1. Trang chủ
  2. » Kỹ Thuật - Công Nghệ

Bsi bs en 60904 10 2010

18 0 0

Đang tải... (xem toàn văn)

Tài liệu hạn chế xem trước, để xem đầy đủ mời bạn chọn Tải xuống

THÔNG TIN TÀI LIỆU

Thông tin cơ bản

Tiêu đề Photovoltaic Devices Part 1: Methods of Linearity Measurement
Trường học British Standards Institution
Chuyên ngành Photovoltaic Device Standards
Thể loại Standards Publication
Năm xuất bản 2010
Thành phố London
Định dạng
Số trang 18
Dung lượng 911,81 KB

Các công cụ chuyển đổi và chỉnh sửa cho tài liệu này

Nội dung

BSI Standards Publication Photovoltaic devices Part 1 0 Methods of l inearity measurement BS EN 60904 1 0 201 0 National foreword This British Standard is the UK implementation of EN 60904 1 0 201 0 I[.]

Trang 1

BSI Standar ds Public ation

Pho tovo ltaic devic es

Part 10: Methods of l nearity meas urement

Trang 2

Nat io al fore word

T is Brit ish St an ard is t he U imple me nt at ion of EN 60 04 -10:2 10 It is

ide nt ic l t o IEC 60 04-10:2 0 It supe rse de s BS EN 60 04 -10:19 8 which is

wit hdrawn

T e UK part ic ipat ion in it s pre parat ion was e nt rust e d t o Te ch ic l C ommit t e e

GE /8 , P hot ovolt aic E e rg S st e ms

A ls of organiz t ions re pre se nt e d on t his commit t e e c n be o t aine d on

re que st t o it s se cre t ary

T is publc at ion doe s not purp r t o inclu e al t he ne c e ssary provisions of a

c ont ra t Use rs are re sp nsible for it s core c t ap lc at ion

© BSI 2 10

ISBN 9 8 0 5 0 64 38 4

ICS 2 160

C omplance wit h a Brit ish St andard can ot co fe r immu it y f om

le gal obl gat ions

This B t ish St an ard was p blshe d u de r t he aut ho t y of t he St an ards

P lc y an St rat e gy C ommit t e e o 30 Ap l 2010

Ame ndme nt s is ue d since pu lcat ion

Amd No Dat e Te xt afe ct e d

Trang 3

EUROPEA N STANDA RD

EN 60904- 10

NORME EUROPÉENNE

EUR OPÄISCHE NOR M

Marc h 2010

Euro e n Committee forElec trot ec hnical Stan ardiz ation

Comité Euro é n deNormalsat ion Elec trotec niq e

Euro äis hesKomitee für Elek trot ec hnisc he Normu g

Ce ntra l Secreta ria t:Ave nu Marnix 17, B - 100 0 Bru se ls

© 2 10 CENELEC - All rig ts of e ploit at io in a y form a d b a y me n re erv ed wo dwid for CENELECmemb rs

En ls version

Phot ov olt aic dev ices

-Part 10: Met hods of l nearity measurement

(IEC 60904-10:2009)

Disposit ifs ph t ov olt ạques

-Part ie 10: Mét ho esde mesure

de la lnéarit é

(CEI 609 4-10:2 09)

Photov olt aisc e Einric ht ungen

-Tei 10: Mes v erahren für die Linearit ät

(IEC 60904-10:2009)

This Euro e n Stan ard was a pro e b CENELEC o 2 10-0 -01 CENELEC memb rs are b u d t o comply

wit h the CEN/CENELEC Intern l Reg latio s which s p late t he con itio s for givin this Euro e n Stan ard

the st atus of a n tio al stan ard wit ho t a y alteratio

Up-to-d t e lsts a d biblo ra hic al refere ces conc ernin suc h n tio al stan ards ma b o tain d o

a plc atio t o the Ce t ral Secretariat or to a y CENELEC memb r

This Euro e n Stan ard e ists in t hre oficial versio s (En lsh, Fre ch, Germa ) A v rsio in a y ot her

la g a e ma e b tra slatio u d r the resp nsibi t y of a CENELEC memb r into its own la g a e a d n tifie

to the Ce tral Secret ariat h s th same status as th oficial v rsio s

CENELEC memb rs are t he n tio al electrot ec hnic al committ ees of Austria, Belgium, Bulg ria, Cro tia, Cy rus,

the Cz ech Rep blc , De mark, Estonia, Finla d, Fra ce, Germa y, Gre c e, Hu g ry, Ic la d, Irela d, Italy,

L tvia, Lithu nia, L ux mb urg, Malta, the Net herla ds, Norwa , Pola d, Port ug l, Roma ia, Slo akia, Slovenia,

Sp in, Swe e , Swit z erla d a d the Unit ed Kin d m

Trang 4

EN 6 9 4-10:2 10 - 2

-Foreword

The t ex t of doc ment 8 /58 /FDIS, fut ure edit ion 2 of IEC 6 9 4-10, pre ared by IEC TC8 , Solar

photovoltaic energ s stems, was s bmit t ed t o t he IEC-CENELEC p ralel vote an w as a prov ed by

CENELEC asEN 6 9 4-10 on 2 10-0 -01

This Euro e n St an ard s p rsedesEN 6 9 4-10:19 8

The main t ec nical c an es w it h regard to t he EN 6 9 4-10:19 8 are as folows:

– Ad ed clau e for two-lamp met hod for

s

lne rity

– Chan ed stan ard deviation as a met ric for lne rity t o p rcent dev iat ion fom lne rity Thiswas done

b cau e a non-lne r dev ice can have a low st an ard deviation an p rcent deviat ion is t he

q ant itat iv e n mb r t hat mat t ers for t he p ramet er of int eres

– R emov ed clau eon sp ct r al resp n iv ity nonlne r ityb cau e it isnot u ed by an PV

t est in / calbr at ion group F r t est in re lPV dev icesit isdific lt t o make t his eror sig ificant in the

sp ct ral mismat ch corect ion fact or w hie st il p s in Isclne rity Me s rin t he resp n iv ity ov er the

ent ire resp n e ran e me n t hat he dev ice w il pro a ly fai t he t emp rat ure lne rity ne r t he b n

ed e

– Ad ed a clau e t o alow s ort circ it lne r ityw ith t emp rat ure or t otal iradian et o b determined

fom a solut e sp ct ral resp n iv ity me s rement s This dat a is routinely re orted in PT primar y

referen e cel calbration cert ificat es

– Ad ed re ort clau e in complan e w it h ISO/IEC 17 2 req ir ement s

– Oft en t he t emp rat ure co ficient of s ort circ it c rent is ver y smal so me s rement erors can

res lt in p rcent deviation out side t he ac e ted ran e Therefore, t he folowin t ex t w as ad ed to

7.3c): “If t he t emp rat ure co ficient of s ort circ it c r ent isles t han 0,1 %/ K , t hen t he device can

b con idered lne rwit h resp ct t o this p ramet er.”

At t ent ion is drawn t o t he p s ibi ty t hat some of t he element s of t his doc ment may b t he s bject of

p t ent rig t s CEN an CENELEC s al not b held resp n ible for ident ifyin an or al s c p t ent

rig t s

The folowin dat es w ere fix ed:

– lat est date by whic the ENhast o b implement ed

at nat ional level bypublcat ion of an identical

nat ional st an ard or by en orsement

(do ) 2 10-12-01

– lat estdate bywhic the national st an ar ds conflct in

w it h t he EN hav e to b wit hdrawn

(dow) 2 13-0 -01

An e ZA has b en ad ed by CENELEC

_ _

Endorsement notice

The t ex t of t he Int ernat ional St an ard IEC 6 9 4-10:2 0 w as a proved by CENELEC as a Euro e n

St an ard w ithout an modificat ion

In t he oficial v ersion, for Biblogra h , t he folowin not es hav e to b ad ed for t he st an ard in icat ed:

IEC 6 9 4-7 NOT Harmo iz d a EN 6 9 4-7

IEC 618 9 NOT Harmo iz d a EN 618 9

Trang 5

- 3 - EN 6 9 4-10:2 10

Annex ZA

(normat iv e)

Normat ive reference t o int ernat ional publ cat ions

wit h t heir cor esponding European publ cat ions

The folow in referen ed doc ment s are in isp n a le for t he a plcat ion of t his doc men F r dat ed

referen es, only t he edit ion cit ed a ples For u dated referen es, t he lat est edition of t he referen ed

doc ment in lu in an amen ment s) a ples

NOT Wh n a int ern t io al p blc tio h s b e mo ifie b c ommo mo ific t io s, n ic t ed b (mo ), th relev ant EN/ HD

a ple

IEC 6 8 1 - Photovoltaicdev ices - Proced res for

t emp rat ure an iradian e corect ion t o

me s red I-V c aract eristic

-IEC 6 9 4-1 - Photovoltaicdev ices

-Part 1: Me s rement of phot ovolt aic c rent

-v olt age c aracterist ic

EN 6 9 4-1

-IEC 6 9 4-3 - Photovoltaicdev ices

-Part 3: Me s rement prin iples for t erest rial

photovoltaic (PV ) solar dev ices w it h referen e

sp ct ral iradian e dat a

EN 6 9 4-3

-IEC 6 9 4-8 - Photovoltaicdev ices

-Part 8: Me s rement of sp ct ral resp n e

of a photovoltaic (PV ) device

EN 6 9 4-8

-IEC 6 9 4-9 - Photovoltaicdev ices

-Part 9: Solar simulat or p rorman e

req irement s

EN 6 9 4-9

-IEC 61215 - Cr ystal ne si con t erest rial photovoltaic (PV )

mod les - Desig q alficat ion an typ

a proval

EN 61215

-IEC 616 6 - Thin-im t erest rial photovolt aic (PV )

mod les - Desig q alficat ion an typ

a proval

EN 616 6

-ISO/IEC 17 2 - General req irement s for t he comp t en e of

t est in an calbrat ion la or at ories

EN ISO/IEC 17 2

Trang 6

-– 2 – 6 9 4-10  IEC:2 0

CONTENTS

1 Sco e an o ject 5

2 Normative ref eren es 5

3 Ap aratu 6

4 Sample selection 6

5 Proced re for c r ent an voltage l ne rity test 6

5.1 Proced re in natural s nlg t .6

5.2 Proced re with a solar simulator 8

5.3 Proced re f or s ort-circ it l ne rity fom a solute sp ctral resp n ivity 9

6 Proced re for s ort-circ it c r ent l ne rity f om two-lamp method 9

6.1 Bac grou d .9

6.2 Ap aratu - Lig t sources A an B 9

6.3 General proced re 9

7 Line rity calc lation 10 7.1 Slo e l ne rity determination 10 7.2 Determination of the s ort circ it c r ent l ne rity u in the two lamp method 1

7.3 Line rity req irements 1

8 Re ort .1

Biblogra h 13

Trang 7

6 9 4-10  IEC:2 0 – 5 –

PHOTOVOLTAIC DEVICES –

Part 10: Methods of l nearity measurement

1 Scope a d object

This p rt of IEC 6 9 4 des rib s proced res u ed to determine the degre of lne rity of an

photovoltaic device p rameter with resp ct to a test p rameter It is primariy inten ed for u e

by calbration la oratories, mod le man facturers an s stem desig ers

Photovoltaic (PV) mod le an s stem p rf orman e evaluation , an p r orman e tran lation

f rom one set of temp rature an ir adian e con ition to another f req ently rely on the u e of

lne r eq ation (se IEC 6 8 1 an IEC 618 9) This stan ard lay down the l ne rity

req irements an test method to en ure that these lne r eq ation wi give satisfactory

res lts In irectly, these req irements dictate the ran e of the temp rature an ir adian e

varia les over whic the eq ation can b u ed

The method of me s rement des rib d in this stan ard a ply to al PV devices an are

inten ed to b car ied out on a sample or on a comp ra le device ofidentical tec nolog They

s ould b p r ormed prior to al me s rement an cor ection proced res that req ire a l ne r

device The methodolog u ed in this stan ard is simiar to that sp cified in IEC 6 8 1 in whic

a l ne r (straig t-l ne) fu ction is f ited to a set of data p ints u in a le st-s uares fit

calc lation routine The variation of the data f rom this fu ction is also calc lated, an the

def i ition of lne rity is expres ed as an al owa le variation p rcentage

A device is con idered lne r when it me ts the req irements of 7.3

General proced res for determinin the degre of l ne rity for these an an other p r orman e

p rameter are des rib d in Clau es 5 an 6

2 Normativ ref ere ces

The f olowin referen ed doc ments are in isp n a le for the a plcation of this doc ment For

dated referen es, only the edition cited a pl es For u dated ref eren es, the latest edition of

the ref eren ed doc ment (in lu in an amen ments) a ples

IEC 6 8 1, P hoto oltaic de ic s – P ro edures for temp rature a d iradia c c re tio s to

me sured I -V c ara teristics

IEC 6 9 4-1, P hoto oltaic de ic s – P art 1: Me sureme t of p oto oltaic c re tv lta e

c ara teristics

IEC 6 9 4-3, P hotov ltaic de ic s – P art 3: Me sureme t prin iples forterestrial p oto oltaic

(P V) solar de ic s with refere c sp ctral iradia c data

IEC 6 9 4-8, P hoto oltaic de ic s – P art 8: Me sureme t of sp ctral resp nse of a

p oto oltaic (P V) de ic

IEC 6 9 4-9, P hoto oltaic de ic s – P art 9: Solar simulator p rorma c re uireme ts

IEC 61215, Crystal n si c n terestrial p oto oltaic (P V) modules – Desig q alfic tio a d

Trang 8

– 6 – 6 9 4-10  IEC:2 0

IEC 616 6, Thin-fim ter estrial p oto oltaic (P V) modules – Desig q alfic tio a d ty e

a pro al

ISO/IEC 17 2 , Ge eral re uireme ts for th c mp ten e of testin a d c lbratio

la oratories

3 Apparatus

a) Eq ipment neces ary to me s re an I-V c rve (se IEC 6 9 4-1)

b) An eq ipment neces ary to c an e the ir adian e over the ran e of interest without

af fectin the relative sp ctral ir adian e distribution an the sp tial u if ormity, s c as

mes f ilters or neutral den ity f ilters

NOT Th e uipme t a d pro e ure u e to c a g th ira ia c are to b v rifie with a ra iometer Th

c a g in relativ s e tral ira ia c distrib tio s o ld n t re ult in more th n 0,5 % c a g in th s

ort-circ it c re t of th d vic (s e IEC 6 9 4-7 a d IEC 6 9 4-8) Me h fiters are b le e to b th b st

meth d f or larg s ra e

c) An eq ipment neces ary to c an e the temp rature of the test sp cimen overthe ran e of

interest

d) A me n for control n the temp rature of the test sp cimen an referen e device, or a

remova le s ade

e) Eq ipment for me s rin the sp ctral resp n e of the test sp cimen (or a re resentative

sample eq ivalent to the test sp cimen) in ac ordan e with IEC 6 9 4-8 to a re e ta i ty

of± 2 % of the re din

NOT IEC 6 9 4-7 pro id smeth d f or th c mp tatio of s e tral mismatc eror intro u e in th te tin

of p oto oltaic d vic s, a d IEC 6 9 4-8 pro id s g id n e f or s e tral me s reme t

4 Sample selection

This proced re s al b a pled to a ful -sized test sp cimen if p s ible If this is not p s ible, a

smal sample eq ivalent in con tru tion an materials s ould b u ed

5 Proc dure f or cur ent and voltage l nearity test

There are thre ac e ta le proced res for p rormin the lne rity test of s ort-circ it c r ent

with resp ct to temp rature an ir adian e There are two ac e ta le proced res for

p r ormin the lne rity test of o en-circ it voltage with resp ct to temp rature an ir adian e

5.1 Proc d re in natural s nl ght

5.1.1 Me s rement in natural s nl g t s al only b made when:

– The total ir adian e is at le st as hig as the up er l mit of the ran e of interest

– The ir adian e variation cau ed by s ort-term os i ation (clou s, haze, or smoke) is

les than ± 2 % of the total ir adian e as me s red by the referen e device

– The win sp ed is les than 2 m⋅s

1

5.1.2 Mou t the referen e device co-planar with the testsp cimen so that b th are normal to

the direct solar b am within ± 1 Con ect to the neces ary in trumentation

NOT Th me s reme ts d s rib d in th f olowin s b la s s s o ld b ma e a e p ditio sly a p s ible

within a f ew h urs o th s me d y to minimiz th eff ect of c a g s in th s e tral c n itio s If n t, s e tral

c r e tio s ma b re uire

5.1.3 If the test sp cimen an ref eren e device are eq ip ed with temp rature controls, set

the controls at the desired level If temp rature controls are not u ed, s ade the test sp cimen

Trang 9

6 9 4-10  IEC:2 0 – 7 –

ref eren e device s ould also sta i ze within ± 1 °C of its eq i brium temp rature b fore

proce din

5.1.4 Remove the s ade (if u ed) an immediately take simultane u re din s of the test

p rameter X

i

, the test sp cimen device p rameter Y

i

an the temp rature an s ort-circ it

c r ent of the referen e device

5.1.5 The ir adian e G

o

s al b calc lated f om the me s red s ort circ it c r ent (I

s ) of

the PV referen e device, an its calbration value at Stan ard Test Con ition , STC (I

rc ) A

cor ection s ould b a pl ed to ac ou t f or the temp rature of the ref eren e device T

m

u in

the c r ent-temp rature co f ficient of the referen e device α

rc

0 0 1

m rc

rc s

o

×

×

I I

5.1.6 If the test p rameter b in varied is the ir adian e, red ce the ir adian e on the test

sp cimen to a k own f raction k

i without aff ectin the sp tial u if ormity or the sp ctral

ir adian e distribution There are variou method by whic to ac ompls this:

a) Usin cal brated, u iform den ity mes f ilters If this method is selected, the ref eren e

device s ould remain u covered by the f ilter d rin the o eration to ena le the in ident

ir adian e to b me s red In this case, k

i

is the fi ter calbration p rameter (f action of l g t

tran mit ed)

b) Usin u cal brated, u iform den ity mes f ilters If this method is selected, the ref eren e

device s ould also b covered by the fi ter d rin the test In this case, k

i

s the ratio of the

ref eren e device s ort-circ it c r ent (I

s ) to its cal bration value (I

rc )

NOT 1 Th ma imum f ilter me h o e in dime sio s o ld b le s th n 1 % of th minimum ln ar

dime sio of th refere c d vic a d th te t s e ime , or a v ria le eror ma o c r d e to p sitio in

c) By control n the an le of in iden e If this method is selected, the ref eren e device s ould

have the same ref lective pro erties as the test sp cimen, an s ould b mou ted co-planar

with the test sp cimen within ± 1 In this case, k

i

is the ratio of the referen e device s

ort-circ it c r ent (I

s ) to its cal bration value (I

rc )

NOT 2 For c ls with thic metal z tio , th rotatio a is s o ld b p ralel to th dire tio ofth metalz d

ln s in ord r to minimiz or elmin te s a owin

5.1.7 Calc late the ir adian e level on the test sp cimen G

i

as f olows:

G

i

= k

i

×G

o

where G

o

is determined by the method des rib d in 5.1.5

5.1.8 If the test p rameter b in varied is the temp rature, adju t the temp rature by me n

of a controler or alternately exp sin an s adin the test sp cimen as req ired to ac ieve

an maintain the desired temp rature Alternately, the test sp cimen may b al owed to

warm-up natural ywith the data recordin proced re of 5.1.4 p rf ormed p riodical y d rin the

warm-up

5.1.9 En ure that the test sp cimen an referen e device temp ratures are sta i zed an

remain con tant within ± 1 °C an that the ir adian e as me s red by the ref eren e device

remain con tant within ± 2 % d rin the data recordin p riod

5.1.10 Re e t ste s 5.1.4 throu h 5.1.9 The value of the test p rameter selected s al b

s c that the ran e of interest is sp n ed in at le st four a proximately eq al in rements A

Trang 10

– 8 – 6 9 4-10  IEC:2 0

5.2 Proc d re with a solar simulator

NOT Emis io lamp s c a x n n s o ld b e alu te b fore u e As th b n g p ofth te t d vic v rie

d e to temp rature c a g s, it c n p s thro g v rio s emis io ln s in th lamp s e trum a d giv ris to s ifts

in p rorma c Ba e o th ln arity of s e tral re p n e a d th lamp s e trum th ma nitu e ofthisef fe tc n

b c lc late b p rormin a mismatc c re tio a a f un tio of temp rature

5.2.1 Mou t the test sp cimen an the ref eren e device co-planar in the test plane of the

simulator so that b th are normal to the center l ne of the b am within ± 2° Con ect to the

neces ary in trumentation

5.2.2 If the test sp cimen an ref eren e device are eq ip ed with temp rature controls, set

the controls at the desired level If temp rature controls are not u ed, alow the test sp cimen

an ref eren e device to sta i ze within ± 1 °C of the ro m air temp rature

5.2.3 Set the ir adian e at the test plane to the up er l mit of the ran e of interest u in the

referen e device me s red c r ent (I

s ), an its cal bration value at STC (I

rc )

5.2.4 Con u t the test an take simultane u re din s of the test p rameter X

i , the test

sp cimen device p rameter Y

i

an the temp rature an s ort-circ it c r ent of the ref eren e

device

5.2.5 The ir adian e G

o

s al b calc lated f rom the me s red s ort circ it c r ent (I

s ) of

the PV ref eren e device, an its calbration value at STC (I

rc ) A cor ection s ould b a pled

to ac ou t for the temp rature of the referen e device T

m , u in the c r ent-temp rature

co f ficient of the ref eren e device α

rc

0 0 1

m rc

rc s

o

×

×

I I

5.2.6 If the test p rameter b in varied is the ir adian e, red ce the ir adian e on the test

sp cimen to a k own f raction k

i without aff ectin the sp tial u if ormity or the sp ctral

ir adian e distribution The variou method by whic to ac ompls this are:

a) by in re sin the distan e b twe n the test plane an the lamp With the ref eren e device

maintained in the same plane as the test sp cimen, k

i

s the ratio of the referen e device

s ort-circ it c r ent (I

s ) to its cal bration value (I

rc );

b) by the u e of an o tical len In this case, k

i

is the ratio of the ref eren e device s ort-circ it

c r ent (I

s

) to its cal bration value (I

rc ) Care s ould b exercised to en ure that the len

do s not sig if i antly c an e the relative sp ctral ir adian e in the wavelen th ran e in

whic the test an ref eren e sp cimen are resp n ive;

c) by control n the an le of in iden e If this method is selected, the distan e b twe n the

lamp source an the sp cimen s al b large to l mit the ir adian e c an e acros the ti ted

s r ace to 0,5 % or les Also, if this method is selected, the radiant b am s al b

col mated, the referen e device s ould have the same ref lective pro erties as the test

sp cimen, an s ould b mou ted co-planar with the test sp cimen In this case, k

i

is the

ratio of the ref eren e device s ort-circ it c r ent (I

s ) to its cal bration value (I

rc );

d) cal brated, u iform den ity mes fiters If this method is selected, the ref eren e device

s ould remain u covered by the f ilter d rin the o eration to ena le the in ident ir adian e

to b me s red In this case, k

i

is the f ilter cal bration p rameter (f action of l g t

tran mit ed);

e) u calbrated, u if orm den ity mes fiters If this method is selected, the referen e device

s ould also b covered by the f ilter d rin the test In this case, k

i

is the ratio of the

referen e device s ort-circ it c r ent (I

s ) to its cal bration value (I

rc )

NOT Th ma imum f ilter me h o e in dime sio s o ld b le s th n 1 %ofth minimum ln ar dime sio

of th ref ere c d vic a d th te t s e ime , or a v ria le eror ma o c r d e to p sitio in

Ngày đăng: 14/04/2023, 14:39

TÀI LIỆU CÙNG NGƯỜI DÙNG

TÀI LIỆU LIÊN QUAN