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    • 专利摘要:
    The present invention relates to a device (1) for measuring a magnetic field (B) and / or an electric field (E) comprising: - a measurement cell (3) containing a gas sensitive to the Zeeman effect and / or to the Stark effect, - a polarized light source (7) whose wavelength is tuned to a gas absorption line sensitive to the Zeeman effect and / or to the Stark effect, - at least one polarimetry system (11) configured to measure a first parameter corresponding to the rotation of a polarization angle due to the crossing of the beam (9) in the measurement cell (3) containing a gas sensitive to the 'Zeeman effect and / or Stark effect, - an absorption measurement system (13) configured to measure a second parameter corresponding to the absorption of the beam (9) by the gas sensitive to the Zeeman effect and / or the Stark effect in the measurement cell (3 ), and - a processing unit (15) configured to combine the measurement of the first parameter corresponding to the rotation of the polarization angle and the absorption measurement to extract a third and / or fourth parameter corresponding respectively to an electric field (E ) and / or magnetic (B) to be measured.
    公开号:FR3075386A1
    申请号:FR1762656
    申请日:2017-12-20
    公开日:2019-06-21
    发明作者:Geoffrey Renon；Paul Vinson
    申请人:SuperGrid Institute SAS；
    IPC主号:
    专利说明:

    Device for measuring an electric and / or magnetic field, in particular in an electrical energy transport conductor
    The field of the present invention relates to the transport of electricity in high voltage alternating current and direct current (High Voltage Alternative Current (HVAC) and High Voltage Direct Current (HVDC) networks and distribution networks). more particularly to a cable for transporting electrical energy from such a network as well as an associated device making it possible to measure an electric and / or magnetic field, even a current and / or a voltage.
    The current development of renewable energies causes new constraints on the level of the electric network because the various places of production of electricity are generally far from each other and far from the areas of consumption. It therefore appears necessary to develop new transport networks capable of transporting electricity over very long distances while minimizing energy losses.
    To meet these constraints, high voltage direct current (HVDC) high-voltage networks (for example 50kV) appear to be a promising solution due to lower line losses and absence of AC networks. incidence of parasitic network capacities over long distances.
    To control the electrical energy transmission network, voltage and / or current are measured at appropriate locations on power lines or substations.
    To do this, we know for example inductive transformers composed of a winding surrounding the electrical conductor / cable for transporting electrical energy and operating on the principle of electromagnetic induction.
    However, such known devices do not allow measurements on cables for transporting electrical energy with direct current.
    Another defect of the known devices is linked to the weight of the winding surrounding the electrical conductor / electrical energy transport cable, especially when the latter is arranged in height. Indeed, in this case, the weight of the winding can cause significant mechanical stresses on the supports of the measuring device.
    More recently, other measurement methods have been developed to overcome the aforementioned defects.
    EP 0453693 relates to an “electric field sensor with Pockels effect”. This sensor presents a crystal intended to be crossed by a polarized monochromatic light beam in order to determine the value of an electric field and its direction.
    The Pockels effect is the appearance of birefringence in a medium created by a static or variable electric field. The birefringence which appears is proportional to the electric field which can therefore be measured.
    The sensor of EP0453693 comprises in particular a light source intended to generate a monochromatic light beam, a probe crystal and a photodetector of the photodiode type for example. The light source is connected to the probe crystal by a single-mode optical fiber and the probe crystal is connected to the detector by an optical fiber with polarization maintenance.
    The probe crystal used has a particular birefringent crystallographic structure when subjected to an electric field so that by measuring the phase difference between the two components of the polarization of the beam having passed through the probe crystal, the electric field can be measured.
    However, the probe crystal used is sensitive to temperature variations which makes its use in an energy transport network subject to climatic variations delicate. In addition, a temperature sensor and a compensation unit must be used to correct the effect of temperature variations on the measurements.
    Another effect that can be used to measure, for example, a current, is the Faraday effect. The Faraday effect results from the interaction between light and a magnetic field in a material. Indeed, the polarization of the light performs a rotation proportional to the component of the magnetic field on the direction of propagation of the light. This component of the magnetic field being proportional to the current in the electrical conductor / energy transport cable, we can then measure the current by measuring the rotation of the polarization.
    An example of such a measuring device is described in EP0108012.
    The device described in this document has an optical fiber wound around the electrical conductor and through which passes a monochromatic light beam generated by a light source, such as for example a laser diode. On the other hand, the device described here presents a device for analyzing the light polarization at the output of the optical fiber. The analysis device comprises a polarizing separator cube, two photodiodes each detecting the intensities of light beams linearly and orthogonally polarized, and an analog unit calculating the representative ratio of the intensity to be measured in the electrical conductor / transport cable of the electric energy.
    In this case too, there is a dependence of the Faraday effect on the temperature, which requires a subsequent correction of the measurement result.
    CN206057424 exploits yet another effect: the Hall effect. This document discloses a current measurement device comprising a Hall effect detector and a temperature detection unit in order to make corrections to the measurements taken as a function of the temperature of the Hall effect detector. The device described here also includes a microprocessor intended to process and correct the voltage data measured by the Hall effect detector. This document specifies that the current passing through the electrical conductor / cable for transporting electrical energy generates a proportional magnetic field making it possible to detect the intensity and the voltage of the current flowing in the electrical conductor / cable for transporting electrical energy.
    The object of the present invention is to provide a device for measuring an electric or magnetic field which can overcome temperature variations and which can be robust enough to be able to be installed in places subject to significant climatic variations.
    To this end, the present invention relates to a device for measuring a magnetic field and / or an electric field comprising:
    a measuring cell containing a gas sensitive to the Zeeman effect and / or to the Stark effect, in particular an alkaline gas, and intended to be placed in a magnetic and / or electric field, a polarized light source whose length wave is tuned to a gas absorption line sensitive to the Zeeman effect and / or to the Stark effect and which emits a beam of light passing through said measurement cell, at least one polarimetry system configured to measure a first parameter corresponding to the rotation of a polarization angle due to the crossing of the beam in the measurement cell containing a gas sensitive to the Zeeman effect and / or to the Stark effect, a absorption measurement system configured to measure a second parameter corresponding to the absorption of the beam by the gas sensitive to the Zeeman effect and / or the Stark effect in the measurement cell, and a processing unit configured to combine the measurement of the first parameter corresponding to the rotation of the polarization angle and the absorption measurement to extract a third and / or fourth parameter corresponding respectively to an electric and / or magnetic field to be measured.
    The invention may further include one or more of the following aspects taken alone or in combination:
    In one aspect, the alkaline gas is, for example, rubidium, lithium, sodium, potassium, cesium or francium.
    The device may include a measuring head comprising a blade separating the light beam from the polarized light source into at least two partial light beams and reflectors to define two measurement branches perpendicular to each other, the measuring cell being arranged in the measuring head at the intersection of the two partial beams.
    The measurement head is for example connected to the polarized light source, the polarimetry system and the absorption measurement system by optical fibers.
    According to another aspect, the path of the light beam passing through the measurement cell has at least one component collinear with the magnetic or electric field to be measured or is collinear with the magnetic or electric field to be measured.
    The measuring cell can be a cube having a first side of length between 0.1 mm and 20 mm and a second side of length between 0.1 mm and 25 mm or a cylinder of height between 0.1 mm and 20 mm and with a diameter between 0.1 mm and 25 mm.
    The polarimetry system is in particular a balanced polarimetry system arranged downstream of the measurement cell and comprising a beam polarizer splitter as well as two associated photodetectors.
    The absorption measurement system comprises, for example, a first and a second beam splitter plates arranged respectively upstream and downstream of the measurement cell as well as two photodetectors associated with each of the beam splitter blades and configured to detect the intensity of the light beam upstream and downstream of the measuring cell.
    The light source is in particular a laser, in particular a laser diode.
    It is possible to provide a single laser light source used both to measure at least one electric field and at least one magnetic field.
    The invention further relates to a unit for measuring a current and / or a voltage at the level of an electrical conductor of medium or high voltage comprising at least one measuring device as defined above and in that the processing unit is further configured to determine, as a function of the distance between the electrical conductor and the measuring cell, a voltage relative to earth and / or an electric current flowing in the conductor.
    The invention further relates to a post in a metallic envelope comprising a metallic envelope enclosing a medium or high voltage electrical conductor, in which it comprises a measuring device as defined above, the measuring cell of which is arranged inside the post, in particular fixed against the internal part of the metal casing.
    Other characteristics and advantages of the invention will emerge from the following description, given by way of example and without limitation, with reference to the appended drawings in which:
    FIG. 1 represents an illustrative diagram concerning the polarization of the light,
    - Figure 2 presents two simplified diagrams modeling energy levels of an alkaline atom, this for part a) in the absence of any electromagnetic field and for part b) in the presence of a magnetic or electric field parallel to the direction of propagation of a beam of light,
    - Figure 3 shows a simplified diagram of a measuring device according to a first embodiment,
    - Figure 4 A is an explanatory diagram of the electric and magnetic fields formed around a current conductor,
    FIG. 4B is a simplified diagram showing two measuring devices arranged around an electric current conductor for measuring both the magnetic field and the electric field at a predetermined distance from the conductor,
    FIG. 5 is a simplified and optimized variant of the embodiment of FIG. 4B,
    FIG. 6 is an exemplary embodiment of a measuring device for measuring electric and / or magnetic fields near several electrical conductors,
    FIG. 7 is a simplified diagram of a second embodiment with a measurement head on the one hand and a measurement base on the other hand connected to each other by optical fibers,
    FIG. 8 is a simplified diagram of a station with a metallic envelope comprising a measuring device according to a third embodiment, and
    - Figures 9 and 10 are simplified diagrams in cross section of an embodiment of a measuring head of Figure 8.
    In all the figures, the elements having identical functions bear the same reference numbers.
    The following embodiments are examples. Although the description refers to one or more embodiments, this does not necessarily mean that each reference relates to the same embodiment, or that the characteristics apply only to a single embodiment. Simple features of different embodiments can also be combined or interchanged to provide other embodiments.
    By “upstream” or “downstream”, the elements are located in the direction of propagation of the light. Thus, a first piece of equipment or element is located upstream of a second piece of equipment or element if the light beam passes first through the first and then the second piece of equipment.
    In this presentation, certain references may be supplemented by a letter designating the purpose of the field to be measured. For example, a photodetector 19 can become a photodetector 19E when it intervenes in the measurement of an electric field and 19B in the case of a magnetic field. A measurement head 33 can become a measurement head 33E when it intervenes in the measurement of an electric field and 33B in the case of a magnetic field or 33EB if it intervenes at the same time for a measurement of a magnetic field B and electric E.
    The present invention relates to any installation of medium or high voltage, alternating or direct current and in particular electrical conductors / cables for transporting electrical energy or, for example, stations with air insulation or stations in metal envelopes.
    The present invention finds a particularly interesting application in a high voltage direct current network (High voltage Direct Current (HVDC) in English) for the transport of electrical energy, that is to say current.
    FIG. 1 represents an illustrative diagram concerning the polarization of the light. A light wave is an electromagnetic wave whose electric field Ê and magnetic field B form a direct trihedron with the direction of propagation of this wave. This electric field evolves during the propagation of this wave by describing a specific shape if we observe it when facing the wave. Thus, the polarization of the wave (direction of the electric field) during its propagation can be classified into 3 categories: rectilinear polarization, circular polarization and elliptical polarization.
    The Zeeman effect (for the magnetic field B) and the Stark effect (for the electric field E) are effects that take place on the electronic energy levels of atoms (alkaline among others). These effects can be seen when you can interact with these energy levels. One way to interact with these levels is to use the interaction of the electronic spins of the atoms in question with photons from resonant light radiation, for example a laser, with the energy level to be interrogated.
    The Zeeman effect or the Stark effect will then be observable using a light wave with linear polarization in interaction with the energy levels involved. This observation is made by controlling the rotation of linear polarization of the light wave.
    These effects can be particularly well observed for example in gases formed from atoms with a single valence electron, such as for example alkaline atoms. The alkalis are widely used in many applications due to the unique valence electron with mismatched spin which can be easily manipulated. Thus, we can approximate the energy of the atom by the energy of the single electron on the valence band.
    However, when it is a gaseous medium, these two Stark and Zeeman effects depend on the density of the medium crossed by the light and therefore also on the temperature.
    Figure 2 for part a) presents a simplified diagram modeling the energy levels of an alkaline atom in the absence of any electromagnetic field.
    It is therefore a simplified energy system at three levels (the fundamental sub-level m F = 0 does not intervene in the atomelaser interaction process that we will describe).
    This system has a fundamental level which is composed of three fundamental sub-levels of moment m F = -1, m F = 0, and m F = +1. This system also has an excited level without momentary sublevels m E = 0.
    When a linearly polarized light wave with a given direction of propagation propagates, we can decompose this linear polarization into the sum of two circular polarizations of opposite direction σ + and σ_.
    Thus the light wave will interact with the two fundamental sub-levels of moment m F = -1 and m F = +1 to put the electron on the excited level of moment m E = 0. This is explained by a rule selection concerning the conservation of the angular momentum and the fact that the σ + wave exchanges a photon of moment +1 and the σ_ wave exchanges a photon of moment -1.
    FIG. 2 concerning part b) shows a simplified diagram modeling the energy levels of an alkaline atom in the presence of a magnetic field B or electric Ê parallel to the direction of propagation p ^ of a beam of light.
    The application of a collinear electric or magnetic field B to the direction of propagation of the light wave causes an energetic displacement of the fundamental sublevels of moment m F = -1 and m F = +1 (positive for the one and negative for the other, and vice versa in case of opposite direction field).
    In the case of an electric field, this effect is called the Stark effect and the value of this energy offset ô ^ rj is:
    ^ nrj = II · 1 'PeI | E Pe | ec l · (1) with μ the dipole moment of the alkaline atom.
    In the case of a magnetic field B this effect is called the Zeeman effect and the value of the energy shift ô ^ rj is then:
    ^ nrj - | fb 'B | eq- (2) with the Boron magneton.
    There is an energy difference of 26n RJ in the case of application of an electric field and 2δθ ΚΙ in the case of application of a magnetic field between the 2 fundamental sublevels of moment m F = -1 and m F = +1 as can be seen in Figure 2b). This therefore generates a difference between the interaction of the component σ + and the component σ_ with the electrons of the alkaline atom considered.
    After mathematical reconstruction of the polarization of the light wave, the linear polarization of the light wave having passed through an alkaline atom medium of length f is rotated by an angle θ of:
    n al -TE 2 eq. (3) θΒ - Ψβ '^ al''B θΡ · (4) with
    - the light material interaction parameter in the presence of an electric field,
    - E the component of the electric field along the axis of propagation of the light wave p ^,
    - matière the light material interaction parameter in the presence of a magnetic field,
    - B the component of the magnetic field along the axis of propagation of the light wave p ^,
    - n al the alkali volume density which is a temperature dependent parameter.
    It is therefore understood that the detection of the rotation of the polarization of the light wave by polarimetry makes it possible, when the density is known or when the latter is fixed, to measure an electric field and / or a magnetic field.
    The density of alkaline gas present in a measuring cell is dependent on the temperature (saturated vapor pressure). In order to overcome this problem, it is proposed to use the phenomenon of absorption of the light beam by the alkaline gas. Indeed, the power P T of the light beam at the output of a measurement cell as a function of the input power P o is given by the relation:
    P T = eq. (5) with i | i Abs the known parameter of light material interaction due to absorption. We then have:
    ln (^) = ΨΑύ 5 n a i · £ eq. (6)
    By isolating in this formula n al :
    "= Eq - (7 >
    And by using equation (7) in equations (3) and (4) above, we can therefore get rid of the effect of temperature.
    θϊ = 1 ΟΐΣ7 ' Ε2 e * < 8 >
    0 s = ln ® ^ 7 ' B e * < 9 >
    FIG. 3 shows an example of a simplified diagram of a measurement device 1 according to a first embodiment combining both the polarimetry and the absorption measurement to result either in a measurement of the magnetic field, or in a measurement electric field as appropriate if the propagation of the light beam is collinear with the magnetic or electric field.
    The measuring device 1 for a magnetic field and / or an electric field comprises a measuring cell 3 containing a gas sensitive to the Zeeman effect and / or to the Stark effect, in particular an alkaline gas, and intended to be placed in a magnetic and / or electric field indicated by arrow 5, a polarized light source 7 whose wavelength is tuned on a gas absorption line sensitive to the Zeeman effect and / or to the Stark effect contained in the measurement cell 3 and which emits a light beam 9 passing through said measurement cell 3, a polarimetry system 11 configured to measure a first parameter corresponding to the rotation of a polarization angle due to the crossing in the gas sensitive to the Zeeman effect and / or to the Stark effect of the beam in the measurement cell 3, an absorption measurement system 13 configured to measure a second parameter corresponding to the absorption by the gas sensitive to the Zeeman effect and / or to the Stark effect of the beam 9 in the measurement cell 3, and a processing unit 15 configured to combine the measurement of the first parameter corresponding to the rotation of the angle of polarization and the absorption measurement to extract a third and / or fourth parameter corresponding respectively to an electric field E and / or magnetic B to be measured.
    The gas sensitive to the Zeeman effect and / or to the Stark effect contained in the measuring cell 3 is therefore in particular an alkaline gas, for example composed of rubidium, lithium, sodium, potassium, cesium atoms or francium.
    The measurement cell 3 is in particular transparent to the wavelength of the light source 7 used. It suffices that only the passage faces of the light beam 9 are transparent. The other surfaces can be opaque which can be advantageous for eliminating possible disturbances by ambient light.
    The measuring cell 3 is for example a cube / parallelepiped having a first side of length between 0.1 mm and 20 mm and a second side of length between 0.1 mm and 25 mm or a cylinder of height between 0 , 1 mm and 20 mm and diameter between 0.1 mm and 25 mm. It therefore has dimensions that are small enough to be able to be installed in any suitable place in an electrical energy transport installation, or even, as will be detailed below, to integrate it into the equipment of this installation. In addition, a small cell allows you to play on the measurement range while impacting the sensitivity.
    The light source 7 is for example a laser, in particular a laser diode. The wavelength of the laser is chosen according to the absorption transition of the alkaline chosen.
    The following table gives examples of wavelengths for a given alkaline and a given transition.
    Alkaline Wavelength At D1 (nm) Wavelength λ Ο2 (nm) jy K = Potassium 39 770.108 766.701 4U K = Potassium 40 41 K = Potassium 41 B3 Rb = Rubidium 85 794.979 780.241 B / Rb = Rubidium 87 Cs = Cesium 894.593 852.347
    The polarimetry system 11 is in particular a balanced polarimetry system which is arranged downstream of the measurement cell 3. This polarimetry system 11 comprises in particular a beam polarizer splitter 17 as well as two associated photodetectors 19 and 21.
    The polarizing beam splitter 17 (“polarizing beam splitter” in English - PBS in the figures) separates the polarization components s and p to send them respectively to the photodetectors 19 and 21 (“photodetector” in English - PD in the figures ), for example photodiodes. For example, the polarization component s is reflected at 90 ° towards the photodetector 19 while the p component crosses the beam polarizer splitter 17 to be detected by the photodetector 21.
    Thus, taking into account the measurement signals from the photodetectors 19 and 21, it is possible to measure the angle of polarization of the light beam at the output of the measurement cell 3 and it is possible to determine, by knowing the starting linear polarization at the output of the light source 7, the variation of the polarization angle which makes it possible to determine the value of the electric and / or magnetic field to be measured.
    For reasons of simplification of explanation and not restrictive, we place ourselves in the situation where the input polarization in the measurement cell is at 45 ° relative to the component s or p of the beam polarizer splitter 17.
    We then have the output signal for the electric field Ë * and for the magnetic field B *, of component E respectively for the electric field and of component B for the magnetic field along the axis of propagation of the laser.
    which is given by:θΕ - “Att ρθ 2 - Ψε ' n al' * 'E 2 eq. (10)θΒ - “AU 'p 2 - Ψβ' n al '*' B r 0 eq. (11) With
    E = component of the electric field E collinear with the direction of propagation of the light beam 9,
    B = component of the collinear magnetic field B with the direction of propagation of the light beam 9,
    - a Att the known or predetermined attenuation coefficient of the light beam
    - Pi the light intensity measured by the photodetector 19
    - P 2 the light intensity measured by the photodetector 21
    - P o the light intensity measured by the photodetector 25
    Of course, it is assumed in our case that Ë * 1! T, that is to say that the light beam is oriented so as to be sensitive only to one of the two electric or magnetic fields.
    In order to be able to adjust the linear polarization of the light beam 9 relative to the beam polarizing splitter 17, a half-wave plate 22 (also noted λ / 2 in the figures) is placed upstream of the measurement cell 3.
    The absorption measurement system 13 will be used to overcome temperature dependence. It includes an upstream part 13A and a downstream part 13B. In more detail, the upstream part 13A comprises a first beam splitter plate 23 (“beamsplitter” in English - BS in the figures) disposed upstream of the measurement cell 3 as well as an associated photodetector 25 configured to detect the intensity light of the light beam 9 upstream of the measurement cell 3. The downstream part 13B comprises a second beam splitting plate 27 disposed downstream of the measurement cell 3, but upstream of the polarimetry system 11, as well as a associated photodetector 29 configured to detect the light intensity of the light beam 9 downstream of the measurement cell 3.
    This temperature-dependent signal can then be corrected with the absorption signal as defined above. The output signal for the electric field of equation (10) or for the magnetic field of equation (11) then becomes:

    TpAbs
    B ^ Abs
    eq. (12) eq. (13)
    A signal independent of the temperature is thus obtained allowing the measurement of the electric field or the magnetic field. To return to the absolute value of the field E or B to be measured, it is for example possible to use a calibration to determine the correspondence between the measurement signal S and the value of the field E or B.
    To then go back to the electric current flowing in an electrical conductor or the voltage with respect to earth, it is necessary to take into account the distance of the measurement cell 3 from the electrical conductor.
    Since the alkaline atoms are confined in the measuring cell, the absorption rate is ultimately only dependent on the temperature. Thus, the use of the signal of P T on the photodetector 29 also allows a local measurement of the temperature. Indeed, the density of alkali n ai is dependent on the temperature T in Kelvin with by the following relation:
    ^ Abs 1Q 18.9848 + aT eq · (14) with a and b parameters specific to each alkali.
    With a mathematical calculation taking into account the signal - so can p o measure the local temperature simultaneously with the measurement of the electric or magnetic field.
    In FIG. 3, the light source 7 directly supplies the optoelectronic assembly which can also be called a measuring head 33.
    Alternatively, the light source 7, that is to say for example a laser, is for example offset from the measuring head 33, the two being connected to each other by an optical fiber.
    FIG. 4 A is an explanatory diagram of the electric F and magnetic fields F formed around a current conductor 31.
    The magnetic field B is circular around the conductor 31, while the electric field F points in a radial direction perpendicular to the magnetic field F.
    FIG. 4B is a simplified diagram showing the same electrical conductor 31 in cross section as well as the electric fields F and magnetic F formed around an electric current conductor 31. In addition, two measuring heads 33E have been indicated schematically , 33B electric (E) and magnetic (B) of two measuring devices 1 arranged around the electric current conductor 31 to measure both the magnetic field and the electric field at a predetermined distance R from the electric conductor 31. In this example embodiment, the light sources 7E and 7B are connected to the respective measurement heads 33E, 33B by optical fibers 41, that is to say 41E between the light source 7E and the measurement head 33E and 41B between the light source 7B and the measuring head 33B.
    As can be seen by the longitudinal orientation of the measurement heads 33E and 33B shown diagrammatically in FIG. 4B, the light beam of the measurement head 33E is in its part passing through the measurement cell 3 collinear with the electric field F and the the light beam from the measuring head 33B is in its part passing through the measuring cell 3 collinear with the magnetic field EL ·
    In this configuration, the electric current I flowing in the electric conductor 31 is given by the relation:
    j 2 tîRB μο eq. (15)
    Where p o is the magnetic permeability of the vacuum.
    Similarly, the voltage of the electrical conductor 31 is obtained with respect to the earth.
    The relationship between the measured electric field E o and the voltage applied to the current conductor 31 V o is given by the following relationship:
    V „= rln (^) E 0 (eq. 16)
    Of course, by performing a calibration with an electrical conductor 31 in which a known current flows, it is possible to calibrate the measurement device 1 and correlate the measurement signals and the parameter to be measured (electric or magnetic field).
    Figure 5 is a simplified and optimized variant of the embodiment of Figure 4B combining the measuring heads 33E and 33B into a single measuring head 33EB. In this case, the measuring head 33EB comprises a plate 35 separating the light beam 9 coming from the polarized light source 7 into two partial light beams 9E and 9B, reflectors for defining two perpendicular measurement branches, one to the other, the measurement cell 3 being arranged in the measurement head at the intersection of the two partial beams 9E and 9B.
    In this assembly, we therefore added to the assembly presented in FIG. 3 with a polarimetry system 11E the separating plate 35 as well as two reflectors 37 and 39 for directing the light beam 9B into the measurement cell 3 by crossing the beam of light 9B perpendicular to that of the beam 9E. At the output of the measurement cell 3, the beam 9B is directed towards a polarimetry system 11 B.
    As shown in FIG. 5, the polarized light beam 9 can be routed to the measuring head 33EB either directly or via an optical fiber 41.
    FIG. 6 is an exemplary embodiment of a measuring device 1 for measuring electric and / or magnetic fields near several electrical conductors 31. In this case, the measuring heads 33, here 33E or B as well as 33EB can be powered by the polarized light beam 9 of a single laser 7. In this example, a measurement head 33E or B is identical to that of FIG. 3 with an orientation of the light beam collinear with the electric field and another measurement head 33EB is identical to that of FIG. 5 for measuring both the electric and magnetic fields of an electric conductor 31.
    FIG. 7 is a simplified diagram of a second embodiment in which for the measurement head part 33EB, the optical / placement functions of the measurement cell 3 and the measurement functions are separated with the optronic components comprising in particular the photodetectors and one or more polarization beam splitters 17E and 17B.
    Thus, the measurement head 33 is divided into a probe head 42 and a measurement base 43.
    The probe head 42 comprises in its center the measurement cell 3. It is further connected to an input optical fiber 411 connected to the light source 7 as well as an output optical fiber 41E for routing the partial beam of light 9E having passed through the measuring cell 3 while being collinear with the electric field E towards a corresponding input of the measuring base 43 and an optical output fiber 41B for routing the partial beam of light 9B having passed through the measuring cell 3 by being collinear with the magnetic field B towards a corresponding input of the measurement base 43. In the probe head 42 are therefore only present, in addition to the measurement cell 41, reflectors 37 and a separating plate 35.
    In the measurement base 43 are installed the light source 7, two polarimetry systems 11E and 11B as well as the absorption measurement system
    13. This configuration makes it possible to place in particular photodetectors 19E, 19B, 21 E, 19B, 21 B, 25, 29 further from the electrical conductor 31, for example a few meters or tens of meters, or even more. Thus the photodetectors 19E, 19B, 21 E, 21 B, 25, 29 can be placed farther from the electrical conductor 31 in order to better overcome potential electromagnetic disturbances which can be generated by the electric and magnetic fields of the electrical conductor 31 on the measurement sensors. Alternatively, the measurement base 43 is installed and integrated in a metal housing serving as a Faraday cage.
    FIG. 8 is a simplified and partial diagram of a metal-cased substation 51 enclosing a medium or high voltage electrical conductor 31 and comprising a measurement device 1 with a measurement base 43 very similar to that of FIG. 7 with the difference that the separation into two partial beams 9E and 9B by the separating blade 35 takes place in the measurement base 43 so that four optical fibers 41 are connected to the probe head 42.
    Figures 9 and 10 are simplified diagrams in cross section of an exemplary embodiment of a probe head 42 of Figure 8 integrated in the metal casing 51 according to two cutting planes perpendicular to each other.
    As can be seen in FIGS. 9 and 10, the measurement cell 3 is arranged inside the metal casing 51 and in particular fixed against the internal part of the metal casing 51.
    To this end, the metal casing 51 comprises at the level of the measuring cell 3 a window 53 fixed by a flange 55 to allow the light beam 9E (FIG. 9) and 9B (FIG. 10) to pass.
    A rear wall 57 of the measurement cell 3 opposite the window 53 is reflective or provided with a mirror.
    Thus, to detect the electric field E (FIG. 9), the light beam 9E evolves in a plane which is perpendicular to the magnetic field B. The light beam 9E enters at a certain angle into the measurement cell 3, is reflected by the rear wall 57 to then be sent to the measurement base 43.
    In this configuration, only the collinear component of the 9E light beam contributes to the Stark effect. The size of the measuring cell 3 can be quite small because the light beam 9E crosses the measuring cell 3 twice (round trip).
    Then, to detect the magnetic field B (FIG. 10), the light beam 9B evolves on a path where it is partly collinear with the magnetic field B and with the electric field E. The light beam 9B returns at a certain angle in the measurement cell 3, is reflected by the rear wall 57 in order then to be sent to the measurement base 43.
    In this configuration, only the collinear components of the electric E and magnetic fields B of the light beam 9B contribute respectively to the Zeeman effect and to the Stark effect. By first determining the electric field E according to the assembly of FIG. 9, one can determine the magnetic field B by the measurement according to the assembly of FIG. 10 by removing from the measurement result by calculation the contribution of the electric field E which is known from the measurement according to the assembly of FIG. 9. The size of the measurement cell 3 can be quite small because the light beam 9B crosses the measurement cell 3 twice (round trip).
    Next, we will give a specific example for current and voltage measurements.
    It is assumed that the alkaline gas used in measuring cell 3 is for example rubidium for the Stark effect and the Zeeman effect.
    The relation between the current in Ampere (A) and the angle of rotation of the polarization Q z for the Zeeman effect is given by:
    o - δ - 1b ' w - “Zeeman (eq. 17) with
    - r the distance between the current conductor 31 and the measuring cell 3 in mm,
    - w the diameter of the light beam 9 in the measuring cell 3 in mm,
    - 1 B length traveled in mm of the part of the path of the light beam 9B which is collinear with the magnetic field B.
    10 _4 rad .- ^ - / A <AZeeman <1,2 10 -3 rad .- ^ / A, this range is mm 2 'ieenidii mm2 / dependent on the chosen energy transition of rubidium. By inverting this equation, we therefore go back to the current in the current conductor 31.
    The relation between the voltage U in kV and the angle of rotation 0 S for the Stark effect is given by:
    (eq. 18) with
    - r 0 the radius of the current conductor 31 in mm,
    - r the distance between the current conductor 31 and the measuring cell 3 in mm,
    - 1 E length traveled in mm of the part of the path of the light beam 9E which is collinear with the electric field E.
    - 4 10 “ 3 rad. ^ / KV 2 <A stark <1,2 10“ 2 rad. ^ / KV 2 mm 2 ' 3ldlR mm 2 ' this range is dependent on the chosen energy transition of rubidium. By inverting this equation, we therefore go back to tension.
    Voltage and alternating current measurement:
    When applying an alternating voltage V (t) = V o cos (œt), an electric field is obtained defined by the following relation:
    Thus, we measure an angle of rotation given by the following relation:
    0g (t) = n al -TE (t) 2 (eq. 20)
    0g ( t ) = Ψε h * 1 {E ° [1 + cos (2œt)] (eq. 21) (eq- 21)
    We then obtain a signal composed of 2 components:
    - a continuous component
    - an alternative component with a frequency 2 times higher
    When applying an alternating current I (t) = I o cos (ωΐ), we obtain a magnetic field defined by the following relation:
    B (t) = 4πμ 0
    Thus, we measure an angle of rotation given by the following relation:
    θβΦ = Ψβ ' n ai *' B (t)
    0g (t) = Ψβ ' n ai'' B o cos (œt) (eq. 22) (eq. 23) (eq. 24)
    It is therefore understood that the present invention is distinguished by its small size, the active part (alkaline gas in the measuring cell 3) for the current and the voltage can be less in volume than 10 cm 3 .
    The active part being a gas in a sealed measuring cell 3, the physical measurement is absolute and does not drift over time. The only drift parameters are controllable parameters (temperature) or which can be calibrated in the remote part.
    The only wearing part is potentially the light source 7 which can be removed from the conductor 31. Maintenance is therefore easy and easy.
    The optical measurement presented above allows a sensitive measurement and with a high bandwidth.
    As described above, the measuring device is easy to implement. The various photodetectors do not need to be in contact with the current conductor 31 for the measurement of current and voltage. This also provides galvanic isolation of the measurement chain from the power grid.
    Finally, the measuring device 1 allows measurements of currents and voltages in direct current as in alternating current.
    权利要求:
    Claims (12)
    [1" id="c-fr-0001]
    1. Device for measuring (1) a magnetic field (B) and / or an electric field (E) comprising:
    a measuring cell (3) containing a gas sensitive to the Zeeman effect and / or to the Stark effect, in particular an alkaline gas, and intended to be placed in a magnetic (B) and / or electric (E) field , a polarized light source (7) whose wavelength is tuned to a gas absorption line sensitive to the Zeeman effect and / or to the Stark effect and which emits a beam of light (9) passing through said measurement cell (3), at least one polarimetry system (11) configured to measure a first parameter corresponding to the rotation of a polarization angle due to the crossing of the beam (9) in the measurement cell (3 ) containing a gas sensitive to the Zeeman effect and / or to the Stark effect, an absorption measurement system (13) configured to measure a second parameter corresponding to the absorption of the beam (9) by the gas sensitive to the Zeeman effect and / or the Stark effect in the measurement cell (3), and a unit processing (15) configured to combine the measurement of the first parameter corresponding to the rotation of the polarization angle and the absorption measurement to extract a third and / or fourth parameter corresponding respectively to an electric field (E) and / or magnetic (B) to be measured.
    [2" id="c-fr-0002]
    2. Measuring device according to claim 1, in which the alkaline gas is rubidium, lithium, sodium, potassium, cesium or francium.
    [3" id="c-fr-0003]
    3. Measuring device according to any one of the preceding claims, in which it comprises a measuring head (33) comprising a separating blade (35) of the light beam (9) coming from the polarized light source (7) in at least two partial beams (9E, 9B) of light and reflectors (37, 39) to define two measuring branches perpendicular to each other, the measuring cell (3) being arranged in the measuring head (33) at the crossing of the two partial beams (9E, 9B).
    [4" id="c-fr-0004]
    4. Measuring device according to the preceding claim, in which the measuring head (33) is connected to the polarized light source (7), the polarimetry system (11) and the absorption measurement system (13) by optical fibers (41).
    [5" id="c-fr-0005]
    5. Device according to any one of the preceding claims, in which the path of the light beam (9) passing through the measuring cell (3) has at least one component collinear with the magnetic (B) or electric (E) field to be measured. or is collinear with the magnetic (B) or electric (E) field to be measured.
    [6" id="c-fr-0006]
    6. Device according to any one of the preceding claims, in which the measuring cell (3) is a cube having a first side of length between 0.1 mm and 20 mm and a second side of length between 0.1 mm and 25 mm or a cylinder with a height between 0.1 mm and 20 mm and a diameter between 0.1 mm and 25 mm.
    [7" id="c-fr-0007]
    7. Device according to any one of the preceding claims, in which the polarimetry system (11) is a balanced polarimetry system disposed downstream of the measurement cell (3) and comprising a beam polarizer splitter (17) as well as two associated photodetectors (19, 21).
    [8" id="c-fr-0008]
    8. Device according to any one of the preceding claims, in which the absorption measurement system (13) comprises a first and a second beam splitter blades (23, 27) disposed respectively upstream and downstream of the measurement cell. (3) as well as two photodetectors (25, 29) associated with each of the beam splitting plates (23, 27) and configured to detect the light intensity of the light beam (9) upstream and downstream of the measurement cell (3).
    [9" id="c-fr-0009]
    9. Device according to any one of the preceding claims, in which the light source (7) is a laser, in particular a laser diode.
    [10" id="c-fr-0010]
    10. Device according to the preceding claim wherein a single source of laser light (7) is used both to measure at least one electric field (E) and at least one magnetic field (B).
    [11" id="c-fr-0011]
    11. Unit for measuring a current and / or a voltage at the level of an electrical conductor (31) of medium or high voltage comprising at least one measuring device (1) according to any one of the preceding claims and in that the processing unit (15) is further configured to determine as a function of the distance between the electrical conductor (31) and the measuring cell (3) a voltage relative to earth and / or an electric current circulating in the conductor (31).
    [12" id="c-fr-0012]
    12. Station in a metal envelope comprising a metal envelope (51) enclosing an electrical conductor (31) medium or high voltage, in which it comprises a measuring device (1) according to any one of claims 1 to 10 including the cell measure (3) is arranged inside the station, in particular fixed against the internal part of the metal casing (51).
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    同族专利:
    公开号 | 公开日
    US20200408855A1|2020-12-31|
    US11099242B2|2021-08-24|
    CN111492252A|2020-08-04|
    EP3729107A1|2020-10-28|
    JP2021508049A|2021-02-25|
    WO2019122693A1|2019-06-27|
    FR3075386B1|2020-07-10|
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    法律状态:
    2018-12-21| PLFP| Fee payment|Year of fee payment: 2 |
    2019-06-21| PLSC| Publication of the preliminary search report|Effective date: 20190621 |
    2019-12-20| PLFP| Fee payment|Year of fee payment: 3 |
    2020-12-28| PLFP| Fee payment|Year of fee payment: 4 |
    2021-12-17| PLFP| Fee payment|Year of fee payment: 5 |
    优先权:
    申请号 | 申请日 | 专利标题
    FR1762656|2017-12-20|
    FR1762656A|FR3075386B1|2017-12-20|2017-12-20|DEVICE FOR MEASURING AN ELECTRIC AND / OR MAGNETIC FIELD ESPECIALLY IN A CONDUCTOR OF ELECTRIC ENERGY TRANSPORT|FR1762656A| FR3075386B1|2017-12-20|2017-12-20|DEVICE FOR MEASURING AN ELECTRIC AND / OR MAGNETIC FIELD ESPECIALLY IN A CONDUCTOR OF ELECTRIC ENERGY TRANSPORT|
    EP18833976.6A| EP3729107A1|2017-12-20|2018-12-18|Device for measuring an electric and/or magnetic field in particular in a conductor for transporting electrical power|
    US16/772,081| US11099242B2|2017-12-20|2018-12-18|Device for measuring an electric and/or magnetic field in particular in a conductor for transporting electrical power|
    PCT/FR2018/053380| WO2019122693A1|2017-12-20|2018-12-18|Device for measuring an electric and/or magnetic field in particular in a conductor for transporting electrical power|
    CN201880081907.1A| CN111492252A|2017-12-20|2018-12-18|Device for measuring electric and/or magnetic fields, in particular in an electrical energy transmission conductor|
    JP2020533792A| JP2021508049A|2017-12-20|2018-12-18|A device that measures a specific electric and / or magnetic field in a conductor to transport power|
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