CN112688637A - Method and system for determining inclined plane irradiance of photovoltaic panel - Google Patents

Method and system for determining inclined plane irradiance of photovoltaic panel Download PDF

Info

Publication number
CN112688637A
CN112688637A CN201910992211.0A CN201910992211A CN112688637A CN 112688637 A CN112688637 A CN 112688637A CN 201910992211 A CN201910992211 A CN 201910992211A CN 112688637 A CN112688637 A CN 112688637A
Authority
CN
China
Prior art keywords
photovoltaic panel
irradiance
determining
time
scattering
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
CN201910992211.0A
Other languages
Chinese (zh)
Inventor
姜文玲
王勃
冯双磊
王伟胜
刘纯
赵艳青
王铮
裴岩
车建峰
张菲
汪步惟
王钊
胡菊
靳双龙
宋宗朋
王姝
滑申冰
刘晓琳
张周祥
林毅
项康利
陈国伟
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
State Grid Corp of China SGCC
China Electric Power Research Institute Co Ltd CEPRI
State Grid Fujian Electric Power Co Ltd
Economic and Technological Research Institute of State Grid Fujian Electric Power Co Ltd
Original Assignee
State Grid Corp of China SGCC
China Electric Power Research Institute Co Ltd CEPRI
State Grid Fujian Electric Power Co Ltd
Economic and Technological Research Institute of State Grid Fujian Electric Power Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by State Grid Corp of China SGCC, China Electric Power Research Institute Co Ltd CEPRI, State Grid Fujian Electric Power Co Ltd, Economic and Technological Research Institute of State Grid Fujian Electric Power Co Ltd filed Critical State Grid Corp of China SGCC
Priority to CN201910992211.0A priority Critical patent/CN112688637A/en
Publication of CN112688637A publication Critical patent/CN112688637A/en
Pending legal-status Critical Current

Links

Images

Classifications

    • 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
    • Y02E10/52PV systems with concentrators

Landscapes

  • Photovoltaic Devices (AREA)

Abstract

The invention relates to a method and a system for determining the inclined plane irradiance of a photovoltaic panel, which comprises the following steps: determining the molecular scattering irradiance of the inclined plane of the photovoltaic panel according to the horizontal plane scattering irradiance of the photovoltaic panel under the clearance condition; respectively determining the direct inclined plane irradiance and the scattered inclined plane irradiance of the photovoltaic panel according to the total horizontal plane irradiance of the photovoltaic panel; and determining the inclined plane irradiance of the photovoltaic panel according to the inclined plane direct irradiance, the inclined plane molecular scattering irradiance and the inclined plane meter scattering irradiance of the photovoltaic panel. The technical scheme provided by the invention has the advantages of simple calculation, high precision and wide application range.

Description

Method and system for determining inclined plane irradiance of photovoltaic panel
Technical Field
The invention relates to the technical field of photovoltaic power generation, in particular to a method and a system for determining inclined plane irradiance of a photovoltaic panel.
Background
The most important influence factor of the photovoltaic output is solar irradiance, and generally, the larger the irradiance received by the photovoltaic panel is, the larger the photovoltaic output is. Since the amount of irradiance received by the plane of the photovoltaic panel is related to the angle of incidence of the sun, the irradiance on the horizontal plane and the inclined plane are not equal and often differ significantly.
In order to obtain as much solar radiation energy as possible, the photovoltaic panels are generally mounted with an inclination with the panel facing towards the equator. Irradiance data common in engineering is the total irradiance in the horizontal plane, which needs to be converted into bevel irradiance, a work called irradiance bevel conversion.
In irradiance ramp conversion, for diffuse radiation, conventional methods typically set the solar radiation to be isotropic and convert from horizontal plane irradiance of the photovoltaic panel to ramp irradiance on that basis.
However, researchers find that the scattered radiation mainly comprises molecular scattering and rice scattering, wherein the molecular scattering is typically isotropic, and the rice scattering is mainly forward scattering, that is, the scattering angle is less than 90 °, so that the traditional method has inaccurate setting of the solar radiation, and the calculation result has large errors.
Disclosure of Invention
Aiming at the defects of the prior art, the invention aims to provide the method for determining the inclined plane irradiance of the photovoltaic panel, which is simple in calculation, high in precision and wide in application range.
The purpose of the invention is realized by adopting the following technical scheme:
the invention provides a method for determining the inclined plane irradiance of a photovoltaic panel, which is improved in that the method comprises the following steps:
determining the molecular scattering irradiance of the inclined plane of the photovoltaic panel according to the horizontal plane scattering irradiance of the photovoltaic panel under the clearance condition;
respectively determining the direct inclined plane irradiance and the scattered inclined plane irradiance of the photovoltaic panel according to the total horizontal plane irradiance of the photovoltaic panel;
and determining the inclined plane irradiance of the photovoltaic panel according to the inclined plane direct irradiance, the inclined plane molecular scattering irradiance and the inclined plane meter scattering irradiance of the photovoltaic panel.
Preferably, the determining the photovoltaic panel oblique plane molecular scattering irradiance according to the horizontal plane scattering irradiance of the photovoltaic panel under the headroom condition comprises:
determining the scattering irradiance S 'of the bevel molecules of the photovoltaic panel at the moment t according to the formula'r,d(t):
Figure BDA0002238618570000021
In the formula, Sr,d(t) the horizontal plane molecule scattering irradiance of the photovoltaic panel at the moment t, and beta is the plate surface inclination angle of the photovoltaic panel;
wherein the horizontal plane molecule scattering irradiance S of the photovoltaic panel at the time t is determined according to the following formular,d(t):
Sr,d(t)=Sd,c(t)
In the formula, Sd,cAnd (t) is the horizontal plane scattering irradiance of the photovoltaic panel at the moment t under the clearance condition.
Further, before determining the photovoltaic panel oblique molecule scattering irradiance according to the horizontal plane scattering irradiance of the photovoltaic panel under the headroom condition, the method further comprises:
determining horizontal plane scattering irradiance S of the photovoltaic panel at the t moment under clearance condition according to the following formulad,c(t):
Sd,c(t)=So(t)·τd(t)·cosθ(t)
In the formula, So(t) solar irradiance, τ, in a plane perpendicular to sunlight at the upper atmospheric boundary at time td(t) is the scattering transparency coefficient at the moment t, and theta (t) is the solar zenith angle at the moment t;
wherein S iso(t) is determined as follows:
Figure BDA0002238618570000022
in the formula (I), the compound is shown in the specification,
Figure BDA0002238618570000023
is the sun constant, doD (t) is the average distance of the day and the ground, and d (t) is the distance of the day and the ground at the time t;
τd(t) is determined as follows:
τd(t)=0.271-0.294·τb(t)
in the formula, τb(t) is the direct transparency coefficient at time t;
τb(t) is determined as follows:
Figure BDA0002238618570000024
in the formula, Mh(t) is the relative large air volume at the location of the photovoltaic panel at the time t;
Mh(t) is determined as follows:
Figure BDA0002238618570000031
in the formula, h is the altitude of the photovoltaic panel;
θ (t) is determined as follows:
Figure BDA0002238618570000032
in which ω (t) is the sun at time tThe time angle is set according to the time of day,
Figure BDA0002238618570000033
and delta (t) is the solar declination angle at the position of the photovoltaic panel at the moment t.
Preferably, the determining of the direct inclined plane irradiance and the diffuse inclined plane meter irradiance of the photovoltaic panel according to the horizontal plane total irradiance of the photovoltaic panel comprises:
determining the scattering ratio of the photovoltaic panel at the location according to the horizontal plane total irradiance of the photovoltaic panel;
determining horizontal plane scattering irradiance and horizontal plane direct irradiance of the photovoltaic panel according to the scattering ratio of the photovoltaic panel;
determining the inclined surface meter scattered irradiance of the photovoltaic panel according to the horizontal surface scattered irradiance of the photovoltaic panel;
and determining the direct inclined plane irradiance of the photovoltaic panel according to the direct horizontal plane irradiance of the photovoltaic panel.
Further, the step of determining the scattering ratio of the photovoltaic panel at the location according to the horizontal plane total irradiance of the photovoltaic panel comprises:
and determining the scattering ratio DF of the photovoltaic panel at the position of the t moment according to the following formula:
Figure BDA0002238618570000034
in the formula, kTThe clearance index of the place where the photovoltaic panel is located at the moment t.
Wherein, the clearance index k of the photovoltaic panel at the t moment is determined according to the following formulaT
Figure BDA0002238618570000035
Wherein S (t) is the total horizontal irradiance of the photovoltaic panel at the time t, SoAnd (t) is the solar irradiance on the plane vertical to the sunlight on the upper air boundary at the time t, and theta (t) is the solar zenith angle at the time t.
Further, the determining of the horizontal plane scattering irradiance and the horizontal plane direct irradiance of the photovoltaic panel according to the scattering ratio of the photovoltaic panel at the location comprises:
determining horizontal plane scattering irradiance S of photovoltaic panel at time t according to the following formulad(t):
Sd(t)=S(t)·DF
Determining horizontal plane direct irradiance S of photovoltaic panel at time t according to the following formulab(t):
Sb(t)=S(t)-Sd(t)
Wherein S (t) is the horizontal plane total irradiance of the photovoltaic panel at the time t, and DF is the scattering ratio of the photovoltaic panel at the time t.
Further, the determining the oblique meter scattering irradiance of the photovoltaic panel according to the horizontal plane scattering irradiance of the photovoltaic panel comprises:
determining the horizontal surface meter scattered irradiance of the photovoltaic panel according to the horizontal surface scattered irradiance of the photovoltaic panel by the following formula:
Sm,d(t)=Sd(t)-Sr,d(t);
determining the oblique surface meter scattering irradiance of the photovoltaic panel according to the horizontal surface meter scattering irradiance of the photovoltaic panel by the following formula:
Figure BDA0002238618570000041
in the formula, Sm,d(t) horizontal surface meter scattered irradiance of the photovoltaic panel at time t, Sd(t) horizontal plane scattered irradiance, S, of the photovoltaic panel at time tr,d(t) is the horizontal plane molecule scattering irradiance, S 'of the photovoltaic panel at time t'm,dAnd (t) is the scattering irradiance of the slope meter of the photovoltaic panel at the moment t, r is the false direct incidence ratio of the location of the photovoltaic panel, theta' (t) is the slope solar incident angle of the photovoltaic panel at the moment t, and theta (t) is the solar zenith angle at the moment t.
Further, the slope solar incident angle θ' (t) of the photovoltaic panel at time t is determined as follows:
θ′(t)=arccos[cosθ(t)×cosβ+sinθ(t)×sinβ×cos(α(t)-ε)]
the solar azimuth angle α (t) at time t is determined as follows:
Figure BDA0002238618570000042
wherein beta is the inclination angle of the surface of the photovoltaic panel, epsilon is the orientation angle of the surface of the photovoltaic panel (when the surface of the photovoltaic panel faces the south, the orientation angle is 180 degrees), alpha (t) is the azimuth angle of the sun at the moment t,
Figure BDA0002238618570000043
and delta (t) is the solar declination angle at the position of the photovoltaic panel at the moment t.
Further, the determining the direct inclined plane irradiance of the photovoltaic panel according to the direct horizontal plane irradiance of the photovoltaic panel includes:
determining the direct bevel irradiance S 'of the photovoltaic panel at the moment t according to the formula'b(t):
Figure BDA0002238618570000051
In the formula, theta' (t) is the inclined plane solar incident angle of the photovoltaic panel at the time t, theta (t) is the solar zenith angle at the time t, SbAnd (t) is the horizontal plane direct irradiance of the photovoltaic panel at the time t.
Preferably, the determining the inclined plane irradiance of the photovoltaic panel according to the inclined plane direct irradiance, the inclined plane molecular scattering irradiance and the inclined plane meter scattering irradiance of the photovoltaic panel includes:
determining the bevel irradiance S' (t) of the photovoltaic panel at the time t according to the following formula:
S′(t)=S′b(t)+S′m,d(t)+S′r,d(t)
of formula (II) S'b(t) is the direct bevel irradiance, S 'of the photovoltaic panel at time t'm,d(t) is the bevel meter scattered irradiance, S 'of the photovoltaic panel at the moment t'r,dAnd (t) is the oblique plane molecular scattering irradiance of the photovoltaic panel at the time t.
The present invention provides a system for determining bevel irradiance of a photovoltaic panel, the improvement comprising:
the first determination module is used for determining the molecular scattering irradiance of the inclined plane of the photovoltaic panel according to the horizontal plane scattering irradiance of the photovoltaic panel under the clearance condition;
the second determining module is used for respectively determining the inclined plane direct irradiance and the inclined plane meter scattering irradiance of the photovoltaic panel according to the horizontal plane total irradiance of the photovoltaic panel;
and the third determining module is used for determining the inclined plane irradiance of the photovoltaic panel according to the inclined plane direct irradiance, the inclined plane molecular scattering irradiance and the inclined plane meter scattering irradiance of the photovoltaic panel.
Preferably, the first determining module includes:
determining the scattering irradiance S 'of the bevel molecules of the photovoltaic panel at the moment t according to the formula'r,d(t):
Figure BDA0002238618570000052
In the formula, Sr,d(t) the horizontal plane molecule scattering irradiance of the photovoltaic panel at the moment t, and beta is the plate surface inclination angle of the photovoltaic panel;
wherein the horizontal plane molecule scattering irradiance S of the photovoltaic panel at the time t is determined according to the following formular,d(t):
Sr,d(t)=Sd,c(t)
In the formula, Sd,cAnd (t) is the horizontal plane scattering irradiance of the photovoltaic panel at the moment t under the clearance condition.
Further, before the first determining module, the method further includes:
determining horizontal plane scattering irradiance S of the photovoltaic panel at the t moment under clearance condition according to the following formulad,c(t):
Sd,c(t)=So(t)·τd(t)·cosθ(t)
In the formula, So(t) solar irradiance, τ, in a plane perpendicular to sunlight at the upper atmospheric boundary at time td(t) is the scattering transparency coefficient at the moment t, and theta (t) is the solar zenith angle at the moment t;
wherein S iso(t) is determined as follows:
Figure BDA0002238618570000061
in the formula (I), the compound is shown in the specification,
Figure BDA0002238618570000062
is the sun constant, doD (t) is the average distance of the day and the ground, and d (t) is the distance of the day and the ground at the time t;
τd(t) is determined as follows:
τd(t)=0.271-0.294·τb(t)
in the formula, τb(t) is the direct transparency coefficient at time t;
τb(t) is determined as follows:
Figure BDA0002238618570000063
in the formula, Mh(t) is the relative large air volume at the location of the photovoltaic panel at the time t;
Mh(t) is determined as follows:
Figure BDA0002238618570000064
in the formula, h is the altitude of the photovoltaic panel;
θ (t) is determined as follows:
Figure BDA0002238618570000065
in the formula, ω (t) is the time angle of the sun at time t,
Figure BDA0002238618570000066
and delta (t) is the solar declination angle at the position of the photovoltaic panel at the moment t.
Preferably, according to the second determination module, the method includes:
the first determining unit is used for determining the scattering ratio of the photovoltaic panel at the position according to the horizontal plane total irradiance of the photovoltaic panel;
the second determining unit is used for determining the horizontal plane scattering irradiance and the horizontal plane direct irradiance of the photovoltaic panel according to the scattering ratio of the photovoltaic panel;
the third determining unit is used for determining the inclined surface meter scattered irradiance of the photovoltaic panel according to the horizontal surface scattered irradiance of the photovoltaic panel;
and the fourth determining unit is used for determining the inclined plane direct irradiance of the photovoltaic panel according to the horizontal plane direct irradiance of the photovoltaic panel.
Further, the first determining unit is configured to:
and determining the scattering ratio DF of the photovoltaic panel at the position of the t moment according to the following formula:
Figure BDA0002238618570000071
in the formula, kTThe clearance index of the place where the photovoltaic panel is located at the moment t.
Wherein, the clearance index k of the photovoltaic panel at the t moment is determined according to the following formulaT
Figure BDA0002238618570000072
Wherein S (t) is the total horizontal irradiance of the photovoltaic panel at the time t, SoAnd (t) is the solar irradiance on the plane vertical to the sunlight on the upper air boundary at the time t, and theta (t) is the solar zenith angle at the time t.
Further, the second determining unit is configured to:
determining horizontal plane scattering irradiance S of photovoltaic panel at time t according to the following formulad(t):
Sd(t)=S(t)·DF
Determining horizontal plane direct irradiance S of photovoltaic panel at time t according to the following formulab(t):
Sb(t)=S(t)-Sd(t)
Wherein S (t) is the horizontal plane total irradiance of the photovoltaic panel at the time t, and DF is the scattering ratio of the photovoltaic panel at the time t.
Further, the third determining unit includes:
determining the horizontal surface meter scattered irradiance of the photovoltaic panel according to the horizontal surface scattered irradiance of the photovoltaic panel by the following formula:
Sm,d(t)=Sd(t)-Sr,d(t);
determining the oblique surface meter scattering irradiance of the photovoltaic panel according to the horizontal surface meter scattering irradiance of the photovoltaic panel by the following formula:
Figure BDA0002238618570000081
in the formula, Sm,d(t) horizontal surface meter scattered irradiance of the photovoltaic panel at time t, Sd(t) horizontal plane scattered irradiance, S, of the photovoltaic panel at time tr,d(t) is the horizontal plane molecule scattering irradiance, S 'of the photovoltaic panel at time t'm,dAnd (t) is the scattering irradiance of the slope meter of the photovoltaic panel at the moment t, r is the false direct incidence ratio of the location of the photovoltaic panel, theta' (t) is the slope solar incident angle of the photovoltaic panel at the moment t, and theta (t) is the solar zenith angle at the moment t.
Further, the slope solar incident angle θ' (t) of the photovoltaic panel at time t is determined as follows:
θ′(t)=arccos[cosθ(t)×cosβ+sinθ(t)×sinβ×cos(α(t)-ε)]
the solar azimuth angle α (t) at time t is determined as follows:
Figure BDA0002238618570000082
wherein beta is the inclination angle of the surface of the photovoltaic panel, epsilon is the orientation angle of the surface of the photovoltaic panel (when the surface of the photovoltaic panel faces the south, the orientation angle is 180 degrees), alpha (t) is the azimuth angle of the sun at the moment t,
Figure BDA0002238618570000083
and delta (t) is the solar declination angle at the position of the photovoltaic panel at the moment t.
Further, the fourth determining unit includes:
determining the direct bevel irradiance S 'of the photovoltaic panel at the moment t according to the formula'b(t):
Figure BDA0002238618570000084
In the formula, theta' (t) is the inclined plane solar incident angle of the photovoltaic panel at the time t, theta (t) is the solar zenith angle at the time t, SbAnd (t) is the horizontal plane direct irradiance of the photovoltaic panel at the time t.
Preferably, the third determining module is configured to:
determining the bevel irradiance S' (t) of the photovoltaic panel at the time t according to the following formula:
S′(t)=S′b(t)+S′m,d(t)+S′r,d(t)
of formula (II) S'b(t) is the direct bevel irradiance, S 'of the photovoltaic panel at time t'm,d(t) is the bevel meter scattered irradiance, S 'of the photovoltaic panel at the moment t'r,dAnd (t) is the oblique plane molecular scattering irradiance of the photovoltaic panel at the time t.
Compared with the closest prior art, the invention has the following beneficial effects:
according to the technical scheme provided by the invention, the molecular scattering irradiance of the inclined plane of the photovoltaic panel is determined according to the horizontal plane scattering irradiance of the photovoltaic panel under the clearance condition; respectively determining the direct inclined plane irradiance and the scattered inclined plane irradiance of the photovoltaic panel according to the total horizontal plane irradiance of the photovoltaic panel; determining the inclined plane irradiance of the photovoltaic panel according to the inclined plane direct irradiance, the inclined plane molecular scattering irradiance and the inclined plane meter scattering irradiance of the photovoltaic panel; the horizontal plane scattered irradiance of the photovoltaic panel is divided into the horizontal plane molecular scattered irradiance of the photovoltaic panel and the horizontal plane molecular scattered irradiance of the photovoltaic panel, and the horizontal plane molecular scattered irradiance of the photovoltaic panel are respectively converted into the inclined plane irradiance molecular scattered irradiance of the photovoltaic panel and the horizontal plane meter scattered irradiance of the photovoltaic panel, so that the fineness and the accuracy of the irradiance calculation of the photovoltaic panel are improved.
According to the technical scheme provided by the invention, the meter scattering is regarded as superposition of direct incidence and various same-nature scatter according to a certain proportion, and an algorithm for converting horizontal surface meter scattering of the photovoltaic panel into inclined surface meter scattering of the photovoltaic panel is provided on the basis.
Drawings
FIG. 1 is a flow chart of a method of determining bevel irradiance of a photovoltaic panel;
FIG. 2 is a graph of horizontal plane irradiance, actual photovoltaic output, and bevel irradiance of a photovoltaic panel;
FIG. 3 is a schematic illustration of the dependence of photovoltaic panel horizontal irradiance on photovoltaic panel actual photovoltaic output and photovoltaic panel bevel irradiance on photovoltaic panel actual photovoltaic output;
fig. 4 is a block diagram of a system for determining bevel irradiance of a photovoltaic panel.
Detailed Description
The following describes embodiments of the present invention in further detail with reference to the accompanying drawings.
In order to make the objects, technical solutions and advantages of the embodiments of the present invention clearer, the technical solutions in the embodiments of the present invention will be clearly and completely described below with reference to the drawings in the embodiments of the present invention, and it is obvious that the described embodiments are some, but not all, embodiments of the present invention. All other embodiments, which can be derived by a person skilled in the art from the embodiments given herein without making any creative effort, shall fall within the protection scope of the present invention.
The invention provides a method for determining the inclined plane irradiance of a photovoltaic panel, which comprises the following steps of:
step 101, determining the molecular scattering irradiance of the inclined plane of the photovoltaic panel according to the horizontal plane scattering irradiance of the photovoltaic panel under the clearance condition;
step 102, respectively determining the inclined plane direct irradiance and the inclined plane meter scattered irradiance of the photovoltaic panel according to the horizontal plane total irradiance of the photovoltaic panel;
and 103, determining the inclined plane irradiance of the photovoltaic panel according to the inclined plane direct irradiance, the inclined plane molecular scattering irradiance and the inclined plane meter scattering irradiance of the photovoltaic panel.
In the preferred embodiment of the present invention, after the solar radiation enters the atmosphere, it encounters gas molecules and suspended solid and liquid particles, and part of the radiation changes direction, forming scattered radiation.
Scattering mainly comprises two types: one is molecular scattering (also called rayleigh scattering), which is mainly caused by gas molecules; the other is rice scattering, mainly caused by suspended particles such as dust, cloud droplets, etc.
Among these, molecular scattering is typically isotropic, i.e., the radiation is directed generally uniformly in all directions. Molecular scattering is less affected by weather conditions and its amount is more stable, typically equal to the total amount of scattered radiation in the net irradiance.
Specifically, the step 101 includes:
determining the scattering irradiance S 'of the bevel molecules of the photovoltaic panel at the moment t according to the formula'r,d(t):
Figure BDA0002238618570000101
In the formula, Sr,d(t) the horizontal plane molecule scattering irradiance of the photovoltaic panel at the moment t, and beta is the plate surface inclination angle of the photovoltaic panel;
wherein the horizontal plane molecule scattering irradiance S of the photovoltaic panel at the time t is determined according to the following formular,d(t):
Sr,d(t)=Sd,c(t)
In the formula, Sd,cAnd (t) is the horizontal plane scattering irradiance of the photovoltaic panel at the moment t under the clearance condition.
Specifically, before the step 101, the method further includes:
determining horizontal plane scattering irradiance S of the photovoltaic panel at the t moment under clearance condition according to the following formulad,c(t):
Sd,c(t)=So(t)·τd(t)·cosθ(t)
In the formula, So(t) solar irradiance, τ, in a plane perpendicular to sunlight at the upper atmospheric boundary at time td(t) is the scattering transparency coefficient at the moment t, and theta (t) is the solar zenith angle at the moment t;
in the preferred embodiment of the present invention, the irradiance of the upper atmospheric boundary depends mainly on the sun-earth relationship, i.e. the position of the sun as seen from the earth's surface coordinate system, which is generally expressed by the sun zenith and azimuth angles.
Wherein S iso(t) is determined as follows:
Figure BDA0002238618570000102
in the formula (I), the compound is shown in the specification,
Figure BDA0002238618570000103
is the sun constant, doD (t) is the average distance of the day and the ground, and d (t) is the distance of the day and the ground at the time t;
τd(t) is determined as follows:
τd(t)=0.271-0.294·τb(t)
in the formula, τb(t) is the direct transparency coefficient at time t;
τb(t) is determined as follows:
Figure BDA0002238618570000111
in the formula, Mh(t) is the relative large air volume at the location of the photovoltaic panel at the time t;
Mh(t) is determined as follows:
Figure BDA0002238618570000112
in the formula, h is the altitude of the photovoltaic panel;
θ (t) is determined as follows:
Figure BDA0002238618570000113
in the formula, ω (t) is the time angle of the sun at time t,
Figure BDA0002238618570000114
and delta (t) is the solar declination angle at the position of the photovoltaic panel at the moment t.
Further, the step 102 includes:
step a, determining the scattering ratio of the position of the photovoltaic panel according to the horizontal plane total irradiance of the photovoltaic panel;
b, determining horizontal plane scattering irradiance and horizontal plane direct irradiance of the photovoltaic panel according to the scattering ratio of the photovoltaic panel;
c, determining the inclined plane meter scattering irradiance of the photovoltaic panel according to the horizontal plane scattering irradiance of the photovoltaic panel;
and d, determining the direct inclined plane irradiance of the photovoltaic panel according to the horizontal plane direct irradiance of the photovoltaic panel.
Still further, the step a includes:
and determining the scattering ratio DF of the photovoltaic panel at the position of the t moment according to the following formula:
Figure BDA0002238618570000115
in the formula, kTThe clearance index of the place where the photovoltaic panel is located at the moment t.
Wherein, the clearance index k of the photovoltaic panel at the t moment is determined according to the following formulaT
Figure BDA0002238618570000121
Wherein S (t) is the total horizontal irradiance of the photovoltaic panel at the time t, SoAnd (t) is the atmospheric upper bound solar irradiance of the photovoltaic panel at the time t, and theta (t) is the solar zenith angle at the time t.
Still further, the step b includes:
determining horizontal plane scattering irradiance S of photovoltaic panel at time t according to the following formulad(t):
Sd(t)=S(t)·DF
Determining horizontal plane direct irradiance S of photovoltaic panel at time t according to the following formulab(t):
Sb(t)=S(t)-Sd(t)
Wherein S (t) is the solar irradiance on the atmospheric upper bound and sunlight vertical plane at the time t, and DF is the scattering ratio of the photovoltaic panel at the time t.
Still further, the step c includes:
determining the horizontal surface meter scattered irradiance of the photovoltaic panel according to the horizontal surface scattered irradiance of the photovoltaic panel by the following formula:
Sm,d(t)=Sd(t)-Sr,d(t);
determining the oblique surface meter scattering irradiance of the photovoltaic panel according to the horizontal surface meter scattering irradiance of the photovoltaic panel by the following formula:
Figure BDA0002238618570000122
in the formula, Sm,d(t) horizontal surface meter scattered irradiance of the photovoltaic panel at time t, Sd(t) horizontal plane scattered irradiance, S, of the photovoltaic panel at time tr,d(t) is the horizontal plane molecule scattering irradiance, S 'of the photovoltaic panel at time t'm,dAnd (t) is the scattering irradiance of the slope meter of the photovoltaic panel at the moment t, r is the false direct incidence ratio of the location of the photovoltaic panel, theta' (t) is the slope solar incident angle of the photovoltaic panel at the moment t, and theta (t) is the solar zenith angle at the moment t.
In the preferred embodiment of the present invention, the false direct ratio r is the ratio of what is statistically considered to be direct in the meter scattering; 1-r refers to the proportion of the meter scatter statistically considered as scatter.
Due to the fact that weather conditions are complex and variable, the false direct lighting ratio does not have a fixed value, but is a statistical mean value. The user can calculate according to local actual data, and can also adopt an empirical coefficient of 0.7.
Still further, the oblique solar incident angle θ' (t) of the photovoltaic panel at time t is determined as follows:
θ′(t)=arccos[cosθ(t)×cosβ+sinθ(t)×sinβ×cos(α(t)-ε)]
the solar azimuth angle α (t) at time t is determined as follows:
Figure BDA0002238618570000131
wherein beta is the inclination angle of the surface of the photovoltaic panel, epsilon is the orientation angle of the surface of the photovoltaic panel (when the surface of the photovoltaic panel faces the south, the orientation angle is 180 degrees), alpha (t) is the azimuth angle of the sun at the moment t,
Figure BDA0002238618570000132
and delta (t) is the solar declination angle at the position of the photovoltaic panel at the moment t.
Still further, the step d includes:
determining the direct bevel irradiance S 'of the photovoltaic panel at the moment t according to the formula'b(t):
Figure BDA0002238618570000133
In the formula, theta' (t) is the inclined plane solar incident angle of the photovoltaic panel at the time t, theta (t) is the solar zenith angle at the time t, SbAnd (t) is the horizontal plane direct irradiance of the photovoltaic panel at the time t.
Further, the step 103 includes:
determining the bevel irradiance S' (t) of the photovoltaic panel at the time t according to the following formula:
S′(t)=S′b(t)+S′m,d(t)+S′r,d(t)
of formula (II) S'b(t) is the direct bevel irradiance, S 'of the photovoltaic panel at time t'm,d(t) is the bevel meter scattered irradiance, S 'of the photovoltaic panel at the moment t'r,dAnd (t) is the oblique plane molecular scattering irradiance of the photovoltaic panel at the time t.
In the best embodiment of the invention, the technical scheme provided by the invention can be applied to the calculation of site selection design, output evaluation, theoretical power, light abandon electric quantity and the like of a photovoltaic power station; the method can also be applied to calculation such as photovoltaic power station power prediction and electric quantity prediction, and has important application value.
By utilizing the technical method provided by the invention, the solar irradiance of the photovoltaic panel can be more accurately obtained, and further, the photovoltaic theoretical power can be more accurately calculated or the photovoltaic power can be more accurately predicted. For example, (a) in fig. 2 shows the horizontal irradiance of the photovoltaic panel at the historical moment, (b) in fig. 2 shows the corresponding output of the photovoltaic panel at the historical moment, and (c) in fig. 2 shows the inclined irradiance of the photovoltaic panel at the historical moment; as can be seen from fig. 2 (a) and fig. 2 (b), the horizontal irradiance of the photovoltaic panel and the inclined plane irradiance of the photovoltaic panel are greatly different from each other, fig. 3 (a) shows the correlation between the horizontal irradiance of the photovoltaic panel and the corresponding output of the photovoltaic panel, fig. 3 (b) shows the correlation between the inclined plane irradiance of the photovoltaic panel and the corresponding output of the photovoltaic panel, and as can be seen from fig. 3 (b) and fig. 3 (a), the correlation between the inclined plane irradiance of the photovoltaic panel and the corresponding output of the photovoltaic panel is stronger than the correlation between the horizontal irradiance of the photovoltaic panel and the corresponding output of the photovoltaic panel.
The invention provides a system for determining the inclined plane irradiance of a photovoltaic panel, as shown in figure 4, the system comprises:
the first determination module is used for determining the molecular scattering irradiance of the inclined plane of the photovoltaic panel according to the horizontal plane scattering irradiance of the photovoltaic panel under the clearance condition;
the second determining module is used for respectively determining the inclined plane direct irradiance and the inclined plane meter scattering irradiance of the photovoltaic panel according to the horizontal plane total irradiance of the photovoltaic panel;
and the third determining module is used for determining the inclined plane irradiance of the photovoltaic panel according to the inclined plane direct irradiance, the inclined plane molecular scattering irradiance and the inclined plane meter scattering irradiance of the photovoltaic panel.
Specifically, the first determining module includes:
determining the scattering irradiance S 'of the bevel molecules of the photovoltaic panel at the moment t according to the formula'r,d(t):
Figure BDA0002238618570000141
In the formula, Sr,d(t) the horizontal plane molecule scattering irradiance of the photovoltaic panel at the moment t, and beta is the plate surface inclination angle of the photovoltaic panel;
wherein the horizontal plane molecule scattering irradiance S of the photovoltaic panel at the time t is determined according to the following formular,d(t):
Sr,d(t)=Sd,c(t)
In the formula, Sd,cAnd (t) is the horizontal plane scattering irradiance of the photovoltaic panel at the moment t under the clearance condition.
Specifically, before the first determining module, the method further includes:
determining horizontal plane scattering irradiance S of the photovoltaic panel at the t moment under clearance condition according to the following formulad,c(t):
Sd,c(t)=So(t)·τd(t)·cosθ(t)
In the formula, So(t) solar irradiance, τ, in a plane perpendicular to sunlight at the upper atmospheric boundary at time td(t) is the scattering transparency coefficient at the moment t, and theta (t) is the solar zenith angle at the moment t;
wherein S iso(t) is determined as follows:
Figure BDA0002238618570000151
in the formula (I), the compound is shown in the specification,
Figure BDA0002238618570000152
is the sun constant, doD (t) is the average distance of the day and the ground, and d (t) is the distance of the day and the ground at the time t;
τd(t) is determined as follows:
τd(t)=0.271-0.294·τb(t)
in the formula, τb(t) is the direct transparency coefficient at time t;
τb(t) is determined as follows:
Figure BDA0002238618570000153
in the formula, Mh(t) is the relative large air volume at the location of the photovoltaic panel at the time t;
Mh(t) is determined as follows:
Figure BDA0002238618570000154
in the formula, h is the altitude of the photovoltaic panel;
θ (t) is determined as follows:
Figure BDA0002238618570000155
in the formula, ω (t) is the time angle of the sun at time t,
Figure BDA0002238618570000156
and delta (t) is the solar declination angle at the position of the photovoltaic panel at the moment t.
Further, according to the second determining module, the method includes:
the first determining unit is used for determining the scattering ratio of the photovoltaic panel at the position according to the horizontal plane total irradiance of the photovoltaic panel;
the second determining unit is used for determining the horizontal plane scattering irradiance and the horizontal plane direct irradiance of the photovoltaic panel according to the scattering ratio of the photovoltaic panel;
the third determining unit is used for determining the inclined surface meter scattered irradiance of the photovoltaic panel according to the horizontal surface scattered irradiance of the photovoltaic panel;
and the fourth determining unit is used for determining the inclined plane direct irradiance of the photovoltaic panel according to the horizontal plane direct irradiance of the photovoltaic panel.
Still further, the first determining unit is configured to:
and determining the scattering ratio DF of the photovoltaic panel at the position of the t moment according to the following formula:
Figure BDA0002238618570000161
in the formula, kTThe clearance index of the place where the photovoltaic panel is located at the moment t.
Wherein, the clearance index k of the photovoltaic panel at the t moment is determined according to the following formulaT
Figure BDA0002238618570000162
Wherein S (t) is the total horizontal irradiance of the photovoltaic panel at the time t, SoAnd (t) is the solar irradiance on the plane vertical to the sunlight on the upper air boundary at the time t, and theta (t) is the solar zenith angle at the time t.
Still further, the second determining unit is configured to:
determining horizontal plane scattering irradiance S of photovoltaic panel at time t according to the following formulad(t):
Sd(t)=S(t)·DF
Determining horizontal plane direct irradiance S of photovoltaic panel at time t according to the following formulab(t):
Sb(t)=S(t)-Sd(t)
Wherein S (t) is the horizontal plane total irradiance of the photovoltaic panel at the time t, and DF is the scattering ratio of the photovoltaic panel at the time t.
Still further, the third determining unit includes:
determining the horizontal surface meter scattered irradiance of the photovoltaic panel according to the horizontal surface scattered irradiance of the photovoltaic panel by the following formula:
Sm,d(t)=Sd(t)-Sr,d(t);
determining the oblique surface meter scattering irradiance of the photovoltaic panel according to the horizontal surface meter scattering irradiance of the photovoltaic panel by the following formula:
Figure BDA0002238618570000163
in the formula, Sm,d(t) horizontal surface meter scattered irradiance of the photovoltaic panel at time t, Sd(t) horizontal plane scattered irradiance, S, of the photovoltaic panel at time tr,d(t) is the horizontal plane molecule scattering irradiance, S 'of the photovoltaic panel at time t'm,dAnd (t) is the scattering irradiance of the slope meter of the photovoltaic panel at the moment t, r is the false direct incidence ratio of the location of the photovoltaic panel, theta' (t) is the slope solar incident angle of the photovoltaic panel at the moment t, and theta (t) is the solar zenith angle at the moment t.
Still further, the oblique solar incident angle θ' (t) of the photovoltaic panel at time t is determined as follows:
θ′(t)=arccos[cosθ(t)×cosβ+sinθ(t)×sinβ×cos(α(t)-ε)]
the solar azimuth angle α (t) at time t is determined as follows:
Figure BDA0002238618570000171
wherein beta is the inclination angle of the surface of the photovoltaic panel, epsilon is the orientation angle of the surface of the photovoltaic panel (when the surface of the photovoltaic panel faces the south, the orientation angle is 180 degrees), alpha (t) is the azimuth angle of the sun at the moment t,
Figure BDA0002238618570000172
and delta (t) is the solar declination angle at the position of the photovoltaic panel at the moment t.
Still further, the fourth determining unit includes:
determining the direct bevel irradiance S 'of the photovoltaic panel at the moment t according to the formula'b(t):
Figure BDA0002238618570000173
In the formula, theta' (t) is the inclined plane solar incident angle of the photovoltaic panel at the time t, theta (t) is the solar zenith angle at the time t, SbAnd (t) is the horizontal plane direct irradiance of the photovoltaic panel at the time t.
Specifically, the third determining module is configured to:
determining the bevel irradiance S' (t) of the photovoltaic panel at the time t according to the following formula:
S′(t)=S′b(t)+S′m,d(t)+S′r,d(t)
of formula (II) S'b(t) is the direct bevel irradiance, S 'of the photovoltaic panel at time t'm,d(t) is the bevel meter scattered irradiance, S 'of the photovoltaic panel at the moment t'r,dAnd (t) is the oblique plane molecular scattering irradiance of the photovoltaic panel at the time t.
As will be appreciated by one skilled in the art, embodiments of the present application may be provided as a method, system, or computer program product. Accordingly, the present application may take the form of an entirely hardware embodiment, an entirely software embodiment or an embodiment combining software and hardware aspects. Furthermore, the present application may take the form of a computer program product embodied on one or more computer-usable storage media (including, but not limited to, disk storage, CD-ROM, optical storage, and the like) having computer-usable program code embodied therein.
The present application is described with reference to flowchart illustrations and/or block diagrams of methods, apparatus (systems), and computer program products according to embodiments of the application. It will be understood that each flow and/or block of the flow diagrams and/or block diagrams, and combinations of flows and/or blocks in the flow diagrams and/or block diagrams, can be implemented by computer program instructions. These computer program instructions may be provided to a processor of a general purpose computer, special purpose computer, embedded processor, or other programmable data processing apparatus to produce a machine, such that the instructions, which execute via the processor of the computer or other programmable data processing apparatus, create means for implementing the functions specified in the flowchart flow or flows and/or block diagram block or blocks.
These computer program instructions may also be stored in a computer-readable memory that can direct a computer or other programmable data processing apparatus to function in a particular manner, such that the instructions stored in the computer-readable memory produce an article of manufacture including instruction means which implement the function specified in the flowchart flow or flows and/or block diagram block or blocks.
These computer program instructions may also be loaded onto a computer or other programmable data processing apparatus to cause a series of operational steps to be performed on the computer or other programmable apparatus to produce a computer implemented process such that the instructions which execute on the computer or other programmable apparatus provide steps for implementing the functions specified in the flowchart flow or flows and/or block diagram block or blocks.
Finally, it should be noted that: the above embodiments are only for illustrating the technical solutions of the present invention and not for limiting the same, and although the present invention is described in detail with reference to the above embodiments, those of ordinary skill in the art should understand that: modifications and equivalents may be made to the embodiments of the invention without departing from the spirit and scope of the invention, which is to be covered by the claims.

Claims (20)

1. A method of determining bevel irradiance of a photovoltaic panel, the method comprising:
determining the molecular scattering irradiance of the inclined plane of the photovoltaic panel according to the horizontal plane scattering irradiance of the photovoltaic panel under the clearance condition;
respectively determining the direct inclined plane irradiance and the scattered inclined plane irradiance of the photovoltaic panel according to the total horizontal plane irradiance of the photovoltaic panel;
and determining the inclined plane irradiance of the photovoltaic panel according to the inclined plane direct irradiance, the inclined plane molecular scattering irradiance and the inclined plane meter scattering irradiance of the photovoltaic panel.
2. The method of claim 1, wherein determining the photovoltaic panel oblique molecular scatter irradiance from the photovoltaic panel horizontal scatter irradiance under headroom conditions comprises:
determining the scattering irradiance S 'of the bevel molecules of the photovoltaic panel at the moment t according to the formula'r,d(t):
Figure FDA0002238618560000011
In the formula, Sr,d(t) the horizontal plane molecule scattering irradiance of the photovoltaic panel at the moment t, and beta is the plate surface inclination angle of the photovoltaic panel;
wherein the horizontal plane molecule scattering irradiance S of the photovoltaic panel at the time t is determined according to the following formular,d(t):
Sr,d(t)=Sd,c(t)
In the formula, Sd,cAnd (t) is the horizontal plane scattering irradiance of the photovoltaic panel at the moment t under the clearance condition.
3. The method of claim 2, wherein prior to determining the photovoltaic panel oblique molecular scatter irradiance based on the photovoltaic panel horizontal scatter irradiance under headroom conditions, further comprising:
determining horizontal plane scattering irradiance S of the photovoltaic panel at the t moment under clearance condition according to the following formulad,c(t):
Sd,c(t)=So(t)·τd(t)·cosθ(t)
In the formula, So(t) solar irradiance, τ, in a plane perpendicular to sunlight at the upper atmospheric boundary at time td(t) is the scattering transparency coefficient at the moment t, and theta (t) is the solar zenith angle at the moment t;
wherein S iso(t) is determined as follows:
Figure FDA0002238618560000012
in the formula (I), the compound is shown in the specification,
Figure FDA0002238618560000013
is the sun constant, doD (t) is the average distance of the day and the ground, and d (t) is the distance of the day and the ground at the time t;
τd(t) is determined as follows:
τd(t)=0.271-0.294·τb(t)
in the formula, τb(t) direct transparency at time tA coefficient;
τb(t) is determined as follows:
Figure FDA0002238618560000021
in the formula, Mh(t) is the relative large air volume at the location of the photovoltaic panel at the time t;
Mh(t) is determined as follows:
Figure FDA0002238618560000022
in the formula, h is the altitude of the photovoltaic panel;
θ (t) is determined as follows:
Figure FDA0002238618560000023
in the formula, ω (t) is the time angle of the sun at time t,
Figure FDA0002238618560000024
and delta (t) is the solar declination angle at the position of the photovoltaic panel at the moment t.
4. The method of claim 1, wherein determining the sloping direct irradiance and the sloping meter diffuse irradiance of the photovoltaic panel from the total horizontal irradiance of the photovoltaic panel comprises:
determining the scattering ratio of the photovoltaic panel at the location according to the horizontal plane total irradiance of the photovoltaic panel;
determining horizontal plane scattering irradiance and horizontal plane direct irradiance of the photovoltaic panel according to the scattering ratio of the photovoltaic panel;
determining the inclined surface meter scattered irradiance of the photovoltaic panel according to the horizontal surface scattered irradiance of the photovoltaic panel;
and determining the direct inclined plane irradiance of the photovoltaic panel according to the direct horizontal plane irradiance of the photovoltaic panel.
5. The method of claim 4, wherein determining the scattering ratio at the locus of the photovoltaic panel from the horizontal plane total irradiance of the photovoltaic panel comprises:
and determining the scattering ratio DF of the photovoltaic panel at the position of the t moment according to the following formula:
Figure FDA0002238618560000025
in the formula, kTThe clearance index of the place where the photovoltaic panel is located at the moment t.
Wherein, the clearance index k of the photovoltaic panel at the t moment is determined according to the following formulaT
Figure FDA0002238618560000031
Wherein S (t) is the total horizontal irradiance of the photovoltaic panel at the time t, SoAnd (t) is the solar irradiance on the plane vertical to the sunlight on the upper air boundary at the time t, and theta (t) is the solar zenith angle at the time t.
6. The method of claim 4, wherein determining the horizontal scattered irradiance and the horizontal direct irradiance of the photovoltaic panel from the scattering ratio at the location of the photovoltaic panel comprises:
determining horizontal plane scattering irradiance S of photovoltaic panel at time t according to the following formulad(t):
Sd(t)=S(t)·DF
Determining horizontal plane direct irradiance S of photovoltaic panel at time t according to the following formulab(t):
Sb(t)=S(t)-Sd(t)
Wherein S (t) is the horizontal plane total irradiance of the photovoltaic panel at the time t, and DF is the scattering ratio of the photovoltaic panel at the time t.
7. The method of claim 4, wherein determining the bevel meter scatter irradiance of the photovoltaic panel from the horizontal plane scatter irradiance of the photovoltaic panel comprises:
determining the horizontal surface meter scattered irradiance of the photovoltaic panel according to the horizontal surface scattered irradiance of the photovoltaic panel by the following formula:
Sm,d(t)=Sd(t)-Sr,d(t);
determining the oblique surface meter scattering irradiance of the photovoltaic panel according to the horizontal surface meter scattering irradiance of the photovoltaic panel by the following formula:
Figure FDA0002238618560000032
in the formula, Sm,d(t) horizontal surface meter scattered irradiance of the photovoltaic panel at time t, Sd(t) horizontal plane scattered irradiance, S, of the photovoltaic panel at time tr,d(t) is the horizontal plane molecule scattering irradiance, S 'of the photovoltaic panel at time t'm,dAnd (t) is the scattering irradiance of the slope meter of the photovoltaic panel at the moment t, r is the false direct incidence ratio of the location of the photovoltaic panel, theta' (t) is the slope solar incident angle of the photovoltaic panel at the moment t, and theta (t) is the solar zenith angle at the moment t.
8. The method of claim 7, wherein θ' (t) is determined by:
θ'(t)=arccos[cosθ(t)×cosβ+sinθ(t)×sinβ×cos(α(t)-ε)]
wherein the solar azimuth angle α (t) at time t is determined by:
Figure FDA0002238618560000041
wherein beta is the inclination angle of the surface of the photovoltaic panel, epsilon is the orientation angle of the surface of the photovoltaic panel (when the surface of the photovoltaic panel faces the south, the orientation angle is 180 degrees),
Figure FDA0002238618560000042
is a photovoltaicAnd the latitude where the plate is located, wherein delta (t) is the solar declination angle where the photovoltaic plate is located at the moment t.
9. The method of claim 4, wherein determining the sloping direct irradiance of the photovoltaic panel from the horizontal plane direct irradiance of the photovoltaic panel comprises:
determining the direct bevel irradiance S 'of the photovoltaic panel at the moment t according to the formula'b(t):
Figure FDA0002238618560000043
In the formula, theta' (t) is the inclined plane solar incident angle of the photovoltaic panel at the time t, theta (t) is the solar zenith angle at the time t, SbAnd (t) is the horizontal plane direct irradiance of the photovoltaic panel at the time t.
10. The method of claim 1, wherein determining the bevel irradiance of the photovoltaic panel from the bevel direct irradiance, the bevel molecular diffuse irradiance, and the bevel meter diffuse irradiance of the photovoltaic panel comprises:
determining the bevel irradiance S' (t) of the photovoltaic panel at the time t according to the following formula:
S'(t)=S'b(t)+S'm,d(t)+S'r,d(t)
of formula (II) S'b(t) is the direct bevel irradiance, S 'of the photovoltaic panel at time t'm,d(t) is the bevel meter scattered irradiance, S 'of the photovoltaic panel at the moment t'r,dAnd (t) is the oblique plane molecular scattering irradiance of the photovoltaic panel at the time t.
11. A system for determining bevel irradiance of a photovoltaic panel, the system comprising:
the first determination module is used for determining the molecular scattering irradiance of the inclined plane of the photovoltaic panel according to the horizontal plane scattering irradiance of the photovoltaic panel under the clearance condition;
the second determining module is used for respectively determining the inclined plane direct irradiance and the inclined plane meter scattering irradiance of the photovoltaic panel according to the horizontal plane total irradiance of the photovoltaic panel;
and the third determining module is used for determining the inclined plane irradiance of the photovoltaic panel according to the inclined plane direct irradiance, the inclined plane molecular scattering irradiance and the inclined plane meter scattering irradiance of the photovoltaic panel.
12. The system of claim 11, wherein the first determination module comprises:
determining the scattering irradiance S 'of the bevel molecules of the photovoltaic panel at the moment t according to the formula'r,d(t):
Figure FDA0002238618560000051
In the formula, Sr,d(t) the horizontal plane molecule scattering irradiance of the photovoltaic panel at the moment t, and beta is the plate surface inclination angle of the photovoltaic panel;
wherein the horizontal plane molecule scattering irradiance S of the photovoltaic panel at the time t is determined according to the following formular,d(t):
Sr,d(t)=Sd,c(t)
In the formula, Sd,cAnd (t) is the horizontal plane scattering irradiance of the photovoltaic panel at the moment t under the clearance condition.
13. The system of claim 12, wherein the first determination module is preceded by:
determining horizontal plane scattering irradiance S of the photovoltaic panel at the t moment under clearance condition according to the following formulad,c(t):
Sd,c(t)=So(t)·τd(t)·cosθ(t)
In the formula, So(t) solar irradiance, τ, in a plane perpendicular to sunlight at the upper atmospheric boundary at time td(t) is the scattering transparency coefficient at the moment t, and theta (t) is the solar zenith angle at the moment t;
wherein S iso(t) is determined as follows:
Figure FDA0002238618560000052
in the formula (I), the compound is shown in the specification,
Figure FDA0002238618560000053
is the sun constant, doD (t) is the average distance of the day and the ground, and d (t) is the distance of the day and the ground at the time t;
τd(t) is determined as follows:
τd(t)=0.271-0.294·τb(t)
in the formula, τb(t) is the direct transparency coefficient at time t;
τb(t) is determined as follows:
Figure FDA0002238618560000054
in the formula, Mh(t) is the relative large air volume at the location of the photovoltaic panel at the time t;
Mh(t) is determined as follows:
Figure FDA0002238618560000061
in the formula, h is the altitude of the photovoltaic panel;
θ (t) is determined as follows:
Figure FDA0002238618560000062
in the formula, ω (t) is the time angle of the sun at time t,
Figure FDA0002238618560000063
and delta (t) is the solar declination angle at the position of the photovoltaic panel at the moment t.
14. The system of claim 11, wherein according to a second determination module, comprising:
the first determining unit is used for determining the scattering ratio of the photovoltaic panel at the position according to the horizontal plane total irradiance of the photovoltaic panel;
the second determining unit is used for determining the horizontal plane scattering irradiance and the horizontal plane direct irradiance of the photovoltaic panel according to the scattering ratio of the photovoltaic panel;
the third determining unit is used for determining the inclined surface meter scattered irradiance of the photovoltaic panel according to the horizontal surface scattered irradiance of the photovoltaic panel;
and the fourth determining unit is used for determining the inclined plane direct irradiance of the photovoltaic panel according to the horizontal plane direct irradiance of the photovoltaic panel.
15. The system of claim 14, wherein the first determination unit is to:
and determining the scattering ratio DF of the photovoltaic panel at the position of the t moment according to the following formula:
Figure FDA0002238618560000064
in the formula, kTThe clearance index of the place where the photovoltaic panel is located at the moment t.
Wherein, the clearance index k of the photovoltaic panel at the t moment is determined according to the following formulaT
Figure FDA0002238618560000065
Wherein S (t) is the total horizontal irradiance of the photovoltaic panel at the time t, SoAnd (t) is the solar irradiance on the plane vertical to the sunlight on the upper air boundary at the time t, and theta (t) is the solar zenith angle at the time t.
16. The system of claim 14, wherein the second determination unit is to:
determining horizontal plane scattering irradiance S of photovoltaic panel at time t according to the following formulad(t):
Sd(t)=S(t)·DF
Determining horizontal plane direct irradiance S of photovoltaic panel at time t according to the following formulab(t):
Sb(t)=S(t)-Sd(t)
Wherein S (t) is the horizontal plane total irradiance of the photovoltaic panel at the time t, and DF is the scattering ratio of the photovoltaic panel at the time t.
17. The system of claim 14, wherein the third determination unit comprises:
determining the horizontal surface meter scattered irradiance of the photovoltaic panel according to the horizontal surface scattered irradiance of the photovoltaic panel by the following formula:
Sm,d(t)=Sd(t)-Sr,d(t);
determining the oblique surface meter scattering irradiance of the photovoltaic panel according to the horizontal surface meter scattering irradiance of the photovoltaic panel by the following formula:
Figure FDA0002238618560000071
in the formula, Sm,d(t) horizontal surface meter scattered irradiance of the photovoltaic panel at time t, Sd(t) horizontal plane scattered irradiance, S, of the photovoltaic panel at time tr,d(t) is the horizontal plane molecule scattering irradiance, S 'of the photovoltaic panel at time t'm,dAnd (t) is the scattering irradiance of the slope meter of the photovoltaic panel at the moment t, r is the false direct incidence ratio of the location of the photovoltaic panel, theta' (t) is the slope solar incident angle of the photovoltaic panel at the moment t, and theta (t) is the solar zenith angle at the moment t.
18. The system of claim 17, wherein the slope solar angle of incidence θ' (t) of the photovoltaic panel at time t is determined as follows:
θ'(t)=arccos[cosθ(t)×cosβ+sinθ(t)×sinβ×cos(α(t)-ε)]
the solar azimuth angle α (t) at time t is determined as follows:
Figure FDA0002238618560000072
wherein beta is the inclination angle of the surface of the photovoltaic panel, epsilon is the orientation angle of the surface of the photovoltaic panel (when the surface of the photovoltaic panel faces the south, the orientation angle is 180 degrees), alpha (t) is the azimuth angle of the sun at the moment t,
Figure FDA0002238618560000073
and delta (t) is the solar declination angle at the position of the photovoltaic panel at the moment t.
19. The system of claim 14, wherein the fourth determination unit comprises:
determining the direct bevel irradiance S 'of the photovoltaic panel at the moment t according to the formula'b(t):
Figure FDA0002238618560000081
In the formula, theta' (t) is the inclined plane solar incident angle of the photovoltaic panel at the time t, theta (t) is the solar zenith angle at the time t, SbAnd (t) is the horizontal plane direct irradiance of the photovoltaic panel at the time t.
20. The system of claim 11, wherein the third determination module is to:
determining the bevel irradiance S' (t) of the photovoltaic panel at the time t according to the following formula:
S'(t)=S'b(t)+S'm,d(t)+S'r,d(t)
of formula (II) S'b(t) is the direct bevel irradiance, S 'of the photovoltaic panel at time t'm,d(t) is the bevel meter scattered irradiance, S 'of the photovoltaic panel at the moment t'r,dAnd (t) is the oblique plane molecular scattering irradiance of the photovoltaic panel at the time t.
CN201910992211.0A 2019-10-18 2019-10-18 Method and system for determining inclined plane irradiance of photovoltaic panel Pending CN112688637A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201910992211.0A CN112688637A (en) 2019-10-18 2019-10-18 Method and system for determining inclined plane irradiance of photovoltaic panel

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201910992211.0A CN112688637A (en) 2019-10-18 2019-10-18 Method and system for determining inclined plane irradiance of photovoltaic panel

Publications (1)

Publication Number Publication Date
CN112688637A true CN112688637A (en) 2021-04-20

Family

ID=75444921

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201910992211.0A Pending CN112688637A (en) 2019-10-18 2019-10-18 Method and system for determining inclined plane irradiance of photovoltaic panel

Country Status (1)

Country Link
CN (1) CN112688637A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN116026455A (en) * 2023-02-22 2023-04-28 中国科学技术大学 Measurement method of high-precision irradiation sensor

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN116026455A (en) * 2023-02-22 2023-04-28 中国科学技术大学 Measurement method of high-precision irradiation sensor

Similar Documents

Publication Publication Date Title
Andrews et al. The effect of spectral albedo on amorphous silicon and crystalline silicon solar photovoltaic device performance
CN108923738B (en) Control method of dual-tracking photovoltaic power generation system based on weather type judgment
US20230289697A1 (en) Optimization design method for photovoltaic system by taking system benefit optimization as target
Shyam S et al. Estimation of hourly solar radiation on horizontal and inclined surfaces in Western Himalayas
Yousuf et al. Solar energy potential estimation by calculating sun illumination hours and sky view factor on building rooftops using digital elevation model
CN108763649B (en) Method for optimizing and evaluating irradiation quantity received by photovoltaic module cell
Santbergen et al. Calculation of irradiance distribution on PV modules by combining sky and sensitivity maps
Hiller et al. TRNSHD—a program for shading and insolation calculations
Baklouti et al. Estimation of solar radiation on horizontal and inclined surfaces in Sfax, TUNISIA
Herrera-Romero et al. RETRACTED: Estimation of the optimum tilt angle of solar collectors in Coatzacoalcos, Veracruz
CN112688637A (en) Method and system for determining inclined plane irradiance of photovoltaic panel
Perers The solar resource in cold climates
CN110764536A (en) Optimization method for flat single-axis photovoltaic tracking system
WO2024067634A1 (en) Method and device for identifying weather state by means of multiple irradiation meters
CN101030301A (en) Virtual computer for remote-sensing distributed image on rolling ground
Cellura et al. A photographic method to estimate the shading effect of obstructions
CN107168381B (en) Method for analyzing influence of terrestrial shape on sun tracking error of heliostat
RU2579169C1 (en) Positioning and solar tracking system for concentrator solar power plant
WO2023115740A1 (en) Method and system for calculating solar radiation energy received by building
CN111596381B (en) Method for estimating direct irradiation proportion by using double radiometers
Strebkov et al. Nontracking solar concentrators with louver heliostats: bar-to-bar effects
CN115689021A (en) Method, device, storage medium and processor for predicting power of photovoltaic power station
CN111596384B (en) Inclined plane radiation prediction method based on weather type effective identification
Bredemeier et al. Large‐scale spatiotemporal calculation of photovoltaic capacity factors using ray tracing: A case study in urban environments
Bredemeier et al. Fast evaluation of rooftop and façade PV potentials using backward ray tracing and machine learning

Legal Events

Date Code Title Description
PB01 Publication
PB01 Publication
SE01 Entry into force of request for substantive examination
SE01 Entry into force of request for substantive examination