KR101098666B1 - Optical Electric-Field Sensors - Google Patents

Abstract

In order to provide an improved type of optical sensor structure that can prevent distortion of a signal caused by changes in the surrounding environment such as temperature or vibration, the present invention includes a light source 21 for generating light, and the light source 21 Phase detection unit 20 for detecting the phase information of the light emitted from the; Lithium niobate 11, an electro-optic crystal material having a property of changing optical refractive index in proportion to the size of an electric field, is disposed on one side of the lithium niobate 11 and polarized light emitted from the light source 21. A sensor unit including a Faraday rotator 12 for rotating the light and a reflection mirror 13 disposed on the other side of the lithium niobate 11 to reflect light emitted from the light source 21 ( 10); And a polarization maintaining optical fiber 31 connecting the sensor unit 10 and the phase detection unit 30.

Description

Optical Electric Field Sensors

The present invention relates to a sensor for measuring the magnitude of an electric field or voltage using light, and has a simple structure compared to the conventional optical sensor, but has an electric field measurement that has a stable operation regardless of environmental changes such as temperature and vibration. It relates to a light sensor for.

The demand for energy, which is increasing day by day, with the development of the industry, predicts that it is difficult to cover the existing electric energy generation facilities. As a result, electricity production facilities using solar or wind power generation are expanding rapidly. . A method of effectively storing electrical energy produced in various places through various power generating facilities is difficult to develop at the source, and the produced electrical energy must be sent directly to where it is needed. Unlike in the past, where most of the electricity was produced by a few power plants, as the number of electric power generation facilities is increased through renewable energy, smart power is provided to supply the most efficient consumption of power produced by various facilities. Management of the power network using the grid is required.

In power transmission systems using smart grid technology, effective power management is made possible by the addition of several functions that were not possible in traditional transmission and distribution systems. First, it must have the function of monitoring the constant and instantaneous power generation such as solar power and wind power generation to keep the amount of power produced in the whole network constant. This can be used to determine whether or not an easily manageable power generation facility, such as thermal power generation, is running when electricity is scarce or surviving. In addition, continuous monitoring of the power supply chain provides the ability to minimize the impact on the entire power network by responding quickly when power demand in some areas changes due to an accident. In other words, if the load resistance connected to the power network changes instantaneously due to an accident, the current supplied spreads over the entire grid, increasing instantaneous power from adjacent areas and causing a chain grid accident. Power monitoring using smart grid Can provide a way to deal with these incidents immediately. In addition, smart grid grids can provide an effective system to monitor for deliberate power leaks or respond immediately to an accident that cuts off the power supply.

The power generated by the power plant is hundreds of megawatts, which can be divided into several stages of power transmission, which are transmitted at high voltages of 110 kV and higher to reduce losses in the transmission line, and currents of several kA or more. In the vicinity of such high-voltage, high-current wires, very strong electromagnetic interference (Electro-Magnetic Interference) occurs, which seriously affects the function of a general electrical instrument, resulting in a large error in measurement results. It was. However, by using the optical sensor that measures the voltage current by using the change in the characteristics of the light, it is possible to accurately measure the voltage and current even in such an EMI environment. This is because light waves used for measurement have the property of propagating independently of electromagnetic waves, and it is also possible to easily pull out a signal measured using an optical fiber to a range that EMI cannot reach.

Optical sensors applied for smart grid can be divided into voltage sensor, current sensor, and temperature sensor, and they have common characteristics that are strong against EMI. Unlike an electric sensor, an optical sensor is made of a dielectric material having no conductivity, not a metallic material, and thus does not cause a problem even in an environment having a strong electromagnetic field. In addition, by using the optical fiber in the process of sending the sensed signal to the module for the final signal processing, EMI problems that may occur during the transmission process is also solved. In addition, since the optical sensor does not require an additional insulation device, it can be made compact and attached to existing equipment while occupying little space. Typical instrument transformers weigh several tons and are usually mounted as a single device. In addition, the optical sensor is free from magnetic ferro-resonance or saturation problems and there is no risk of fatal accidents, such as explosions that can occur with conventional oil-insulated equipment.

As described above, the optical sensor for measuring voltage among the optical sensors applied for the smart grid is generally measured by using an electro-optic material which has a characteristic in which the optical refractive index changes in proportion to the magnitude of the electric field generated by the voltage. to be. Lithium Niobate (LiNbO3) crystal, which is known as a representative electro-optic material, has a property that the refractive index of the material changes in proportion to the magnitude of the electric field applied from the outside, and the refractive index changes depending on the direction of the electric field. . When an electric field is applied in a direction parallel to the optical axis from the outside, the polarization component parallel to the optical axis and the polarization component perpendicular to the optical axis undergo different refractive index changes, and detect the polarization state appearing in the output light. The size can be measured. Based on the operation principle, the results of fabricating an electric field sensor by fabricating an optical waveguide device on a lithium niobate substrate are reported. In addition, an optical voltage sensor for measuring a voltage of 230 bilion using three electro-optic field sensors is being implemented. In addition, after winding the dual-mode optical fiber having an elliptic core along the circumference of the cylindrical quartz crystal with an insulator, it is made by using the size of the electric field according to the deformation generated in the crystal by the piezo-electric effect generated by the electric field A voltage sensor to measure is also proposed. In addition, recently, a field sensor has been disclosed in which a Bragg grating is fabricated on a lithium niobate electro-optic material to monitor a reflection wavelength that is changed due to an electro-optic effect.

The present invention provides an optical sensor structure of an improved type that can prevent distortion of a signal generated by changes in the surrounding environment such as temperature or vibration in an optical sensor for sensing the magnitude of an electric field generated by voltage using light. It aims to provide. That is, the present invention uses a method of rotating the input polarization and the output polarization by 90 degrees using a Faraday polarization rotator, and uses a method of compensating for a signal change caused by a change in the external environment. It is an object of the present invention to provide an optical sensor that does not generate distortion of sensing information even when the power of the light source is changed by environmental changes by transmitting in the form of phase information.

It is still another object of the present invention to propose an optical voltage sensor that can be easily assembled using optical fiber collimators and flat panel components without using an optical waveguide device. Conventionally, in order to use an optical waveguide device having a structure of several microns in size, a device must be manufactured by using a complicated semiconductor manufacturing process, and manufacturing equipment having a precision of submicron degree in the packaging step should be used. On the other hand, the proposed technology expands the light from the optical fiber to the size of millimeter using the collimator, and then attaches the Faraday rotator, lithium niobate, and the reflecting mirror made of flat type in order to easily assemble it. There is a merit that can be produced.

The present invention includes a light source 21 for generating light, the phase detection unit 20 for detecting the phase information of the light emitted from the light source 21; Lithium niobate 11, an electro-optic crystal material having a property of changing optical refractive index in proportion to the size of an electric field, is disposed on one side of the lithium niobate 11 and polarized light emitted from the light source 21. A sensor unit including a Faraday rotator 12 for rotating the light and a reflection mirror 13 disposed on the other side of the lithium niobate 11 to reflect light emitted from the light source 21 ( 10); And a polarization maintaining optical fiber 31 connecting the sensor unit 10 and the phase detection unit 30.

In the present invention, the light generated by the light source 21 is incident on the Faraday rotator 12 of the sensor unit 10, passes through the lithium niobate 11, and then the reflection mirror 13 ) May be reflected back to the phase detector 20.

Here, the Faraday rotator 12 may rotate the polarization of the light reflected by the reflective mirror 13 via the lithium niobate 11 by 90 degrees.

Here, the phase detector 20 may include a power splitter 23 for splitting the light input from the sensor unit 10, and a light of one side of the light split from the power splitter 23. Phase modulator 25 for modulating the phase, Polarization controller 24 for converting the polarization of the light of the other side of the light split from the power splitter 23, and the phase modulator ( Change in optical power proportional to the phase difference of the light coupler 22b in which the light output from the light source 25 and the light output from the polarization converter 24 cause the light interference and the light interfered in the light coupler 22b. It may include a photo detector (27a) (27b) for measuring the.

Here, between the phase modulator 25 and the optical coupler 22b and between the polarization converter 24 and the optical coupler 22b, polarizers 26a and 26b which pass only one of TE polarization and TM polarization are passed. May each be further interposed.

In the present invention, a collimator lens 32 may be further interposed between the polarization maintaining optical fiber 31 and the Faraday rotator 12.

According to the present invention, it is possible to implement an optical voltage sensor that operates stably regardless of external environment changes. In addition, it can be used as a sensor that can accurately measure the voltage value in the environment with severe electromagnetic interference by transmitting a high voltage current using this. In addition, it is possible to produce a low-cost mass production because it not only has a stable operating characteristics compared to the conventional optical voltage sensor, but also has the advantage of manufacturing the sensor through an easy process.

1 is a block diagram of an optical sensor for electric field measurement according to an embodiment of the present invention.
FIG. 2 is a diagram illustrating a phase detector of the optical sensor for electric field measurement of FIG. 1.

Hereinafter, exemplary embodiments of the present invention will be described in detail with reference to the accompanying drawings.

1 is a block diagram of an optical sensor for electric field measurement according to an embodiment of the present invention.

Referring to FIG. 1, an optical sensor 1 for electric field measurement according to an exemplary embodiment of the present invention may include a sensor unit 10 for measuring an electric field and a phase detector 20 for detecting phase information generated in proportion to an electric field. ). The light source (see 21 in FIG. 2) is included in the phase detector 20, and the sensor unit 10 and the phase detector 20 are connected through the polarization maintaining optical fiber 31. In this case, a collimator lens 32 is further interposed between the sensor unit 10 and the polarization maintaining optical fiber 31 to convert light from the minute light source (see 21 in FIG. 2) into parallel rays. Can be.

Herein, the sensor unit 10 includes lithium niobate 11, an electro-optic crystal material having a property of changing optical refractive index in proportion to the size of an electric field, and Faraday rotator 12 and reflections disposed on the left and right sides thereof. It comprises a mirror 13.

This will be described in more detail as follows.

The structure which is used most commonly as a general optical voltage sensor is a form which measures the change in the polarization state of the light wave which passes through the material which has an electro-optic effect. In the case of lithium niobate (LiNbO3), which is typically used, when an external electric field is present in the crystal axial direction, a phase of light waves having polarization in that direction is changed. In this case, the magnitude of the phase change of the light wave is different for the polarization component in the direction perpendicular to the crystal axis. Therefore, when light waves having components of the direction parallel to the crystal axis and components perpendicular to the same magnitude are incident on the crystal, a relative phase difference occurs between the two polarization components during the passage of the crystal, thereby causing the polarization state of the output light. Will change. By measuring the polarization state that changes in proportion to the intensity of the external electric field using this principle, it becomes possible to measure the intensity of the applied electric field.

In a sensor using such a lithium niobate crystal, the most important factor is to make the input polarization state incline with the optical axis inclined by 45 degrees. To this end, a method of arranging the polarizer tilted 45 degrees in front of the sensor input unit may be applied. However, even at this time, there is a difficulty in that the light transmitted to the sensor unit maintains a constant polarization state, and a difficulty in introducing a method of transmitting an optical signal to the sensor unit while maintaining an accurate polarization state using a polarization maintaining optical fiber. Existed.

In order to solve such a problem, in the optical sensor for electric field measurement (1) according to an embodiment of the present invention, in order to implement an optical voltage sensor that is stable and operates under the influence of temperature or vibration, an electro-optic crystal material A polarization rotating reflection interferometer comprising a Faraday rotator 12 and a reflection mirror 13 attached to the left and right sides of the phosphorus lithium niobate 11 provides optical phase information for a sensor signal generated in proportion to an external electric field. It is characterized by the delivery in form.

Here, the Faraday rotator 12 serves to rotate the polarization of the light wave returned by hitting the reflection mirror 13 through the lithium niobate 11 by 90 degrees, and inside the polarization maintaining optical fiber 31. Provides the ability to offset phase changes that may occur in That is, by using a sensor that transmits a signal as optical phase information rather than general optical intensity information and converts optical phase information into optical intensity information in an optical signal processing unit of an output unit, even if the optical intensity changes due to an external environment It does not affect sensing.

In detail, the light input to the sensor unit 10 through the polarization maintaining optical fiber 31 has a polarization component in a fast axis and a slow axis direction having an initial phase difference, and is polarized in the process of being reflected by the sensor unit 10 and returned. Since the conversion proceeds, the initial phase difference cancels each other out. In this process, the phase change caused by the external temperature change or the vibration is also canceled, and only the phase difference value generated by the external electric field in the lithium niobate 11 remains, which is finally detected by the phase detector 20 to determine the electric field value. It is sensed.

The optical sensor using the polarization rotation reflection interferometer can minimize the signal distortion caused by the unwanted polarization coupling phenomenon generated in the sensor unit 10. That is, in the conventional optical sensor, when the polarization coupling occurs, the polarization state of the output portion is affected, whereas in the proposed structure, a light source having a short coherence length may be used so that interference does not occur immediately even when the polarization coupling occurs. By using this, it is possible to fundamentally block the signal change caused by the minute polarization coupling generated inside the crystal material and to implement a sensor having stable operating characteristics.

After transmitting the phase difference value generated by the sensor to the signal processor, the phase detection optical signal processor generates an optical output signal according to the phase value. Using this method, the phase difference due to the birefringence between the polarizations of the photonic crystal sensor can be compensated using the phase modulator, and the operating point of the sensor can be always maintained at the point where the sensitivity is maximized. . In addition, it has a function to compensate for the change in the operating point caused by the temperature change of the sensor unit using a phase modulator.

The sensing process in the sensor unit 10 will be described in detail as follows.

Light incident from the light source of the phase detector 20 (see 21 in FIG. 2) through the polarization maintaining optical fiber 31 is first passed through the Faraday rotator 12, and the polarization direction is shifted by 45 degrees. The optical axis of the lithium niobate 11 is aligned and attached to the optical axis of the polarization maintaining optical fiber 31 by being twisted by 45 degrees. Therefore, the polarization parallel to the fast axis of the polarization maintaining optical fiber 31 is incident on the optical axis direction polarization component of the lithium niobate 11 crystal, and the slow axis component is incident on the direction component perpendicular to the crystal optical axis. When the direction of the external electric field to be sensed is parallel to the optical axis direction of the crystal, the polarization component of the directional component experiences the largest refractive index change, and the vertically polarized component experiences a relatively small refractive index change. This difference in refractive index causes a difference in the phase change value of each direction polarization component, and affects the polarization state of the output light.

The light passing through the lithium niobate 11 crystal passes through the inside of the crystal once again in the opposite direction through the reflective mirror 13, and the phase change value is doubled. After passing through the Faraday rotator 12 again, each polarization is rotated by 45 degrees and finally undergoes a polarization change by 90 degrees. Eventually, the light incident along the fast axis travels along the optical axis of the crystal, is reflected, and then outputs and returns to the slow axis component. After passing through the sensor, the slow axis component returns to the fast axis component. This process is called polarization rotation reflection.

As such, the reflected light returned with phase information proportional to the magnitude of the electric field causes the phase detector 20 to interfere with each other to obtain light intensity information proportional to the phase value.

Such a phase detector 20 will be described in detail with reference to FIG. 2.

Referring to FIG. 2, which shows the configuration of the phase detector of the optical sensor for electric field measurement of FIG. 1, the phase detector 20 includes a laser diode 21, a 3-dB coupler 22a and 22b. , Power splitter 23, polarization controller 24, phase modulator 25, polarizer 26a and 26b and photodetector 27a (27b).

First, the light output from the light source 21, that is, the laser diode, passes through the first light combiner 22a and proceeds to the sensor unit 10. At this time, the polarization direction of the light output from the light source 21 is connected to the first optical coupler 22a by tilting the light by 45 degrees, thereby generating TE polarization and TM polarization inside the optical waveguide, and then transmitting the optical polarization through the optical waveguide. Then, the first optical coupler 22a passes.

After the light is divided into two optical waveguides up and down while passing through the first optical coupler 22a, the light traveling to the lower output of the first optical coupler 22a is lost and disappears. On the other hand, the light traveling to the upper output of the first optical coupler 22a is incident to the sensor unit 10 through the polarization maintaining optical fiber 31.

In detail, the light incident on the sensor unit 10 passes through a Faraday rotator 12 located in front of the sensor unit 10, and the polarization direction of the TE polarization and the TM polarization are rotated by 45 degrees, respectively. . The linearly polarized light whose angle is changed passes through the lithium niobate 11 crystal in which the refractive index is sensitive to the electric field. At this time, in order to measure the phase change with respect to the Y-axis and X-axis polarization components generated by the electric field applied in the Z-axis direction, the input polarization components are adjusted through the axial direction of the crystal. It should be made parallel to the axial direction. In other words, the TM polarization component transmitted through the polarization maintaining optical fiber 31 should proceed to the X-axis direction component of the lithium niobate 11 crystal after the polarization is rotated by 45 degrees in the Faraday rotator 12.

The polarization components having passed through the lithium niobate 11 crystal are reflected by the reflection mirror 13 and returned in the opposite direction. In this process, the phase change caused by the electro-optic effect is doubled. The returned light undergoes 45-degree polarization rotation while passing through the Faraday rotator 12. The light is not returned to its original direction but is output as light that is twisted by 90 degrees with the original polarization direction. That is, the TE component of the input light is changed to the TM component while passing through two 45 degree Faraday rotators 12, and the input TM component is changed to the output TE component.

The phase change value due to the external electric field is left as a relative phase difference between the two polarization components, and the phase detector 20 is configured at the output terminal in order to convert the phase difference into an optical power difference to be detected by a photodetector. Should be.

The light, which has passed through the field measurement crystal material and is reflected and has a phase difference according to the electric field size, is again divided into two paths through the first light combiner 22a. At this time, the light propagating toward the light source 21 is disappeared by an isolator (not shown) located in front of the light source 21, and the light propagating toward the other is directed toward the photodetector 27a and 27b. .

Light output from the first optical combiner 22a passes through a power splitter 23 and is split into two paths. Light traveling to the left output of the power splitter 23 passes through the thermo-optic phase modulator 25 to be phase-modulated, and then only the TE polarization survives through the first polarizer 26a. On the other hand, the light traveling to the right output of the power splitter 23 passes through the polarization converter 24 and the second polarizer 26b, where the TE polarized light is actually a TM polarized component reflected by the sensor.

Finally, light passing through two different paths meets each other at the second optical coupler 22b to cause optical interference. As a result, the TE polarization component and the TM polarization component reflected by the sensor unit 10 cause interference with each other, and cause reinforcement or destructive interference according to the phase difference between each other. After the interference, the optical power change proportional to the phase difference can be measured by the two photo detectors 27a and 27b. Subsequently, if two light outputs are differentially amplified, it is possible to amplify and obtain a light output change signal due to interference.

According to the present invention, it is possible to implement an optical voltage sensor that operates stably regardless of external environment changes. In addition, it can be used as a sensor that can accurately measure the voltage value in the environment with severe electromagnetic interference by transmitting a high voltage current using this. In addition, it is possible to produce a low-cost mass production because it not only has a stable operating characteristics compared to the conventional optical voltage sensor, but also has the advantage of manufacturing the sensor through an easy process.

As described above, the present invention is not limited to the described embodiments, and various modifications and changes can be made without departing from the spirit and scope of the present invention, which will be apparent to those skilled in the art. Therefore, such modifications or variations will have to be belong to the claims of the present invention.

1: field sensor 10: sensor
11: Lithium niobate 12: Faraday rotator
13: reflection mirror 20: phase detector
21: laser diode 22a, 22b: optical coupler (3-dB coupler)
23: Power splitter
24: Polarization controller
25: Phase modulator
26a, 26b: Polarizer
27a, 27b: Photodetector
31: polarization maintaining optical fiber

Claims (6)

A phase detector 20 which includes a light source 21 for generating light and detects phase information of light emitted from the light source 21;
A sensor unit (10) including lithium niobate (11), an electro-optic crystal material having a property of changing an optical refractive index in proportion to an electric field; And
It includes a polarization maintaining optical fiber 31 connecting the sensor unit 10 and the phase detection unit 30,
The sensor unit 10 is formed of a polarization rotating reflection interferometer having Faraday rotator 12 and the reflection mirror 13 is disposed on the left and right of the lithium niobate 11,
Light composed of two polarization components incident through the polarization maintaining optical fiber 31 is transmitted to the lithium niobate 11 through the Faraday rotator 12 and the lithium niobate ( The two polarization components which are phase shifted through 11 are passed through the lithium niobate 11 once again in the opposite direction through the reflective mirror 13 to the Faraday rotator 12, and the Faraday rotator ( The two polarization components passing through 12 are transmitted to the phase detector 20 through the polarization maintaining optical fiber 31 again.
An optical sensor for electric field measurement, in which a phase change value due to an external electric field remains as a relative phase difference between two polarization components, so that the optical power change is measured by the phase detector 20. The method of claim 1,
The Faraday rotator (12) is an optical sensor for electric field measurement, characterized in that for rotating the polarization of the light reflected back to the reflection mirror (13) via the lithium niobate (11) by 90 degrees. The method of claim 1,
The phase detector 20,
A power splitter 23 for splitting light received from the sensor unit 10;
Phase modulator 25 for modulating the phase of the light of one side of the light branched from the power splitter 23,
A polarization controller 24 for converting polarization of light of the other side of the light branched from the power splitter 23;
A light combiner 22b in which the light output from the phase modulator 25 and the light output from the polarization converter 24 cause optical interference,
And an optical detector (27a) (27b) for measuring a change in optical power proportional to the phase difference of light causing interference in the optical coupler (22b). The method of claim 3, wherein
Between the phase modulator 25 and the optical coupler 22b and between the polarization converter 24 and the optical coupler 22b, polarizers 26a and 26b which pass only one of TE polarization or TM polarization are respectively respectively. Optical sensor for electric field measurement, characterized in that the intervening. The method of claim 1,
An optical sensor for electric field measurement, characterized in that a collimator lens (32) is further interposed between the polarization maintaining optical fiber (31) and the Faraday rotator (12).
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