jj study of physiologically required selectivity

6
Wei Zhang i j j J ) j j ) J J j 1 J J J ~ } J J J J I J J 1 j J J .. . ~ ~ I J ~ j j j } ,L Life Science Journal, 2 (1), 2005, Zhang, Physwwgically Required Selectivity Gxfficients of Potentiometric Sensors Study of Physiologically Required Selectivity Coefficients of Potentiometric Sensors in Clinical Assays 26246 Fieldstone Drive, Novi, MI 48108, USA;[email protected] Abstract: Required selectivity mefficients of ion-selective electrodes (ISEs) in physiological analysis are studied based on the ronventional Nirolski- Eisenman equation and a newly proposed ronsistent approach with the worst allowable error (1 % ) . The physiologically required selectivity mefficients from both methods are rompared in this work. The revised ronsistent approach gives out a more reasonable description of selectivity even in case of the unequally charged primary and interfering ions. An Mi+ -selective electrode using ionophore E1H 5504 is tested to measure the selectivity of free Mi+ against the interfering ions in physiological levels. Obviously the required selectivity mefficients derived from the ronsistent approach shows the more accurate description of selectivity than the ronventional one. For evaluating the applicability of ISEs in physiological solution, the ronsistent required selectivity mefficients provide the re<L'iOnablecriteria especially regarding the primaryand interferingionsof differentcharges. [Life ScienceJournal. 2005;2(0 :40 - 45J (ISSN: 1097- 8135). Keywords: selectivity mefficients; ion selective electrodes; magnesium; physiological assay; ETH 5504 1 Introduction ~ I Potentiometric ion-selective electrodes (ISEs) based on neutral inonphore are widely used in clinical assays and abo integrated in diagnostic analyzers[1-3]. The selectivity pattern of any ion-selective electrode is clearly the most important character that often reflects whether a sensor may be reliably employed in analysing the target electrolyte over other coexisting interfering ions. One important application of ISE is detecting electrolyte ion activities in whole blood or serum in which a small mncentration range of electrolyte ex- tremely mandates the measuring accuracy. The ISE should achieve a sufficient selectivity pattern of the pri- mary ion over coexisting interfering ions (semndary ions) to meet the physiological requirement of worst al- lowable error of 1 % [4]. Conventionally, the required selectivity coefficients for physiological analysis are de- rived from the well-known semi-empirical Nimlsky- Eisenman (N-E) equation[5,6]: E - E o RT I ( K jX>tz.lz. ) - i + F n ai + ij aj' } z. z where E is the measured electromotive force (EMF) of the electrode in the sanrple, all mnstant potential mn- tributions are included in E? ; K?j\s the selectivity coef- ficient; Zi and Zj are the charges of primary ion I and interfering ion ] ; ai and aj are the sanrple activities of I and]; and R, T and F have their usual meanings. It is well known that the selectivity coefficient is, in theo- ry, a mnstant parameter for a particular electrode, irre- spective of the charges of primary and interfering ions since K?jt is a function of EO values respectively for two http://www.sciencepub. org (1) ions of interest. Although the N-E equation is, with some excep- tions[7,8], accurate for ions of the sanre charge, the se- lectivity coefficient of ISEs derived from this equation may lead to an inmnsistent description for unequally charged primary ion and interfering ion. For instance, taking primary ion as interfering ion and vice versa does not give the sanre predicted electrcrle potential[9]. In fact, when the monovalent and divalent ions mnsidered as primary and interfering ions, this discrepancy can amount to 8 mV or more than 30 % activity variation. Such discrepancy of selectivity is a serious limitation of N- E equation that may lead to wrong practical predic- tions. A lot of discussions on this problem have been mnducted and many new modification approaches of N- E equation have also been proposed[8,1O,1l]. In 1998, a mnsistent fonnalism was proposed by Zhang et al[9] with modifying the mnventional N-E equation with in- troduction of mnsistent selectivity coefficient KijfJS E = E? + W'ln( aillz; + KiJrcaYz)) (2) where KijfJSis defined as mnsistent selectivity coefficient and KeafJS = ( Kl!'ts ) lIz; ZJ ZJ With this modification, the selectivity coefficient KijfJS is mmpletely independent of the charge number of the ions involved. In measuring ion activity in intercellular fluid sanr- pIes, ion-seleCtive electrode should specifically respond to the activity of target ion with a sufficient discrimina- tion over the CD-existinginterfering ions. The minimum selectivity requirement of ISEs determines the applica- (3) " , I J <' J J j J ) J . 40 . editor@sciencepub. net

Upload: others

Post on 20-Jun-2022

4 views

Category:

Documents


0 download

TRANSCRIPT

Page 1: jJ Study of Physiologically Required Selectivity

Wei Zhang

ijjJ)

jj

)JJj

1

J

J

J

~

}

J

JJJI

J

J1

jJJ...

~~I

J~

jjj

},L

Life Science Journal, 2 (1), 2005, Zhang, Physwwgically Required Selectivity Gxfficients of Potentiometric Sensors

Study of Physiologically Required Selectivity Coefficients

of Potentiometric Sensors in Clinical Assays

26246 FieldstoneDrive, Novi, MI 48108, USA;[email protected]

Abstract: Required selectivity mefficients of ion-selective electrodes (ISEs) in physiological analysis are studied based on the

ronventional Nirolski- Eisenman equation and a newly proposed ronsistent approach with the worst allowable error (1 % ) .The physiologically required selectivity mefficients from both methods are rompared in this work. The revised ronsistent

approach gives out a more reasonable description of selectivity even in case of the unequally charged primary and interfering

ions. An Mi+ -selective electrode using ionophore E1H 5504 is tested to measure the selectivity of free Mi+ against the

interfering ions in physiological levels. Obviously the required selectivity mefficients derived from the ronsistent approach

shows the more accurate description of selectivity than the ronventional one. For evaluating the applicability of ISEs in

physiological solution, the ronsistent required selectivity mefficients provide the re<L'iOnablecriteria especially regarding the

primaryand interferingionsof differentcharges. [Life ScienceJournal. 2005;2(0 :40 - 45J (ISSN: 1097- 8135).

Keywords: selectivity mefficients; ion selective electrodes; magnesium; physiological assay; ETH 5504

1 Introduction

~I

Potentiometric ion-selective electrodes (ISEs)based on neutral inonphore are widely used in clinical

assays and abo integrated in diagnostic analyzers[1-3].The selectivity pattern of any ion-selective electrode isclearly the most important character that often reflects

whether a sensor may be reliably employed in analysingthe target electrolyte over other coexisting interferingions. One important application of ISE is detectingelectrolyte ion activities in whole blood or serum in

which a small mncentration range of electrolyte ex-tremely mandates the measuring accuracy. The ISEshould achieve a sufficient selectivity pattern of the pri-mary ion over coexisting interfering ions (semndaryions) to meet the physiological requirement of worst al-

lowable error of 1 % [4]. Conventionally, the requiredselectivity coefficients for physiological analysis are de-rived from the well-known semi-empirical Nimlsky-Eisenman (N-E) equation[5,6]:

E - E o RT I ( K jX>tz.lz.)- i + F n ai + ij aj' }z.z

where E is the measured electromotive force (EMF) ofthe electrode in the sanrple, all mnstant potential mn-

tributions are included in E? ; K?j\s the selectivity coef-ficient; Zi and Zj are the charges of primary ion I and

interfering ion ] ; ai and aj are the sanrple activities of Iand]; and R, T and F have their usual meanings. Itis well known that the selectivity coefficient is, in theo-ry, a mnstant parameter for a particular electrode, irre-

spective of the charges of primary and interfering ionssince K?jt is a function of EO values respectively for two

http://www.sciencepub. org

(1)

ions of interest.

Although the N-E equation is, with some excep-

tions[7,8], accurate for ions of the sanre charge, the se-lectivity coefficient of ISEs derived from this equationmay lead to an inmnsistent description for unequallycharged primary ion and interfering ion. For instance,taking primary ion as interfering ion and vice versa does

not give the sanre predicted electrcrle potential[9]. Infact, when the monovalent and divalent ions mnsidered

as primary and interfering ions, this discrepancy canamount to 8 mV or more than 30 % activity variation.Such discrepancy of selectivity is a serious limitation of

N-E equation that may lead to wrong practical predic-tions. A lot of discussions on this problem have beenmnducted and many new modification approaches of N-

E equation have also been proposed[8,1O,1l]. In 1998, a

mnsistent fonnalism was proposed by Zhang et al[9]with modifying the mnventional N-E equation with in-

troduction of mnsistent selectivity coefficient KijfJS

E = E? + W'ln( aillz; + KiJrcaYz)) (2)

where KijfJSis defined as mnsistent selectivity coefficientand

KeafJS = (Kl!'ts ) lIz;ZJ ZJ

With this modification, the selectivity coefficient KijfJSis mmpletely independent of the charge number of theions involved.

In measuring ion activity in intercellular fluid sanr-pIes, ion-seleCtive electrode should specifically respondto the activity of target ion with a sufficient discrimina-tion over the CD-existinginterfering ions. The minimum

selectivity requirement of ISEs determines the applica-

(3)

",IJ<'

JJ

jJ

)J

. 40 . editor@sciencepub. net

Page 2: jJ Study of Physiologically Required Selectivity

I (t

r

~..

Life Science Journal, 2 ( 1 ), 2005, Zhang, Physiologimlly Required Selectivity Gefficients of Potentiometric Sensors

~ bility of certain ISEs and the accuracy of assays. Thephysiologicallyrequiredselectivitymefficientsare calcu-lated assuming an allowableerror of 1% (0. 01) in theworst caseof a maximumquantity of interferingion anda minimum quantity of primary ion within physiologicalrange.

Traditionally, the required selectivity mefficientsare calculatedbasedon the a:mventionalNimlsky-Eisen-man equation, assuming an allowable error of 1%(0. 01) in the worst caseof a maximum quantity of in-terfering ion and a minimum quantity of primary ionwithin the physiologicalrange by the following equa-tion[12]:

~lL

...

(..

...

C'"l10.

r..

l (Krt)r equiml~ 0.01 . ai,/min

. )z. za.' }

} ,rnax10. or

..II,.

log(Kr)requim!~ log(O.01 . a~,~)a" }} ,rnax

~ When electrode is calibrated by physiological back-ground S)lutions, the variationsof interfering ion activi-ty around its medium value need to be mnsidered. Thedifference between the activity of the calibrator aj ,cal

d th unkn 1.

(z./z. z./z

)an e own S) utIon aj' aj:d. - aj' j , mn-tributes to the actual interference. Then, Eq. (5) canbe then changed to:

..

IL

l,'-LIl a. ..,nun

log(K\~?)requirOO~ log I 0.01. z/z z/z I (6)aj:d. - aj' }

Obviously, the required selectivity mefficients in Eq.(5) and (6) are inaccurate in case of unequal charge

numbers of the mncemed ions (Zi oF Zj ), which is o-riginated from the discrepancy of the mnventional N-Eequation.

In order to get the mnsistent selectivity criteria forphysiological assay with lSEs, the mnsisterit required

selectivity mefficients are derived from the newly modi-fied N- E equation for a given allowed relative error,

1 % (0. 01), in the measurement of physiological S)lu-tion[2] :

[

lIz.

]

a. ,',nun

log(Kij)requiml ~ log 0.01 . 1kaj,r.rlJx

..

\.I..,

lI.

L

lI.......

~L...

... With the physiological background calibration, the mn-sistent required selectivity mefficient is described as:

liz,

jlog(Kij)requim!~logl 0.01' lIZai'mh,lIz (8)

a } -a. }} ,rnax }

It is shown that Eq. (7) and (8) are obviouslydifferentfrom Eq. (5) and Eq. (6). For primary and

interfering ions of different charges (Zi oF Zj ), the mn-

sistent required selectivity mefficients log ( K\jt) requirOOgives out the reliable cri~eria to determine the applicabil-

..J

~lI

L..~

ll~

http://www.sciencepub. org

ity of lSEs, which gets rid of the discrepancy from the

mnventional N-E equation. In this work, an Mi+ -se-

lective electrode with iononphore EIH 5504[13] wasused to check the selectivity mefficient in physiologicalmeasurements.

(4)

2 Experiments

2.1 ReagentsAll chemicalswere of analytical reagent grade or

higher purity. The followingchemicalswere purchasedfrom Fluka Chemie AG, Buchs, Switzerland: MgClz,eao2, KO, NaO, KTpOPB (potassium tetrakis(4-chlorophenyl)bonite), PVC (poly( vinyl chloride),high molecular weight) and tetrahydrofuran (1HF,distilled prior to use). The Mi+ -selective ionophoreEIH 5504 (1, 3, 5-tris [ 10-(methyl-7, 9-dioxo-6, 10-diazadecyl)benzene]) and the plasticizer EIH 8045(12-( 4-ethylphenyl)dodecyl-2-nitrophenyl-ether) weresynthesizedas describedin['Z,14].Ibubly distilled waterwas used throughout. .

2.2 Membranepreparationand EMF measurementThe PVC-basedMi + -ISE membranewas pre-

pared as describedelsewhere[13,15]using 1 wt% Mi+ -selective ionophore; 155 mol% (relative to theionophore) lipophilicanionic sites KTpOPB; 65 wt%plasticizer, EIH 8045; and 33 wt % PVc. Theworking electrode was assembledby cutting disks of 7mm diameter out of the membrane (thickness is about150 pm). The disk was mounted into a Phillips elec-trode body (ISE - 561, GlasblasereiMoller, ZUrich).A S)lutionof O.1M MgC12was used as the internal fill-

i~ S)!utionfor the Mi + -selectiveelectrode.After mnditioning the electrode in O. 1M MgC12

for 24 hours, EMF measurementswere conductedwithfollowing cell: Hg, I-I&O2 I KO (satd.) MMKO(3.0 M) MM sample S)lution II membrane II internalS)lution (MgClz, 0.1 M) IAgO, Ag.

The calomel reference electrode corresponded tothe free-flowing double-junctiontype[16].The cell po-tential was measuredusing an Apple nGS (Apple Com-puter, Cupertino, CA, USA) equipped with a 7150Digital Multimeter (~lartron Instrumentation, UK).The single-ion molal molar activities in physiologicalelectrolyte situation were calculated using the Pitzerprogram[17].The selectivitymefficientswere measuredbased on the IUPAC recommendedprocedureof sepa-rate S)lutionmethod.All EMF valueswere correctedfor

changes in the liquid-junctionpotential, Ej' using theHendefS)n formalism[18].All potentiometric measure-mentS were performed at ambient temperature(~25°C) .2.3 The main cationsin physiologicalsolution

In physiological fluids, the main cations are Na + ,

L

(5)"

"

(7)

. 41 . editor@sciencepub. net

j

Page 3: jJ Study of Physiologically Required Selectivity

j}JJJ

Life S::ienceJournal, 2 (1); 2005, Zhang, Physiowgically Required Seleaivity QJejficients of Potentiometric Sensors

K+ , ci + and Me?+ which play important roles in.bi-ological functions. In human blood serum, the intercel-lular concentrations of these cations vary in certainrang~" that are listed in Table 1. In calculating the re-quired selectivity coefficients of ISEs for physiologicalassays, an allowable measuring error of 1. 0% is con-sidered with minimum level of a physiological molar ac-tivity. The required selectivity coefficients for detectingmain inorganic cations in physiological solution are cal-culated assuming an allowable error of 1. 0 % at theminimum level of a physiological molar activity of thedetecting ion. The sensors are measured with- andwithout the calibration of physiological ion background(Dc, assuming variation of the background ion molalitylevel around the mean physiological points, Table 1).

The calculation without background calibration(Eq. (5) and Eq. (7» is based on the maximum level

max. level

6.0X 10-4

2.1xlO-4

1.3x 10-3

4.4XlO-4

4.8X 10-3

3.5xlO~3

0.143

0.106

JJ}

;JJJ1.,J1

l1

jJJJJJJ.~

J

)JJJ

J

J,&I

.-

JJ

of interfering ion aj,rrnxand the minimum level of pri-mary ion ai ,min' For obtaining the required selectivitycoefficients with the background calibration (Eq. (6)and Eq. (8», the minimum level of the primary ion

ai,min and the medium level of the interfering ion aj,calis considered for the background calibration.

3 Results and Discussion

3. 1 G)Jnparison of methods for calculating the re-quired selectivity coefficients

The required selectivity coefficients of ISE for dif-ferent primary ions are calculated based on the conven-tional N-E equation and the modified consistent N-E e-quation. The obtained required selectivity coefficientswith and without the physiological background calibra-tion (Eq. (6) and Eq. (8» are compared in Table 2.

Thble1. The main cation levels in physiological 'solution

min. level Medium level

'Fdble 2. Comparison of the required selectivity coefficients of ISEs for measuring the main inorganic cations in physiological solutions,assuming an allowable error of 1 . 0 % at the lower level of the physiological range of the detecting ion. .

Conventional( 1 KiD!) . ' Consistent ( 1 KiD') .

~ ~,~ ~ ~,~

Secondary no with Secondary no withion calibration calibration ion calibration calibration

Cation

Mi+

Ca2+

K+

Na+

PrimaryIon

..~

JI

JjJJ

jjJJ

.L

Mi+

Ca2+

K+

~ Na+

editor@sciencepub. net

~}

~

JJ

iJ

http://www.sciencepub. org . 42 .

Concentration c (M) 3.0X 10-4 4.5X 10-4

molar activity a (M) 1.1XlO-4 1.6xlO-4

Concentration c (M) LOX 10-3 1.15 X 10-3

molar activity a (M) 3.4X 10-4 3.9xlO-4

Concentration c (M) 3.3xlO-3 4.05 X 10-3

molar activity a (M) 2.4X 10-3 2.9xlO-3

Concentration c (M) 0.134 0.138

molar activity a (M) 0.099 0.103

Ca2+ -2.4 -1.5 Ca2+ -2.2 -1.0

K+ -0.9 -0.3 K+ -1.4 -0.6

Na+ -3.8 -2.6 Na+ -2.9 -1.4

Mi+ -1.8 -1.1 Mi+ -1.9 -0.9

K+ -0.6 -0.0 K+ -1. 3 -0.5

Na+ -3.5 -2.3 Na+ -2.8 -1.2

Mi+ -2.8 -1.8 Mi+ -2.8 -1.8

Ca2+ -2.9 -1. 7 Ca2+ -2.9 -1. 7

Na+ -3.6 -2.1 Na+ -3.6 -2.1

Mi+ -1.2 -0.2 Mi+ -1.2 -0.2

Ca2+ -1. 3 -0.1 c".l+ -1. 3 -0.1

K+ -0.5 0.3 K+ -0.5 0.3

Page 4: jJ Study of Physiologically Required Selectivity

[['L

l[l

(

~

~

ttllllllll...ll

tllllll....

L

l

tl[.,.l[lL

[..J,

Life £'ience ]aurrw.l, 2 ( 1), 2005, Zhang, Physiou)gically Required Selectivity Gxfficients of Potenticmwtric Sensors

Because the modified consistent N- E equation re-moves the influence from the ion charge-dependence,the consistent required selectivity coefficient

(Kijn.')requiredreasonably illustrates the preference of thesensor to the primary ion over interfering ions, especial-ly for measuring the unequally charged primary and in-terfering ions. It can be seen from Table 2 and Table 3that when monovalent ion (K + or Na+) is consideredas the primary ion, two methods give out the equal re-

quired selectivity coefficients (Kijn.s )rffjuired

(K~Y) rffjuired'However, the consistent coefficient val-

ues of log (Kijn.s)requiredfor divalent primary ions

(Mi+ or Ca2+) are significantly different from the

conventional ones of log (Kijt)rffjuired' The logarithm of

the required selectivity coefficient for Mi+ over Ca2+changesfrom - 2. 4 to - 2. 2 and the one for Mi +

over K+ from - O.9 to - 1. 4. As well, the log

(Kijt) '1"'1uiredfor Mi + over Na + decrea.'3esfrom - 3. 8to - 2. 9. Such differences lead to the nece&sityof ap-

plying the consistent formulism of the required selectivi-ty coefficient for divalent primary ions.

3.2 Mi + -selective electrode and the required selec-tivity coefficients in physiological analysis

In recent years, studies of developing selective

Mi+ potentiometric sensors have been intensively con-ducted in many groups and the adequate discrimination

between Mi+ and Ca2+ is still the main target[19-21].Suzuki et al[22] synthesised a selective Mi+ ionophoreK22B5 which logarithm of selectivity coefficient of

Mi + over Ca2+ was reported as - 2. 5 measuredwiththe IUP AC recommended separate solution method

(SSM)[23]. The inadequate selectivity against monova-

lent cations (Na + and K+) of this kind of Mi +ionophoresmade the correspondingMi + membraneelectrodes hard to be applied in physiological assays.

Spichiger et al developedan Mi + selective electrodebased on ionophore ETH 5504 which has high selectivi-

ty over ci+ , K+ and Na + while its high lipophilicityprevents ETH 5504 leaching from plasticized PVCmembrane.So far, many Mi + selective microelec-

trodes basedon variousMi + ionophores have also been

reported in measuring the physiological systems[24-28].In serum samples, the intercellular Mi+ molar

activity range (0. 46 ~ 0.66 M) is much lower thatCa2+ level range (1. 01~ 1. 26 M) and the discrimina-tion of Mi+ over Ca2+ is very critic for accurate mea-

surement of Mi+ in physiological assays. The selectiv-

ity coefficients of Mi+ -selective electrode based onionophore ETH 5504 was determined according to theIUPAC recommended separate solution method

.ll

(l

f

http://www.sciencepub. org

(SSM)[23] as well as the newly modified consistentSSM[9].

In order to ensure the selectivity coefficients of

Mi+ -ISEs to reflect the "worst case" in physiologicalsituation, the minimlllll level of Mi + and the maxi-mlllll levels of interfering ions were used in calculatingthe selectivity coefficients. EMF values of the minimlllll

physiological level Mi+ were compared with that ofmaximlllll physiological levels of other interfering ions,

Ca2+ ,Na+ and K+ separately (Figure 1). Two sets

selectivitycoefficientsfor Mi+ - ISE, logK~.J and

logK~:J , were calculated based on both the conven-tional N-E method and the modified consistent N- E

method. As shown in Figure 2, the selectivity coeffi-

cients (SSM) of Mi + -selective electrode based on bothmethods were obtained by using electrolyte solutions ofstandard concentration (0. 1 M) and of physiologicalmedilllll levels of primary and interfering ions (Table1).

It can be seen from the results in Figure 2 that the

selectivity pattern of Mi+ -selective electrode withETH 5504 were measured based on both approaches ofthe conventional and the modified consistent approach-

es. The selectivityof Mi + against ci + reaches - 1. 0~ - 1. 8 with conventionalSSM approach and - 1.0~ -1. 2 with the consistent method. llith values sat-

isfied the physiologically required selectivity coefficientscalculated from Eq. (6) (conventional approach,

loge Kijt) rffjuired= - 1. 5) and Eq. (8) (consistent ap-

proach, log( Kijn.s)rffjuired= - 1. 0) with physiologicalbackground calibration. However, for the direct mea-surements without background calibration, the selectiv-ity still has space to improve. Regarding the interferingmonovalent cations of K+ and Na+, this Mi +- ISEshowed the adequate selectivity over K+ even for non-calibrationmeasurementof Mi + either with conven-

tional method (log( Kijt) rffjuired= - O.9) and consistentmethod (log ( Kijn.s)required= ~ 1. 4). However, thediscriminationagainst Na+ of this Mi + -ISE also re-quires the physiological background calibration so as to

satisfy the physiological requirement (with background

calibration, log (Kijt) required= - 2. 6 andloge K'jjn.s)required= - 1. 4). According to this compari-son, it is obviousthat the physiologicalbackgroundcali-bration is really needed for using the Mi+ -ISE withionophore ETH 5504 to measure free intercellularMi + level.This requirement can predict the necessaryenhancing space of selectivity pattern for developing fu-ture Mi + -ISEs in direct measurements in physiologicalassays.

I.

. 43 . editor@sciencepub. net

Page 5: jJ Study of Physiologically Required Selectivity

)]

Life S::ienceJournal, 2 (1), 2005, Zhang, Physiologically Required Selrrtivity Qyefjicients of Potentimnetnc Sensors J)

jj

~

JJJ)jiJ

J

J

JJ)JjJ,J

~

JJ

J

J

J,J~

JJJ

J

Figure 1. Selectivity measurement in the "worst case" for Mi+ -ISE in physiological electrolyte situationA:O,3rnMMgC~; B:1.3rnMCaCI2; C:4,SrnMKCl; D:140rnMNaCL

0 M

~~ -2..s ca~K ~

,/Na "" /~"'---_..--

-1

-3

-4

-5 (a)conventional N-E (h)consistent N-E ,IJ

JJJ}..

j

j.L

-6

~0~U)U)

~.."'6JJ0

],.>...c;:..~U)U)

~

.....'""-E.~;:c"....'Scr"....

~

~"0c:

;:c".~6-"....

M

~K~~Ca ~~//Na

Figure 2. The comparison of the Mi + -selectivity coefficients with required selectivity coefficients.

(a) Conventional N-E method; (b).. Consistent N-E method.

4 Q)nclusion

-In conclusion, the physiologically required selec-

tivity coefficients of ISEs for physiological analysis werestudied by comparing the conventional N- E method andthe modified consistent N-E method. The modified

consistent method eliminates the discrepancies originat-ed from the conventional N-E equation for unequallycharged primary and interfering ions. Indeed, the con-sistent required selectivity coefficients for the divalent

primary ion (Mi+ or ea2+) gives out a more accurate

calculation that the conventional one and provides a rea-S]nable criteria for evaluating the applicability of ISEs in

.http; / /www.sciencepub. org

physiological assays. However for the monovalent pri-

mary ion (K+ or Na + ), the required selectivity coeffi-cients calculated with two methods are identical. For

comparing the perfonnances of ISE in the physiologicalS]lution with the required selectivity pattern, the elec-trode was checked in the" worst case" of minimum level

of primary ion and maximum level of interfering ion inphysiological S]lution. Indeed, the modified consistentrequired selectivity coefficients are more accurate thanthe ones derived from the conventional N-E equation,which provides the more reliable criteria for evaluatingthe applicability of ion-selective electrodes in physiologi-cal assays.

~"J"J)

1

J

j]

. 44 . editor@sciencepub. net

'"'"""-E

4 l'6JJ "0

i] 03 :? 5]

,. .">. ".....-a. ....

'SS.

'Scr

2 -1cr "" ....

U)U) ....U)

Page 6: jJ Study of Physiologically Required Selectivity

[[t[ll...l

tll...

lt(

t~

llllI\

llL.~

l,llllI'-I~~

Life Science Journal, 2 (1), 2005, ZIulng, Physiologically Required Selectivity Gxfficients of PotentiO/11£tricSensors

Correspondence to:Wei Zhang26246 Fieldstone Drive

Novi, Michigan 48108, USAllelephone:734-355-9682Email: [email protected]

References1. Bakker E, Prestch E. Anal Chern 2002:74;420A.

2. Spichiger UE, Chemical Se=rs and Bi==rs for Medicaland Biological Applications. Wiley VCH, Weinheim, Ger-many 1998. .

3. Bakker E, Diamond D, Lewenstam A, Pretsch E. AnalChim Acta 1999: 393 ; 11.

4.Spichiger UE, Eugster R, Haase E, Rumpf G, Gehrig P,Schmid A, Rusterholz B, Simon W. Fresenius J Anal Chern1991:341;727.

5. Nicolsky BP. Zh Fiz Khim 1937; 10;495.6. Eisenman G, Rudin m, Casdy Ju. Science 1957: 126;

831.7. Umezawa G, Umezawa K, S3.toH. Pure Appl Chern 1995;

67;507.8. Bakker- E, Meruva RK, Pretsch E, Meyerhoff M. Anal

Chern 1994:66;3021.9. Zhang W, Fakler A, Demuth C, Spichiger UE. Anal Chim

Acta 1998:375;211.10. Cattrall RW, Drew DM. Anal Chim Acta 1975: 77 ;9.11. Bagg], Vinen R. Anal Chern 1972: 44 ; 1773.12. Spichiger UE. ETH Thesis No. 8803, 1989.

Ll

tllLII"

ltll.

ll.J..

J.~

tt http;/ /www.sciencepub. org

13. Zhang W, Jermy L, Spichiger UE. Analytical Sciences2000;16;11.

14. Eugster R, Rosatzin T, Rusterholz B, Aebersold B, Pedraz-za U, Ruegg D, Schmid A, Spichiger UE, Simon. AnalChim Acta 1993:289; 1.

15. Oesch U, Br=ka Z, Simon W. Anal Chern 1986; 58;2289.

16. DolmerRE, WegmannD, Mon WE, SimonW. kal Chern1986:58;2585.

17. Pitzer KS. Geochim Cosmochim Acta 1984:48;723.18. Henderson P. Zeitschrift f(ir Physikalische Chemie 1907: 59;

118.

19. Maj-Zurawska M. Chemia Analityczna 1997:42; 187.20. Toth K, Lindner E, Horvath M, Jeney J, Pungor E, Bitter

I, Agai B, Toke L. Electroana1ysis 1993:5;781.21. Spichiger UE. Electroana11993:5;739.22. Suzuki K, .Watanabe K, Matsumoto Y, Kobayashi M, S3.to

S, Siswanta D, Hisamoto H. Anal Chern 1995; 67 ;324.23. Guilbault GG, Durst RA, Frant MS, Freiser H, Hansen

EH, Light TS, Pungor E, Rechniz G, Rice NM, RohmTJ, Simon W, Thomas DR. Pure Appl Chern 1976: 48;129.

24. Zhang W, Trutmarm AC, Luethi D, McGuiganJAS. Mag-nesium Bulletin 1995:17;125.

25.Gunzel D, Schlue WR. Biomatals 2002;15;237.26. Zhang X, Fakler A, Spichiger UE. Electroana11998: 10;

1174.

27. Gunzel D, Muller A, Durry S, Schlue WR. ElectrochimicaActa 1999;44;3785.

28. Spichiger UE, Fakler A. Electrochimica Acta 1997; 42;3137.

~

. 45 . editor@sciencepub. net