2017
DOI: 10.1016/j.molliq.2017.01.073
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Surface structures of binary mixture of ionic liquids

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Cited by 17 publications
(25 citation statements)
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“…where Ai is here the molar surface area of component i, n = A1/A2, and x2 s can be obtained simply from x1 s + x2 s = 1. Although, as noted by Nakajima et al, 29 the prediction is not too far from their observed HRBS result at x = 0.5, the qualitative behaviour over the full range of x measured in our RAS-LIF experiments is very poorly reproduced by eqn (4). The level of agreement is again not materially changed by modest differences in the surface tension values reported here and elsewhere.…”
Section: Predictions Based On Surface Tensions Of Pure Componentssupporting
confidence: 53%
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“…where Ai is here the molar surface area of component i, n = A1/A2, and x2 s can be obtained simply from x1 s + x2 s = 1. Although, as noted by Nakajima et al, 29 the prediction is not too far from their observed HRBS result at x = 0.5, the qualitative behaviour over the full range of x measured in our RAS-LIF experiments is very poorly reproduced by eqn (4). The level of agreement is again not materially changed by modest differences in the surface tension values reported here and elsewhere.…”
Section: Predictions Based On Surface Tensions Of Pure Componentssupporting
confidence: 53%
“…These areas could be estimated simply from bulk densities with an assumption of cubic geometry, or ostensibly more accurately from the observed areal atomic densities in their HRBS experiments. 15 U N -area estimates 29 and our own measured surface tensions for [C2mim](1-x)[C12mim]x[NTf2] mixtures above, the dependence of surface mole fraction on bulk mole fraction shown in Fig. 6 is predicted, where it is compared with our RAS-LIF measurements of surface exposure.…”
Section: Predictions Based On Surface Tensions Of Pure Componentsmentioning
confidence: 65%
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