2018
DOI: 10.1039/c7cp07611h
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Interaction of testosterone-based compounds with dodecyl sulphate monolayers at the air–water interface

Abstract: A series of atomistic molecular dynamics simulations were performed for investigating the interactions between three different testosterone-based compounds (testosterone (T), testosterone propionate (TP) and testosterone enanthate (TE)) and sodium dodecyl sulphate (SDS) and ammonium dodecyl sulphate (ADS) monolayers, which vary only in the sodium or ammonium counterions used to neutralise the sulphate headgroup. These simulations were used to investigate how the structural and interfacial properties of the mon… Show more

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Cited by 2 publications
(4 citation statements)
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“…We then observe multiple local maxima in the region z < 0 (the larger of those at z ≈ −4 Å, with another at z ≈ −6 Å). This shows that water molecules are able to permeate past the monolayer headgroups, as has been previously observed for SDS monolayers. , This behavior is not seen at the air–water interface, where the water intrinsic density decays monotonically, as shown in Figure S5c,d here. A hard confinement matrix, such as graphite or kaolinite, does not allow permeation of water through the interface to yield the secondary peak.…”
Section: Resultssupporting
confidence: 75%
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“…We then observe multiple local maxima in the region z < 0 (the larger of those at z ≈ −4 Å, with another at z ≈ −6 Å). This shows that water molecules are able to permeate past the monolayer headgroups, as has been previously observed for SDS monolayers. , This behavior is not seen at the air–water interface, where the water intrinsic density decays monotonically, as shown in Figure S5c,d here. A hard confinement matrix, such as graphite or kaolinite, does not allow permeation of water through the interface to yield the secondary peak.…”
Section: Resultssupporting
confidence: 75%
“…This shows that water molecules are able to permeate past the monolayer headgroups, as has been previously observed for SDS monolayers. [54][55][56]58 This behavior is not seen at the air−water interface, where the water intrinsic density decays monotonically, 2 as shown in Figure S5c,d here. A hard confinement matrix, such as graphite 4 or kaolinite, 8 does not allow permeation of water through the interface to yield the secondary peak. The permeation of water past the monolayer headgroups is probably aided by the bulky CTAB headgroups, whose mutually repulsive Coulombic interactions require mediation by water and counterions to form a stable monolayer.…”
Section: ■ Results and Discussionmentioning
confidence: 82%
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