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Tiêu đề Explosive Atmospheres – Part 32-1: Electrostatic Hazards, Guidance
Trường học Geneva University
Chuyên ngành Electrical and Electronics Engineering
Thể loại Technical Standard
Năm xuất bản 2017
Thành phố Geneva
Định dạng
Số trang 362
Dung lượng 6,27 MB

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Also k nown as th Inter natio al Electr otech ical Voca ular y IE o ln... 13 B.1 In e div dis harg s in olvin in ulatin s ld materials.. 13 B.2.2 Calc late maximum safe flow v lo itie f

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Edition 1.1 2 17-0

Explosiv e atmospher es –

Part 3 -1: Ele trostatic hazards, guidanc

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1 Sc p 14

2 Normativ refere c s 14

3 Terms an d finitio s 17

4 Nome clature 2

5 Ge eral 21

6 Static ele tricity in s l d materials 2

6.1 Ge eral c n id ratio s 2

6.2 Th u e of c n u tiv or dis ipativ materials in plac of in ulatin o e 2

6.2.1 Ge eral c n id ratio s 2

6.2.2 Dis ipativ s ld materials 2

6.2.3 Earthin of c n u tiv an dis ipativ items 2

6.3 Pre autio s re uire wh n u in in ulatin s ld materials 2

6.3.1 Ge eral 2

6.3.2 Re trictio s o th siz of c arg able in ulatin s rfac s 2

6.3.3 Earth d metal me h s 2

6.3.4 In ulatin c atin s o earth d c n u tiv s rfac s 2

6.3.5 Co d ctiv or dis ipativ c atin s o in ulatin materials 2

6.3.6 Static dis ipativ ag nts 3

6.3.7 Humidificatio 3

6.3.8 Io isatio / Charg Ne tral satio 3

6.3.9 Meth d to d termin th in e divity of dis harg s 31

6.4 Co v y r b lts an tran mis io b lts 3

6.4.1 Ge eral 3

6.4.2 Co v y r b lts 3

6.4.3 Tran mis io b lts 3

7 Static ele tricity in lq id 3

7.1 Ge eral c n id ratio s 3

7.1.1 Oc ur e c of flammable atmo p ere 3

7.1.2 Ig itio s n itivity an lmitatio s to th s o e of ad ic 3

7.1.3 Chargin me hanisms 3

7.1.4 Charg ac umulatio an c n u tivity clas ificatio s 3

7.1.5 In e div dis harg s pro u e d rin l q id han ln o eratio s 3

7.2 Summary of pre autio s again t ig itio hazard d rin lq id han l n o eratio s 3

7.2.1 Earthin an av idan e of is late c n u tors 3

7.2.2 Re trictin c arg g n ratio 3

7.2.3 Av idan e of a flammable atmo p ere 3

7.2.4 Promotin c arg dis ipatio 3

7.3 T n s an Co tain rs 3

7.3.1 Ge eral 3

7.3.2 Co d ctiv tan s an c ntain rs 4

7.3.3 T n s an c ntain rs mad e tirely of dis ipativ material 5

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7.6 Gau in an sampln in tan s 6

7.6.1 Ge eral 6

7.6.2 Pre autio s d rin gau in an sampl n 6

7.7 Pip s an h s as embl e for l q id 61

7.7.1 Ge eral 61

7.7.2 Pip s 61

7.7.3 Ho e an h s as embl e 6

7.8 Sp cial fi in pro e ure 7

7.8.1 Aircraf fu l n 7

7.8.2 Road tan er d l v rie 71

7.8.3 Retai fi in statio s 7

7.8.4 Mo i e or temp rary l q id han ln e uipme t 7

7.9 Plant pro e s s (ble din , stir in , mixin , cry tal satio an stir e reactors) 7

7.9.1 Ge eral 7

7.9.2 Earthin 7

7.9.3 In-l n ble din 7

7.9.4 Ble din in v s els or tan s 7

7.9.5 Jet mixin 7

7.9.6 Hig s e d mixin 7

7.10 Sprayin l q id an tan cleanin 7

7.10.1 Ge eral 7

7.10.2 T n cleanin with low or me ium pre s re water jets (u to ab ut 12 bar) 7

7.10.3 T n cleanin with low c n u tivity l q id 7

7.10.4 T n cleanin with hig pre s re water or s lv nt jets (ab v 12 bar) 7

7.10.5 Steam cleanin tan s 7

7.10.6 Water d lu e s stems 8

7.1 Glas s stems 8

7.1 1 Ge eral 8

7.1 2 Pre autio s to b tak n for low c n u tivity l q id 8

8 Static ele tricity in gas s 81

8.1 Ge eral 81

8.2 Grit blastin 81

8.3 Fire e tin uis ers 8

8.4 In rtin 8

8.5 Steam cleanin 8

8.6 Ac id ntal leakag of c mpre s d gas 8

8.7 Sprayin of flammable paints an p wd rs 8

8.7.1 Ge eral 8

8.7.2 Earthin 8

8.7.3 Plastic s ray cabin ts 8

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9.1 Ge eral 8

9.2 Dis harg s, o c r e c an in e divity 8

9.3 Pro e ural meas re 8

9.3.1 Ge eral 8

9.3.2 Humidificatio 8

9.3.3 Ho e for p e matic tran fer 8

9.3.4 Io isatio 8

9.4 Bulk materials in th ab e c of flammable gas s an vap urs 8

9.4.1 Ge eral 8

9.4.2 Eq ipme t an o je ts mad of c n u tiv or dis ipativ materials 8

9.4.3 Eq ipme t an o je ts mad of in ulatin materials 8

9.4.4 Du t s parators 8

9.4.5 Sio an Co tain rs 8

9.5 Ad itio al re uireme ts for b lk material in th pre e c of flammable gas s an vap urs 9

9.5.1 Ge eral 9

9.5.2 Meas re for re istivity greater e ual 10 MΩ m 9

9.5.3 Meas re for re istivity le s than 10 MΩ m 9

9.5.4 Fi in of b lk material into a c ntain r 9

9.6 Fle ible interme iate b lk c ntain rs (FIBC) 9

9.6.1 Ge eral 9

9.6.2 Ad itio al pre autio s wh n u in FIBC 9

10 Static ele tricity wh n han l n e plo iv s an ele tro-e plo iv d vic s 9

10.1 Ex lo iv s man facture, han l n an storag 9

10.1.1 Ge eral 9

10.1.2 First d gre prote tio 9

10.1.3 Interme iate prote tio 9

10.1.4 Se o d d gre prote tio 9

10.2 Han l n of ele tro-e plo iv d vic s 10

10.2.1 Ge eral 10

10.2.2 Earthin 10

10.2.3 Pre autio s d rin storag an is u 101

10.2.4 Pre autio s d rin pre aratio for u e 101

1 Static ele tricity o p o le 101

1 1 Ge eral c n id ratio s 101

1 2 Static dis ipativ flo rs 10

1 3 Dis ipativ an c n u tiv fo twear 10

1 4 Su pleme tary d vic s for earthin of p o le 10

1 5 Clothin 10

1 6 Glo e 10

1 7 Oth r Items 10

12 Ele tro tatic s o k 10

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13.2.2 Practical criteria 1 0

13.3 Earthin re uireme ts in practical s stems 1 2

13.3.1 Al-metal s stems 1 2

13.3.2 Metal plant with in ulatin parts 1 3

13.3.3 In ulatin materials 1 4

13.3.4 Co d ctiv an dis ipativ materials 1 5

13.3.5 Earthin via intrin ic safety circ its 1 5

An e A (informativ ) Fu dame tals of static ele tricity 121

A.1 Ele tro tatic c argin 121

A.1.1 Intro u tio 121

A.1.2 Co tact c argin 121

A.1.3 Co tact c argin of lq id 121

A.1.4 Charg g n ratio o lq id flowin in pip s 12

A.1.5 Charg g n ratio in fiters 12

A.1.6 Charg g n ratio d rin stir in an mixin of lq id 12

A.1.7 Setl n p te tials 12

Trang 10

A.3.1 Intro u tio 12

A.3.2 Spark 12

A.3.3 Coro a 13

A.3.4 Bru h dis harg s 13

A.3.5 Pro agatin bru h dis harg s 131

A.3.6 Lig tnin l k dis harg s 131

A.3.7 Co e dis harg s 13

A.4 Meas reme ts for ris as e sme t 13

An e B (informativ ) Ele tro tatic dis harg s in s e ific situatio s 13

B.1 In e div dis harg s in olvin in ulatin s ld materials 13

B.1.1 Ge eral 13

B.1.3 Bru h dis harg s from in ulatin s l d materials 13

B.1.4 Pro agatin bru h dis harg s from in ulatin s l d materials 13

B.2 In e div dis harg s pro u e d rin l q id han ln 13

B.2.1 Ge eral 13

B.2.2 Calc late maximum safe flow v lo itie for fi in me ium

-siz d v rtical axis storag tan s 13

B.3 In e div dis harg s pro u e d rin p wd r han l n an storag 13

B.3.6 Spark dis harg s in p wd r pro e s s 13

B.3.7 Bru h dis harg s in p wd r pro e s s 13

B.3.8 Coro a dis harg s in p wd r pro e s s 13

B.3.9 Pro agatin bru h dis harg s in p wd r pro e s s 13

An e C (informativ ) Flammabi ty pro ertie of s b tan e 14

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G.9.4 Te t sample 16

G.9.5 Pro e ure for mo eable items 16

G.9.6 Pro e ure for in tal e items 161

Fig re 4 – Difere c b twe n earthin an b n in 10

Fig re 5 – Hazard u earth d c n u tor in c ntact with a flowin in ulator 1 4

Fig re A.1 – Eq ivale t ele trical circ it for an ele tro tatical y c arg d c n u tor 12

Trang 13

Fig re G.3 – Meas rin c l for lq id c n u tivity 15

Fig re G.4 – Ig itio pro e 16

Fig re G.5 – Perforate plate of ig itio pro e 16

Fig re G.6 – Example of an ar an eme t for meas reme t of c arg d cay 17

Fig re G.7 – Ele tro e for meas rin breakthro g v ltag of s e ts 17

T ble 1 – Bo n ary lmits at (2 ± 2) °C an (2 ± 5) % RH for th c aracterisatio of

s ld materials an e ample for th clas ificatio of o je ts 2

T ble 2 – Maximum alowe is late capacitan e in Zo e with e plo iv atmo p ere 2

T ble 3 – Re trictio o siz of in ulatin s ld materials in hazard u areas 2

T ble 4 – Maximum ac e table tran fer e c arg 3

T ble 5 – Re uireme ts for c n e or b lts 3

T ble 6 – Re uireme ts for tran mis io b lts 3

T ble 7 – Co d ctivitie an relaxatio time of s me lq id 3

T ble 8 – Pre autio s for fi in larg c n u tiv tan s with low c n u tivity l q id 4

T ble 9 – Fi in rate l mits for fi in me ium-siz d v rtical-axis tan s thro g s h d le 4 pip s 4

T ble 10 – Velo ity an fi in rate l mits for loadin low c n u tivity lq id into s ort (N=1), fix d h riz ntal axis tan s via s h d le 4 pip s 4

T ble 1 – Ve icle an c mpartme ts s itable for hig -s e d loadin for ADR c mplant v hicle 5

T ble 12 – Influ n e of th s lp ur c nte t o mid le disti ate v lmits for road tan ers 51

T ble 13 – Velo ity an fi in rate l mits for road tan ers bas d o s h d le 4 pip s; rate for h s s wi b simiar 51

T ble 14 – Velo ity an fi in rate l mits for loadin rai tan ers 5

T ble 15 – Clas ificatio of e d- o-e d h s re istan e for c ntrol of hazard from static ele tricity an stray c r e t 6

T ble 16 – ISO 8 31 clas ificatio of h s grad s 6

T ble 17 – Hy rid grad s of h s s an h s as emble 6

T ble 18 – Ho e s le tio T ble for flammable l q id s rvic 6

T ble 19 – Us of th difere t ty e of FIBC 9

T ble 2 – In er l n rs an FIBC: c mbinatio s that are p rmis ible an n t p rmis ible in hazard u atmo p ere 9

T ble 21 – Determinatio of re uireme t for ele tro tatic dis ipativ prote tiv clothin

an oth r items of p rs nal prote tiv e uipme t 10

T ble 2 – Summary of maximum earthin re istan e for th c ntrol of static

ele tricity in hazard u areas 1 1

T ble A.1 – Charg b i d u o p wd rs 12

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EXPLOSIVE ATMOSPHERES –

Part 32-1: Electrostatic hazards, guidance

FOREWORD

1) Th Intern tio al Electrotech ical Commis io (IEC) is a worldwid org nizatio for sta d rdizatio comprisin

al n tio al electrotech ical commite s (IEC Natio al Commite s) Th o ject of IEC is to promote

intern tio al co-o eratio o al q estio s co cernin sta d rdizatio in th electrical a d electro ic fields To

this e d a d in a ditio to oth r activities, IEC p blsh s Intern tio al Sta d rds, Tech ical Sp cificatio s,

Tech ical Re orts, Pu lcly Av ia le Sp cificatio s (P S) a d Guid s (h re fer refere to as “IEC

Pu lcatio (s) Th ir pre aratio is e truste to tech ical commite s; a y IEC Natio al Commite intereste

in th su ject d alt with may p rticip te in this pre aratory work Intern tio al g v rnme tal a d n

n-g v rnme tal org nizatio s laisin with th IEC also p rticip te in this pre aratio IEC cola orates closely

with th Intern tio al Org nizatio for Sta d rdizatio (ISO) in ac ord nce with co ditio s d termin d by

a re me t b twe n th two org nizatio s

2) Th formal d cisio s or a re me ts of IEC o tech ical maters expres , as n arly as p s ible, a intern tio al

co se sus of o inio o th rele a t su jects since e ch tech ical commite h s re rese tatio from al

intereste IEC Natio al Commite s

3) IEC Pu lcatio s h v th form of recomme d tio s for intern tio al use a d are ac e te by IEC Natio al

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Pu lcatio s is ac urate, IEC ca n t b h ld resp nsible for th way in which th y are use or for a y

misinterpretatio by a y e d user

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th later

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DISCLAIMER

This Consol dated versio is n t an of icial IEC Standard an ha be n prepared for

us r co venienc Only the cur ent versions of the stan ard an its amendment s)

are to be co sidered the of icial d cuments

This Co sol dated versio of IEC TS 6 079-3 -1 be rs the edition n mber 1.1 It

co sists of the first editio (2 13-0 ) [d cuments 31/10 3/DTS an 31/1076/RVC] an its

amen ment 1 (2 17-0 ) [documents 31/12 7/DT and 31/12 3/RVC] The te h ic l

co tent is identic l to the ba e edition an its amen ment

In this Redl ne version, a vertic l l ne in the margin sh ws where the te h ic l co tent

is mo ified by amen ment 1 Ad itio s are in gre n text, deletions are in strikethro gh

red text A s parate Final versio with al change a c pted is avai able in this

p bl c tion

Trang 16

• th s bje t is sti u d r te h ical d v lo me t or wh re, for an oth r reas n, th re is th

future b t n imme iate p s ibi ty of an agre me t o an Internatio al Stan ard

Te h ical s e ificatio s are s bje t to re iew within thre y ars of p blcatio to d cid

wh th r th y can b tran forme into Internatio al Stan ard

IEC/TS 6 0 9-3 -1, whic is a te h ical s e ificatio , has b e pre are b IEC Te h ical

Commite 31: Eq ipme t for e plo iv atmo p ere , an IEC Te h ical Commite 101:

Ele tro tatic

This p blcatio has b e drafe in ac ordan e with th ISO/IEC Dire tiv s, Part 2

A lst of al parts of th IEC 6 0 9 s rie , u d r th g n ral title Ex lo sive atmosp he re s, can

b fo n o th IEC we site

Th c mmite has d cid d that th c nte ts of th bas p blcatio an its ame dme t wi

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IMPORTANT – The 'colo r inside' log o the cover page of this p bl c tio in ic te

that it contains colours which are co sidered to be us ful for the cor e t

u derstandin of its contents Us rs sh uld therefore print this d cument usin a

colo r printer

A bi n ual v rsio of this p blcatio may b is u d at a later date

Trang 17

• from German : TRBS 215 :2 0 , Preve ting risks ofignitio due to ele ctrostatic c arges,

• from Sh l Internatio al Petrole m: Static ele ctric ity – Te h ic l a d safety aspe c ts,

• from th US: NFPA 7 , R e comme nde d Prac tic o Static Ele ctricity (2 0 7),

• from Japan: JNIOSH TR4 , R e comme datio ns for Requ ireme ts fo r Avo iding Ele c trostatic

Ha ards in Industry (20 0 7),

• from ASTM, EUROPIA, IEC, Internatio al c amb r of s ip in , ISO etc

It giv s th b st avai able ac e te state of th art g idan e for th av idan e of hazard d e

to static ele tricity

This d c me t is mainly write for d sig ers an u ers of pro e s s an e uipme t,

man facturers an te t h u e It can als b u e b s p l ers of e uipme t (e.g mac in s)

an flo rin or ap arel wh n n pro u t famiy or d dicate pro u t stan ard e ists or wh re

th e istin stan ard d e n t d al with ele tro tatic hazard

A s c n part, IEC 6 0 9-3 -2, Electro static Ha ards, Te sts, is u d r d v lo me t

Trang 18

1 Scope

This part of IEC 6 0 9 giv s g idan e ab ut th e uipme t, pro u t an pro e s pro ertie

n c s ary to av id ig itio an ele tro tatic s o k hazard arisin from static ele tricity as

wel as th o eratio al re uireme ts n e e to e s re safe u e of th e uipme t, pro u t or

pro e s It can b u e in a ris as e sme t of ele tro tatic hazard or for th pre aratio of

pro u t fami y or d dicate pro u t stan ard for ele trical or n n-ele trical mac in s or

e uipme t

Th hazard as o iate with static ele tricity in in u trial pro e s s an e viro me ts that

mo t c mmo ly giv pro lems are c n id re Th s pro e s s in lu e th han ln of

s ld , lq id , p wd rs, gas s, s ray an e plo iv s In eac cas , th s urc an nature of

th ele tro tatic hazard are id ntifie an s e ific re omme datio s are giv n for d aln with

th m

Th p rp s of this d c me t is to pro id stan ard re omme datio s for th c ntrol of static

ele tricity, s c as earthin of c n u tors, re u tio of c argin an re trictio of c arg able

areas of in ulators In s me cas s static ele tricity play an inte ral part of a pro e s, e.g

ele tro tatic c atin , b t ofe it is an u welc me sid efe t an it is with th lat er that this

g idan e is c n ern d If th stan ard re omme datio s giv n in this d c me t are fulfi e it

can b e p cte that th ris of hazard u ele tro tatic dis harg s in an e plo iv

atmo p ere is at an ac e tably low le el

If th re uireme ts of this d c me t can ot b fulfi e , alternativ ap roac e can b ap l e

u d r th c n itio that at least th same le el of safety is ac ie e

Basic informatio ab ut th g n ratio of u d sirable static ele tricity in s l d , lq id ,

gas s, e plo iv s, an als o p o le, to eth r with d s riptio s of h w th c arg s

IEC/TR 613 0-1

This Te h ical Sp cificatio is n t ap l cable to th hazard of static ele tricity relatin to

lg tnin or to damag to ele tro ic c mp n nts

This Te h ical Sp cificatio is n t inte d d to s p rs d stan ard that c v r s e ific

pro u ts an in u trial situatio s

2 Normative referenc s

Th folowin d c me ts, in wh le or in part, are n rmativ ly refere c d in this d c me t an

are in is e sable for its ap lcatio For date refere c s, o ly th e itio cite ap le For

ame dme ts) ap l e

IEC 6 0 9-0:2 1 , Ex losive atmo sp ere s – Part 0: Equ ipme t – Ge ne ral re qu ire me ts

IEC 6 0 9-10-1, Ex lo sive atmosp he res – Part 10-1: C las ificatio n o f are s – Exp losive gas

atmosp e re s

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IEC 6 0 9-2 -1, Exp lo sive atmo sp e res – Part 2 -1: Mate rial c ara teristics fo r g as a d

va our c las ific atio n – Te st meth ds a d data

IEC 6 0 9-3 -2

1

:2 15, Ex lo sive atmo sp ere s – Part 32-2: Ele c tro static h z rds – Te sts

IEC 6 0 3, Meth ods of te st fo r volume re sistivity a d surfac e re sistivity o f sold ele ctric al

insu lating mate rials

IEC 6 16 , Meth ds of te st fo r th dete rmin tio of th insu latio resista c e of sold

insu lating materials

IEC 613 0-2-3, Ele c trostatics – Part 2-3: Me th ds o f te st fo r dete rmining th re sista c e a d

re sistivity ofsold pla ar mate rials used to avoid ele ctrostatic c arg e a cu mu latio

IEC 613 0-4-1, Ele tro statics – Part 4-1: Sta dard test me tho ds fo r sp cific a plc atio s –

Ele c tric al re sistan c e offlo or c o ve rings a d instale d floo rs

IEC 613 0-4-3, Ele tro statics – Part 4-3: Sta dard test me tho ds fo r sp cific a plc atio s –

Foo twe r

IEC 613 0-4-4:2 12, Ele tro statics – Part 4-4: Sta dard te st meth ds fo rsp e cific a p licatio s

– Ele tro static clas ific tio n of fle xib le inte rmediate b ulk containe rs (FIBC)

ISO 2 4, Co ve yo r belts – Ele ctrical c o nductivity – Sp e c ific tio a d te st meth d

ISO 6 9 , Petroleum p ro ducts – Aviatio a d disti ate fu e ls – De termin tio o f ele ctric al

co nductivity

ISO 8 31, Ru bb e r a d plastics ho se s a d ho se as e mb lie s – De termin tio of ele trical

re sista c e

ISO 9 6 , Belt drive s; ele ctric al conductivity of a tistatic e dle ss sy c hro nous be lts;

c arac teristics a d te st meth d

ISO 1210 -1, Safety o f mac hine ry – Basic c ncepts, ge e ral p rinc iple s fo r de sign – Part 1:

Basic te rmin logy, me th dology

ISO 16 9 , Tyre s – Ele tric al re sista c – Te st me tho d fo r me suring ele c trical re sista ce of

tyres o a te st rig

ISO 21 7 , Light conve yor be lts – De te rmin tio o f ele ctrical re sista ce s

ISO 21 7 , Lig ht c o nve o r b elts – De termin tio of th ele c trostatic field g e nerated by a

running lght c o nve yo r b elt

ISO 21 8 -1, Light conve yo r b elts – Part 1: Princ ip al c ara te ristics a d ap plc atio ns

—————————

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ASTM D4 0 -9 , Sta dard Te st Meth d fo r Ele c tric al C onductivity o fLiqu id Hydro c arb ons by

Pre c isio Mete r

ASTM E5 2-8 , Sta dard te st meth d for minimu m ignitio e ergy a d qu e nching dista c e in

gase us mixture s

ASTM E2 19-0 , Sta dard te st me tho d for minimum ignitio e e rgy of a dust clou d in air

ASTM F15 , Sta dard Test Me tho d fo r Electric l R e sista c of C onduc tive a d Static

Dis ip tive Resi e t Flo ring

ASTM F19 1, Sta dard Te st Meth d fo r Ele c tric al Resista c e of Tire s Unde r L ad On th

Te st Be nc h

BS 5 5 : Code o f prac tic e fo r contro l o f u nde sira le static ele c tricity

Part 1: Ge e ral c nside ratio ns

Part 2: R e comme datio s fo r p rticu lar industrial situ atio ns

BS 7 0 , Meth ds fo r me sureme nts in electro statics – Part 2 Te st me tho ds

DIN 51412-1, Te sting of pe trole u m p ro ducts; de te rmin tio of th ele c tric al c o nductivity,

lab o ratory me tho d

DIN 51412-2, Te sting of p etro leu m p roduc ts; de termin tio of th ele ctrical c o nductivity; field

meth d

EN 10 1, R e si e t flo or c ve rings – De termin tio o f th ele c tric l re sista c

EN 1 4 -3, Pro te cting clo the s – Ele c tro static p rop e rtie s – Part 3: Test meth d for me suring

th c harg e dis ip atio

EN 1 4 -5, Protective c lothing – Ele c tro static p ro pe rties – Part 5: Material p ero rma c e a d

de sig n requ ireme ts

EN 13 0, Rub b er a d plastic ho se s a d ho se as emb lie s fo r me sured fu el disp nsing

systems – Sp cific atio n

EN 13 1, R u bb er ho se s a d h se as emb lie s for aviatio fuel h ndlng – Sp e c ific tio

EN 13 6 -1, No -e le c tric l equipme t fo r p te tialy flamma le atmo sp ere s – Part 1: Basic

principle s a d ge neral requ ireme ts

EN 1412 , Undergrou nd pip work fo r p trol fi ing statio s

EN 14 7 , C o nve o r belts fo r use in u nde rgrou nd instalatio s – Ele tric al a d flammab ilty

safe ty re qu ire me ts

Inte rn tio nal Safe ty Guide fo r Oi Ta ke rs a d Termin ls (ISGOTT), fifh e itio , Internatio al

c amb r of s ip in , 2 0

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© IEC 2 17

JNIOSH TR 4 , Rec mme datio s fo r Requ ireme ts fo r Avoiding Ele c trostatic Ha ards in

Industry

NFPA 7 , R e comme nde d p ra tice o static ele ctricity

SAE J16 5, Su rfa e ve icle re comme nde d p ra tice – Fuel systems a d C o mpo ne ts –

Ele c tro static Charge Mitigatio

3 Terms and definitions

For th p rp s s of this d c me t th folowin terms an d finitio s ap ly:

3.1

antistatic

c n u tiv or dis ipativ

Note 1 to e try: Use to d s rib a material th t is inca a le of retainin a sig ifica t electrostatic ch rg wh n

in co tact with e rth In this co text th word is commo ly use to d s rib a typ of fo twe r a d a tistatic

a ditiv s (A As) for use with lq ids

Note 2 to e try: Prefere term is co d ctiv or dis ip tiv d p n in o which is corect

3.2

co d ctive

havin a re istivity or re istan e b low th dis ipativ ran e (s e 3.7) al owin stray c r e t

arc an ele tro tatic s o k to o c r

Note 1 to e try: Co d ctiv materials or o jects are n ith r dis ip tiv n r insulatin a d are inca a le of

retainin a sig ifica t electrostatic ch rg wh n in co tact with e rth

Note 2 to e try: Bo n ary lmits for th co d ctiv ra g are giv n for sold materials, e closures a d some

o jects in 6.1 (Ta le 1), a d for b lk materials in 9.1 For certain items, sp cial d finitio s are maintain d in oth r

sta d rds (se 3.3, 3.8 a d 3.9)

Note 3 to e try: Pro uct sta d rds a d oth r sta d rds co erin electrostatic pro erties ofe inclu e sp cific

d finitio s of “co d ctiv ” which a ply o ly to items co ere by th se sta d rds a d may b difere t to th

d finitio s giv n h re Se e.g ISO 8 31 a d ISO 8 3 for h se a d h se as embles

3.3

co d ctive fo twe r

fo twear e s rin that a p rs n stan in o a c n u tiv flo r has a re istan e to earth low

e o g to e s re dis ipatio of ele tro tatic c arg s e e in partic larly hazard u situatio s

(e.g wh n han ln s n itiv e plo iv s) b t n t hig e o g to pre e t a hazard u

ele trical s o k at v ltag s le s than 5 0 V

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Note 1 to e try: Dis ip tiv materials or o jects are n ith r co d ctiv n r insulatin b t, lk co d ctiv items,

safely lmit co tact ch rgin a d/or dis ip te e e th maximum ch rgin cure ts as ociate with th ir d sig e

a plcatio wh n in co tact with e rth

Note 2 to e try: Bo n ary lmits for th dis ip tiv ra g are giv n for sold materials, e closures a d some

o jects in Ta le 1, a d for b lk materials in 9.1 For certain items, sp cial d finitio s are maintain d in oth r

sta d rds (se 3.3, 3.8 a d 3.9)

Note 3 to e try: Pro uct sta d rds ofe inclu e sp cific d finitio s of “dis ip tiv ” which a ply o ly to items

co ere by th se sta d rds a d may b difere t to th d finitio sgiv n h re

3.8

dis ipative clothin

clothin that me ts th material an d sig re uireme ts s e ifie in EN 1 4 -5

3.9

dis ipative footwe r

fo twear e s rin that a p rs n stan in o a c n u tiv or dis ipativ flo r has a re istan e

to earth low e o g to e s re dis ipatio of ele tro tatic c arg s b t hig e o g to pre e t

a hazard u ele trical s o k at v ltag s le s than 5 0 V

area in whic flammable or e plo iv gas/vap ur-air or d st air mixture or aero ols are, or

can b , pre e t in s c q antitie as to re uire s e ial pre autio s again t ig itio

Note 1 to e try: Se IEC 6 0 9-10-1a d IEC 6 0 9-10-2 A sh rt summary is giv n in An ex D

3.13

high chargin

a pro e s that g n rate a hig er rate of ele tro tatic c argin than simple man al

o eratio s

E AMPLE Ru bin , cle nin with a cloth, raisin from a se t, walkin , wipin of cloth s etc

Note 1 to e try: Typical examples of hig ch rgin o eratio s inclu e e.g th flow of insulatin lq ids or

p wd rs a d hig v lta e spray ch rgin

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© IEC 2 17

3.14

h brid mixture

an e plo ible h tero e e u mixture, c mprisin gas or vap ur with s s e d d partic late

s ld or l q id, in whic th total flammable gas c n e tratio is at least 10 % of its lower

flammable lmit (L L) an th total s s e d d partic late c n e tratio is at least 10 % of its

minimum e plo ible c n e tratio (MEC)

3.15

insulatin

havin a re istivity or re istan e that is hig er than th dis ipativ ran e (s e 3.7)

Note 1 to e try: Insulatin materials or o jects are n ith r co d ctiv n r dis ip tiv Electrostatic ch rg s ca

ac umulate o th m a d d n t re diy dis ip te e e wh n th y are in co tact with e rth

Note 2 to e try: Bo n ary lmits for th insulatin ra g are giv n for sold materials, e closures a d some

o jects in Ta le 1, for b lk materials in 9.1 For certain items, sp cial d finitio s are maintain d in oth r sta d rds

(se 3.3, 3.8 a d 3.9)

Note 3 to e try: Pro uct sta d rds a d oth r sta d rds co erin electrostatic pro erties ofe inclu e sp cific

d finitio s of “insulatin ” which a ply o ly to items co ere by th se sta d rds a d may b difere t to th

d finitio s giv n h re Se e.g ISO 8 31 a d ISO 8 3 for h se a d h se as embles

Note 4 to e try: Th a jectiv “n n-co d ctiv ” h s ofe b e use as a s n nym for insulatin It is a oid d in

this d cume t as it co ld b ta e to me n eith r “insulatin ” or “insulatin or dis ip tiv ” a d this may le d to

Note 1 to e try: Th resista ce d p n s u o th v lume or surface resistivity of th materials a d th dista ce

b twe n th ch se p int of me sureme t a d e rth

Note 2 to e try: On commo co fig ratio (e.g in IEC 613 0-4-1, ISO 10 6 a d A TM F15 ) uses a circular

electro e, (6 ± ) mmin diameter

3.18

minimum ig itio energ

MIE

minimum e erg that can ig ite a mixture of a s e ifie flammable material with air or o y e ,

meas re b a stan ard pro e ure

Note 1 to e try: Se A TM E5 2-8 for g ses a d v p urs, IEC 612 1-2-3, A TM E2 19-0 a d E 13 21 for

relaxatio time

time d rin whic th ele tro tatic c arg o a s l d s rfac or in th b lk of a lq id or

p wd r d cay e p n ntial y to 1/e (i.e ab ut 3 %) of its original valu (s e A.2.2)

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Note 2 to e try: Th surface resista ce is d p n e t u o th electro e co fig ratio Th surface resista ce

me sure with th example electro e co fig ratio is te times lower th n th surface resistivity

Note 3 to e try: Sof co d ctiv ru b r strip electro es are prefere o er siv r p int electro es

3.2

surfa e re istivity

re istan e acro s o p site sid s of a s rfac of u it le gth an u it width c mmo ly

e pre s d in o ms (or o ms/s uare)

Note 1 to e try: This co fig ratio is use e.g in A TM D2 7 a d B 7 0 -2

3.2

v lume re istivity

re istan e of a b d of u it le gth an u it cro s-s ctio al area e pre s d in o m metre

4 Nomenclature

Ele tro tatic safety re ulatio s u e man adje tiv s to clas ify th c n u tin abi ty of

materials an o je ts Difere t re ulatio s an dif ere t in u trie u e difere t adje tiv s

an , e e wh n th same adje tiv s are u e , th ir d finitio s can vary Th n me clature

that is s stematical y folowe in this d c me t is giv n h re in ord r to av id c nfu io an

to as ist with tran latio :

Sol d materials are clas ifie as c n u tiv , dis ipativ or in ulatin ac ordin to th ir

v lume re istivity (s e 3.2, 3.7 an 3.15) Bo n ary l mits are giv n in Table 1

Sol d obje ts an texti e are clas ifie as c n u tiv , dis ipativ or in ulatin ac ordin to

th ir s rfac or leakag re istan e, d p n in o ap lcatio (s e 3.2, 3.7 an 3.15)

Bo n ary lmits for e clo ure an s me o je ts are giv n in Table 1 For c rtain items,

s e ial d finitio s are maintain d in oth r stan ard (s e 3.3, 3.8 an 3.9)

Bulk materials (p wders etc.) are clas ifie as low, me ium or hig re istivity ac ordin to

th ir v lume re istivity (s e 9.1 for b u dary lmits)

Liquids are clas ifie as hig , me ium or low c n u tivity ac ordin to th ir ele trical

c n u tivity (s e 7.1.4 for b u dary lmits)

NOT More d tais a o t electrostatic pro erties, co ce ts a d termsare giv n in An exesAto G

Re istanc s hav mainly b e state in e p n ntial form in oth r d c me ts Howe er,

e p n nts are smal fig re , an th e p n nts 6, 8 an 9 mainly u e in ele tro tatic are

easi y misread in printe or proje te d c me ts, an e e u readable if th y o c r in n te

For this reas n this d c me t u e SI prefix s in tead of e p n nts:

103

Ω = 1 kΩ

106

Ω = 1 MΩ

108

Ω = 10 MΩ

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© IEC 2 17

109

Ω = 1 GΩ

101

A = 1 mA

10-6

A = 1 µA

10-9

A = 1 nA

10-12

A = 1 pA

Static ele tricity o c rs c mmo ly in in u try an dai y lfe Man of th efe ts are harmle s

an eith r pas c mpletely u n tic d or are simply a n isan e, b t static ele tricity can als

giv ris to a hazard u situatio In s c situatio s, th hazard can g n ral y b re u e b

c arg relaxatio (s e An e A)

Hazard cau e b ele tro tatic c arg in lu e:

a) ig itio an / or e plo io of flammable atmo p ere , s e IEC 6 0 9-0 an EN 13 6 -1;

b) ele tro tatic s o k in c mbinatio with an th r hazard (e.g fal, trip) − s e ISO 1210 -1;

c) ele tro tatic s o k givin ris to injury or d ath, s e ISO 1210 -1;

d) damag to ele tro ic (n t c v re b this d c me t

In ad itio , static ele tricity can intro u e o eratio al pro lems d rin man facturin an

han ln pro e s s, e.g b cau in article to ad ere to eac oth r, or b atractin d st

Static ele tricity is g n rate b :

a) th c ntact an s paratio of s ld e.g th mo eme t of c n e or b lts, plastic fi m,

etc o er rolers, th mo eme t of a p rs n;

b) th flow of l q id or p wd rs, an th pro u tio of s ray ;

c) in u tio p e ome a, i.e o je ts reac hig p te tial or b c me c arg d d e to b in in

an ele tric field

Th ac umulatio of ele tro tatic c arg can giv ris to hazard an pro lems in a wid

partic larly in c emicals, p armac uticals, p trole m an fo d pro e sin in u trie

Be au e of th larg n mb r of in u trial pro e s s that c uld b in olv d it is n t p s ible

to giv d taie informatio rele ant to al of th m In tead, this d c me t atempts to

th m This informatio s o ld e able th plant o erator to tak whate er pre autio s c uld b

n c s ary to av id ig itio s of p te tialy flammable atmo p ere an ele tro tatic s o k

For c n e ie c this d c me t is divid d into a n mb r of clau e Th s d al with pro lems

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© IEC 2 17

f ele tro tatic pro lems cau e b p o le;

g) av idan e of ele tro tatic s o k;

h) earthin an b n in of plant an mac in ry;

As this d c me t is v ry c mple , c re tly e aluatin th ele tro tatic hazard of pro u ts

an pro e s s may n t b eas for n w read rs For this reas n a u iv rsal y ap l cable

informativ An e F has b e ap e d d whic refere c s th rele ant s ctio s of this

d c me t in th c r e t ord r

It is v ry s ld m that an ele tro tatic hazard can b treate b its lf Pre autio s again t

ele tro tatic hazard s o ld b in ad itio to oth r pre autio s, e.g e plo io prote tio

Th y s o ld als b c n iste t with pre autio s tak n to av id oth r hazard that may b

pre e t, s c as ig itio s d e to oth r cau e , an to icity It is imp rtant that al s urc s of

ris in a s stem of work are c n id re an that a balan e ap roac to safety that c v rs al

ris s is ad pte In partic lar, care s o ld b e ercis d in th pro isio of earthin s stems

wh re th y can interfere with oth r prote tiv s stems, e.g cath dic prote tio or intrin icaly

safe ele trical e uipme t

6 Static electricity in sol d materials

6.1 General considerations

Sol d materials are u ual y c aracteris d as in ulatin , dis ipativ or c n u tiv ac ordin to

th ir v lume re istivity En lo ure are u ual y clas ifie ac ordin to th ir s rfac re istan e

or re istivity (meas re ac ordin to IEC 6 0 9-0, IEC 6 16 , IEC 6 0 3 or IEC 613 0-2-3 or

e uivale t meth d ) Meas rin d tais wi als b d alt with in IEC 6 0 9-3 -2

2

s rfac clas ificatio s are e uivale t b cau e th s rfac re istivity is te time hig er than

th s rfac re istan e for th s e ifie ele tro e g ometrie For oth r s e ific ap lcatio s

difere t d finitio s may b ap l cable (e.g leakag re istan e in th cas of flo rs) Th

thre h ld mo t c mmo ly u e for th s p rp s s are s own in Table 1

—————————

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© IEC 2 17

Table 1 – Bo ndary l mits at (2 ± 2) °C an (2 ± 5) % RH for the chara teris tion

of sol d materials an example for the cla sific tio of obje ts

as embly (Ω)

a

Wh re local ambie t co ditio s are sig ifica tly difere t from th state worst case test co ditio of

(2 ± 2)°C a d (2 ± 5) % RH, oth r test co ditio s may b use afer a careful h zard e alu tio In some

co ntries, esp cialy d rin winter, a relativ h midity of (12 ± 3) % at (2 ± 2) °C is a a pro riate test

e viro me t for q alfyin e uipme t As th resista ce of n n-metals usu ly d p n s stro gly o th

me surin v lta e, th me surin v lta es (ypicaly 5 0 to 1 0 0 V) sh uldb ch se to b co siste t with

th p rp se of th me sureme t a d state with th test result

b

Ac ordin to ISO 8 31, th v lu s for h ses are me sure at (5 ± 5) % RH a d are th latest o es ta e

from Ta le 15 in 7.7.3.1 In th p st, slg tly difere t v lu s h v b e use in ISO a d CE ELEC

d cume ts Oth r clas ificatio s may b use by in ustry sta d rds for sp cific a plcatio s (e.g in

ISO 8 31 co d ctiv h ses for in ustry a plcatio s, dis ip tiv a tistatic h ses for a tomo ie a plcatio s)

which d esn t n ces ariy imply electrostaticsafety

En lo ure criteria are to pre e t trib -c argin an th s d n t n c s ari y dis ipate c arg

d p site from u s e ifie pro e s s within th e clo ure

Difere t valu s meas re at 5 % RH hav b e ap le in th past in th ab e c of a

d h midifie te t c amb r an are c n id re to er o th safe sid This ap roac has n w

b e dis o tin e , an lmits at 5 % RH are, e c pt for h s s, giv n in oth r d c me ts

o ly Th y s o ld o ly b u e if an ap ro riate clmate is n t avaiable As th c arg abi ty

of materials is hig er at 2 % RH c mpare to 3 % RH, th former valu of 3 % RH has

b e re u e to (2 ± 5) % RH A relativ h midity at th lower part of th interval s o ld b

ap l e d rin meas reme ts wh n v r p s ible

Wh n c aracterizin n n-h mo e o s materials th meas re valu s s o ld b av rag d

an ro n e to th n are t ord r of mag itu e u le s oth rwis s e ifie b th te t meth d

No -h mo e e u materials may e hibit difere t re istivity in difere t dire tio s

In tead of meas rin re istan e, th rate of c arg d cay may b u e to c aracteriz th

dis ipativ b havio r of clothin (s e EN 1 4 -3 an EN 1 4 -5)

Ele trical y in ulatin s l d materials are c mmo ly u e in man forms, in lu in pip s,

c ntain rs, s e ts, c atin s an ln rs Th u e of ele tricaly in ulatin s l d materials in

hazard u areas can giv ris to man ele tro tatic hazard , in partic lar:

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© IEC 2 17

a) c n u tiv o je ts c uld b is late from earth b th material an c uld th n reac a

hig ele trical p te tial an giv ris to s ark (s e A.3.2);

b) c arg s o th s rfac of th material c uld lead to bru h dis harg s (s e A.3.4);

c) a c mbinatio of c n u tiv an in ulatin materials in th pre e c of prolfic c arg

g n rators (s e 12.3) c uld lead to e erg tic pro agatin bru h dis harg s (s e A.3.5)

Meas re to ad re s th s hazard are giv n in 6.2, 6.3 an 6.4

If in ulatin materials are u e , a ris as e sme t is n c s ary to id ntify if th re is an

pro e s that can lead to dire t pro u tio of or in ire t in u tio of ele tro tatic c argin o

in ulate materials that are pre e t in th lo atio

6.2 The us of con uctive or dis ipative materials in pla e of insulating o e

6.2.1 General co sideratio s

It is g n ral y g o practic to minimis th u e of in ulatin materials in hazard u areas

Whie this may b ac ie e primari y b th u e of in ere tly c n u tiv materials (e.g

metals), man materials whic u e to b avai able o ly in in ulatin forms (e.g ru b rs or

plastic ) are n w avai able in grad s whic me t th re uireme ts to b c n id re

c n u tiv or dis ipativ as giv n in T ble 1 This in reas in c n u tivity is ty icaly

ac ie e eith r b ad in c n u tiv in re ie ts (e.g carb n blac ) to its c mp sitio , or b

ap lyin h gro c pic ag nts to its s rfac that atract atmo p eric moisture − c n u tiv

p lymers, laminate with c n u tiv eleme ts an metal s d fims hav al b e d v lo e

for impro e static dis ipatio

It is imp rtant that s c c n u tiv an dis ipativ materials are earth d relably ac ordin to

Clau e 13 an are lo g lastin ac ordin to Clau e 13 Als , if c n u tiv or dis ipativ

c atin s are u e to mak an in ulatin material n n-c arg able, it is imp rtant that s c

c atin s are pro erly earth d, an that th ir d rabi ty an s itabi ty for u e in hazard u

areas (partic larly Zo e 0 an Zo e 1) is d mo strate for th partic lar ap lcatio

An th r c n id ratio is that th u e of a hig pro ortio of ad itiv s s c as carb n blac

may d grad th p y ical pro ertie (primariy stre gth an c emical re istan e) of th

material This may re d r s c materials u s itable for c rtain ap lcatio s This can b

av id d b u in intrin ical y c n u tiv p lymers as a c n u tin in re ie t or c atin Care

s o ld b tak n to e s re s f icie tly hig c n e tratio s of dis ipativ ad itiv s an th ir

u iform distrib tio

NOT It is n t p s ible to d termin wh th r materials may b dis ip tiv or co d ctiv by th ir colo r Black

p lymers may n t b dis ip tiv , a d mo ern co d ctiv or dis ip tiv materials may b a aia le in a v riety of

colo rs

F bric , e.g fiter cloth, can b mad dis ipativ b in orp ratin stainle s ste l or oth r

c n u tiv or dis ipativ fibre in th fabric Care has to b tak n to e s re that, as a re ult

of was in or me hanical stre s, th o eral c n u tivity of th fabric is maintain d an

is late patc e of c n u tiv fibre are n t forme

6.2.2 Dis ipative sol d materials

A s ld material is d fin d as dis ipativ if its s rfac re istan e, s rfac re istivity or v lume

re istivity me t th c mbin d criteria s t o t in 6.1

In g n ral, pro idin that dis ipativ materials are c n e te to earth ac ordin to Clau e 13,

n furth r prote tiv meas re n e to b tak n Howe er, in pro e s s in olvin hig s e d

s paratio (e.g c n e or an tran mis io b lts, s e 6.4) lower re istivitie an re istan e

can b re uire

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NOT 1 For materials with resistivities at th to e d of th dis ip tiv ra g th re wi b sig ifica t co straints

o th p s ible g ometry of a ma ufacture item if th re uireme ts of Cla se 13 are to b met (e.g lo g pip s or

thin fiame ts wi n t me t th e rthin re uireme ts whist thin sh ets with a larg e rth co tact are wi )

In s me cas s, partic larly with plastic fims or s e tin , a material is ad e to at ract

atmo p eric moisture to th s rfac , th s in reasin s rfac c n u tivity Care s o ld b

tak n wh re this ty e of dis ipativ plastic fim or s e tin is u e in low h midity c n itio s:

in e viro me ts with low h midity ( y ical y < 0 %), it can b c me in ulatin an ac umulate

ele tro tatic c arg

It s o ld b e s re that a dis ipativ c atin can ot b was e away or ru b d of an

can ot lo e its efe tiv n s o er time Oth rwis s c a c atin wo ld o ly b ap ro riate

as a temp rary meas re to re u e ac umulatio of static ele tric c arg

Dis ipativ ag nts u e in pac agin s o ld b c mpatible with th pro u t c ntain d within

th pac ag Ab orptio of th dis ipativ ag nts b pro u t with whic it is in c ntact may

cau e pro u t c ntaminatio an / or lo s of dis ipativ pro ertie of th pac ag

NOT 2 New static dis ip tiv a ditiv s are a aia le which incre se th v lume resistivity a d are, th refore,

les se sitiv to h midity b t are also afecte by a in as are oth r a ditiv s

NOT 3 Th resista ce of dis ip tiv materialsma e from ru b r v lca ize with carb n black may incre se with

d cre sin temp rature Such materials may, for example, b dis ip tiv (~10 MΩ) at 2 ˚C b t insulatin

(~10 TΩ) at 0 ˚C

6.2.3 Earthing of con uctive an dis ipative items

Al metal an oth r c n u tiv or dis ipativ material s o ld b c n e te to earth ac ordin

to Clau e 13 with th e c ptio of v ry smal items Th capacitan e of is late items

d p n s o th ir siz , s ro n in materials an pro imity to oth r c n u tors an may b

v ry difere t u d r in tale or n n-in tale c n itio s Th maximum al owable capacitan e

of is late items d p n s o th ig itabi ty of th gas s, vap urs an d st e pre s d b th

re re e tativ gas gro p I I A, I B an I C (IEC 6 0 9-2 -1, s e D.3) or d st gro p I

IEC 6 0 9-10-2, s e D.2) as s own in T ble 2, takin ac o nt of th fol owin :

a) Capacitan e b low 3 pF n e n t b earth d pro id d that th o je t can ot reac a

hazard u p te tial an is n t situate in Zo e 0 wh n gas s or vap urs b lo gin to

Gro p I C are u e

b) In Zo e 1 wh re gas s or vap urs b lo gin to Gro p I A are u e , an in Zo e 2 an

21 th maximum alowe is late capacitan e may b in reas d to 6 pF pro id d hig

c argin pro e s s d n t o c r

c) In d st Zo e 2 an 21 an in Gro p I th maximum al owe is late capacitan e may

b furth r in reas d to 10 pF pro id d that eith r hig c argin pro e s s d n t o c r or

o ly p wd rs with minimum ig itio e ergie hig er than 10 mJ are han le

d) Th l mits in T ble 2 are n t ab olute valu s that pre e t in e div dis harg s, b t th y

merely re u e th ris of o c r e c to a g n raly ac e te low le el

e) Han h ld d vic s an han to ls are e p cte to b earth d via th u er In an cas of

d u t th u er s o ld e s re earthin of th d vic wh n workin in hazard u areas

f Pe ple are c n u tiv items havin s ficie t capacitan e to pro u e an in e div

dis harg Th y, th refore, s o ld b earth d ac ordin to Clau e 1 b fore e terin a

hazard u area Zo e 0, 1, 2 , 21 or Gro p I

Capacitan e s o ld b meas re ac ordin to IEC 6 0 9-0, 2 15

NOT It is s h d le to re ise thismeth d a d mo e it to IEC 6 0 9-3 -2

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Table 2 – Maximum al owed isolated c pa itanc in Zo e with ex losive atmosp ere

ca a le of g n ratin h zard us p te tials

NOT 1 Th su divisio s are b se o th maximum exp rime tal safe g p (ME G) or th minimum ig itio

cure t ratio (MIC ratio) of th explosiv g s atmosp ere in which th e uipme t may b instale (se

IEC 6 0 9-2 -1) More d tais ca b fo n in C.6 a d D.3

NOT 2 Ma u l ru bin isusu ly n t co sid re to b a hig ch rgin proces

For dis ipativ materials with a s rfac re istan e e c e in 10 GΩ earthin may n t b

n c s ary In an cas of d u t an ad itio al te t is n c s ary to pro e ele tro tatic safety of

u earth d o je ts (e.g 6.3.9)

6.3 Pre autio s required when usin insulatin sol d materials

6.3.1 General

Th re trictio s o th u e of in ulatin materials in hazard u areas d p n o th

clas ificatio of th hazard u area ac ordin to IEC 6 0 9-10-1 an IEC 6 0 9-10-2:

a) in Zo e 0, in ulatin s l d materials s o ld o ly b u e if c argin pro e s s capable of

g n ratin hazard u p te tials wi n t o c r eith r d rin n rmal o eratio in lu in

mainte an e an cleanin or e e in th cas of rare malfu ctio s;

b) in Zo e 1, in ulatin s l d materials s o ld o ly b u e if c argin pro e s s capable of

g n ratin hazard u p te tials wi n t o c r eith r d rin n rmal o eratio in lu in

mainte an e an cleanin or in th cas of l k ly malfu ctio s;

c) in Zo e 2, in ulatin s l d materials s o ld o ly b u e if c argin pro e s s capable of

g n ratin hazard u p te tials are u l k ly to o c r d rin n rmal o eratio in lu in

mainte an e an cleanin

pro agatin bru h dis harg s (s e A.3) Howe er, practical e p rie c , e p rime tal

e id n e an th ab e c of in id nts in icate that bru h dis harg s d n t ig ite e e

ig itio s n itiv p wd r clo d in th ab e c of an flammable gas or vap ur

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NOT 1 Synth tic fa ric use in cloths for cle nin or wipin ca d v lo suficie t static electric ch rg to

pro uce dis h rg s ca a le of ig itin solv nt v p urs Typicaly, ch rg g n ratio incre ses with th sp e a d

vig ur of th wipin actio Th material b in cle n d or wip d, if insulatin , also ca ac umulate suficie t

ch rg to pro uce a ince div dis h rg Coto or s nth tic fa ric tre te with a static dis ip tiv comp u d

may b re uire if static electric ch rg g n ratio n e s to b co trole , esp cialy if flamma le insulatin

solv nts are b in use for cle nin or wipin

NOT 2 Th prese ce of co tamin tio (e.g gre se or moisture) may afect th p te tial ig itio h zard wh n

usin insulatin materials

NOT 3 Co d ctiv solds, o jects or lq ids may form h zard us isolate co d ctiv isla ds if prese t o

ch rg d insulatin surfaces

In ad itio , to pre e t in e div dis harg s th pre autio s giv n in 6.3.2 to 6.3.4 s o ld b

tak n in al Zo e wh re th u e of in ulatin s l d materials is u av idable Th pre autio s

giv n in 6.3.2 to 6.3.4 relate to th av idan e of in e div bru h dis harg s, that giv n in

6.3.4 als relate to pro agatin bru h dis harg s

6.3.2 Re trictio s on the siz of charge ble insulating surfa e

Wh re th u e of c arg able in ulatin material in a hazard u area is n c s ary, th

maximum al owable siz of in ulatin s rfac d p n s o th ig itabi ty of th gas s an

vap urs e pre s d b th re re e tativ gro p I I A, I B, I C (IEC 6 0 9-2 -1) or th

re re e tativ d st gro p I (IEC 6 0 9-0) an th clas ificatio of th hazard u area

(IEC 6 0 9-10-1 an IEC 6 0 9-10-2, s e D.2) as s own in T ble 3, takin ac o nt of th

folowin :

a) for s e t materials th area is d fin d b th e p s d (c arg able) area;

b) for c rv d or ir e ularly s ap d o je ts th area is th proje tio of th o je t givin th

maximum area;

c) for lo g narow materials, s c as cable s eath or pip s, th maximum siz is d fin d b

th tran v rs dime sio (i.e th diameter for a cable s eath or pip ); alth u h wh n it is

c ie it s o ld b treate as for a s e t;

d) e e smaler diameters can b re uire for narow pip s or tu e c ntainin flowin

l q id or p wd rs;

e) n rmal ele tric cable are u ual y ac e table in al z n s Se IEC 6 0 9-14 Very thic

in ulatin lay rs o thic cable s o ld, h we er, b te te e p rime tal y e.g ac ordin

to IEC 6 0 9-0:2 0 , 2 14

NOT It is s h d le to re ise thismeth d a d mo e it to IEC 6 0 9-3 -2

It is e s ntial that n n-c n u tiv s l d materials u e in hazard u areas d n t e c e th

maximum area or width valu s giv n in T ble 3 for th z n within whic it is u e u le s it

can b e p rime tal y s own that hazard u ele tro tatic c arg s are n t to b e p cte

(s e 6.3.9) or c argin me hanisms wi n t o c r at an time An e ample of th last name

cas is sig s or lamp at th c i n whic are n rmal y n t e p s d to an c argin

me hanisms In this cas , a warnin “Clean with a water-wet cloth o ly an al ow to dry

naturaly” is s ficie t to av id c argin wh n cleanin

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Table 3 – Re trictio on siz of insulatin sol d materials in ha ard us are s

Max

are

(mm2

) Max

width

(mm) Max

are

(mm2

)Max

) Max

)Max

)Max

NOT 2 Eq ipme t mark d I B is suita le for a plcatio s re uirin Gro p I A e uipme t Simiarly, e uipme t

mark d IC is suita le for a plcatio s re uirin Gro p I A or Gro p I B e uipme t

NOT 3 Th se b rd r lmits are also use e.g in IEC 6 0 9-0, CE ELEC TR 5 4 4, TRB 215 , JNIOS

TR4 , a d B 5 5

NOT 4 Th su divisio s are b se o th maximum exp rime tal safe g p (ME G) or th minimum ig itio

cure t ratio (MIC ratio) of th explosiv g s atmosp ere in which th e uipme t may b instale (se

IEC 6 0 9-2 -1) More d tais ca b fo n in C.6 a d D.3

NOT 5 Th lmits in Ta le 3 are n t a solute v lu s th t pre e t ince div dis h rg s, th y merely re uce it

to a g n raly ac e te low le el

NOT 6 Th prese t state of k owle g in icates th t th re is n ig itio risk d e to brush dis h rg s in th

case of se sitiv d sts pro idin th t th re are n flamma le g ses or v p urs (se An ex A.3.4) Howe er,

ch rg g n ratio proces es stro g r th n ma u l ru bin may cre te ince div pro a atin brush dis h rg s

u d r certain circumsta ces (se 6.3.4.2)

6.3.3 Earthed metal me he

Th areas giv n in T ble 3 can b in reas d b a factor of fo r b in orp ratin an earth d

me h (or metal frame) into th in ulatin s l d or b wrap in s c a me h aro n its s rfac

In ad itio :

a) th lay r thic n s ab v th me h s o ld b re tricte to th valu s giv n in 6.3.4.2 to

pre e t bru h dis harg s; an

b) pro agatin bru h dis harg s s o ld b pre e te ac ordin to 6.3.4.3; an

c) s e ial care s o ld b tak n to pre e t or d te t break whic c uld lead to is late

c n u tiv parts whic pre e t a greater ele tro tatic hazard than an in ulatin s rfac

6.3.4 Insulatin coatings o e rthed co ductive surfa e

6.3.4.1 General

L y rs or c atin s of in ulatin s l d o earth d c n u tiv s rfac s (in partic lar metal

s rfac s) can giv ris to bru h an / or pro agatin bru h dis harg s d p n in o s v ral

factors

6.3.4.2 Av idanc of brush dis harge

With re ard to bru h dis harg s, practical e p rie c s ows that th s dis harg s are

u lk ly to b in e div if:

a) hig ele tro tatic c argin pro e s s are av id d (e.g re eate fi in an emptyin of a

c n u tiv drum c ntainin an in ulatin ln r); an ,

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© IEC 2 17

b) th thic n s of th lay r d e n t e c e a valu of 2 mm in th cas of gas s an

vap urs of gro p I I A an I B an a valu of 0,2 mm in th cas of gas s an vap urs

of gro p I C For d sts th re is n thic n s lmitatio u le s th p wd r lay r can form a

hig re istan e c ntin o s fim, e.g b s lf p lymerizatio or reactio with water

NOT 1 Ma u l ru bin is usu lyn t co sid re to b a hig ch rgin proces

NOT 2 Th thin er th co tin th les ince div are th brush dis h rg s cre te by ma u l ru bin of th

surface, a d th more ince div are th pro a atin brush dis h rg s cre te by stro g r electrostatic ch rgin

proces es o th surface

Howe er, in th cas of flu rinate p lymers an e p rime tal e aluatio of th c arg abi ty

is re omme d d, e.g ac ordin to IEC 6 0 9-0:2 0 , 2 14

NOT It is s h d le to re ise this meth d a d mo e it to IEC 6 0 9-3 -2

6.3.4.3 Av idanc of pro agatin brush dis harge

Pro agatin bru h dis harg s can o c r wh n hig or re eate ele tro tatic c argin

pro e s s act o in ulatin lay rs or c atin s o c n u tiv s rfac s Th s dis harg s can

b pre e te b o e or more of th folowin meas re :

a) Av id havin thin in ulatin c atin s o metals or oth r c n u tiv materials Pro agatin

bru h dis harg s te d to o c r with thin c atin s; th y can n rmal y b pre e te b

havin thic n s e greater than 10 mm;

b) Re u e th s rfac or v lume re istivity of th c atin It is n t k own pre is ly what

le els are re uire to pre e t th o c r e c of pro agatin bru h dis harg s, b t th

valu s for dis ipativ materials giv n in T ble 1 an a leakag re istan e le s than

10 GΩ are k own to b s ficie tly low;

c) Us a c atin with a low diele tric stre gth (break own v ltag for s ld h mo e o s

materials le s than 4 kV, in th cas of wo e fabric 6 kV, s e A.3.5) Su h c atin s

ele tricaly break d wn b fore a pro agatin bru h dis harg can d v lo Th diele tric

stre gth s o ld b meas re ac ordin to IEC 6 2 3-2 in c mbinatio with IEC 6 2 3-1,

or IEC 6 0 9-3 -2

5

d) Av id hig or re eate c argin pro e s s (e.g air io s in th vicinity of hig v ltag

ele tro e , hig s e d flowin l q id an p e matic tran fer of p wd rs, an pap r or

plastic fois tran p rte b mac in s)

NOT 1 Du to th ir slg t p rosity, layers of solv nt or water b se p int or lo se p wd r usu ly h v a low

bre k own v lta e so th t pro a atin brush dis h rg s are dificult to o tain from such layers

NOT 2 Co tin s forme by b kin o a a ple p wd r a d e amel usu ly h v to hig a bre k own v lta e

to a oid pro a atin brush dis h rg s

NOT 3 Polymer fims which are wo n o to a re l or are lfe from a co d ctiv or insulatin surface ca

acq ire bip lar ch rg s ie e u l a d o p site ch rg s o th two surface of th fim This ca le d to brush

dis h rg sa d oc asio aly e e to pro a atin brush dis h rg s

NOT 4 Ma u l ru bin is n t n rmaly co sid re a hig ch rgin proces

6.3.5 Con uctive or dis ipative coatings o insulatin materials

Sp cial care is n c s ary wh n ap lyin a c n u tiv or dis ipativ c atin o an in ulatin

s rfac to e s re a u iform distrib tio of th c n u tiv particle No -u iform distrib tio

may lead to is late c n u tiv islan s whic can b c arg d easi y b in ulate s rfac s in

th ir vicinity Su h is late c n u tiv islan s pre e t a greater ele tro tatic hazard than an

in ulatin s rfac

Co d ctiv c atin s s o ld b earth d as oth r c n u tors in ac ordan e with Clau e 13

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6.3.6 Static dis ipative agents

Dis ipativ antistatic ag nts are fre u ntly u e o clothin an flo rs an to in reas th

c n u tivity of l q id an materials Care s o ld b tak n to g arante th pre e c of a

s ficie t c n e tratio of th s ag nts to ac ie e th d sire fu ctio For e ample,

dis ipativ ag nts may b c me di ute or was e o t Th refore, th ir efe tiv n s n e s to

b mo itore an maintain d No -migratory p rman nt antistatic p lymer ad itiv s hav

re e tly b e d v lo e to o erc me th s lmitatio s

6.3.7 Humidific tio

Th s rfac re istivity of s me in ulatin s l d materials can b re u e to dis ipativ le els

if th relativ h midity is maintain d ab v ab ut 6 % Ev n th u h damp air is n t

c n u tiv , water / moisture may ad orb o th s rfac of man materials d p n in o th

h dro c pic nature of th material This may b s ficie t to pre e t ac umulatio of static

ele tricity, pro id d th re is a s itable path to earth

Howe er, wh reas th s rfac of s me materials (e.g glas or natural fibre ) can ad orb

e o g moisture to e s re a s rfac c n u tivity that is s ficie t to pre e t ac umulatio of

static ele tricity, oth r materials d n t (e.g p lytetraflu ro th le e or p ly th le e) an are

capable of ac umulatin a static ele tric c arg e e at hig relativ h midity Als , wh n th

h midity fals b low ab ut 3 %, materials whic are s s e tible to h midificatio g n raly

return to b in hig ly in ulatin In reasin th relativ h midity, th refore, is n t ef e tiv in

al cas s an , in g n ral, it s o ld n t b u e as th s le prote tiv meas re This is

partic lar imp rtant in Zo e 0

6.3.8 Io is tio / Charge Neutral s tio

6.3.8.1 General

Io isatio of th air is a meth d of makin th air lo al y io -ric s that c arg s o in ulatin

s ld materials can b n utral s d It is partic larly u eful for n utralsin c arg o in ulatin

plastic s e ts or fi ms Meth d that may b emplo e in lu e th s giv n in 6.3.8.2 to

6.3.8.5 Ne tral satio can ot s c e d if th rate at whic c arg is g n rate e c e s th

rate at whic io s are s p l e to th air, or can migrate to th c arg d s rfac , or if s ficie t

io s of th d sire p larity are n t pre e t Co s q e tly, c re t in talatio an re ular

mainte an e is e s ntial for th s d vic s, takin into c n id ratio factors that can

influ n e th ir efe tiv n s s c as e viro me tal c n itio s (e.g d st an temp rature)

an p sitio in of th d vic in relatio to th material pro e s d, mac in parts, an p o le

Th re u tio of c arg at an o e p int in th o eratio d e n t pre e t g n ratio of

c arg in later ste s of th pro e s, s io is rs may b re uire at a n mb r of lo atio s

Po itio in is imp rtant, an efe tiv n s of in ivid al in tal atio s s o ld b c nfirme b

field meas reme t of re id al c arg or v ltag In partic lar, for fi ms an s e ts it is

n c s ary to e s re that io s are dire te at th c r e t sid to av id formin a bip lar lay r

whic c uld giv ris to pro agatin bru h dis harg s

Coro a p ints remain fu ctio al o ly as lo g as th y are clean an s arp Ac umulatio of

c ntaminants (e.g in , c atin s lutio , or pap r d st an c r o io pro u ts s o ld b

c ntrole b an efe tiv mainte an e pro ram

Io is rs s o ld b s le te b th ir c arg g n ratio rate or b th ir c arg d cay time

Th y s o ld n t b u e in Zo e 1, I C u le s th ris s hav b e e aluate b an e p rt

Furth rmore th y s o ld n t b u e in Zo e 0 as th o ly safety meas re

6.3.8.2 Pa sive io is rs

Pointe ele tro e s c as earth d s arp n e le , fin wire or c n u tiv tin el pro u e

c ro a dis harg s wh n plac d in th ele tric field from a hig ly c arg d s rfac Th s

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efe tiv n s an may, in ad itio pro u e dis harg s if pas iv io is rs are n t pro erly

earth d

6.3.8.3 Active io is rs

Activ io is rs pro u e io s b ap lyin a hig v ltag to a n mb r of c ro a p ints

Commercial s stems c mmo ly u e alternatin v ltag s in th ran e 5 kV to 10 kV Th u e

of a hig v ltag p wer s p ly el minate th l mitatio of pas iv n utralz rs in c ntrol of

c arg s havin field b low th c ro a o s t thre h ld Th c re ts from th c ro a p ints

are lmite eith r b hig re istan e or capacitiv c u l n

Activ io is rs s o ld b s itable for th lo atio in whic th y are u e an s o ld b

d sig e an c n tru te to pre e t b in a p s ible s urc of ig itio Th y re uire careful

d sig to e s re that th s p ly of io s is balan e with th re uireme ts of th pro e s

6.3.8.4 Radioa tive / sof x-ray io is rs

Radioactiv an s f x-ray s urc s io is th s ro n in air an can b u e to dis ipate th

c arg s from a c arg d b d Su h io isatio its lf d e n t pre e t an ig itio hazard b t is,

h we er, l mite in its efe tiv n s (p rforman e d teriorate with th d cay of th

radioactiv material)

6.3.8.5 Io is d air blowers

Io is d air blowers u in eith r hig v ltag s or radioactiv s urc s are u e mainly for

dis ipatin c arg s from awkwardly s ap d o je ts Howe er, th io c n e tratio can

rapidly d creas d wn tream d e to re ombinatio or ad orptio of th io s b th wals As

a re ult, it is dific lt to c n e th io is d air o er larg distan e Th parts c ntainin th

hig v ltag s s o ld b plac d in a n n-hazard u area u le s th y hav b e ap ro riately

c rtifie

NOT Th fu ctio of a io iser ca b teste byth meth d d s rib d in IEC 613 0-4-7

6.3.9 Meth ds to determine the inc n ivity of dis harge

If th re uireme ts in 6.3.2 to 6.3.8 are n t ap l cable, an e p rime tal d terminatio of a

valu for th in e divity of p s ible dis harg s may b h lpful

On meth d is to c arg th sample u d r worst cas c n itio s as hig ly as p s ible (at

least to th maximum le el that c uld o c r in s rvic ) to pro o e dis harg s to an earth d

MIE valu This meth d is d s rib d in IEC 613 0-4-4

Th maximum c arg tran fer e b a dis harg is ofe u e to giv an in icatio of th

in e divity of s ark an bru h dis harg s in tead of u in an e plo iv gas mixture This

meth d is d s rib d in IEC 6 0 9-0:2 0 , 2 14 T ble 4 s ows a s mmary of al ap l cable

thre h ld lmits

NOT It is s h d le to re ise this meth d a d mo e it to IEC 6 0 9-3 -2

Sp cial care s o ld b tak n to e s re that th te t sample is c arg d as hig ly as p s ible,

that in u e c arg s are c mp n ate for an that o ly o e sin le dis rete dis harg is

re ord d

—————————

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2 0 nCa

a

Valu s o ly v ld for sp rk dis h rg sfrom u e rth d co d ctiv or dis ip tiv p rts

NOT 1 Th lmits for Zo e 1 a d Zo e 21 e sure th t ince div dis h rg s sh uld n t oc ur d rin n rmal

o eratio Th lmits for Zo e 0 a d 2 are furth r re uce to ac o nt for a n rmal situ tio s a d th hig le el

of safety re uire for th se zo es

NOT 2 For th expla atio of E L se IEC 6 0 9-0 or An ex E

NOT 3 Al of th v lu s co tain a certain safety margin Rece t work in icates th t th v lu hith rto use for

I B co tains a lower safety margin th n al oth r v lu s To e u lze al safety margins th v lu s for I B h v

b e re uce from3 nC to 2 nC

6.4 Co vey r belts and transmis io belts

6.4.1 General

Belts u e for tran mis io of p wer or th tran p rtatio of s ld materials can g n rate a

s paratio of th c ntactin s rfac s (primariy a drivin s af an a b lt Th amo nt of

c arg ac uire d p n s o th material of th c n e or b lt as wel as th materials of th

drivin s af an th rolers, an in reas s with th v lo ity an te sio of th b lt an th

width of th area of c ntact

Th c arg ac uire b th b lt can o ly b safely dis ipate to earth via th earth d

c n u tiv rolers if th c n e or b lt is s ficie tly dis ipativ Material that is s i e from

th e d of a c n e or b lt into a h p er or c ute can car y a sig ificant c arg Co d ctiv or

dis ipativ b lts can ot b e p cte to remo e c arg from an in ulatin c n e e pro u t

b) th s rfac re istan e o b th sid s of th b lt are b low 7 MΩ meas re with th

ele tro e c nfig ratio in 3.21, or

c) in cas s wh re th b lt c n ists of lay rs of difere t materials th b lt is c n id re to b

dis ipativ if th re istan e (meas re at 2 °C an 5 % relativ h midity) b twe n th

two o p site o ter s rfac s is b low 1 GΩ

NOT Surface resista ces me sure ac ordin to ISO 2 4 a d E 14 7 are at (2 ± 2) °C a d (5 ± 5) %

relativ h midity a d with a in er circular electro e of 2 mm in diameter, o ter rin electro e with 12 mm in er

a d 15 mm o ter diameter Surface resista ces me sure with th electro e co fig ratio d s rib d in 3.21 are

exactly fo r times lower

T ble 5 s ows a s mmary of al meas re that are re uire for c n e or b lts ac ordin to

Trang 37

dis ip tiv ac ordin to th d finitio of 6.4.2

NOT No informatio isa aia le for b lt v locities > 0 m/s

For e plo io Gro p I th re uireme ts of Zo e 1 (I A & I B) ap ly Howe er, in ulatin c al

d st c n e ors tran p rtin hardly ig itable c n u tiv c al d st an simiar c n e ors may

b u e if a ris as e sme t pro id s a low ris of ig itio

T ble 5 an th re uireme ts in 6.4.2 d n t ap ly to b lts whic dis ipate c arg b c ro a

Su h b lts hav to b te te b e p rts e.g b meas rin th ir c arg abi ty u d r worst

cas c n itio s

A lay r of wax or dirt o th b lt c uld in reas th c arg abi ty of th b lt an als its

re istan e an this c uld in reas th c argin hazard Care s o ld b tak n to e s re that

re airs d n t in reas th valu s giv n It is e s ntial that lay rs of in ulatin ad e iv s

u e to c n e t th b lt d n t inter u t th c n u tiv path

Lig t c n e or b lts as d s rib d in ISO 21 8 -1 fre u ntly hav to c mply with hig ly

s e ial s d c stomer’s d man s For th s cas s, th s e ific stan ard ISO 21 7 , Light

co nve yo r be lts – D ete rmin tio ofe le c tric l re sista ce s an ISO 21 7 , Light c onve yo r b elts

– D ete rmin tio ofth ele ctrostatic field g ene rated b y a ru nning lg ht c nve o r b elt e ist an

6.4.3 Transmis io belts

Tran mis io b lts are V-b lts an flat b lts whic driv rotatin parts or mac in s Th

amo nt of c arg ac uire b th b lt d e to th c ntin o s s paratio of th c ntactin

s rfac s d p n s o th material of th b lt an p le s an in reas s with th v lo ity an

te sio of th b lt an th width of th c ntact area Ac ordin to ISO 9 6 an ISO 1813 a

tran mis io b lt material is d eme to b dis ipativ if:

R × B /L ≤ 6 0 kΩ

wh re L is th distan e b twe n two c n u tiv ele tro e (e.g grap ite, si v r paint, metal

ele tro e) o a tran mis io b lt, B is th width of th flat b lt or d u le th width of th sid

fac of th V-b lt, an R th meas re re istan e b twe n th ele tro e at (2 ± 2) °C, with

n moisture c n e satio

NOT In old r d cume ts (e.g CE ELEC TR 5 4 4), th ac e ta ce criteria was R × B ≤ 10 kΩ m, wh re R is

th resista ce me sure at th in er sid of th mo nte tra smis io b lt b twe n a electro e h lfway b twe n

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© IEC 2 17

fulfime t of this R × B criterio d p n s o th dista ce b twe n th two p ley it is imp s ible to ch racterise a

b lt material as dis ip tiv For this re so ISO 9 6 a d ISO 1813 giv a dis ip tiv criteria which is in e e d nt

from th le gth of th b lt If th dista ce b twe n two p ley ex e ds 0,6 m th re uireme ts of b th

ISO sta d rds are a tomaticaly fulfi e by th R × B criterio in old r d cume ts state a o e

T ble 6 s ows a s mmary of al meas re that are re uire ac ordin to th clas ificatio of

th hazard u area ac ordin to IEC 6 0 9-10-1 an IEC 6 0 9-10-2:

Table 6 – Req irements for transmis io belts

dis ip tiv ac ordin to th d finitio in 6.4.3

NOT No informatio is a aia le for b lt v locities > 0 m/s

For e plo io Gro p I th re uireme ts of Zo e 1 (I A & I B) ap ly

T ble 6 an th re uireme ts in 6.4.3 d n t ap ly to b lts whic dis ipate c arg b c ro a

Su h b lts hav to b te te b e p rts e.g b meas rin th ir c arg abi ty u d r worst

cas c n itio s

In cas s wh re th b lt c n ists of lay rs of difere t materials th b lt is c n id re to b

dis ipativ if th re istan e acro s it d e n t e c e 1 GΩ (re istan e meas re at 2 °C

an 5 % relativ h midity)

A lay r of wax or dirt o th b lt c uld in reas th c arg abi ty of th b lt an als its

re istan e an this c uld in reas th c argin hazard Care s o ld b tak n to e s re that

re airs d n t in reas th valu s giv n It is e s ntial that lay rs of in ulatin ad e iv s

u e to c n e t th b lt d n t inter u t th c n u tiv path

7 Static electricity in l quids

7.1 General considerations

lq id s rfac temp rature re uire to pro u e a flammable atmo p ere b this pro e s

Howe er, b cau e of th u c rtaintie in olv d in flas p int meas reme t, difere c s

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© IEC 2 17

e tabl s in l q id s rfac (rath r than b lk) temp rature, it is pru e t to as ume that a

flammable atmo p ere c uld e ist e e wh n th lq id temp rature is b low th flas p int

b a c rtain safety margin Th margin d p n s o th le el of u c rtainty ab ut temp rature,

lq id c mp sitio etc For wel-c ntrol e c n itio s a margin of 5 °C for p re lq id an at

least 1 °C for mixture is ty ical y n e e

Wh re tan s are e p s d to dire t s nl g t an lq id temp rature are n t mo itore it

s o ld b as ume that a flammable atmo p ere c uld b pre e t wh n han ln lq id with

flas p ints u to 6 °C In areas of hig ambie t temp rature an stro g s nl g t, flammable

atmo p ere may o c r e e with lq id that hav flas p ints ab v 6 °C

Wh n han l n a l q id at a temp rature that is wel ab v its flas p int, th saturate

vap ur may giv an o er-ric (i.e n n- lammable) atmo p ere Howe er, th actual

atmo p ere ab v th lq id may n t b saturate (e.g b cau e of v ntiatio ) an s may b

flammable It is th refore n c s ary to as ume that th atmo p ere c uld b flammable

u le s it can b s own oth rwis Co s q e tly, for low flas -p int lq id , th pre e c of

an o er-ric atmo p ere s o ld n t g n ral y b rel e u o as th o ly c ntrol meas re

In s me circ mstan e , th flammable atmo p ere is n t d e to th l q id b in han le b t

d e to re id e of v latie lq id or vap ur from earler o eratio s with th same e uipme t or

from n arb o eratio s Re id al vap urs can o c r d rin switc loadin , in whic a lq id

havin a hig flas p int (e.g die el) is load d into a tan whic pre io sly c ntain d a l q id

with a low flas p int (e.g gas ln ) A hig pro ortio of road tan er fire has b e

as o iate with switc -loadin

7.1.2 Ig itio s nsitivity and lmitatio s to the s o e of ad ic

Th s n itivity of a flammable atmo p ere to ele tro tatic ig itio d p n s o th

c n e tratio an minimum ig itio e erg (MIE − s e C.6) of th flammable material A

h lpful rule of th mb is that th mo t easiy ig itable vap ur c n e tratio is ap ro imately

d u le th c n e tratio at th lower flammable lmit Be au e of th c n e tratio ef e t, a

mixture mad with a hig MIE material at its mo t easi y ig itable c n e tratio may b more

s n itiv to ig itio than a mixture mad with a low MIE material at a vap ur c n e tratio

that l e o ly ju t within th flammable ran e

For e ui brium vap ur/air mixture create b flammable l q id , th mo t easi y ig itable

vap ur c n e tratio is ty ical y ac ie e at temp rature of ap ro imately 10 °C to 2 °C

ab v th flas p int Flammable l q id of interme iate v lati ty te d to pro u e th ir mo t

easi y ig itable mixture at c mmo ambie t temp rature : s c lq id in lu e tolu n

( las p int 6 °C), pro yl ac tate ( las p int 10 °C) an ac to itrie ( las p int 2 °C)

Th g n ral pre autio s giv n in this c apter are d sig e to pre e t th ig itio of materials

with MIEs of 0,2 mJ or more wh n pre e t at th mo t easi y ig itable vap ur c n e tratio

Th y are th s ap l cable to th mo t easiy ig itable mixture in air of th vap urs of c mmo

flammable l q id s c as parafinic an aromatic s lv nts, h dro arb n fu ls an man

organic s lv nts (s e l st of MIE in T ble C.2) At ty ical ambie t temp rature , th safety

margin are at a minimum wh n han ln flammable lq id of interme iate v lati ty s c as

th s lste ab v In s c o eratio s, partic lar care s o ld th refore b tak n to e s re

that al re omme d d pre autio s are di g ntly fol owe

Alth u h Ex lo io Gro p are n t as ig e o th basis of MIE (s e C.6), th pre autio s

re uire in th pre e c of mo t Ex lo io Gro p I A vap urs are lk ly to b simi ar to th s

giv n h re for MIEs of 0,2 mJ an ab v Ad itio al pre autio s are, h we er, lk ly to b

re uire wh re th atmo p ere ab v th l q id is more s n itiv to ig itio This situatio

wi aris , for e ample, with th mo t readiy ig itable mixture in air of v latie materials that

hav MIEs of le s than 0,2 mJ (mo t Ex lo io Gro p I B an I C materials) or with o y e

-ric mixture Alth u h g n ral ad ic has n t b e d v lo e for th s more s n itiv

atmo p ere , re omme datio s are giv n for a few s e ific activitie Wh re th y are giv n,

th ad itio al pre autio s for th more s n itiv materials are e plcitly id ntifie as s c in

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© IEC 2 17

7.1.3 Chargin me hanisms

Liq id can b c me ele tro tatical y c arg d wh n th y mo e relativ to c ntactin s ld or

if th re are two or more immis ible l q id p as s an th re is mo eme t Th s rayin of

lq id can als create a hig ly c arg d mist or s ray Furth r d tai s of c arg g n ratio

an c arg ac umulatio in l q id are giv n in A.1.3 to A.1.7 (g n ratio ) an A.2.2

(ac umulatio )

7.1.4 Charge a cumulatio an con uctivity cla sific tions

Th le el of c arg ac umulatio in a partic lar lq id, an th refore th ele tro tatic hazard

that can b create , is stro gly d p n e t u o its ele trical c n u tivity an diele tric

c n tant (relativ p rmitivity), ε

r To d s rib th p s ible hazard an as o iate mean of

pre e tio , th c n u tivitie of l q id hav b e clas ifie as fol ows:

For l q id with a diele tric c n tant that is s b tantialy hig er than 2 or for lq id wh s

diele tric c n tant is u k own, th b rd r lmit for low c n u tivity is u ual y s t to 10 pS/m

Th u p r b rd r lmit of me ium c n u tivity remain at 10 0 0 pS/m

NOT 10 pS/m is co sid re suficie t for u k own cases b ca se few, if a y, low co d ctivity lq ids h v a

relativ p rmitivity sig ifica tly hig er th n 4

Hazard u le els of c arg ac umulatio are mo t c mmo ly as o iate with lq id of low

c n u tivity Howe er, th y can o c r with me ium or hig c n u tivity lq id in pro e s s

that pro u e mists or s ray , wh n tran p rtin me ium c n u tivity l q id thro g

in ulatin pip s or d rin two-p as mixin o eratio s

In g n ral, p lar s lv nts s c as alc h ls, k to e an water hav a hig c n u tivity, whi e

c n u tivitie an relaxatio time for a n mb r of lq id are giv n in T ble 7

NOT 1 A more complete lst inclu in a wid r ra g of lq ids a d dielectricco sta t d ta isgiv n in N P -7

NOT 2 Biofu ls a d hydrocarb n fu ls ble d d with biocomp n nts ca h v a wid ra g of co d ctivity

d p n in o th ir comp sitio

NOT 3 Test meth ds for me surin th co d ctivity of a lq id are giv n in e.g A TM D4 0 -9 , DIN 51412-1,

DIN 51412-2 a d ISO 6 9

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