CN111948751B - Design method of optical fiber current transformer optical fiber sensing ring based on 650nm wave band - Google Patents

Design method of optical fiber current transformer optical fiber sensing ring based on 650nm wave band Download PDF

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CN111948751B
CN111948751B CN202010766939.4A CN202010766939A CN111948751B CN 111948751 B CN111948751 B CN 111948751B CN 202010766939 A CN202010766939 A CN 202010766939A CN 111948751 B CN111948751 B CN 111948751B
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王国臣
高鸿泽
高伟
李社
于飞
王梓丞
苗伟琪
王茁
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Harbin Institute of Technology Shenzhen
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    • G02OPTICS
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    • G02B6/00Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
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    • G01MEASURING; TESTING
    • G01RMEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
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    • G01R15/245Adaptations providing voltage or current isolation, e.g. for high-voltage or high-current networks using light-modulating devices using magneto-optical modulators, e.g. based on the Faraday or Cotton-Mouton effect
    • G01R15/246Adaptations providing voltage or current isolation, e.g. for high-voltage or high-current networks using light-modulating devices using magneto-optical modulators, e.g. based on the Faraday or Cotton-Mouton effect based on the Faraday, i.e. linear magneto-optic, effect
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    • G01RMEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
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Abstract

本发明是一种基于650nm波段的光纤电流互感器光纤传感环的设计方法。本发明属于全光纤电流传感设计技术技术领域,本方法设置光纤的截面结构有多层空气孔;根据折射率导引型手性光子晶体光纤中PMMA中灰黄霉素的浓度,确定光纤的手性参数;确定光纤的空气填充比的取值范围,并任取满足要求的数值作为光纤最终的空气填充比大小;根据得到的光纤的手性参数和空气填充比,确定光纤的晶格常数的取值范围,并任取满足要求的数值作为光纤最终的晶格常数大小。本发明采用性光子晶体光纤传感环方案的光纤电流互感器系统的比差为0.235%,证明了设计的手性光子晶体光纤参数设计的合理性,并表明了光纤电流互感器系统电流测量准确度提升程度。

Figure 202010766939

The invention is a design method of the optical fiber sensing ring of the optical fiber current transformer based on the 650nm band. The invention belongs to the technical field of all-fiber current sensing design. In the method, the cross-sectional structure of the optical fiber is provided with multi-layer air holes; Chiral parameter; determine the value range of the air filling ratio of the optical fiber, and take any value that meets the requirements as the final air filling ratio of the optical fiber; determine the lattice constant of the optical fiber according to the obtained chirality parameter and air filling ratio of the optical fiber The value range of , and any value that meets the requirements is taken as the final lattice constant of the fiber. The ratio difference of the optical fiber current transformer system using the chiral photonic crystal optical fiber sensing ring scheme of the present invention is 0.235%, which proves the rationality of the designed chiral photonic crystal optical fiber parameter design, and shows that the current measurement of the optical fiber current transformer system is accurate. degree of improvement.

Figure 202010766939

Description

一种基于650nm波段的光纤电流互感器光纤传感环的设计 方法A Design Method of Optical Fiber Sensing Ring of Optical Fiber Current Transformer Based on 650nm Band

技术领域technical field

本发明涉及全光纤电流传感设计技术领域,是一种基于650nm波段的光纤电流互感器光纤传感环的设计方法。The invention relates to the technical field of all-fiber current sensing design, and relates to a design method for an optical fiber sensing ring of an optical fiber current transformer based on a 650 nm waveband.

背景技术Background technique

光纤电流互感器是一种基于法拉第旋光效应的光纤类传感器,由于其具有绝缘性好,可靠性高,宽频域和良好的暂态特性等优点被广泛的应用于电力传输行业和电解铝行业,这些行业都对光纤电流互感器的电流测量提出了高精度的要求。其中主要限制系统准确度的因素是源于系统光纤传感环的不理想。偏振光在理想的光纤传感环中以圆偏振光的形式传输,但光纤由于其制作工艺的不理想会存在残余的线性双折射,这会导致偏振光的偏振面发生一个旋转,产生一个与法拉第效应无法区分的误差信号,使得光在系统传输的过程中产生偏振误差,进而降低了系统测量电流的准确度。Optical fiber current transformer is a kind of optical fiber sensor based on Faraday rotation effect. It is widely used in power transmission industry and electrolytic aluminum industry due to its advantages of good insulation, high reliability, wide frequency range and good transient characteristics. These industries all put forward high-precision requirements for the current measurement of fiber-optic current transformers. One of the main factors limiting the accuracy of the system is the imperfection originating from the system's fiber optic sensing loop. Polarized light is transmitted in the form of circularly polarized light in an ideal optical fiber sensing ring, but the optical fiber will have residual linear birefringence due to its unsatisfactory manufacturing process, which will cause a rotation of the polarization plane of the polarized light, resulting in a The indistinguishable error signal caused by the Faraday effect causes polarization errors in the system transmission of light, which in turn reduces the accuracy of the current measured by the system.

因此,为了提高系统测量电流的准确度,需要考虑增加光纤传感环的圆双折射或者减小其残余线性双折射。现有的主流方案为采用采用旋转熊猫型硅基保偏光纤作为系统的光纤传感环。这种光纤是将熊猫型硅基线保偏光纤的两根应力丝在熔融状态下围绕着纤芯进行拉伸并匀速旋转,由于平均效应使得离轴旋转应力丝引起的有效圆双折射增强。然而,这种光纤现在还存在一些问题。第一,光纤应力丝旋转速率是不均匀的,这也就意味着其螺距也是不均匀的,这会使得光纤中存在残余的线性双折射。第二,光纤在拉丝的过程中存在着极大的应力,这种应力随着时间的推移会引起纤芯的光弹特性发生变化,这会使得其线性双折射的抑制效果逐渐减弱。光纤中存在的这些问题都限制了系统准确度的进一步提升。因此,需要寻找一种新型的高度保圆偏光纤提高光纤电流互感器系统电流测量的准确度。Therefore, in order to improve the accuracy of the current measurement of the system, it is necessary to consider increasing the circular birefringence of the fiber sensing ring or reducing its residual linear birefringence. The current mainstream solution is to use a rotating panda-type silicon-based polarization-maintaining fiber as the optical fiber sensing ring of the system. In this fiber, the two stress filaments of the panda-type silicon baseline polarization-maintaining fiber are stretched around the core in a molten state and rotated at a uniform speed. Due to the averaging effect, the effective circular birefringence caused by the off-axis rotation of the stress filaments is enhanced. However, there are still some problems with this fiber. First, the rotational rate of the fiber stress filament is non-uniform, which means that its pitch is also non-uniform, which results in residual linear birefringence in the fiber. Second, there is a great stress in the fiber drawing process. This stress will cause the photoelastic properties of the fiber core to change over time, which will gradually weaken its linear birefringence suppression effect. These problems in the fiber limit the further improvement of the system accuracy. Therefore, it is necessary to find a new type of highly circular-maintaining polarization fiber to improve the current measurement accuracy of the fiber-optic current transformer system.

发明内容SUMMARY OF THE INVENTION

本发明为减小光纤电流互感器系统中由于光纤传感环存在残余线性双折射而引入的偏振误差,进而提高光纤电流互感器系统电流测量准确度,本发明提供了一种基于650nm波段的光纤电流互感器光纤传感环的设计方法,本发明提供了以下技术方案:In order to reduce the polarization error introduced by the residual linear birefringence of the optical fiber sensing ring in the optical fiber current transformer system, and further improve the current measurement accuracy of the optical fiber current transformer system, the invention provides an optical fiber based on the 650nm band. The present invention provides the following technical solutions:

一种基于650nm波段的光纤电流互感器光纤传感环的设计方法,包括以下步骤:A method for designing an optical fiber sensing ring of an optical fiber current transformer based on a 650nm band, comprising the following steps:

步骤1:采用折射率导引型手性光子晶体光纤,设置光纤的截面结构有多层空气孔,;Step 1: Use a refractive index-guided chiral photonic crystal fiber, and set the cross-sectional structure of the fiber to have multiple air holes;

步骤2:根据折射率导引型手性光子晶体光纤中PMMA中灰黄霉素的浓度,确定光纤的手性参数;Step 2: According to the concentration of griseofulvin in PMMA in the refractive index-guided chiral photonic crystal fiber, determine the chiral parameter of the fiber;

步骤3:根据得到的光纤的手性参数和和确定的晶格常数,确定光纤的空气填充比的取值范围,并任取一数值作为光纤最终的空气填充比大小;Step 3: According to the obtained chirality parameters of the optical fiber and the determined lattice constant, determine the value range of the air filling ratio of the optical fiber, and take any value as the final air filling ratio of the optical fiber;

步骤4:根据得到的光纤的手性参数和空气填充比,确定光纤的晶格常数的取值范围,并任取一数值作为光纤最终的晶格常数大小。Step 4: Determine the value range of the lattice constant of the fiber according to the obtained chirality parameter and air filling ratio, and take any value as the final lattice constant of the fiber.

优选地,所述步骤1具体为:Preferably, the step 1 is specifically:

设置光纤的截面结构共有5层空气孔,光纤截面的每一层空气孔均为正六边形排列,光纤中心的最内层空气孔为第1层空气孔,光纤中心的最外层空气孔为第5层空气孔,从最内层到最外层层数编号逐层递增;There are 5 layers of air holes in the cross-sectional structure of the optical fiber. Each layer of air holes in the optical fiber cross-section is arranged in a regular hexagon. The innermost air hole in the center of the fiber is the first layer of air holes, and the outermost air hole in the center of the fiber is The fifth layer of air holes, the number of layers from the innermost layer to the outermost layer increases layer by layer;

对于第1层空气孔来说,包含的所有的6个空气孔到光纤中心的距离为Λ,且对于整个光纤横截面上的空气孔其距离均相等,为Λ,所有空气孔均为圆孔且直径均相等均为d,将光纤空气孔的直径大小与其晶格常数的比值与定义光纤的空气填充比,为d/Λ。For the first layer of air holes, the distance from all 6 air holes to the center of the fiber is Λ, and the distances for the air holes on the entire optical fiber cross-section are the same, which is Λ, and all air holes are round holes And the diameters are all equal to d, the ratio of the diameter of the fiber air hole to its lattice constant and the air filling ratio of the defined fiber is d/Λ.

优选地,所述步骤2具体为:Preferably, the step 2 is specifically:

当PMMA中灰黄霉素的浓度为0.067g/cm时,对应的旋光率δ0采用Boltzmann公式表示,通过下式表示对应的旋光率δ0When the concentration of griseofulvin in PMMA is 0.067g/cm, the corresponding optical rotation δ 0 is expressed by the Boltzmann formula, and the corresponding optical rotation δ 0 is expressed by the following formula:

Figure BDA0002615038720000021
Figure BDA0002615038720000021

其中,B1和B2均为常数,B1=1.46×10·nm2/mm,B2=1.82×1010°·nm4/mm;Wherein, B 1 and B 2 are both constants, B 1 =1.46×10 ·nm 2 /mm, B 2 =1.82×10 10° ·nm 4 /mm;

根据旋光率δ0确定手性参数,通过下式确定手性参数ξ0The chiral parameter is determined according to the optical rotation δ 0 , and the chiral parameter ξ 0 is determined by the following formula:

Figure BDA0002615038720000022
Figure BDA0002615038720000022

k0=2π/λk 0 =2π/λ

其中,k0为光波矢,λ为光源的光波长。Among them, k 0 is the light wave vector, and λ is the light wavelength of the light source.

优选地,所述步骤3具体为:Preferably, the step 3 is specifically:

在确定的手性参数和空气孔到光纤中心的距离下,通过二维手性平面波展开法计算出不同空气填充比下手性光子晶体光纤导模和空间填充模的有效折射率,当光纤基模的有效折射率大于空间填充模的有效折射率且光纤高阶模的有效折射率小于空间填充模的有效折射率时,保证光在光纤中进行单模传输,将空气填充比设计为满足所有空气填充比的数值。Under the determined chirality parameters and the distance from the air hole to the center of the fiber, the effective refractive index of the guided mode and space-filling mode of the chiral photonic crystal fiber with different air filling ratios is calculated by the two-dimensional chiral plane wave expansion method. When the effective refractive index of the optical fiber is greater than the effective refractive index of the space-filling mode and the effective refractive index of the high-order mode of the fiber is smaller than the effective refractive index of the space-filling mode, the single-mode transmission of light in the fiber is guaranteed, and the air-filling ratio is designed to satisfy all air-filling ratios value of .

优选地,所述步骤4具体为:Preferably, the step 4 is specifically:

在确定的手性参数和空气填充比下,通过二维手性平面波展开法计算出不同晶格常数下手性光子晶体光纤导模和空间填充模的有效折射率,当光纤基模的有效折射率大于空间填充模的有效折射率且光纤高阶模的有效折射率小于空间填充模的有效折射率时,能够保证光在光纤中进行单模传输,将晶格常数设计为满足所有晶格常数的数值。Under the determined chirality parameters and air filling ratio, the effective refractive index of the guided mode and space-filling mode of the chiral photonic crystal fiber with different lattice constants is calculated by the two-dimensional chiral plane wave expansion method. When the effective refractive index of the fundamental mode of the fiber is When the effective refractive index is greater than the effective refractive index of the space-filling mode and the effective refractive index of the high-order mode of the fiber is smaller than that of the space-filling mode, the single-mode transmission of light in the fiber can be ensured, and the lattice constant is designed to satisfy all lattice constants.

本发明具有以下有益效果:The present invention has the following beneficial effects:

本发明本方案代替了原有的硅基扭转保圆偏光纤传感环方案,不仅具有成本低的优点,还通过对手性光子晶体光纤传感环结构参数的优化设计提升了光纤电流互感器系统电流测量的准确度,使得系统的比差从4.5%降低到了0.235%。The scheme of the present invention replaces the original silicon-based torsional circular-maintaining optical fiber sensing ring scheme, not only has the advantages of low cost, but also improves the optical fiber current transformer system by optimizing the design of the structural parameters of the chiral photonic crystal optical fiber sensing ring The accuracy of the current measurement reduces the ratio difference of the system from 4.5% to 0.235%.

采用硅基扭转熊猫型保圆偏光纤传感环方案的光纤电流互感器系统的比差为4.5%,而采用性光子晶体光纤传感环方案的光纤电流互感器系统的比差为0.235%,该结果有力的证明了本专利设计的手性光子晶体光纤参数设计的合理性,并表明了光纤电流互感器系统电流测量准确度提升程度。The ratio difference of the fiber optic current transformer system using the silicon-based twisted panda-type circular polarization fiber sensing ring scheme is 4.5%, while the ratio difference of the fiber optic current transformer system using the photonic crystal fiber sensing ring scheme is 0.235%. This result strongly proves the rationality of the parameter design of the chiral photonic crystal fiber designed in this patent, and shows the degree of improvement of the current measurement accuracy of the fiber optic current transformer system.

附图说明Description of drawings

图1为光纤截面结构示意图;Figure 1 is a schematic diagram of a cross-sectional structure of an optical fiber;

图2为晶体光纤导模和空间填充模的有效折射率随光纤的空气填充比的变化关系图;Figure 2 is a graph showing the relationship between the effective refractive index of the guided mode and the space-filling mode of the crystal fiber and the air filling ratio of the fiber;

图3为晶体光纤导模和空间填充模的有效折射率随光纤的晶格常数的变化关系图;Fig. 3 is a graph showing the variation of the effective refractive index of the guided mode and the space-filling mode of the crystal fiber with the lattice constant of the fiber;

图4为手性光子晶体光纤传感环的光纤电流互感器系统和采用硅基扭转保圆偏光纤传感环的光纤电流互感器系统的比差随被测电流之间的变化关系。Figure 4 shows the relationship between the ratio difference and the measured current between the fiber optic current transformer system of the chiral photonic crystal fiber sensing ring and the fiber optic current transformer system using the silicon-based twisted circularly polarized fiber sensing ring.

具体实施方式Detailed ways

以下结合具体实施例,对本发明进行了详细说明。The present invention is described in detail below with reference to specific embodiments.

具体实施例一:Specific embodiment one:

本发明提供一种基于650nm波段的光纤电流互感器光纤传感环的设计方法,具体为:The invention provides a design method of an optical fiber current transformer optical fiber sensing ring based on a 650nm band, specifically:

一种基于650nm波段的光纤电流互感器光纤传感环的设计方法,包括以下步骤:A method for designing an optical fiber sensing ring of an optical fiber current transformer based on a 650nm band, comprising the following steps:

步骤1:采用折射率导引型手性光子晶体光纤,设置光纤的截面结构有多层空气孔,确定空气孔到光纤中心的距离;Step 1: Use a refractive index-guided chiral photonic crystal fiber, set the cross-sectional structure of the fiber to have multiple air holes, and determine the distance from the air hole to the center of the fiber;

所述步骤1具体为:The step 1 is specifically:

设置光纤的截面结构共有5层空气孔,光纤截面的每一层空气孔均为正六边形排列,光纤中心的最内层空气孔为第1层空气孔,光纤中心的最外层空气孔为第5层空气孔,从最内层到最外层层数编号逐层递增,空气孔A1,A2,…,A6为第1层空气孔,空气孔B1,B2,…,B12为第2层空气孔,空气孔C1,C2,…,C18为第3层空气孔,空气孔D1,D2,…,D24为第4层空气孔,空气孔E1,E2,…,E30为第5层空气孔;There are 5 layers of air holes in the cross-sectional structure of the optical fiber. Each layer of air holes in the optical fiber cross-section is arranged in a regular hexagon. The innermost air hole in the center of the fiber is the first layer of air holes, and the outermost air hole in the center of the fiber is The fifth layer of air holes, the number of layers increases from the innermost layer to the outermost layer. Air holes A1, A2, ..., A6 are the first layer of air holes, and air holes B1, B2, ..., B12 are the second layer. Air holes, air holes C1, C2, ..., C18 are the third layer air holes, air holes D1, D2, ..., D24 are the fourth layer air holes, air holes E1, E2, ..., E30 are the fifth layer air holes ;

对于第1层空气孔来说,包含的所有的6个空气孔A1,A2,…,A6到光纤中心的距离为Λ,且对于整个光纤横截面上的空气孔其距离均相等,为Λ,所有空气孔均为圆孔且直径均相等均为d,将光纤空气孔的直径大小与其晶格常数的比值与定义光纤的空气填充比,为d/Λ。For the first layer of air holes, the distance from all six air holes A1, A2, ..., A6 to the center of the fiber is Λ, and the distances for the air holes on the entire fiber cross-section are equal, which is Λ, All air holes are round holes with equal diameters and are d. The ratio of the diameter of the air holes of the fiber to its lattice constant and the air filling ratio of the defined fiber is d/Λ.

优选地,空气孔到光纤中心的距离Λ取为4μm。Preferably, the distance Λ from the air hole to the center of the optical fiber is taken as 4 μm.

步骤2:根据折射率导引型手性光子晶体光纤中PMMA中灰黄霉素的浓度,确定光纤的手性参数;Step 2: According to the concentration of griseofulvin in PMMA in the refractive index-guided chiral photonic crystal fiber, determine the chiral parameter of the fiber;

所述步骤2具体为:The step 2 is specifically:

当PMMA中灰黄霉素的浓度为0.067g/cm时,对应的旋光率δ0采用Boltzmann公式表示,通过下式表示对应的旋光率δ0When the concentration of griseofulvin in PMMA is 0.067g/cm, the corresponding optical rotation δ 0 is expressed by the Boltzmann formula, and the corresponding optical rotation δ 0 is expressed by the following formula:

Figure BDA0002615038720000041
Figure BDA0002615038720000041

其中,B1和B2均为常数,B1=1.46×10·nm2/mm,B2=1.82×1010°·nm4/mm;Wherein, B 1 and B 2 are both constants, B 1 =1.46×10 ·nm 2 /mm, B 2 =1.82×10 10° ·nm 4 /mm;

根据旋光率δ0确定手性参数,通过下式确定手性参数ξ0The chiral parameter is determined according to the optical rotation δ 0 , and the chiral parameter ξ 0 is determined by the following formula:

Figure BDA0002615038720000042
Figure BDA0002615038720000042

k0=2π/λk 0 =2π/λ

其中,k0为光波矢,λ为光源的光波长。Among them, k 0 is the light wave vector, and λ is the light wavelength of the light source.

步骤3:根据得到的光纤的手性参数和空气孔到光纤中心的距离,确定光纤的空气填充比;Step 3: Determine the air filling ratio of the fiber according to the obtained chirality parameter of the fiber and the distance from the air hole to the center of the fiber;

所述步骤3具体为:The step 3 is specifically:

在确定的手性参数和空气孔到光纤中心的距离下,通过二维手性平面波展开法计算出不同空气填充比下手性光子晶体光纤导模和空间填充模的有效折射率,当光纤基模的有效折射率大于空间填充模的有效折射率且光纤高阶模的有效折射率小于空间填充模的有效折射率时,保证光在光纤中进行单模传输,将空气填充比设计为满足所有空气填充比的数值。Under the determined chirality parameters and the distance from the air hole to the center of the fiber, the effective refractive index of the guided mode and space-filling mode of the chiral photonic crystal fiber with different air filling ratios is calculated by the two-dimensional chiral plane wave expansion method. When the effective refractive index of the optical fiber is greater than the effective refractive index of the space-filling mode and the effective refractive index of the high-order mode of the fiber is smaller than the effective refractive index of the space-filling mode, the single-mode transmission of light in the fiber is guaranteed, and the air-filling ratio is designed to satisfy all air-filling ratios value of .

步骤4:根据得到的光纤的手性参数和空气填充比,确定光纤的晶格常数。Step 4: Determine the lattice constant of the fiber according to the obtained chirality parameter and air filling ratio.

所述步骤4具体为:The step 4 is specifically:

在确定的手性参数和空气填充比下,通过二维手性平面波展开法计算出不同晶格常数下手性光子晶体光纤导模和空间填充模的有效折射率,当光纤基模的有效折射率大于空间填充模的有效折射率且光纤高阶模的有效折射率小于空间填充模的有效折射率时,能够保证光在光纤中进行单模传输,将晶格常数设计为满足所有晶格常数的数值。Under the determined chirality parameters and air filling ratio, the effective refractive index of the guided mode and space-filling mode of the chiral photonic crystal fiber with different lattice constants is calculated by the two-dimensional chiral plane wave expansion method. When the effective refractive index of the fundamental mode of the fiber is When the effective refractive index is greater than the effective refractive index of the space-filling mode and the effective refractive index of the high-order mode of the fiber is smaller than that of the space-filling mode, the single-mode transmission of light in the fiber can be ensured, and the lattice constant is designed to satisfy all lattice constants.

光纤电流互感器系统的比差可以表示为:The ratio difference of the fiber optic current transformer system can be expressed as:

Figure BDA0002615038720000043
Figure BDA0002615038720000043

其中in

Figure BDA0002615038720000051
Figure BDA0002615038720000051

Figure BDA0002615038720000052
Figure BDA0002615038720000052

其中N为线圈匝数,其大小为N=10;V为光纤的维尔德常数,I为被测电流,Δβ为光纤中的残余线性双折射,T为光纤的固有圆双折射。Among them, N is the number of turns of the coil, and its size is N=10; V is the Verdet constant of the fiber, I is the measured current, Δβ is the residual linear birefringence in the fiber, and T is the inherent circular birefringence of the fiber.

对于硅基扭转熊猫型保圆偏光纤来说,其维尔德常数大小为V1=4.37μrad/A,残余线性双折射Δβ1=1571rad/m,圆双折射为T1=38080rad/m。对于手性光子晶体光纤来说,其维尔德常数大小为V2=3.13μrad/A,残余线性双折射Δβ2=0.468rad/m,圆双折射T2=4.7617rad/m。当被测电流值I从0A增加到1000A时,可以分别得到采用硅基扭转熊猫型保圆偏光纤传感环和采用手性光子晶体光纤传感环的系统比差对比图,如图4所示。仿真结果表明,采用硅基扭转熊猫型保圆偏光纤传感环方案的光纤电流互感器系统的比差为4.5%,而采用性光子晶体光纤传感环方案的光纤电流互感器系统的比差为0.235%,该结果有力的证明了本专利设计的手性光子晶体光纤参数设计的合理性,并表明了光纤电流互感器系统电流测量准确度提升程度。For the silicon-based twisted panda-type circularly-maintaining polarized fiber, its Verdet constant is V 1 =4.37μrad/A, the residual linear birefringence Δβ 1 =1571rad/m, and the circular birefringence is T 1 =38080rad/m. For a chiral photonic crystal fiber, its Verdet constant is V 2 =3.13 μrad/A, the residual linear birefringence Δβ 2 =0.468rad/m, and the circular birefringence T 2 =4.7617rad/m. When the measured current value I increases from 0A to 1000A, a comparison chart of the system ratio difference between the silicon-based twisted panda-type circularly-maintaining polarization fiber sensing ring and the chiral photonic crystal fiber sensing ring can be obtained, as shown in Figure 4. Show. The simulation results show that the ratio difference of the fiber optic current transformer system using the silicon-based twisted panda-type circular polarization fiber sensing ring scheme is 4.5%, while the ratio difference of the fiber optic current transformer system using the photonic crystal fiber sensing ring scheme It is 0.235%. This result strongly proves the rationality of the parameter design of the chiral photonic crystal fiber designed by this patent, and shows the degree of improvement of the current measurement accuracy of the fiber current transformer system.

具体实施例二:Specific embodiment two:

一种基于650nm波段的光纤电流互感器光纤传感环的设计方法,包括以下步骤:A method for designing an optical fiber sensing ring of an optical fiber current transformer based on a 650nm band, comprising the following steps:

步骤1.采用折射率导引型手性光子晶体光纤来替代原有的旋转熊猫型硅基保圆偏光纤。这种光纤的基底材料为掺有手性分子灰黄霉素的聚甲基丙烯酸甲酯(PMMA)。其光纤的截面结构共有5层空气孔,如图1所示。其中(1)为光纤的基底材料组成,光纤截面的每一层空气孔均为正六边形排列。定义最靠近光纤中心的那一层空气孔为第1层空气孔,最远离光纤中心的那一层空气孔为第5层空气孔,从最内层到最外层层数编号逐层递增。在图1中,设计的手性光子晶体光纤中心没有空气孔,空气孔A1,A2,…,A6为第1层空气孔,空气孔B1,B2,…,B12为第2层空气孔,空气孔C1,C2,…,C18为第3层空气孔,空气孔D1,D2,…,D24为第4层空气孔,空气孔E1,E2,…,E30为第5层空气孔。对于第1层空气孔来说,其中包含的所有的6个空气孔A1,A2,…,A6距离光纤中心的距离为Λ,且对于整个光纤横截面上的空气孔其距离均相等,为Λ,将这个距离定义为光纤的晶格常数。所有空气孔均为圆孔且直径均相等,为d。将光纤空气孔的直径大小与其晶格常数的比值与定义光纤的空气填充比,为d/Λ。Step 1. Use a refractive index-guided chiral photonic crystal fiber to replace the original rotating panda-type silicon-based circularly-maintaining fiber. The base material of this optical fiber is polymethyl methacrylate (PMMA) doped with the chiral molecule griseofulvin. The cross-sectional structure of its optical fiber has a total of 5 layers of air holes, as shown in Figure 1. Wherein (1) is the base material composition of the optical fiber, and each layer of air holes in the optical fiber cross-section is arranged in a regular hexagon. The layer of air holes closest to the center of the fiber is defined as the first layer of air holes, and the layer of air holes farthest from the center of the fiber is defined as the fifth layer of air holes. The number of layers increases from the innermost layer to the outermost layer. In Figure 1, there is no air hole in the center of the designed chiral photonic crystal fiber. Air holes A1, A2, ..., A6 are the first layer of air holes, and air holes B1, B2, ..., B12 are the second layer of air holes. The holes C1, C2, ..., C18 are the third layer air holes, the air holes D1, D2, ..., D24 are the fourth layer air holes, and the air holes E1, E2, ..., E30 are the fifth layer air holes. For the first layer of air holes, the distances of all 6 air holes A1, A2,..., A6 from the center of the fiber are Λ, and the distances for the air holes on the entire fiber cross-section are equal, which is Λ , defining this distance as the lattice constant of the fiber. All air holes are round holes and have the same diameter, d. The ratio of the diameter of the fiber air hole to its lattice constant and the air filling ratio of the defined fiber is d/Λ.

步骤2.在设计完光纤的截面结构后,首先需要确定光纤的手性参数。光纤的手性参数是一个与光波长相关的函数,具体计算过程如下:Step 2. After designing the cross-sectional structure of the optical fiber, it is first necessary to determine the chiral parameters of the optical fiber. The chirality parameter of the fiber is a function related to the wavelength of light, and the specific calculation process is as follows:

当PMMA中灰黄霉素的浓度为0.067g/cm时,对应的旋光率δ0用Boltzmann公式可以表示为:When the concentration of griseofulvin in PMMA is 0.067g/cm, the corresponding optical rotation δ 0 can be expressed as:

Figure BDA0002615038720000061
Figure BDA0002615038720000061

其中,B1和B2均为常数,其数值分别为B1=1.46×10·nm2/mm,B2=1.82×1010°·nm4/mm。则手性参数ξ0可以由下式计算得到:Wherein, B 1 and B 2 are both constants, and their values are B 1 =1.46×10 ·nm 2 /mm, and B 2 =1.82×10 10° ·nm 4 /mm, respectively. Then the chiral parameter ξ 0 can be calculated by the following formula:

Figure BDA0002615038720000062
Figure BDA0002615038720000062

其中,k0为光波矢,其数值为k0=2π/λ,λ为光源的光波长,其数值为λ=650nm。计算可得手性参数ξ0=-1.1482×10-8rad·μm。Wherein, k 0 is the light wave vector, and its value is k 0 =2π/λ, and λ is the light wavelength of the light source, and its value is λ=650nm. The calculated chirality parameter ξ 0 =-1.1482×10 -8 rad·μm.

步骤3.接下来需要确定光纤的空气填充比。这里取光纤的晶格常数Λ=4μm,手性参数ξ0=-1.1482×10-8rad·μm。光纤的空气填充比d/Λ的取值为从0.04到0.6,步长为0.02。此时可以得到手性光子晶体光纤导模和空间填充模的有效折射率neff随光纤的空气填充比d/Λ的变化关系,如图2所示。当光纤导模的有效折射率大于其空间填充模的有效折射率时,导模光能够在光纤中进行稳定的传输。当光纤的空气填充比小于0.08时,光纤基模的有效折射率和高阶模的有效折射率均小于空间填充模的有效折射率;当光纤的空气填充比大于0.46时,光纤基模的有效折射率和高阶模的有效折射率均大于空间填充模的有效折射率;由于需要保证光纤中只存在一种模式的光进行传输,也就是基模光在光纤中的传输,因此需要基模的有效折射率大于空间填充模的有效折射率而高阶模的有效折射率小于空间填充模的有效折射率。因此此时需要保证光纤的空气填充比d/Λ在0.08~0.46之间。Step 3. Next, the air filling ratio of the fiber needs to be determined. Here, the lattice constant of the fiber is Λ=4μm, and the chirality parameter ξ 0 =-1.1482×10 -8 rad·μm. The value of the air filling ratio d/Λ of the optical fiber is from 0.04 to 0.6 with a step size of 0.02. At this time, the relationship between the effective refractive index n eff of the guided mode and the space-filling mode of the chiral photonic crystal fiber with the air filling ratio d/Λ of the fiber can be obtained, as shown in Figure 2. When the effective refractive index of the guided mode of the fiber is greater than the effective refractive index of the space-filling mode, the guided mode light can be stably transmitted in the fiber. When the air-filling ratio of the fiber is less than 0.08, the effective refractive index of the fiber fundamental mode and the effective refractive index of the higher-order mode are both smaller than the effective refractive index of the space-filling mode; when the air-filling ratio of the fiber is greater than 0.46, the effective refractive index of the fiber fundamental mode The effective refractive index of the high-order mode and the high-order mode are both greater than the effective refractive index of the space-filling mode; since it is necessary to ensure that there is only one mode of light in the fiber for transmission, that is, the transmission of the fundamental mode light in the fiber, the effective refractive index of the fundamental mode is required. It is greater than the effective refractive index of the space-filling mode and the effective refractive index of the higher-order mode is less than the effective refractive index of the space-filling mode. Therefore, it is necessary to ensure that the air filling ratio d/Λ of the optical fiber is between 0.08 and 0.46.

步骤4.最后需要确定光纤的晶格常数。根据内容3中确定的空气填充比的取值范围,这里任取其中的一个数值。取光纤的空气填充比为0.42,手性参数ξ0=-1.1482×10- 8rad·μm。光纤的晶格常数Λ的取值为从0.4μm到7μm,步长为0.2μm。此时可以得到手性光子晶体光纤导模和空间填充模的有效折射率neff随光纤的晶格常数Λ的变化关系,如图3所示。当光纤的晶格常数小于1.2μm时,光纤基模和高阶模的有效折射率均小于空间填充模的有效折射率;当光纤的晶格常数大于4.4μm时,光纤基模和高阶模的有效折射率均大于空间填充模的有效折射率;由于需要保证光纤中只存在一种模式的光进行传输,也就是基模光在光纤中的传输,因此需要基模的有效折射率大于空间填充模的有效折射率而高阶模的有效折射率小于空间填充模的有效折射率。因此此时需要保证光纤的晶格常数Λ在1.2μm~4.4μm之间。这里取Λ=4μm。Step 4. Finally, the lattice constant of the fiber needs to be determined. According to the value range of the air filling ratio determined in Content 3, one of the values is arbitrarily selected here. The air filling ratio of the optical fiber is taken as 0.42, and the chirality parameter ξ 0 =-1.1482×10 - 8 rad·μm. The value of the lattice constant Λ of the fiber ranges from 0.4 μm to 7 μm with a step size of 0.2 μm. At this time, the relationship between the effective refractive index n eff of the guided mode and the space-filling mode of the chiral photonic crystal fiber with the lattice constant Λ of the fiber can be obtained, as shown in Figure 3. When the lattice constant of the fiber is less than 1.2 μm, the effective refractive index of the fundamental mode and the higher-order mode of the fiber are both smaller than the effective refractive index of the space-filling mode; when the lattice constant of the fiber is greater than 4.4 μm, the effective refractive index of the fundamental mode and the higher-order mode of the fiber are greater than the effective refractive index of the space-filling mode; since it is necessary to ensure that there is only one mode of light in the fiber for transmission, that is, the transmission of the fundamental mode light in the fiber, the effective refractive index of the fundamental mode needs to be greater than the effective refractive index of the space-filling mode. The effective index of refraction for higher order modes is less than the effective index of refraction for space-filling modes. Therefore, it is necessary to ensure that the lattice constant Λ of the optical fiber is between 1.2 μm and 4.4 μm. Here, Λ=4 μm is taken.

光纤电流互感器系统的比差可以表示为:The ratio difference of the fiber optic current transformer system can be expressed as:

Figure BDA0002615038720000063
Figure BDA0002615038720000063

其中in

Figure BDA0002615038720000071
Figure BDA0002615038720000071

其中N为线圈匝数,其大小为N=10;V为光纤的维尔德常数,I为被测电流,Δβ为光纤中的残余线性双折射,T为光纤的固有圆双折射。Among them, N is the number of turns of the coil, and its size is N=10; V is the Verdet constant of the fiber, I is the measured current, Δβ is the residual linear birefringence in the fiber, and T is the inherent circular birefringence of the fiber.

对于硅基扭转熊猫型保圆偏光纤来说,其维尔德常数大小为V1=4.37μrad/A,残余线性双折射Δβ1=1571rad/m,圆双折射为T1=38080rad/m。对于手性光子晶体光纤来说,其维尔德常数大小为V2=3.13μrad/A,残余线性双折射Δβ2=0.468rad/m,圆双折射T2=4.7617rad/m。当被测电流值I从0A增加到1000A时,可以分别得到采用硅基扭转熊猫型保圆偏光纤传感环和采用手性光子晶体光纤传感环的系统比差对比图,如图4所示。仿真结果表明,采用硅基扭转熊猫型保圆偏光纤传感环方案的光纤电流互感器系统的比差为4.5%,而采用性光子晶体光纤传感环方案的光纤电流互感器系统的比差为0.235%,该结果有力的证明了本专利设计的手性光子晶体光纤参数设计的合理性,并表明了光纤电流互感器系统电流测量准确度提升程度。For the silicon-based twisted panda-type circularly-maintaining polarized fiber, its Verdet constant is V 1 =4.37μrad/A, the residual linear birefringence Δβ 1 =1571rad/m, and the circular birefringence is T 1 =38080rad/m. For a chiral photonic crystal fiber, its Verdet constant is V 2 =3.13 μrad/A, the residual linear birefringence Δβ 2 =0.468rad/m, and the circular birefringence T 2 =4.7617rad/m. When the measured current value I increases from 0A to 1000A, a comparison chart of the system ratio difference between the silicon-based twisted panda-type circularly-maintaining polarization fiber sensing ring and the chiral photonic crystal fiber sensing ring can be obtained, as shown in Figure 4. Show. The simulation results show that the ratio difference of the fiber optic current transformer system using the silicon-based twisted panda-type circular polarization fiber sensing ring scheme is 4.5%, while the ratio difference of the fiber optic current transformer system using the photonic crystal fiber sensing ring scheme It is 0.235%. This result strongly proves the rationality of the parameter design of the chiral photonic crystal fiber designed by this patent, and shows the degree of improvement of the current measurement accuracy of the fiber current transformer system.

本方案提出了一种新型聚合物材料的光子晶体光纤传感环方案,本方案代替了原有的硅基扭转保圆偏光纤传感环方案,不仅具有成本低的优点,还通过对手性光子晶体光纤传感环结构参数的优化设计提升了光纤电流互感器系统电流测量的准确度,使得系统的比差从4.5%降低到了0.235%。This scheme proposes a new type of polymer material photonic crystal fiber sensing ring scheme. This scheme replaces the original silicon-based twisted circular polarization fiber sensing ring scheme. It not only has the advantages of low cost, but also uses chiral photons. The optimized design of the structural parameters of the crystal fiber sensing ring improves the accuracy of the current measurement of the fiber optic current transformer system, which reduces the ratio difference of the system from 4.5% to 0.235%.

以上所述仅是一种基于650nm波段的光纤电流互感器光纤传感环的设计方法的优选实施方式,一种基于650nm波段的光纤电流互感器光纤传感环的设计方法的保护范围并不仅局限于上述实施例,凡属于该思路下的技术方案均属于本发明的保护范围。应当指出,对于本领域的技术人员来说,在不脱离本发明原理前提下的若干改进和变化,这些改进和变化也应视为本发明的保护范围。The above is only a preferred embodiment of a design method for an optical fiber current transformer optical fiber sensing ring based on a 650 nm wavelength band, and the protection scope of a design method for an optical fiber current transformer optical fiber sensing ring based on a 650 nm wavelength band is not limited to In the above-mentioned embodiments, all technical solutions under this idea belong to the protection scope of the present invention. It should be pointed out that for those skilled in the art, some improvements and changes without departing from the principle of the present invention should also be regarded as the protection scope of the present invention.

Claims (2)

1.一种基于650nm波段的光纤电流互感器光纤传感环的设计方法,其特征是:包括以下步骤:1. a design method based on the optical fiber current transformer optical fiber sensing ring of 650nm wave band, it is characterized in that: comprise the following steps: 步骤1:采用折射率导引型手性光子晶体光纤,设置光纤的截面结构有多层空气孔;Step 1: Use a refractive index-guided chiral photonic crystal fiber, and set the cross-sectional structure of the fiber to have multiple air holes; 所述步骤1具体为:The step 1 is specifically: 设置光纤的截面结构共有5层空气孔,光纤截面的每一层空气孔均为正六边形排列,光纤中心的最内层空气孔为第1层空气孔,光纤中心的最外层空气孔为第5层空气孔,从最内层到最外层层数编号逐层递增;There are 5 layers of air holes in the cross-sectional structure of the optical fiber. Each layer of air holes in the optical fiber cross-section is arranged in a regular hexagon. The innermost air hole in the center of the fiber is the first layer of air holes, and the outermost air hole in the center of the fiber is The fifth layer of air holes, the number of layers from the innermost layer to the outermost layer increases layer by layer; 对于第1层空气孔来说,包含的所有的6个空气孔到光纤中心的距离为Λ,且对于整个光纤横截面上的空气孔其距离均相等,为Λ,所有空气孔均为圆孔且直径均相等均为d,将光纤空气孔的直径大小与其晶格常数的比值与定义光纤的空气填充比,为d/Λ;For the first layer of air holes, the distance from all 6 air holes to the center of the fiber is Λ, and the distances for the air holes on the entire optical fiber cross-section are the same, which is Λ, and all air holes are round holes And the diameters are all equal to d, the ratio of the diameter of the fiber air hole to its lattice constant and the air filling ratio of the defined fiber is d/Λ; 步骤2:根据折射率导引型手性光子晶体光纤中PMMA中灰黄霉素的浓度,确定光纤的手性参数;Step 2: According to the concentration of griseofulvin in PMMA in the refractive index-guided chiral photonic crystal fiber, determine the chiral parameter of the fiber; 所述步骤2具体为:The step 2 is specifically: 当PMMA中灰黄霉素的浓度为0.067g/cm时,对应的旋光率δ0采用Boltzmann公式表示,通过下式表示对应的旋光率δ0When the concentration of griseofulvin in PMMA is 0.067g/cm, the corresponding optical rotation δ 0 is expressed by the Boltzmann formula, and the corresponding optical rotation δ 0 is expressed by the following formula:
Figure FDA0003757279340000011
Figure FDA0003757279340000011
其中,B1和B2均为常数,B1=1.46×10·nm2/mm,B2=1.82×1010°·nm4/mm;Wherein, B 1 and B 2 are both constants, B 1 =1.46×10 ·nm 2 /mm, B 2 =1.82×10 10° ·nm 4 /mm; 根据旋光率δ0确定手性参数,通过下式确定手性参数ξ0The chiral parameter is determined according to the optical rotation δ 0 , and the chiral parameter ξ 0 is determined by the following formula:
Figure FDA0003757279340000012
Figure FDA0003757279340000012
k0=2π/λk 0 =2π/λ 其中,k0为光波矢,λ为光源的光波长;Among them, k 0 is the light wave vector, and λ is the light wavelength of the light source; 步骤3:根据得到的光纤的手性参数和确定的晶格常数,确定光纤的空气填充比的取值范围,并任取一数值作为光纤最终的空气填充比大小;Step 3: According to the obtained chirality parameter of the optical fiber and the determined lattice constant, determine the value range of the air filling ratio of the optical fiber, and take any value as the final air filling ratio of the optical fiber; 所述步骤3具体为:The step 3 is specifically: 在确定的手性参数和空气孔到光纤中心的距离下,通过二维手性平面波展开法计算出不同空气填充比下手性光子晶体光纤导模和空间填充模的有效折射率,当光纤基模的有效折射率大于空间填充模的有效折射率且光纤高阶模的有效折射率小于空间填充模的有效折射率时,保证光在光纤中进行单模传输,将空气填充比设计为满足所有空气填充比的数值;Under the determined chirality parameters and the distance from the air hole to the center of the fiber, the effective refractive index of the guided mode and space-filling mode of the chiral photonic crystal fiber with different air filling ratios is calculated by the two-dimensional chiral plane wave expansion method. When the effective refractive index of the optical fiber is greater than the effective refractive index of the space-filling mode and the effective refractive index of the high-order mode of the fiber is smaller than the effective refractive index of the space-filling mode, the single-mode transmission of light in the fiber is guaranteed, and the air-filling ratio is designed to satisfy all air-filling ratios the value of ; 步骤4:根据得到的光纤的手性参数和空气填充比,确定光纤的晶格常数的取值范围,并任取一数值作为光纤最终的晶格常数大小。Step 4: Determine the value range of the lattice constant of the fiber according to the obtained chirality parameter and air filling ratio, and take any value as the final lattice constant of the fiber.
2.根据权利要求1所述的一种基于650nm波段的光纤电流互感器光纤传感环的设计方法,其特征是:所述步骤4具体为:2. a kind of design method based on the optical fiber current transformer optical fiber sensing ring of 650nm wave band according to claim 1, is characterized in that: described step 4 is specifically: 在确定的手性参数和空气填充比下,通过二维手性平面波展开法计算出不同晶格常数下手性光子晶体光纤导模和空间填充模的有效折射率,当光纤基模的有效折射率大于空间填充模的有效折射率且光纤高阶模的有效折射率小于空间填充模的有效折射率时,能够保证光在光纤中进行单模传输,将晶格常数设计为满足所有晶格常数的数值。Under the determined chirality parameters and air filling ratio, the effective refractive index of the guided mode and space-filling mode of the chiral photonic crystal fiber with different lattice constants is calculated by the two-dimensional chiral plane wave expansion method. When the effective refractive index of the fundamental mode of the fiber is When the effective refractive index is greater than the effective refractive index of the space-filling mode and the effective refractive index of the high-order mode of the fiber is smaller than that of the space-filling mode, the single-mode transmission of light in the fiber can be ensured, and the lattice constant is designed to satisfy all lattice constants.
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