Potentiometric Sensors with Ion-Exchange Donnan Exclusion MembranesClick to copy article linkArticle link copied!
Abstract
Potentiometric sensors that exhibit a non-Hofmeister selectivity sequence are normally designed by selective chemical recognition elements in the membrane. In other situations, when used as detectors in separation science, for example, membranes that respond equally to most ions are preferred. With so-called liquid membranes, a low selectivity is difficult to accomplish since these membranes are intrinsically responsive to lipophilic species. Instead, the high solubility of sample lipids in an ionophore-free sensing matrix results in a deterioration of the response. We explore here potentiometric sensors on the basis of ion-exchange membranes commonly used in fuel cell applications and electrodialysis, which have so far not found their way into the field of ion-selective electrodes. These membranes act as Donnan exclusion membranes as the ions are not stripped of their hydration shell as they interact with the membrane. Because of this, lipophilic ions are no longer preferred over hydrophilic ones, making them promising candidates for the detection of abundant ions in the presence of lipophilic ones or as detectors in separation science. Two types of cation-exchanger membranes and one anion-exchange membrane were characterized, and potentiometric measuring ranges were found to be Nernstian over a wide range down to about 10 μM concentrations. Depending on the specific membrane, lipophilic ions gave equal response to hydrophilic ones or were even somewhat discriminated. The medium and long-term stability and reproducibility of the electrode signals were found to be promising when evaluated in synthetic and whole blood samples.
Experimental Section
Reagents, Materials, and Equipment
Procedures
Results and Discussion
membrane | ion (J) | slope (mV) | EJ° (mV) | log(KI,Jpot) |
---|---|---|---|---|
FAB | Cl– | –57.8 ± 0.3 | 13.5 ± 0.7 | 0 |
ClO4– | –60.5 ± 0.6 | –78.9 ± 3.4 | 1.5 ± 0.1 | |
SCN– | –58.4 ± 0.9 | –75.4 ± 4.2 | 1.5 ± 0.1 | |
NO3– | –57.7 ± 1.0 | –19.4 ± 3.1 | 0.5 ± 0.1 | |
Nafion | Na+ | 59.5 ± 0.3 | 242.2 ± 2.7 | 0 |
Li+ | 61.5 ± 0.1 | 243.5 ± 0.3 | 0.02 ± 0.01 | |
K+ | 56.7 ± 0.2 | 245.8 ± 1.2 | 0.06 ± 0.02 | |
Ca2+ | 57.8 ± 0.6 | 250.7 ± 2.5 | 0.15 ± 0.08 | |
Mg2+ | 60.3 ± 0.9 | 256.8 ± 2.5 | 0.5 ± 0.1 | |
FKL | Na+ | 51.5 ± 0.4 | 255.1 ± 2.5 | 0 |
Li+ | 51.9 ± 0.8 | 230.2 ± 3.6 | –0.4 ± 0.1 | |
K+ | 64.8 ± 0.6 | 289.3 ± 0.7 | 0.6 ± 0.1 | |
Ca2+ | 59.4 ± 2.5 | 287.1 ± 6.1 | 1.1 ± 0.3 | |
Mg2+ | 58.4 ± 3.4 | 284.1 ± 5.1 | 1.0 ± 0.3 |
Conclusions
Supporting Information
Additional information as noted in text. This material is available free of charge via the Internet at http://pubs.acs.org.
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Most electronic Supporting Information files are available without a subscription to ACS Web Editions. Such files may be downloaded by article for research use (if there is a public use license linked to the relevant article, that license may permit other uses). Permission may be obtained from ACS for other uses through requests via the RightsLink permission system: http://pubs.acs.org/page/copyright/permissions.html.
Acknowledgment
The authors thank the Swiss National Science Foundation for supporting this research. This work also forms part of a project funded by the Australian Research Council (DP0987851).
References
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References
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- 23Kong, X. Q.; Schmidt-Rohr, K. Polymer 2011, 52, 1971– 197423https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC3MXksFKksbY%253D&md5=30a0de34aee274cf814e3ae0c109fc35Water-polymer interfacial area in Nafion: Comparison with structural modelsKong, Xueqian; Schmidt-Rohr, KlausPolymer (2011), 52 (9), 1971-1974CODEN: POLMAG; ISSN:0032-3861. (Elsevier Ltd.)The water-polymer interfacial area per vol., S/V, which is reflected in the Porod region of small-angle scattering data, is an important parameter of different models of the Nafion fuel cell membrane. Therefore, published exptl. S/V data of Nafion are compared over a wide range of hydration levels with various structural models featuring stiff polymer backbones, in particular the parallel water-channel and the polymer ribbon models. The S/V curve at intermediate hydration levels typical of fuel-cell conditions (ca. 20 vol% water) matches that of the parallel water-channel model with mol. corrugation. At higher hydration levels, i.e. for membranes soaked in water or autoclaved at elevated pressures, the polymer-ribbon model matches the decreasing S/V ratio with increasing water content, while the polymer-bundle model predicts a higher surface area. However, the ribbon or bundle models cannot apply at low hydration (< 3 water mols. per Nafion side group), since it is shown that the interfacial area in this regime must increase strongly with hydration, being detd. by the available surface area of the water mols. The pronounced asymmetry of the plot of S/V vs. water vol. fraction is explained in terms of the difference in the diams. of the water mols. and the polymer aggregates.
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- 29Meier, P. C. Anal. Chim. Acta 1982, 136, 363– 36829https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADyaL38XhvVyjt74%253D&md5=8439cadce59ff58afe28484d9ba6790eTwo-parameter Debye-Hueckel approximation for the evaluation of mean activity coefficients of 109 electrolytesMeier, P. C.Analytica Chimica Acta (1982), 136 (), 363-8CODEN: ACACAM; ISSN:0003-2670.Among the published formula for the calcn. of mean activity coeffs., the most reliable and comprehensive are those recently recommended by the National Burea of Stds. In many applications, the ionic strength does not exceed ∼1 M, and the NBS functions can be approximated by a 2-parameter Debye-Hueckel model. The limits of applicability (e.g., 1% deviation from the corresponding NBS model) are listed. The procedure makes efficient use of calculator memory.
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