CN106249068A - A kind of ferromagnetic element no-load characteristic low frequency measurement method - Google Patents

A kind of ferromagnetic element no-load characteristic low frequency measurement method Download PDF

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CN106249068A
CN106249068A CN201610536618.9A CN201610536618A CN106249068A CN 106249068 A CN106249068 A CN 106249068A CN 201610536618 A CN201610536618 A CN 201610536618A CN 106249068 A CN106249068 A CN 106249068A
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frequency
loss
ferromagnetic element
calculate
current
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CN106249068B (en
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刘鑫
梁仕斌
姚陈果
刘涛
王磊
田庆生
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YUNNAN ELECTRIC TECHNOLOGIES Co Ltd
Electric Power Research Institute of Yunnan Power System Ltd
Yunnan Electric Power Test and Research Institute Group Co Ltd
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YUNNAN ELECTRIC TECHNOLOGIES Co Ltd
Electric Power Research Institute of Yunnan Power System Ltd
Yunnan Electric Power Test and Research Institute Group Co Ltd
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    • 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
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01RMEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R33/00Arrangements or instruments for measuring magnetic variables
    • G01R33/12Measuring magnetic properties of articles or specimens of solids or fluids
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01RMEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R33/00Arrangements or instruments for measuring magnetic variables
    • G01R33/12Measuring magnetic properties of articles or specimens of solids or fluids
    • G01R33/123Measuring loss due to hysteresis

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  • General Physics & Mathematics (AREA)
  • Condensed Matter Physics & Semiconductors (AREA)
  • Measuring Magnetic Variables (AREA)

Abstract

A kind of low frequency measurement method of ferromagnetic element no-load characteristic, mainly comprise the steps: the first step: according to T-shaped equivalent circuit, set up high-pressure side open circuit equivalent circuit, apply, in low-pressure side, the low-frequency sine that 2 frequencies are different, calculate the core loss under each frequency;Second step: the unit magnetic hysteresis of unit of account cycle generation and eddy-current loss WeAnd Wh, and calculate the core loss P converted to power frequencyCoren;3rd step: calculate the exciting current I converted to power frequency according to eddy current backoff algorithmexn, harmonic content K(k), excitation voltage Un;4th step: calculate open circuit loss Pn;5th step: draw PCoren‑Un, Iexn‑UnRelation curve, and K(k)‑UnHarmonic content form.The method uses low-frequency power to replace power frequency supply to carry out test can lower experiment power supply capacity, reduction testing equipment volume and weight at double, makes experimentation cost lower.

Description

A kind of ferromagnetic element no-load characteristic low frequency measurement method
Technical field
The invention belongs to ferromagnetic element no-load characteristic field of measuring technique, mainly comprise open circuit loss, excitation property, zero load Current harmonic content is measured, and is specifically related to the ferromagnetic elements such as transformator, transformer, reactor.
Background technology
The ferromagnetic elements such as transformator, transformer, reactor as power transmission and transforming equipment most important in power system, its performance Quality directly affect the safety of power system, economical operation.The open circuit loss of ferromagnetic element, excitation property and no-load current Harmonic content is the important indicator of reaction ferromagnetic element iron core performance." GB1094.1-2013 power transformer Part I: total Then ", it is desirable to open circuit loss and no-load current are measured as routine test, can lack as the local checked and find in test product magnetic circuit Fall into and general defect.Regulation in " JB/T501-2006 power transformer test directive/guide ": when carrying out no-load test, should be each from test product The rated voltage of high-pressure side winding (generally low pressure winding) the supply rated frequency in winding, remaining winding is opened a way;Transformator No-load current harmonic measure is special test, consists of detection no-load current harmonic wave and numerical value is to check saturated journey unshakable in one's determination Degree, the reasonability of checking design." GB22071.1-2008 transformer test guidance part 1: current transformer " and " GB 22071.2-2008 transformer test guidance part 2: voltage transformer " all specify to need voltage (electric current) transformer is carried out Excitation property is tested." GB 1094.6-2011 power transformer the 6th part: reactor " also specify reactor and must carry out zero load The measurement of loss.But along with the raising of line voltage grade, electric pressure and the capacity of the ferromagnetic elements such as transformator the most gradually increase Greatly, it is the biggest to carry out testing equipment capacity required during no-load test, volume and weight, causes no-load test program multiple Miscellaneous, operator's personal safety can not get ensureing.
Therefore, finding a kind of new energy short form test process, the ferromagnetic element alleviating testing equipment weight and volume is unloaded Characteristic test method is necessary.
Summary of the invention
For the deficiency of above-mentioned existing ferromagnetic element no-load characteristic measuring method, the present invention proposes a kind of employing low frequency Power supply carries out ferromagnetic element no-load test.From E=4.44fN Φ, the saturation voltage unshakable in one's determination of ferromagnetic element is basic with power supply frequently Rate is directly proportional, under the excitation of low-frequency power, it is possible to be substantially reduced supply voltage, and no-load current is basically unchanged, thus can become The capacity of demultiplication small test power supply.Measure open circuit loss, no-load current and the harmonic characterisitic thereof under low frequency, further according to related algorithm Calculate open circuit loss, no-load current and the harmonic content thereof converted to industrial frequency experiment, reach to replace with low-frequency tests The purpose of industrial frequency experiment.Test proves, this method has preferable concordance with directly using industrial frequency experiment method.
In order to achieve the above object, the present invention adopts the following technical scheme that
A kind of low frequency measurement method of ferromagnetic element no-load characteristic, is characterized in that:
1, the equivalent-circuit model of ferromagnetic element high-pressure side open circuit is set up, shown in Fig. 1.Wherein RdcFor the unidirectional current on winding Resistance, LσFor this side winding leakage inductance, ReFor eddy-current loss equivalent resistance, the nonlinear inductance L of band hysteresis ringmFor magnetizing inductance, magnetic Stagnant loss PhIt is included in LmIn.iexT () is exciting current, imT () is for flowing through LmMagnetizing current, ieT () is eddy-current loss equivalence Electric current, u (t) is the excitation voltage being applied on winding;
2, ferromagnetic element open circuit loss is mainly core loss, and core loss is mainly by magnetic hystersis loss and eddy-current loss group Become:
P C o r e = P h + P e = C h fB m n V + C e Δ 2 f 2 B m 2 V = W h f + W e f 2 - - - ( 1 )
In formula, PhAnd PeIt is respectively magnetic hystersis loss and eddy-current loss;CeFor eddy current loss factor, resistivity determines;ChFor magnetic Stagnant loss factor, material character determines;BmFor magnetic flux peak value unshakable in one's determination;F is frequency;V is core volume;Δ is stalloy thickness;Wh And W (W/Hz)e(W/Hz2) it is respectively unit magnetic hysteresis and eddy-current loss that each cycle of magnetization produces.If therefore ensureing different frequency B under ratemUnanimously, then it is believed that We、WhFor constant, during test, it is ensured that the U/f under different frequency is consistent, then it is believed that Bm Equal.W can be obtained by the core loss under two different frequencieshAnd WeValue;
3, allowing winding high voltage side open a way, low-pressure side applies voltage, records voltage electricity when U/f is equal under two different frequencies Flow data.The computing formula of iron loss:
P F e = 1 T ∫ 0 T u ( t ) · i e x ( t ) d t - I e x 2 · R d c - - - ( 2 )
In formula, u (t) is consequently exerted at the voltage at winding two ends, iexT () is exciting current, IexIt it is its virtual value;
4, calculate iron loss corresponding under each frequency, obtain:
P C o r e 1 = W h f 1 + W e f 1 2 P C o r e 2 = W h f 2 + W e f 2 2 - - - ( 3 ) ;
5, by formula (3), solve equation and can try to achieve WeAnd WhFor:
W e = f 1 P C o r e 2 - f 2 P C o r e 1 f 1 f 2 ( f 2 - f 1 ) W h = f 2 2 P C o r e 1 - f 1 2 P C o r e 2 f 1 f 2 ( f 2 - f 1 ) - - - ( 4 ) ;
6, therefore, the iron loss under power frequency is converted:
P C o r e n = f n W h + f n 2 W e - - - ( 5 )
Wherein, fnFor rated frequency, generally 50Hz or 60Hz;
7, iron loss electric current can be divided into magnetic hystersis loss electric current and eddy loss currents:
I F e = I h + I e = P F e E = W h f E + W e f 2 E - - - ( 6 )
In formula, IFe、Ih、IeFor the virtual value of corresponding current, by E=KvfNBmS, knows that E is directly proportional to frequency f, therefore eddy current Loss current ieIt is directly proportional to frequency first power, magnetic hystersis loss electric current ihUnrelated with frequency.And because of B under different frequencymIt is equal, So imEqual, under conversion to power frequency exciting current:
8, because of eddy loss currents ieIt is directly proportional to frequency first power, the eddy current under conversion to power frequency:
Ien=Ie·fn/f (7)
9, being known by Fig. 1, eddy current, containing only fundametal compoment, therefore has only to when calculating exciting current mend eddy current In the fundametal compoment to exciting current repaid, phasor diagram is as in figure 2 it is shown, conversion is to the exciting current fundametal compoment under power frequency:
10, the exciting current under power frequency is converted:
I e x n = I e x n ( 1 ) 2 + Σ k = 2 ∞ I e x ( k ) 2 - - - ( 9 )
Wherein, Iex(k)For kth subharmonic current virtual value under low frequency;
11, no-load current harmonic wave percent:
K ( k ) = I e x n ( k ) I e x n × 100 % - - - ( 10 )
K(k)The percent of fundamental current virtual value is accounted for for kth subharmonic current, due to positive and negative half axial symmetry of waveform symmetry, Even harmonic content is substantially zeroed.Therefore k takes 1,3,5,7 ..., during k > 1, low frequency is humorous with the no-load current high order under power frequency excitation Wave amplitude is equal, i.e. Iexn(k)=Iex(k)
12, the open circuit loss under rated frequency is converted:
P n = P C o r e n + P C u n = P C o r e n + I e x n 2 · R d c - - - ( 11 ) ;
13, the least due to the pressure drop in leakage inductance during zero load, can ignore, the excitation voltage under conversion to rated frequency:
Un=E fn/f+Iexn·Rdc (12)。
The most just the conversion excitation voltage U to power frequency can be obtainedn(power frequency excitation voltage virtual value) and the zero load under power frequency Loss, exciting current and the corresponding relation of no-load current harmonic content thereof, reach to use low-frequency tests to replace industrial frequency experiment Purpose.
Comparing with existing technology, the present invention possesses following advantage:
1. use low-frequency sine power supply to test, can reduction experiment power supply capacity at double, volume and weight, make Test process is convenient, and cost is lower;
2. reduce test voltage, the insulating properties of test equipment are required low, has ensured the safety of testing crew.
Accompanying drawing explanation
In order to make the no-load characteristic measuring method of the ferromagnetic element of the present invention, principle apparent, below in conjunction with accompanying drawing Described in further detail to the present invention, wherein:
The equivalent circuit diagram of a kind of ferromagnetic element high-pressure side open circuit that Fig. 1 provides for the embodiment of the present invention;
The phasor diagram that a kind of ferromagnetic element exciting current that Fig. 2 provides for the embodiment of the present invention compensates;
A kind of ferromagnetic element no-load characteristic low frequency measurement method preferred embodiment principle that Fig. 3 provides for the embodiment of the present invention Figure;
A kind of ferromagnetic element no-load characteristic measuring method schematic diagram that Fig. 4 provides for the embodiment of the present invention;
Fig. 5 measures for employing this method that the embodiment of the present invention provides and the contrast of power frequency actual measurement, and (a) is that open circuit loss is surveyed Amount contrast, (b) is that excitation property measures contrast.
Detailed description of the invention
The embodiment of the present invention provides a kind of low frequency measurement method of ferromagnetic element no-load characteristic, in order to make the art Personnel are better understood from the technical scheme in the present invention, below in conjunction with the drawings and specific embodiments in the embodiment of the present invention Technical scheme carry out clearly, be fully described by, it is clear that described embodiment is only a part of embodiment of the present invention, and It is not all, of embodiment.Based on the embodiment in the present invention, those of ordinary skill in the art are not making creative work The every other embodiment obtained under premise, all should belong to the scope of protection of the invention.
It is as follows that it measures process:
See Fig. 4, for the measuring method schematic diagram of the present invention.
Step 100: according to T-shaped equivalent-circuit model, set up the equivalent circuit opened a way in ferromagnetic element side (high-pressure side), as Shown in Fig. 1, wherein RdcFor the D.C. resistance on winding, LσFor this side winding leakage inductance, ReFor eddy-current loss equivalent resistance, band magnetic hysteresis The nonlinear inductance L of windingmFor magnetizing inductance, magnetic hystersis loss PhIt is included in LmIn.iexT () is exciting current, imT () is for flowing through LmMagnetizing current, ieT () is eddy-current loss equivalent current, u (t) is the excitation voltage being applied on winding;
Step 200: the measurement process schematic of the preferred embodiment that the present invention provides is as in figure 2 it is shown, high-pressure side open circuit, low Pressure side applies the low-frequency sine (ensureing that the U/f under different frequency is equal) of 2 frequencies, and data acquisition unit record is the most electric Current voltage data, calculate the core loss under each frequency according to formula (2);
Step 300: calculate unit magnetic hystersis loss W in each cycle of magnetization according to formula (3)~(4)hWith eddy-current loss We
Step 400: calculate the core loss P converted to power frequency according to formula (5)Coren
Step 500: calculate the eddy current I converted to power frequency according to formula (6)~(8)e, exciting current fundametal compoment Iexn(1)
Step 600: calculate the exciting current I converted to power frequency according to formula (9)~(10)exnAnd harmonic content K(k)
Step 700: calculate open circuit loss P converted to power frequency according to formula (11)n
Step 800: calculate excitation voltage virtual value U converted to power frequency according to formula (12)n
Step 900: draw PCoren-Un, Iexn-UnRelation curve, and K(k)-UnHarmonic content form.
The above is only the detailed description of the invention of the present invention, makes to skilled artisans appreciate that or realize this Bright.Multiple amendment to these embodiments will be apparent to one skilled in the art, as defined herein General Principle can realize without departing from the spirit or scope of the present invention in other embodiments.Therefore, the present invention It is not intended to be limited to the embodiments shown herein, and is to fit to and principles disclosed herein and features of novelty phase one The widest scope caused.

Claims (5)

1. the low frequency measurement method of a ferromagnetic element no-load characteristic, it is characterised in that comprise the steps:
Step one: according to T-shaped equivalent circuit, sets up high-pressure side open circuit equivalent circuit, applies different low of 2 frequencies in low-pressure side Frequency sine-wave, calculates the core loss under each frequency;
Step 2: use that interpolation calculation frequency is different, equal E/f time core loss, calculate not under voltage unit period produce Raw unit magnetic hysteresis and eddy-current loss WeAnd Wh, and calculate the core loss P converted to power frequencyCoren
Step 3: calculate the exciting current I converted to power frequency according to eddy current backoff algorithmexn, harmonic content K(k), excitation Voltage Un
Step 4: calculate open circuit loss P according to the iron loss under conversion to power frequency and copper lossn
Step 5: draw PCoren-Un, Iexn-UnRelation curve, and K(k)-UnHarmonic content form.
2. require the low frequency measurement method of described a kind of ferromagnetic element no-load characteristic according to right 1, it is characterised in that step one institute The U/f that the core loss stated is to ensure that under ferromagnetic element different frequency is equal, to ensure the magnetic flux B under different frequencymEqual bar Core loss under part.
3. require the low frequency measurement method of described a kind of ferromagnetic element no-load characteristic according to right 1, it is characterised in that described step W described in rapid twoeAnd WhIt is to obtain according to the core loss linear equation in two unknowns group solving under two frequencies.
4. require the low frequency measurement method of described a kind of ferromagnetic element no-load characteristic according to right 1, it is characterised in that described step Eddy current, because eddy current is containing only fundametal compoment, is only compensated exciting current by the eddy current backoff algorithm described in rapid three In fundametal compoment.
5. require the low frequency measurement method of described a kind of ferromagnetic element no-load characteristic according to right 1, it is characterised in that described step Copper loss described in rapid four is to be updated in Ohm's law be calculated according to the exciting current under conversion to power frequency.
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CN106908745A (en) * 2017-01-10 2017-06-30 云南电力试验研究院(集团)有限公司 A kind of experiment and the computational methods of ferromagnetic element excitation property and open circuit loss based on low-frequency square-wave
CN107102229A (en) * 2017-05-26 2017-08-29 国家电网公司 The transformer model implementation method of idle-loaded switching-on Transient calculation
CN108231389A (en) * 2017-05-31 2018-06-29 上海申世电气有限公司 A kind of filter reactor core loss design method
RU2755053C1 (en) * 2020-12-14 2021-09-13 Федеральное государственное бюджетное образовательное учреждение высшего образования Иркутский государственный университет путей сообщения (ФГБОУ ВО ИрГУПС) Method for determining magnetic losses in a transformer
RU2764780C1 (en) * 2021-02-05 2022-01-21 Федеральное государственное бюджетное образовательное учреждение высшего образования Иркутский государственный университет путей сообщения (ФГБОУ ВО ИрГУПС) Method for determining the indicator of the degree of magnetic induction in hysteresis losses for steel of a transformer core
RU2781946C1 (en) * 2021-07-05 2022-10-21 Федеральное государственное бюджетное образовательное учреждение высшего образования Иркутский государственный университет путей сообщения (ФГБОУ ВО ИрГУПС) Method for determining eddy current losses in the magnetic core of a transformer

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CN106908745A (en) * 2017-01-10 2017-06-30 云南电力试验研究院(集团)有限公司 A kind of experiment and the computational methods of ferromagnetic element excitation property and open circuit loss based on low-frequency square-wave
CN106908745B (en) * 2017-01-10 2019-05-28 云南电力试验研究院(集团)有限公司 A kind of test and calculation method of the ferromagnetic element excitation property based on low-frequency square-wave and no-load loss
CN107102229A (en) * 2017-05-26 2017-08-29 国家电网公司 The transformer model implementation method of idle-loaded switching-on Transient calculation
CN107102229B (en) * 2017-05-26 2020-09-11 国家电网公司 Method for realizing transformer model for no-load switching transient calculation
CN108231389A (en) * 2017-05-31 2018-06-29 上海申世电气有限公司 A kind of filter reactor core loss design method
RU2755053C1 (en) * 2020-12-14 2021-09-13 Федеральное государственное бюджетное образовательное учреждение высшего образования Иркутский государственный университет путей сообщения (ФГБОУ ВО ИрГУПС) Method for determining magnetic losses in a transformer
RU2764780C1 (en) * 2021-02-05 2022-01-21 Федеральное государственное бюджетное образовательное учреждение высшего образования Иркутский государственный университет путей сообщения (ФГБОУ ВО ИрГУПС) Method for determining the indicator of the degree of magnetic induction in hysteresis losses for steel of a transformer core
RU2781946C1 (en) * 2021-07-05 2022-10-21 Федеральное государственное бюджетное образовательное учреждение высшего образования Иркутский государственный университет путей сообщения (ФГБОУ ВО ИрГУПС) Method for determining eddy current losses in the magnetic core of a transformer
RU2788080C1 (en) * 2021-10-14 2023-01-16 Федеральное государственное бюджетное образовательное учреждение высшего образования Иркутский государственный университет путей сообщения (ФГБОУ ВО ИрГУПС) Method for determining eddy current losses in the steel of a transformer magnetic circuit
RU2796600C1 (en) * 2022-08-03 2023-05-26 Федеральное государственное бюджетное образовательное учреждение высшего образования Иркутский государственный университет путей сообщения (ФГБОУ ВО ИрГУПС) Method for determining magnetic losses in a transformer
RU2815818C1 (en) * 2023-05-24 2024-03-22 Федеральное государственное бюджетное образовательное учреждение высшего образования Иркутский государственный университет путей сообщения (ФГБОУ ВО ИрГУПС) Method of determining the degree of magnetic induction in abnormal losses of a transformer core

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