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Standard(s): IEC 60112/2003 No. Year
( W; d. _) f$ T: I5 A$ @Ed. 4.0: J$ m `& W$ _7 V1 d0 I
DSH
( U0 i) b" a) `# x- |) q07248 `- q/ ]: J+ n6 ^
2008
0 c# V5 \# w) G# lCategories: Various, General
2 {" _/ G) t) z. A S& x9 cSubclause(s): 7.3
# H5 D& r. ~" r7 _! m( _Developed by: WG4- x# w! v5 C9 v) v! u, f3 X9 \
Subject: Measurement of+ m) e* e# g: q- Y- F% ?& H
conductivity
8 b/ b1 [: O1 \7 KKey words:
; G6 n8 ?4 h+ {) `$ W6 d- Tracking solution
6 ^; [# \3 {) p N$ \# y5 j# O- Conductivity
/ m$ x/ H. ]5 h- IEC 60589
/ O% Z6 `7 x1 R2 V- E" J5 XDecision approved at the9 W+ F! J( t# C
46th CTL Plenary Meeting,
" ?; x/ M4 W, K# Q1 ein 2009
# o) W: p( T' V! p2 g7 g; hQuestion:
4 V _7 u* m& H8 |8 U1 }5 [Clause 7.3 requires that the conductivity of the tracking test solution “be measured with alternating, P4 Q" ? g6 ?5 K8 n
voltage at a frequency in the range 1 kHz to 2 kHz. The procedure is described in IEC 60589”.' \) w0 A9 h( u
The procedure in IEC 60589 utilises conical flasks with reflux condensors, platinised platinum8 k, ~ B; Q6 _/ x% A7 d n2 {
electrodes, a conductivity cell and a resistance bridge. This appears to be a chemical standard rather
$ s5 I" F# H4 @; [; Q! f3 M8 u# j2 pthan an appropriate electrical test laboratory measurement technique.5 C4 w; Y) [# R* A$ g
Are CBTL:& }; r& {' V4 }4 v: h
- (a) expected to use this method of measurement for solution conductivity; or) y \. C+ ?! W! s
- (b) can a suitable conductivity meter with a measurement frequency in the range 1 kHz to 2 kHz
; L* J2 i' [! H/ W: Z! fbe used; or( F/ a5 h4 W' D' e& j
- (c) can any suitable conductivity meter (different measurement range) be used.
1 x* V% X; s! W- }, ZDecision:- |* m7 m* F, c$ w
The Group decided that the “use of any appropriate conductivity meter with sufficient accuracy and( m& o$ u% E' R! K; @7 f: K6 N8 M
uncertainty including the probe” is the only practical one - item (c) above.$ P7 p6 d$ h8 r: k( Z/ x" q" D
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