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. 2014 May 23:4:5047.
doi: 10.1038/srep05047.

Strong non-classical induction forces in ion-surface interactions: general origin of Hofmeister effects

Affiliations

Strong non-classical induction forces in ion-surface interactions: general origin of Hofmeister effects

Xinmin Liu et al. Sci Rep. .

Abstract

Hofmeister effects continue to defy all-encompassing theories, and their origin is still a matter of debate. We observed strong Hofmeister effects in Ca2+/Na+ exchange on a permanently charged surface over a wide range of ionic strengths. They could not be attributed to dispersion forces, classical induction forces, ionic size, or hydration effects. We demonstrated that another stronger force was active in the ion-surface interactions, and which would create Hofmeister effects in general. The strength of this force was up to 10(4) times that of the classical induction force, and could be comparable to the Coulomb force. Coulomb, dispersion and hydration effects appeared to be interwined to affect the force. The presence of the observed strong non-classical induction force implied that energies of non-valence electrons of ions/atoms at the interface might be heavily underestimated in current theories, and possibly just those underestimated energies of non-valence electrons determined Hofmeister effects.

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Conflict of interest statement

The authors declare no competing financial interests.

Figures

Figure 1
Figure 1
Comparison between calculated (formula image) and experimental data (formula image). KE is the experimental selectivity coefficient; KC is the calculated selectivity coefficient based on the classical theory.
Figure 2
Figure 2
KE/KCvs. φ0 (V).
Figure 3
Figure 3
Comparison between theoretical curves of KC+I (formula image) and KE (formula image).
Figure 4
Figure 4
Comparison between theoretical curves of KC+NI (formula image) and KE (formula image).
Figure 5
Figure 5
formula imagevs. φ0 (V) under different a0Na/a0Ca ratios (numbers aside dots are the values of a0Na/a0Ca).
Figure 6
Figure 6
The schematic diagram of a cation that is strongly polarized in an external electric field and the field is weakened by the polarization.

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