CN110532639A - Cable intermediate joint contact surface calculation of contact resistance method based on magnetic induction intensity - Google Patents

Cable intermediate joint contact surface calculation of contact resistance method based on magnetic induction intensity Download PDF

Info

Publication number
CN110532639A
CN110532639A CN201910718661.0A CN201910718661A CN110532639A CN 110532639 A CN110532639 A CN 110532639A CN 201910718661 A CN201910718661 A CN 201910718661A CN 110532639 A CN110532639 A CN 110532639A
Authority
CN
China
Prior art keywords
cable core
cable
contact resistance
sections
copper pipe
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
CN201910718661.0A
Other languages
Chinese (zh)
Other versions
CN110532639B (en
Inventor
邱立
张望
陈伟
常鹏
苏攀
江进波
熊奇
曹成
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.)
China Three Gorges University CTGU
Original Assignee
China Three Gorges University CTGU
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 China Three Gorges University CTGU filed Critical China Three Gorges University CTGU
Priority to CN202310496092.6A priority Critical patent/CN116611288A/en
Priority to CN201910718661.0A priority patent/CN110532639B/en
Priority to CN202310502935.9A priority patent/CN116562089A/en
Publication of CN110532639A publication Critical patent/CN110532639A/en
Application granted granted Critical
Publication of CN110532639B publication Critical patent/CN110532639B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01RMEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R27/00Arrangements for measuring resistance, reactance, impedance, or electric characteristics derived therefrom
    • G01R27/02Measuring real or complex resistance, reactance, impedance, or other two-pole characteristics derived therefrom, e.g. time constant
    • G01R27/08Measuring resistance by measuring both voltage and current
    • GPHYSICS
    • G06COMPUTING; CALCULATING OR COUNTING
    • G06FELECTRIC DIGITAL DATA PROCESSING
    • G06F30/00Computer-aided design [CAD]
    • G06F30/20Design optimisation, verification or simulation
    • G06F30/23Design optimisation, verification or simulation using finite element methods [FEM] or finite difference methods [FDM]
    • GPHYSICS
    • G06COMPUTING; CALCULATING OR COUNTING
    • G06FELECTRIC DIGITAL DATA PROCESSING
    • G06F2113/00Details relating to the application field
    • G06F2113/16Cables, cable trees or wire harnesses
    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02ATECHNOLOGIES FOR ADAPTATION TO CLIMATE CHANGE
    • Y02A90/00Technologies having an indirect contribution to adaptation to climate change
    • Y02A90/30Assessment of water resources
    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02EREDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E60/00Enabling technologies; Technologies with a potential or indirect contribution to GHG emissions mitigation

Landscapes

  • Physics & Mathematics (AREA)
  • Engineering & Computer Science (AREA)
  • General Physics & Mathematics (AREA)
  • Theoretical Computer Science (AREA)
  • Computer Hardware Design (AREA)
  • Evolutionary Computation (AREA)
  • Geometry (AREA)
  • General Engineering & Computer Science (AREA)
  • Measurement Of Resistance Or Impedance (AREA)

Abstract

Calculation of contact resistance method of the invention, it chooses the first cable core and the corresponding crimping copper pipe outer surface C point of the second cable core contact surface is magnetic flux density measurement point, measure the all-in resistance Rs of AB sections of cables, construct the equivalent circuit of AB sections of cables, two-dimensional finite element model is established, contact resistance R is finally calculatedj1、Rj2、Rj3.Another calculation of contact resistance method of the invention, first search coil is set at the contact surface of crimping the first cable core of copper pipe inner surface and the second cable core, in crimping copper pipe outer surface, the second search coil is set, apply alternating voltage, the voltage effective value U of record the first search coil output between the end A, the end B1With the voltage effective value U of the second search coil output2;And then contact resistance R is calculatedj1、Rj2、Rj3.Method of the invention can measure, be calculated the contact resistance of each contact surface of cable intermediate joint, convenient for find, analyze cable intermediate joint there are the problem of.

Description

Cable intermediate joint contact surface calculation of contact resistance method based on magnetic induction intensity
Technical field
The invention belongs to power cable fields, and in particular to the cable intermediate joint based on magnetic induction intensity contacts face contact Resistance calculations method.
Background technique
The service life of cable depends primarily on the degree of aging of cable insulation material, and the temperature of cable insulation material is An important factor for influencing its aging speed;Wherein, cable intermediate joint is the region most easily to generate heat in whole cable run again, main It to be influenced by the contact resistance of cable intermediate joint.Therefore, accurately the contact resistance of measurement cable intermediate joint to effectively commenting The service life for estimating cable is significant.However, in the calculating or measurement method of current cable intermediate joint contact resistance, only It is capable of measuring cable intermediate joint overall contact resistance, is unable to measure the contact resistance of each contact surface.Publication No. The Chinese patent " a method of for calculating three-core cable transition joint aluminium hydraulic pressed connecting pipe contact resistance " of CN104635056B is open A kind of method for calculating three-core cable transition joint aluminium hydraulic pressed connecting pipe contact resistance, comprising: 1) take length in 10kV three-core cable Equal two sections are spent, one section includes cable intermediate joint, and one section is cable body;2) using electric drill to the two section of three core electricity taken Same root core wire is punched in cable, and the position of punching is each section of cable ends;3) using up-flow equipment to 10kV three-core cable High current is loaded, then takes two sections of cable cores, two sections of voltages, record current and voltage data using ohmmeter measurement;4) root Two sections of cable core both end voltages are taken according to measurement and by the electric current of cable, calculate aluminium hydraulic pressed connecting pipe and core at cable intermediate joint Between contact resistance.Obviously, the contact resistance that this method obtains is the overall contact resistance of transition joint.Publication No. The Chinese patent " a kind of cable intermediate joint aluminium hydraulic pressed connecting pipe at calculation of contact resistance method " of CN107203688A discloses a kind of electricity Calculation of contact resistance method at cable transition joint aluminium hydraulic pressed connecting pipe, comprising: S1, in conjunction with the regular twisting process of cable core calculates its strand Close outer diameter D 1;After S2, cable core press, conductor circumscribed circle diameter D2 is calculated;S3, assume each layer conductor deformation quantity after crimping It is identical, calculate inscribed circle and circumcircle radial difference dc;S4, the effective contact length for calculating compacted stranded conductor cross section outer layer le;S5, assume that conductor and casing come into full contact with, calculate the real contact area As of transition joint conductor crimping connection;S6, calculating Contact resistance R between cable core and aluminium hydraulic pressed connecting pipej.Similarly, this method can only measure cable intermediate joint overall contact resistance, It is unable to measure the contact resistance of each contact surface.
Summary of the invention
Technical problem of the invention is that the measurement of existing cable intermediate joint, calculation method can only measure in cable indirectly Head overall contact resistance, can not obtain the contact resistance of each contact surface of cable intermediate joint.
Present invention aim to address the above problem, the cable intermediate joint contact face contact based on magnetic induction intensity is provided Resistance calculations method can measure the contact resistance for obtaining each contact surface of cable intermediate joint, and then find, among analysis cable Connector there are the problem of, improve cable safety in operation.
The technical scheme is that the cable intermediate joint contact surface calculation of contact resistance method based on magnetic induction intensity, For measuring, calculating the contact resistance of the AB section cable with transition joint, the first cable core and the second cable core are chosen The corresponding crimping copper pipe outer surface C point of contact surface is magnetic flux density measurement point, is included the following steps,
Step 1: selecting and the length without transition joint of AB sections of cable same sizes is 1 meter of cable core, measure To the cable core resistance R of unit length0
Step 2: the all-in resistance R of AB sections of cables of measurements
Step 3: the geometric parameter of AB sections of cables of measurement, the diameter d including cable core, the length of the first cable core L1, the length L of the second cable core2, the diameter D of copper pipe is crimped, the length of copper pipe and the first cable core intersection is crimped L3, crimp the length L of copper pipe and the second cable core intersection4
Step 4: according to the rated current virtual value I of AB sections of cablesm, being passed through size to AB sections of cables is ImDC current, The magnetic induction density B of crimping copper pipe outer surface C point is measured using gaussmeterm
Step 5: the equivalent circuit of AB sections of cables of building constructs transition joint contact resistance Rj1、Rj2、Rj3With AB sections of cables All-in resistance RsMathematical relationship, wherein Rj1For the contact resistance for docking contact surface of the first cable core and the second cable core, Rj2For the contact resistance of the first cable core and the crimping contact surface for crimping copper pipe, Rj3For the second cable core with crimp copper pipe Crimping contact surface contact resistance;
Step 6: establishing the two-dimensional finite element model of AB sections of cables using finite element software, magnetic induction intensity survey is calculated Measure the magnetic induction density B of pointj, and the electric current I of the electric current Ix by changing cable core and crimping copper pipem-Ix, so that Bj=Bm
Step 7: the contact resistance R of cable intermediate joint contact surface is obtained by calculationj1, the first cable core with crimp copper Contact resistance R at the contact surface of pipej2, the second cable core and the contact resistance R at the contact surface for crimping copper pipej3
In step 5, the all-in resistance R of AB sections of cabless=R1+Rj1*(Rj2+Rj3)/(Rj1+Rj2+Rj3)+R2,Rj2/Rj3=L3/ L4, the conductor resistance R of the first cable core1=R0*L1, the conductor resistance R of the second cable core2=R0*L2
In step 6, the two-dimensional finite element model that AB sections of cables are established using finite element software is included the following steps,
Step 1: according to the axial symmetry of AB sections of cables, establishing the two-dimensional finite element model of AB sections of cables, including the first electricity Cable core, the second cable core, crimping copper pipe, air section;
Step 2: the first cable core, the second cable core, the material properties for crimping copper pipe, the first cable is respectively set Core, the second cable core, crimping copper pipe, air section relative permeability be set as 1, the first cable core, the second cable The conductivity of core is set as the conductivity of cable conductor, and the conductivity for crimping copper pipe is set as copper conductivity, the electricity of air section Conductance is set as 0;
Step 3: the boundary condition of two-dimensional finite element model is set;
Step 3.1: axial symmetry boundary condition is set at the cable axis of two-dimensional finite element model;
Step 3.2: on the boundary that the two-dimensional finite element model boundary setting magnetic induction intensity that magnetic induction intensity is 0 is 0 Condition;
Step 4: the current source that two-dimensional finite element model is arranged is Im, that is, the electric current at the end A, the end B that flow through AB sections of cables is Im, the first cable core is set as I with the Chong Die zone current of crimping copper pipex, the second cable core with crimping copper pipe it is Chong Die Zone current be set as Ix, the electric current for crimping copper pipe is set as Im-Ix
Step 5: enabling Ix=0, starting finite element software calculates the Magnetic Induction Density Distribution of two-dimensional finite element model, record two Tie up the magnetic induction density B of finite element model C pointj0
Step 6: enabling Ix=Im, the Magnetic Induction Density Distribution of starting finite element software calculating two-dimensional finite element model, record two Tie up the magnetic induction density B of finite element model C pointjm
Step 7: changing IxSize, so that Bj=Bm
In the two-dimensional finite element model of AB sections of cables, Bj=BmWhen, electric current Ix=Im*(Bm-Bj0)/(Bjm-Bj0)。
It is described that contact resistance R is calculatedj1、Rj2、Rj3,
Contact resistance
Contact resistance
Contact resistance
Cable intermediate joint contact surface calculation of contact resistance method of the another kind based on magnetic induction intensity of the invention, is crimping First search coil is set at the contact surface of the first cable core of copper pipe inner surface and the second cable core, in crimping copper pipe appearance The second search coil is arranged in face, and contact surface calculation of contact resistance method includes the following steps,
Step 1: selecting and the length without transition joint of AB sections of cable same sizes is 1 meter of cable core, measure To the cable core resistance R of unit length0
Step 2: the geometric parameter of AB sections of cables of measurement, the length L including the first cable core1, the second cable core Length L2, crimp the length L of copper pipe and the first cable core intersection3, crimp copper pipe and the second cable core intersection Length L4
Step 3: the equivalent circuit of AB sections of cables of building constructs transition joint contact resistance Rj1、Rj2、Rj3With AB sections of cables All-in resistance RsMathematical relationship, wherein Rj1For the contact resistance for docking contact surface of the first cable core and the second cable core, Rj2For the contact resistance of the first cable core and the crimping contact surface for crimping copper pipe, Rj3For the second cable core with crimp copper pipe Crimping contact surface contact resistance;
Step 4: applying alternating voltage between end in the end A of AB sections of cables, B, make to form alternating current in AB sections of cables, remember Record the voltage effective value U of the first search coil output1With the voltage effective value U of the second search coil output2
Step 5: each contact surface contact resistance R of cable intermediate joint is obtained by calculationj1,Rj2,Rj3
In step 3, Rs=R1+Rj1*(Rj2+Rj3)/(Rj1+Rj2+Rj3)+R2,Rj2/Rj3=L3/L4;First cable core Conductor resistance R1=R0*L1, the conductor resistance R of the second cable core2=R0*L2
In step 5,
Contact resistance
Contact resistance
Contact resistance
Compared with prior art, the beneficial effects of the invention are as follows can measure, each contact surface of cable intermediate joint is calculated Contact resistance, convenient for find, analyze cable intermediate joint there are the problem of.In addition, choosing connecing for magnetic flux density measurement point Electric shock resistance calculation method, convenient for understanding the Magnetic Induction Density Distribution situation in cable intermediate joint region;Connecing for search coil is set Electric shock resistance calculation method is easily operated, and calculation amount is small, convenient to carry out.
Detailed description of the invention
Present invention will be further explained below with reference to the attached drawings and examples.
Fig. 1 is the structural schematic diagram of the AB section cable with transition joint.
Fig. 2 is the equivalent circuit diagram of the AB section cable with transition joint.
Fig. 3 is the process of the cable intermediate joint contact surface calculation of contact resistance method of the invention based on magnetic induction intensity Figure;
Fig. 4 is the two-dimensional finite element model of AB sections of cables.
Fig. 5 is the structural schematic diagram that the AB section cable of search coil is arranged.
Fig. 6 is another cable intermediate joint contact surface calculation of contact resistance method based on magnetic induction intensity of the invention Flow chart.Description of symbols in figure: the first cable core 1;Second cable core 2;Crimp copper pipe 3;First cable core and The docking contact surface 4 of two cable cores;First cable core and the crimping contact surface 5 for crimping copper pipe;Second cable core and pressure Connect the crimping contact surface 6 of copper pipe;First search coil 7, the second search coil 8, the air section 9. of two-dimensional finite element model
Specific embodiment
Embodiment one
Fig. 1 show the AB section cable with transition joint, wherein 2 specification phase of the first cable core 1 and the second cable core Together.
As shown in figure 3, the cable intermediate joint contact surface calculation of contact resistance method based on magnetic induction intensity, for surveying Amount, the contact resistance for calculating the AB section cable with transition joint choose the docking of the first cable core and the second cable core The corresponding 3 outer surface C point of crimping copper pipe of contact surface 4 is magnetic flux density measurement point, is included the following steps,
Step 1: selecting and the length without transition joint of AB sections of cable same sizes is 1 meter of cable core, measure To the cable core resistance R of unit length0
Step 2: the all-in resistance R of AB sections of cables of measurements
Step 3: the geometric parameter of AB sections of cables of measurement, the diameter d including cable core, the length of the first cable core 1 L1, the length L of the second cable core 22, the diameter D of copper pipe 3 is crimped, the length of copper pipe 3 and 1 intersection of the first cable core is crimped Spend L3, crimp the length L of copper pipe 3 and 2 intersection of the second cable core4
Step 4: according to the rated current virtual value I of AB sections of cablesm, being passed through size to AB sections of cables is ImDC current, The magnetic induction density B of crimping copper pipe outer surface C point is measured using gaussmeterm
Step 5: the equivalent circuit of AB sections of cables of building, as shown in Fig. 2, building transition joint contact resistance Rj1、Rj2、Rj3 With AB sections of cable all-in resistance RsMathematical relationship, wherein Rj1Contact surface 4 is docked for the first cable core and the second cable core Contact resistance, Rj2For the contact resistance of the first cable core and the crimping contact surface 5 for crimping copper pipe, Rj3For the second cable The contact resistance of core and the crimping contact surface 6 for crimping copper pipe;The all-in resistance R of AB sections of cabless=R1+Rj1*(Rj2+Rj3)/(Rj1+Rj2 +Rj3)+R2,Rj2/Rj3=L3/L4, the conductor resistance R of the first cable core 11=R0*L1, the conductor resistance of the second cable core 2 R2=R0*L2
Step 6: establishing the two-dimensional finite element model of AB sections of cables using finite element software, magnetic induction intensity survey is calculated Measure the magnetic induction density B of pointj, and the electric current I of the electric current Ix by changing cable core and crimping copper pipe 3m-Ix, so that Bj=Bm
Step 7: contact resistance R is obtained by calculationj1、Rj2、Rj3
In step 6, the two-dimensional finite element model that AB sections of cables are established using finite element software is included the following steps,
Step 1: according to the axial symmetry of AB sections of cables, the two-dimensional finite element model of AB sections of cables is established, as shown in figure 4, Including the first cable core 1, the second cable core 2, crimping copper pipe 3, air section 9;
Step 2: the first cable core 1, the second cable core 2, the material properties for crimping copper pipe 3, the first electricity is respectively set Cable core 1, the second cable core 2, crimping copper pipe 3, air section 9 relative permeability be set as 1, the first cable core 1, the The conductivity of two cable cores 2 is set as the conductivity of cable conductor, and the conductivity of crimping copper pipe 3 is set as copper conductivity, empty The conductivity in gas region 9 is set as 0;
Step 3: the boundary condition of two-dimensional finite element model is set;
Step 3.1: axial symmetry boundary condition is set at the cable axis of two-dimensional finite element model;
Step 3.2: on the boundary that the two-dimensional finite element model boundary setting magnetic induction intensity that magnetic induction intensity is 0 is 0 Condition;
Step 4: the current source that two-dimensional finite element model is arranged is Im, that is, the electric current at the end A, the end B that flow through AB sections of cables is Im, the first cable core 1 is set as I with the Chong Die zone current of crimping copper pipe 3x, the second cable core 2 with crimp copper pipe 3 The zone current of overlapping is set as Ix, crimping copper pipe 3 electric current be set as Im-Ix
Step 5: enabling Ix=0, starting finite element software calculates the Magnetic Induction Density Distribution of two-dimensional finite element model, record two Tie up the magnetic induction density B of finite element model C pointj0
Step 6: enabling Ix=Im, the Magnetic Induction Density Distribution of starting finite element software calculating two-dimensional finite element model, record two Tie up the magnetic induction density B of finite element model C pointjm
Step 7: changing IxSize, so that Bj=Bm
Bj=BmWhen, electric current Ix=Im*(Bm-Bj0)/(Bjm-Bj0);
In step 7,
Contact resistance
Contact resistance
Contact resistance
Embodiment two
Fig. 5 show the AB section cable of setting search coil, and the first cable core 1 is identical with 2 specification of the second cable core, It crimps 3 the first cable core of inner surface of copper pipe and is provided with the first search coil 7 at contact surface 4 with docking for the second cable core, Crimping 3 outer surface of copper pipe is provided with the second search coil 8.
As shown in fig. 6, the cable intermediate joint contact surface calculation of contact resistance method based on magnetic induction intensity, including it is following Step,
Step 1: selecting and the length without transition joint of AB sections of cable same sizes is 1 meter of cable core, measure To the cable core resistance R of unit length0
Step 2: the geometric parameter of AB sections of cables of measurement, the length L including the first cable core 11, the second cable core 2 Length L2, crimp the length L of copper pipe 3 and 1 intersection of the first cable core3, crimp copper pipe 3 and be overlapped with the second cable core 2 Partial length L4
Step 3: the equivalent circuit of AB sections of cables of building, as shown in Fig. 2, building transition joint contact resistance Rj1、Rj2、Rj3 With AB sections of cable all-in resistance RsMathematical relationship, wherein Rj1Contact surface 4 is docked for the first cable core and the second cable core Contact resistance, Rj2For the contact resistance of the first cable core and the crimping contact surface 5 for crimping copper pipe, Rj3For the second cable The contact resistance of core and the crimping contact surface 6 for crimping copper pipe;
Step 4: applying alternating voltage between end in the end A of AB sections of cables, B, make to form alternating current in AB sections of cables, remember Record the voltage effective value U of the first search coil 7 output1With the voltage effective value U of the second search coil 8 output2
Step 5: each contact surface contact resistance R of cable intermediate joint is obtained by calculationj1,Rj2,Rj3
In step 3, Rs=R1+Rj1*(Rj2+Rj3)/(Rj1+Rj2+Rj3)+R2,Rj2/Rj3=L3/L4;First cable core 1 Conductor resistance R1=R0*L1, the conductor resistance R of the second cable core 22=R0*L2
In step 5,
Contact resistance
Contact resistance
Contact resistance

Claims (8)

1. the cable intermediate joint contact surface calculation of contact resistance method based on magnetic induction intensity, in measuring, calculate and having Between connector AB section cable contact resistance, choose the first cable core and the corresponding crimping copper pipe of the second cable core contact surface C point in outer surface is magnetic flux density measurement point, which is characterized in that includes the following steps,
Step 1: selecting and the length without transition joint of AB sections of cable same sizes is 1 meter of cable core, measure and obtain list The cable core resistance R of bit length0
Step 2: the all-in resistance R of AB sections of cables of measurements
Step 3: the geometric parameter of AB sections of cables of measurement, the diameter d including cable core, the length L of the first cable core1, second The length L of cable core2, the diameter D of copper pipe is crimped, the length L of copper pipe and the first cable core intersection is crimped3, crimp copper The length L of pipe and the second cable core intersection4
Step 4: according to the rated current virtual value I of AB sections of cablesm, being passed through size to AB sections of cables is ImDC current, use The magnetic induction density B of gaussmeter measurement crimping copper pipe outer surface C pointm
Step 5: the equivalent circuit of AB sections of cables of building constructs transition joint contact resistance Rj1、Rj2、Rj3It is always electric with AB sections of cables Hinder RsMathematical relationship, wherein Rj1For the contact resistance for docking contact surface of the first cable core and the second cable core, Rj2For The contact resistance of first cable core and the crimping contact surface for crimping copper pipe, Rj3For the second cable core and the crimping for crimping copper pipe The contact resistance of contact surface;
Step 6: establishing the two-dimensional finite element model of AB sections of cables using finite element software, magnetic flux density measurement point is calculated Magnetic induction density Bj, and the electric current I of the electric current Ix by changing cable core and crimping copper pipem-Ix, so that Bj=Bm
Step 7: contact resistance R is obtained by calculationj1、Rj2、Rj3
2. each contact surface calculation of contact resistance method of the cable intermediate joint according to claim 1 based on magnetic-field measurement, It is characterized in that, in step 6, the two-dimensional finite element model that AB sections of cables are established using finite element software, including following step Suddenly,
Step 1: according to the axial symmetry of AB sections of cables, establishing the two-dimensional finite element model of AB sections of cables, including the first cable Core, the second cable core, crimping copper pipe, air section;
Step 2: be respectively set the first cable core, the second cable core, crimp copper pipe material properties, the first cable core, Second cable core, crimping copper pipe, air section relative permeability be set as 1, the first cable core, the second cable core Conductivity is set as the conductivity of cable conductor, and the conductivity for crimping copper pipe is set as copper conductivity, the conductivity of air section It is set as 0;
Step 3: the boundary condition of two-dimensional finite element model is set;
Step 3.1: axial symmetry boundary condition is set at the cable axis of two-dimensional finite element model;
Step 3.2: the boundary condition for being 0 in the two-dimensional finite element model boundary setting magnetic induction intensity that magnetic induction intensity is 0;
Step 4: the current source that two-dimensional finite element model is arranged is Im, that is, the electric current at the end A, the end B that flow through AB sections of cables is Im, the The zone current Chong Die with crimping copper pipe of one cable core is set as Ix, the area Chong Die with crimping copper pipe of the second cable core Domain electric current is set as Ix, the electric current for crimping copper pipe is set as Im-Ix
Step 5: enabling Ix=0, starting finite element software calculates the Magnetic Induction Density Distribution of two-dimensional finite element model, and record two dimension has Limit the magnetic induction density B of meta-model C pointj0
Step 6: enabling Ix=Im, the Magnetic Induction Density Distribution of starting finite element software calculating two-dimensional finite element model, recording two dimension has Limit the magnetic induction density B of meta-model C pointjm
Step 7: changing IxSize, so that Bj=Bm
3. each contact surface calculation of contact resistance method of the cable intermediate joint according to claim 2 based on magnetic-field measurement, It is characterized in that, the all-in resistance R of AB sections of cabless=R1+Rj1*(Rj2+Rj3)/(Rj1+Rj2+Rj3)+R2,Rj2/Rj3=L3/L4, first The conductor resistance R of cable core1=R0*L1, the conductor resistance R of the second cable core2=R0*L2
4. each contact surface calculation of contact resistance method of the cable intermediate joint according to claim 2 based on magnetic-field measurement, It is characterized in that, in step 7, Bj=BmWhen, electric current Ix=Im*(Bm-Bj0)/(Bjm-Bj0)。
5. each contact surface calculation of contact resistance method of the cable intermediate joint according to claim 3 based on magnetic-field measurement, It is characterized in that, described be calculated contact resistance Rj1、Rj2、Rj3,
Contact resistance
Contact resistance
Contact resistance
6. the cable intermediate joint contact surface calculation of contact resistance method based on magnetic induction intensity, which is characterized in that in crimping copper First search coil is set at the contact surface of the first cable core of pipe internal surface and the second cable core, in crimping copper pipe outer surface Second search coil is set, contact surface calculation of contact resistance method includes the following steps,
Step 1: selecting and the length without transition joint of AB sections of cable same sizes is 1 meter of cable core, measure and obtain list The cable core resistance R of bit length0
Step 2: the geometric parameter of AB sections of cables of measurement, the length L including the first cable core1, the length of the second cable core L2, crimp the length L of copper pipe and the first cable core intersection3, crimp the length of copper pipe and the second cable core intersection L4
Step 3: the equivalent circuit of AB sections of cables of building constructs transition joint contact resistance Rj1、Rj2、Rj3It is always electric with AB sections of cables Hinder RsMathematical relationship, wherein Rj1For the contact resistance for docking contact surface of the first cable core and the second cable core, Rj2For The contact resistance of first cable core and the crimping contact surface for crimping copper pipe, Rj3For the second cable core and the crimping for crimping copper pipe The contact resistance of contact surface;
Step 4: apply alternating voltage between end in the end A of AB sections of cables, B, makes to form alternating current in AB sections of cables, record the The voltage effective value U of one search coil output1With the voltage effective value U of the second search coil output2
Step 5: each contact surface contact resistance R of cable intermediate joint is obtained by calculationj1、Rj2、Rj3
7. each contact surface calculation of contact resistance method of the cable intermediate joint according to claim 6 based on magnetic-field measurement, It is characterized in that, in step 3, Rs=R1+Rj1*(Rj2+Rj3)/(Rj1+Rj2+Rj3)+R2,Rj2/Rj3=L3/L4;First cable core Conductor resistance R1=R0*L1, the conductor resistance R of the second cable core2=R0*L2
8. each contact surface calculation of contact resistance method of the cable intermediate joint according to claim 7 based on magnetic-field measurement, It is characterized in that, in step 5,
Contact resistance
Contact resistance
Contact resistance
CN201910718661.0A 2019-08-05 2019-08-05 Cable intermediate joint contact surface contact resistance calculation method based on magnetic induction intensity Active CN110532639B (en)

Priority Applications (3)

Application Number Priority Date Filing Date Title
CN202310496092.6A CN116611288A (en) 2019-08-05 2019-08-05 Cable contact resistance calculation method based on detection coil
CN201910718661.0A CN110532639B (en) 2019-08-05 2019-08-05 Cable intermediate joint contact surface contact resistance calculation method based on magnetic induction intensity
CN202310502935.9A CN116562089A (en) 2019-08-05 2019-08-05 Cable contact resistance calculation method based on finite element software simulation magnetic induction intensity

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201910718661.0A CN110532639B (en) 2019-08-05 2019-08-05 Cable intermediate joint contact surface contact resistance calculation method based on magnetic induction intensity

Related Child Applications (2)

Application Number Title Priority Date Filing Date
CN202310496092.6A Division CN116611288A (en) 2019-08-05 2019-08-05 Cable contact resistance calculation method based on detection coil
CN202310502935.9A Division CN116562089A (en) 2019-08-05 2019-08-05 Cable contact resistance calculation method based on finite element software simulation magnetic induction intensity

Publications (2)

Publication Number Publication Date
CN110532639A true CN110532639A (en) 2019-12-03
CN110532639B CN110532639B (en) 2023-06-02

Family

ID=68661428

Family Applications (3)

Application Number Title Priority Date Filing Date
CN201910718661.0A Active CN110532639B (en) 2019-08-05 2019-08-05 Cable intermediate joint contact surface contact resistance calculation method based on magnetic induction intensity
CN202310496092.6A Pending CN116611288A (en) 2019-08-05 2019-08-05 Cable contact resistance calculation method based on detection coil
CN202310502935.9A Pending CN116562089A (en) 2019-08-05 2019-08-05 Cable contact resistance calculation method based on finite element software simulation magnetic induction intensity

Family Applications After (2)

Application Number Title Priority Date Filing Date
CN202310496092.6A Pending CN116611288A (en) 2019-08-05 2019-08-05 Cable contact resistance calculation method based on detection coil
CN202310502935.9A Pending CN116562089A (en) 2019-08-05 2019-08-05 Cable contact resistance calculation method based on finite element software simulation magnetic induction intensity

Country Status (1)

Country Link
CN (3) CN110532639B (en)

Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2007163398A (en) * 2005-12-16 2007-06-28 Tokyo Electric Power Co Inc:The Resistance measuring tool and resistance measuring instrument for compression connection tube
JP2009175062A (en) * 2008-01-28 2009-08-06 Furukawa Electric Co Ltd:The Contact resistance measurement method and measurement apparatus of terminal pressure-bonding section
US8588876B1 (en) * 2011-03-10 2013-11-19 The Florida State University Research Foundation, Inc. Electric joint design to be used in electromagnetic coils made with high-temperature superconducting tape, aspected wire, or cable
CN105912813A (en) * 2016-05-04 2016-08-31 苏州华天国科电力科技有限公司 Method for calculating crimping resistance at joint of middle connector of high-voltage single-core cable
CN107609308A (en) * 2017-10-11 2018-01-19 广州供电局有限公司 The measuring method and device of equivalent resistance at cable connector connecting tube

Patent Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2007163398A (en) * 2005-12-16 2007-06-28 Tokyo Electric Power Co Inc:The Resistance measuring tool and resistance measuring instrument for compression connection tube
JP2009175062A (en) * 2008-01-28 2009-08-06 Furukawa Electric Co Ltd:The Contact resistance measurement method and measurement apparatus of terminal pressure-bonding section
US8588876B1 (en) * 2011-03-10 2013-11-19 The Florida State University Research Foundation, Inc. Electric joint design to be used in electromagnetic coils made with high-temperature superconducting tape, aspected wire, or cable
CN105912813A (en) * 2016-05-04 2016-08-31 苏州华天国科电力科技有限公司 Method for calculating crimping resistance at joint of middle connector of high-voltage single-core cable
CN107609308A (en) * 2017-10-11 2018-01-19 广州供电局有限公司 The measuring method and device of equivalent resistance at cable connector connecting tube

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
刘国建等: "基于有限元分析的电缆中间接头电阻研究", 《电力与能源》 *

Also Published As

Publication number Publication date
CN116562089A (en) 2023-08-08
CN116611288A (en) 2023-08-18
CN110532639B (en) 2023-06-02

Similar Documents

Publication Publication Date Title
CN108334695B (en) Finite element setting method based on contact resistance of ground wire and preformed armor rods
Tang et al. Stranded wire with uninsulated strands as a low-cost alternative to litz wire
CN104635056B (en) A kind of method for calculating three-core cable transition joint aluminium hydraulic pressed connecting pipe contact resistance
CN111783344B (en) Method for simulating and analyzing cable defects based on magnetic field distribution characteristics
CN112632828A (en) Transformer finite element modeling method with transposition structure
CN105912813B (en) A kind of calculation method of high voltage single-core cable transition joint junction crimping resistance
CN110532639A (en) Cable intermediate joint contact surface calculation of contact resistance method based on magnetic induction intensity
EP2977994A1 (en) Wire and coil
CN106816291A (en) A kind of distribution transformer for simulating short circuit in winding state
CN206610719U (en) A kind of distribution transformer for simulating short circuit in winding state
JP5489349B2 (en) ELECTRICAL CHARACTERISTICS ANALYSIS METHOD, ELECTRIC CHARACTERISTICS ANALYSIS PROGRAM, AND ELECTRICAL CHARACTERISTICS ANALYZER
CN110896265B (en) Stator duplex winding equivalent air gap modeling method in switched reluctance motor temperature field analysis
CN103162853B (en) A kind of Submersible Motor Stator winding temperature pick-up unit and detection method
CN110781589B (en) Method for detecting overheating fault of lap joint of gas insulated metal closed power transmission line
CN107634433A (en) Aluminum conductor crimping technique based on sensing hot pressing base
CN110456155B (en) Method for measuring contact resistance of each contact surface of cable intermediate joint
Takau et al. Low frequency modelling of induction heaters using series equivalent circuit, transformer equivalent circuit and finite element analysis
CN113468789B (en) Temperature rise simulation method for ground wire-wire clamp assembly under lightning stroke effect
CN107194027A (en) Aluminium hydraulic pressed connecting pipe Heat Transfer Calculation at a kind of cable intermediate joint
CN209513911U (en) Sheet resistance test fixture
Zaika et al. The generalized mathematical model of heat conduction in a complex multi-layered area
CN112949122A (en) Design method of transmission line hardware
Huang et al. Digital twin modeling and temperature field analysis of transformer windings
CN2648754Y (en) Heating and temperature measuring integral electric cable
CN105024250B (en) Adaptor for connecting resistor to cable assembly

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