• Aucun résultat trouvé

Experimental solubility of silica in nano-pores

N/A
N/A
Protected

Academic year: 2021

Partager "Experimental solubility of silica in nano-pores"

Copied!
2
0
0

Texte intégral

(1)

HAL Id: insu-01291793

https://hal-insu.archives-ouvertes.fr/insu-01291793

Submitted on 23 Mar 2016

HAL is a multi-disciplinary open access

archive for the deposit and dissemination of

sci-entific research documents, whether they are

pub-lished or not. The documents may come from

teaching and research institutions in France or

abroad, or from public or private research centers.

L’archive ouverte pluridisciplinaire HAL, est

destinée au dépôt et à la diffusion de documents

scientifiques de niveau recherche, publiés ou non,

émanant des établissements d’enseignement et de

recherche français ou étrangers, des laboratoires

publics ou privés.

Experimental solubility of silica in nano-pores

Lionel Mercury, Majda Bouzid, Jean-Michel Matray

To cite this version:

Lionel Mercury, Majda Bouzid, Jean-Michel Matray. Experimental solubility of silica in nano-pores.

20th annual V.M. Goldschmidt Conference, Jun 2012, Montréal, Canada. �insu-01291793�

(2)

Goldschmidt 2012 Conference Abstracts

Mineralogical Magazine | www.minersoc.org 2100

Pre-eruptive conditions of

ore-forming magma that produced the

Henderson molybdenite deposit, CO:

Insights from melt inclusions and

mineral thermobarometry

CELESTINE N.MERCER1*,ALBERT H.HOFSTRA1,TODOR I.

TODOROV1, AND ERIN E.MARSH1

1USGS, Denver, USA, cmercer@usgs.gov (* presenting author)

The Henderson ore body is a Climax-type porphyry molybdenum deposit related to Oligocene high-silica rhyolite intrusions of the Red Mountain Complex near Empire, Colorado [1, 2]. The Hideaway Park rhyolite ashflow tuff outcrops 17 km NE of the Henderson deposit, and is thought to be a co-genetic extrusive expression of the intrusive complex that formed the Henderson deposit [3, 4]. We use quartz-hosted melt inclusions and phenocryst mineral chemistry to place constraints on the pre-eruptive magmatic conditions (P, T, fO2, fS2), volatile contents (H2O, CO2, F, Cl, S), and

metal concentrations to better understand the process of metal segregation within Climax-type ore-forming stocks.

Melt inclusions in the Hideaway Park rhyolite are comprised of glass, devitrified glass, crystals, and vapor. Crystals typically include quartz, alkali feldspar, magnetite, fluorite, zircon, and monazite. No molybdenite crystals have yet been identified within the crystallized inclusions, however some inclusions likely contain them because preliminary trace element analysis by LA-ICP-MS reveals several inclusions with anomalously high Mo concentrations (15-115 ppm) compared to the modal Mo concentration (10 ppm).

Accessory minerals in the Hideaway Park rhyolite include magnetite, ilmenite, biotite, zircon, and monazite. Preliminary magnetite-ilmenite pairs indicate crystallization at an fO2 of

NNO+1.7 and an aT iO2 of 0.4 [6].

SEM-CL images of quartz phenocrysts show alternating bright-to-dark euhedral growth rims and resorbed zones. Ti concentrations in quartz measured by electron microprobe range from 39 to 66 ppm corresponding to crystallization temperatures [7] between 720-qC (assuming aT iO2 = 0.4 and a preliminary pressure estimate of

2 kbar, equivalent to a shallow crustal magma reservoir at ~6 km depth). Quartz phenocrysts contain zircon inclusions, but pyrrhotite and molybdenite inclusions have not yet been found in any phenocrysts. Given that the Henderson deposit was formed in an extensional tectonic regime, carries a deep crustal/upper mantle signature (Mo/Rb = 0.013-0.040), and is only moderately oxidized, the magma is likely to be saturated with both molybdenite and pyrrhotite [5]. Assuming pyrrhotite and magnetite saturation at 750qC and an fO2 of NNO+1.7, the Hideaway Park rhyolite should

saturate with molybdenite with 8 ppm Mo in the melt [5]. The modal Mo value of 10 ppm may be indicative of a slightly higher average crystallization temperature (+10-20qC) or a slightly higher prevailing fO2 of NNO+2.

[1] Wallace (1978) B Soc Econ Geol 73, 325-368. [2] Seedorff (2004) Econ Geol 99, 3-37. [3] Adams (2009) GSA Annual

Meeting 93-7. [4] Geissman (1992) GSA B 104, 1031-1047. [5]

Audétat (2011) J Petrol 52, 891-904. [6] Ghiorso (2008) Am J Sci

308, 957-1039. [7] Huang (in press) Geochim Cosmochim Ac.

Experimental solubility of silica in

nano-pores

LIONEL MERCURY1,*,MAJDA BOUZID2,3,JEAN-MICHEL

MATRAY3

1 Institut des Sciences de la Terre d’Orléans, UMR 7327 Université

d’Orléans/CNRS/BRGM, 1A rue de la Férollerie, 45071 Orléans Cedex, France. (* presenting author)

2 IDES, UMR 8148 CNRS/Université Paris-Sud, bâtiment 504,

91405 Orsay cedex, France

3 IRSN, DEI/SARG/LETS, BP 17, 92262 Fontenay-aux-Roses

cedex, France

We used a pressure membrane extractor (Model 1020, Soil Moisture Equipment Corp.) to study the silica content at equilibrium with the decreasing pore sizes of amorphous silica. The principle is to extract the aqueous solution through a sequential process from the larger (micrometric) pores to the thinner (some nm) pores. Each extraction step is followed by an equilibration period.

The measurements confirmed earlier observations [1,2] that the concentration in dissolved silica decreases when the extraction pressure increases. The direct conclusion is that the silica solubility is pore-size dependent. These results are interpreted with the Young-Laplace relationship, at constant silica-solution surface tension, which means to attribute an elasto-capillary pressure to the solid.

Figure 1: Decreasing silica solubility extracted from pores having

decreasing radii.

The geological implication can be illustrated using a simple scheme (e.g. [3]), wherein aquifer compartments with changing pore sizes are successively put along a flowing line (in series). Depending on the modeling assumption (pore sizes, succession type, equilibrium state of the solution), this process can result in a preferential cementation of the thin or the large pores.

Our experiments demonstrate that the negative curvature of the solids has a geochemical feed-back on the solid-solution interactions, with a threshold size at around 0.1 μm.

[1] Dandurand J.-L., Mizele J., Schott J., Bourgeat F., Valles V., and Tardy Y. (1982) Sci. Géol. Bull. 35, 71−79. [2] Emmanuel S. and Berkowitz B. (2007) Geophys. Research Letters 34, L06404. [3] Mizele J., Dandurand J.-L., and Schott J. (1985) Surf. Sci. 162, 830-837. 0.6 0.7 0.7 0.8 0.8 0.9 0.9 1.0 1.0 0.02 0.04 0.06 0.08 0.10 0.12 (SiO 2 ) / (SiO 2 1/rpore(nm-1) 6 nm 6 nm bis 15 nm bis Data from [1]

calculated Si/Si°, Jsolid-water= 133 mJ/m²

Figure

Figure 1: Decreasing silica solubility extracted from pores having  decreasing radii.

Références

Documents relatifs

(3), results for the Boolean model of disks are extended to other 2D models: aligned squares (3.1), disks where the distance function is non-zero (3.2) and multiscale 2D Boolean

Dad hasn’t moved the lawn (tondre la pelouse ) Andrew has taken the dog out for a walk?. Maria has finished cleaning

The upper image shows a YBCO sample containing Zr-2411 nanoparticles with an average particle diameter of 40 nm and an area density of 35 µm -2 ; the average particle height is 15

For example, Hequembourg, Livingston, and Parks (2013) found that lesbian and bisexual women were more likely to experience sexual violence than heterosexual women, with

cently for variational inequalities by Noor and Yen to variational inclu- sions relying on Wiener-Hopf equation techniques.. We prove the continui- ty and the Lipschitz continuity

If the organization’s primary objectives are other than safeguarding intangible cultural heritage, please explain how its safeguarding objectives relate to those

On one hand, our results extends the result in [7] to the more general problem and, on the other hand, our result provides an alternative improvement of the result in [9].. Unlike

To fix the ideas we shall choose one particular subcone, the asymptotic tangent cone, which contains the Clarke cone and coinciding with the intermediate cone