CN101813756A - Method for manufacturing transient high-frequency magnetic field of power system - Google Patents
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Abstract
Description
技术领域technical field
本发明属于电力系统时变磁场测量技术领域,尤其涉及一种电力系统瞬态高频磁场的测量方法。The invention belongs to the technical field of time-varying magnetic field measurement in power systems, and in particular relates to a method for measuring transient high-frequency magnetic fields in power systems.
背景技术Background technique
变电站等存在高电压、大电流设备的场所,电磁环境非常复杂。不论是从了解和优化电气设备性能的角度出发,还是从分析电磁环境对人的生理影响的角度考虑,都需要对相关的电磁环境进行准确测量。电磁环境包括电场和磁场两大方面,需分别根据不同的原理进行测量。Substations and other places where there are high-voltage and high-current equipment, the electromagnetic environment is very complicated. Whether it is from the perspective of understanding and optimizing the performance of electrical equipment, or from the perspective of analyzing the physiological impact of the electromagnetic environment on people, it is necessary to accurately measure the relevant electromagnetic environment. The electromagnetic environment includes two aspects of electric field and magnetic field, which need to be measured according to different principles.
磁场测量是指空间或磁性材料中磁通、磁感应强度(磁通密度)、磁场强度等的测量。空间的磁感应强度与磁场强度成线性关系,因而空间磁场测量的主要测量量是磁感应强度。Magnetic field measurement refers to the measurement of magnetic flux, magnetic induction (magnetic flux density), magnetic field strength, etc. in space or magnetic materials. The magnetic induction intensity in space is linearly related to the magnetic field intensity, so the main measurement quantity of the space magnetic field measurement is the magnetic induction intensity.
恒定磁场的测量较容易,方法也比较多。常用的测量仪器有:力矩磁强计、旋转线圈磁强计、磁通门磁强计、霍尔效应磁强计、核磁共振磁强计、磁位计,或配合冲击检流计进行测量等。The measurement of a constant magnetic field is easier and there are many methods. Commonly used measuring instruments are: torque magnetometer, rotating coil magnetometer, fluxgate magnetometer, Hall effect magnetometer, nuclear magnetic resonance magnetometer, magnetometer, or with impact galvanometer for measurement, etc. .
时变磁场的测量通常是根据法拉第电磁感应定律,将磁场测量问题转变为电量的测量。这一方法需要有一个测量线圈,将其置于待测磁场中,磁场随时间变化会在线圈中产生感应电动势e=-dψ/dt,式中ψ为测量线圈交链的磁链。若线圈的面积足够小,则可认为线圈内磁场的分布是均匀的,那么e=-NSdB/dt,式中N为测量线圈的匝数,S为测量线圈的面积,B为垂直于测量线圈所在平面的磁感应强度分量,B的方向与e的方向满足右手螺旋关系。The measurement of time-varying magnetic field is usually based on Faraday's law of electromagnetic induction, which converts the problem of magnetic field measurement into the measurement of electric quantity. This method requires a measuring coil, which is placed in the magnetic field to be measured, and the magnetic field changes with time to generate an induced electromotive force e=-dψ/dt in the coil, where ψ is the flux linkage of the measuring coil. If the area of the coil is small enough, it can be considered that the distribution of the magnetic field in the coil is uniform, then e=-NSdB/dt, where N is the number of turns of the measuring coil, S is the area of the measuring coil, and B is perpendicular to the measuring coil The magnetic induction intensity component of the plane, the direction of B and the direction of e satisfy the right-handed spiral relationship.
目前基于上述原理主要有两种测量方法,其一是直接测量感应电动势,因为感应电动势与磁链的变化率成正比,所以测得的只是磁感应强度对时间的导数,而不是磁感应强度本身,需要另加积分电路,带来额外的误差;其二是在测量线圈中串联采样电阻,测量采样电阻上的电压,此时因测量线圈闭合,满足方程e+Ri+Ldi/dt=0,式中,i为测量线圈中的电流,R为采样电阻的阻值,L为测量线圈的等效电感,由上式可见,采样电阻上的电压与磁感应强度既非线性关系,也非导数关系,它们之间的具体关系与参数R、L以及磁场的变化率有关。由此可见,目前基于电磁感应原理测量磁场的方法均不能准确反映空间的磁感应强度。At present, there are mainly two measurement methods based on the above principles. One is to directly measure the induced electromotive force, because the induced electromotive force is proportional to the rate of change of the flux linkage, so what is measured is only the derivative of the magnetic induction intensity with respect to time, not the magnetic induction intensity itself. Adding an integral circuit brings additional errors; the second is to connect the sampling resistor in series in the measuring coil to measure the voltage on the sampling resistor. At this time, because the measuring coil is closed, the equation e+Ri+Ldi/dt=0 is satisfied, where , i is the current in the measuring coil, R is the resistance value of the sampling resistor, and L is the equivalent inductance of the measuring coil. It can be seen from the above formula that the voltage on the sampling resistor and the magnetic induction intensity are neither nonlinear nor derivative. The specific relationship between them is related to the parameters R, L and the rate of change of the magnetic field. It can be seen that the current methods of measuring the magnetic field based on the principle of electromagnetic induction cannot accurately reflect the magnetic induction intensity of the space.
利用霍尔原理可以测量正弦稳态磁场,但对于瞬态磁场的测量则比较困难,误差较大。The sinusoidal steady-state magnetic field can be measured using the Hall principle, but it is more difficult to measure the transient magnetic field, and the error is large.
发明内容Contents of the invention
针对上述时变磁场测量方法的不足,本发明提供了一种电力系统瞬态高频磁场测量方法,其特征在于:Aiming at the deficiencies of the above-mentioned time-varying magnetic field measurement method, the present invention provides a method for measuring the transient high-frequency magnetic field of a power system, which is characterized in that:
将测量线圈直接闭合,这样测量线圈中的电流是电感电流,测量线圈中的感应电动势与测量线圈的等效电感的电压平衡,其表达式为e+Ldi/dt=0,将e=-NSdB/dt代入,可知测量线圈中的电流与磁感应强度成线性关系,因而将该电流作为被测量能准确反映空间的磁感应强度。Close the measuring coil directly, so that the current in the measuring coil is the inductive current, the induced electromotive force in the measuring coil is balanced with the voltage of the equivalent inductance of the measuring coil, its expression is e+Ldi/dt=0, and e=-NSdB Substituting /dt, it can be seen that the current in the measuring coil has a linear relationship with the magnetic induction intensity, so the current is used as the measured magnetic induction intensity that can accurately reflect the space.
为了避免在测量线圈中串入采样电阻,本发明采用磁耦合的方式,将测量线圈与电流探头的线圈通过磁环进行磁耦合,测量线圈1闭合并穿过磁环,电流探头的线圈也穿过磁环。根据磁耦合的原理可知,电流探头的线圈中的电流与测量线圈中的电流成比例关系。光电转换器与电流探头相连,将电量转换为光信号,通过光纤传送到处理和存储设备。In order to avoid connecting the sampling resistor in series in the measuring coil, the present invention adopts a magnetic coupling method, and magnetically couples the measuring coil and the coil of the current probe through a magnetic ring, the measuring coil 1 is closed and passes through the magnetic ring, and the coil of the current probe also passes through the magnetic ring. over the ring. According to the principle of magnetic coupling, the current in the coil of the current probe is proportional to the current in the measuring coil. The optical-to-electrical converter is connected to the current probe to convert the electrical quantity into an optical signal, which is transmitted to the processing and storage device through the optical fiber.
本发明将磁感应强度的测量转变为电流的测量,能够准确测量正弦稳态磁场,尤其可以测量瞬态高频磁场。本发明可以普遍应用于电磁环境中的瞬态高频磁场的测量,尤其是电力系统的发电厂、变电站等其它存在强磁场的环境。The invention converts the measurement of the magnetic induction intensity into the measurement of the current, can accurately measure the sinusoidal steady-state magnetic field, and can especially measure the transient high-frequency magnetic field. The invention can be generally applied to the measurement of transient high-frequency magnetic fields in electromagnetic environments, especially in power plants, substations and other environments with strong magnetic fields in power systems.
附图说明Description of drawings
下面结合附图对本发明作详细说明:The present invention is described in detail below in conjunction with accompanying drawing:
图1为本发明的原理框图;Fig. 1 is a block diagram of the present invention;
图2为本发明的测量线圈与电流探头的线圈通过磁环进行磁耦合的示意图;Fig. 2 is the schematic diagram that the measuring coil of the present invention and the coil of current probe carry out magnetic coupling through magnetic ring;
图3为本发明的测量线圈与高精度电流互感器通过磁环耦合的示意图。Fig. 3 is a schematic diagram of the coupling between the measuring coil and the high-precision current transformer through the magnetic ring of the present invention.
附图标记:Reference signs:
1-测量线圈、2-磁环、3-电流探头的线圈、4-电流探头、1-Measuring coil, 2-Magnetic ring, 3-Current probe coil, 4-Current probe,
5-光电转换器、6-处理和存储设备、7-高精度电流互感器。5-photoelectric converter, 6-processing and storage equipment, 7-high precision current transformer.
具体实施方式Detailed ways
实施例一Embodiment one
如图1所示,测量线圈1置于待测磁场中,因磁场随时间变化,在测量线圈1中产生感应电动势。若测量线圈1的面积相对待测磁场的分布足够小,则可认为测量线圈1内的磁场是均匀分布的,测量线圈1交链的磁通与磁感应强度成正比。As shown in FIG. 1 , the measuring coil 1 is placed in the magnetic field to be measured. Since the magnetic field changes with time, an induced electromotive force is generated in the measuring coil 1 . If the area of the measuring coil 1 is small enough relative to the distribution of the magnetic field to be measured, it can be considered that the magnetic field in the measuring coil 1 is uniformly distributed, and the interlinked magnetic flux of the measuring coil 1 is proportional to the magnetic induction intensity.
测量线圈1闭合并穿过磁环2,测量线圈1中的感应电动势与测量线圈1的等效电感的电压平衡,因而可知磁感应强度与测量线圈1中的电流成线性关系。电流探头4的线圈3也穿过磁环2,如图2所示。根据磁耦合原理,可知线圈3的电流与测量线圈1的电流成线性关系,因而可得线圈3的电流与磁感应强度成线性关系。光电转换器5与电流探头4相连,并将电量转换为光信号,通过光纤传送到处理和存储设备6。处理和存储设备6首先要将光信号转换为数字量,对测得的数据进行保存和计算,通过人机交互界面显示测量结果。因为磁感应强度是矢量,所以测量电磁环境的磁场时,每一点都应该按照直角坐标系测量三个分量,才能合成得到该点的磁感应强度的大小和方向。磁感应强度除以真空的磁导率即得到该点的磁场强度。The measuring coil 1 is closed and passes through the magnetic ring 2, and the induced electromotive force in the measuring coil 1 is balanced with the voltage of the equivalent inductance of the measuring coil 1, so it can be seen that the magnetic induction intensity has a linear relationship with the current in the measuring coil 1. The
实施例二Embodiment two
如图3所示,测量线圈1置于待测磁场中,磁环2穿过测量线圈1,高精度电流互感器7实现了图1中线圈3、电流探头4、光电转换器5、处理和存储设备6的功能,磁环2也是高精度电流互感器7的组成部分。As shown in Figure 3, the measuring coil 1 is placed in the magnetic field to be measured, the magnetic ring 2 passes through the measuring coil 1, and the high-precision current transformer 7 realizes the
具体实施方式可以归纳为:测量线圈1穿过磁环2,并且测量线圈1直接闭合。将测量线圈1置于待测磁场中,测量线圈1中会产生感应电流,该感应电流与垂直于测量线圈1包围平面的磁感应强度B的分量成线性关系。用高精度电流互感器7测得测量线圈1中的感应电流,从而可测得与测量线圈1包围平面垂直的磁感应强度B的分量。测量电磁环境的磁场时,每一点都应该按照直角坐标系测量三个分量,才能合成得到该点的磁感应强度的大小和方向。磁感应强度除以真空的磁导率即得到该点的磁场强度。The specific implementation method can be summarized as follows: the measuring coil 1 passes through the magnetic ring 2, and the measuring coil 1 is directly closed. When the measuring coil 1 is placed in the magnetic field to be measured, an induced current will be generated in the measuring coil 1 , and the induced current has a linear relationship with the component of the magnetic induction intensity B perpendicular to the plane surrounded by the measuring coil 1 . The induced current in the measuring coil 1 is measured by a high-precision current transformer 7, so that the component of the magnetic induction intensity B perpendicular to the plane surrounded by the measuring coil 1 can be measured. When measuring the magnetic field of the electromagnetic environment, each point should measure three components according to the Cartesian coordinate system, so as to synthesize the magnitude and direction of the magnetic induction intensity of the point. The magnetic field strength at that point is obtained by dividing the magnetic induction by the magnetic permeability of the vacuum.
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Cited By (6)
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CN102495382A (en) * | 2011-11-30 | 2012-06-13 | 四川电力科学研究院 | Transient magnetic field recorder |
CN102621507A (en) * | 2012-04-14 | 2012-08-01 | 河北工业大学 | Obtaining method of direct current magnetic biasing hysteresis loop of transformer core material |
CN103134971A (en) * | 2011-11-29 | 2013-06-05 | 上海舜宇海逸光电技术有限公司 | Conductor current measurement device |
CN103353584A (en) * | 2013-06-29 | 2013-10-16 | 西北矿冶研究院 | High-frequency magnetic field detecting and shielding device |
CN103398794A (en) * | 2013-07-29 | 2013-11-20 | 哈尔滨电机厂有限责任公司 | On-line monitoring system for end parameters of large power generating equipment |
CN113777386A (en) * | 2021-11-11 | 2021-12-10 | 武汉精熔潮电气科技有限公司 | Method for detecting steady-state transient current by Hall based on partial iron core and application thereof |
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Cited By (8)
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CN103134971A (en) * | 2011-11-29 | 2013-06-05 | 上海舜宇海逸光电技术有限公司 | Conductor current measurement device |
CN103134971B (en) * | 2011-11-29 | 2015-10-21 | 思源电气股份有限公司 | Conductor current measurement device |
CN102495382A (en) * | 2011-11-30 | 2012-06-13 | 四川电力科学研究院 | Transient magnetic field recorder |
CN102621507A (en) * | 2012-04-14 | 2012-08-01 | 河北工业大学 | Obtaining method of direct current magnetic biasing hysteresis loop of transformer core material |
CN103353584A (en) * | 2013-06-29 | 2013-10-16 | 西北矿冶研究院 | High-frequency magnetic field detecting and shielding device |
CN103353584B (en) * | 2013-06-29 | 2016-04-13 | 西北矿冶研究院 | High-frequency magnetic field detecting and shielding device |
CN103398794A (en) * | 2013-07-29 | 2013-11-20 | 哈尔滨电机厂有限责任公司 | On-line monitoring system for end parameters of large power generating equipment |
CN113777386A (en) * | 2021-11-11 | 2021-12-10 | 武汉精熔潮电气科技有限公司 | Method for detecting steady-state transient current by Hall based on partial iron core and application thereof |
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