CN107247196A - A kind of multi purpose space charge-measuring system and measuring method - Google Patents

A kind of multi purpose space charge-measuring system and measuring method Download PDF

Info

Publication number
CN107247196A
CN107247196A CN201710552011.4A CN201710552011A CN107247196A CN 107247196 A CN107247196 A CN 107247196A CN 201710552011 A CN201710552011 A CN 201710552011A CN 107247196 A CN107247196 A CN 107247196A
Authority
CN
China
Prior art keywords
measurement
sample
pulse
bottom electrode
charge
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
CN201710552011.4A
Other languages
Chinese (zh)
Other versions
CN107247196B (en
Inventor
郑晓泉
钱雨峰
黎颖
雷伟群
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.)
Xian Jiaotong University
Original Assignee
Xian Jiaotong 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 Xian Jiaotong University filed Critical Xian Jiaotong University
Priority to CN201710552011.4A priority Critical patent/CN107247196B/en
Publication of CN107247196A publication Critical patent/CN107247196A/en
Application granted granted Critical
Publication of CN107247196B publication Critical patent/CN107247196B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01RMEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R29/00Arrangements for measuring or indicating electric quantities not covered by groups G01R19/00 - G01R27/00
    • G01R29/24Arrangements for measuring quantities of charge
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01RMEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R29/00Arrangements for measuring or indicating electric quantities not covered by groups G01R19/00 - G01R27/00
    • G01R29/12Measuring electrostatic fields or voltage-potential
    • G01R29/14Measuring field distribution
    • 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
    • Y02E30/00Energy generation of nuclear origin
    • Y02E30/30Nuclear fission reactors

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Length-Measuring Devices Using Wave Or Particle Radiation (AREA)

Abstract

A kind of multi purpose space charge-measuring system and measuring method, the measuring system includes measurement Top electrode, measure bottom electrode, the pulse generating unit being connected with measurement Top electrode pulse incoming end, the DC high-voltage source being connected with measurement Top electrode high pressure incoming end, sample is arranged between measurement Top electrode and measurement bottom electrode;Measuring bottom electrode includes metal shell, it is arranged on the bottom electrode upper cover plate contacted at the top of metal shell and with sample lower surface, it is arranged on the thin film sensor being close in metal shell and with bottom electrode upper cover plate lower surface, the metal shielding covered on outside thin film sensor, the low-noise amplifier being connected with thin film sensor, the panel connector on metal shell is embedded in, low-noise amplifier is connected with panel connector;The oscillograph being connected by integrating circuit matched line with panel connector;The invention also discloses measuring method;The present invention not only has Conventional spatial charge measurement function, and the plate tensile sample electric charge injection being also equipped with simulation space vacuum high energy electron environment to different-thickness and dissipation law and electric charge, Electric Field Distribution carry out the function of on-line measurement.

Description

A kind of multi purpose space charge-measuring system and measuring method
Technical field
The invention belongs to carry out space charge distribution measurement techniques field in dielectric material using pulse electroacoustic method, and in particular to one Plant multi purpose space charge-measuring system and measuring method.
Background technology
Dielectric directly influences equipment as electric, electronic device key components, its electric, ageing properties Reliability of operation and life-span.Research shows that space charge is a key factor for causing electrostrictive polymer aging, the sky of material Between distribution of charges can intuitively reflect electrostrictive polymer degree of aging, mechanism collapse, trap density and its distribution.Space environment is to causing Its device reliability effect most serious be various energy electronics, electronics is gathered in inside dielectric material or surface can all form height Electrostatic potential, and trigger the pulsed discharge for having a strong impact on electronic system normal work, electronic device is directly resulted in when serious and is punctured Or burn.Distribution of space charge of the dielectric material under high-energy electron irradiation is studied, the operational reliability for ensureing spacecraft It is significant with the life-span.
By 20 years developments, pulse electroacoustic method (PEA) has been widely used in studying hollow electricity of solid dielectric insulation Lotus is distributed.But the general measure space charge system based on pulse electroacoustic method cannot be used for space environmental simulation and carry out electron beam Space charge on-line measurement in the case of irradiation, and applicable size of sample scope is extremely narrow, only below 0.5mm thickness.
The content of the invention
In order to overcome the shortcomings of that above-mentioned prior art is present, it is an object of the invention to provide a kind of multi purpose space electric charge Measuring system and measuring method, the system not only have Conventional spatial charge measurement function, and measurement range is extended into 5mm And following thick sample, and possess the board-like material sample electric charge under simulation space vacuum high energy electron environment to different-thickness Injection and dissipation law and electric charge, Electric Field Distribution carry out the function of on-line measurement.
To reach above-mentioned purpose, the present invention uses following technical scheme:
A kind of multi purpose space charge-measuring system, including measurement Top electrode 1, measure bottom electrode 12, with measurement Top electrode 1 The pulse generating unit 2 of the adjustable pulse parameter of pulse incoming end connection, the direct current being connected with the measurement high pressure incoming end of Top electrode 1 High-voltage power supply 3, sample is arranged between measurement Top electrode 1 and measurement bottom electrode 12;The measurement bottom electrode 12 includes metal shell 8, Be arranged on the top of metal shell 8 and the bottom electrode upper cover plate 4 contact with the lower surface of sample, be arranged on metal shell 8 it is interior and with What the lower surface of bottom electrode upper cover plate 4 was close to changes the thin film sensor 5 of thickness, the metal screen covered on outside thin film sensor 5 Shell 6 is covered, the low-noise amplifier 7 being connected with thin film sensor 5 is embedded in the panel connector 9 on metal shell 8, panel connector 9 In have signal transmission mouth and a plant-grid connection mouthful, be respectively used to spread out of signal that low-noise amplifier 7 amplifies and to low Noise amplifier 7 is powered, and low-noise amplifier 7 is connected with panel connector 9;The product being connected with the signal transmission mouth of panel connector 9 Parallel circuit matched line 10, is connected to the oscillograph 11 of the other end of integrating circuit matched line 10.
The measurement Top electrode 1 is the autonomous patent of invention (patent No. of applicant:The 0359855.X of ZL 2,011 1) in electricity Pole.
The pulse generating unit 2 can adjust the amplitude and pulsewidth of input pulse signal according to sample thickness, while thin Film sensors 5 are by adjusting the thickness of film to adapt to the measurement of different-thickness sample so that whole measuring system is realized to not The plate tensile sample material of stack pile is measured;The pulse amplitude adjustable extent of the pulse generating unit 2 is 0~3600V, arteries and veins Wide adjustable range is 5ns~150ns;The film thickness adjustable range of thin film sensor 5 is 5 μm~100 μm;Measurable examination Sample thickness range is 0.1mm~5mm.
The system under normal atmospheric environment external dc high pressure carry out general measure, applications voltage range for 1kV~ 50kV;The distribution of space charge situation of sample can also be measured in real time under electron irradiation environment simultaneously, electron energy scope is 10keV~10MeV, and the system can carry out experiment measurement in the case of vertical radiation and horizontal radiation.
The measurement Top electrode 1 is fixedly connected with measurement bottom electrode 12 by screw rod with nut.
The integrating circuit matched line 10 is mainly made up of electric capacity and resistance, the distortion for eliminating waveform.
The measuring method of multi purpose space charge-measuring system described above, using pulse radio-acoustic method as general principle, When applying high direct voltage progress general measure under normal atmospheric environment, the source of measurement electric charge is the DC high-voltage source 3 of pressure;Root The selection of pulse parameter and sensor thickness is carried out according to the thickness of measurement sample;The pressure of DC high-voltage source 3 causes quilt in sample The electric charge of certain polarity is injected, the pulse that pulse generating unit 2 is applied can produce phase when by sample internal charge position Answer the ping ripple of polarity;Ping ripple is received and turned by thin film sensor 5 after being transferred through sample and bottom electrode upper cover plate 4 It is changed into electric signal, the electric signal waveform exported afterwards amplifies by low-noise amplifier 7, and integrated Circuit Matching line 10 is carried out Waveform modification, is finally received by oscillograph 11, is afterwards demarcated obtained waveform and denoising to signal data, finally Obtain the distribution of charges and electric-field intensity distribution of sample;
The charge collection principle of sample under electron irradiation environment is directly injected into for electronics, should under electron irradiation environment The measurement of system need not access DC voltage, so not needing DC high-voltage source 3, electricity is directly received using Top electrode 1 is measured Son injection, electrons stay directly forms space charge, the pulse excitation then sent using pulse generating unit 2 inside sample Go out the acoustic signals related to electric charge, acoustic signals are transmitted with sample and bottom electrode upper cover plate 4 for medium, by film-sensing Device 5 receives and is converted into corresponding electric signal;Subsequent electric signal amplifies by low-noise amplifier 7, then integrated circuit Distribution 10 carries out waveform modification, is finally obtained by oscillograph 11, obtained waveform is demarcated and gone to signal data afterwards Make an uproar processing, the final distribution of charges and electric-field intensity distribution for obtaining sample
Compared to the prior art the present invention, has the following advantages that:
1st, advantage of the multi purpose space charge-measuring system of the present invention compared with common space charge measuring system be such as Under:(1) system can apply high direct voltage progress general measure under normal atmospheric environment;(2) measurement sample thickness by 0.1mm once extends to 5mm;(3) can in the environment of electron irradiation on-line measurement space charge.The tune of impressed DC voltage Adjusting range is 1kV~50kV, and the excursion of electron radiation energy energy is 10keV~10MeV.
2nd, pulse generating unit 2 can continuously adjust the amplitude and pulsewidth of input pulse signal according to institute's test specimens thickness, Thin film sensor 5 can adjust the thickness of sensor according to institute test specimens thickness, with needed for obtaining the different plate tensile samples of measurement Measurement sensitivity and resolution ratio.Pulse amplitude continuous tuning range be 0~3600V, pulsewidth continuously adjust scope for 5ns~ 150ns;Piezoelectric transducer thickness adjustable range is 5 μm~100 μm;Measurable sample thickness scope is 0.1mm~5mm.
3rd, the measuring electrode of the measuring system is fixed using the direction being mechanically fixed, and can meet positive or lateral The requirement of experiment of measurement, applicability is more extensive.
4th, it is measurement Top electrode 1 to employ the electrode in the 0359855.X of Patent No. ZL 2,011 1, can be monitored in real time Electric charge injection and the dissipation law of sample are observed, is provided conveniently for the on-line measurement in situ of material space electric charge.The electrode exists Without applying high direct voltage during progress high-energy electron irradiation measurement.It is height to extend through the through hole of Top electrode bottom surface by upper electrode surface Can electron injection to plate tensile sample passage.
5th, whole measuring system includes the insulating materials and overcoat in upper/lower electrode and line, using radiation resistant polymer Material, can not only protect this measuring system, and will not be because organic material deaerates and influences measurement.
Brief description of the drawings
Fig. 1 is the connection diagram of multi purpose space charge-measuring system of the present invention.
Fig. 2 is the measurement result schematic diagram of multi purpose space charge-measuring system of the present invention, wherein:Fig. 2 (a) is general big General measure design sketch under compression ring border, Fig. 2 (b) is the measurement effect figure under electron irradiation environment.
Embodiment
Operation principle of the present invention is described in more detail below in conjunction with the accompanying drawings.
As shown in figure 1, a kind of multi purpose space charge-measuring system of the invention, including measurement Top electrode 1, measure bottom electrode 12, the pulse generating unit 2 for the adjustable pulse parameter being connected with the measurement pulse incoming end of Top electrode 1, with the measurement high pressure of Top electrode 1 The DC high-voltage source 3 of incoming end connection, sample is arranged between measurement Top electrode 1 and measurement bottom electrode 12;The measurement bottom electrode 12 include metal shell 8, are arranged on the top of metal shell 8 and the bottom electrode upper cover plate 4 contacted with the lower surface of sample, are arranged on The thin film sensor 5 for changing thickness being close in metal shell 8 and with the lower surface of bottom electrode upper cover plate 4, covers on film-sensing Metal shielding 6 outside device 5, the low-noise amplifier 7 being connected with thin film sensor 5, is embedded in the panel on metal shell 8 There are a signal transmission mouth and a plant-grid connection mouthful in joint 9, panel connector 9, be respectively used to outflow low-noise amplifier 7 and put Big signal and powered to low-noise amplifier 7, low-noise amplifier 7 is connected with panel connector 9;With the signal of panel connector 9 The integrating circuit matched line 10 of mouth connection is transmitted, the oscillograph 11 of the other end of integrating circuit matched line 10 is connected to.
A kind of measuring method of multi purpose space charge-measuring system of the present invention is:Substantially original is used as using pulse radio-acoustic method Reason, when applying high direct voltage progress general measure under normal atmospheric environment, measures high direct voltage of the source of electric charge for pressure Source 3.The selection of pulse parameter and sensor thickness is carried out according to the thickness of measurement sample.The pressure of DC high-voltage source 3 causes examination The electric charge of certain polarity is injected into sample, the pulse that clock 2 is applied can produce phase when by sample internal charge position Answer the ping ripple of polarity.Ping ripple is received and turned by thin film sensor 5 after being transferred through sample and bottom electrode upper cover plate 4 It is changed into electric signal, the electric signal waveform exported afterwards amplifies by low-noise amplifier 7, and integrated Circuit Matching line 10 is carried out Waveform modification, is finally received by oscillograph 11, is afterwards demarcated obtained waveform and denoising to signal data, finally Obtain the distribution of charges and electric-field intensity distribution of sample.Fig. 2 (a) in general measure effect such as Fig. 2 under normal atmospheric environment It is shown, as can be seen from the figure:The interface charge peak at waveform two ends is one positive one negative heterocharge peak.Due to can basis The situation adjustment pulse of sample and the parameter of sensor, it is ensured that the sensitivity of measurement, so the feature at electric charge peak is bright in waveform It is aobvious, and there is no in the presence of Circuit Matching line serious waveform " overshoot " phenomenon occur.
The charge collection principle of sample under electron irradiation environment is directly injected into for electronics, should under electron irradiation environment The measurement of system need not access DC voltage, so not needing DC high-voltage source 3, upper electricity is measured using the patent independently invented Pole 1 directly receives electron injection, and electrons stay directly forms space charge in material internal, then utilizes pulse generating unit 2 The pulse excitation sent goes out the acoustic signals related to electric charge, and acoustic signals are carried out with sample and bottom electrode upper cover plate 4 for medium Transmission, is received by thin film sensor 5 and is converted into corresponding electric signal.Subsequent electric signal amplifies by low-noise amplifier 7, so Waveform modification is carried out by integrating circuit matched line 10, is finally obtained by oscillograph 11, afterwards by obtained waveform to signal number According to being demarcated and denoising, the final distribution of charges and electric-field intensity distribution for obtaining sample.Figure in measurement effect such as Fig. 2 Shown in 2 (b), the figure is the waveform that on-line measurement is obtained under horizontal radiation environment, as can be seen from the figure:With normal atmospheric environment Lower traditional measurements are different, and the interface charge peak at the waveform two ends that on-line measurement is obtained is the positive charge peak of same polarity.Sample In the corresponding negative electrical charge peak of space charge that is produced because of electron irradiation it is fairly obvious, this is to have selected suitable pulse and thin The result of film sensors parameter.
The principle and embodiment of the present invention are set forth invention applies specific embodiment, above example Illustrate the method and its core concept for being only intended to help to understand the present invention;Simultaneously for those of ordinary skill in the art, according to According to the thought of the present invention, corresponding variation is done in specific embodiments and applications, protection scope of the present invention is belonged to.

Claims (6)

1. a kind of multi purpose space charge-measuring system, it is characterised in that:Including measurement Top electrode (1), bottom electrode (12) is measured, The pulse generating unit (2) for the adjustable pulse parameter being connected with measurement Top electrode (1) pulse incoming end, with measurement Top electrode (1) The DC high-voltage source (3) of high pressure incoming end connection, sample is arranged between measurement Top electrode (1) and measurement bottom electrode (12);It is described Measuring bottom electrode (12) includes metal shell (8), is arranged on the lower electricity contacted at the top of metal shell (8) and with the lower surface of sample Pole upper cover plate (4), be arranged in metal shell (8) and with bottom electrode upper cover plate (4) lower surface is close to changes the thin of thickness Film sensors (5), cover on the outside metal shielding (6) of thin film sensor (5), the low noise being connected with thin film sensor (5) Amplifier (7), being embedded in the panel connector (9) on metal shell (8), panel connector (9) has a signal transmission mouth and one Individual plant-grid connection mouthful, is respectively used to spread out of the signal of low-noise amplifier (7) amplification and gives low-noise amplifier (7) power supply, low Noise amplifier (7) is connected with panel connector (9);The integrating circuit matched line being connected with the signal transmission mouth of panel connector (9) (10), it is connected to the oscillograph (11) of integrating circuit matched line (10) other end.
2. multi purpose space charge-measuring system according to claim 1, it is characterised in that:The pulse generating unit (2) amplitude and pulsewidth of input pulse signal can be adjusted according to sample thickness, while thin film sensor (5) is by adjusting film Thickness to adapt to the measurement of different-thickness sample so that whole measuring system is realized to be entered to the plate tensile sample material of different-thickness Row measurement;The pulse amplitude adjustable extent of the pulse generating unit (2) is 0~3600V, the adjustable range of pulsewidth for 5ns~ 150ns;The film thickness adjustable range of thin film sensor (5) is 5 μm~100 μm;Measurable sample thickness scope is 0.1mm ~5mm.
3. multi purpose space charge-measuring system according to claim 1, it is characterised in that:The system is in general atmosphere ring External dc high pressure carries out general measure under border, and application voltage range is 1kV~50kV;Simultaneously also can be in electron irradiation environment The distribution of space charge situation of the lower sample of measurement in real time, electron energy scope is 10keV~10MeV, and the system is in vertical spoke Penetrate and horizontal radiation in the case of can all carry out experiment measurement.
4. multi purpose space charge-measuring system according to claim 1, it is characterised in that:The measurement Top electrode (1) It is fixedly connected with measurement bottom electrode (12) by screw rod with nut.
5. multi purpose space charge-measuring system according to claim 1, it is characterised in that:The integrating circuit matched line (10) mainly it is made up of electric capacity and resistance, the distortion for eliminating waveform.
6. the measuring method of multi purpose space charge-measuring system described in claim 1, it is characterised in that:Made with pulse radio-acoustic method For general principle, when applying high direct voltage progress general measure under normal atmospheric environment, the source of measurement electric charge is pressure DC high-voltage source (3);The selection of pulse parameter and sensor thickness is carried out according to the thickness of measurement sample;DC high-voltage source (3) Pressure to be injected into the electric charge of certain polarity in sample, the pulse that pulse generating unit (2) is applied is by sample The ping ripple of corresponding polarity can be produced during portion's Charge sites;Ping ripple be transferred through sample and bottom electrode upper cover plate (4) it Received afterwards by thin film sensor (5) and be changed into electric signal, the electric signal waveform exported afterwards is put by low-noise amplifier (7) Greatly, and integrated Circuit Matching line (10) carry out waveform modification, finally by oscillograph (11) receive, afterwards by obtained waveform pair Signal data is demarcated and denoising, the final distribution of charges and electric-field intensity distribution for obtaining sample;
The charge collection principle of sample under electron irradiation environment is directly injected into for electronics, the system under electron irradiation environment Measurement need not access DC voltage, so do not need DC high-voltage source (3), electricity is directly received using Top electrode (1) is measured Son injection, electrons stay directly forms space charge inside sample, and the pulse then sent using pulse generating unit (2) is swashed The acoustic signals related to electric charge are sent, acoustic signals are transmitted with sample and bottom electrode upper cover plate (4) for medium, by film Sensor (5) receives and is converted into corresponding electric signal;Subsequent electric signal amplifies by low-noise amplifier (7), then through product Parallel circuit matched line (10) carries out waveform modification, is finally obtained by oscillograph (11), afterwards by obtained waveform to signal data Demarcated and denoising, the final distribution of charges and electric-field intensity distribution for obtaining sample.
CN201710552011.4A 2017-07-07 2017-07-07 Multifunctional space charge measuring system and measuring method Active CN107247196B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201710552011.4A CN107247196B (en) 2017-07-07 2017-07-07 Multifunctional space charge measuring system and measuring method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201710552011.4A CN107247196B (en) 2017-07-07 2017-07-07 Multifunctional space charge measuring system and measuring method

Publications (2)

Publication Number Publication Date
CN107247196A true CN107247196A (en) 2017-10-13
CN107247196B CN107247196B (en) 2023-04-07

Family

ID=60015436

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201710552011.4A Active CN107247196B (en) 2017-07-07 2017-07-07 Multifunctional space charge measuring system and measuring method

Country Status (1)

Country Link
CN (1) CN107247196B (en)

Cited By (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN108181517A (en) * 2017-12-28 2018-06-19 全球能源互联网研究院有限公司 A kind of device and method for being used to detect high-voltage cable joint Space-charge
CN109239434A (en) * 2018-08-03 2019-01-18 上海交通大学 The measuring device of surface potential on-line monitoring
CN110398672A (en) * 2019-07-31 2019-11-01 国网陕西省电力公司电力科学研究院 A kind of sample structure and method measuring insulating materials ionization and charge transport parameters
CN110515021A (en) * 2019-08-29 2019-11-29 西安交通大学 A kind of bearing calibration of free voltage waveform effect down space charge test
CN112147425A (en) * 2020-08-27 2020-12-29 西安交通大学 Low-temperature space charge measuring system
CN112327116A (en) * 2020-11-05 2021-02-05 北京理工大学 Discharge detection system and method based on parylene film and charged particles
CN114167155A (en) * 2021-11-26 2022-03-11 华北电力大学 Novel electrode structure adaptive to photoelectronics space charge measurement method
CN117590100A (en) * 2023-11-27 2024-02-23 兰州理工大学 Space charge measurement method and system based on non-contact vibration measurement

Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH06258380A (en) * 1993-03-05 1994-09-16 Fujikura Ltd Detecting method for defect or impurity of insulator
CN101706537A (en) * 2009-11-16 2010-05-12 华北电力大学 PEA space charge test device capable of testing conductive current
CN102495300A (en) * 2011-11-15 2012-06-13 西安交通大学 Multifunctional high voltage electrode for measuring space charge
CN103605008A (en) * 2013-11-20 2014-02-26 上海电力学院 System and method for measuring high voltage cable space charges based on electroacoustic pulse method

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH06258380A (en) * 1993-03-05 1994-09-16 Fujikura Ltd Detecting method for defect or impurity of insulator
CN101706537A (en) * 2009-11-16 2010-05-12 华北电力大学 PEA space charge test device capable of testing conductive current
CN102495300A (en) * 2011-11-15 2012-06-13 西安交通大学 Multifunctional high voltage electrode for measuring space charge
CN103605008A (en) * 2013-11-20 2014-02-26 上海电力学院 System and method for measuring high voltage cable space charges based on electroacoustic pulse method

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
周凯等: "基于电声脉冲法的空间电荷直接测量仪的研制", 《仪器仪表学报》 *

Cited By (11)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN108181517A (en) * 2017-12-28 2018-06-19 全球能源互联网研究院有限公司 A kind of device and method for being used to detect high-voltage cable joint Space-charge
CN109239434A (en) * 2018-08-03 2019-01-18 上海交通大学 The measuring device of surface potential on-line monitoring
CN109239434B (en) * 2018-08-03 2020-10-30 上海交通大学 Measuring device for on-line monitoring of surface potential
CN110398672A (en) * 2019-07-31 2019-11-01 国网陕西省电力公司电力科学研究院 A kind of sample structure and method measuring insulating materials ionization and charge transport parameters
CN110398672B (en) * 2019-07-31 2021-08-03 国网陕西省电力公司电力科学研究院 Sample structure and method for measuring ionization and charge transfer parameters of insulating material
CN110515021A (en) * 2019-08-29 2019-11-29 西安交通大学 A kind of bearing calibration of free voltage waveform effect down space charge test
CN110515021B (en) * 2019-08-29 2020-08-18 西安交通大学 Correction method for space charge test under action of arbitrary voltage waveform
CN112147425A (en) * 2020-08-27 2020-12-29 西安交通大学 Low-temperature space charge measuring system
CN112327116A (en) * 2020-11-05 2021-02-05 北京理工大学 Discharge detection system and method based on parylene film and charged particles
CN114167155A (en) * 2021-11-26 2022-03-11 华北电力大学 Novel electrode structure adaptive to photoelectronics space charge measurement method
CN117590100A (en) * 2023-11-27 2024-02-23 兰州理工大学 Space charge measurement method and system based on non-contact vibration measurement

Also Published As

Publication number Publication date
CN107247196B (en) 2023-04-07

Similar Documents

Publication Publication Date Title
CN107247196A (en) A kind of multi purpose space charge-measuring system and measuring method
Imburgia et al. Review of space charge measurement systems: Acoustic, thermal and optical methods
CN101706537B (en) PEA space charge test device capable of testing conductive current
CN101738546B (en) Device, system and method for measuring space charges by using electro-acoustic (PEA) method
CN101907659B (en) Temperature controllable PEA space charge test device
CN108089068B (en) Composite flat plate sample three-dimensional space charge measuring device based on electroacoustic pulse method
CN105548732B (en) Insulating materials Space Charge Properties measuring system and method under a kind of temperature rise in short-term
CN103105542B (en) High voltage electrode device for pulsed electro-acoustic space charge measuring system
CN103543339A (en) Method and device for analyzing alternating current-and-direct current space charge test data of dielectric sample
CN102944763A (en) System and method for in-situ testing of internal electric charge and electric field distribution of dielectric material
Fursa et al. Mechanoelectrical transformations in heterogeneous materials with piezoelectric inclusions
Dennison et al. Pulsed electro-acoustic (PEA) measurements of embedded charge distributions
Ren et al. An improved calibration method for the measurement of space charge inside insulating materials
Gerhard-Multhaupt et al. Electric-field profiles in electron-beam-charged polymer electrets
Singh A review of developments in thermal techniques for charge profile measurements in polymer electrets
Perrin et al. Measurement of internal charge distribution in dielectrics using the pulsed electro-acoustic method in non contact mode
CN207096347U (en) A kind of multi purpose space charge-measuring system
CN114646818A (en) Space charge non-contact test system and method
Hussaini et al. Review of space-charge measurement using pulsed electro-acoustic method: Advantages and limitations
Florkowski et al. Effects of nanosecond impulse and step excitation in pulsed electro acoustic measurements on signals for space charge determination in high-voltage electrical insulation
CN107677896B (en) Same district timesharing conductance space charge measurement device based on ontology capacitance
CN104237659A (en) In-situ measurement device and method for space charges of dielectric material under electron irradiation
Capineri et al. Comparisons between PZT and PVDF thick films technologies in the design of low-cost pyroelectric sensors
DE102013110900A1 (en) Test head for air-coupled ultrasound
CN104833859B (en) A kind of plane plate specimen distribution of space charge pressure wave method measurement apparatus

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