AGFA T2000 XL appendix Elect romagnet ic Int erference

Models: T2000 XL

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n Die B e lü f t u n g s ö f f n u n g e n d ie n e n z u r L u f t z irk u lat io n d ie d as G e rät v o r

Üb e rh it z u n g s c h ü t z . S o rg e n S ie d af ü r, d aß d ie s e Ö f f n u n g e n n ic h t ab g e d e c k t we rd e n .

n Die Ne t z an s c h u lßs t e c k d o s e mu ß au s G rü n d e n d e r e le k t ris c h e n S ic h e rh e it e in e n S c h u t z le it e rk o n t ak t h ab e n .

n Du rc h d ie L ü f t u n g s ö f f n u n g e n d ü rf e n n ie mals G e g e n s t än d e o d e r

Flü s s ig k e it e n in d as G e rät g e lan g e n . Die s k ö n n t e e in e n B ran d b z w. e le k t ris c h e n S c h lag au s lö s e n .

n Ö f f n e n S ie n ie mals d as G e rät . Das G e rät d arf au s G rü n d e n d e r e le k t ris c h e n S ic h e rh e it n u r v o n au t h o ris ie rt e m S e rv ic e p e rs o n al g e ö f f n e t we rd e n .

nDie S t e c k d o s e s o llt e n ah e d e m G e rät u n d le ic h t z u g än g lic h s e in .

Elect romagnet ic Int erference

Du o S c an T2 0 0 0 X L is d e s ig n e d t o c o mp ly wit h :

nE N5 0 0 8 1 -1

nE N5 0 0 8 2 -1

nFCC 2 0 7 1 8 , p art 1 5 , s u b p art B , c las s B

Fe de ra l Co mmunic a tio ns Co mmis s io n Ra dio Fre que nc y Inte rfe re nc e S ta te me nt .

v No t e : Th is e q u ip me n t h as b e e n t e s t e d an d f o u n d t o c o mp ly wit h t h e limit s f o r a Clas s B d ig it al d e v ic e , p u rs u an t t o P art 1 5 o f t h e FCC Ru le s . Th e s e limit s are d e s ig n e d t o p ro v id e re as o n ab le p ro t e c t io n ag ain s t h armf u l in t e rf e re n c e wh e n t h e e q u ip me n t is o p e rat e d in a re s id e n t ial in s t allat io n . Th is e q u ip me n t g e n e rat e s , u s e s , an d c an rad iat e rad io f re q u e n c y e n e rg y an d if n o t in s t alle d an d u s e d in ac c o rd an c e wit h t h e in s t ru c t io n man u al may c au s e h armf u l

in t e rf e re n c e t o rad io c o mmu n ic at io n s . Ho we v e r, t h e re is n o g u aran t e e t h at in t e rf e re n c e will n o t o c c u r in a p art ic u lar in s t allat io n . I f t h is e q u ip me n t d o e s c au s e h armf u l in t e rf e re n c e t o rad io o r t e le v is io n re c e p t io n , wh ic h c an b e

d e t e rmin e d b y t u rn in g t h e e q u ip me n t o f f an d o n , t h e u s e r is e n c o u rag e d t o t ry t o c o rre c t t h e in t e rf e re n c e b y o n e o r mo re o f t h e f o llo win g me as u re s :

nRe o rie n t o r re lo c at e t h e re c e iv in g an t e n n a.

n I n c re as e t h e s e p arat io n b e t we e n t h e e q u ip me n t an d re c e iv e r.

n

Co n n e c t t h e e q u ip me n t in t o an o u t le t o n a c irc u it d if f e re n t f ro m t h at t o wh ic h

 

t h e re c e iv e r is c o n n e c t e d .

n

Co n s u lt t h e d e ale r o r an e x p e rie n c e d rad io TV t e c h n ic ian f o r h e lp .

A p p e n d i x C — Du o S c a n T2 0 0 0 X L Re g u l a t i o n Co mp l i a n c e 52

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AGFA T2000 XL appendix Elect romagnet ic Int erference