CN108645372B - Large-span transmission conductor suspension point dynamic bending strain measurement method - Google Patents

Large-span transmission conductor suspension point dynamic bending strain measurement method Download PDF

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CN108645372B
CN108645372B CN201810567111.9A CN201810567111A CN108645372B CN 108645372 B CN108645372 B CN 108645372B CN 201810567111 A CN201810567111 A CN 201810567111A CN 108645372 B CN108645372 B CN 108645372B
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suspension point
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CN108645372A (en
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阳林
冯展浩
郝艳捧
甘久林
李立浧
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South China University of Technology SCUT
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    • GPHYSICS
    • G01MEASURING; TESTING
    • G01BMEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
    • G01B21/00Measuring arrangements or details thereof, where the measuring technique is not covered by the other groups of this subclass, unspecified or not relevant
    • G01B21/32Measuring arrangements or details thereof, where the measuring technique is not covered by the other groups of this subclass, unspecified or not relevant for measuring the deformation in a solid
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01LMEASURING FORCE, STRESS, TORQUE, WORK, MECHANICAL POWER, MECHANICAL EFFICIENCY, OR FLUID PRESSURE
    • G01L1/00Measuring force or stress, in general
    • G01L1/24Measuring force or stress, in general by measuring variations of optical properties of material when it is stressed, e.g. by photoelastic stress analysis using infrared, visible light, ultraviolet
    • G01L1/242Measuring force or stress, in general by measuring variations of optical properties of material when it is stressed, e.g. by photoelastic stress analysis using infrared, visible light, ultraviolet the material being an optical fibre
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01PMEASURING LINEAR OR ANGULAR SPEED, ACCELERATION, DECELERATION, OR SHOCK; INDICATING PRESENCE, ABSENCE, OR DIRECTION, OF MOVEMENT
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Abstract

本发明公开了一种大跨越输电导线悬挂点动弯应变测量方法,包括以下步骤:S1、监测导线微风振动状态,采用拉力传感器持续测量导线水平张力;S2、监测架空输电线环境状况,采用风速测量仪持续测量导线运行时的风速;S3、根据所测风速,利用能量平衡法计算出导线微风振动的特征参量;S4、利用求解所得导线微风振动的振幅以及频率代入已知导线振动的惯性力求解获得导线振动稳定时的惯性力F,将惯性力F代替考虑电线刚度的悬挂点处静态弯曲应力关系式中的静态支点反力,得到导线微风振动时悬挂点处的动弯应力。所述方法通过测量导线运行的水平张力和风速来估算悬挂点动弯应变,能更加准确地对大跨越输电导线的动弯应变值进行测量,避免事故的发生。

Figure 201810567111

The invention discloses a method for measuring the jogging bending strain of a large-span power transmission wire, comprising the following steps: S1, monitoring the breeze vibration state of the wire, and using a tension sensor to continuously measure the horizontal tension of the wire; S2, monitoring the environmental condition of the overhead transmission line, using the wind speed The measuring instrument continuously measures the wind speed when the wire is running; S3. According to the measured wind speed, use the energy balance method to calculate the characteristic parameters of the wire breeze vibration; S4. Use the amplitude and frequency of the obtained wire breeze vibration to substitute the known inertial force of the wire vibration Solve to obtain the inertial force F when the wire is vibrating stable, replace the inertial force F with the static fulcrum reaction force in the static bending stress relationship at the suspension point considering the wire stiffness, and obtain the dynamic bending stress at the suspension point when the wire vibrates in the breeze. The method estimates the dynamic bending strain of the suspension point by measuring the horizontal tension and wind speed of the running wire, and can measure the dynamic bending strain value of the large-span transmission wire more accurately, thereby avoiding the occurrence of accidents.

Figure 201810567111

Description

一种大跨越输电导线悬挂点动弯应变测量方法A method for measuring long-span transmission wire suspension point-bending strain

技术领域technical field

本发明涉及电力领域中的架空导线微风振动在线监测技术领域,特别涉及一种大跨越输电导线悬挂点动弯应变测量方法。The invention relates to the technical field of on-line monitoring of breeze vibration of overhead wires in the field of electric power, in particular to a method for measuring the bending strain of a large-span power transmission wire by hanging point motion.

背景技术Background technique

输电线路的微风振动又称涡激振动,当风速约为0.5m/s~10m/s的稳定风吹向输电线时,在导线/地线的背风侧产生上下交替的卡门旋涡,引起上下交变的力作用于输电线上,使其在垂直平面内发生上下有规律的波浪状往复运动。微风振动的频率在3Hz~150Hz之间,最大振幅一般不大于输电线直径的1~2倍,振动的持续时间一般达数小时,有时可达数日不止。工程上常以导线振动时由于弯曲而产生的横截面应变值即动弯应变值来评定微风振动的强度。振动波在悬挂点处形成波节点,受悬垂线夹的约束该节点不能自由旋转,因此常出现比档距中更大的动弯应变值,导线的疲劳断股常于此发生。The breeze vibration of the transmission line is also known as the vortex-induced vibration. When the stable wind with a wind speed of about 0.5m/s ~ 10m/s blows to the transmission line, alternating up and down Karman vortices are generated on the leeward side of the conductor/ground wire, causing up and down crossovers. The variable force acts on the transmission line, causing it to have a regular wave-like reciprocating motion up and down in the vertical plane. The frequency of breeze vibration is between 3Hz and 150Hz, the maximum amplitude is generally not greater than 1 to 2 times the diameter of the transmission line, and the duration of vibration is generally several hours, sometimes more than several days. In engineering, the cross-sectional strain value, that is, the dynamic bending strain value, is often used to evaluate the strength of the breeze vibration due to the bending of the wire when it vibrates. The vibration wave forms a wave node at the suspension point, and the node cannot rotate freely due to the constraint of the suspension clamp, so a larger dynamic bending strain value than the span often occurs, and the fatigue strand of the wire often occurs here.

《导线振动测量标准化》认为测量线夹出口89mm处的电线对线夹的相对位移A89与导线悬挂点处的动弯应变成线性关系,而与振动频率、波长、张力、档距和线夹有、无转动等因素基本无关。据此,目前普遍采用结构简单,加工、安装方便,具有良好机电耦合特性的悬臂梁式传感器通过测量线夹出口89mm处的弯曲振幅来计算悬挂点处的动弯应变。但根据实测资料对比,该线性关系受到振动频率、振幅、电线张力和刚度等因素的影响,可能会有±50%的误差。对于大跨越所使用的各特种导线,影响更大,尤其是大跨越输电导线发生微风振动时,导线的水平张力无法认为保持不变,因此不能准确估算得到大跨越输电导线悬挂点处的动弯应变。"Wire Vibration Measurement Standardization" considers that the relative displacement A89 of the wire to the wire clamp at the outlet of the wire clamp at 89mm and the dynamic bending strain at the suspension point of the wire become a linear relationship, and it is related to the vibration frequency, wavelength, tension, span and wire. Factors such as clamping and non-rotation are basically irrelevant. According to this, cantilever beam sensors with simple structure, convenient processing and installation, and good electromechanical coupling characteristics are generally used at present to calculate the dynamic bending strain at the suspension point by measuring the bending amplitude at 89mm of the outlet of the wire clamp. However, according to the comparison of the measured data, the linear relationship is affected by factors such as vibration frequency, amplitude, wire tension and stiffness, and there may be an error of ±50%. For the special conductors used in large spans, the impact is greater, especially when the large span transmission conductors vibrate in the breeze, the horizontal tension of the conductors cannot be considered to remain unchanged, so the dynamic bending at the suspension points of the large span transmission conductors cannot be accurately estimated. strain.

发明内容SUMMARY OF THE INVENTION

本发明的目的在于克服上述现有技术的不足,针对大跨越输电导线的微风振动,考虑振动频率、波长、张力、档距以及电线刚度的影响,提供了一种大跨越输电导线悬挂点动弯应变测量方法,所述方法通过测量导线运行的水平张力和风速来估算悬挂点动弯应变,能更加准确地对大跨越输电导线的动弯应变值进行测量,从而能更加准确地评估输电导线的运行状况,避免事故的发生。The object of the present invention is to overcome the deficiencies of the above-mentioned prior art, and for the breeze vibration of the large-span transmission wire, considering the influence of vibration frequency, wavelength, tension, span and wire stiffness, a large-span transmission wire suspension jog bend is provided. A strain measurement method, the method estimates the dynamic bending strain of the suspension point by measuring the horizontal tension and wind speed of the running wire, and can more accurately measure the dynamic bending strain value of the large-span transmission wire, so as to more accurately evaluate the dynamic bending strain of the transmission wire. operating conditions to avoid accidents.

本发明的目的可以通过如下技术方案实现:The purpose of the present invention can be realized by following technical scheme:

一种大跨越输电导线悬挂点动弯应变测量方法,所述方法包括以下步骤:A method for measuring long-span transmission wire suspension point-bending strain, the method comprises the following steps:

S1、监测导线微风振动状态,采用拉力传感器持续测量导线水平张力,记录下导线水平张力的变化;S1. Monitor the breeze vibration state of the wire, use the tension sensor to continuously measure the horizontal tension of the wire, and record the change of the horizontal tension of the wire;

S2、监测架空输电线环境状况,采用风速测量仪持续测量导线运行时的风速;S2. Monitor the environmental condition of the overhead transmission line, and use an anemometer to continuously measure the wind speed when the wire is running;

S3、根据步骤S2所测风速,利用能量平衡法计算出导线微风振动的特征参量,即微风振动稳定时,风输入导线的功率与导线自阻尼功率相等,利用风速与导线振幅、频率的关系式获得导线微风振动的特征参量,即导线微风振动的振幅和频率;S3. According to the wind speed measured in step S2, use the energy balance method to calculate the characteristic parameters of the wire breeze vibration, that is, when the breeze vibration is stable, the power of the wind input wire is equal to the self-damping power of the wire, and the relationship between the wind speed and the wire amplitude and frequency is used. Obtain the characteristic parameters of the wire breeze vibration, that is, the amplitude and frequency of the wire breeze vibration;

S4、根据步骤S1和步骤S3对导线悬挂点处的动弯应变进行估算,即利用求解所得导线微风振动的振幅A0以及频率f代入已知导线振动的惯性力求解获得导线振动稳定时的惯性力F,将惯性力F代替考虑电线刚度的悬挂点处静态弯曲应力关系式中的静态支点反力,得到导线微风振动时悬挂点处的动弯应力。S4. Estimate the dynamic bending strain at the suspension point of the wire according to step S1 and step S3, that is, use the amplitude A 0 and frequency f of the obtained wire breeze vibration to substitute the inertial force of the known wire vibration to obtain the inertia when the wire vibration is stable. Force F, the inertial force F is replaced by the static fulcrum reaction force in the static bending stress relationship at the suspension point considering the stiffness of the wire, and the dynamic bending stress at the suspension point when the wire vibrates in the breeze is obtained.

进一步地,步骤S1中,具体通过将拉力传感器布置在线夹出口处,通过拉力传感器连续测量导线的水平拉力变化情况来实现。Further, in step S1, it is specifically realized by arranging the tension sensor at the outlet of the wire clamp, and continuously measuring the change of the horizontal tension of the wire through the tension sensor.

进一步地,所述拉力传感器采用光纤光栅应变传感器。Further, the tensile force sensor adopts a fiber grating strain sensor.

进一步地,步骤S2中,具体通过将风速测量仪安装在悬挂导线的线夹处,通过风速测量仪持续测量导线所处环境的风速来实现。Further, in step S2, it is specifically realized by installing the anemometer at the clip of the hanging wire, and continuously measuring the wind speed of the environment where the wire is located by the anemometer.

进一步地,步骤S3的具体过程为:Further, the specific process of step S3 is:

首先,计算风输入导线的功率PW,公式如下:First, calculate the power P W of the wind input wire with the following formula:

Figure BDA0001684815660000021
Figure BDA0001684815660000021

式中,

Figure BDA0001684815660000022
表示动态升力系数,与风速有关;ρ表示空气密度,单位为kg/m3;V表示风速,单位为m/s;D表示导线外径,单位为m;f表示导线微风振动的频率,单位为Hz;A0表示导线微风振动的振幅,单位为m;其中动态升力系数
Figure BDA0001684815660000023
的求解公式如下:In the formula,
Figure BDA0001684815660000022
Represents the dynamic lift coefficient, which is related to the wind speed; ρ represents the air density, the unit is kg/m 3 ; V represents the wind speed, the unit is m/s; D represents the outer diameter of the wire, the unit is m; f represents the frequency of the wind vibration of the wire, the unit is Hz; A 0 represents the amplitude of the breeze vibration of the wire, the unit is m; where the dynamic lift coefficient
Figure BDA0001684815660000023
The solution formula is as follows:

Figure BDA0001684815660000024
Figure BDA0001684815660000024

式中,s表示司脱罗哈数,与圆柱体的雷诺数有关,在实用范围内为0.185~0.2,此处采用0.2;In the formula, s represents the Sterloha number, which is related to the Reynolds number of the cylinder, and is 0.185 to 0.2 in the practical range, and 0.2 is used here;

然后,计算导线的自阻尼功率Pc,导线自阻尼是表征导线振动时自身消耗或吸收能量的能力,是单位长度导线所消耗的功率,公式如下:Then, calculate the self-damping power P c of the wire. The self-damping of the wire represents the ability of the wire to consume or absorb energy when it vibrates. It is the power consumed by the unit length of the wire. The formula is as follows:

Figure BDA0001684815660000031
Figure BDA0001684815660000031

式中,y0表示导线的最大双振幅,K、β、α三个系数因导线规格而异,能够通过导线自阻尼测试获得;如AACSR-400型钢芯铝合金绞线,K=5.428×10-5、α=2.967-4.174f×10-3、β=5.0。In the formula, y 0 represents the maximum double amplitude of the wire, and the three coefficients K, β, and α vary with the wire specifications, and can be obtained through the wire self-damping test; such as AACSR-400 steel-cored aluminum alloy stranded wire, K=5.428×10 -5 , α=2.967-4.174f×10 -3 , β=5.0.

最后,计算导线微风振动的振幅A0:当其他各参数已知时,以导线微风振动的频率f为参量坐标,以导线的最大双振幅y0为自变量,绘制出风输入导线的功率PW与导线的自阻尼功率Pc的关系图,相同频率的PW和Pc曲线交点对应下的振幅y0即为功率平衡点的稳定振幅,即导线微风振动的振幅A0;导线微风振动稳定时,振动频率f能够表示为风速V的单一函数:Finally, calculate the amplitude A 0 of the wire breeze vibration: when other parameters are known, take the frequency f of the wire breeze vibration as the parameter coordinate, and use the maximum double amplitude y 0 of the wire as the independent variable to draw the wind input power P of the wire The relationship between W and the self-damping power P c of the wire, the amplitude y 0 corresponding to the intersection of the P W and P c curves of the same frequency is the stable amplitude of the power balance point, that is, the amplitude A 0 of the wire breeze vibration; the wire breeze vibration When stable, the vibration frequency f can be expressed as a single function of the wind speed V:

Figure BDA0001684815660000032
Figure BDA0001684815660000032

式中,s表示司脱罗哈数,与圆柱体的雷诺数有关,在实用范围内为0.185~0.2,此处采用0.2。In the formula, s represents the Sterloha number, which is related to the Reynolds number of the cylinder.

进一步地,所述步骤S4具体包括以下过程:Further, the step S4 specifically includes the following process:

S4.1、根据以下式子计算半波长内导线振动稳定时的惯性力F:S4.1. Calculate the inertial force F when the vibration of the wire is stable within half-wavelength according to the following formula:

Figure BDA0001684815660000033
Figure BDA0001684815660000033

理论上,微风振动稳定时,式中的f应为考虑电线刚度的固有频率,而本发明认为输电导线是张紧的小刚度梁,实际档距可达数百米,忽略自身的抗弯刚度对导线振动的惯性力F误差一般不超过5%,因此该惯性力的计算是偏于安全的;Theoretically, when the breeze vibration is stable, f in the formula should be the natural frequency considering the stiffness of the wire, and the present invention considers the transmission wire to be a tensioned beam with small stiffness, and the actual span can reach hundreds of meters, ignoring its own bending stiffness. The inertial force F error for wire vibration is generally not more than 5%, so the calculation of the inertial force is relatively safe;

式中,m表示导线单位长度的质量,λ表示档内导线振动的波长,单位为m,振动稳定时由以下式子表示:In the formula, m represents the mass of the wire per unit length, λ represents the wavelength of the vibration of the wire in the gear, the unit is m, and the vibration is stable by the following formula:

Figure BDA0001684815660000034
Figure BDA0001684815660000034

式中,T0表示导线水平张力;In the formula, T 0 represents the horizontal tension of the wire;

S4.2、根据以下式子计算考虑电线刚度的悬挂点处静态弯曲应力σ:S4.2. Calculate the static bending stress σ at the suspension point considering the stiffness of the wire according to the following formula:

Figure BDA0001684815660000035
Figure BDA0001684815660000035

式中,E表示导线的弹性系数,参考导线参数,例如LGJ-800/100导线的弹性系数为67000N/mm2;J表示导线断面的惯性矩,对直径为d的单股导线J=πd4/64;C表示导线断面上所求最大弯曲应力点到弯曲中性层间的距离此处指股丝的半径r,参考导线参数;p0表示试验档中央所施加的集中荷载,单位为N;l表示档距,h表示悬挂点的高度差,

Figure BDA0001684815660000041
为静态支点反力;In the formula, E represents the elastic coefficient of the wire, refer to the parameters of the wire, for example, the elastic coefficient of the LGJ-800/100 wire is 67000N/mm 2 ; J represents the moment of inertia of the wire section, and for a single-strand wire with a diameter of d, J=πd 4 /64; C represents the distance from the point of maximum bending stress on the conductor section to the bending neutral layer, where the radius r of the strand refers to the conductor parameters; p 0 represents the concentrated load applied in the center of the test file, the unit is N ; l represents the gear distance, h represents the height difference of the suspension point,
Figure BDA0001684815660000041
is the static fulcrum reaction force;

S4.3、将导线振动的惯性力F代替考虑电线刚度的悬挂点处静态弯曲应力关系式中的静态支点反力,得到导线微风振动时悬挂点处的动弯应力σcS4.3. Substitute the inertial force F of the wire vibration for the static fulcrum reaction force in the static bending stress relationship at the suspension point considering the wire stiffness, and obtain the dynamic bending stress σ c at the suspension point when the wire vibrates in the breeze:

Figure BDA0001684815660000042
Figure BDA0001684815660000042

导线微风振动时悬挂点处的动弯应力σc的单位为N/mm2,根据动弯应力与动弯应变的关系,得到导线微风振动时线夹处的动弯应变εcThe unit of dynamic bending stress σ c at the suspension point when the wire vibrates in breeze is N/mm 2 . According to the relationship between dynamic bending stress and dynamic bending strain, the dynamic bending strain ε c at the clamp when the wire vibrates in breeze is obtained:

Figure BDA0001684815660000043
Figure BDA0001684815660000043

导线微风振动时线夹处的动弯应变εc的单位为μεThe unit of dynamic bending strain ε c at the clip is μ ε when the wire vibrates in breeze.

本发明与现有技术相比,具有如下优点和有益效果:Compared with the prior art, the present invention has the following advantages and beneficial effects:

本发明提供的大跨越输电导线悬挂点动弯应变测量方法,通过测量导线运行的水平张力和风速来估算悬挂点动弯应变,一方面考虑输电导线振动频率、波长、以及电线刚度的问题,另一方面认为大跨越导线在微风振动下水平张力是随时改变的,能更加准确地对大跨越输电导线的动弯应变值进行测量,从而能更加准确地评估输电导线的运行状况,避免事故的发生。The method for measuring the jogging bending strain of a large-span transmission wire provided by the present invention estimates the jogging bending strain of the suspension by measuring the horizontal tension and wind speed of the running wire. On the one hand, it is believed that the horizontal tension of large-span conductors changes at any time under breeze vibration, and the dynamic bending strain value of large-span transmission conductors can be measured more accurately, so as to more accurately evaluate the operation of transmission conductors and avoid accidents. .

附图说明Description of drawings

图1为本发明实施例大跨越输电导线悬挂点动弯应变测量方法的流程图。FIG. 1 is a flow chart of a method for measuring the bending strain of a large-span transmission wire suspension point according to an embodiment of the present invention.

图2为本发明实施例大跨越输电导线悬挂点动弯应变测量方法中相关测量装置的安装示意图。FIG. 2 is a schematic diagram of the installation of a related measuring device in the method for measuring the bending strain of a suspension point of a large-span transmission wire according to an embodiment of the present invention.

其中,1-杆塔横担,2-悬垂绝缘子串,3-光纤光栅拉力传感器,4-风速测量仪,5-架空输电线路导线。Among them, 1- pole tower cross arm, 2- pendant insulator string, 3- fiber grating tension sensor, 4- wind speed measuring instrument, 5- overhead transmission line conductor.

具体实施方式Detailed ways

下面结合实施例及附图对本发明作进一步详细的描述,但本发明的实施方式不限于此。The present invention will be described in further detail below with reference to the embodiments and the accompanying drawings, but the embodiments of the present invention are not limited thereto.

实施例:Example:

本实施例提供的大跨越输电导线悬挂点动弯应变测量方法中相关测量装置的安装示意图如图2所示,包括杆塔横担(1)、悬垂绝缘子串(2)、光纤光栅拉力传感器(3)、风速测量仪(4)和架空输电线路导线(5),所述方法的流程图如图1所示,包括以下步骤:Figure 2 shows a schematic diagram of the installation of a related measuring device in the method for measuring long-span transmission wire suspension point-bending strain provided by this embodiment, including a pole tower cross arm (1), a suspension insulator string (2), and a fiber grating tension sensor (3). ), an anemometer (4) and an overhead transmission line wire (5), the flow chart of the method is shown in Figure 1 and includes the following steps:

S1、监测导线微风振动状态,采用拉力传感器持续测量导线水平张力,记录下导线水平张力的变化;具体通过将光纤光栅拉力传感器(3)布置在线夹出口处,通过光纤光栅拉力传感器(3)连续测量导线的水平拉力变化情况来实现。S1. Monitor the breeze vibration state of the wire, use the tension sensor to continuously measure the horizontal tension of the wire, and record the change of the horizontal tension of the wire; specifically, by arranging the fiber grating tension sensor (3) at the outlet of the wire clamp, and continuously through the fiber grating tension sensor (3) It is realized by measuring the change of the horizontal tension of the wire.

S2、监测架空输电线环境状况,采用风速测量仪持续测量导线运行时的风速;具体通过将风速测量仪(4)安装在悬挂导线的线夹处,通过风速测量仪(4)持续测量导线所处环境的风速来实现。S2. Monitor the environmental condition of the overhead transmission line, and use an anemometer to continuously measure the wind speed when the wire is running; specifically, by installing the anemometer (4) at the clip of the hanging wire, and continuously measuring the wind speed by the anemometer (4) wind speed in the environment.

S3、根据步骤S2所测风速,利用能量平衡法计算出导线微风振动的特征参量,即微风振动稳定时,风输入导线的功率与导线自阻尼功率相等,利用风速与导线振幅、频率的关系式获得导线微风振动的特征参量,即导线微风振动的振幅和频率;具体过程为:首先,计算风输入导线的功率PW,公式如下:S3. According to the wind speed measured in step S2, use the energy balance method to calculate the characteristic parameters of the wire breeze vibration, that is, when the breeze vibration is stable, the power of the wind input wire is equal to the self-damping power of the wire, and the relationship between the wind speed and the wire amplitude and frequency is used. Obtain the characteristic parameters of the wire breeze vibration, that is, the amplitude and frequency of the wire breeze vibration; the specific process is: first, calculate the power P W of the wind input to the wire, the formula is as follows:

Figure BDA0001684815660000051
Figure BDA0001684815660000051

式中,

Figure BDA0001684815660000052
表示动态升力系数,与风速有关;ρ表示空气密度,单位为kg/m3;V表示风速,单位为m/s;D表示导线外径,单位为m;f表示导线微风振动的频率,单位为Hz;A0表示导线微风振动的振幅,单位为m;其中动态升力系数
Figure BDA0001684815660000053
的求解公式如下:In the formula,
Figure BDA0001684815660000052
Represents the dynamic lift coefficient, which is related to the wind speed; ρ represents the air density, the unit is kg/m 3 ; V represents the wind speed, the unit is m/s; D represents the outer diameter of the wire, the unit is m; f represents the frequency of the wind vibration of the wire, the unit is Hz; A 0 represents the amplitude of the breeze vibration of the wire, the unit is m; where the dynamic lift coefficient
Figure BDA0001684815660000053
The solution formula is as follows:

Figure BDA0001684815660000054
Figure BDA0001684815660000054

式中,s表示司脱罗哈数,与圆柱体的雷诺数有关,在实用范围内为0.185~0.2,此处采用0.2;In the formula, s represents the Sterloha number, which is related to the Reynolds number of the cylinder, and is 0.185 to 0.2 in the practical range, and 0.2 is used here;

然后,计算导线的自阻尼功率Pc,导线自阻尼是表征导线振动时自身消耗或吸收能量的能力,是单位长度导线所消耗的功率,公式如下:Then, calculate the self-damping power P c of the wire. The self-damping of the wire represents the ability of the wire to consume or absorb energy when it vibrates. It is the power consumed by the unit length of the wire. The formula is as follows:

Figure BDA0001684815660000055
Figure BDA0001684815660000055

式中,y0表示导线的最大双振幅,K、β、α三个系数因导线规格而异,能够通过导线自阻尼测试获得;如AACSR-400型钢芯铝合金绞线,K=5.428×10-5、α=2.967-4.174f×10-3、β=5.0。In the formula, y 0 represents the maximum double amplitude of the wire, and the three coefficients K, β, and α vary with the wire specifications, and can be obtained through the wire self-damping test; such as AACSR-400 steel-cored aluminum alloy stranded wire, K=5.428×10 -5 , α=2.967-4.174f×10 -3 , β=5.0.

最后,计算导线微风振动的振幅A0:当其他各参数已知时,以导线微风振动的频率f为参量坐标,以导线的最大双振幅y0为自变量,绘制出风输入导线的功率PW与导线的自阻尼功率Pc的关系图,相同频率的PW和Pc曲线交点对应下的振幅y0即为功率平衡点的稳定振幅,即导线微风振动的振幅A0;导线微风振动稳定时,振动频率f能够表示为风速V的单一函数:Finally, calculate the amplitude A 0 of the wire breeze vibration: when other parameters are known, take the frequency f of the wire breeze vibration as the parameter coordinate, and use the maximum double amplitude y 0 of the wire as the independent variable to draw the wind input power P of the wire The relationship between W and the self-damping power P c of the wire, the amplitude y 0 corresponding to the intersection of the P W and P c curves of the same frequency is the stable amplitude of the power balance point, that is, the amplitude A 0 of the wire breeze vibration; the wire breeze vibration When stable, the vibration frequency f can be expressed as a single function of the wind speed V:

Figure BDA0001684815660000061
Figure BDA0001684815660000061

式中,s表示司脱罗哈数,与圆柱体的雷诺数有关,在实用范围内为0.185~0.2,此处采用0.2。In the formula, s represents the Sterloha number, which is related to the Reynolds number of the cylinder.

S4、根据步骤S1和步骤S3对导线悬挂点处的动弯应变进行估算,即利用求解所得导线微风振动的振幅A0以及频率f代入已知导线振动的惯性力求解获得导线振动稳定时的惯性力F,将惯性力F代替考虑电线刚度的悬挂点处静态弯曲应力关系式中的静态支点反力,得到导线微风振动时悬挂点处的动弯应力。具体包括以下过程:S4. Estimate the dynamic bending strain at the suspension point of the wire according to step S1 and step S3, that is, use the amplitude A 0 and frequency f of the obtained wire breeze vibration to substitute the inertial force of the known wire vibration to obtain the inertia when the wire vibration is stable. Force F, the inertial force F is replaced by the static fulcrum reaction force in the static bending stress relationship at the suspension point considering the stiffness of the wire, and the dynamic bending stress at the suspension point when the wire vibrates in the breeze is obtained. Specifically, it includes the following processes:

S4.1、根据以下式子计算半波长内导线振动稳定时的惯性力F:S4.1. Calculate the inertial force F when the vibration of the wire is stable within half-wavelength according to the following formula:

Figure BDA0001684815660000062
Figure BDA0001684815660000062

理论上,微风振动稳定时,式中的f应为考虑电线刚度的固有频率,而本发明认为输电导线是张紧的小刚度梁,实际档距可达数百米,忽略自身的抗弯刚度对导线振动的惯性力F误差一般不超过5%,因此该惯性力的计算是偏于安全的;Theoretically, when the breeze vibration is stable, f in the formula should be the natural frequency considering the stiffness of the wire, and the present invention considers the transmission wire to be a tensioned beam with small stiffness, and the actual span can reach hundreds of meters, ignoring its own bending stiffness. The inertial force F error for wire vibration is generally not more than 5%, so the calculation of the inertial force is relatively safe;

式中,m表示导线单位长度的质量,λ表示档内导线振动的波长,单位为m,振动稳定时由以下式子表示:In the formula, m represents the mass of the wire per unit length, λ represents the wavelength of the vibration of the wire in the gear, the unit is m, and the vibration is stable by the following formula:

Figure BDA0001684815660000063
Figure BDA0001684815660000063

式中,T0表示导线水平张力;In the formula, T 0 represents the horizontal tension of the wire;

S4.2、根据以下式子计算考虑电线刚度的悬挂点处静态弯曲应力σ:S4.2. Calculate the static bending stress σ at the suspension point considering the stiffness of the wire according to the following formula:

Figure BDA0001684815660000064
Figure BDA0001684815660000064

式中,E表示导线的弹性系数,参考导线参数,例如LGJ-800/100导线的弹性系数为67000N/mm2;J表示导线断面的惯性矩,对直径为d的单股导线J=πd4/64;C表示导线断面上所求最大弯曲应力点到弯曲中性层间的距离此处指股丝的半径r,参考导线参数;p0表示试验档中央所施加的集中荷载,单位为N;l表示档距,h表示悬挂点的高度差,

Figure BDA0001684815660000071
为静态支点反力;In the formula, E represents the elastic coefficient of the wire, refer to the parameters of the wire, for example, the elastic coefficient of the LGJ-800/100 wire is 67000N/mm 2 ; J represents the moment of inertia of the wire section, and for a single-strand wire with a diameter of d, J=πd 4 /64; C represents the distance from the point of maximum bending stress on the conductor section to the bending neutral layer, where the radius r of the strand refers to the conductor parameters; p 0 represents the concentrated load applied in the center of the test file, the unit is N ; l represents the gear distance, h represents the height difference of the suspension point,
Figure BDA0001684815660000071
is the static fulcrum reaction force;

S4.3、将导线振动的惯性力F代替考虑电线刚度的悬挂点处静态弯曲应力关系式中的静态支点反力,得到导线微风振动时悬挂点处的动弯应力σcS4.3. Substitute the inertial force F of the wire vibration for the static fulcrum reaction force in the static bending stress relationship at the suspension point considering the wire stiffness, and obtain the dynamic bending stress σ c at the suspension point when the wire vibrates in the breeze:

Figure BDA0001684815660000072
Figure BDA0001684815660000072

导线微风振动时悬挂点处的动弯应力σc的单位为N/mm2,根据动弯应力与动弯应变的关系,得到导线微风振动时线夹处的动弯应变εcThe unit of dynamic bending stress σ c at the suspension point when the wire vibrates in breeze is N/mm 2 . According to the relationship between dynamic bending stress and dynamic bending strain, the dynamic bending strain ε c at the clamp when the wire vibrates in breeze is obtained:

Figure BDA0001684815660000073
Figure BDA0001684815660000073

导线微风振动时线夹处的动弯应变εc的单位为μεThe unit of dynamic bending strain ε c at the clip is μ ε when the wire vibrates in breeze.

以上所述,仅为本发明专利较佳的实施例,但本发明专利的保护范围并不局限于此,任何熟悉本技术领域的技术人员在本发明专利所公开的范围内,根据本发明专利的技术方案及其发明专利构思加以等同替换或改变,都属于本发明专利的保护范围。The above is only a preferred embodiment of the patent of the present invention, but the protection scope of the patent of the present invention is not limited to this. The technical solution and the invention patent concept of the invention are equivalently replaced or changed, all belong to the protection scope of the invention patent.

Claims (4)

1.一种大跨越输电导线悬挂点动弯应变测量方法,其特征在于,所述方法包括以下步骤:1. a large-span power transmission wire suspension point-motion bending strain measurement method, is characterized in that, described method comprises the following steps: S1、监测导线微风振动状态,采用拉力传感器持续测量导线水平张力,记录下导线水平张力的变化,具体通过将拉力传感器布置在线夹出口处,通过拉力传感器连续测量导线的水平拉力变化情况来实现;S1. Monitor the breeze vibration state of the wire, use the tension sensor to continuously measure the horizontal tension of the wire, and record the change of the horizontal tension of the wire. Specifically, the tension sensor is arranged at the outlet of the wire clamp, and the tension sensor is used to continuously measure the change of the horizontal tension of the wire. S2、监测架空输电线环境状况,采用风速测量仪持续测量导线运行时的风速;具体通过将风速测量仪安装在悬挂导线的线夹处,通过风速测量仪持续测量导线所处环境的风速来实现;S2. Monitor the environmental conditions of the overhead transmission line, and use an anemometer to continuously measure the wind speed when the wire is running; specifically, install the anemometer at the clip of the hanging wire, and use the anemometer to continuously measure the wind speed of the environment where the wire is located. ; S3、根据步骤S2所测风速,利用能量平衡法计算出导线微风振动的特征参量,即微风振动稳定时,风输入导线的功率与导线自阻尼功率相等,利用风速与导线振幅、频率的关系式获得导线微风振动的特征参量,即导线微风振动的振幅和频率;S3. According to the wind speed measured in step S2, use the energy balance method to calculate the characteristic parameters of the wire breeze vibration, that is, when the breeze vibration is stable, the power of the wind input wire is equal to the self-damping power of the wire, and the relationship between the wind speed and the wire amplitude and frequency is used. Obtain the characteristic parameters of the wire breeze vibration, that is, the amplitude and frequency of the wire breeze vibration; S4、根据步骤S1和步骤S3对导线悬挂点处的动弯应变进行估算,即利用求解所得导线微风振动的振幅A0以及频率f代入已知导线振动的惯性力求解获得导线振动稳定时的惯性力F,将惯性力F代替考虑电线刚度的悬挂点处静态弯曲应力关系式中的静态支点反力,得到导线微风振动时悬挂点处的动弯应力。S4. Estimate the dynamic bending strain at the suspension point of the wire according to step S1 and step S3, that is, use the amplitude A 0 and frequency f of the obtained wire breeze vibration to substitute the inertial force of the known wire vibration to obtain the inertia when the wire vibration is stable. Force F, the inertial force F is replaced by the static fulcrum reaction force in the static bending stress relationship at the suspension point considering the stiffness of the wire, and the dynamic bending stress at the suspension point when the wire vibrates in the breeze is obtained. 2.根据权利要求1所述的一种大跨越输电导线悬挂点动弯应变测量方法,其特征在于:所述拉力传感器采用光纤光栅应变传感器。2 . The method for measuring long-span power transmission wire suspension point-bending strain according to claim 1 , wherein the tension sensor is a fiber grating strain sensor. 3 . 3.根据权利要求1所述的一种大跨越输电导线悬挂点动弯应变测量方法,其特征在于,步骤S3的具体过程为:3. a kind of large-span transmission wire suspension point-motion bending strain measurement method according to claim 1, is characterized in that, the concrete process of step S3 is: 首先,计算风输入导线的功率PW,公式如下:First, calculate the power P W of the wind input wire with the following formula:
Figure FDA0002434908040000011
Figure FDA0002434908040000011
式中,
Figure FDA0002434908040000012
表示动态升力系数,与风速有关;ρ表示空气密度,单位为kg/m3;V表示风速,单位为m/s;D表示导线外径,单位为m;f表示导线微风振动的频率,单位为Hz;A0表示导线微风振动的振幅,单位为m;其中动态升力系数
Figure FDA0002434908040000013
的求解公式如下:
In the formula,
Figure FDA0002434908040000012
Represents the dynamic lift coefficient, which is related to the wind speed; ρ represents the air density, the unit is kg/m 3 ; V represents the wind speed, the unit is m/s; D represents the outer diameter of the wire, the unit is m; f represents the frequency of the wind vibration of the wire, the unit is Hz; A 0 represents the amplitude of the breeze vibration of the wire, the unit is m; where the dynamic lift coefficient
Figure FDA0002434908040000013
The solution formula is as follows:
Figure FDA0002434908040000014
Figure FDA0002434908040000014
式中,s表示司脱罗哈数,与圆柱体的雷诺数有关,在实用范围内为0.185~0.2,此处采用0.2;In the formula, s represents the Sterloha number, which is related to the Reynolds number of the cylinder, and is 0.185 to 0.2 in the practical range, and 0.2 is used here; 然后,计算导线的自阻尼功率Pc,公式如下:Then, calculate the self-damping power P c of the wire, the formula is as follows:
Figure FDA0002434908040000021
Figure FDA0002434908040000021
式中,y0表示导线的最大双振幅,K、β、α三个系数因导线规格而异,能够通过导线自阻尼测试获得;In the formula, y 0 represents the maximum double amplitude of the wire, and the three coefficients K, β, and α vary with the wire specifications, and can be obtained through the wire self-damping test; 最后,计算导线微风振动的振幅A0:当其他各参数已知时,以导线微风振动的频率f为参量坐标,以导线的最大双振幅y0为自变量,绘制出风输入导线的功率PW与导线的自阻尼功率Pc的关系图,相同频率的PW和Pc曲线交点对应下的振幅y0即为功率平衡点的稳定振幅,即导线微风振动的振幅A0;导线微风振动稳定时,振动频率f能够表示为风速V的单一函数:Finally, calculate the amplitude A 0 of the wire breeze vibration: when other parameters are known, take the frequency f of the wire breeze vibration as the parameter coordinate, and use the maximum double amplitude y 0 of the wire as the independent variable to draw the wind input power P of the wire The relationship between W and the self-damping power P c of the wire, the amplitude y 0 corresponding to the intersection of the P W and P c curves of the same frequency is the stable amplitude of the power balance point, that is, the amplitude A 0 of the wire breeze vibration; the wire breeze vibration When stable, the vibration frequency f can be expressed as a single function of the wind speed V:
Figure FDA0002434908040000022
Figure FDA0002434908040000022
式中,s表示司脱罗哈数,与圆柱体的雷诺数有关,在实用范围内为0.185~0.2,此处采用0.2。In the formula, s represents the Sterloha number, which is related to the Reynolds number of the cylinder.
4.根据权利要求3所述的一种大跨越输电导线悬挂点动弯应变测量方法,其特征在于,所述步骤S4具体包括以下过程:4. a kind of large-span transmission wire suspension point-motion bending strain measurement method according to claim 3, is characterized in that, described step S4 specifically comprises following process: S4.1、根据以下式子计算半波长内导线振动稳定时的惯性力F:S4.1. Calculate the inertial force F when the vibration of the wire is stable within half-wavelength according to the following formula:
Figure FDA0002434908040000023
Figure FDA0002434908040000023
式中,dx为任意微段电线,x为电线长度方向,m表示导线单位长度的质量,λ表示档内导线振动的波长,单位为m,振动稳定时由以下式子表示:In the formula, dx is any micro-segment wire, x is the length direction of the wire, m is the mass of the wire per unit length, λ is the wavelength of the wire vibration in the gear, the unit is m, and the vibration is stable by the following formula:
Figure FDA0002434908040000024
Figure FDA0002434908040000024
式中,T0表示导线水平张力;s表示司脱罗哈数;In the formula, T 0 represents the horizontal tension of the wire; s represents the Sterloha number; S4.2、根据以下式子计算考虑电线刚度的悬挂点处静态弯曲应力σ:S4.2. Calculate the static bending stress σ at the suspension point considering the stiffness of the wire according to the following formula:
Figure FDA0002434908040000025
Figure FDA0002434908040000025
式中,E表示导线的弹性系数;J表示导线断面的惯性矩,对导线外径为D的单股导线J=πD4/64;C表示导线断面上所求最大弯曲应力点到弯曲中性层间的距离,此处指股丝的半径r;p0表示试验档中央所施加的集中荷载,单位为N;l表示档距,h表示悬挂点的高度差,
Figure FDA0002434908040000031
为静态支点反力;
In the formula, E represents the elastic coefficient of the wire; J represents the moment of inertia of the wire section, and for a single-strand wire with an outer diameter of D, J=πD 4 /64; C represents the maximum bending stress point on the wire section to the bending neutrality The distance between layers, here refers to the radius r of the strands; p 0 represents the concentrated load applied in the center of the test gear, the unit is N; l represents the gear distance, h represents the height difference of the suspension point,
Figure FDA0002434908040000031
is the static fulcrum reaction force;
S4.3、将导线振动的惯性力F代替考虑电线刚度的悬挂点处静态弯曲应力关系式中的静态支点反力,得到导线微风振动时悬挂点处的动弯应力σcS4.3. Substitute the inertial force F of the wire vibration for the static fulcrum reaction force in the static bending stress relationship at the suspension point considering the wire stiffness, and obtain the dynamic bending stress σ c at the suspension point when the wire vibrates in the breeze:
Figure FDA0002434908040000032
Figure FDA0002434908040000032
导线微风振动时悬挂点处的动弯应力σc的单位为N/mm2,根据动弯应力与动弯应变的关系,得到导线微风振动时线夹处的动弯应变εcThe unit of dynamic bending stress σ c at the suspension point when the wire vibrates in breeze is N/mm 2 . According to the relationship between dynamic bending stress and dynamic bending strain, the dynamic bending strain ε c at the clamp when the wire vibrates in breeze is obtained:
Figure FDA0002434908040000033
Figure FDA0002434908040000033
导线微风振动时线夹处的动弯应变εc的单位为μεThe unit of dynamic bending strain ε c at the clip is μ ε when the wire vibrates in breeze.
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