CN113194704A - Method for protecting working circuit in cavity - Google Patents

Method for protecting working circuit in cavity Download PDF

Info

Publication number
CN113194704A
CN113194704A CN202110509211.8A CN202110509211A CN113194704A CN 113194704 A CN113194704 A CN 113194704A CN 202110509211 A CN202110509211 A CN 202110509211A CN 113194704 A CN113194704 A CN 113194704A
Authority
CN
China
Prior art keywords
cavity
metal strip
resonance
shielding box
rectangular
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
CN202110509211.8A
Other languages
Chinese (zh)
Other versions
CN113194704B (en
Inventor
徐乐
何瑶
李蕊
何帆
杨晓宁
杨勇
李文淼
李西园
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Xidian University
Original Assignee
Xidian University
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Xidian University filed Critical Xidian University
Priority to CN202110509211.8A priority Critical patent/CN113194704B/en
Publication of CN113194704A publication Critical patent/CN113194704A/en
Application granted granted Critical
Publication of CN113194704B publication Critical patent/CN113194704B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Classifications

    • HELECTRICITY
    • H05ELECTRIC TECHNIQUES NOT OTHERWISE PROVIDED FOR
    • H05KPRINTED CIRCUITS; CASINGS OR CONSTRUCTIONAL DETAILS OF ELECTRIC APPARATUS; MANUFACTURE OF ASSEMBLAGES OF ELECTRICAL COMPONENTS
    • H05K9/00Screening of apparatus or components against electric or magnetic fields
    • H05K9/0007Casings
    • H05K9/0049Casings being metallic containers

Abstract

The invention belongs to the technical field of electromagnetic protection, and relates to a method for inhibiting a cavity resonance mode, which is characterized by comprising the following steps: at least comprises the following steps: 1) obtaining the size l multiplied by a multiplied by b of an inner cavity of the rectangular shielding box; wherein l, a and b are the length, width and height of the inner cavity; 2) finding out a resonance point close to the frequency of the working circuit and a resonance point of the rectangular shielding box which has the largest influence on the circuit; 3) designing a corresponding metal frame according to the resonance points obtained in the step 1), and fixing the metal frame at the bottom of the shielding box cover plate through welding to inhibit the resonance points of the resonant cavity; 4) checking whether the box body is assembled properly, finishing properly and improperly, cutting off partial materials of the box body, and returning to the step 4). Aiming at the defect of the shielding efficiency of a rectangular metal shielding box at a resonant frequency point, the method for inhibiting the resonant mode of the cavity is low in cost and convenient to process, so that the circuit working at the resonant frequency point of the cavity can be protected.

Description

Method for protecting working circuit in cavity
Technical Field
The invention belongs to the technical field of electromagnetic protection, and relates to a method for protecting a working circuit in a cavity, which can be used for protecting a circuit working at a special frequency point in a shielding cavity.
Background
The presence of a large number of sensitive electronic components in an electronic device, typically a low noise amplifier, may be disturbed by an external complex electromagnetic environment and may not function properly, or may even be damaged.
In order to protect the circuit, protective measures have to be introduced. Metal with high conductivity (such as aluminum) has good reflection to external electromagnetic waves and low cost enough, so that the metal can be made into a cavity for shielding the electromagnetic waves to protect a circuit. Rectangular metal shield boxes are widely used to protect electrical circuits.
But the rectangle metal shielding box has the gap certainly because of the problem of processing simultaneously, and when the shielding box received electromagnetic pulse irradiation, the electromagnetic wave can get into inside the metal cavity through the gap coupling, forms different resonant modes at specific frequency point, to the electronic components and parts of work at these frequency points, the electromagnetic resonance in the cavity can produce serious interference even, and pure rectangle shielding cavity can't play effectual guard action, probably causes the destruction to the circuit because the resonance electromagnetic environment in the cavity on the contrary.
Disclosure of Invention
Aiming at the defect of the shielding efficiency of the rectangular metal shielding box at the resonant frequency point, the invention provides the method for protecting the working circuit in the cavity, which has low cost and convenient processing, so as to protect the circuit working at the resonant frequency point of the cavity.
The object of the invention is achieved in that a method for protecting a working circuit inside a cavity is characterized in that: at least comprises the following steps:
1) obtaining the size l multiplied by a multiplied by b of an inner cavity of the rectangular shielding box; wherein l, a and b are the length, width and height of the inner cavity;
2) finding out a resonance point close to the frequency of the working circuit and a resonance point of the rectangular shielding box which has the largest influence on the circuit;
3) designing a corresponding metal frame according to the resonance points obtained in the step 1), and fixing the metal frame at the bottom of the shielding box cover plate through welding to inhibit the resonance points of the resonant cavity;
4) checking whether the box body is assembled properly, finishing properly and improperly, cutting off partial materials of the box body, and returning to the step 4).
The length, the width and the height of the inner cavity are l, a and b in the step 1), and the conditions are met (l is more than a and more than b).
The step 2) comprises the following steps:
(1) the top surface of the cavity in the rectangular shielding box is formed by the bottom surface of the box cover, and the top surface of the inner cavity is arranged to be a multiplied by l; a rectangular coordinate system is established by taking a vertex of the bottom surface of the inner cavity as an original point, the axis of the wide edge of the bottom surface is the + x axis, the axis of the high edge of the inner cavity is the + y axis, the axis of the long edge of the bottom surface is the + z axis, and the electric field in the cavity obeys the wave equation:
Figure BDA0003059073720000021
wherein
Figure BDA0003059073720000022
Is the vector of the electric field in the cavity,
Figure BDA0003059073720000023
in order to be the laplacian operator,
Figure BDA0003059073720000024
k is the angular frequency, mu, of the corresponding electric field0Is the magnetic permeability in vacuum, epsilon0Is the dielectric constant in vacuum.
(2) As can be known from the theory of resonant cavity, the electric field longitudinal field component in the resonant cavity is obeyed
Figure BDA0003059073720000025
m, n and p are non-negative integers and are respectively the half period number of the electric field in the length, width and height directions, and at least two positive integers are arranged in the m, n and p, and different m, n and p correspond to different resonance modes;
(3) recording different resonance frequency points as fmnp
Figure BDA0003059073720000031
Wherein c the speed of light: 3X 108m/s, finding the resonance point close to the working circuit frequency, and finding the resonance point with the maximum influence on the circuit, namely min (| f)mnp-f0L) |), take note of f at that timemnpIs FMNP
And 3) designing a corresponding metal frame according to the resonance point, and fixing the metal frame at the bottom of the shielding box cover plate by welding to inhibit the resonance point of the resonant cavity.
The metal frame is composed of two different types of rectangular metal strips, and comprises M strips with length of about l and width of about l
Figure BDA0003059073720000032
The length of the P pieces is about a, and the width of the P pieces is about a
Figure BDA0003059073720000033
The type II metal strip of (1).
The first metal strip is parallel to the long edge of the box cover, and two ends of the first metal strip are aligned with two wide edges of the box cover.
The x coordinate of the geometric center of the straight metal strip is
Figure BDA0003059073720000034
k is a positive odd number; the length of the P roots is about a.
The two-type metal strip is parallel to the wide edge of the box cover, and two ends of the two-type metal strip are aligned with two long edges of the box cover.
Of said two types of metal stripThe z coordinate of the geometric center is
Figure BDA0003059073720000035
k is a positive odd number.
The thickness of the metal strips of the first type metal strip and the second type metal strip is h, the size of the metal strips of the first type metal strip and the second type metal strip can be reasonably selected according to the space allowance in the shielding box, and the two types of metal strips are mutually vertically embedded to jointly form a metal frame with the total thickness of h.
Compared with the shielding box which is used only, the shielding box has the following advantages:
1) the cost is low, and the device has the advantages of low cost,
the material required for improving the shielding effectiveness is metal, and can be metal materials such as aluminum, iron, steel and the like, and the amount of the material required for modification is small.
2) Convenient processing
Only the cover of the shielding box is processed, and the specific resonance mode is restrained by using the space allowance of the shielding box so as to protect the circuit.
Simulation results show that the method improves the shielding effectiveness of frequency points needing to be protected.
Drawings
FIG. 1 is a flow chart of an implementation of the present invention;
fig. 2 is an open cover structure of a rectangular shield case;
FIG. 3 is a general structure of a shield case lid welded with a metal frame;
FIG. 4 shows the rectangular shielding box with the inner cavity size of 90X 30X 160 and the unit of mm, the invention is used for restraining f101Graph comparing the shielding effectiveness at the center of the cavity for the mold and without the present invention;
FIG. 5 shows the rectangular shielding box with the inner cavity size of 90X 30X 160 and the unit of mm, the invention is used for restraining f102Graph comparing the shielding effectiveness at the center of the cavity for the mold and without the use of the present invention.
Detailed Description
Referring to fig. 1 and 2, the specific implementation steps of the present invention are as follows:
step 1: obtaining the size of a cavity in the rectangular shielding body;
assuming that the size l multiplied by a multiplied by b, a, b and l of an inner cavity of the rectangular shielding box is the length, width and height of the inner cavity (l is more than a and more than b), the top surface of the rectangular inner cavity is formed by the bottom surface of the box cover, the top surface of the inner cavity is set to be a multiplied by l, a rectangular coordinate system is established by taking a vertex of the bottom surface of the inner cavity as an origin, the axis of the wide side of the bottom surface is the + x axis, the axis of the high side of the inner cavity is the + y axis, and the axis of the long side of the bottom surface is the + z axis.
Step 2: calculating the frequency f of the circuit to be protected0A proximate cavity resonance point;
setting the frequency f of the circuit to be protected0Calculating the sum f0Close cavity resonance points, different resonance points being denoted fmnpM, n and p are respectively the number of the resonant standing waves in the length, width and height directions, m, n and p are non-negative integers, and at least two positive integers are provided
Figure BDA0003059073720000051
Wherein the speed of light c is 3 × 108m/s, finding a resonance point close to the frequency of the operating circuit, i.e. m, n, p makes | fmnp-f0Minimum, | remember f at this timemnpIs FMNP
And step 3: and designing a corresponding metal frame according to the resonance mode, and welding the metal frame to the bottom of the cover plate of the shielding box.
The metal frame is made up of two different types of rectangular metal strips.
As shown in FIG. 3, M pieces having a length of about l and a width of about l are included
Figure BDA0003059073720000052
The first metal strip is parallel to the long edge of the box cover, two ends of the first metal strip are aligned with two wide edges of the box cover, and the geometric center of the first metal strip isxThe coordinates are
Figure BDA0003059073720000053
The length of the P root is about a, and the width of the P root is about a
Figure BDA0003059073720000054
The second type metal strip is parallel to the wide edge of the box cover, two ends of the second type metal strip are aligned with two long edges of the box cover, and the z coordinate of the geometric center of the second type metal strip is
Figure BDA0003059073720000055
The thickness of the two types of metal strips is h, the size of the two types of metal strips can be reasonably selected according to the space allowance in the shielding box, and the two types of metal strips are vertically embedded to jointly form a metal frame with the total thickness of h.
And 4, step 4: the shielding box after welding the metal frame can be cut off part of materials properly so as to facilitate the assembly of the box body.
The effects of the present invention can be further verified by the following simulation experiments.
Experiment 1, when the internal size of the rectangular shielding box is 90 × 30 × 160 and the unit is mm, the working mode f is suppressed by adopting the invention101I.e., the shielding effectiveness at about 1.9Ghz needs to be improved, the simulated shielding effectiveness is shown in fig. 4. Suppression of f with the invention101After resonance, the shielding effectiveness at 1.9Ghz is improved from-19.8 dB to 24.3 dB.
Experiment 2, when the internal size of the rectangular shielding box is 90 × 30 × 160 and the unit is mm, the working mode f is suppressed by adopting the invention102I.e., the shielding effectiveness at about 2.5Ghz needs to be improved, the simulated shielding effectiveness is shown in fig. 5. Suppression of f with the invention102After resonance, the shielding effectiveness at 2.5Ghz is improved from-21.7 dB to 27.8 dB.
The experiments show that the electromagnetic resonance of the cavity in the shielding box can be obviously inhibited after the shielding box is adopted, and the shielding efficiency is improved.

Claims (10)

1. A method for protecting a working circuit in a cavity is characterized in that: at least comprises the following steps:
1) obtaining the size a multiplied by b multiplied by l of an inner cavity of the rectangular shielding box; wherein, a, b and l are the length, width and height of the inner cavity;
2) finding out a resonance point close to the frequency of the working circuit and a resonance point of the rectangular shielding box which has the largest influence on the circuit;
3) designing a corresponding metal frame according to the resonance points obtained in the step 1), and fixing the metal frame at the bottom of the shielding box cover plate through welding to inhibit the resonance points of the resonant cavity;
4) checking whether the box body is assembled properly, finishing properly and improperly, cutting off partial materials of the box body, and returning to the step 4).
2. The method of claim 1, wherein the method further comprises: the length, the width and the height of the inner cavity body of the step 1) are defined as follows (l is more than a and more than b).
3. The method of claim 1, wherein the method further comprises: the step 2) comprises the following steps:
(1) the top surface of the cavity in the rectangular shielding box is formed by the bottom surface of the box cover, and the top surface of the inner cavity is arranged to be a multiplied by l; a rectangular coordinate system is established by taking a vertex of the bottom surface of the inner cavity as an original point, the axis of the wide edge of the bottom surface is the + x axis, the axis of the high edge of the inner cavity is the + y axis, the axis of the long edge of the bottom surface is the + z axis, and the electric field in the cavity obeys the wave equation:
Figure FDA0003059073710000011
wherein
Figure FDA0003059073710000021
Is the vector of the electric field in the cavity,
Figure FDA0003059073710000022
in order to be the laplacian operator,
Figure FDA0003059073710000023
k is the angular frequency, mu, of the corresponding electric field0Is the magnetic permeability in vacuum, epsilon0Is the dielectric constant in vacuum.
(2) As can be known from the theory of resonant cavity, the electric field longitudinal field component in the resonant cavity is obeyed
Figure FDA0003059073710000024
m, n and p are non-negative integers and are respectively the half period number of the electric field in the length, width and height directions, and at least two positive integers are arranged in the m, n and p, and different m, n and p correspond to different resonance modes;
(1) recording different resonance frequency points as fmnp
Figure FDA0003059073710000025
Wherein c the speed of light: 3X 108m/s, finding the resonance point close to the working circuit frequency, and finding the resonance point with the maximum influence on the circuit, namely min (| f)mnp-f0L) |), take note of f at that timemnpIs FMNP
4. The method of claim 1, wherein the method further comprises: and 3) designing a corresponding metal frame according to the resonance point, and fixing the metal frame at the bottom of the shielding box cover plate by welding to inhibit the resonance point of the resonant cavity.
5. The method of claim 4, wherein the method further comprises the steps of: the metal frame is composed of two different types of rectangular metal strips, and comprises M strips with length of about l and width of about l
Figure FDA0003059073710000026
The length of the P pieces is about a, and the width of the P pieces is about a
Figure FDA0003059073710000027
The type II metal strip of (1).
6. The method of claim 5, wherein the method further comprises: the first metal strip is parallel to the long edge of the box cover, and two ends of the first metal strip are aligned with two wide edges of the box cover.
7. The method of claim 5, wherein the method further comprises: the x coordinate of the geometric center of the straight metal strip is
Figure FDA0003059073710000031
k is a positive odd number.
8. The method of claim 5, wherein the method further comprises: the two-type metal strip is parallel to the wide edge of the box cover, and two ends of the two-type metal strip are aligned with two long edges of the box cover.
9. The method of claim 5, wherein the method further comprises: the z coordinate of the geometric center of the two-type metal strip is
Figure FDA0003059073710000032
k is a positive odd number.
10. The method of claim 5, wherein the method further comprises: the thickness of the metal strips of the first type metal strip and the second type metal strip is h, the size of the metal strips of the first type metal strip and the second type metal strip can be reasonably selected according to the space allowance in the shielding box, and the two types of metal strips are mutually vertically embedded to jointly form a metal frame with the total thickness of h.
CN202110509211.8A 2021-05-10 2021-05-10 Method for protecting working circuit in cavity Active CN113194704B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN202110509211.8A CN113194704B (en) 2021-05-10 2021-05-10 Method for protecting working circuit in cavity

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN202110509211.8A CN113194704B (en) 2021-05-10 2021-05-10 Method for protecting working circuit in cavity

Publications (2)

Publication Number Publication Date
CN113194704A true CN113194704A (en) 2021-07-30
CN113194704B CN113194704B (en) 2022-09-27

Family

ID=76980986

Family Applications (1)

Application Number Title Priority Date Filing Date
CN202110509211.8A Active CN113194704B (en) 2021-05-10 2021-05-10 Method for protecting working circuit in cavity

Country Status (1)

Country Link
CN (1) CN113194704B (en)

Citations (20)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2002196027A (en) * 2000-12-26 2002-07-10 Fukui Prefecture Device for evaluating shielding effect and method for measuring shielding effect
EP1372212A1 (en) * 2002-06-12 2003-12-17 Matsushita Electric Industrial Co., Ltd. Dielectric resonator and high frequency circuit element using the same
JP2012228149A (en) * 2011-04-22 2012-11-15 Yazaki Corp Resonance type non-contact power supply system
CN103308798A (en) * 2013-05-27 2013-09-18 华北电力大学 Method for testing shielding effectiveness of electromagnetic shielding material
US20130313328A1 (en) * 2012-05-25 2013-11-28 Omni-Id Cayman Limited Shielded Cavity Backed Slot Decoupled RFID TAGS
CN104411151A (en) * 2014-12-01 2015-03-11 南京师范大学 Microwave circuit packaging and shielding box based on three-dimensional printing manufacturing technology
CN204408843U (en) * 2014-12-30 2015-06-17 明泰科技股份有限公司 Conducting element is utilized to change the shielding device of resonant resistance and frequency
CN105072836A (en) * 2015-08-18 2015-11-18 西安电子科技大学 Transparent electromagnetic shielding box based on graphene and indium tin oxide films
CN105929240A (en) * 2016-05-04 2016-09-07 南京大学 Resonator apparatus and measurement method for measuring surface intrinsic impedance of high-temperature superconductive film
CN106654539A (en) * 2017-01-18 2017-05-10 华南理工大学 Filtering antenna based on metal integrated structure
CN208093700U (en) * 2017-12-22 2018-11-13 香港凡谷發展有限公司 A kind of structure for promoting TEM all dielectric performance of filter
CN109193088A (en) * 2018-09-17 2019-01-11 电子科技大学 A kind of efficient 220GHz triple-frequency harmonics frequency mixer using single die
CN109581096A (en) * 2018-10-18 2019-04-05 上海无线电设备研究所 Metal shield materials shield effectiveness analysis model and its measurement method under screened room
US20190191599A1 (en) * 2017-04-11 2019-06-20 Murata Manufacturing Co., Ltd. Electromagnetic wave shielding material, building material with electromagnetic wave shield, and article with electromagnetic wave shielding material
WO2020048063A1 (en) * 2018-09-04 2020-03-12 香港凡谷发展有限公司 Cavity high-q three-mode dielectric resonance structure and filter containing resonance structure
CN111259521A (en) * 2020-01-09 2020-06-09 华北电力大学 Equivalent impedance extraction method and system for opening on shielding box with rectangular metal cavity
CN111447817A (en) * 2020-02-10 2020-07-24 天津大学 Method for improving system-level electromagnetic interference
CN111500150A (en) * 2020-05-09 2020-08-07 杨勇华 Molybdenum disulfide-barium ferrite epoxy resin electromagnetic shielding coating and preparation method thereof
EP3698427A1 (en) * 2017-10-18 2020-08-26 Telefonaktiebolaget LM Ericsson (PUBL) A tunable resonance cavity
CN112736496A (en) * 2020-12-22 2021-04-30 北京工业大学 Ultra-wideband phased array radar antenna circuit

Patent Citations (21)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2002196027A (en) * 2000-12-26 2002-07-10 Fukui Prefecture Device for evaluating shielding effect and method for measuring shielding effect
EP1372212A1 (en) * 2002-06-12 2003-12-17 Matsushita Electric Industrial Co., Ltd. Dielectric resonator and high frequency circuit element using the same
JP2012228149A (en) * 2011-04-22 2012-11-15 Yazaki Corp Resonance type non-contact power supply system
US20130313328A1 (en) * 2012-05-25 2013-11-28 Omni-Id Cayman Limited Shielded Cavity Backed Slot Decoupled RFID TAGS
CN103308798A (en) * 2013-05-27 2013-09-18 华北电力大学 Method for testing shielding effectiveness of electromagnetic shielding material
CN104411151A (en) * 2014-12-01 2015-03-11 南京师范大学 Microwave circuit packaging and shielding box based on three-dimensional printing manufacturing technology
CN204408843U (en) * 2014-12-30 2015-06-17 明泰科技股份有限公司 Conducting element is utilized to change the shielding device of resonant resistance and frequency
CN105072836A (en) * 2015-08-18 2015-11-18 西安电子科技大学 Transparent electromagnetic shielding box based on graphene and indium tin oxide films
CN105929240A (en) * 2016-05-04 2016-09-07 南京大学 Resonator apparatus and measurement method for measuring surface intrinsic impedance of high-temperature superconductive film
CN106654539A (en) * 2017-01-18 2017-05-10 华南理工大学 Filtering antenna based on metal integrated structure
CN210610201U (en) * 2017-04-11 2020-05-22 株式会社村田制作所 Electromagnetic wave shield, building material with electromagnetic wave shield, and article with electromagnetic wave shield
US20190191599A1 (en) * 2017-04-11 2019-06-20 Murata Manufacturing Co., Ltd. Electromagnetic wave shielding material, building material with electromagnetic wave shield, and article with electromagnetic wave shielding material
EP3698427A1 (en) * 2017-10-18 2020-08-26 Telefonaktiebolaget LM Ericsson (PUBL) A tunable resonance cavity
CN208093700U (en) * 2017-12-22 2018-11-13 香港凡谷發展有限公司 A kind of structure for promoting TEM all dielectric performance of filter
WO2020048063A1 (en) * 2018-09-04 2020-03-12 香港凡谷发展有限公司 Cavity high-q three-mode dielectric resonance structure and filter containing resonance structure
CN109193088A (en) * 2018-09-17 2019-01-11 电子科技大学 A kind of efficient 220GHz triple-frequency harmonics frequency mixer using single die
CN109581096A (en) * 2018-10-18 2019-04-05 上海无线电设备研究所 Metal shield materials shield effectiveness analysis model and its measurement method under screened room
CN111259521A (en) * 2020-01-09 2020-06-09 华北电力大学 Equivalent impedance extraction method and system for opening on shielding box with rectangular metal cavity
CN111447817A (en) * 2020-02-10 2020-07-24 天津大学 Method for improving system-level electromagnetic interference
CN111500150A (en) * 2020-05-09 2020-08-07 杨勇华 Molybdenum disulfide-barium ferrite epoxy resin electromagnetic shielding coating and preparation method thereof
CN112736496A (en) * 2020-12-22 2021-04-30 北京工业大学 Ultra-wideband phased array radar antenna circuit

Non-Patent Citations (4)

* Cited by examiner, † Cited by third party
Title
汪柳平等: "有孔矩形腔的屏蔽效能及其对谐振抑制研究", 《电波科学学报》 *
潘晓东等: "不完全屏蔽腔体辐射耦合电场增强效应防护方法", 《电波科学学报》 *
芦卓然,徐乐等: "强电磁脉冲辐照单线线缆的SPICE等效电路模型实现", 《微波学报》 *
陈琛: "谐振式无线电能传输系统的若干电磁问题研究及优化设计", 《东南大学》 *

Also Published As

Publication number Publication date
CN113194704B (en) 2022-09-27

Similar Documents

Publication Publication Date Title
TWI672092B (en) Electronic device, method of arranging an electromagnetic interference suppressor and communication device
EP3096594A1 (en) Circuit protection structure and electronic device
CN113194704B (en) Method for protecting working circuit in cavity
EP0342971B1 (en) Electric device
TW201444462A (en) Fixed structure of printed circuit board and shield case
EP1596643B1 (en) EMI gasket
WO2020068268A1 (en) Electromagnetic interference shielding for a circuit board
JPH1187977A (en) Electrical circuit constitution arranged in casing
JPH08316679A (en) Electromagnetic shielding box and electric equipment having this case
Scharstein Mellin transform solution for the static line-source excitation of a dielectric wedge
US9060417B2 (en) Device for attenuating propagation of electromagnetic emissions from an enclosure
CN106535606B (en) Radio frequency shielding device
CN213597826U (en) Radiation-proof electromagnetic shielding door
JP2005072207A (en) Microwave amplifier circuit
Nešić et al. Analysis of hexagonal and square TLM air-vent models against incident plane wave direction
JP2001015975A (en) Leakage electromagnetic wave preventing packing
CN206249197U (en) A kind of multifunctional combination computer
US7847750B2 (en) Antenna device adapted for portable radio apparatus
RU2610515C1 (en) Method to increase noise immunity of vehicles
CN111124059A (en) Computer mainframe with magnetic shielding function
KR100480049B1 (en) Electron wave shelter for wireless communication device
Harberts et al. Quasi-electrostatic shielding of dissipative cylindrical shells
KR100211990B1 (en) Shield device against electromagnetic wave
CN2804954Y (en) Internal connection type card reading unit with prevention of electromagnetic wave interference
CN102458030B (en) A kind of electrostatic shielding body being applicable to image sensor chip

Legal Events

Date Code Title Description
PB01 Publication
PB01 Publication
SE01 Entry into force of request for substantive examination
SE01 Entry into force of request for substantive examination
GR01 Patent grant
GR01 Patent grant