1-20 OF 1487 RESULTS FOR

liquid-vapor interface

Results shown limited to content with bounding coordinates.
Follow your search
Access your saved searches in your account

Would you like to receive an alert when new items match your search?
Close Modal
Sort by
Journal Article
Published: 01 August 2002
Vadose Zone Journal (2002) 1 (1): 14–37.
... assumptions are used in deriving the average cross-sectional flow velocities in these regimes: (i) that equilibrium liquidvapor interfaces remain stable under slow laminar flows and (ii) that flow pathways are parallel. Liquidvapor interfacial configurations for different matric potentials are calculated...
FIGURES | View All (19)
Image
The effect of the critical bubble radius on the pressure differential across the liquid-vapor interface. For all critical bubble radii, the pressure differential increases with decreasing temperature (increasing surface tension). At a given temperature, the pressure differential increases with decreasing critical bubble radius.
Published: 01 November 2009
F igure 9. The effect of the critical bubble radius on the pressure differential across the liquid-vapor interface. For all critical bubble radii, the pressure differential increases with decreasing temperature (increasing surface tension). At a given temperature, the pressure differential
Journal Article
Published: 01 November 2009
American Mineralogist (2009) 94 (11-12): 1569–1579.
...F igure 9. The effect of the critical bubble radius on the pressure differential across the liquid-vapor interface. For all critical bubble radii, the pressure differential increases with decreasing temperature (increasing surface tension). At a given temperature, the pressure differential...
FIGURES | View All (15)
Image
Interface relationships between sulfide liquid, silicate liquid, and a vapor bubble (VB). A) Calculations of the interfacial tensions (γ) between sulfide melt (S), silicate melt (M), and vapor (V) from Mungall et al. (2015). B) An experimental charge displaying the concave sulfide from Mungall et al. (2015). C) Example from Norilsk 1 upper taxitic layers where sulfide is almost entirely encapsulated by relic VB. Sample N1-24-39.3A. D) Example from Norilsk 1 taxitic layers; VB and sulfide display a straight interface (though now detached). Sample N1-6-373.9. E) Example from Kharaelakh picrogabbrodolerite, where VB is concave to sulfide.
Published: 01 September 2020
Fig. 10. Interface relationships between sulfide liquid, silicate liquid, and a vapor bubble (VB). A) Calculations of the interfacial tensions ( γ ) between sulfide melt (S), silicate melt (M), and vapor (V) from Mungall et al. (2015) . B) An experimental charge displaying the concave sulfide
Image
Various fluid inclusions in the high-degree greisen zone. (a) A cross-polarized transmitted-light image of quartz and topaz crystals. (b) Sketch illustrating the minerals seen in (a). The core of the large quartz grain in the upper left corner is of magmatic origin (compare to Q1 in Fig. 5) and epitactically overgrown by greisen quartz (Q2 in Fig. 5). The two quartz generations were distinguished using cathodoluminescence. The areas marked with insets in (a) show magnified examples of the rim of the large quartz (c) and topaz (d), respectively. The fluid inclusions inside the magmatic quartz in (c) follow typical planar secondary inclusion trails and comprise secondary liquid (sL), secondary vapor (sV), and secondary brine (sB) inclusions. Some examples, marked by ending with a number, are shown magnified and individually focused on the right. Liquid and brine types are distinguished here by the absence or presence of halite and other daughter crystals in the liquid. On the interface between magmatic quartz and greisen quartz overgrowth, irregularly shaped primary vapor (pV) and primary brine (pB) inclusions are found along with abundant mineral inclusions (see Fig. 4). The fluid inclusions in topaz (d) are often attached to the abundant mineral inclusions and subgrain boundaries in the topaz, which may obscure some fluid inclusions or lead to postentrapment modification. Numerous small and uniform liquid (L) and some larger vapor (V) inclusions can nevertheless be identified. The absence of obvious trails suggests primary origin for all of the fluid inclusions in topaz, but secondary modification cannot be excluded. pL = primary liquid.
Published: 01 June 2024
are distinguished here by the absence or presence of halite and other daughter crystals in the liquid. On the interface between magmatic quartz and greisen quartz overgrowth, irregularly shaped primary vapor (pV) and primary brine (pB) inclusions are found along with abundant mineral inclusions (see Fig. 4
Journal Article
Published: 01 May 2006
Vadose Zone Journal (2006) 5 (2): 784–800.
... temperatures and water contents were in good agreement with measured values. Analyses of the distributions of the liquid and vapor fluxes vs. depth showed that soil water dynamics are strongly associated with the soil temperature regime. The soil–atmosphere interface is an important boundary condition...
FIGURES | View All (13)
Image
Schematic diagram of a volcanic system to illustrate processes involving bubble-crystal or bubble-liquid aggregates. The magmas are volatile-rich and bubbles are largely attached to magnetite and sulfide liquid phases. Discussed are: intrusion of a magnetite-rich foam into shallow faults (Knipping et al., 2015); accumulation of magnetite-bubble aggregates at interfaces between underplating mafic magmas and overlying intermediate magmas (Edmonds et al., 2014) and the congruent dissolution of sulfide liquid into aqueous vapor, which then outgasses from the volcano (Mungall et al., 2015).
Published: 01 July 2015
faults ( Knipping et al., 2015 ); accumulation of magnetite-bubble aggregates at interfaces between underplating mafic magmas and overlying intermediate magmas ( Edmonds et al., 2014 ) and the congruent dissolution of sulfide liquid into aqueous vapor, which then outgasses from the volcano ( Mungall et
Image
Raman spectra collected from the vapor bubble in MI SCL14-D92-3-1 at different conditions and depths. The yellow spectrum was collected from the MI at room temperature while focusing the laser at the glass/bubble interface in July 2014 and shows the H2O fluid band. The black spectrum was collected at 150 °C while focusing the laser in the glass in the MI and shows the OH and H2O band at ~3550 cm−1. Note the difference between the peak positions of liquid H2O in the synthetic fluid inclusion and at the glass/bubble interface and those of hydroxyl and molecular water dissolved in the silicate glass. The red spectrum represents the H2O band collected at 150 °C while focusing the laser at the glass/bubble interface in the MI. Notice that the H2O band of liquid water was not observed at 150 °C, while a peak at ~1650 cm−1 was only detected at this temperature (a.u. = arbitrary units). (Color online.)
Published: 01 July 2016
Figure 3 Raman spectra collected from the vapor bubble in MI SCL14-D92-3-1 at different conditions and depths. The yellow spectrum was collected from the MI at room temperature while focusing the laser at the glass/bubble interface in July 2014 and shows the H 2 O fluid band. The black spectrum
Image
Different types of fluid inclusions hosted by veins. A) Two-phase intermediate-density fluid inclusions with vapor (V) and liquid (L) filling the available space in equal proportions. Triangular opaque solids, probably chalcopyrite (Cpy), are present in almost all inclusions of this type. B) Vapor fluid inclusion filled mainly by vapor (~90 vol %) and a thin rim of liquid wetting the fluid-crystal interface. Chalcopyrite daughter crystals are commonly present. C) B1 fluid inclusions with small bubbles (~20 vol %) and halite (H). D) High-temperature B2 fluid inclusion with large vapor bubble (~30 vol %). E) Complex B3 fluid inclusion with several daughter crystals besides halite, such as sylvite (S), red flakes of hematite (Hem), and blueish, birefringent, commonly elongated, transparent anhydrite (Anh). Chalcopyrite is also present but not visible here, because it is covered by the vapor bubble. F) Boiling trail hosting brine (B) and vapor fluid inclusions (FIs). G) Low-salinity aqueous fluid inclusions (AQ2) within euhedral dull-luminescent paint vein quartz. H) Rectangular aqueous fluid inclusions hosted by anhydrite in D veins (AQ3). I) Low-temperature, irregular, and flat aqueous fluid inclusions may be associated with D vein formation (AQ3). J) Primary aqueous (AQ) fluid inclusion assemblage (FIA) along growth zone in euhedral paint vein quartz (Q4). This assemblage contains high-salinity aqueous inclusions (AQ1) in which dissolution of hydrohalite was visible during freezing experiments. High-salinity (AQ1) and low-salinity aqueous fluid inclusions (AQ2) are indistinguishable at room temperature.
Published: 01 August 2022
. B) Vapor fluid inclusion filled mainly by vapor (~90 vol %) and a thin rim of liquid wetting the fluid-crystal interface. Chalcopyrite daughter crystals are commonly present. C) B 1 fluid inclusions with small bubbles (~20 vol %) and halite (H). D) High-temperature B 2 fluid inclusion with large
Journal Article
Published: 01 August 2010
The Canadian Mineralogist (2010) 48 (4): 1025–1039.
... O-undersaturated granite at high temperature. Moreover, the absence of back reactions at the leucosome–melanosome interface shows that saturation in H 2 O was not attained during cooling. This indicates that the leucosome, although likely the locus of partial melting, is a K-rich cumulate left over...
FIGURES | View All (9)
Journal Article
Journal: Geology
Published: 01 September 2004
Geology (2004) 32 (9): 761–764.
...-salinity vapor enriched in volatile S. This vapor can contract directly to an aqueous liquid, by cooling at elevated pressure above the critical curve of the salt-water fluid system. Physical and chemical conditions are matched when magmatic fluid is released through a gradually downward-retracting...
FIGURES
Journal Article
Published: 01 November 2004
American Mineralogist (2004) 89 (11-12): 1673–1679.
... consistent with the effects of dissolved H 2 O on the liquid-vapor interfacial free energy in haplogranite magma ( Mangan and Sisson 2000 ) and the liquid-crystal interfacial free energy in the one-component Li-disilicate system ( Davis et al. 1997 ). The DIT states that the interfacial region between...
FIGURES
Journal Article
Published: 01 August 2004
American Mineralogist (2004) 89 (8-9): 1254–1259.
... nucleated at low overpressure (e.g., 0.75 MPa), hydrate formed at the vapor-liquid interface, encrusting the bubbles with less than 1 g of hydrate accumulation in the first minute. When a higher overpressure was required for nucleation (e.g., 1.3 MPa), hydrate was observed to form abruptly not only...
FIGURES | View All (4)
Series: Reviews in Economic Geology
Published: 01 January 2018
DOI: 10.5382/rev.20.09
EISBN: 9781629491189
... below and presented in Tables 7 through 10 and Figure 14 . Late calcite associated with drusy quartz from Yenkeh Kand Valley contains liquid-rich inclusions with ≤80% degree of fill and minor vapor-rich and liquid-only inclusions. The liquidrich inclusions have T fm of –0.6°C, salinities...
FIGURES | View All (19)
Image
Schematic cross sections through the Famatina Cu-Mo-Au system, illustrating the inferred fluid evolution paths from the deep porphyry setting (a) through the transitional QSP stage (b) to the shallow high-sulfidation epithermal environment (c), based on continued ascent of magmatic-hydrothermal fluid in a progressively cooling and eroding hydrothermal system. White arrows indicate the source fluid exsolving from a crystallizing magma at progressively greater depth. Black arrows highlight the progressive input of meteoric water. Fluid columns (“chimneys”) to the right of each cartoon section schematically illustrate the evolving phase state of the single- and two-phase fluids along their upflow path. Fluids are shaded to denote the fluid density, varying between low-density vapor (white) and dense liquids of various salinities (black). Note that the vaporlike fluid in b and c evolves, through contraction, to become more dense on ascent and cooling, and thus liquid-like at epithermal depths (in contrast to the high-temperature vapor discharge at the surface in a). Constrictions denote confined permeability, which are likely to lead to pressure fluctuations between lithostatic conditions at the magmatic interface, and pressures that are increasingly controlled by the density of the fluid phase where veins are open to the eroding surface, i.e., hydrostatic (or vaporstatic) conditions.
Published: 01 June 2009
section schematically illustrate the evolving phase state of the single- and two-phase fluids along their upflow path. Fluids are shaded to denote the fluid density, varying between low-density vapor (white) and dense liquids of various salinities (black). Note that the vaporlike fluid in b and c evolves
Journal Article
Published: 01 May 2007
European Journal of Mineralogy (2007) 19 (3): 339–344.
... of the calcite bubbles acting on the chemical composition of the solution. This can be achieved because our crystals form around gas cavities whose size is strictly related to the interfacial energy between the liquid and the vapor phase. A comparison between size variation and the surface tension trend...
FIGURES | View All (7)
Journal Article
Published: 01 August 2004
Vadose Zone Journal (2004) 3 (3): 806–818.
.... The first step involves transition from liquid to vapor phase at the liquidvapor interface (vaporization). The second step is the transport of vapor from the high concentration area at the evaporating surface to the low concentration area of the ambient air. Accurate modeling of these coupled processes...
FIGURES | View All (10)
Journal Article
Published: 01 February 2015
Clays and Clay Minerals (2015) 63 (1): 15–29.
...: Hydrogen bonding and vibrational spectroscopy, in the bulk liquid and at the liquid/vapor interface . Chemical Physics Letters , 470 , 13 – 20 . Bertie J.E. Ahmed M.K. Eysel H.H. ( 1989 ) Infrared intensities of liquids. 5. Optical and dielectric constants, integrated intensities...
FIGURES | View All (10)
Journal Article
Published: 01 November 2011
Vadose Zone Journal (2011) 10 (4): 1173–1184.
... ). Tuller et al. (1999 , Fig. 1 ) showed that pore space geometry (the pore shape and angularity of grains) has a marked influence on imbibition and drainage processes. During imbibition, the liquidvapor interface grows within corners of angular pores with increasing potential (or capillary pressure...
FIGURES | View All (13)
Journal Article
Published: 01 July 2016
American Mineralogist (2016) 101 (7): 1691–1695.
...Figure 3 Raman spectra collected from the vapor bubble in MI SCL14-D92-3-1 at different conditions and depths. The yellow spectrum was collected from the MI at room temperature while focusing the laser at the glass/bubble interface in July 2014 and shows the H 2 O fluid band. The black spectrum...
FIGURES