antenna generates an optimal radio frequency magnetic field, enabling the while-drilling nuclear magnetic resonance probe to excite a resonance signal according to the optimal radio frequency magnetic field, receiving a feedback signal corresponding to the resonance signal, and acquiring undisturbed formation information based on the feedback signal.

For a specific implementation process and principle of step 407 in this embodiment, reference may be made to the foregoing embodiments, and details are not described herein.

Fig. 5 is a schematic structural diagram of an antenna equivalent model of a nuclear magnetic resonance while drilling probe antenna according to an embodiment of the present invention. The MWD probe antenna is of a solenoid type structure, as shown in FIG. 5, and for convenience of observation and calculation, the solenoid coil form of the MWD probe antenna is equivalent to an independent coil form. The antenna parameters of the MWD nuclear magnetic resonance probe antenna are variable parameters and can comprise coil line width, coil spacing, solenoid diameter, coil turn number and the like, the antenna parameters can be calculated according to an antenna equivalent model, and the distribution position of an antenna coil on a cylindrical surface can be determined according to the antenna parameters, namely the winding position of each turn of antenna is determined.

The method for configuring the MWD probe antenna includes acquiring a static magnetic field of a MWD probe, determining a target radio-frequency magnetic field corresponding to the static magnetic field, constructing a residual constraint term according to a relation between current density and inductance, further establishing an inductance function, determining a constraint condition of the inductance function on the inductance, performing partial derivative calculation on the inductance function according to the constraint condition, determining an optimal regularization parameter of the inductance function based on an iteration method, solving the inductance function according to the optimal regularization parameter, determining current density, solving the flow function according to the current density, determining an antenna parameter of the MWD probe antenna, constructing the MWD probe antenna according to the antenna parameter, designing the MWD probe antenna through a reverse design method, and enabling the designed MWD probe antenna to generate an optimal shot similar to the theoretical target radio-frequency magnetic field in practical application The frequency magnetic field improves the signal-to-noise ratio of the while-drilling nuclear magnetic resonance probe, so that the while-drilling nuclear magnetic resonance logging instrument can accurately detect the information of the undisturbed formation.

Fig. 6 is a schematic structural diagram of an antenna configuration device of a nuclear magnetic resonance while drilling probe according to an embodiment of the present invention. As shown in fig. 6, the apparatus for configuring an antenna of a nuclear magnetic resonance while drilling probe provided in this embodiment may include: an acquisition module 61, a determination module 62 and an execution module 63.

The acquisition module 61 is used for acquiring a static magnetic field of the nuclear magnetic resonance probe while drilling and determining a target radio frequency magnetic field corresponding to the static magnetic field according to the static magnetic field;

the determining module 62 is configured to determine, according to the target radio frequency magnetic field, an antenna parameter of the nuclear magnetic resonance while drilling probe antenna when the inductance value is minimum;

and the execution module 63 is configured to construct a while-drilling nuclear magnetic resonance probe antenna according to the antenna parameters, so that the while-drilling nuclear magnetic resonance probe antenna generates an optimal radio frequency magnetic field, so that the while-drilling nuclear magnetic resonance probe can excite a resonance signal according to the optimal radio frequency magnetic field, receive a feedback signal corresponding to the resonance signal, and acquire undisturbed formation information based on the feedback signal.

In an optional implementation manner, the determining module 62 is specifically configured to:

establishing an inductance function according to a target radio frequency magnetic field, and determining a constraint condition of the inductance function on inductance;

and constraining the inductance function by using the constraint condition, and determining the antenna parameters of the MWD probe antenna when the inductance value of the inductance function is minimum.

In an optional implementation manner, when the determining module 62 establishes an inductance function according to a target radio frequency magnetic field, and determines a constraint condition of the inductance function on the inductance, it is specifically configured to:

constructing a residual constraint term of current density relative to inductance according to a target radio frequency magnetic field, and establishing an inductance function according to the residual constraint term;

and determining the constraint condition of the inductance function on the inductance.

In an optional implementation manner, when the determining module 62 determines the antenna parameter of the mri probe antenna when the inductance function is constrained by using the constraint condition and the inductance value of the inductance function is minimum, specifically:

according to the constraint conditions, performing partial derivative calculation on the inductance function, and determining the optimal regularization parameter of the inductance function;

and determining antenna parameters of the MWD probe antenna according to the optimal regularization parameters and the inductance function.

In an optional implementation manner, when the determining module 62 performs partial derivative calculation on the inductance function according to the constraint condition, and determines the optimal regularization parameter of the inductance function, specifically, the determining module is configured to:

judging whether the partial derivative value of the inductance function is equal to a preset threshold value or not according to a preset initial regularization parameter;

if so, the regularization parameter corresponding to the inductance function is the optimal regularization parameter;

and if not, updating the regularization parameter until the partial derivative value of the inductance function is equal to a preset threshold value.

In an optional implementation manner, when the partial derivative value of the inductance function is not equal to the preset threshold, the determining module 62 updates the regularization parameter until the partial derivative value of the inductance function is equal to the preset threshold, specifically configured to:

if the partial derivative value of the inductance function is smaller than a preset threshold value, increasing the regularization parameter until the partial derivative value of the inductance function is equal to the preset threshold value;

and if the partial derivative value of the inductance function is larger than a preset threshold value, reducing the regularization parameter until the partial derivative value of the inductance function is equal to the preset threshold value.

In an optional implementation manner, when determining the antenna parameter of the mri probe antenna according to the optimal regularization parameter and the inductance function, the determining module 62 is specifically configured to:

solving the inductance function according to the optimal regularization parameter to determine current density;

and solving the convection function according to the current density to determine the antenna parameters of the MWD probe antenna.

The configuration device for the nuclear magnetic resonance probe while drilling antenna provided by the embodiment can execute the technical scheme of the method embodiment, and the implementation principle and the technical effect are similar, and are not described herein again.

Fig. 7 is a schematic structural diagram of an mri probe antenna configuration device according to an embodiment of the present invention. As shown in fig. 7, the apparatus for configuring an antenna of a nuclear magnetic resonance while drilling probe provided in this embodiment includes: a memory 71 and at least one processor 72;

the memory 71 stores computer-executable instructions;

the at least one processor 72 executes computer-executable instructions stored in the memory 71, so that the at least one processor performs the method for configuring an antenna of a nuclear magnetic resonance while drilling probe according to any of the embodiments described above.

Wherein the memory 71 and the processor 72 may be connected by a bus 73.

Specific implementation principles and effects of the while-drilling nuclear magnetic resonance probe antenna configuration device provided in this embodiment may refer to relevant descriptions and effects corresponding to the embodiments shown in fig. 1 to 5, and are not described herein again.

An embodiment of the present invention further provides a computer-readable storage medium, where a computer executing instruction is stored in the computer-readable storage medium, and when a processor executes the computer executing instruction, the method according to any of the above embodiments is implemented.

The computer readable storage medium may be, among others, ROM, Random Access Memory (RAM), CD-ROM, magnetic tape, floppy disk, optical data storage device, and the like.

In the embodiments provided in the present invention, it should be understood that the disclosed apparatus and method may be implemented in other ways. For example, the above-described apparatus embodiments are merely illustrative, and for example, a division of modules is merely a division of logical functions, and an actual implementation may have another division, for example, a plurality of modules or components may be combined or integrated into another system, or some features may be omitted, or not executed. In addition, the shown or discussed mutual coupling or direct coupling or communication connection may be an indirect coupling or communication connection through some interfaces, devices or modules, and may be in an electrical, mechanical or other form.

The storage medium may be implemented by any type or combination of volatile or non-volatile memory devices, such as Static Random Access Memory (SRAM), electrically erasable programmable read-only memory (EEPROM), erasable programmable read-only memory (EPROM), programmable read-only memory (PROM), read-only memory (ROM), magnetic memory, flash memory, magnetic or optical disks. A storage media may be any available media that can be accessed by a general purpose or special purpose computer.

An exemplary storage medium is coupled to the processor such the processor can read information from, and write information to, the storage medium. Of course, the storage medium may also be integral to the processor. The processor and the storage medium may reside in an Application Specific Integrated Circuits (ASIC). Of course, the processor and the storage medium may reside as discrete components in an electronic device or host device.

Finally, it should be noted that: the above embodiments are only used for illustrating the technical solutions of the present application, and not for limiting the same; although the present application has been described in detail with reference to the foregoing embodiments, it should be understood by those of ordinary skill in the art that: the technical solutions described in the foregoing embodiments may still be modified, or some or all of the technical features may be equivalently replaced; and the modifications or the substitutions do not make the essence of the corresponding technical solutions depart from the scope of the technical solutions of the embodiments of the present application.