CN113945802B - Method and device for measuring space potential below high-voltage transmission line - Google Patents

Method and device for measuring space potential below high-voltage transmission line Download PDF

Info

Publication number
CN113945802B
CN113945802B CN202111238587.6A CN202111238587A CN113945802B CN 113945802 B CN113945802 B CN 113945802B CN 202111238587 A CN202111238587 A CN 202111238587A CN 113945802 B CN113945802 B CN 113945802B
Authority
CN
China
Prior art keywords
voltage
transmission line
measuring
electric field
space
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.)
Active
Application number
CN202111238587.6A
Other languages
Chinese (zh)
Other versions
CN113945802A (en
Inventor
杨勃
徐禄文
杨滔
邹军
刘佳
王万彪
李龙
龙英凯
杨华夏
张盈
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.)
Electric Power Research Institute of State Grid Chongqing Electric Power Co Ltd
State Grid Corp of China SGCC
Original Assignee
Electric Power Research Institute of State Grid Chongqing Electric Power Co Ltd
State Grid Corp of China SGCC
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 Electric Power Research Institute of State Grid Chongqing Electric Power Co Ltd, State Grid Corp of China SGCC filed Critical Electric Power Research Institute of State Grid Chongqing Electric Power Co Ltd
Priority to CN202111238587.6A priority Critical patent/CN113945802B/en
Publication of CN113945802A publication Critical patent/CN113945802A/en
Application granted granted Critical
Publication of CN113945802B publication Critical patent/CN113945802B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01RMEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R31/00Arrangements for testing electric properties; Arrangements for locating electric faults; Arrangements for electrical testing characterised by what is being tested not provided for elsewhere
    • G01R31/08Locating faults in cables, transmission lines, or networks
    • 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

Abstract

The invention provides a method and a device for measuring space potential below a high-voltage transmission line, wherein the method comprises the following steps: placing an analog charge under the high-voltage transmission line; measuring and calculating induction voltage generated by the space potential of the analog charge below the power transmission line by using a voltage dividing device; the distortion effect of the simulated charge on the space electric field below the power transmission line is considered, the distortion potential is corrected, and the electric field intensity in the vertical direction of the space below the high-voltage power transmission line is obtained; the relation between the space potential below the power transmission line and the height of the measuring point on the ground is established according to the electric field intensity value in the vertical direction obtained in the step S3, and the device comprises a conductor ball, a supporting structure and a voltage measuring structure. The voltage distortion correction is carried out on the voltage measured by the device by using an analog charge method, the structure of the measuring device is simple, the sensitivity is higher, and the measured data is accurate.

Description

Method and device for measuring space potential below high-voltage transmission line
Technical Field
The invention relates to the technical field of high-voltage transmission line induced voltage measurement, in particular to a method and a device for measuring space potential below a high-voltage transmission line.
Background
With the rapid development of national economy and the continuous increase of electricity load, the voltage level of a power grid is continuously increased, the space density of an overhead line is continuously increased, and the overhead line is in close contact with surrounding residents, although the electromagnetic field intensity below the overhead power transmission line is limited by the national environmental protection standard, even if the environmental protection standard is reached, the problem of induction electricity disturbing the residents still exists, so that a certain amount of environmental protection complaints and disputes are caused. Therefore, the measurement of the space induction potential below the overhead line needs to be carried out, and corresponding protective measures are adopted by measuring the induction voltage, so that disputes are avoided. Meanwhile, the induced voltage below the high-voltage transmission line is weak, and the sensitivity of the measuring device is also high.
Disclosure of Invention
The invention aims to at least solve the technical problems that whether safety measures for protecting induced voltage are needed to be adopted below a power transmission line lacks corresponding technical guidance and a measuring device which can measure the induced potential below a high-voltage line regularly and is sensitive enough is not available in the prior art due to the lack of a method for measuring the induced potential below the overhead line.
To this end, the first aspect of the present invention provides a method for measuring a space potential under a high-voltage transmission line.
The invention provides a method for measuring the space potential below a high-voltage transmission line, which comprises the following steps:
s1: placing an analog charge under the high-voltage transmission line;
s2: measuring and calculating induction voltage generated by the space potential of the analog charge below the power transmission line by using a voltage dividing device;
s3: the distortion effect of the simulated charge on the space electric field below the power transmission line is considered, the distortion potential is corrected, and the electric field intensity in the vertical direction of the space below the high-voltage power transmission line is obtained;
s4: and (3) establishing the relation between the space potential below the power transmission line and the height of the belt measuring point from the ground according to the electric field intensity value in the vertical direction obtained in the step (S3).
According to the technical scheme, the method for measuring the space potential below the high-voltage transmission line can be provided with the following additional technical characteristics:
further, in step S1, the analog charge is a spherical shell structure, and the spherical shell structure is made of a good conductor.
Further, the voltage measured after being divided by the voltage divider is
Figure GDA0003348407550000021
The induced voltage of the analog charge is:
Figure GDA0003348407550000022
wherein k is the transformation ratio coefficient of the voltage divider.
Further, in step S3, the vertical direction of the near area under the high voltage transmission line is approximately equal to the uniform electric field, the analog charge is divided into n charged rings, n matching points are found on the surface of the analog charge, and the potential equation is written for each matching point k, which has the following relationship:
Figure GDA0003348407550000023
wherein ,
Figure GDA0003348407550000024
is the induced voltage under the action of the original electric field; />
Figure GDA0003348407550000025
The applied voltage of n circular rings of the conductor ball to the matching point k; e (E) 0 The electric field strength of the uniform strong electric field in the vertical direction; h is a k Matching the height of the point from the ground for the column writing equation; τ i To simulate the amount of charge carried by a charged torus, i=1, 2,3,; />
Figure GDA0003348407550000026
An induced voltage which is the analog charge obtained in the step S2; p is a potential coefficient;
writing the above-mentioned writable potential equation for each point column to obtain the equation set as follows:
Figure GDA0003348407550000027
wherein Στ=0, and bringing into the equation set yields the electric field strength E of Fang Yunjiang electric field under the power line 0
Further, in step S4, the relationship between the space potential below the power transmission line and the height of the measured point from the ground is:
Figure GDA0003348407550000028
wherein ,ht For the height of the point to be measured from the ground,
Figure GDA0003348407550000029
to place the original potential at the analog charge.
The second aspect of the invention provides a measuring device for the space potential below a high-voltage transmission line.
The invention provides a measuring device for space potential below a high-voltage transmission line, which is used for the measuring method for space potential below the high-voltage transmission line.
In the technical scheme, the conductor ball is placed in an electric field of a space below a high-voltage transmission line as analog charge, is of a ball shell structure and is made of good conductive materials, copper, iron, aluminum and other materials can be adopted as the conductor ball, the copper ball shell is selected as the conductor ball, the support structure provides a supporting function for the conductor ball, the voltage measurement structure can measure the induced voltage of the conductor ball in the electric field of the space below the high-voltage transmission line, and the voltage measurement structure needs to keep a certain safety distance with the conductor ball.
According to the technical scheme, the measuring device for the space potential below the high-voltage transmission line can be further provided with the following additional technical characteristics:
in the above technical scheme, the voltage measurement structure comprises a voltage dividing device and a voltmeter, wherein the cable is connected with the voltage dividing device, and the voltmeter is connected with the voltage dividing device.
In this technical scheme, cable one end is connected with the conductor ball through the aviation connector, and the other end is connected with bleeder mechanism, and the induced voltage of conductor ball obtains the voltage value of easy measurement through bleeder mechanism, utilizes the voltmeter to survey and gets the voltage value after, according to bleeder mechanism's transformation ratio coefficient, obtains the induced voltage of conductor ball, adopts this kind of measurement mode, realizes more easily to effectively improve measuring device's sensitivity.
In the above technical scheme, the voltage divider comprises a high-resistance voltage divider, the high-resistance voltage divider comprises a first resistor R1, a first capacitor C1, a second resistor R2 and a second capacitor C2, wherein a conductor ball is connected with one end of the first resistor R1, the other end of the first resistor R1 is connected with one end of the second resistor R2, the other end of the second resistor R2 is connected with the ground, the first capacitor C1 is connected in parallel with two ends of the first resistor R1, the second capacitor C2 is connected in parallel with two ends of the second resistor R2, and two ends of the second resistor R2 are connected with a voltmeter in parallel.
In the technical scheme, reliable grounding of the high-resistance voltage divider is realized through connection of the second resistor R2 and the ground, and the resistance values of the first resistor R1 and the second resistor R2 are respectively Z 1 and Z2 The transformation ratio coefficient k of the voltage dividing device is:
Figure GDA0003348407550000031
in any of the above technical solutions, the supporting structure includes a bracket and a cradle head, the bracket is connected with the cradle head, the conductor ball is disposed on the cradle head, and the cradle head is detachably and insulatively connected with the conductor ball.
In the technical scheme, the bracket is detachably connected with the cradle head, so that the cradle head is convenient to assemble and disassemble, the cradle head and the conductor ball can be detachably connected through the supporting nut, the insulating sheath is wrapped by the supporting nut, insulation between the cradle head and the conductor ball is realized, and the influence of the cradle head and the bracket on simulation charge is eliminated.
In any of the above aspects, the support structure is insulated from the ground.
In this technical scheme, bearing structure can utilize insulating tripod as the support realization and ground insulation, and insulating tripod can select wooden tripod, also can set up insulating cover or insulating pad that satisfies the requirement in the support bottom, when improving the measurement accuracy, guarantees the personal and the equipment safety in the measurement process.
In summary, due to the adoption of the technical scheme, the beneficial effects of the invention are as follows: by using an analog charge method, voltage distortion correction is performed according to the relation between the voltage and the electric field and the voltage measured by the measuring device, the measuring method and the measuring device for reliably measuring the space potential below the high-voltage transmission line are provided, the measuring device has a simple structure, high sensitivity and accurate measured data.
Additional aspects and advantages of the invention will be set forth in part in the description which follows, or may be learned by practice of the invention.
Drawings
The foregoing and/or additional aspects and advantages of the invention will become apparent and may be better understood from the following description of embodiments taken in conjunction with the accompanying drawings in which:
FIG. 1 is a flow chart of a method of measuring a space potential under a high voltage transmission line according to an embodiment of the present invention;
fig. 2 is a schematic structural diagram of a measurement device for space potential under a high-voltage transmission line according to an embodiment of the present invention;
fig. 3 is a schematic diagram of a method for measuring a space potential under a high voltage transmission line according to an embodiment of the present invention.
The correspondence between the reference numerals and the component names in fig. 2 is:
1. a conductor ball; 2. a support structure; 3. a voltage measurement structure; 4. a cable; 5. a voltage dividing device; 6. a voltmeter; 7. a high-resistance voltage divider; 8. a bracket; 9. a cradle head; 10. a support nut; 11. an air joint.
Detailed Description
In order that the above-recited objects, features and advantages of the present invention will be more clearly understood, a more particular description of the invention will be rendered by reference to the appended drawings and appended detailed description. It should be noted that, in the case of no conflict, the embodiments of the present application and the features in the embodiments may be combined with each other.
In the following description, numerous specific details are set forth in order to provide a thorough understanding of the present invention, however, the present invention may be practiced otherwise than as described herein, and therefore the scope of the present invention is not limited to the specific embodiments disclosed below.
A method for measuring a space potential under a high-voltage transmission line according to some embodiments of the present invention is described below with reference to fig. 1 to 3.
Some embodiments of the present application provide a method for measuring a space potential below a high-voltage transmission line.
As shown in fig. 1 to 3, a first embodiment of the present invention provides a method for measuring a space potential below a high-voltage transmission line, which includes the following steps:
s1: placing an analog charge under the high-voltage transmission line;
s2: measuring and calculating induction voltage generated by the space potential of the analog charge below the power transmission line by using a voltage dividing device;
s3: the distortion effect of the simulated charge on the space electric field below the power transmission line is considered, the distortion potential is corrected, and the electric field intensity in the vertical direction of the space below the high-voltage power transmission line is obtained;
s4: and (3) establishing the relation between the space potential below the power transmission line and the height of the belt measuring point from the ground according to the electric field intensity value in the vertical direction obtained in the step (S3).
In the step S1, the analog charge is a spherical shell structure, and the spherical shell structure is made of a good conductor.
The voltage measured after being divided by the voltage divider is
Figure GDA0003348407550000051
The induced voltage of the analog charge is:
Figure GDA0003348407550000052
wherein k is the transformation ratio coefficient of the voltage divider.
In step S3, the vertical direction of the near area under the high-voltage power transmission line is approximately equal to the uniform electric field, as shown in fig. 3, the analog charge is divided into n charged rings, n matching points are found on the surface of the analog charge, and the potential equation is written for each matching point k, which has the following relationship:
Figure GDA0003348407550000053
wherein ,
Figure GDA0003348407550000054
is the induced voltage under the action of the original electric field; />
Figure GDA0003348407550000055
The applied voltage of n circular rings of the conductor ball to the matching point k; e (E) 0 The electric field strength of the uniform strong electric field in the vertical direction; h is a k Matching the height of the point from the ground for the column writing equation; τ i To simulate the amount of charge carried by a charged torus, i=1, 2,3,; />
Figure GDA0003348407550000056
An induced voltage which is the analog charge obtained in the step S2; p is a potential coefficient, and the calculation method of p is as follows:
Figure GDA0003348407550000061
writing the above-mentioned writable potential equation for each point column to obtain the equation set as follows:
Figure GDA0003348407550000062
wherein Στ=0, and bringing into the equation set yields the electric field strength E of Fang Yunjiang electric field under the power line 0
The system of column writing equations is:
Figure GDA0003348407550000063
in the above
Figure GDA0003348407550000064
All are conductor ball measuring voltages +.>
Figure GDA0003348407550000065
N+1 unknowns in the above equation, n+1 equations can be solved to obtain the electric field intensity E of Fang Yunjiang under the transmission line 0
Further, in step S4, the relationship between the space potential below the power transmission line and the height of the measured point from the ground is:
Figure GDA0003348407550000066
wherein ,ht For the height of the point to be measured from the ground,
Figure GDA0003348407550000067
to place the original potential at the analog charge.
Some embodiments of the present application provide a measurement device for a space potential below a high-voltage transmission line.
A second embodiment of the present invention proposes a measurement device for a space potential under a high voltage transmission line, and on the basis of the first embodiment, as shown in fig. 1 to 3, the measurement device includes a conductor ball 1, a support structure 2, and a voltage measurement structure 3, wherein the support structure 2 is disposed on the ground, the conductor ball 1 is connected with the support structure 2, and the voltage measurement structure 3 is connected with the conductor ball 1 through a cable 4.
In this embodiment, the conductive ball 1 is placed as an analog charge in the electric field in the space under the high-voltage transmission line, the conductive ball 1 is in a spherical shell structure and is made of a good conductive material, and may be made of copper, iron, aluminum or other materials, preferably, the conductive ball 1 is a copper spherical shell, the supporting structure 2 provides a supporting function for the conductive ball 1, the voltage measuring structure 3 may measure the induced voltage of the conductive ball 1 in the electric field in the space under the high-voltage transmission line, and the voltage measuring structure 3 needs to keep a certain safety distance from the conductive ball 1.
A third embodiment of the present invention proposes a measurement device for a space potential under a high-voltage transmission line, and on the basis of the above embodiments, as shown in fig. 1 to 3, the voltage measurement structure 3 includes a voltage dividing device 5 and a voltmeter 6, the cable 4 is connected with the voltage dividing device 5, and the voltmeter 6 is connected with the voltage dividing device 5.
In this embodiment, one end of the cable 4 is connected with the conductor ball 1 through the aviation connector 11, the other end is connected with the voltage divider 5, the induced voltage of the conductor ball 1 obtains a voltage value which is easier to measure through the voltage divider 5, after the voltage value is measured by the voltmeter 6, the induced voltage of the conductor ball 1 is obtained according to the transformation ratio coefficient of the voltage divider 5, by adopting the measuring mode, the implementation is easier, and the sensitivity of the measuring device is effectively improved.
The fourth embodiment of the present invention provides a measurement device for a space potential below a high-voltage transmission line, and based on the above embodiments, as shown in fig. 1 to 3, the voltage divider 5 includes a high-resistance voltage divider 7, where the high-resistance voltage divider 7 includes a first resistor R1, a first capacitor C1, a second resistor R2, and a second capacitor C2, where the conductor ball 1 is connected to one end of the first resistor R1, the other end of the first resistor R1 is connected to one end of the second resistor R2, the other end of the second resistor R2 is connected to ground, the first capacitor C1 is connected in parallel to two ends of the first resistor R1, the second capacitor C2 is connected in parallel to two ends of the second resistor R2, and two ends of the second resistor R2 are connected in parallel to the voltmeter 6.
In this embodiment, the second resistor R2 is connected to ground to achieve reliable grounding of the high-resistance voltage divider 7, and the resistances of the first resistor R1 and the second resistor R2 are Z1 and Z2 respectively, so that the transformation ratio coefficient k of the voltage divider 5 is:
Figure GDA0003348407550000071
a fifth embodiment of the present invention proposes a device for measuring a space potential under a high-voltage transmission line, and on the basis of any of the above embodiments, as shown in fig. 1 to 3, the support structure 2 includes a bracket 8 and a cradle head 9, the bracket 8 is connected with the cradle head 9, the conductor ball 1 is disposed on the cradle head 9, and the cradle head 9 is detachably and insulatively connected with the conductor ball 1.
In this embodiment, the bracket 8 is detachably connected with the cradle head 9, so that the cradle head 9 and the conductor ball 1 can be conveniently assembled and disassembled, the cradle head 9 and the conductor ball 1 can be detachably connected through the supporting nut 10, the supporting nut 10 wraps the insulating sheath, insulation between the cradle head 9 and the conductor ball 1 is realized, and the influence of the cradle head 9 and the bracket 8 on simulation charge is eliminated.
A sixth embodiment of the present invention proposes a method for measuring a space potential under a high voltage transmission line, and on the basis of any of the above embodiments, as shown in fig. 1 to 3, the supporting structure 2 is insulated from the ground.
In this embodiment, the support structure 2 may utilize an insulating tripod as the support 8 to achieve insulation from the ground, the insulating tripod may be a wooden tripod, or an insulating sleeve or an insulating pad meeting the requirements may be disposed at the bottom of the support 8, so as to improve the accuracy of measurement and ensure the safety of personnel and equipment in the measurement process.
In the description of the present specification, the terms "one embodiment," "some embodiments," "particular embodiments," and the like, mean that a particular feature, structure, material, or characteristic described in connection with the embodiment or example is included in at least one embodiment or example of the present invention. In this specification, schematic representations of the above terms do not necessarily refer to the same embodiment or example. Furthermore, the particular features, structures, materials, or characteristics described may be combined in any suitable manner in any one or more embodiments or examples.

Claims (9)

1. The method for measuring the space potential below the high-voltage transmission line is characterized by comprising the following steps of:
s1: placing an analog charge under the high-voltage transmission line;
s2: measuring and calculating induction voltage generated by the space potential of the analog charge below the power transmission line by using a voltage dividing device;
s3: the distortion effect of the simulated charge on the space electric field below the power transmission line is considered, the distortion potential is corrected, and the electric field intensity in the vertical direction of the space below the high-voltage power transmission line is obtained;
s4: establishing a relation between the space potential below the power transmission line and the height of the belt measuring point from the ground according to the electric field intensity value in the vertical direction obtained in the step S3;
in step S3, the vertical direction of the near area under the high-voltage power transmission line is approximately equal to the uniform electric field, the analog charge is divided into n charged rings, n matching points are found on the surface of the analog charge, and the potential equation can be written for each matching point k, so that the following relationship exists:
Figure QLYQS_1
wherein ,
Figure QLYQS_2
is the induced voltage under the action of the original electric field; />
Figure QLYQS_3
The applied voltage of n circular rings of the conductor ball to the matching point k;
Figure QLYQS_4
the electric field strength of the uniform strong electric field in the vertical direction; />
Figure QLYQS_5
Matching the height of the point from the ground for the column writing equation; />
Figure QLYQS_6
To simulate the charge amount of the charged ring, +.>
Figure QLYQS_7
;/>
Figure QLYQS_8
An induced voltage which is the analog charge obtained in the step S2;pis the potential coefficient;
writing the above-mentioned writable potential equation for each point column to obtain the equation set as follows:
Figure QLYQS_9
wherein ,
Figure QLYQS_10
the electric field strength of Fang Yunjiang electric field under the transmission line is obtained by taking the equation set>
Figure QLYQS_11
2. The method according to claim 1, wherein in the step S1, the analog charge is in a spherical shell structure, and the spherical shell structure is made of a good conductor.
3. A high voltage transmission line according to claim 1The method for measuring the space potential under the road is characterized in that the voltage measured after being divided by a voltage divider is
Figure QLYQS_12
The induced voltage of the analog charge is:
Figure QLYQS_13
wherein k is the transformation ratio coefficient of the voltage divider.
4. The method for measuring the space potential below the high-voltage transmission line according to claim 1, wherein in the step S4, the relation between the space potential below the transmission line and the height of the belt measuring point from the ground is:
Figure QLYQS_14
wherein ,
Figure QLYQS_15
for the height of the point to be measured from the ground, +.>
Figure QLYQS_16
To place the original potential at the analog charge.
5. A measuring device for the space potential under a high voltage transmission line, which is used for the measuring method for the space potential under the high voltage transmission line according to any one of the claims 1 to 4, and is characterized by comprising a conductor ball (1), a supporting structure (2) and a voltage measuring structure (3), wherein the supporting structure (2) is arranged on the ground, the conductor ball (1) is connected with the supporting structure (2), and the voltage measuring structure (3) is connected with the conductor ball (1) through a cable (4).
6. The measuring device for the space potential below the high-voltage transmission line according to claim 5, wherein the voltage measuring structure (3) comprises a voltage dividing device (5) and a voltmeter (6), the cable (4) is connected with the voltage dividing device (5), and the voltmeter (6) is connected with the voltage dividing device (5).
7. The device for measuring the space potential below the high-voltage transmission line according to claim 6, wherein the voltage divider (5) comprises a high-resistance voltage divider (7), the high-resistance voltage divider (7) comprises a first resistor (R1), a first capacitor (C1), a second resistor (R2) and a second capacitor (C2), wherein the conductor ball (1) is connected with one end of the first resistor (R1), the other end of the first resistor (R1) is connected with one end of the second resistor (R2), the other end of the second resistor (R2) is connected with the ground, the first capacitor (C1) is connected in parallel with two ends of the first resistor (R1), the second capacitor (C2) is connected in parallel with two ends of the second resistor (R2), and the two ends of the second resistor (R2) are connected with the voltmeter (6) in parallel.
8. The measuring device of the space potential under the high-voltage transmission line according to any one of claims 6 or 7, characterized in that the supporting structure (2) comprises a bracket (8) and a holder (9), the bracket (8) is connected with the holder (9), the conductor ball (1) is arranged on the holder (9), and the holder (9) is detachably and insulatively connected with the conductor ball (1).
9. A measuring device of the space potential under a high voltage transmission line according to any of the claims 5 to 7, characterized in that the support structure (2) is insulated from ground.
CN202111238587.6A 2021-10-25 2021-10-25 Method and device for measuring space potential below high-voltage transmission line Active CN113945802B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN202111238587.6A CN113945802B (en) 2021-10-25 2021-10-25 Method and device for measuring space potential below high-voltage transmission line

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN202111238587.6A CN113945802B (en) 2021-10-25 2021-10-25 Method and device for measuring space potential below high-voltage transmission line

Publications (2)

Publication Number Publication Date
CN113945802A CN113945802A (en) 2022-01-18
CN113945802B true CN113945802B (en) 2023-06-20

Family

ID=79332063

Family Applications (1)

Application Number Title Priority Date Filing Date
CN202111238587.6A Active CN113945802B (en) 2021-10-25 2021-10-25 Method and device for measuring space potential below high-voltage transmission line

Country Status (1)

Country Link
CN (1) CN113945802B (en)

Citations (11)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4328461A (en) * 1979-07-02 1982-05-04 Mcdonnell Douglas Corporation Apparatus for and method of measuring a high voltage electric field
JP2001255342A (en) * 2000-03-08 2001-09-21 Hitachi Ltd Voltage sensor
CN101696990A (en) * 2009-10-20 2010-04-21 重庆大学 Method for testing electricity of ultrahigh-voltage transmission line based on electric field measurement and system thereof
JP2011064465A (en) * 2009-09-15 2011-03-31 Toshiba Corp Line constant measuring method and protection control measuring device
CN103984876A (en) * 2014-06-11 2014-08-13 国家电网公司 Calculation method for synthetic electric field of ultrahigh voltage direct-current transmission line crossing complex terrain
CN103995986A (en) * 2014-06-11 2014-08-20 国家电网公司 Power frequency electric field computing method for rolling ground overhead transmission line based on charge simulation method
CN106557618A (en) * 2016-11-03 2017-04-05 合肥华义电气科技有限公司 A kind of transformer station's electric field appraisal procedure
CN107085646A (en) * 2017-04-28 2017-08-22 国家电网公司 A kind of field strength measurement method in ground under transmission line of electricity
CN110879918A (en) * 2019-11-13 2020-03-13 国网天津市电力公司电力科学研究院 Simulation calculation method of alternating current transmission line electromagnetic environment based on analog charge method
CN112881818A (en) * 2021-01-15 2021-06-01 广州穗能通能源科技有限责任公司 Electric field intensity measuring method, electric field intensity measuring device, computer equipment and storage medium
CN113203898A (en) * 2021-07-05 2021-08-03 北京科技大学 Non-contact surface potential testing method for ionized air

Patent Citations (11)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4328461A (en) * 1979-07-02 1982-05-04 Mcdonnell Douglas Corporation Apparatus for and method of measuring a high voltage electric field
JP2001255342A (en) * 2000-03-08 2001-09-21 Hitachi Ltd Voltage sensor
JP2011064465A (en) * 2009-09-15 2011-03-31 Toshiba Corp Line constant measuring method and protection control measuring device
CN101696990A (en) * 2009-10-20 2010-04-21 重庆大学 Method for testing electricity of ultrahigh-voltage transmission line based on electric field measurement and system thereof
CN103984876A (en) * 2014-06-11 2014-08-13 国家电网公司 Calculation method for synthetic electric field of ultrahigh voltage direct-current transmission line crossing complex terrain
CN103995986A (en) * 2014-06-11 2014-08-20 国家电网公司 Power frequency electric field computing method for rolling ground overhead transmission line based on charge simulation method
CN106557618A (en) * 2016-11-03 2017-04-05 合肥华义电气科技有限公司 A kind of transformer station's electric field appraisal procedure
CN107085646A (en) * 2017-04-28 2017-08-22 国家电网公司 A kind of field strength measurement method in ground under transmission line of electricity
CN110879918A (en) * 2019-11-13 2020-03-13 国网天津市电力公司电力科学研究院 Simulation calculation method of alternating current transmission line electromagnetic environment based on analog charge method
CN112881818A (en) * 2021-01-15 2021-06-01 广州穗能通能源科技有限责任公司 Electric field intensity measuring method, electric field intensity measuring device, computer equipment and storage medium
CN113203898A (en) * 2021-07-05 2021-08-03 北京科技大学 Non-contact surface potential testing method for ionized air

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
用模拟电荷法求解高压输电线附近电磁场;杨文翰;《电网技术》;第32卷(第2期);第47-55页 *

Also Published As

Publication number Publication date
CN113945802A (en) 2022-01-18

Similar Documents

Publication Publication Date Title
CN109459621B (en) Non-contact type measuring system for conductor suspension potential
CN105467235B (en) The test method and device that cable is interfered in electromagnetic radiation
CN109799377A (en) Electric railway step voltage and contact voltage test macro and its method
CN113945802B (en) Method and device for measuring space potential below high-voltage transmission line
CN103760402B (en) Voltage compensating method is affected based on the threephase potential transformer of D_dot principle and three-phase
US20140291537A1 (en) An ionization chamber
CN109324305B (en) Capacitive voltage divider for linearity calibration of impulse voltage divider
US20130069664A1 (en) Indirect non-contact high voltage measurement on electrical power line
CN111141785B (en) Soil resistivity measuring device, method and storage medium
CN217404404U (en) Volume resistivity measuring device for cable buffer layer
CN217766808U (en) Power frequency electric field measuring device calibration system
CN207908574U (en) Contact net voltage non-contact type measuring device
CN205919776U (en) Charge coil position detecting device
CN110542797B (en) Method for testing contact performance difference between different grounding materials and soil
CN212083300U (en) Air ion detector signal amplifier calibrating device
CN114184850B (en) Electric field reciprocity-based method for measuring space potential below power transmission line
CN111999564A (en) Method and device for calculating internal dielectric constant value of cable accessory
CN207689575U (en) A kind of surface resistivity measuring device of GIS disc insulators
CN102539920B (en) Multipurpose induction conductivity measuring electrode
CN209590136U (en) A kind of insulator volume resistance measuring device
CN117471149A (en) Voltage measurement system of suspended potential conductor below overhead transmission line
CN205210138U (en) Plug -in components with high -pressure electric energy meter of cable accessories structure
CN219978439U (en) High-safety high-voltage electric bridge proportion detection device
AU2021104699A4 (en) System and method for multi-dimensional balanced magnetic field measurement
CN108627786A (en) Different voltages waveform subscript quasi-electric field generating means and electric field measuring apparatus calibrating installation

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