• 专利附录
  • 专利说明
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    • 专利摘要:
    The photovoltaic system being intended to deliver an electric current (I), the method comprises the measurement steps (E0) of values representative of the electric current (I) delivered by the photovoltaic installation, of adjustment (E2) of a variable current jump threshold (S (ti)), as a function of measured values, of detection (E3) of a current jump having an amplitude greater than an adjusted current jump threshold as a function of values measured before the jump and detecting (E5) an electric arc on detection of a current jump.
    公开号:FR3044487A1
    申请号:FR1561622
    申请日:2015-12-01
    公开日:2017-06-02
    发明作者:Nicolas Chaintreuil；Stephane Siat；Christian Kern
    申请人:Commissariat a lEnergie Atomique CEA；Socomec SA；Commissariat a lEnergie Atomique et aux Energies Alternatives CEA；
    IPC主号:
    专利说明:

    Title: Method and device for detecting an electric arc in a photovoltaic system
    TECHNICAL FIELD OF THE INVENTION The invention relates to a method and a device for detecting an electric arc in a photovoltaic installation. It also relates to a photovoltaic installation equipped with such a device. State of the art
    Photovoltaic installations operate with continuous electrical current and voltage, which is problematic in the event of the appearance of an electric arc. Such an electric arc can for example appear because of a lack of connections, following the opening of a connector in charge or further degradation of a connector by corrosion. In continuous current and voltage, there is no natural extinction of the electric arc by zero crossing of the voltage and current, as is generally the case in alternating current. The electric arc generates a plasma that emits a very strong heat for a long time. Such a plasma is destructive and often generates fire. For safety reasons, it is therefore important to detect the presence of a potential electric arc in a photovoltaic installation and to interrupt it in order to avoid any deterioration or fire.
    An electric arc corresponding to a plasma which appears between two electrodes formed for example by two ends of an open conductor or locally interrupted due to degradation. The appearance of an electric arc is accompanied by a short-term positive or negative voltage front or voltage jump, of the order of a few microseconds, and having a voltage value, called arc voltage Varc, which is characteristic. This arc voltage depends on the material of the electrodes. It is generally between 10V and 30V. If the electrodes are copper for example, the arc voltage Varc is of the order of 12V. As a result, a sudden increase, between 10V and 30V, of a voltage measured in a photovoltaic installation is therefore characteristic of the appearance of an electric arc in the installation. As the plasma of the electric arc acts as a resistance that increases over time, the initial voltage front is followed by a gradual increase in the measured voltage until an open circuit voltage is reached.
    A known solution for detecting an electric arc in a photovoltaic installation is based on the detection of a positive (or negative) voltage edge characterized by a sudden increase (or decrease) in voltage, lasting a few microseconds and a value corresponding to the arc voltage Varc, typically between 10V and 30V. For this purpose, for example, the voltage at the terminals of a photovoltaic module of the installation is measured. The voltage measurement at the terminals of the photovoltaic module makes it possible to detect a possible electric arc located outside this photovoltaic module. However, it does not detect an electric arc that would occur within the photovoltaic module itself. In the case of an installation comprising several photovoltaic modules, it is therefore necessary to measure the voltage across several modules to cover the entire installation. Such a solution requires several measurement sensors and is therefore expensive.
    Another known solution for detecting an electric arc in a photovoltaic installation is based on the measurement of the current in the photovoltaic installation and the white noise introduced by the electric arc into the current signal. Such a solution requires only one current sensor that can be installed anywhere in the photovoltaic system, for example at the input of an inverter interposed between the photovoltaic installation and the electrical network and intended to convert the current. continuous delivered by an alternating current. Such a solution is less expensive and more flexible, but unreliable.
    The present invention improves the situation.
    OBJECT OF THE INVENTION To this end, the invention relates to a method for detecting an electric arc in a photovoltaic installation intended to deliver an electric current, characterized in that it comprises the following steps: • Measurement of values representative of the electric current delivered by the photovoltaic system; • Adjustment of a variable current jump threshold, based on measured values; • Detection of a current jump having an amplitude greater than a current jump threshold adjusted according to values measured before the jump; • Detection of an electric arc on detection of a jump of current.
    The method of detecting an electric arc of the invention is based on a measurement of the electric current produced by the photovoltaic installation, or a representative electrical quantity or image of this electric current. Thanks to this, only one measuring sensor is needed to monitor the entire photovoltaic system. The adjustment of the current jump threshold as a function of the current produced by the installation makes it possible to take into account the amplitude fluctuations of the current jumps caused by electric arcs, which can be due to variations in the level of illumination of the light. the photovoltaic installation and / or an offset of an operating point of a photovoltaic module of the installation relative to its point of maximum power. As a result, the method of the invention is simple, inexpensive to implement, and robust.
    In a particular embodiment, the adjustment of the variable current jump threshold uses a law of variation of the threshold as a function of a nominal current of the photovoltaic installation comprising a phase of increasing the current jump threshold according to said rated current. In this case, the threshold increase phase can be linear.
    Advantageously, the threshold variation law comprises a constant current jump threshold phase for photovoltaic system nominal current values below a low limit between OA and 8A, advantageously between 0.8A and 1.2A, in particular equal to 1 A.
    Advantageously, the threshold variation law comprises a constant current jump threshold phase for current values delivered by the photovoltaic system greater than a high limit.
    In a particular embodiment, for the detection of the current jump, the current jump threshold is adjusted as a function of an average current calculated over a time window of a duration of between 50ps and 500ms preceding the current jump.
    Advantageously, the measured values representative of the current delivered by the photovoltaic installation being sampled, to detect a current jump, a set of 2N successive samples is recorded, N constituting a given depth of detection, and a jump detection algorithm is executed. calculating the difference between the sum of the N oldest samples and the sum of the N most recent samples, and checking whether the calculated difference is greater, in absolute value, than an adjusted current jump threshold.
    Advantageously, the jump detection algorithm is executed for two distinct detection depths N and M, and an electric arc is detected only if it is determined that the differences calculated for the two depths are greater, in absolute value, than the corresponding thresholds. . As a result, low frequency phenomena and high frequency phenomena varying the current are filtered.
    The size N can be adapted to filter dynamic variations of the current of the photovoltaic installation characterized by a characteristic frequency belonging to a frequency band between 1 Hz and 1000 Hz.
    The size M can be adapted to filter dynamic variations of the current of the photovoltaic installation characterized by a characteristic frequency belonging to a frequency band between 100 kHz and 1000 kHz.
    In a particular embodiment, the method comprises a step of detecting a variation in the noise level of a signal of the measured values greater than a critical variation.
    The detection of a variation of the noise level makes it possible to complete the detection of a current jump in order to search for the presence of an electric arc in the installation. In particular, it makes it possible to detect certain particular arcs which do not cause a detectable current jump. Thanks to this, the electric arc detection is even more robust and reliable.
    Advantageously, the measured values being sampled, during the step of detecting a variation of the noise level, the variance of measured values sampled over a sample window sliding in time is calculated.
    Advantageously, the step of detecting a variation of the noise level is repeatedly performed on the same samples by modifying parameters so as to detect different types of specific electric arcs. The invention also relates to a device for detecting an electric arc in a photovoltaic installation intended to deliver an electric current, characterized in that it comprises the following steps: a module for measuring values representative of the electric current delivered by the photovoltaic installation; A module for adjusting a variable current jump threshold, as a function of measured values; A module for detecting a current jump having an amplitude greater than a current jump threshold adjusted according to values measured before the jump.
    Advantageously, the device comprises an analog-digital converter for sampling the measured values representative of the current delivered by the photovoltaic installation, sampled measured value storage means for storing a set of 2N successive samples, N constituting a depth of detection given, and in that the current jump detection module is arranged to execute a jump detection algorithm of calculating the difference between the sum of the oldest N samples and the sum of the most recent N samples, and to verify, if the calculated difference is greater, in absolute value, than an adjusted current jump threshold.
    Advantageously, the device comprises a module for detecting a variation in the noise level of a signal formed by the measured values greater than a critical variation. The invention also relates to a security system for a photovoltaic installation, characterized in that it comprises a device for detecting an electric arc as defined above and an intervention device for putting the photovoltaic installation into operation. safety in case of electric arc. The invention also relates to a photovoltaic installation characterized in that it comprises an electric arc detection device as defined above or a security system as defined above.
    Brief description of the drawings The invention will be better understood with the aid of the following description of a particular embodiment of the method for detecting an electric arc in a photovoltaic installation of the invention and an embodiment particular of a corresponding detection device, with reference to the accompanying drawings in which: - Figure 1 shows a diagram of an example of a photovoltaic installation incorporating the detection device of Figure 6; FIGS. 2A and 2B show two examples of current signals delivered by a photovoltaic installation each comprising a current jump caused by an electric arc; FIG. 3 represents various characteristic curves of current-voltage of a photovoltaic installation, subjected to different irradiances (or illumination powers); FIGS. 4A and 4B show laws or characteristics of variation of a current jump threshold as a function of a nominal current of the photovoltaic installation; FIG. 5 represents a flowchart of the method for detecting an electric arc in a photovoltaic installation according to a particular embodiment of the invention; FIG. 6 represents a functional block diagram of a processing unit of the detection device, adapted to implement processing steps of the method of FIG. 5.
    DETAILED DESCRIPTION OF PARTICULAR EMBODIMENTS OF THE INVENTION The invention aims to detect the presence of an electric arc within the photovoltaic installation 100. It is based on the measurement of the electric current I supplied by the photovoltaic installation 100 or of a representative electrical quantity, or image, of this electric current I. In FIG. 1, there is shown schematically an example of a photovoltaic installation 100. This comprises, in known manner, several connected photovoltaic modules (PV) 1. to an inverter 2. The PV modules 1 are here identical. The inverter 2 is intended to convert the direct current I produced by the photovoltaic modules 2 into an alternating current and to supply it to an electrical network 3.
    The method of the invention seeks to detect the presence or absence of an electric arc within a photovoltaic installation 100. Such an electric arc can occur anywhere in the installation 100, for example between the photovoltaic modules 1 and the inverter 2 (as represented by the electric arc 4 in FIG. 1), or in a photovoltaic module 1, or on a link connecting in series several photovoltaic modules 1 (as represented by the electric arc 14 in Figure 1).
    An electric arc causes a considerable variation of the voltage within the electrical installation 100. At first, the appearance of the electric arc is accompanied by a positive or negative front or voltage jump, of a duration of the order of a few microseconds and an amplitude equal to a characteristic arc voltage Varc. The value of this arc voltage Varc is typically between 10V and 30V. It depends on the electrode material between which the electric arc is formed.
    A photovoltaic module has a current-voltage characteristic of its own. This can be represented in the form of a curve, generally called "l-V curve", comprising a set of operating points of the photovoltaic module. The curve IV connects a short-circuit operating point, for which the voltage is zero and the current is equal to the short circuit current Icc, and an open circuit operating point, for which the current is zero and the voltage is equal to the open circuit voltage Voc- The electrical power delivered by the photovoltaic module is the product of the voltage V at its terminals by the current I it generates. It is maximum at a specific point of the curve defined by a given current lmpp and a given voltage Vmpp. This maximum power point MPP (maximum power point) is located in an inflection zone of the current-voltage curve. The shape of the curve l-V of a photovoltaic module depends on the irradiance received by the module, that is to say the power of light energy received. FIG. 3 shows several curves IV, referenced C1 to C4, of the same photovoltaic module 1 subjected to different levels of illumination or irradiance: the curve C1 corresponds to an average illumination level of 1102 W. / m2; curve C2 corresponds to an average illumination level of 729 W / m2; curve C3 corresponds to an average illumination level of 307 W / m2; curve C4 corresponds to an average illumination level of 64 W / m2.
    On each of the curves C1, C2 and C3, there is shown the maximum power point P1mpp, P2mpp, P3mpp · On the curve C1, there is shown an operating point P1 'shifted (to the left) with respect to the power point maximum P1mpp · Generally, the photovoltaic system is set so that the photovoltaic modules it integrates operate at their maximum power point. However, due for example to a non-uniform illumination level on the various photovoltaic modules of the installation, one or more modules may have an offset operating point, such as the point PT.
    When an electric arc such as the electric arc 4 or 14 (FIG. 1) appears in the photovoltaic system 100, the voltage at the terminals of each photovoltaic module 1 increases suddenly by the arc voltage Varc · This voltage jump, In this case, the positive amplitude amplitude Varc has the effect of moving the operating point of the photovoltaic module on the curve IV towards the right, as shown in FIG. 3, to a new operating point having a voltage equal to V0 +. Varc (where V0 represents the voltage of the photovoltaic module before the arc). The displacement of the operating point of the photovoltaic module is accompanied by a negative jump here (or decrease or fall) of the operating current of the photovoltaic module 1, of an amplitude dlarc · Contrary to the amplitude of the jump of voltage which is fixed and equal to Varc, the amplitude dlarc of the jump of current is variable. It varies according to the position of the operating point on the curve l-V and according to the level of illumination of the photovoltaic module. For example, with reference to the curve C1 of FIG. 3, if the operating point of the PV module 1 is a point P1 'shifted to the left on the curve IV with respect to the point of maximum power P1mpp, the current jump has a very small amplitude. Moreover, the lower the level of illumination, the more the curve l-V flattens and the amplitude dlarc of the current jump decreases, including the point of maximum power.
    FIG. 1 diagrammatically shows a device 5 for detecting an electric arc, according to one particular embodiment of the invention, for the photovoltaic installation 100. The detection device 5 comprises a measurement module 6 intended to measuring the electric current I supplied by the photovoltaic installation 100, or a representative electrical quantity or image of this electric current I. In this case, the measurement module 6 comprises a shunt resistor 7, placed on an electrical connection of the photovoltaic installation 100 (for example at the input of the inverter 2 as shown in FIG. 6), and a voltage measurement sensor 8 intended to measure the voltage across the resistor 7. The current I supplied by the photovoltaic installation 100 is proportional to the voltage U across the resistor 7, according to the equation: / = ^ * U (where R is the value of the resistor 7). The voltage U measured here is therefore the image of the direct current I delivered by the photovoltaic installation 100.
    The measuring sensor 8 is connected by a communication link 9 to a processing unit 10 intended. The purpose of the processing unit 10 is to analyze the data and / or measurement signals transmitted by the measurement sensor 8 in order to detect the presence of a possible electric arc in the photovoltaic installation. Here, it comprises an analog-to-digital converter 20 for digitizing or sampling the voltage signal measured by the sensor 8 in order to obtain measured and sampled voltage values which are representative of the current I of the photovoltaic installation. As a variant, the analog-digital converter could be integrated in the measurement sensor 8. The function of the processing unit 10 is to detect an electric arc by analyzing the values measured by the sensor 8 representative of the electric current I supplied by the photovoltaic installation, by implementing the method of detection of an electric arc which will be described later.
    With reference to FIG. 6, the processing unit 10 comprises the following hardware and / or software components: the analog-digital converter 20; storage memories 21 for storing measured and sampled values and calculated data; a module 22 for adjusting a variable current threshold, as a function of measured values representative of the current I of the photovoltaic installation 100; a module 23 for detecting a current jump having an amplitude greater than a current jump threshold adjusted according to values measured before the jump; a module 24 for detecting a variation in the noise level of a signal formed by the measured values; a control module 25 intended to control the respective operations of the modules 21, 22 and 23 and to determine the presence or absence of an electric arc in the installation 100 as a function of the results provided by the detection module 22 and / or by the detection module 23 - a computing unit 26, in this case a microcontroller, intended to implement data processing and calculations and to control the operation of the processing unit 10.
    The modules 22 to 25 here are software components intended to be executed by the microcontroller 26.
    The hardware and / or software components of the processing unit 10 are adapted to implement the method described below. The processing unit 10 is connected to an intervention device 12 by a communication link 11. The function of the intervention device 12 is to interrupt an electric arc detected by the processing unit 10, on the order of the here, to avoid any risk of deterioration or fire.
    The arcing detection device 5 and the intervention device 12 form a security system for photovoltaic installation.
    A particular embodiment of the method for detecting an electric arc in the photovoltaic installation 100 intended to deliver an electric current I will now be described with reference to FIG.
    The method comprises a step E0 for measuring voltage values across the resistor 7. The measured voltage values are proportional and therefore representative, or images, of the electric current I delivered by the photovoltaic installation 100. In short, the measurement achieved is to measure the current I delivered by the photovoltaic system 100, to a multiplicative factor. Alternatively, the resistor 7 and the voltage measurement sensor 8 could be replaced by a current measurement sensor. The measured signal, representative of the current I, is transmitted to the processing unit 10. The measurement step EO is followed by a sampling step E1, during which the measured signal is sampled with a sampling frequency FeCh chosen. This can be between 50kHz and 1000kHz. Thus, the measured values representative of the current I of the photo voltaic installation 100 are digitized by sampling into data representative of the current I, which will be referred to hereinafter as "current data". Sampling is here carried out by the CAN converter 20 of the processing device 10. Alternatively, in the case of a measurement sensor integrating an analog-digital converter, it could be achieved by the sensor itself. The digitized current data is stored in memories 21. For example, three buffers or "buffers" each having a storage capacity of 256 points or samples are used.
    The method then comprises a step E2 of adjusting a current jump threshold S. The detection of an electric arc according to the invention is based on the detection of a current jump, as shown in FIG. having an amplitude greater than a determined current jump threshold S. This current jump threshold S is variable and must be adjusted over time as a function of the measured values representative of the current I of the photo voltaic installation 100. The threshold S is adjusted according to a variation law of the current jump threshold as a function of the nominal current I n of the installation 100, as represented by way of illustrative example in FIG. 4A. By "nominal" current ln, is meant the current delivered by the photovoltaic system 100 under normal operating conditions (in particular without arcing), each photovoltaic module 1 of the installation 100 operating at an operating point of its curve IV. With reference to FIG. 4A, the variation law of the threshold S comprises here: a first phase with a constant current jump threshold S1 for nominal current values ln of the photovoltaic system 100 below a low limit of between 0A and 8A, advantageously between 0.8A and 1.2A, for example equal to 1A; a second phase with a constant current jump threshold S2 for nominal current values ln of the photovoltaic installation greater than a high limit, here equal to 10A (by way of illustrative example); an intermediate phase of increasing variation, or increase, of the current jump threshold as a function of the nominal current ln, the increase here being linear, for currents between the low limit (here 1A) and the high limit ( here 10A).
    Thus, according to the variation law as represented in FIG. 4A, the current jump threshold S is equal to a first value S1, when the nominal current I n of the photovoltaic installation 100 is less than or equal to the low limit ( here 1A), then increases linearly until reaching a second value S2 when the nominal current ln of the photovoltaic installation 100 is equal to the high limit (here 10A) and finally stagnates at this value S2 when the nominal current ln of the photovoltaic installation 100 is greater than the upper limit (here 10A). In FIG. 4A, the threshold values are expressed in digits. The digitization of the current value gives level data corresponding to a number of digits. The digit therefore represents a current resolution. For example, if a digit represents 0.1 A, 100 digits represent 10A. In the particular embodiment described here, 1A corresponds to 113 digits. In general, 1A could correspond to a number of digits for example between 50 and 400. It would be possible to envisage other forms of variation law of the current jump threshold as a function of the nominal (or operating) current of the photovoltaic installation 100.
    During step E2, in order to determine the adjusted threshold S valid at a given instant t ,, denoted S (t,), the processing module 10 calculates an average value of the current I on an analysis window containing a series of X measured and sampled values, ie a series of X samples, covering a time period slightly earlier than the instant t ,, centered on a moment (ΐ, -τ) where τ represents a time shift. However, the analysis window should not be too far from the instant t ,, and contain a sufficient and reasonable number of samples to take into account possible variations and acquire the information sufficiently quickly. The duration of the window is for example between 10ps and 500ms. It covers a period before the jump. The time offset (τ) must be at least one buffer (256 samples) and advantageously less than 100 buffers. We denote "FA (trx)" this analysis window and "lm0y (ti-x)" the average value of the current I calculated on this analysis window. Thus, the threshold S (t,) that should be applied at time t, is calculated on the basis of an analysis window FA (trx) slightly shifted in time before this time t, and centered on a moment (ΐ, -χ). This slight time shift is adapted so that, in the event of a current jump from the current I at the instant t ,, or substantially at the instant t, the average current value lm0y (ti-x) used for determining the applicable threshold S (t,) corresponds to the average current supplied by the photovoltaic installation 100 just before the jump. The threshold S is thus updated, or adjusted, at each instant t, by a succession of instant t, with i = 1, 2, .... The threshold S (tj) is calculated using the law of predefined variation, as shown in Figure 4A, for a "nominal" current equal to the determined average current value lmoy (trx).
    The method then comprises a step E3 for detecting a current jump. This step is implemented at each instant t, from previously recorded current data. It aims to detect a current drop of an amplitude greater than the current jump threshold adjusted and valid at this time t ,. The detection of a current jump uses a detection algorithm as described below. The jump detection algorithm uses a set of 2N successive samples recorded, in other words 2N sampled values representative of current I. The number "N" constitutes a depth of detection (or analysis or treatment). Let echk be the sample of index k. The algorithm comprises the implementation of the following steps: - calculating the sum of the N most recent echk samples with index k varying from 0 to N-1, and the sum of the N oldest echk samples with index k varying from N to 2N-1 (the N "most recent" echk samples having been measured after the "oldest" N samples), during a first calculation step E30; - then calculate the difference dN between the sum of the N oldest samples of index k varying from N to 2N-1 and the sum of the N most recent samples of index k varying from 0 to N-1, ie dN = ΣΙ ^ ν1 echk - Σ% = ο echk, in a second calculation step E31; - Check if the difference dN calculated is greater, in absolute value, the threshold S (tj) determined for the moment t, (compared with this threshold) during a test step E32.
    In the embodiment described here, the jump detection algorithm is executed for a first detection depth N, by implementing steps E30 to E32, and for a second detection depth M, by implementing steps E'30 to E'32 similar to steps E30 to E32 but with a change in depth. The depth M is strictly greater than the depth N. In the embodiment described here, N is equal to 8 and M is equal to 128. FIG. 4B shows two threshold curves S_N and S_M corresponding to the laws of variation of the threshold expressed in digits as a function of the nominal current ln of the photovoltaic installation 100, respectively applicable for the depth N and for the depth M. At a threshold S (t,) expressed in terms of amperes corresponds to two equivalent thresholds SnIl) and Sm (i) expressed in digits and applicable for depths N and M respectively. The execution of the jump detection algorithm for two distinct N and M detection depths makes it possible to filter low-frequency dynamic variations (for the depth N) and high-frequency dynamic variations (for the depth M) of the current of photovoltaic installation 100. These dynamic variations of the current I are due to events other than electric arcs. For example, it may be a decrease in the current produced by the installation 100 because of a cloud that decreases the illumination received or current variations related to impulse spurious phenomena. The depth N is adapted so as to filter dynamic variations of the current I of the photovoltaic installation 100 characterized by a characteristic frequency belonging to a frequency band of between 1 Hz and 1000 Hz. The depth M is adapted so as to filter dynamic variations of the current I of the photovoltaic installation 100 characterized by a characteristic frequency belonging to a frequency band between 100 kHz and 1000 kHz. More generally, the values of N and M can be chosen within a wide range, between 3 and 1500, to obtain satisfactory results from a sampling frequency of between 50 kHz and 10 MHz.
    During a test step E33, it is determined whether the two comparison steps E32 and E'32 provide positive results, in other words if the differences dN and dM calculated for the two depths N and M are greater than the respective thresholds. If the test E33 is positive, the differences dN and dM calculated for the two depths N and M being both greater than the respective thresholds, the presence of an electric arc is detected in the photovoltaic installation 100 during a step E5. Thus, an electric arc is detected only if the differences calculated for the two depths N and M are greater than the corresponding thresholds. In the case of a negative test, the preceding steps are reiterated at a later time tj + i.
    The method also comprises the execution of an algorithm for detecting a variation ΔΒ of the noise level of the signal measured by the measurement sensor 8, during a step E4, making it possible to detect an increase in the noise level greater than a threshold or critical ABS variation. An electric arc is accompanied by an increase in the noise level of the current signal I of the photovoltaic installation 100, due to the noise generated by the plasma of the electric arc. The algorithm for detecting a variation in the noise level aims to detect this increase in the noise level from the measured values representative of the current I of the photovoltaic installation 100, sampled and recorded in buffers. For this purpose, any known method of signal processing can be used to detect the variation of the noise level of a signal.
    For example, the algorithm for detecting a variation in the noise level may be based on the calculation of the variance of sampled measured values, on a sliding sample window in the sample time, and on the detection of a sample. critical threshold exceeded by this variance.
    In case of detection of a variation of the noise level ΔΒ greater than the critical variation or ABS threshold, during the step E4, an electric arc is detected in the photovoltaic installation and the process proceeds to the step E5.
    In the event of non-detection of a variation of the noise level ΔΒ greater than the critical variation or ABS threshold during the step E4, the method repeats the step E5 for a time-shifted analysis window. The algorithm for detecting a variation of the noise level can be executed several times on the same samples by modifying certain parameters of the algorithm so as to detect different types of specific arcs or to discard a false arc detection. caused by a particular event (for example when starting the photo voltaic installation at rated current at the point of maximum power). The algorithm for detecting a variation of the noise level makes it possible to complete the detection performed by the detection algorithm of a current jump. In particular, in cases where the electric arc does not cause a current jump having a sufficient amplitude to be detected (for example because of a low level of illumination of the photovoltaic system or because of a point operating mode shifted to the left on the curve IV with respect to the point of maximum power), the algorithm for detecting a variation in the noise level nevertheless makes it possible to detect a possible electric arc. The current jump detection algorithm and the noise level variation detection algorithm of a current jump can be executed in parallel. The presence of an electric arc is detected if at least one of the two steps E3 and E4 produces a positive electric arc detection result.
    When an electric arc is detected (step E5), the processing unit 10 transmits a command to secure the photovoltaic installation 100, during a step E6, to the intervention device 12. This security may be based on remotely controlled switches. It can be achieved by an order to interrupt the operation of the photovoltaic system, which stops the electric arc, thereby eliminating any risk of degradation and / or fire. By way of illustrative example, FIGS. 2A and 2B show current signals measured with the presence of an electric arc. In FIG. 2A, the electric arc causes a negative current jump which will be detected by the step E3 of detecting a current jump, in the case of implementation of the previously described detection method. In FIG. 2B, the current returns very quickly to its initial value after the current jump, with an increase in the noise level. In this case, the electric arc will be detected by the step E4 of detecting a variation of the noise level, in case of implementation of the previously described detection method.
    权利要求:
    Claims (19)
    [1" id="c-fr-0001]
    1. A method for detecting an electric arc in a photovoltaic installation (100) intended to deliver an electric current (I), characterized in that it comprises the following steps: • Measurement (E0) of values representative of the electric current ( I) delivered by the photovoltaic system (100); • Adjustment (E2) of a variable current jump threshold (S (ti)), as a function of measured values; • Detection (E3) of a current jump having an amplitude greater than a current jump threshold adjusted according to values measured before the jump; • Detection (E5) of an electric arc on detection of a current jump.
    [2" id="c-fr-0002]
    2. Method according to claim 1, characterized in that the adjustment (E3) of the variable current jump threshold uses a law of variation of the threshold as a function of a nominal current of the photovoltaic installation comprising a phase of increase. the current jump threshold as a function of said nominal current.
    [3" id="c-fr-0003]
    3. Method according to the preceding claim, characterized in that the step of increasing the threshold is linear.
    [4" id="c-fr-0004]
    4. Method according to claim 2 or 3, characterized in that the variation law of the threshold comprises a constant current jump threshold phase for nominal current values photovoltaic installation below a low limit between OA and 8A , advantageously between 0.8A and 1.2A, especially equal to 1 A.
    [5" id="c-fr-0005]
    5. Method according to one of claims 2 to 4, characterized in that the threshold variation law comprises a constant current jump threshold phase for current values delivered by the photovoltaic system greater than a high limit.
    [6" id="c-fr-0006]
    6. Method according to one of the preceding claims, characterized in that, for the detection of the current jump (E3), the current jump threshold is adjusted as a function of an average current calculated over a time window of one duration between 50ps and 500ms preceding the current jump.
    [7" id="c-fr-0007]
    7. Method according to one of the preceding claims, characterized in that the measured values representative of the current delivered by the photovoltaic installation being sampled (E1), to detect a current jump, a set of 2N successive samples is recorded, N constituting a given depth of detection, and performing a jump detection algorithm of calculating (E31) the difference between the sum of the oldest N samples and the sum of the most recent N samples, and checking (E32) if the calculated difference is greater, in absolute value, than an adjusted current jump threshold.
    [8" id="c-fr-0008]
    8. Method according to the preceding claim, characterized in that one executes the jump detection algorithm for two distinct detection depths N and Μ (E31, E32, E'31, E'32), and an arc is detected. only if it is determined that the differences calculated for the two depths are greater, in absolute value, than the corresponding thresholds.
    [9" id="c-fr-0009]
    9. Method according to the preceding claim, characterized in that the size N is adapted to filter dynamic variations of the current of the photovoltaic installation characterized by a characteristic frequency belonging to a frequency band between 1 Hz and 1000Hz.
    [10" id="c-fr-0010]
    10. The method of claim 7 or 8, characterized in that the size M is adapted to filter dynamic variations of the current of the photovoltaic installation characterized by a characteristic frequency belonging to a frequency band between 100kHz and 1000kHz.
    [11" id="c-fr-0011]
    11. Method according to one of the preceding claims, characterized in that it comprises a step (E4) for detecting a variation in the noise level of a signal of the measured values greater than a critical variation.
    [12" id="c-fr-0012]
    12. Method according to the preceding claim, characterized in that, the measured values being sampled, during the step of detecting a variation in the noise level, the variance of sampled measured values is calculated, in particular on a window of slippery samples in time.
    [13" id="c-fr-0013]
    13. Method according to one of claims 10 and 11, characterized in that the step of detecting a variation of the noise level repeatedly on the same samples by modifying parameters so as to detect different types. specific arcs.
    [14" id="c-fr-0014]
    14. A device for detecting an electric arc in a photovoltaic installation (100) intended to deliver an electric current (I), characterized in that it comprises the following steps: a module (6) for measuring values representative of the electric current (I) delivered by the photovoltaic system (100); A module (22) for adjusting a variable current jump threshold (S (t,)), as a function of measured values; A module (23) for detecting a current jump having an amplitude greater than a current jump threshold adjusted according to values measured before the jump.
    [15" id="c-fr-0015]
    15. Device according to the preceding claim, characterized in that it comprises an analog-digital converter for sampling the measured values representative of the current delivered by the photovoltaic installation, means for storing sampled measured values for storing a set of 2N successive samples, N constituting a given depth of detection, and in that the module (23) for detecting a current jump is arranged to execute a jump detection algorithm consisting of calculating the difference between the sum of the N samples the oldest and the sum of the N most recent samples, and to check, if the difference calculated is greater, in absolute value, to a threshold of current jump adjusted.
    [16" id="c-fr-0016]
    16. Device according to one of claims 14 and 15, characterized in that it comprises a detection module of a variation of the noise level of a signal formed by the measured values greater than a critical variation.
    [17" id="c-fr-0017]
    17. Security system for a photovoltaic installation, characterized in that it comprises an arcing detection device according to one of claims 14 to 16 and an intervention device for putting the photovoltaic installation in safety. in case of electric arc.
    [18" id="c-fr-0018]
    18. Photovoltaic installation, characterized in that it comprises an electric arc detection device according to one of claims 14 to 16.
    [19" id="c-fr-0019]
    19. Photovoltaic installation, characterized in that it comprises a security system according to claim 17.
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    同族专利:
    公开号 | 公开日
    WO2017093420A1|2017-06-08|
    EP3384592B1|2020-04-22|
    US10958060B2|2021-03-23|
    EP3384592A1|2018-10-10|
    FR3044487B1|2017-12-22|
    ES2796364T3|2020-11-26|
    US20180358797A1|2018-12-13|
    引用文献:
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    US20120134058A1|2009-08-14|2012-05-31|Fronius International Gmbh|Method for detecting arcs in photovoltaic systems and such a photovoltaic system|
    US20140373894A1|2013-06-25|2014-12-25|Volterra Semiconductor Corporation|Photovoltaic Panels Having Electrical Arc Detection Capability, And Associated Systems And Methods|
    CN104092440A|2014-07-21|2014-10-08|阳光电源股份有限公司|Photovoltaic system direct-current arc fault detection method, device, processor and system|US10778142B2|2015-12-01|2020-09-15|Commissariat A L'energie Atomique Et Aux Energies Alternatives|Method and device for evaluating the energy produced by an electric arc in a photovoltaic installation|
    US10910992B2|2015-12-01|2021-02-02|Commissariat A L'energie Atomique Et Aux Energies Alternatives|Method and device for detecting a stray electric arc in a photovoltaic installation|US10673229B2|2010-11-09|2020-06-02|Solaredge Technologies Ltd.|Arc detection and prevention in a power generation system|
    US9008978B2|2011-06-17|2015-04-14|Sunfield Semiconductor, Inc.|System and method for arc detection in solar power arrays|
    FR2983968B1|2011-12-09|2014-01-10|Commissariat Energie Atomique|METHOD AND DEVICE FOR DETECTING ELECTRIC ARC IN A PHOTOVOLTAIC INSTALLATION|
    US9431816B2|2012-09-28|2016-08-30|Eaton Corporation|Direct current arc fault detector and circuit interrupter, and method of detecting an arc in a direct current power circuit|
    US9025287B2|2012-12-19|2015-05-05|Stmicroelectronics S.R.L.|Arc fault detection equipment and method using low frequency harmonic current analysis|
    FR3002644B1|2013-02-22|2015-03-27|Commissariat Energie Atomique|METHOD AND DEVICE FOR DETECTING ELECTRIC ARC IN A PHOTOVOLTAIC INSTALLATION|
    JP6642075B2|2016-02-10|2020-02-05|オムロン株式会社|Arc handling control device and arc handling control method|JP6561197B2|2016-02-26|2019-08-14|シャープ株式会社|Power supply device using solar cell, electronic device such as communication device including the same, and signboard device|
    IT201700032303A1|2017-03-23|2018-09-23|St Microelectronics Srl|OPERATING PROCEDURE OF PHOTOVOLTAIC GENERATORS, CIRCUIT, DEVICE AND CORRESPONDENT SYSTEM|
    法律状态:
    2016-12-29| PLFP| Fee payment|Year of fee payment: 2 |
    2017-06-02| PLSC| Publication of the preliminary search report|Effective date: 20170602 |
    2018-01-02| PLFP| Fee payment|Year of fee payment: 3 |
    2018-12-31| PLFP| Fee payment|Year of fee payment: 4 |
    2019-12-30| PLFP| Fee payment|Year of fee payment: 5 |
    2020-12-28| PLFP| Fee payment|Year of fee payment: 6 |
    优先权:
    申请号 | 申请日 | 专利标题
    FR1561622A|FR3044487B1|2015-12-01|2015-12-01|METHOD AND DEVICE FOR DETECTING AN ELECTRIC ARC IN A PHOTOVOLTAIC INSTALLATION|FR1561622A| FR3044487B1|2015-12-01|2015-12-01|METHOD AND DEVICE FOR DETECTING AN ELECTRIC ARC IN A PHOTOVOLTAIC INSTALLATION|
    ES16806039T| ES2796364T3|2015-12-01|2016-12-01|Procedure and device for detecting an electric arc in a photovoltaic installation|
    US15/780,113| US10958060B2|2015-12-01|2016-12-01|Method and device for detecting an electric arc in a photovoltaic installation|
    EP16806039.0A| EP3384592B1|2015-12-01|2016-12-01|Method and device for detecting an electric arc in a photovoltaic installation|
    PCT/EP2016/079466| WO2017093420A1|2015-12-01|2016-12-01|Method and device for detecting an electric arc in a photovoltaic installation|
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