2014
DOI: 10.1016/j.pss.2013.04.010
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On the edge of habitability and the extremes of liquidity

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Cited by 21 publications
(23 citation statements)
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“…In the case of degassing at room temperature the halite behaves like the pure NaCl taking some less water. This very small amount of water is due to the formation of predeliquescence layers on the crystal surfaces as reported by Bruzewicz et al (2011) and Hansen-Goos et al (2014). Layer heights of some nm were calculated by Hansen-Goos in accordance with our findings taking into account the surface area estimated for the crystals in halite or the pure NaCl.…”
Section: Water Sorption Properties Of the Materials At Equilibriumsupporting
confidence: 90%
“…In the case of degassing at room temperature the halite behaves like the pure NaCl taking some less water. This very small amount of water is due to the formation of predeliquescence layers on the crystal surfaces as reported by Bruzewicz et al (2011) and Hansen-Goos et al (2014). Layer heights of some nm were calculated by Hansen-Goos in accordance with our findings taking into account the surface area estimated for the crystals in halite or the pure NaCl.…”
Section: Water Sorption Properties Of the Materials At Equilibriumsupporting
confidence: 90%
“…The size distribution at RH w ≈ 70% in the iced chamber shows a minor reduction of smaller particles accompanied by a slight enhancement of larger particles. Although this trend could indicate water uptake below the DRH (Wise et al, 2008;Alshawa et al, 2009;Bruzewicz et al, 2011;Hansen-Goos et al, 2014;Hsiao et al, 2016), it could also result from experimental uncertainties. The different wall conditions (iced versus uniced) and possible salt impurities may also lead to slight changes.…”
Section: Resultsmentioning
confidence: 99%
“…(10) to a sodium chloride particle of a representative atmospheric diameter 0.8 µm in the accumulation mode (Lewis and Schwartz, 2004;Lohmann et al, 2016). The growth factor is assumed such that the particle will lead to a solvated brine droplet of radius 1.36 µm, and for consistency with previous work we choose a temperature of 20 • C and a saturated concentration of [NaCl] sat = 5.4 mol L −1 (Haynes, 2012), which is also used to calculate the Debye length. The value for surface charge q s = 0.12 C m −2 is taken from Kobayashi et al (2014), while the HG14 value A h = −1.5 × 10 −20 is used, and the expression for the water activity of a NaCl solution is taken from Tang et al (1997).…”
Section: Applying Refined Köhler Theorymentioning
confidence: 99%
“…Standard values 0.12 (Kobayashi et al, 2014) −1.5 × 10 −20 (HG14) 5400 (Haynes, 2012) 3 nm (b) 0.3 −7.5 × 10 −20 8800 4 nm (a) 0.3 −9 × 10 −20 8270 4 nm (b) 0.3 −4 × 10 −20 8000 5 nm (a) 0.1 −9 × 10 −20 7050 5 nm (b) 0.4 −2.5 × 10 −20 7620 7.5 nm (a) 0.6 −9 × 10 −20 6700 7.5 nm (b) 0.002 −3 × 10 −20 7020 10 nm (b) 0.01 −15 × 10 −20 6500 15 nm (a) 2.7 × 10 −6 −5 × 10 −20 6300 15 nm (b) 0.02 −4 × 10 −20 6300 20 nm (b) 0.3 −5.5 × 10 −20 6000 25 nm (a) 0. Figure 3.…”
Section: Applying Refined Köhler Theorymentioning
confidence: 99%