CN114169246B - Design method of high-performance low-noise magnetic shielding barrel - Google Patents

Design method of high-performance low-noise magnetic shielding barrel Download PDF

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CN114169246B
CN114169246B CN202111518732.6A CN202111518732A CN114169246B CN 114169246 B CN114169246 B CN 114169246B CN 202111518732 A CN202111518732 A CN 202111518732A CN 114169246 B CN114169246 B CN 114169246B
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barrel
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CN114169246A (en
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周向阳
谢晓旋
赵风文
王维乾
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Beihang University
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Abstract

The invention discloses a design method of a high-performance low-noise magnetic shielding barrel, which takes four layers of magnetic shielding barrels as research objects, aims at the problem of simultaneously realizing optimization of magnetic shielding performance and magnetic noise, establishes an optimization scheme of structural parameters of the four layers of magnetic shielding barrels through a constrained multi-parameter particle swarm optimization method, and optimizes the length of the innermost barrel
Figure DDA0003407895540000011
Radius of innermost barrel
Figure DDA0003407895540000012
Thickness t of each layer i Inter-layer axial spacing DL i Inter-layer radial spacing DR i And 12 structural parameters are equal, so that the design effect of high shielding performance and low noise is realized. The invention is based on the particle swarm optimization algorithm, improves the axial shielding factor of the magnetic shielding barrel by one order of magnitude, reduces the magnetic noise by 15 percent, and can be widely applied to the field of weak magnetic measurement to manufacture a weak magnetic environment.

Description

Design method of high-performance low-noise magnetic shielding barrel
Technical Field
The invention relates to a design method of a high-performance low-noise magnetic shielding barrel, which can improve the axial shielding factor of the magnetic shielding barrel by one order of magnitude and reduce the magnetic noise by 15 percent, and belongs to the technical field of magnetic shielding.
Background
The theoretical sensitivity of the atomic spin magnetometer can reach
Figure BDA0003407895520000011
Becomes a research hotspot in the field of weak magnetic measurement and realizes ultrahigh sensitivityThe premise of extremely weak magnetic measurement is that the interference of an external magnetic field and a noise signal is fully isolated, and the measurement is usually realized by adopting a multi-layer magnetic shielding barrel. Because the sensitivity of the atomic spin magnetometer is limited by the background magnetic field noise signal in practical work, it is necessary to develop a high-performance low-noise magnetic shielding barrel.
The performance indexes of the magnetic shielding barrel comprise magnetic shielding factors and magnetic noise, and the structural design of the current magnetic shielding barrel only considers the magnetic shielding factors and ignores the influence of the magnetic noise, so that the designed magnetic shielding barrel cannot achieve the optimal performance.
Disclosure of Invention
The technical problems to be solved by the invention are as follows: the design method of the high-performance low-noise magnetic shielding barrel is used for improving the shielding performance and reducing the magnetic noise.
The technical solution of the invention is as follows: a design method of a high-performance low-noise magnetic shielding barrel comprises the following steps:
(1) Establishing a four-layer magnetic shielding barrel with a cover total radial magnetic shielding factor model:
Figure BDA0003407895520000012
establishing a four-layer magnetic shielding barrel total axial magnetic shielding factor model with a cover:
Figure BDA0003407895520000013
wherein the content of the first and second substances,
Figure BDA0003407895520000014
is the radial magnetic shielding factor of the ith layer of magnetic shielding barrel,
Figure BDA0003407895520000021
the axial shielding factor of the ith layer of magnetic shielding barrel,
Figure BDA0003407895520000022
for the rod-like demagnetization factor of the ith shield layer,
μ i is the permeability of the ith layer of material, f i =1+L i /100D i End cover shielding factor for the ith layer axial shielding factor, D i Is the i-th shielding layer outer diameter, L i Is the i-th shielding layer outer length, t i The thickness of the ith shielding layer (i is more than or equal to 1 and less than or equal to 4).
(2) Establishing a magnetic noise model generated by the innermost magnetic shielding barrel:
Figure BDA0003407895520000023
/>
wherein, mu 0 =4π×10 -7 N/A 2 Is a vacuum magnetic permeability, r 1 =D 1 /2-t 1 K =1.38 × 10 as the innermost inner radius -23 J/K is boltzmann constant, T is kelvin temperature, σ is electrical conductivity of the innermost shielding material, G is a coefficient related to aspect ratio L/D, and when L/D =1, 1.5, 2, G is 0.657, 0.460, 0.438, respectively.
(3) Establishing a total volume model of the four-layer magnetic shielding barrel with the cover:
Figure BDA0003407895520000024
wherein the content of the first and second substances,
Figure BDA0003407895520000025
is the volume of the ith layer of magnetic shielding barrel. d i Is the i-th inner diameter of the shielding layer, l i The length of the ith shielding layer (i is more than or equal to 1 and less than or equal to 4).
(4) Establishing a four-layer magnetic shielding barrel structure model containing all structural parameters influencing magnetic shielding performance and magnetic noise:
Figure BDA0003407895520000026
wherein DL i For the axial spacing between the i-th and i + 1-th shield layers, including DL 1 ,DL 2 ,DL 3 ;DR i For the radial spacing between the ith and (i + 1) th shielding layers, including DR 1 ,DR 2 ,DR 3 ;t i Is the thickness of the ith shielding layer, including t 1 ,t 2 ,t 3 ,t 4
Figure BDA0003407895520000031
Is the average radius of the innermost layer; />
Figure BDA0003407895520000032
Is the average length of the innermost layer. Four-layer magnetic shielding bucket structure capable of being used by>
Figure BDA0003407895520000033
t 1 ,t 2 ,t 3 ,t 4 ,DL 1 ,DL 2 ,DL 3 ,DR 1 ,DR 2 ,DR 3 And determining 12 parameters, wherein i is more than or equal to 1 and less than or equal to 4.
(5) Substituting the structural model of the four-layer magnetic shielding barrel in the step (4) into the total axial magnetic shielding factor model of the four-layer magnetic shielding barrel with the cover in the step (1) to obtain the total axial shielding factor model S ' of the four-layer magnetic shielding barrel with the cover, wherein the total axial shielding factor model S ' comprises 12 structural parameters influencing magnetic shielding performance and magnetic noise ' Atot
Figure BDA0003407895520000034
Substituting the structure model of the four-layer magnetic shielding barrel in the step (4) into the magnetic noise model generated by the innermost magnetic shielding barrel in the step (2) to obtain a magnetic noise model delta B ' of the four-layer magnetic shielding barrel with the cover, wherein the magnetic noise model delta B ' comprises 12 structural parameters influencing the magnetic shielding performance and the magnetic noise ' eddy
Figure BDA0003407895520000035
Substituting the structure model of the four-layer magnetic shielding barrel in the step (4) into the total volume model of the four-layer magnetic shielding barrel with cover in the step (3) to obtain a total volume model V ' of the four-layer magnetic shielding barrel with cover, wherein the total volume model V ' contains 12 structural parameters influencing magnetic shielding performance and magnetic noise ' tot
Figure BDA0003407895520000036
(6) Setting four layers of magnetic shielding barrel initial structure parameters, and calculating total axial shielding factor under the structure parameters
Figure BDA0003407895520000037
Magnetic noise>
Figure BDA0003407895520000038
Total volume->
Figure BDA0003407895520000039
Figure BDA00034078955200000310
Setting 12 structural parameter change intervals affecting the magnetic shielding performance and the magnetic noise in the above (4):
Figure BDA00034078955200000311
(7) Is prepared from S 'in the above (5)' Atot As an optimization target, the method of (6) above
Figure BDA00034078955200000312
As a first constraint condition, the value in (6) is selected>
Figure BDA0003407895520000041
As a second constraint condition, a multi-parameter particle swarm algorithm with constraint is adopted to influence the magnetic shielding performance and the magnetic noise in the step (4)The 12 structural parameters are optimized to obtain the structural parameters of the four-layer magnetic shielding barrel when the axial shielding factor of the four-layer magnetic shielding barrel with the cover is maximum, and the magnetic noise of the four-layer magnetic shielding barrel with the cover is maximum under the structural parameters and is recorded as ^ er>
Figure BDA0003407895520000042
(8) Delta B 'of the above (5)' eddy As an optimization target, the following (6)
Figure BDA0003407895520000043
As a constraint condition one, the value in (6) is selected>
Figure BDA0003407895520000044
And (3) as a constraint condition II, optimizing 12 structural parameters influencing the magnetic shielding performance and the magnetic noise in the step (4) by adopting a multi-parameter particle swarm algorithm with constraint to obtain a four-layer magnetic shielding barrel structural parameter when the magnetic noise of the four-layer magnetic shielding barrel with the cover is minimum, and recording the four-layer magnetic shielding barrel with the cover as the minimum magnetic noise>
Figure BDA0003407895520000045
(9) In the above (7)
Figure BDA0003407895520000046
And (8) above>
Figure BDA0003407895520000047
Forming magnetic noise variation interval
Figure BDA0003407895520000048
Equally divide this section 10 into->
Figure BDA0003407895520000049
Wherein
Figure BDA00034078955200000410
(10) Is prepared from S 'in the above (5)' Atot The optimization objective was to obtain V 'in the above (5)' tot As a constraint one, will
Figure BDA00034078955200000411
Sequentially serving as a constraint condition II, performing 11 sub-optimization on 12 structural parameters influencing the magnetic shielding performance and the magnetic noise in the step (4) by adopting a multi-parameter particle swarm algorithm with constraint to obtain the jth sub-optimized maximum value & ltSUB & gt & lt/SUB & gt & lt/SUB & gt of axial shielding factors of four layers of covered magnetic shielding barrels>
Figure BDA00034078955200000412
The corresponding 4-layer magnetic shielding barrel structure parameters are recorded as follows:
Figure BDA00034078955200000413
substituting the obtained 4-layer magnetic shielding barrel structure parameters into the four-layer magnetic shielding barrel with cover magnetic noise model delta B 'in the step (5)' eddy Solving the magnetic noise corresponding to the jth sub-optimization
Figure BDA00034078955200000414
1≤j≤11。
(11) Sequentially calculating according to 11 sub-optimization results in (10) above
Figure BDA00034078955200000415
Is recorded as Delta S j Successively count->
Figure BDA00034078955200000416
Is recorded as Delta B j J is more than or equal to 1 and less than or equal to 10, and calculating delta S j /ΔδB j Plotting Δ S j /ΔδB j And changing the curve, selecting a maximum point of the curve, wherein 12 structural parameters of the 4 layers of magnetic shielding barrels corresponding to the point are the final optimization result.
Compared with the prior art, the invention has the advantages that:
(1) The invention comprehensively considers two indexes of magnetic shielding factor and magnetic noise in the design process, and calculates through particle swarm with constrained multi-parameterMethod, average length of innermost layer of magnetic shielding barrel
Figure BDA0003407895520000051
Average radius of innermost layer->
Figure BDA0003407895520000052
Thickness t of each layer i Inter-layer axial spacing DL i Inter-layer radial spacing DR i The magnetic noise is effectively reduced while the shielding performance of the magnetic shielding barrel is greatly improved by 12 parameters through optimization design, compared with the magnetic noise before optimization, the axial shielding factor of the optimized magnetic shielding barrel is improved by one order of magnitude, and the magnetic noise is reduced by 15%, so that the design requirements of high shielding performance and low noise can be met simultaneously;
(2) The invention discloses a relation curve of magnetic noise variation and axial magnetic shielding factor variation under different structural parameters in the optimization process of the magnetic shielding barrel, and provides theoretical reference for the optimization design of the magnetic shielding barrel of the atomic spin magnetometer.
Drawings
FIG. 1 is an axial cross-sectional view of a 4-layer magnetic shielding can in accordance with the present invention;
FIG. 2 shows Δ S in the present invention j /ΔδB j Graph is shown.
Detailed Description
The invention is further described with reference to the following figures and detailed description.
As shown in fig. 1, the magnetic shielding barrel designed by the present invention specifically includes the following contents:
(1) Establishing a four-layer magnetic shielding barrel with a cover total radial magnetic shielding factor model:
Figure BDA0003407895520000053
establishing a four-layer magnetic shielding barrel total axial magnetic shielding factor model with a cover:
Figure BDA0003407895520000054
wherein the content of the first and second substances,
Figure BDA0003407895520000055
is the radial magnetic shielding factor of the ith layer of magnetic shielding barrel,
Figure BDA0003407895520000056
the axial shielding factor of the i-th layer magnetic shielding barrel,
Figure BDA0003407895520000057
for the rod-like demagnetization factor of the ith shield layer,
μ i is the permeability of the ith layer of material, f i =1+L i /100D i End cap shielding coefficient of axial shielding factor of i-th layer, D i Is the i-th shield layer outer diameter, L i Is the ith outer shield length, t i Is the ith shield layer thickness.
(2) Establishing a magnetic noise (eddy current noise) model generated by the innermost magnetic shielding barrel:
Figure BDA0003407895520000061
wherein mu 0 =4π×10 -7 N/A 2 Is a vacuum permeability of r 1 =D 1 /2-t 1 K =1.38 × 10 as the innermost inner radius -23 J/K is boltzmann constant, T is kelvin temperature, σ is electrical conductivity of the innermost shielding material, G is a coefficient related to aspect ratio L/D, and when L/D =1, 1.5, 2, G is 0.657, 0.460, 0.438, respectively.
(3) Establishing a total volume model of the four-layer magnetic shielding barrel with the cover:
Figure BDA0003407895520000062
wherein the content of the first and second substances,
Figure BDA0003407895520000063
is the volume of the ith layer of magnetic shielding barrel. d i Is the i-th shield layer inner diameter, l i Is the length in the ith shield layer.
(4) Establishing a four-layer magnetic shielding barrel structure model containing all structural parameters influencing magnetic shielding performance and magnetic noise:
Figure BDA0003407895520000064
wherein DL i For the axial spacing between the i-th and i + 1-th shield layers, including DL 1 ,DL 2 ,DL 3 ;DR i For the radial spacing between the i-th and i + 1-th shielding layers, including DR 1 ,DR 2 ,DR 3 ;t i Is the thickness of the ith shielding layer, including t 1 ,t 2 ,t 3 ,t 4
Figure BDA0003407895520000065
Is the average radius of the innermost layer; />
Figure BDA0003407895520000066
Is the average length of the innermost layer. Four-layer magnetic shielding bucket structure consisting of>
Figure BDA0003407895520000067
t 1 ,t 2 ,t 3 ,t 4 ,DL 1 ,DL 2 ,DL 3 ,DR 1 ,DR 2 ,DR 3 And 12 parameters are determined.
(5) Substituting the structural model of the four-layer magnetic shielding barrel in the step (4) into the total axial magnetic shielding factor model of the four-layer magnetic shielding barrel with the cover in the step (1) to obtain the total axial shielding factor model S 'of the four-layer magnetic shielding barrel with the cover, which contains 12 structural parameters influencing the magnetic shielding performance and the magnetic noise' Atot
Figure BDA0003407895520000071
Substituting the structure model of the four-layer magnetic shielding barrel in the step (4) into the magnetic noise model generated by the innermost magnetic shielding barrel in the step (2) to obtain a magnetic noise (eddy current noise) model delta B 'of the four-layer magnetic shielding barrel with the cover, wherein the model comprises 12 structural parameters influencing the magnetic shielding performance and the magnetic noise' eddy
Figure BDA0003407895520000072
Substituting the structural model of the four-layer magnetic shielding barrel in the step (4) into the total volume model of the four-layer magnetic shielding barrel with the cover in the step (3) to obtain a total volume model V ' of the four-layer magnetic shielding barrel with the cover, wherein the total volume model V ' contains 12 structural parameters influencing magnetic shielding performance and magnetic noise ' tot
Figure BDA0003407895520000073
/>
(6) Setting four layers of magnetic shielding barrel initial structure parameters, and calculating total axial shielding factor under the structure parameters
Figure BDA0003407895520000074
Figure BDA0003407895520000075
12 structural parameters (including the average length of the innermost layer) affecting the magnetic shield performance and the magnetic noise in the above (4) were set
Figure BDA0003407895520000076
Average radius of innermost layer->
Figure BDA0003407895520000077
Thickness t of each layer i Inter-layer axial spacing DL i Inter-layer radial spacing DR i ) The variation interval:
Figure BDA0003407895520000078
(7) Is prepared from S 'in the above (5)' Atot As an optimization target, the method of (6) above
Figure BDA0003407895520000079
As a first constraint condition, the value in (6) is selected>
Figure BDA00034078955200000710
And (3) as a constraint condition II, optimizing 12 structural parameters influencing the magnetic shielding performance and the magnetic noise in the step (4) by adopting a multi-parameter particle swarm algorithm with constraint to obtain the structural parameters of the four-layer magnetic shielding barrel when the axial shielding factor of the four-layer magnetic shielding barrel with the cover is maximum, and marking the structural parameters as the maximum magnetic noise of the four-layer magnetic shielding barrel with the cover under the structural parameters>
Figure BDA00034078955200000711
(8) Delta B 'of the above (5)' eddy As an optimization target, the method of (6) above
Figure BDA00034078955200000712
As a constraint condition one, the value in (6) is selected>
Figure BDA0003407895520000081
And (3) as a constraint condition II, optimizing 12 structural parameters influencing the magnetic shielding performance and the magnetic noise in the step (4) by adopting a multi-parameter particle swarm algorithm with constraint to obtain a four-layer magnetic shielding barrel structural parameter when the magnetic noise of the four-layer magnetic shielding barrel with the cover is minimum, and recording the four-layer magnetic shielding barrel with the cover as the minimum magnetic noise>
Figure BDA0003407895520000082
(9) In the above (7)
Figure BDA0003407895520000083
And (8) above>
Figure BDA0003407895520000084
Forming magnetic noise variation interval
Figure BDA0003407895520000085
Equally divide the interval 10 into->
Figure BDA0003407895520000086
Wherein
Figure BDA0003407895520000087
(10) Is prepared from S 'in the above (5)' Atot The optimization objective was V 'in the above item (5)' tot As a constraint one, will
Figure BDA0003407895520000088
Sequentially serving as constraint conditions II, carrying out 11 sub-optimization on 12 structural parameters influencing the magnetic shielding performance and the magnetic noise in the step (4) by adopting a multi-parameter particle swarm algorithm with constraint to obtain the jth sub-optimized maximum value of axial shielding factors of the four-layer magnetic shielding barrel with the cover>
Figure BDA0003407895520000089
The corresponding parameters of the 4-layer magnetic shielding barrel structure are recorded as follows:
Figure BDA00034078955200000810
substituting the obtained 4-layer magnetic shielding barrel structure parameters into the four-layer magnetic shielding barrel with cover magnetic noise model delta B 'in the step (5)' eddy Solving the magnetic noise corresponding to the jth sub-optimization
Figure BDA00034078955200000811
(1≤j≤11)。
(11) Sequentially calculating according to 11 sub-optimization results in (10) above
Figure BDA00034078955200000812
Is recorded as Delta S j Sequentially calculate
Figure BDA00034078955200000813
Is recorded as Delta B j J is more than or equal to 1 and less than or equal to 10, and calculating delta S j /ΔδB j Plotting Δ S j /ΔδB j A curve showing the variation of the axial shielding factor as a function of the variation of the magnetic noise, Δ S j /ΔδB j The larger the value is, the faster the axial shielding factor is increased, the slower the magnetic noise is increased, and the better the optimization effect of the magnetic shielding barrel is. Selecting Δ S j /ΔδB j Maximum point in the curve, this time optimized maximum point was taken at j = 7: delta S 7 /ΔδB 7 =12220, i.e. step (10) 8 th optimization, the corresponding four-layer magnetic shielding barrel structure parameters are:
Figure BDA00034078955200000814
the corresponding axial magnetic shielding is as follows:
Figure BDA00034078955200000815
the magnetic noise is:
Figure BDA00034078955200000816
obtaining the optimized structural parameters of the four-layer magnetic shielding barrel, and finishing the optimization design.
Therefore, the shielding factor of the magnetic shield bucket after optimization is 2.1350 × 10 compared with that of the magnetic shield bucket before optimization 3 Increased to 3.8327 × 10 4 Increased by an order of magnitude, magnetic noise (eddy current noise)
Figure BDA0003407895520000091
Reduced to
Figure BDA0003407895520000092
The reduction is 15%.
As shown in FIG. 2, Δ S plotted according to the invention j /ΔδB j Graph with ordinate of total axial screenShading factor variation Δ S j And magnetic noise variation amount delta B j The abscissa is the total axial shielding factor and the magnetic noise change times, the curve reveals the relationship between the axial total shielding factor variation and the magnetic noise variation in the optimization process, and Delta S in the curve j /ΔδB j The larger the value is, the faster the axial shielding factor is increased, the slower the magnetic noise is increased, the better the optimization effect of the magnetic shielding barrel is, and Delta S is selected in the design j /ΔδB j And taking the four-layer magnetic shielding barrel structure corresponding to the maximum point as a final optimization result. The maximum point of this optimization is obtained at j = 7: delta S 7 /ΔδB 7 =12220, i.e. step (10) 8 th optimization, the corresponding four-layer magnetic shielding barrel structure parameters are:
Figure BDA0003407895520000093
the corresponding axial magnetic shielding is as follows:
Figure BDA0003407895520000094
the magnetic noise is:
Figure BDA0003407895520000095
ΔS j /ΔδB j the curve chart reveals the relationship between the magnetic noise variation and the axial magnetic shielding factor variation under different structural parameters in the optimization process of the magnetic shielding barrel, and provides theoretical reference for the optimization design of the magnetic shielding barrel of the atomic spin magnetometer.
The above description is only of the preferred embodiments of the present invention, and it should be noted that: it will be apparent to those skilled in the art that various modifications and adaptations can be made without departing from the principles of the invention and these are intended to be within the scope of the invention.
Those matters not described in detail in the present specification are well known in the art to which the skilled person pertains.

Claims (2)

1. A design method of a high-performance low-noise magnetic shielding barrel is characterized by comprising the following steps:
(1) Establishing a four-layer magnetic shielding barrel with a cover total radial magnetic shielding factor model:
Figure QLYQS_1
establishing a four-layer magnetic shielding barrel total axial magnetic shielding factor model with a cover:
Figure QLYQS_2
wherein the content of the first and second substances,
Figure QLYQS_3
is the radial magnetic shielding factor of the ith layer of magnetic shielding barrel,
Figure QLYQS_4
the axial shielding factor of the ith layer of magnetic shielding barrel,
Figure QLYQS_5
is the rod-like demagnetization factor of the ith shield layer,
μ i permeability of the ith layer material, f i =1+L i /100D i End cap shielding coefficient of axial shielding factor of i-th layer, D i Is the i-th shielding layer outer diameter, L i Is the ith outer shield length, t i Is the thickness of the ith shielding layer;
(2) Establishing a magnetic noise model generated by the innermost magnetic shielding barrel:
Figure QLYQS_6
wherein, mu 0 =4π×10 -7 N/A 2 Is a vacuum permeability of r 1 =D 1 /2-t 1 K =1.38 × 10 as the innermost inner radius -23 J/K is boltzmann constant, T is kelvin temperature, σ is electrical conductivity of the innermost shielding material, G is a coefficient related to aspect ratio L/D, and when L/D =1, 1.5, 2, G is 0.657, 0.460, 0.438, respectively;
(3) Establishing a total volume model of the four-layer magnetic shielding barrel with the cover:
Figure QLYQS_7
wherein the content of the first and second substances,
Figure QLYQS_8
is the volume of the i-th layer magnetic shielding barrel, d i Is the i-th inner diameter of the shielding layer, l i Is the length in the ith shielding layer;
(4) Establishing a four-layer magnetic shielding barrel structure model containing all structural parameters influencing magnetic shielding performance and magnetic noise:
Figure QLYQS_9
/>
wherein, DL i For the axial spacing between the i-th and i + 1-th shield layers, including DL 1 ,DL 2 ,DL 3 ;DR i For the radial spacing between the i-th and i + 1-th shielding layers, including DR 1 ,DR 2 ,DR 3 ;t i Is the thickness of the ith shielding layer, including t 1 ,t 2 ,t 3 ,t 4
Figure QLYQS_10
Is the innermost average radius; />
Figure QLYQS_11
Four-layer magnetic shielding bucket structure with average length of innermost layer>
Figure QLYQS_12
Figure QLYQS_13
t 1 ,t 2 ,t 3 ,t 4 ,DL 1 ,DL 2 ,DL 3 ,DR 1 ,DR 2 ,DR 3 Determining 12 parameters;
(5) Substituting the four-layer magnetic shielding barrel structure model in the step (4) into the four-layer covered magnetic shielding barrel total axial magnetic shielding factor model in the step (1) to obtain a four-layer covered magnetic shielding barrel total axial shielding factor model S 'containing 12 structural parameters influencing magnetic shielding performance and magnetic noise' Atot
Figure QLYQS_14
Substituting the structure model of the four layers of magnetic shielding barrels in the step (4) into the magnetic noise model generated by the innermost layer of magnetic shielding barrel in the step (2) to obtain a magnetic noise model delta B ' of the four layers of magnetic shielding barrels with covers, wherein the magnetic noise model delta B ' comprises 12 structure parameters influencing the magnetic shielding performance and the magnetic noise ' eddy
Figure QLYQS_15
Substituting the four-layer magnetic shielding barrel structure model in the step (4) into the four-layer covered magnetic shielding barrel total volume model in the step (3) to obtain a four-layer covered magnetic shielding barrel total volume model V 'containing 12 structural parameters influencing magnetic shielding performance and magnetic noise' tot
Figure QLYQS_16
(6) Setting four layers of magnetic shielding barrel initial structure parameters, and calculating total axial shielding factor under the structure parameters
Figure QLYQS_17
Setting 12 structural parameter change intervals influencing magnetic shielding performance and magnetic noise in the step (4):
Figure QLYQS_18
(7) By S 'in step (5)' Atot As an optimization target, the step (6) is
Figure QLYQS_19
As a constraint condition one, the step (6)
Figure QLYQS_20
And (3) as a constraint condition II, optimizing 12 structural parameters influencing the magnetic shielding performance and the magnetic noise in the step (4) by adopting a multi-parameter particle swarm algorithm with constraint to obtain the structural parameters of the four-layer magnetic shielding barrel when the axial shielding factor of the four-layer magnetic shielding barrel with the cover is maximum, and marking the structural parameters as the maximum magnetic noise of the four-layer magnetic shielding barrel with the cover under the structural parameters>
Figure QLYQS_21
(8) By delta B 'in step (5)' eddy As an optimization target, the step (6) is
Figure QLYQS_22
As a first constraint, the value in step (6) is->
Figure QLYQS_23
And (5) as a constraint condition II, optimizing 12 structural parameters influencing the magnetic shielding performance and the magnetic noise in the step (4) by adopting a multi-parameter particle swarm algorithm with constraint to obtain a four-layer magnetic shielding barrel structural parameter when the magnetic noise of the four-layer magnetic shielding barrel with cover is minimum, and marking as ^ 12 when the magnetic noise of the four-layer magnetic shielding barrel with cover is minimum under the structural parameter>
Figure QLYQS_24
(9) In step (7)
Figure QLYQS_25
And (8) in>
Figure QLYQS_26
Forming magnetic noise change interval>
Figure QLYQS_27
Equally divide the interval 10 into->
Figure QLYQS_28
Wherein->
Figure QLYQS_29
(10) Is prepared from S 'in step (5)' Atot As an optimization target, V 'in the step (5)' tot As a constraint one, will
Figure QLYQS_30
Sequentially serving as constraint conditions II, wherein j is more than or equal to 1 and less than or equal to 11; carrying out 11 sub-optimization on 12 structural parameters influencing the magnetic shielding performance and the magnetic noise in the step (4) by adopting a multi-parameter particle swarm algorithm with constraint to obtain the maximum value of the axial shielding factor (H) of the jth sub-optimized four-layer covered magnetic shielding barrel>
Figure QLYQS_31
The corresponding parameters of the 4-layer magnetic shielding barrel structure are recorded as follows:
Figure QLYQS_32
substituting the obtained 4-layer magnetic shielding barrel structure parameters into the four-layer magnetic shielding barrel with cover magnetic noise model delta B 'in the step (5)' eddy Solving the magnetic noise corresponding to the jth sub-optimization
Figure QLYQS_33
1≤j≤11;
(11) According to 11 suboptimal results in step (10), calculating in sequence
Figure QLYQS_34
Is recorded as Delta S j Sequentially calculate
Figure QLYQS_35
Is recorded as Delta B j J is more than or equal to 1 and less than or equal to 10, and calculating delta S j /ΔδB j Plotting Δ S j /ΔδB j And changing the curve, selecting a maximum point of the curve, wherein 12 structural parameters of the 4 layers of magnetic shielding barrels corresponding to the point are the final optimization result.
2. The design method of a high-performance low-noise magnetic shielding barrel according to claim 1, characterized in that: the four layers of magnetic shielding barrels are made of permalloy.
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