CN111651909A - Performance optimization method for photovoltaic/thermal heat collector based on thermodynamic model - Google Patents

Performance optimization method for photovoltaic/thermal heat collector based on thermodynamic model Download PDF

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CN111651909A
CN111651909A CN202010734703.2A CN202010734703A CN111651909A CN 111651909 A CN111651909 A CN 111651909A CN 202010734703 A CN202010734703 A CN 202010734703A CN 111651909 A CN111651909 A CN 111651909A
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photovoltaic
thermal
layer
collector
heat
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杨琦
童水光
童哲铭
宣婷
唐宁
何俊楠
陈皓
陆成
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Hangzhou Boiler Group Co Ltd
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Abstract

A performance optimization method for a photovoltaic/thermal collector comprises the following steps: s1: collecting parameters of a photovoltaic/thermal collector; s2: inputting the parameters into a photovoltaic/thermal collector thermodynamic model in software; s3: calculating thermal, electrical and comprehensive properties of the photovoltaic/thermal collector from the thermodynamic model of the photovoltaic/thermal collector; s4: changing the parameters in the step S1 in MATLAB software, and correspondingly calculating the thermal property, the electrical property and the comprehensive property of the photovoltaic/thermal heat collector; s5: and the MATLAB software generates a waveform diagram according to the parameter change and the corresponding calculation result in the step S4, optimizes the waveform diagram and outputs an optimization result. The invention provides a method for optimizing the performance of a photovoltaic/thermal heat collector based on a thermodynamic model, which can improve the electrical efficiency of the photovoltaic/thermal heat collector, thereby improving the performance of supplying power to a boiler, adapting to the analysis of the heat collector under different working conditions and complex environmental conditions, and improving the analysis efficiency and the economy.

Description

Performance optimization method for photovoltaic/thermal heat collector based on thermodynamic model
Technical Field
The invention belongs to the field of solar energy application technology optimization, and particularly relates to a method for optimizing the performance of a photovoltaic/thermal heat collector based on a thermodynamic model.
Background
A Solar photovoltaic/thermal (PV/T) comprehensive utilization system is a Solar high-efficiency utilization technology capable of simultaneously obtaining high-grade electric energy and heat energy. The system combines photovoltaic and light heat together, and the photovoltaic part utilizes solar energy to produce the electric energy, and the light heat part is collected with the energy that photovoltaic cell is difficult to the conversion with the heat energy form, provides heat energy when promoting photovoltaic cell generating efficiency. The heat collector is a core component for realizing the comprehensive utilization of photovoltaic/heat by the PV/T system, and the performance of the heat collector determines the photovoltaic and photothermal utilization effects of the PV/T system. Therefore, the performance optimization method of the photovoltaic/thermal collector is designed, and the method has important significance for improving the high efficiency and the economical efficiency of the PV/T comprehensive utilization system.
Through the detection of the prior art, less research is found on the performance optimization of the phase-change material photovoltaic/thermal heat collector for supplying power to the boiler. The optimization of the collector has the following defects: (1) most researches only analyze single influence factors, and for a heat collector system working in a complex environment and under various working conditions, the analysis difficulty and cost are increased; (2) the operation performance of the heat collector is influenced by multi-factor interaction, a comprehensive and reasonable optimization result is difficult to obtain by a single-factor analysis mode, and finally the operation economy and safety of a heat collector system are reduced.
Disclosure of Invention
In order to solve the problems, the invention provides a method for optimizing the performance of a photovoltaic/thermal heat collector based on a thermodynamic model, which can improve the electrical efficiency of the photovoltaic/thermal heat collector, thereby improving the performance of supplying power to a boiler, adapting to the analysis of the heat collector under different working conditions and complex environmental conditions, and improving the analysis efficiency and the economy.
The technical scheme of the invention is as follows:
a method for constructing a thermodynamic model of a photovoltaic/thermal heat collector comprises the following steps:
s1: establishing a thermodynamic model by using simulation software;
s2: dividing the thermodynamic model into eight layers;
s3: an energy balance equation formula established in each layer of the thermodynamic model;
s4: and completing the construction of a thermodynamic model of the photovoltaic/thermal heat collector.
Preferably, the simulation software is MATLAB software.
Preferably, the layered structure of the thermodynamic model sequentially comprises a glass layer, a first EVA layer, a battery piece, a second EVA layer, a back plate layer, a PCM layer, an air layer and a heat insulation layer from top to bottom.
Preferably, the energy balance equation of each layer of the thermodynamic model is as follows:
glass layer:
Figure 684185DEST_PATH_IMAGE001
a first EVA layer:
Figure 539009DEST_PATH_IMAGE002
battery piece:
Figure 318746DEST_PATH_IMAGE003
a second EVA layer:
Figure 651638DEST_PATH_IMAGE004
a back plate layer:
Figure 902229DEST_PATH_IMAGE005
a PCM layer:
Figure 724691DEST_PATH_IMAGE006
air layer:
Figure 929408DEST_PATH_IMAGE007
insulating layer:
Figure 3674DEST_PATH_IMAGE008
wherein,
Figure 672553DEST_PATH_IMAGE009
the solar irradiation amount is the amount of solar irradiation,
Figure 102135DEST_PATH_IMAGE010
is the surface area of the heat collector,
Figure 856464DEST_PATH_IMAGE011
Figure 593476DEST_PATH_IMAGE012
Figure 54544DEST_PATH_IMAGE013
Figure 484389DEST_PATH_IMAGE014
respectively the absorptivity of the glass layer, the first EVA layer, the battery piece and the back plate layer,
Figure 663697DEST_PATH_IMAGE015
Figure 938821DEST_PATH_IMAGE016
Figure 582292DEST_PATH_IMAGE017
respectively the transmissivity of the glass layer, the second EVA layer and the cell sheet,
Figure 917458DEST_PATH_IMAGE018
the heat exchange quantity of convection between the glass layer and the environment,
Figure 584063DEST_PATH_IMAGE019
the heat exchange quantity between the glass layer and the environmental radiation,
Figure 662877DEST_PATH_IMAGE020
the radiation heat exchange quantity between the glass layer and the ground,
Figure 160855DEST_PATH_IMAGE021
the glass layer and the first EVA layer conduct heat,
Figure 368720DEST_PATH_IMAGE022
the first EVA layer and the cell sheet conduct heat,
Figure 319358DEST_PATH_IMAGE023
is the electric energy output by the photovoltaic cell,
Figure 139547DEST_PATH_IMAGE024
the heat conduction between the battery plate and the second EVA layer,
Figure 492031DEST_PATH_IMAGE025
the second EVA layer conducts heat with the backsheet layer,
Figure 434579DEST_PATH_IMAGE026
in order to obtain the packing factor of the photovoltaic panel,
Figure 810197DEST_PATH_IMAGE027
is the thermal conductivity of the back plate layer and the PCM layer,
Figure 230814DEST_PATH_IMAGE028
for the accumulated heat absorption of the PCM layer,
Figure 703383DEST_PATH_IMAGE029
is the heat absorption of the PCM layer per unit time,
Figure 754516DEST_PATH_IMAGE030
for the convective heat transfer of the PCM layer with air,
Figure 679747DEST_PATH_IMAGE031
in order to collect the heat from the air,
Figure 904055DEST_PATH_IMAGE032
the convection heat exchange quantity of the air and the heat-insulating layer is adopted,
Figure 401770DEST_PATH_IMAGE033
the heat exchange quantity of the heat preservation layer and the environment is convection. The parameters are partially generated in the iterative process of the energy balance equation, and the other part is a fixed value.
The invention also provides a performance optimization method of the photovoltaic/thermal heat collector, which is based on the thermodynamic model of the photovoltaic/thermal heat collector and is characterized by comprising the following steps:
s1: collecting parameters of the photovoltaic/thermal collector steps;
s2: inputting the parameters into a photovoltaic/thermal collector thermodynamic model in simulation software;
s3: calculating thermal, electrical and comprehensive properties of the photovoltaic/thermal collector from the thermodynamic model of the photovoltaic/thermal collector;
s4: changing the parameters in the step S1 in simulation software, and correspondingly calculating the thermal performance, the electrical performance and the comprehensive performance of the photovoltaic/thermal heat collector;
s5: and the MATLAB software generates a waveform diagram according to the parameter change and the corresponding calculation result in the step S4, optimizes the waveform diagram and outputs an optimization result.
Preferably, the parameters in step S1 specifically include a collector structure parameter, a photovoltaic panel parameter, a physical property parameter of the shape-stabilized phase change material, and an environmental parameter.
Preferably, the structural parameters of the heat collector comprise the length of a photovoltaic panel, the width of the photovoltaic panel, an encapsulation coefficient, the height of a flow channel and air flow, the parameters of the photovoltaic panel comprise the thickness, the heat conductivity coefficient, the transmissivity, the absorptivity and the emissivity of each layer, the physical parameters of the shape-stabilized phase-change material comprise phase-change temperature, phase-change latent heat, specific heat capacity, density and heat conductivity, and the environmental parameters comprise ambient temperature, irradiance and wind speed;
the structural parameters of the heat collector, the parameters of the photovoltaic panel and the physical parameters of the shape-stabilized phase-change material are extracted from a photovoltaic/thermal heat collector system database, and the environmental parameters are acquired through a real-time data server.
Preferably, the calculation of the heat, electricity and comprehensive performance of the photovoltaic/thermal collector in the step S3 is divided into a fixed weather condition calculation and a variable weather condition, and when the photovoltaic/thermal collector is in the fixed weather condition, all layers except the phase change layer are regarded as a stable state; when the device is in a weather-changing condition, the changes of all the layers except the PCM layer are regarded as quasi-static processes;
the thermal property, the electrical property and the comprehensive property of the photovoltaic/thermal heat collector are calculated by calculating the thermal efficiency of the heat collector
Figure 686121DEST_PATH_IMAGE034
Electric efficiency
Figure 98647DEST_PATH_IMAGE035
exergy efficiency
Figure 126646DEST_PATH_IMAGE036
Is determined by the calculation of (a);
the heat collector thermal efficiency calculation formula is as follows:
Figure 245912DEST_PATH_IMAGE037
the calculation formula of the electrical efficiency is as follows:
Figure 435585DEST_PATH_IMAGE038
the calculation formula of the exergy efficiency is as follows:
Figure 335408DEST_PATH_IMAGE039
wherein,
Figure 839201DEST_PATH_IMAGE040
Figure 140870DEST_PATH_IMAGE041
wherein,
Figure 501444DEST_PATH_IMAGE042
as the flow rate of the air is,
Figure 888563DEST_PATH_IMAGE043
is the specific heat capacity of the air,
Figure 196048DEST_PATH_IMAGE044
is the temperature of the air outlet, and,
Figure 86643DEST_PATH_IMAGE045
in order to be the air inlet temperature,
Figure 883698DEST_PATH_IMAGE046
in order to improve the photoelectric conversion efficiency of the cell,
Figure 928752DEST_PATH_IMAGE047
in the form of a heat quantity exergy,
Figure 102244DEST_PATH_IMAGE048
in the form of an electrical power exergy,
Figure 112926DEST_PATH_IMAGE049
is the heat absorption of the PCM layer per unit time,
Figure 18565DEST_PATH_IMAGE050
in the form of a unit of time,
Figure 114697DEST_PATH_IMAGE009
the solar irradiation amount is the amount of solar irradiation,
Figure 826301DEST_PATH_IMAGE010
is the surface area of the heat collector,
Figure 629172DEST_PATH_IMAGE026
in order to obtain the packing factor of the photovoltaic panel,
Figure 768029DEST_PATH_IMAGE015
Figure 351457DEST_PATH_IMAGE016
Figure 538856DEST_PATH_IMAGE017
the transmissivity of the glass layer, the transmissivity of the second EVA layer and the transmissivity of the cell sheet are respectively.
Preferably, the optimization process in step S4 specifically includes optimization of the PCM layer and optimization of the air flow rate, and the parameters changed during the optimization of the PCM layer are PCM layer thickness, phase change temperature, and PCM thermal conductivity.
Preferably, the PCM layer optimization specifically adopts a three-factor three-level orthogonal experimental design, and L93 is selected4Orthogonal table, the average exergy efficiency is used as the index to obtain the optimized result.
The invention has the beneficial effects that:
1. according to the invention, the influence of the PCM layer and the air flow on the heat efficiency, the electric efficiency and the comprehensive efficiency of the photovoltaic/thermal heat collector can be obtained, the optimal result is obtained, the design and the arrangement of the photovoltaic/thermal heat collector are guided, the electric efficiency of the photovoltaic/thermal heat collector is improved, and therefore, the performance of supplying power to a boiler is improved; the effect of relieving the air temperature in office buildings or residential buildings is enhanced, so that the body feeling comfort level is improved;
2. the invention can obtain the influence mode of each factor on the performance of the photovoltaic/thermal heat collector when the weather condition is stable and the weather condition changes, and is suitable for the analysis of the heat collector under different working conditions and complex environmental conditions;
3. the invention designs an orthogonal test for three factors of the thickness, the phase-change temperature and the heat conductivity coefficient of the PCM layer, reduces the interference of the interaction of the three factors on performance analysis, and improves the analysis efficiency and the economy.
Drawings
Fig. 1 is an energy transfer model of a photovoltaic/thermal collector of the present invention.
Fig. 2 is a sectional structural view of a photovoltaic/thermal collector of the present invention.
Fig. 3 is a method for optimizing the performance of a photovoltaic/thermal collector for supplying power to a boiler according to the present invention.
Description of reference numerals: 101. a glass layer; 102. a first EVA layer; 103. a battery piece; 104. a second EVA layer; 105. a backsheet layer; 106. a PCM layer; 107. an air layer; 108. and (7) an insulating layer.
Detailed Description
The embodiments of the present invention will be described in detail below with reference to the accompanying drawings.
A method for constructing a thermodynamic model of a photovoltaic/thermal collector, as shown in fig. 1 and 2, comprises the following steps:
1. the thermodynamic model was established using MATLAB software.
2. The thermodynamic model is divided into eight layers, namely a glass layer, a first EVA layer, a battery piece, a second EVA layer, a back plate layer, a PCM layer, an air layer and a heat insulation layer from top to bottom in sequence. In FIG. 1
Figure 524130DEST_PATH_IMAGE051
Is the convection heat transfer quantity between the glass layer and the environment,
Figure 833888DEST_PATH_IMAGE052
the glass layer and the first EVA layer conduct heat,
Figure 340831DEST_PATH_IMAGE053
the heat conduction between the battery plate and the second EVA layer,
Figure 394237DEST_PATH_IMAGE054
is the thermal conductivity of the back plate layer and the PCM layer,
Figure 234017DEST_PATH_IMAGE055
the heat transfer quantity of the heat preservation layer and the environment is convection,
Figure 652360DEST_PATH_IMAGE056
is the amount of heat absorbed by the air layer,
Figure 944801DEST_PATH_IMAGE057
is the glass layer and the amount of sky radiation,
Figure 801899DEST_PATH_IMAGE058
the first EVA layer and the cell sheet conduct heat,
Figure 496185DEST_PATH_IMAGE059
the second EVA layer conducts heat with the backsheet layer,
Figure 85430DEST_PATH_IMAGE060
the heat quantity is convected between the heat-insulating layer and the air layer,
Figure 130746DEST_PATH_IMAGE061
g is the solar radiation, the heat absorption of the PCM layer.
3. The energy balance equation formula established in each layer of the thermodynamic model is as follows:
glass layer:
Figure 463639DEST_PATH_IMAGE001
a first EVA layer:
Figure 12432DEST_PATH_IMAGE002
battery piece:
Figure 100473DEST_PATH_IMAGE003
a second EVA layer:
Figure 803725DEST_PATH_IMAGE004
a back plate layer:
Figure 2625DEST_PATH_IMAGE005
a PCM layer:
Figure 405924DEST_PATH_IMAGE006
air layer:
Figure 664868DEST_PATH_IMAGE007
insulating layer:
Figure 356880DEST_PATH_IMAGE008
wherein,
Figure 93892DEST_PATH_IMAGE009
the solar irradiation amount is the amount of solar irradiation,
Figure 617277DEST_PATH_IMAGE010
is the surface area of the heat collector,
Figure 984805DEST_PATH_IMAGE011
Figure 960851DEST_PATH_IMAGE012
Figure 501554DEST_PATH_IMAGE013
Figure 145024DEST_PATH_IMAGE014
respectively the absorptivity of the glass layer, the first EVA layer, the battery piece and the back plate layer,
Figure 417874DEST_PATH_IMAGE015
Figure 146796DEST_PATH_IMAGE016
Figure 225610DEST_PATH_IMAGE017
respectively the transmissivity of the glass layer, the second EVA layer and the cell sheet,
Figure 159806DEST_PATH_IMAGE018
the heat exchange quantity of convection between the glass layer and the environment,
Figure 665873DEST_PATH_IMAGE019
the heat exchange quantity between the glass layer and the environmental radiation,
Figure 882091DEST_PATH_IMAGE020
the radiation heat exchange quantity between the glass layer and the ground,
Figure 702280DEST_PATH_IMAGE021
the glass layer and the first EVA layer conduct heat,
Figure 54763DEST_PATH_IMAGE022
the first EVA layer and the cell sheet conduct heat,
Figure 997312DEST_PATH_IMAGE023
is the electric energy output by the photovoltaic cell,
Figure 435246DEST_PATH_IMAGE024
the heat conduction between the battery plate and the second EVA layer,
Figure 793546DEST_PATH_IMAGE025
the second EVA layer conducts heat with the backsheet layer,
Figure 266116DEST_PATH_IMAGE026
in order to obtain the packing factor of the photovoltaic panel,
Figure 113986DEST_PATH_IMAGE027
is the thermal conductivity of the back plate layer and the PCM layer,
Figure 976900DEST_PATH_IMAGE028
for the accumulated heat absorption of the PCM layer,
Figure 201208DEST_PATH_IMAGE029
is the heat absorption of the PCM layer per unit time,
Figure 528284DEST_PATH_IMAGE030
for the convective heat transfer of the PCM layer with air,
Figure 812635DEST_PATH_IMAGE031
in order to collect the heat from the air,
Figure 661380DEST_PATH_IMAGE032
the convection heat exchange quantity of the air and the heat-insulating layer is adopted,
Figure 423800DEST_PATH_IMAGE033
the heat exchange quantity of the heat preservation layer and the environment is convection. The parameters are partially generated in the iterative process of the energy balance equation, and the other part is a fixed value.
4. And completing the construction of a thermodynamic model of the photovoltaic/thermal heat collector.
The photovoltaic/thermal collector thermodynamic model is established based on the following assumptions:
(1) the total solar irradiance is direct solar irradiance, scattered irradiance is ignored, and reflection and scattering of solar irradiation in the heat collector are ignored;
(2) the transverse heat transfer of each layer in the heat collector is neglected, and the longitudinal temperature distribution of each layer is considered to be uniform;
(3) neglecting the heat capacity of each layer (except the phase change layer) in the heat collector, each layer does not absorb heat;
(4) neglecting convection and radiation between the side surface of the heat-insulating layer and the outside and radiation between the bottom of the heat-insulating layer and the environment;
the wind speed and the thermal physical property and optical performance of each layer of material (except the phase change layer) are kept unchanged.
As shown in fig. 3, a method for optimizing the performance of a photovoltaic/thermal collector based on a thermodynamic model of the photovoltaic/thermal collector includes the following steps:
1. and (6) collecting parameters.
The parameters related to parameter acquisition comprise collector structure parameters, photovoltaic panel parameters, shape-stabilized phase-change material physical property parameters and environment parameters, wherein the collector structure parameters comprise photovoltaic panel length, photovoltaic panel width, packaging coefficient, runner height and air flow, the photovoltaic panel parameters comprise thickness of each layer, heat conductivity coefficient, transmissivity, absorptivity and emissivity, the shape-stabilized phase-change material physical property parameters comprise phase-change temperature, phase-change latent heat, specific heat capacity, density and heat conductivity coefficient, and the environment parameters comprise environment temperature, irradiance and wind speed. The solar collector system comprises a photovoltaic/thermal collector system database, a real-time data server, a heat collector, a photovoltaic panel, a shaping phase change material and a shaping phase change material, wherein the structural parameters of the heat collector, the parameters of the photovoltaic panel and the physical parameters of the shaping phase change material are extracted from the photovoltaic/thermal collector system database, and the environmental parameters are obtained through the real-.
2. And calculating the heat, electricity and comprehensive performance of the photovoltaic/thermal heat collector.
The calculation of the heat, electricity and comprehensive performance of the photovoltaic/thermal heat collector is divided into the calculation of a fixed weather condition and the calculation of a variable weather condition. When weather conditions are determined, all layers except the phase change layer are regarded as stable states; when weather conditions change, the changes of all the layers except the PCM layer are regarded as quasi-static processes.
The calculation of the heat, electricity and comprehensive performance of the photovoltaic/thermal heat collector comprises the calculation of the thermal efficiency of the heat collector
Figure 605382DEST_PATH_IMAGE034
Electric efficiency
Figure 998318DEST_PATH_IMAGE035
exergy efficiency
Figure 898140DEST_PATH_IMAGE036
The calculation formulas are respectively as follows;
Figure 464251DEST_PATH_IMAGE037
Figure 500340DEST_PATH_IMAGE038
Figure 64177DEST_PATH_IMAGE039
wherein,
Figure 451296DEST_PATH_IMAGE040
Figure 555518DEST_PATH_IMAGE041
wherein,
Figure 649376DEST_PATH_IMAGE042
as the flow rate of the air is,
Figure 446431DEST_PATH_IMAGE043
is the specific heat capacity of the air,
Figure 55266DEST_PATH_IMAGE044
is the temperature of the air outlet, and,
Figure 228759DEST_PATH_IMAGE045
in order to be the air inlet temperature,
Figure 675658DEST_PATH_IMAGE046
in order to improve the photoelectric conversion efficiency of the cell,
Figure 643614DEST_PATH_IMAGE047
in the form of a heat quantity exergy,
Figure 739746DEST_PATH_IMAGE048
in the form of an electrical power exergy,
Figure 185771DEST_PATH_IMAGE049
is the heat absorption of the PCM layer per unit time,
Figure 254221DEST_PATH_IMAGE050
in the form of a unit of time,
Figure 393079DEST_PATH_IMAGE009
the solar irradiation amount is the amount of solar irradiation,
Figure 976507DEST_PATH_IMAGE010
is the surface area of the heat collector,
Figure 163906DEST_PATH_IMAGE026
in order to obtain the packing factor of the photovoltaic panel,
Figure 149179DEST_PATH_IMAGE015
Figure 458938DEST_PATH_IMAGE016
Figure 529662DEST_PATH_IMAGE017
the transmissivity of the glass layer, the transmissivity of the second EVA layer and the transmissivity of the cell sheet are respectively.
The air specific heat capacity can be obtained by looking up a table according to the air inlet temperature at that time, the air outlet temperature and the air inlet temperature can be obtained by measuring according to a temperature measuring instrument, the photoelectric conversion efficiency of the cell can be classified into parameters of the photovoltaic panel, and the calculation of the heat absorption capacity of the PCM layer in unit time is generated in the iterative calculation process of an energy balance equation.
3. And the performance of the photovoltaic/thermal heat collector is optimized.
Optimization of photovoltaic/thermal collector performance includes optimization of PCM layer, optimization of air flow rate includes optimization of PCM layer thickness, optimization of phase transition temperature, optimization of PCM thermal conductivity. The optimization mode adopts three-factor three-level orthogonal experimental design and selects L934Orthogonal table, three factors are PCM layer thickness, phase transition temperature and thermal conductivity coefficient respectively, and the test index is average exergy efficiency.
The optimization method is that the electric and thermal comprehensive performance results are optimized by changing the values of the thickness of the PCM layer, the phase change temperature, the heat conductivity coefficient and the air flow in the thermodynamic model and giving the variation range of the parameters, and the optimized results are finally output.
The photovoltaic/thermal collector applied in this embodiment is a flat plate type air solar photovoltaic/thermal collector, and the structure thereof sequentially includes a polysilicon encapsulation photovoltaic plate, a Phase Change Material (PCM) layer, a groove type air flow channel, and an insulating layer from top to bottom.
In the embodiment of the invention, the composite shape-stabilized phase change material prepared from paraffin, high-density polyethylene and expanded graphite is selected, and the content of the expanded graphite can be adjusted according to actual conditions. Heat conductivity coefficient of composite shape-stabilized phase-change material
Figure 520752DEST_PATH_IMAGE062
The calculation formula of (2) is as follows:
Figure 360532DEST_PATH_IMAGE063
wherein,
Figure 841192DEST_PATH_IMAGE064
the thermal conductivity of the phase-change material when the expanded graphite is not added,
Figure 569851DEST_PATH_IMAGE065
in order to obtain the content of the expanded graphite,
Figure 426949DEST_PATH_IMAGE066
is the thermal conductivity of graphite.
Finally, it should be noted that: the above-mentioned embodiments are only specific embodiments of the present invention, which are used for illustrating the technical solutions of the present invention and not for limiting the same, and the protection scope of the present invention is not limited thereto, although the present invention is described in detail with reference to the foregoing embodiments, those skilled in the art should understand that: any person skilled in the art can modify or easily conceive the technical solutions described in the foregoing embodiments or equivalent substitutes for some technical features within the technical scope of the present disclosure; such modifications, changes or substitutions do not depart from the spirit and scope of the present invention in its spirit and scope. Are intended to be covered by the scope of the present invention. Therefore, the protection scope of the present invention shall be subject to the protection scope of the claims.

Claims (10)

1. A method for constructing a thermodynamic model of a photovoltaic/thermal heat collector is characterized by comprising the following steps:
s1: establishing a thermodynamic model;
s2: dividing the thermodynamic model into eight layers;
s3: establishing an energy balance equation formula in each layer of the thermodynamic model;
s4: and completing the construction of a thermodynamic model of the photovoltaic/thermal heat collector.
2. The method for constructing a thermodynamic model of a photovoltaic/thermal collector according to claim 1, wherein the thermodynamic model is constructed by MATLAB.
3. The method for constructing the thermodynamic model of the photovoltaic/thermal collector according to claim 1, wherein the thermodynamic model has a layered structure comprising, from top to bottom, a glass layer, a first EVA layer, a cell sheet, a second EVA layer, a back sheet layer, a PCM layer, an air layer, and an insulating layer.
4. The method for constructing a thermodynamic model of a photovoltaic/thermal collector according to claim 3, wherein the equation of the energy balance of each layer of the thermodynamic model is as follows:
glass layer:
Figure 518749DEST_PATH_IMAGE001
a first EVA layer:
Figure 435890DEST_PATH_IMAGE002
battery piece:
Figure 215627DEST_PATH_IMAGE003
a second EVA layer:
Figure 610836DEST_PATH_IMAGE004
a back plate layer:
Figure 362892DEST_PATH_IMAGE005
a PCM layer:
Figure 185354DEST_PATH_IMAGE006
air layer:
Figure 452387DEST_PATH_IMAGE007
insulating layer:
Figure 87506DEST_PATH_IMAGE008
5. a method for optimizing the performance of a photovoltaic/thermal collector based on the thermodynamic model of the photovoltaic/thermal collector of claim 3, comprising the steps of:
s1: collecting parameters of a photovoltaic/thermal collector;
s2: inputting the parameters into a photovoltaic/thermal collector thermodynamic model in simulation software;
s3: calculating thermal, electrical and comprehensive properties of the photovoltaic/thermal collector from the thermodynamic model of the photovoltaic/thermal collector;
s4: changing the parameters in the step S1 in MATLAB software, and correspondingly calculating the thermal property, the electrical property and the comprehensive property of the photovoltaic/thermal heat collector;
s5: and the MATLAB software generates a waveform diagram according to the parameter change and the corresponding calculation result in the step S4, optimizes the waveform diagram and outputs an optimization result.
6. The method for optimizing the performance of a photovoltaic/thermal collector according to claim 5, wherein the parameters in the step S1 specifically include collector structure parameters, photovoltaic panel parameters, physical parameters of the shaped phase change material, and environmental parameters.
7. The method for optimizing the performance of a photovoltaic/thermal collector according to claim 6, wherein the collector structural parameters include photovoltaic panel length, photovoltaic panel width, packing factor, runner height, and air flow rate, the photovoltaic panel parameters include layer thickness, thermal conductivity, transmittance, absorptance, emissivity, the shape phase change material physical parameters include phase change temperature, phase change latent heat, specific heat capacity, density, thermal conductivity, and the environmental parameters include ambient temperature, irradiance, and wind speed;
the structural parameters of the heat collector, the parameters of the photovoltaic panel and the physical parameters of the shape-stabilized phase-change material are extracted from a photovoltaic/thermal heat collector system database, and the environmental parameters are acquired through a real-time data server.
8. The method for optimizing the performance of the photovoltaic/thermal collector according to claim 7, wherein the calculation of the thermal, electrical and comprehensive performance of the photovoltaic/thermal collector in the step S3 is divided into a constant weather condition calculation and a variable weather condition calculation, and when the photovoltaic/thermal collector is in the constant weather condition, all layers except the phase change layer are regarded as a steady state; when the device is in a weather-changing condition, the changes of all the layers except the PCM layer are regarded as quasi-static processes;
the thermal property, the electrical property and the comprehensive property of the photovoltaic/thermal heat collector are calculated by calculating the thermal efficiency of the heat collector
Figure 756385DEST_PATH_IMAGE009
Electric efficiency
Figure 749748DEST_PATH_IMAGE010
exergy efficiency
Figure 441761DEST_PATH_IMAGE011
Is determined by the calculation of (a);
the heat collector thermal efficiency calculation formula is as follows:
Figure 178773DEST_PATH_IMAGE012
the calculation formula of the electrical efficiency is as follows:
Figure 702158DEST_PATH_IMAGE013
the calculation formula of the exergy efficiency is as follows:
Figure 69685DEST_PATH_IMAGE014
wherein,
Figure 311311DEST_PATH_IMAGE015
Figure 586434DEST_PATH_IMAGE016
wherein,
Figure 167588DEST_PATH_IMAGE017
as the flow rate of the air is,
Figure 502755DEST_PATH_IMAGE018
is the specific heat capacity of the air,
Figure 667895DEST_PATH_IMAGE019
is the temperature of the air outlet, and,
Figure 746709DEST_PATH_IMAGE020
in order to be the air inlet temperature,
Figure 244687DEST_PATH_IMAGE021
in order to improve the photoelectric conversion efficiency of the cell,
Figure 16333DEST_PATH_IMAGE022
in the form of a heat quantity exergy,
Figure 904655DEST_PATH_IMAGE023
in the form of an electrical power exergy,
Figure 787160DEST_PATH_IMAGE024
is the heat absorption of the PCM layer per unit time,
Figure 139644DEST_PATH_IMAGE025
is a unit time.
9. The method for optimizing the performance of a photovoltaic/thermal collector according to claim 8, wherein the optimization process in step S4 includes optimization of PCM layer and optimization of air flow, and the parameters changed during the optimization of PCM layer are PCM layer thickness, phase transition temperature, PCM thermal conductivity.
10. The method for optimizing the performance of a photovoltaic/thermal collector according to claim 9, wherein the PCM layer optimization specifically employs a three-factor three-level orthogonal experimental design, selecting L934Orthogonal table, the average exergy efficiency is used as the index to obtain the optimized result.
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