Aging of nuclear glass analogues Aurlie Verney-Carron Since 2010: - - PowerPoint PPT Presentation

aging of nuclear glass analogues
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Aging of nuclear glass analogues Aurlie Verney-Carron Since 2010: - - PowerPoint PPT Presentation

Aging of nuclear glass analogues Aurlie Verney-Carron Since 2010: Assistant Professor at LISA, France 2009-2010: Post-doc at CRPG on Li isotopes to trace basaltic glass alteration 2005-2008: PhD at CEA on the Study of archaeological analog for


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Aging of nuclear glass analogues

Aurélie Verney-Carron

Since 2010: Assistant Professor at LISA, France 2009-2010: Post-doc at CRPG on Li isotopes to trace basaltic glass alteration 2005-2008: PhD at CEA on the Study of archaeological analog for the validation

  • f nuclear glass long-term behavior models

Joint ICTP-IAEA International School on Nuclear Waste Vitrification, 27 Sept. 2019

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Objectives of analogs study

ü Different examples : long-term durability of natural glasses, retention of transition elements used as colorants in stained glass windows, contribution of cracks of Roman glass blocks, … ü It requires to demonstrate the analogy between the different glasses

Ancient glass (short-term alteration) Nuclear glass (short-term alteration) REASONING BY ANALOGY

  • A is similar to C in certain known

respects.

  • A has some further feature B.
  • Therefore, probably, C also has

the feature B. Ancient glass (long-term alteration) Nuclear glass (long-term alteration) A C B

?

q To know the long-term alteration

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Objectives of analogs study

?

q To validate the predictive capacity of alteration models

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Studies of ancient glasses

Basaltic glass Obsidian Roman glass (shipwreck)

Embiez Iulia Felix

Buried archaeological glass

Verney-Carron et al. (2008, 2010a,b) Ryan et al. (in prep) Strachan et al. (2014) Ewing (1979, 2001) Allen (1983) Birchard (1984) Byers et al. (1985) Lutze et al. (1985) Grambow et al. (1986) Ewing and Jercinovic (1987); Jercinovic and Ewing (1988) Cowan and Ewing (1989) Crovisier et al. (1989; 1992) Murakami et al. (1989) Arai et al. (1989) Werme et al. (1990) Morgenstein & Schettel (1994) Techer et al. (2001, 2001a,b) Parruzot et al. (2015) Ducasse et al. (2018) Macquet and Thomassin (1992) Saint-Denis Sterpenich and Libourel (2001, 2006) Magonthier et al. (1992) Rani et al. (2013, 2015) Strachan & Pierce (2010) PNNL-19752 Report Weaver et al. (2016) Michelin et al. (2015)

Stained glass windows

Sterpenich and Libourel (2001, 2006)

Vitreous slags Chondrites

Morlok and Libourel (2013) Libourel et al. (2011)

Tektites Vitrified forts

Sjöblom et al. (2013)

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Order

A- NATURAL GLASSES

  • I. Volcanic glasses
  • II. Properties: long-term durability
  • III. Analogy between basaltic glass and nuclear glass
  • IV. Analogy between obsidian and nuclear glass
  • V. Primitive meteorites (chondrites)

B- HUMAN-MADE GLASSES

  • I. The stained glass windows
  • II. Vitreous slags : interactions glass / iron
  • III. Roman glass alteration modeling
  • IV. Pre-viking Swedish hillfort glass / LAW glasses
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A- Natural glasses

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  • I. Volcanic glasses

Volcanic rocks are formed by the fast cooling of magma (lava) at the Earth surface in different geodynamic contexts.

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The composition influences the viscosity and the vitrification. Glass < high viscosity (to inhibit the crystallization) + sudden cooling to chill the material to a glass

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BASALTIC GLASS Low viscosity à high cooling rate (oceanic seafloor, subglacial volcanoes) OBSIDIAN high viscosity but rare

Main locations of natural glasses: oceanic seafloor and Large Igneous Provinces (LIP)

Deccan traps Siberian traps Iceland Columbia River North Atlantic LIP Afar Parana

Pillow lavas in Iceland (vitreous crust) Hyaloclastites

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  • II. Properties : long-term durability

Richet (2009) Verre Rocks from Figeac (Lot, France) – 280 My

glass pyroxene plagioclase Þ Old natural glasses despite tectonic and erosion

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Parruzot (2015) Initial rate (lab) at 5°C

Þ The apparent alteration rate decreases with time. Þ The field alteration rate (confined medium) is lower than the lab alteration rate. 1 µm / 10000 y 1 µm / 1 My 1 µm / y

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Þ Measurement of the residual rate using a t-dependent law and Na diffusion coefficients using a √t law

Parruzot et al. (2015)

rr = 9.6·10-6 g/m²/d at 90°C rr = 4.0·10-6 g/m²/d at 30°C D = 2.5·10-25 g/m²/d at 90°C D = 4.7·10-26 g/m²/d at 30°C

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Þ Extrapolation of a linear residual rate measured at the laboratory consistent with ancient samples

Parruzot (2015) Initial rate (lab) at 5°C

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  • III. Analogy between BG and NG
  • Phenomenology

NUCLEAR GLASS

From Gin et al. (2017) Gin et al. (2001)

BASALTIC GLASS

Smectites, zeolites Gel palagonite Fibrous palagonite Alteration front Smectites, calcite, oxides, zeolites)

Glass

From Zhou & Fyfe (1989) Zhou et al. (2001)

Þ Similar alteration facies

TEM image of an Icelandic basaltic glass (0,1 My) [Crovisier et al., 2003] TEM image of an oceanic basaltic glass (10,1 Ma): saponite at 10 Å [Zhou et al., 2001].

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SLIDE 15
  • Kinetics

NUCLEAR / BASALTIC GLASS

Parruzot et al. (2015)

  • rr (ISG) = 2·10-4 g/m²/d (90°C)
  • rr (BG) = 9.6·10-6 g/m²/d (90°C) at pH 7
  • rr (BG) = 4·10-3 g/m²/d (90°C) at pH 9,3

Forward dissolution rate Residual rate Þ Similar alteration rates

Techer et al. (2000) Ducasse et al. (2018)

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BASATIC GLASS T = 90°C, pH 7 (at 90°C) Si saturated solution t = 600 d

Ducasse et al. (2018)

Þ Complete depletion in Na, Ca, B Þ Si (~ Al, Ti) in the alteration layer (clays and amorphous silica) Þ Enrichment in 29Si (// solution)

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Ducasse et al. (2018) ISG : Gin et al. (2015,2017)

(a) Quick interdiffusion and hydrolysis → release of Na and Ca and B (b) Precipitation of clays (Si, Al, Fe, Mg, Ti) and SiO2(am) (c) The remaining silicate network dissolves and SiO2(am) precipitates (d) The layer of secondary phases grows up, sustaining glass dissolution

Þ Differences with ISG Glass ISG: selective dissolution à passivating layer (glass alteration is limited by water diffusion) BG: congruent dissolution à clays (equilibrium) The dissolution is controlled by the hydrolysis of the glass network and is sustained by the precipitation of secondary phases. BASATIC GLASS COMPARISON WITH NUCLEAR GLASS Þ A similar phenomenology but different mechanisms controlling the long-term alteration rate (due to composition)

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  • IV. Analogy between obsidian and NG

Rani et al. (2013, 2015)

SiO2 Al2O3 Na2O K2O CaO MgO Fe2O3 tot TiO2 LOI 69.50 12.00 3.50 3.71 1.00 0.07 2.63 0.182 7.11

  • Composition
  • Phenomenology: dioctahedral

smectite

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SLIDE 19
  • V. Primitive meteorites (chondrites)
  • Fe and Mg minerals, Si-Al glass, Fe-Ni metal and

clays à glass / iron / clays (storage)

  • Different alteration stages between 50 and 150°C

Morlok et al. (2013)

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B- Human-made glasses

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  • I. The stained glass windows
  • Archaeological stained glass (buried in soils)

Sterpenich and Libourel (2001)

Stained glass excavated from the site of Notre- Dame-de Bourg (Digne), 12th century

Þ High retention of transition elements and heavy metals

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Þ Partial retention of transition elements and heavy metals

  • Stained glass weathered in atmosphere

Sterpenich and Libourel (2001)

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  • Analogy

NUCLEAR GLASS T = 90°C

Valle et al. (2010)

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STAINED GLASS T = 30°C 1 month Dynamic conditions Þ Indication on the long-term partition of transition elements and similar mechanisms far from saturation

Verney-Carron et al. (2017)

Pristine glass Gel layer

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  • II. Vitreous slags : interactions glass / iron

Godon et al. (2013)

Comparison between experimental results (diamonds), modelling with sorption of Si (dashed lines) and sorption of Si + precipitation of iron silicates.

Þ Iron increases glass alteration rate due to the precipitation of Fe-silicates

EXPERIMENT T = 50°C Synthetic clay- based groundwater EXPERIMENT SON68 + iron (10 µm) + Bure argilite + water T = 90°C for 18 months

Þ Formation of Fe-silicates Þ Alteration thickness = r0/2 Þ Iron sustains a high alteration rate

De Combarieu et al. (2011)

SON68 SON68 + magnetite SON68 + 2 x magnetite

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Þ Analogy: vitreous slag / glass package and steel container

Michelin et al. (2013, 2015)

Site of Glinet (Normandy) Blast furnace 16th c. Soil saturated with anoxic water SiO2 : 62 à 77 %, Al2O3 : 5 à 9 %, CaO : 16 à 25 % VITREOUS SLAGS

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Þ Fe-silicates precipitation is a long-term mechanism but there is a drop in the alteration rate in cracks Siderite (Fe1-xCaxCO3) Fe-silicates Alteration thickness: ~ 20 µm (external cracks) / 2-6 µm (internal cracks) Gel Pristine glass

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SLIDE 28
  • III. Roman glass alteration modeling

Alteration for 1800 years In a stable environment (seawater at 15°C) Morphological analogy

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29

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Border zone (BZ)

  • Thick altered cracks
  • Smectites
  • 84 % of total alteration

Smectites

Internal zone (IZ)

  • Thin altered cracks (5-20 µm)
  • Hydrated glass (and smectites)
  • Cracks density 6x higher
  • 16 % of total alteration

Smectites Hydrated glass

Þ Low contribution of internal cracks to global alteration (+ sealing) ALTERATION PHENOMENOLOGY

1 cm

Verney-Carron et al. (2008)

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31

Na+ H+

pH

diffusion

saturation

SiO2

Glass Leached glass smectites

pH, Mg, CO3

2-

carbonates

Þ Need to model the coupling between chemistry and transport

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SLIDE 32

32

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van der Lee (2005) ; van der Lee et De Windt (2002) ; Lagneau (2005)

1st step: interdiffusion

  • Arch. glass

SiO2 Na2O CaO Al2O3 Li2O SiO2(aq) Ca2+ Al3+ Na+ Li+

Leached glass

SiO2 CaO Al2O3

  • D

+ D

2nd step: dissolution/precipitation

Leached glass

SiO2 CaO Al2O3

  • r

SiO2(aq) Ca2+ Al3+

LogK

Secondary phases

GEOCHEMICAL MODEL HYTEC software Thermodynamic database (Chess – EQ3/6)

Pure water: analcime, gyrolite, tobermorite Seawater: saponite, calcite, aragonite + brucite, portlandite, gibbsite

[ ]

÷ ø ö ç è æ - × × =

+

RT H DNa 93600 exp 678 .

37 .

[ ]

[ ]

÷ ÷ ø ö ç ç è æ

  • ×

÷ ø ö ç è æ - × × × =

  • +

b te Cristobali

K SiO H RT H r

4 4 32 . 9

1 85600 exp 10 73 . 6

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SLIDE 34

34

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Simulation results of 2 cracks (≠ apertures a and ≠ distance from the external surface)

a = 100 µm - 1 cm

Þ The external cracks are in contact with a diluted medium à r0

a = 2 µm – 5.6 cm

Þ Good agreement between simulations and observations Þ Validation of the predictive capacity of the geochemical model Þ Strong coupling between chemistry and transport

Verney-Carron et al. (2010a,b)

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Sext = 7 x Sgeo Sint = 79 x Sgeo Þ If only the internal surfaces were leached, more than 650,000 years would be necessary for complete alteration

  • f the Roman glass blocks, but external surfaces alteration would limit the lifetime to about 20,000 years.
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Transposition to nuclear glass alteration Sgeo = 1.7 m² Sext = 5 x Sgeo Sint = 40 x Sgeo T = 50°C (after 4000 years) r0 = 5.1 µm/y rr = 0.008 µm/y D (50°C, pH 7) = 6.8·10-23 m²/s Þ If like for Roman glass, internal surfaces are controlled by diffusion, 5% of alteration after 100 000 years.

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  • IV. Pre-viking Swedish hillfort glass / LAW glasses

Þ It could be a good analogue of LAW glasses

Weaver et al. (2018)

Broborg, Sweden 500 CE

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Outcomes

  • No composition analogy BUT
  • Important to study other kinds of glasses

à General understanding of glass alteration (even minerals) : similar mechanisms but different kinetics.

  • Important to continue the modeling work

à To demonstrate the feasibility and the predictive capacity à To extend the range of applications of nuclear glass models

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Atacama tektite

Tektites: rich in Si, Al and low H2O content

Tektites

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Impactites:

Lybian desert glass

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Þ No protective role of the alteration layer

  • Stained glass weathered in atmosphere

Lombardo et al. (2010)

Enrichment in D at the interface of samples exposed at 90 %RH (14 months)

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Magma can have a different composition ↔ partial melting, fractional crystallization, assimilation of surrounding crust. Melting of peridotite (5-20 %) à basalt composition Melting of continental crust à rhyolite

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The composition influences the viscosity and the vitrification. Glass < high viscosity (to inhibit the crystallization) + sudden cooling to chill the material to a glass

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  • Tektites and impactites

Impactite is formed by the impact of a meteorite and tektites from terrestrial debris ejected far from the impact.

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46

Lunar glass Ti Lunar basalt Figeac Basalt Andesite Phonolite Rhyolite Lybian glass Rochechouart Fulgurite Impactite

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EXPERIMENTAL VALIDATION SUMMARY ü Alkalis and pH: good simulation pH is an important parameter of the coupling between chemistry and transport ü Ca: underestimated at low pH due to its release by interdiffusion However, Ca is highly concentrated in seawater ü Si: overestimated at high pH (interactions with Ca) and in seawater (stoichiometry) Change of the database (smectites) Þ The chemical model can be coupled with transport and tested on long-term

7 8 9 10 11 12 100 200 300 400 Durée en j pH pH exp pH sim

Experiment in seawater at 50°C and SA/V = 20 cm-1

0.00 0.01 0.02 0.03 0.04 0.05 0.06 50 100 150 200 Durée en j [i] en mol∙ℓ

  • 1

Mg exp Mg sim 0.000 0.001 0.002 0.003 0.004 0.005 50 100 150 200

Durée en j

[i] en mol∙ℓ

  • 1

Si exp Si sim