DISTRIBUTION OF WATER-MOLECULES AT AG(111) ELECTROLYTE INTERFACE AS STUDIED WITH SURFACE X-RAY-SCATTERING/

Citation
Mf. Toney et al., DISTRIBUTION OF WATER-MOLECULES AT AG(111) ELECTROLYTE INTERFACE AS STUDIED WITH SURFACE X-RAY-SCATTERING/, Surface science, 335(1-3), 1995, pp. 326-332
Citations number
32
Categorie Soggetti
Chemistry Physical
Journal title
ISSN journal
00396028
Volume
335
Issue
1-3
Year of publication
1995
Pages
326 - 332
Database
ISI
SICI code
0039-6028(1995)335:1-3<326:DOWAAE>2.0.ZU;2-0
Abstract
The spatial distribution of water molecules at solid-electrolyte inter faces has received extensive theoretical study, due to the importance of this interface in electrochemistry and other sciences. Such studies suggest that adjacent to the interface water is arranged in several l ayers, that the molecular arrangements in the inner layer is similar t o bulk water, and that the inner-layer molecules have an oxygen-up (ox ygen-down) average orientation for negative (positive) electrode charg e (or, equivalently, potential). However, little of this has been veri fied by experimental measurements. In this paper we report surface X-r ay scattering measurements of the water distribution perpendicular to a Ag(111)-electrolyte interface in 0.1M NaF at two potentials: +0.52 a nd -0.23 V from the potential of zero charge (PZC) on the electrode. W e find that, first, the water is ordered in layers extending about thr ee molecular diameters from the electrode. Second, the extent of order ing and the distance between the electrode and first water layer depen d on potential, the latter being consistent with an oxygen-up (oxygen- down) average molecular orientation for negative (positive) electrode potential. Third, the inner water layer contains 1.55 X 10(15) (at -0. 23 V) and 2.6 X 10(15) (at +0.52 V) water molecules per cm(-2), remark ably more than expected from the bulk water density (i.e., similar to 1.15 x 10(15) cm(-2)). Such a large compression shows that the molecul ar arrangements in the inner layer are significantly different from bu lk, which has not been anticipated in current models of charged, aqueo us interfaces. We give a qualitative explanation of this large density as resulting from the strong electric field at the charged Ag(111) el ectrode and present a tentative model of the molecular arrangements.