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Potentiometry  and Ion-Selective Electrodes Potentiometry  and Ion-Selective Electrodes

Potentiometry and Ion-Selective Electrodes - PowerPoint Presentation

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Potentiometry and Ion-Selective Electrodes - PPT Presentation

1 Lecture 2 If metals are the only useful materials for constructing indicator electrodes then there would be few useful applications of potentiometry In 1901 Haber Fritz discovered the existence of a change in potential across a glass membrane when its two sides are in solutions of diffe ID: 674854

potential ion selective membrane ion potential membrane selective activity solution electrode analyte electrodes cell reference equation selectivity ions constant

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Slide1

Potentiometry and Ion-Selective Electrodes

1

Lecture 2Slide2

If metals are the only useful materials for constructing indicator electrodes, then there would be few useful applications of potentiometry

. In 1901 , Haber Fritz discovered the existence of a change in potential across a glass membrane when its two sides are in solutions of different acidity. The existence of this membrane potential led to the development of a whole new class of indicator electrodes called ion-selective electrodes (ISEs).

2

Emergence of Ion-Selective ElectrodesSlide3

In addition to the glass pH electrode, ion-selective electrodes are available for a wide range of ions. It is also possible to construct a membrane electrode for a neutral analyte

by using a chemical reaction to generate an ion that can be monitored with an ion-selective electrode. The development of new membrane electrodes continues to be an active area of research.

3Slide4

A Typical Ion-Selective electrode

- Made from an ion-conducting membrane (ion-exchange material that allows ions of one electrical charge to pass through)

- Internal Reference electrode

- Internal solution (solution inside electrode) contains ion of interest with constant activity

- Ion of interest is usually mixed with membrane material

- Membrane is nonporous and water insoluble

4Slide5

The potential difference between the internal reference electrode and the internal membrane surface is constant, as fixed by its design (e.g. the nature of the reference electrode and the activity (

ai,reference) of the reference solution). Alternatively, the potential difference, which appears between the external surface of the membrane and the sample solution (

E

memb

), depends upon the activity of the target ion (a

i

,

solution

).

The potential difference across the membrane is described by the

Nernst

equation:

5Slide6

6

Schematic diagram of an electrochemical cell for potentiometric

measurementsSlide7

Since the electrochemical cell includes two reference electrodes: one immersed in the ion-selective electrode’s internal solution and one in the sample, the cell potential, therefore, is:

Ecell =

E

ref

(int

)

E

ref

(sample)

+ Emem

+

Ej

7Slide8

- [Analyte ion,

i] inside the electrode ≠

[analyte ion,

i] outside the

electrode.

-

Develop a

potential difference across the membrane

Generally (at 25

o

C

)

- 10-fold change in activity implies 59/z

i

mV change in

E, for singly charged ions.

-

z

i

is the charge on the

analyte

ion (negative for anions)- zi = +1 for K+, zi = +2 for Ca2+, zi = -2 for CO32-

ION-SELECTIVE ELECTRODES (ISE)

8Slide9

Debye-Hückel

Equation

- Relates activity coefficients to ionic strength (at 25

o

C

)

α

= size of

hydrated ion

in

picometers

(1 pm = 10

-12

m

)

µ = ionic strength

9

Activity

(

a

i

) rather than

molarity

is measured by

ISEs

-

z

i

= ionic charge

(±)

a

i

=

γ

i

c

i

where

γ

i

= activity coefficient (between 0 and 1)Slide10

Ionic strength

- A measure of the concentration of all ions

in solution

with

their charges taken into account

10Slide11

11

Three main groups of ISEs

- Glass membrane electrodes

- Liquid membrane electrodes

Solid state electrodes

In addition to other types of ion-selective electrodesSlide12

The side figure shows a typical potentiometric

electrochemical cell equipped with an ion-selective electrode. The short hand notation for this cell is written below.

where the ion-selective membrane is shown by the vertical slash separating the two solutions containing analyte (the sample solution) and the ion-selective electrode’s internal solution.

12

Membrane PotentialsSlide13

The electrochemical cell includes two reference electrodes: one immersed in the ion-selective electrode’s internal solution and one in the sample. The cell potential, therefore, is:

Ecell

=

E

ref(int

)

E

ref

(sample)

+ Ememb

+

Ej

For an analyte ion A which has an activity a

A

, the membrane potential can be written as:

13

Since the activity of the

analyte

ion in the internal solution is constant.Slide14

where Ememb

is the potential across the membrane. Because the junction potential and the potential of the two reference electrodes are constant, any change in Ecell

is a result of a change in the membrane’s potential.

The

analyte’s

interaction with the membrane generates a membrane potential if there is a difference in its activity on the membrane’s two sides.

14Slide15

Asymmetry Potential

When a membrane of an ion selective electrode is immersed in a solution having the same concentration as that of the internal filling solution, then there should be no measurable potential difference. If such a potential exists, this potential is referred to as asymmetry potential. It is usually few mV (can be up to 40 mV).

15Slide16

16Slide17

Current is carried through the membrane by the movement of either the analyte

or an ion already present in the membrane’s matrix. The membrane potential is given by the following Nernst-like equation:

where (

a

A

)

samp

is the

analyte’s

concentration in the sample, (

aA)int

is the concentration of

analyte in the ion-selective electrode’s internal solution, and z is the

analyte’s charge. Ideally, E

memb

is zero when (

a

A

)

int

= (

a

A

)samp. The term Easym, is an asymmetry potential, which accounts for the fact that Ememb is usually not zero under these conditions. 17Slide18

Substitution, assuming a temperature of 25 o

C, and a constant analyte concentration in the fill solution, and rearranging gives:

where K is a constant that includes the potentials of the two reference electrodes, the junction potentials, the asymmetry potential, and the

analyte's

activity term in the internal solution.

The equation above is a general equation and applies to all types of ion-selective electrodes.

18Slide19

Look at the Ca

2+ ISE which uses a phosphate based

ionophore

:

Employs

cation

-exchanger that has high affinity (

diester

of phosphoric acid)

The

basis is the ability of phosphate ions to form stable

complexes

with calcium ions

Selective towards

calcium

Inner solution is a

fixed concentration of

calcium

chloride

The Cell

potential is given

by:

What happens at the membrane surface?

19Slide20

20Slide21

Sodium ion ISE

The specific glass used in the early work for constructing sodium ion selective electrodes refere

to

Eisenman

, and uses his NAS11-18 glass, containing 11mol of Na

2

O, 18mol of Al

2

O

3

and 71mol of SiO2. The electrode was essentially a slightly modified glass electrode with a membrane thickness of around 0.25mm.

In brief, it would appear that the amorphous crystal lattice of glass contains numerous regions into which sodium ions fit. The lattice has enough gaps in it (perhaps about 4 angstrom wide) that sodium ions are able to migrate from gap to gap. Perhaps no single ion would ever migrate across the comparatively very large width of the entire membrane, but enough of them change position that some end up in the reference solution inside the electrode, and - more importantly - a potential difference develops across the membrane, which is proportional to the

cation

concentration in the sample solution.

21Slide22

22Slide23

A Li

+

ISE

23Slide24

Potassium ion ISE

The potassium-selective electrode features a PVC membrane doped with a potassium-selective ionophore. Radiometer do not specify which, but

valinomycin

is historically a popular choice. It is a

macrolide antibiotic with a ring-shaped molecule (the image below,

valinomycin

is the prototypical model

ionophore

).

The potassium ion measures about 1.33 angstrom across, and just about fits the cavity as depicted, which is between 2.7 and 3.3 angstrom across. An electrode with a

valinomycin

-impregnated PVC membrane can be up to 5000 times more selective for potassium when compared to sodium.

24Slide25

25Slide26

26Slide27

General Scheme of

Cation

Selective Membrane

27Slide28

A Chloride ISE

Traditionally, quaternary ammonium salts have been used as a chloride-selective ionophore admixture into PVC, together

wih

a

plastiiser like o

-

nitrophenyl

octyl

ether (NPOE). However, researchers and clinicians complained that these membranes showed poor selectivity over

salicylate anions and heparin (both with a high anionic charge). Subsequently,

ionophores

such as mercury(n

) EDTA and indium porphyrins were developed. Less rare-earth-dependent solutions today include neutral carriers as tridodecylmethylammonium chloride (TDMAC).

28Slide29

29Slide30

selectivity of membranesNicolsky-Eisenman

equation

A membrane potential develops due to physiochemical interactions between the

analyte

and active sites on the membrane’s surface. Because the signal depends on this physiochemical process, most membranes are not selective toward a single

analyte

. Instead, the membrane potential is proportional to the concentration of each ion that interacts with the membrane’s active sites. We can rewrite the potential equation above to include the contribution of an

interferent

, B, to the potential, and study the case where the same potential is obtained using different activities of

analyte

and

interferent

.

30Slide31

31Slide32

32Slide33

(known as Nicolsky-Eisenman equation) where

zA and z

B

are the charges of the analyte and the

interferent, and K

AB

is a selectivity coefficient accounting for the relative response of the

interferent

. The selectivity coefficient is defined as:

where

a

A

and aB are the activities of analyte

and

interferent

yielding identical cell potentials. When the selectivity

coeffcient

is 1.00 the membrane responds equally to the

analyte

and the

interferent

.

33Slide34

Generally, for analyte

i and several interferents(j), the Nicolsky-Eisenman

equation can be written as:

where

E

mV

is the measured potential; the constant includes the standard potential of the electrode, the reference electrode potential, the asymmetry potential, and the junction potential.

34Slide35

1. Fixed interference method

The potential of a cell comprising an ion-selective electrode and a reference electrode is measured with solutions of constant level of interference,

a

B

, and varying activity of the primary ion,

a

A

. The potential values obtained are plotted versus the activity of the primary ion. The intersection of the extrapolation of the linear portions of this curve will indicate the value of

a

A

which is to be used to calculate K

AB

from the equation:

where both

z

A

and

z

B

have the same signs, positive or negative. Slide36

The right Diagram showing the experimental determination of an ion-selective electrode’s

selectivity for an

analyte

. The activity of

analyte

corresponding to the intersection of the two

lin

-

ear portions of the curve, (

a

A)

inter

, produces a cell potential identical to that of the interferent

. The equation for the selectivity coefficient, KA,I, is shown in red.

36Slide37

Selectivity coefficients for most commercially available ion-selective electrodes are provided by the manufacturer. If the selectivity coefficient is not known, it is easy to determine its value experimentally by preparing a series of solutions, each containing the same activity of

interferent, (aI

)

add

, but a different activity of analyte. As shown in figure, a plot of cell potential versus the log of the

analyte’s

activity has two distinct linear regions.

37Slide38

When the analyte’s activity is

signifcantly larger than KA,I*(a

I

)

add, the potential is a linear function of log(a

A

). If K

A,I

*(

a

I)add is

signifcantly

larger than the analyte’s

activity, however, the cell potential remains constant. The activity of analyte and interferent

at the intersection of these two linear regions is used to calculate K

A,I

. It should be indicated that there are several other methods to calculate K

A,I.

38Slide39

2. Fixed primary ion method (FPM)

The potential of a cell comprising an ion-selective electrode and a reference electrode (ISE cell) is measured for solutions of constant activity of the primary ion,

a

A

, and varying activity of the interfering ion, a

B

.

The potential values obtained are plotted vs. the logarithm of the activity of the interfering ion. The intersection of the extrapolated linear portions of this plot indicates the value of

a

B

that is to be used to calculate K

AB

from the following equation:

39Slide40

3. Two solutions method (TSM)

This method involves measuring potentials of a pure solution of the primary ion, E

A

, and a mixed solution containing the primary and interfering ions, E

A+B. The

potentiometric

selectivity coefficient is calculated by inserting the value of the potential difference, ∆E = E

A+B

– E

A

, into the following equation:

40Slide41

4. Matched potential method (MPM)

This method does not depend on the

Nicolsky–Eisenman

equation at all.

In this method, the potentiometric

selectivity coefficient is defined as the activity ratio of primary and interfering ions that give the same potential change under identical conditions.

At first, a known activity (

a

A

') of the primary ion solution is added into a reference solution that contains a fixed activity (

a

A

) of primary ions, and the corresponding potential change (∆E) is recorded. Next, a solution of an interfering ion is added to the reference solution until the same potential change (∆E) is recorded. The selectivity coefficient is calculated from the relation:

41Slide42

IIa. Separate solution method

The potential of a cell comprising an ion-selective electrode and a reference electrode is measured with each of two separate solutions, one containing the ion A at the activity

a

A

(but no B), the other containing the ion B at the same activity

a

B

=

a

A

(but no A). If the measured values are EA and EB

, respectively, the value of K

AB may be calculated from the equation:

This method is recommended only if the electrode exhibits a

Nernstian

response. It is less desirable because it does not represent as well the actual conditions under which the electrodes are used. Slide43

Separate solution method (EA = E

B)[SSM (EA

= E

B

)] The log a vs

E relation of an ISE for the primary and interfering ions are obtained independently. Then, the activities that correspond to the same electrode potential value are used to determine the K

AB

value.

43

IIb

. Separate solution methodSlide44

However, it has been reported by many researchers that some discrepancies were found among selectivity coefficients determined under different conditions, e.g., with different activities of the primary and/or interfering ions and/or by different methods.

This suggests that the selectivity coefficient is not a physical constant but a value which changes according to experimental conditions!!!.

44