ASTM E1511-1993(2010) Standard Practice for Testing Conductivity Detectors Used in Liquid and Ion Chromatography《液相和离子色谱法用试验导电检波器的标准操作规程》.pdf
《ASTM E1511-1993(2010) Standard Practice for Testing Conductivity Detectors Used in Liquid and Ion Chromatography《液相和离子色谱法用试验导电检波器的标准操作规程》.pdf》由会员分享,可在线阅读,更多相关《ASTM E1511-1993(2010) Standard Practice for Testing Conductivity Detectors Used in Liquid and Ion Chromatography《液相和离子色谱法用试验导电检波器的标准操作规程》.pdf(6页珍藏版)》请在麦多课文档分享上搜索。
1、Designation: E1511 93 (Reapproved 2010)Standard Practice forTesting Conductivity Detectors Used in Liquid and IonChromatography1This standard is issued under the fixed designation E1511; the number immediately following the designation indicates the year oforiginal adoption or, in the case of revisi
2、on, the year of last revision. A number in parentheses indicates the year of last reapproval. Asuperscript epsilon () indicates an editorial change since the last revision or reapproval.1. Scope1.1 This practice covers the testing of the performance ofconductivity detectors used as the detection com
3、ponent of aliquid or ion chromatography system.1.2 The values stated in SI units are to be regarded asstandard. No other units of measurement are included in thisstandard.2. Referenced Documents2.1 ASTM Standards:2E1151 Practice for Ion Chromatography Terms and Rela-tionships3. Terminology3.1 See Pr
4、actice E1151.3.2 Definitions:3.2.1 cell constantthe cell constant (K) of a conductivitycell is equal to 1/A,sok = GK.3.2.1.1 DiscussionIf the cell constant of the flow-throughcell used is equal to one, then the conductivity equals theconductance. Although the cell constant is often specified forcond
5、uctivity detectors, there is little practical value in knowingthe constant as long as the detector is properly calibrated forconductivity.3.2.2 conductancethe conductance (G) of a solution is theinverse of the resistance measured between two electrodes in acell, expressed in units of siemens (S), eq
6、ual to inverse ohms.3.2.2.1 DiscussionThe term resistance refers specificallyto the dc resistance to ionic current, independent of thecapacitive reactance at the interfaces between the electrodesand the solution.3.2.3 conductivitysince the conductance is dependent onboth the conductive properties of
7、 the solution and on thedimensions of the electrodes and the cell, the conductivity (k)of the solution is defined to be independent of electrode andcell dimensions. Specifically,k5G1A(1)where:1 = the distance between two planer disk electrodes, andA = the electrodes surface area.3.2.3.1 DiscussionIn
8、 liquid and ion chromatography, celldimensions are commonly measured in centimetres, so theunits of k are S/cm. (Alternatively, the SI units of S/m may beused. S/m = 100 S/cm.)3.2.4 driftthe average slope of the noise envelope ex-pressed in nano siemens per centimetre per hour as measuredover a peri
9、od of 1 h.3.2.5 equivalent conductivityof an ionic solute, the con-tribution of the solute to the total conductivity of the solution,measured in microsiemens per centimetre, divided by itsconcentration in milliequivalents/litre.3.2.6 flow dependence ratethe change in measured con-ductivity as a func
10、tion of flow rate.3.2.7 limiting equivalent conductivityof an ionic solute,its equivalent conductivity extrapolated to infinite dilution.3.2.8 linear rangeof a conductivity detector for a givensolute in a specific solvent, the concentration range of solutefor which the detector response factor is wi
11、thin 5 % of theresponse factor in the middle of the range as determined fromthe linearity plot specified in Section 11.3.2.8.1 DiscussionThe lower limit may be limited bynoise, and the upper limit by deviation from linearity. (Theupper limit may instead be limited by the maximum full-scaledeflection
12、 on the detectors least sensitive output range.)3.2.9 long-term noisethe maximum amplitude in nanosiemens per centimetre for all random variations of the detectoroutput of frequencies between 2 and 60 cycles per hour.3.2.9.1 DiscussionLong-term noise represents noise thatcan be mistaken for eluting
13、peaks.1This practice is under the jurisdiction of ASTM Committee E13 on MolecularSpectroscopy and Separation Science and is the direct responsibility of Subcom-mittee E13.19 on Separation Science.Current edition approved Nov. 1, 2010. Published November 2010. Originallyapproved in 1993. Last previou
14、s edition approved in 2005 as E1511 - 93(2005).DOI: 10.1520/E1511-93R10.2For referenced ASTM standards, visit the ASTM website, www.astm.org, orcontact ASTM Customer Service at serviceastm.org. For Annual Book of ASTMStandards volume information, refer to the standards Document Summary page onthe AS
15、TM website.1Copyright ASTM International, 100 Barr Harbor Drive, PO Box C700, West Conshohocken, PA 19428-2959, United States.3.2.10 minimum detectabilityof a conductivity detector,that concentration of solute in a specific solvent that corre-sponds to twice the short-term noise.3.2.10.1 DiscussionB
16、ecause of the difficulty of pumpingsolvents through the chromatographic system without anycontamination of the solvents from the system, this quantitycan only be measured with solutes retained by a column. Sinceminimum detectability is dependent on the chromatographicsystem used, it is not measured
17、in this practice. However, if theminimum detectability of a solute is measured on one systemwith one detector, the minimum detectability can be predictedwhen other detectors are tested on the same system bycomparing the measured values of short-term noise.3.2.11 response factorof a conductivity dete
18、ctor, the mea-sured conductivity response of a solute divided by the soluteconcentration.3.2.12 response time of the detectorthe time required forthe output of the detector to change from 10 to 90 % of the newequilibrium value when the composition of the eluent ischanged in a stepwise manner, within
19、 the linear range of thedetector.3.2.12.1 DiscussionAslow response time has the effect oflimiting resolution for efficient peaks such as early elutingpeaks and those from highly efficient columns or microborecolumns. Response time is generally dependent on threefactors: (a) cell volume, (b) volume o
20、f heat transfer tubingleading to the cell, and (c) electronic filtering of the output.3.2.13 sensitivitythe detector response divided by concen-tration, which is also the response factor (11.1.1).3.2.13.1 DiscussionSensitivity is therefore by definitionthe same for all properly calibrated conductivi
21、ty detectors.(Sensitivity is often confused with minimum detectability,which is dependent on both sensitivity and noise.) Therefore,the calibration of the detector should be measured, and ifnecessary, adjusted. Follow the manufacturers procedure forcalibrating the detector. The procedure in Section
22、9 is used bymany manufacturers and is useful for the tests in this practice.3.2.14 short-term noisethe maximum amplitude in nanosiemens per centimetre for all random variations of the detectoroutput of a frequency greater than one cycle per minute.3.2.14.1 DiscussionShort-term noise determines thesm
23、allest signal detectable by a conductivity detector, limits theprecision available for the determination of trace samples, andmay set the lower limit of linearity.4. Summary of Practice4.1 Four different tests are performed to characterize adetector.4.1.1 Noise and drift are measured while a solutio
24、n isflowing through the detector cell. The test is performed usingtwo different solutions: deionized water (DI) and 1 mMpotassium chloride (KCl).4.1.2 Linear range is determined by preparing a plot ofresponse factor versus the log of solute concentration usingstandard solutions of KCl and hydrochlor
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