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Ion-Selective Electrodes With Ionophore-Doped Sensing Membranes

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2548 Supramolecular devices<br />

<strong>Ion</strong>-selective<br />

electrode<br />

EMF<br />

Reference<br />

electrode<br />

Ag/AgCl<br />

Inner filling<br />

solution<br />

Reference electrolyte<br />

<strong>Ion</strong>-selective<br />

membrane<br />

Sample<br />

Bridge electrolyte<br />

Capillary<br />

E<br />

Profile of electrical potential, EMF: a sum of phase boundary potentials<br />

The only sample-dependent<br />

phase boundary potential (ideally)<br />

EMF<br />

Cu Ag AgCl KCl LiOAc Sample <strong>Selective</strong><br />

aqueous aqueous membrane<br />

KCl AgCl Ag Cu<br />

aqueous<br />

Figure 9 In the ideally currentless potentiometric measurement with an ISE, the measured potential is the sum of the all phase<br />

boundary potentials.<br />

cell are associated with ohmic drop, V ohm . The latter is<br />

the potential difference between the two ends of any ionic<br />

or electric conductor with resistance R when an electrical<br />

current, i, flows through it. It can be readily calculated as<br />

Ri, but since ion-selective potentiometry is almost always<br />

performed under nearly perfectly currentless conditions, the<br />

ohmic drop in an ISE measurement is negligibly small.<br />

Consequently, the EMF in a potentiometric measurement<br />

equals the sum of all phase boundary potentials, as they<br />

are illustrated in Figure 9.<br />

Importantly, only two phase boundary potentials arise at<br />

interfaces between the sample and a neighboring phase and,<br />

consequently, all but those two phase boundary potentials<br />

add up to one sample-independent term, E const :<br />

EMF = ∑ E PB<br />

=E const + E PB(salt bridge/sample) + E PB(sample/ISE membrane)<br />

≈ E ′ const + E PB(sample/ISE membrane) (6)<br />

Indeed, by choosing an appropriate electrolyte of high<br />

concentration for the salt bridge separating the sample from<br />

the reference electrode (lithium acetate in the example<br />

of Figure 9), the phase boundary potential at the salt<br />

bridge/sample interface can be kept very small and sample<br />

independent. 1, 54 The only remaining phase boundary potential<br />

that is not included in the constant term is the phase<br />

boundary potential between the aqueous sample and the<br />

ionophore-doped sensing phase, which explains the logarithmic<br />

dependence of the EMF on the sample activity.<br />

In the classical ISE setup, the ionophore-doped hydrophobic<br />

sensing phase separates the sample from the inner filling<br />

solution of the selective electrode. It is typically referred to<br />

as ion-selective membrane, a term that should, however, be<br />

interpreted with care. In most other applications of membranes,<br />

such as in filtration, osmosis, electrolysis, and gas<br />

separation, selective transport through the membrane is a<br />

key requirement and high transmembrane fluxes are very<br />

desirable. The complete opposite is true for ISE membranes.<br />

While ion movements over nanometers within the charge<br />

separation layer at the phase boundary between the sample<br />

and the membrane phase are key to the establishment<br />

of the ISE response, net ion transport through ISE membranes<br />

is not a requirement for the ISE response. Quite<br />

to the contrary, net fluxes of the ions of interest between<br />

the sample and the inner filling solution of an ISE worsen

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