1992
DOI: 10.1021/j100187a040
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Vapor adsorption on mica and silicon: entropy effects, layering, and surface forces

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Cited by 212 publications
(249 citation statements)
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“…This was achieved through humidity reduction in the atmosphere surrounding the sample. While cellular chromatin is in a more aqueous environment than that employed here, it has been shown that a 1 A thick layer of water is present on mica in 10% humidity (Beaglehole & Christenson, 1992). Owing to the hygroscopic nature of residual buffer salts, it is likely that even more moisture resides around the chromatin, allowing for more physiologically relevant chromatin structures to be observed.…”
Section: Discussionmentioning
confidence: 80%
“…This was achieved through humidity reduction in the atmosphere surrounding the sample. While cellular chromatin is in a more aqueous environment than that employed here, it has been shown that a 1 A thick layer of water is present on mica in 10% humidity (Beaglehole & Christenson, 1992). Owing to the hygroscopic nature of residual buffer salts, it is likely that even more moisture resides around the chromatin, allowing for more physiologically relevant chromatin structures to be observed.…”
Section: Discussionmentioning
confidence: 80%
“…The conditions of transition between these two modes can be very complicated and have been the subject of several studies [17,18]. A recent work from Zitzler [19] has shown that the critical oscillation amplitude that triggers the transition between IC and NC modes on a silica glass surface is an increasing function of the relative humidity and, thus, of the thickness of the condensed water layer, according to experimental investigations performed by Beaglehole and Christenson [20]. The estimation of the energy which is dissipated in the tip-surface interaction is consistent with a model based on the formation and rupture of a capillary neck (1) between the AFM tip and the nanometric water layer.…”
Section: Resultsmentioning
confidence: 99%
“…Again using DMT theory, this repulsive interaction is given by F r =−͑4 / 3͒E * R 1/2 ͑a 0 − d͒ 3/2 , where The capillary force arises from the interactions between thin films of water of depth h that cover the sample and cantilever tip due to ambient humidity. 6,[15][16][17] As the separation d falls below a critical distance d on =2h, a connective column of liquid is established. Upon retracting away from the surface, the liquid column forms a meniscus and neck, until eventually breaking as the separation increases beyond a critical distance d off = V 1/3 − V 2/3 / 5R, where V is the meniscus volume.…”
Section: The Physical Modelmentioning
confidence: 99%