CN113114105A - Dynamic measurement method for output characteristics of photovoltaic cell assembly - Google Patents

Dynamic measurement method for output characteristics of photovoltaic cell assembly Download PDF

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CN113114105A
CN113114105A CN202110259265.3A CN202110259265A CN113114105A CN 113114105 A CN113114105 A CN 113114105A CN 202110259265 A CN202110259265 A CN 202110259265A CN 113114105 A CN113114105 A CN 113114105A
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carrier
coordinate system
photovoltaic cell
angular velocity
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CN113114105B (en
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彭乐乐
张亚飞
张慧玲
王天宇
江威
关博
郑树彬
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Shanghai University of Engineering Science
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    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02SGENERATION OF ELECTRIC POWER BY CONVERSION OF INFRARED RADIATION, VISIBLE LIGHT OR ULTRAVIOLET LIGHT, e.g. USING PHOTOVOLTAIC [PV] MODULES
    • H02S50/00Monitoring or testing of PV systems, e.g. load balancing or fault identification
    • H02S50/10Testing of PV devices, e.g. of PV modules or single PV cells
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01CMEASURING DISTANCES, LEVELS OR BEARINGS; SURVEYING; NAVIGATION; GYROSCOPIC INSTRUMENTS; PHOTOGRAMMETRY OR VIDEOGRAMMETRY
    • G01C9/00Measuring inclination, e.g. by clinometers, by levels
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01PMEASURING LINEAR OR ANGULAR SPEED, ACCELERATION, DECELERATION, OR SHOCK; INDICATING PRESENCE, ABSENCE, OR DIRECTION, OF MOVEMENT
    • G01P15/00Measuring acceleration; Measuring deceleration; Measuring shock, i.e. sudden change of acceleration
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01PMEASURING LINEAR OR ANGULAR SPEED, ACCELERATION, DECELERATION, OR SHOCK; INDICATING PRESENCE, ABSENCE, OR DIRECTION, OF MOVEMENT
    • G01P3/00Measuring linear or angular speed; Measuring differences of linear or angular speeds
    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02EREDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E10/00Energy generation through renewable energy sources
    • Y02E10/50Photovoltaic [PV] energy

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Abstract

The invention relates to a dynamic measurement method for output characteristics of a photovoltaic cell module, which is used for acquiring the output voltage or current value of a photovoltaic cell when a carrier fixedly provided with a solar cell panel moves, and comprises the following steps: 1) respectively calibrating a geographic coordinate system and a carrier coordinate system; 2) acquiring acceleration, angular velocity and inclination angle data of a moving carrier in real time; 3) converting the acceleration and angular velocity data from a carrier coordinate system to a geographic coordinate system; 4) fusing acceleration, angular velocity and inclination angle data based on a Kalman filtering fusion algorithm to obtain more accurate carrier motion attitude angle data; 5) and acquiring the illumination intensity received by the solar cell panel according to the carrier motion attitude angle data, and dynamically acquiring the output characteristic of the photovoltaic cell by combining a photovoltaic cell mathematical model and the relation between the environment and the model parameter. Compared with the prior art, the method has the advantages of considering the dynamic environment of the carrier, accurately estimating and the like.

Description

Dynamic measurement method for output characteristics of photovoltaic cell assembly
Technical Field
The invention relates to the technical field of photovoltaic power generation, in particular to a dynamic measurement method for output characteristics of a photovoltaic cell module under the condition of carrier motion.
Background
Solar energy is popular in the world as one of the most potential clean energy sources in the world. The photovoltaic cell is widely applied to various occasions, such as spaceflight, unmanned aerial vehicles, ships, rail vehicles and other motion carriers. However, in recent years, the output characteristics of photovoltaic cells are mostly studied domestically and abroad based on that the photovoltaic module is in a static state, the static output characteristics of the photovoltaic cells are studied by changing external environmental conditions, and the situation in a carrier motion state needs to be considered in order to improve the conversion efficiency of the photovoltaic module to the maximum extent to realize high-power generation.
From the aspect of a measurement method, the existing measurement method for the output characteristic of the photovoltaic module under the motion condition is less researched, the output characteristic of the photovoltaic module is difficult to obtain by adopting a traditional direct measurement method under the action of complex mechanical vibration, and the measurement method relying on a single sensor is easily influenced by low-frequency accumulated errors, so that the measurement precision is low. How to accurately measure the dynamic output characteristics of the photovoltaic module under the condition that the photovoltaic module is subjected to multi-frequency nonlinear vibration becomes a problem of priority in photovoltaic cell characteristic analysis.
Disclosure of Invention
The invention aims to overcome the defects of the prior art and provide a method for dynamically measuring the output characteristic of a photovoltaic cell module.
The purpose of the invention can be realized by the following technical scheme:
a dynamic measurement method for output characteristics of a photovoltaic cell module is used for accurately acquiring output voltage or current values of a photovoltaic cell when a carrier fixedly provided with a solar cell panel moves, and comprises the following steps:
1) respectively calibrating a geographic coordinate system and a carrier coordinate system;
2) acquiring acceleration, angular velocity and inclination angle data of a moving carrier in real time;
3) converting the acceleration and angular velocity data from a carrier coordinate system to a geographic coordinate system;
4) under a unified geographic coordinate system, fusing acceleration, angular velocity and inclination angle data based on a Kalman filtering fusion algorithm to obtain more accurate carrier motion attitude angle data, namely motion attitude angle data of the solar cell panel;
5) and acquiring the illumination intensity received by the solar cell panel according to the carrier motion attitude angle data, and dynamically acquiring the output characteristic of the photovoltaic cell by combining a photovoltaic cell mathematical model and the relation between the environment and the model parameter.
The step 1) specifically comprises the following steps:
11) establishing a geographical coordinate system with its origin at the center of mass of the carrier, ZtAxis pointing from origin to sky along local geographical vertical line, XtAxis perpendicular to ZtIn the plane of the axis and pointing in the direction of the north pole along the local meridian, YtThe shaft always points east along the local latitude line;
12) establishing a carrier coordinate system, wherein the origin of the carrier coordinate system is the same as the origin of the geographic coordinate system and is the carrier centroid, XbThe axial direction being forward along the longitudinal axis of the carrier, YbThe axial direction is along the transverse axis of the carrier to the right, ZbAxis orthogonal to XbAnd YbA shaft.
And 2) acquiring triaxial acceleration data, triaxial angular velocity data and inclination angle data under a carrier coordinate system in real time through an inertia measurement unit arranged on the motion carrier, wherein the inertia measurement unit comprises an accelerometer, a gyroscope and an inclinometer.
The step 3) specifically comprises the following steps:
31) obtaining a rotation matrix based on inertial information and European space rotation theory
Figure BDA0002969290850000021
32) And (4) converting the coordinate system of the triaxial acceleration and the angular velocity data under the carrier coordinate system by adopting an Euler angle method according to the rotation matrix to obtain the triaxial acceleration and the angular velocity data under the geographic coordinate system.
In the step 32), the coordinate conversion formula of the triaxial acceleration and angular velocity data in the geographic coordinate system is as follows:
Figure BDA0002969290850000022
Figure BDA0002969290850000023
Figure BDA0002969290850000024
wherein the content of the first and second substances,
Figure BDA0002969290850000031
respectively, three-axis acceleration under a geographic coordinate system,
Figure BDA0002969290850000032
respectively, three-axis acceleration under a carrier coordinate system,
Figure BDA0002969290850000033
respectively, the three-axis angular velocity under the geographic coordinate system,
Figure BDA0002969290850000034
three-axis angular velocity in a carrier coordinate system, theta,
Figure BDA00029692908500000314
ψ is an angle of rotation about the x, y, z axes, respectively.
The step 4) specifically comprises the following steps:
41) according to the three-axis angular velocity data under the geographic coordinate system
Figure BDA0002969290850000035
Establishing a system state prediction equation;
42) according to triaxial acceleration data under a geographic coordinate system
Figure BDA0002969290850000036
And inclination data
Figure BDA0002969290850000037
Establishing a system observation equation;
43) motion attitude angle is recurrently solved by utilizing five core formulas of Kalman filtering algorithm
Figure BDA0002969290850000038
In the step 41), the expression of the system state prediction equation is as follows:
Figure BDA0002969290850000039
where X (k) is the system state vector at time k,
Figure BDA00029692908500000310
the motion attitude angle of the carrier at the k moment under the geographic coordinate system,
Figure BDA00029692908500000311
three-axis angular velocity data at the moment k-1 in a geographic coordinate system, W (k) is dynamic noise at the moment k in the system, and dk is sampling time.
In the step 42), the expression of the system observation equation is:
Figure BDA00029692908500000312
wherein, z (k) is an observation vector at the time k, and v (k) is observation noise at the time k of the system.
The step 5) specifically comprises the following steps:
51) obtaining the illumination intensity S received by the solar cell panel at the current moment according to the carrier motion attitude angle data, and then:
Figure BDA00029692908500000313
Figure BDA0002969290850000045
wherein (theta)etetet)TIs the included angle between the illumination intensity and the photovoltaic cell panel,
Figure BDA0002969290850000041
is the initial angle of illumination intensity with respect to the three axes of the geographic coordinate system,
Figure BDA0002969290850000042
for carrier motion attitude angle data, S0The illumination intensity irradiated on the plane of the cell panel;
52) obtaining the current I of the photovoltaic cell at the current moment according to the illumination intensityLThen, there are:
Figure BDA0002969290850000043
wherein, ILrFor the photoproduction current, k, of a battery under standard test conditionsiIs the temperature coefficient of current, TrIs a temperature value under standard test conditions, T is a battery temperature, SrThe illumination intensity under the standard condition;
53) and calculating according to the photovoltaic cell five-parameter model to obtain a photovoltaic cell output characteristic curve.
In the step 53), the expression of the photovoltaic cell five-parameter model is as follows:
Figure BDA0002969290850000044
wherein, ILFor photovoltaic cell monomer current, i.e. photo-generated current, IOFor reverse saturation current of the battery, USIs the output voltage of the photovoltaic cell, q is the charge constant, K is the Prziman constant, n is the ideal factor of the diode, RSFor connecting equivalent resistance, R, in series with the batteryPThe equivalent resistance is connected in parallel with the battery, and I is the output current of the photovoltaic battery.
Compared with the prior art, the invention has the following advantages:
the invention considers that under the condition of nonlinear vibration of a carrier, acceleration, angular velocity and inclination angle data of the carrier under the motion condition are acquired in real time through an inertial measurement unit arranged on the motion carrier, and data acquired by three different sensors are fused based on a Kalman filtering fusion algorithm to obtain a more accurate and wider carrier motion attitude angle.
And secondly, on the basis of the existing static photovoltaic cell power generation output model, establishing a dynamic photovoltaic cell output model, and accurately acquiring the output power, the output voltage and the output current of the dynamic photovoltaic cell.
Drawings
FIG. 1 is a flow chart of the method of the present invention.
Fig. 2 is a schematic view of a motion carrier.
Fig. 3 is a diagram of the vibration angle transformation of the photovoltaic cell.
Fig. 4 is a graph of the relationship between the vibration of the photovoltaic cell and the illumination intensity.
Fig. 5 is a train vehicle/track coupling dynamics model.
Fig. 6 is a dynamic output voltage-current (V-I) curve of a photovoltaic cell in motion.
Fig. 7 is a dynamic output voltage-power (V-P) curve of a photovoltaic cell under motion.
Fig. 8 is a dynamic output curve of the maximum power point voltage of the photovoltaic cell under the continuous motion of the carrier.
Fig. 9 is a dynamic output curve of the maximum power point current of the photovoltaic cell under the continuous motion of the carrier.
Fig. 10 is a dynamic output curve of the maximum power point current of the photovoltaic cell under the continuous motion of the carrier.
Detailed Description
Examples
The invention provides a dynamic measurement method for output characteristics of a photovoltaic cell module, which is characterized in that an inertia measurement unit (an accelerometer, a gyroscope and an inclinometer) arranged on a motion carrier (a vehicle body) is utilized to collect acceleration, angular velocity and inclination angle data of the motion carrier in real time, the three data are fused based on a Kalman filtering fusion algorithm to obtain more accurate and wider motion attitude angles of the carrier, and a dynamic photovoltaic cell model is established based on a photovoltaic cell mathematical model to accurately and quickly obtain the output voltage or current value of a dynamic photovoltaic cell.
As shown in fig. 1, the method specifically includes the following steps:
step 1: respectively calibrating a geographic coordinate system and a carrier coordinate system;
step 2: acquiring acceleration, angular velocity and inclination angle data in real time by using an inertial measurement unit (an accelerometer, a gyroscope and an inclinometer) arranged on a motion carrier;
and step 3: performing conversion calculation of acceleration and angular velocity data from a carrier coordinate system to a geographic coordinate system;
and 4, step 4: under a unified geographic coordinate system, fusing acceleration, angular velocity and inclination angle data based on a Kalman filtering fusion algorithm to obtain a more accurate carrier motion attitude angle;
and 5: and establishing a dynamic photovoltaic cell model based on the photovoltaic cell mathematical model to obtain the output voltage or current value of the dynamic photovoltaic cell.
The detailed description of each step is as follows:
step 1: coordinate system calibration, as shown in fig. 2, a geographical coordinate system and a carrier coordinate system are established according to the geographical position of the carrier at the initial moment, the geographical coordinate system (i.e. t system),origin O is the center of mass of the carrier, ZtAxis pointing from origin to sky along local geographical vertical, XtAxis perpendicular to ZtIn the plane of the axis, pointing in the direction of the north pole along the local meridian, YtThe axis always points to the east along the local latitude line, and the direction of the coordinate axis of the geographic coordinate system does not change along with the movement of the carrier.
A carrier coordinate system (namely a b system), the origin is defined as the same as the geographic coordinate system and is the center of mass, X, of the carrierbThe axial direction being forward along the longitudinal axis of the carrier, YbThe axial direction is along the transverse axis of the carrier to the right, ZbAxis orthogonal to XbAnd YbAnd the coordinate axis direction of the carrier coordinate system can change along with the movement of the carrier at any moment.
Step 2, data acquisition: real-time acquisition of three-axis acceleration of a moving carrier by accelerometers, gyroscopes and inclinometers
Figure BDA0002969290850000061
Three-axis angular velocity
Figure BDA0002969290850000062
And the angle of inclination
Figure BDA0002969290850000063
And (4) data.
Step 3, posture conversion: rotation matrix by Euler angle method
Figure BDA0002969290850000064
In the course of the description, it is,
Figure BDA0002969290850000065
the coordinate transformation matrix for expressing the carrier from a b system to a t system comprises:
Figure BDA0002969290850000066
because the data collected by the accelerometer and the gyroscope installed on the carrier are based on the carrier coordinate system, the acceleration and the angular velocity data need to be converted into the initial geographic coordinate system through attitude conversion, and the following steps are included:
Figure BDA0002969290850000067
Figure BDA0002969290850000068
and 4, information fusion: and the Kalman filtering carries out real-time state accurate estimation on the target data through a system state prediction equation and an observation equation.
Setting a state prediction equation and an observation equation of a dynamic system as follows:
X(k)=A(k-1|k)X(k-1)+B(k-1|k)U(k-1)+W(k-1)
Z(k)=H(k)X(k)+V(k)
wherein, X (k) is a system state vector at the time k, A (k-1| k) is a state transition matrix from the time k-1 to the time k, B (k-1| k) is an input system control matrix from the time k-1 to the time k, U (k-1) is a control quantity of the system at the time k-1, Z (k) is an observation vector at the time k, H (k) is a measurement matrix at the time k, W (k) is dynamic noise at the time k, and V (k) is observation noise at the time k.
For convenience of processing, it is assumed that there is no control quantity input in the system, and the dynamic noise w (k) and the observation noise v (k) are both zero, and they are independent from each other, and the specific flow of kalman filtering is:
pre-estimating:
Figure BDA0002969290850000069
calculating a pre-estimation covariance matrix: p (k | k-1) ═ a (k-1| k) P (k-1| k-1) aT(k-1|k)+Q
Calculating a Kalman gain matrix: k (k) ═ p (k) HT(k)[H(k)P(k)HT(k)+R]-1
Updating estimation:
Figure BDA0002969290850000071
and (3) covariance updating: p (k) ═ I-k (k) h (k) ] P (k | k-1)
(1) The state prediction equation of the system is as follows:
Figure BDA0002969290850000072
wherein θ (k),
Figure BDA0002969290850000073
Psi (k) is the motion attitude angle of the carrier at the k moment under the geographic coordinate system,
Figure BDA0002969290850000074
for the angular velocity data at time k-1, W (k) is the dynamic noise at time k of the system.
(2) The system's observation equation is:
Figure BDA0002969290850000075
where V (k) is the observed noise at time k of the system.
After a state prediction equation and an observation equation of the system are constructed, the fused carrier motion attitude angle can be recursively solved by five core formulas of Kalman filtering.
Step 5, photovoltaic cell dynamic modeling, which specifically comprises the following steps:
(1) obtaining the illumination intensity S received by the solar panel at the current moment according to the carrier motion attitude angle data, as shown in fig. 3 and 4, there are:
Figure BDA0002969290850000076
Figure BDA0002969290850000077
wherein (theta)etetet)TIs the included angle between the illumination intensity and the photovoltaic cell panel,
Figure BDA0002969290850000078
is the initial angle of illumination intensity with respect to the three axes of the geographic coordinate system,
Figure BDA0002969290850000079
for carrier motion attitude angle data, S0The illumination intensity irradiated on the plane of the cell panel;
(2) in the embodiment, the photovoltaic cell dynamic modeling adopts a photovoltaic cell five-parameter model, and the expression is as follows:
Figure BDA0002969290850000081
in the formula ILIs the monomer current of the solar cell, also called photo-generated current, A; i isOIs the reverse saturation current of the battery, A; u shapeSIs the output voltage of the solar cell, V; q is a charge constant, 1.6 × 10-19C; k is Primuman constant, K is 1.38 × 10-23J/K; n is the ideal factor of the diode; t is the battery temperature, K; rSThe equivalent resistance, omega, is the series connection of the battery; rpThe battery is connected with an equivalent resistor omega in parallel; i is the photovoltaic cell output current, A.
The relationship among the five parameters of the photovoltaic cell, the illumination intensity and the temperature is as follows:
Figure BDA0002969290850000082
Figure BDA0002969290850000083
Figure BDA0002969290850000084
Figure BDA0002969290850000085
n=nr
in the formula ILrThe cell generates a current under standard test conditions (T25 ℃, S1000W/m 2), a; ki-temperature coefficient of current; t-cell temperature, deg.C; tr-temperature value under standard test conditions, 25 ℃; s-illumination intensity, W/m 2; sr-light intensity in standard case, 1000W/m 2; ior-diode reverse saturation current under standard test conditions, A; EG-semiconductor forbidden band broadband in photovoltaic cells, typical value of EG under standard test conditions is 1.12 eV; b is equal to about 0.217.
Simulation example
According to the invention, a photovoltaic cell dynamic simulation model is built under a Simulink platform, and the output voltage or current value of the dynamic photovoltaic cell is obtained.
(1) SIMPACK vehicle body modeling
In order to obtain an acceleration value and an angular velocity value under the condition of train vibration, a train vehicle/track coupling dynamic model is established by using a multi-body dynamic software SIMPACK, as shown in figure 5, the model totally comprises 1 train body, 2 frameworks, 4 wheel pairs and 7 rigid bodies, and the rigid bodies are considered to be symmetrical from the front to the back and from the left to the right of the center of mass in the model. The vehicle body is connected with the framework through a secondary suspension spring damping device, and the framework is connected with the wheel pair through a primary suspension spring damping device.
Adding a German orbit spectrum into the model as model excitation, and carrying out simulation to obtain the acceleration gx、gy、gzAngular velocity wx、wy、wz
(2) Matlab photovoltaic cell dynamic model simulation
A photovoltaic cell dynamic simulation model is built on a Matlab/Simulink platform, a photovoltaic cell module with the model of MSX-60 is selected as a simulation object, and data obtained by simulation of a SIMPACK model is input into the photovoltaic cell dynamic simulation model after complementary filtering processing.
(3) Analysis of results
Fig. 6 is a dynamic output voltage-current (V-I) curve of the photovoltaic cell in a motion state, and fig. 7 is a dynamic output voltage-power (V-P) curve of the photovoltaic cell in a motion state. It can be seen from fig. 6 and 7 that both graph output curves conform to the photovoltaic cell output characteristics, and that over time, the V-I, V-P curve is changing, i.e. it is illustrated that carrier motion has an effect on the photovoltaic cell output characteristics.
Fig. 8 shows the photovoltaic cell maximum power point voltage dynamic output curve under the continuous movement of the carrier. Fig. 8 shows that the output voltage of the maximum power output point of the photovoltaic cell is continuously changed under the condition that the carrier is continuously changed, and the change is obvious.
Fig. 9 shows the maximum power point current dynamic output curve of the photovoltaic cell under the continuous motion of the carrier. Fig. 9 shows that the output current of the maximum power output point of the photovoltaic cell is continuously changed under the condition that the carrier is continuously changed, and the change is obvious.
Fig. 10 shows the maximum power point current dynamic output curve of the photovoltaic cell under the continuous motion of the carrier. Fig. 10 shows that the output current of the maximum power output point of the photovoltaic cell is continuously changed under the condition that the carrier is continuously changed, and the change is obvious.
It is finally necessary to point out here: the above description is only a preferred embodiment of the present invention and should not be taken as limiting the invention, and any modifications, equivalents and improvements made within the spirit and principle of the present invention should be included in the scope of the present invention.

Claims (10)

1. A dynamic measurement method for output characteristics of a photovoltaic cell module is used for accurately acquiring output voltage or current values of a photovoltaic cell of a carrier fixedly provided with a solar cell panel under the condition of motion, and is characterized by comprising the following steps:
1) respectively calibrating a geographic coordinate system and a carrier coordinate system;
2) acquiring acceleration, angular velocity and inclination angle data of a moving carrier in real time;
3) converting the acceleration and angular velocity data from a carrier coordinate system to a geographic coordinate system;
4) under a unified geographic coordinate system, fusing acceleration, angular velocity and inclination angle data based on a Kalman filtering fusion algorithm to obtain more accurate carrier motion attitude angle data, namely motion attitude angle data of the solar cell panel;
5) and acquiring the illumination intensity received by the solar cell panel according to the carrier motion attitude angle data, and dynamically acquiring the output characteristic of the photovoltaic cell by combining a photovoltaic cell mathematical model and the relation between the environment and the model parameter.
2. The method according to claim 1, wherein the step 1) specifically comprises the following steps:
11) establishing a geographical coordinate system with its origin at the center of mass of the carrier, ZtAxis pointing from origin to sky along local geographical vertical line, XtAxis perpendicular to ZtIn the plane of the axis and pointing in the direction of the north pole along the local meridian, YtThe shaft always points east along the local latitude line;
12) establishing a carrier coordinate system, wherein the origin of the carrier coordinate system is the same as the origin of the geographic coordinate system and is the carrier centroid, XbThe axial direction being forward along the longitudinal axis of the carrier, YbThe axial direction is along the transverse axis of the carrier to the right, ZbAxis orthogonal to XbAnd YbA shaft.
3. The method as claimed in claim 1, wherein in step 2), the three-axis acceleration data, the three-axis angular velocity data and the tilt angle data in the carrier coordinate system are collected in real time by an inertial measurement unit mounted on the moving carrier, wherein the inertial measurement unit comprises an accelerometer, a gyroscope and a tilt angle meter.
4. The method according to claim 1, wherein the step 3) specifically comprises the following steps:
31) based on inertiaObtaining a rotation matrix by using the sexual information and European space rotation theory
Figure FDA0002969290840000011
32) And (4) converting the coordinate system of the triaxial acceleration and the angular velocity data under the carrier coordinate system by adopting an Euler angle method according to the rotation matrix to obtain the triaxial acceleration and the angular velocity data under the geographic coordinate system.
5. The method as claimed in claim 4, wherein in the step 32), the coordinate transformation formula of the triaxial acceleration and angular velocity data in the geographic coordinate system is:
Figure FDA0002969290840000021
Figure FDA0002969290840000022
Figure FDA0002969290840000023
wherein the content of the first and second substances,
Figure FDA0002969290840000024
respectively, three-axis acceleration under a geographic coordinate system,
Figure FDA0002969290840000025
respectively, three-axis acceleration under a carrier coordinate system,
Figure FDA0002969290840000026
respectively, the three-axis angular velocity under the geographic coordinate system,
Figure FDA0002969290840000027
three-axis angular velocity in a carrier coordinate system, theta,
Figure FDA0002969290840000028
ψ is an angle of rotation about the x, y, z axes, respectively.
6. The method for dynamically measuring the output characteristic of the photovoltaic cell module according to claim 1, wherein the step 4) specifically comprises the following steps:
41) according to the three-axis angular velocity data under the geographic coordinate system
Figure FDA0002969290840000029
Establishing a system state prediction equation;
42) according to triaxial acceleration data under a geographic coordinate system
Figure FDA00029692908400000210
And inclination data
Figure FDA00029692908400000211
Establishing a system observation equation;
43) motion attitude angle is recurrently solved by utilizing five core formulas of Kalman filtering algorithm
Figure FDA00029692908400000212
7. The method according to claim 6, wherein in step 41), the expression of the system state prediction equation is:
Figure FDA00029692908400000213
where X (k) is the system state vector at time k,
Figure FDA00029692908400000214
the motion attitude angle of the carrier at the k moment under the geographic coordinate system,
Figure FDA0002969290840000031
three-axis angular velocity data at the moment k-1 in a geographic coordinate system, W (k) is dynamic noise at the moment k in the system, and dk is sampling time.
8. The method according to claim 7, wherein in step 42), the expression of the system observation equation is:
Figure FDA0002969290840000032
wherein, z (k) is an observation vector at the time k, and v (k) is observation noise at the time k of the system.
9. The method according to claim 1, wherein the step 5) specifically comprises the following steps:
51) obtaining the illumination intensity S received by the solar cell panel at the current moment according to the carrier motion attitude angle data, and then:
Figure FDA0002969290840000033
Figure FDA0002969290840000034
wherein (theta)etetet)TIs the included angle between the illumination intensity and the photovoltaic cell panel,
Figure FDA0002969290840000035
is the initial angle of illumination intensity with respect to the three axes of the geographic coordinate system,
Figure FDA0002969290840000036
for carrier motion attitude angle data, S0The illumination intensity irradiated on the plane of the cell panel;
52) obtaining the current I of the photovoltaic cell at the current moment according to the illumination intensityLThen, there are:
Figure FDA0002969290840000037
wherein, ILrFor the photoproduction current, k, of a battery under standard test conditionsiIs the temperature coefficient of current, TrIs a temperature value under standard test conditions, T is a battery temperature, SrThe illumination intensity under the standard condition;
53) and calculating according to the photovoltaic cell five-parameter model to obtain a photovoltaic cell output characteristic curve.
10. The method according to claim 9, wherein in step 53), the expression of the photovoltaic cell five-parameter model is:
Figure FDA0002969290840000041
wherein, ILFor photovoltaic cell monomer current, i.e. photo-generated current, IOFor reverse saturation current of the battery, USIs the output voltage of the photovoltaic cell, q is the charge constant, K is the Prziman constant, n is the ideal factor of the diode, RSFor connecting equivalent resistance, R, in series with the batteryPThe equivalent resistance is connected in parallel with the battery, and I is the output current of the photovoltaic battery.
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Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN115268442A (en) * 2022-07-27 2022-11-01 湖州丽天智能科技有限公司 Automatic deviation rectifying method and system for photovoltaic cleaning robot and cleaning robot

Citations (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20120152313A1 (en) * 2010-12-17 2012-06-21 Greenvolts, Inc Various tracking algorithms and apparatus for a two axis tracker assembly in a concentrated photovoltaic system
CN105300379A (en) * 2015-10-13 2016-02-03 上海新纪元机器人有限公司 Kalman filtering attitude estimation method and system based on acceleration
CN106655444A (en) * 2015-10-28 2017-05-10 华为终端(东莞)有限公司 Electronic equipment and charging method thereof
CN107478223A (en) * 2016-06-08 2017-12-15 南京理工大学 A kind of human body attitude calculation method based on quaternary number and Kalman filtering
CN108225308A (en) * 2017-11-23 2018-06-29 东南大学 A kind of attitude algorithm method of the expanded Kalman filtration algorithm based on quaternary number
CN109873610A (en) * 2019-03-19 2019-06-11 福州大学 Diagnosing failure of photovoltaic array method based on IV characteristic and depth residual error network
CN109933929A (en) * 2019-03-20 2019-06-25 重庆大学 Equivalent series resistance calculation method
CN110702116A (en) * 2019-10-08 2020-01-17 沈阳航空航天大学 Unit sun vector solving method and measuring device based on photocell array current
CN111207773A (en) * 2020-01-16 2020-05-29 大连理工大学 Attitude unconstrained optimization solving method for bionic polarized light navigation

Patent Citations (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20120152313A1 (en) * 2010-12-17 2012-06-21 Greenvolts, Inc Various tracking algorithms and apparatus for a two axis tracker assembly in a concentrated photovoltaic system
CN105300379A (en) * 2015-10-13 2016-02-03 上海新纪元机器人有限公司 Kalman filtering attitude estimation method and system based on acceleration
CN106655444A (en) * 2015-10-28 2017-05-10 华为终端(东莞)有限公司 Electronic equipment and charging method thereof
CN107478223A (en) * 2016-06-08 2017-12-15 南京理工大学 A kind of human body attitude calculation method based on quaternary number and Kalman filtering
CN108225308A (en) * 2017-11-23 2018-06-29 东南大学 A kind of attitude algorithm method of the expanded Kalman filtration algorithm based on quaternary number
CN109873610A (en) * 2019-03-19 2019-06-11 福州大学 Diagnosing failure of photovoltaic array method based on IV characteristic and depth residual error network
CN109933929A (en) * 2019-03-20 2019-06-25 重庆大学 Equivalent series resistance calculation method
CN110702116A (en) * 2019-10-08 2020-01-17 沈阳航空航天大学 Unit sun vector solving method and measuring device based on photocell array current
CN111207773A (en) * 2020-01-16 2020-05-29 大连理工大学 Attitude unconstrained optimization solving method for bionic polarized light navigation

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
杨莹 等: "NWP卡尔曼滤波光伏功率的预测模型", 《黑龙江科技大学学报》 *

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN115268442A (en) * 2022-07-27 2022-11-01 湖州丽天智能科技有限公司 Automatic deviation rectifying method and system for photovoltaic cleaning robot and cleaning robot

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