Modeling the electrochemical properties and the complex conductivity of calcite

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1 Modeling the electrochemical properties and the complex conductivity of calcite Shuai Li Philippe Leroy Damien Jougnot André Revil Nicolas Devau Frank Heberling Mohamed Azaroual

Ghorbani (2007) Pierre and Marie Curie University > Phase shift between imposed current and measured

2 Complex conductivity in frequency or spectral induced polarization (SIP) > Sinusoidal electrical current injected. Electrical potential difference measured. Thesis A. Ghorbani (2007) Pierre and Marie Curie University > Phase shift between imposed current and measured voltage. > Method sensitive to conduction and polarization currents at the solid/water interface and inside conductive metals. jeudi 9 mars 2017 > 2

Complex conductivity (CC) or complex resistivity > Method developed initially for the mining exploration because of its sensitivity to conduction and

Application of the CC method in hydrogeophysics to estimate for instance the transport properties of porous media for environmental and hydrogeological

3 Complex conductivity (CC) or complex resistivity > Method developed initially for the mining exploration because of its sensitivity to conduction and polarization currents in conductive metals. > High increase of the accuracy of CC measurements, inversion and interpretation during the last decades. Application of the CC method in hydrogeophysics to estimate for instance the transport properties of porous media for environmental and hydrogeological investigations. > Example: monitoring remediation of groundwaters contaminated by organic pollutants using zero valent iron microparticles. Orozco et al. (2015) EST jeudi 9 mars 2017 > 3

4 Grain polarization model > However, frequency behavior of SIP spectra still not exactly known.? > Necessity to develop mechanistic SIP models describing key transport phenomena at the pore scale responsible for the measured SIP response. > Grain polarization model applied to calcite precipitation in porous media. jeudi 9 mars 2017 > 4

(2010), On the complex conductivity signatures of calcite

5 Grain polarization model of calcite - experimental data (1) > Spectral induced polarization (SIP) experiment of calcite precipitation Wu et al. (2010), On the complex conductivity signatures of calcite precipitation, Journal of Geophysical Research: Biogeosciences. jeudi 9 mars 2017 > 5

6 Grain polarization model of calcite - experimental data (2) > Measured sample complex conductivities s * (w) = I(w)/(U(w)k) s * (w) = s + is = se i s= (s ² +s ²) 0.5 = tan -1 (s /s ) s /s I(w): injected sinusoidal current U(w): measured electrical potential difference k: geometric factor : phase shift between measured electric potential difference and imposed current s sensitive to conduction currents s sensitive to polarization currents > Imaginary conductivity response of calcite precipitation s f s f jeudi 9 mars 2017 > 6

Zeta potential of the calcite/water interface > Surface complexation and dissolution/precipitation phenomena controlled by the electrical double layer (EDL) surrounding calcite in water.

7 Zeta potential of the calcite/water interface > Surface complexation and dissolution/precipitation phenomena controlled by the electrical double layer (EDL) surrounding calcite in water. > No reliable surface charge density measurements of calcite in water. > Zeta potential: key parameter to constrain surface complexation models of the calcite/water interface. > Helmholtz-Smoluchowski (HS) equation used to infer zeta potentials from streaming potential measurements. > Is the HS equation reliable to describe the zeta potential of calcite particle? jeudi 9 mars 2017 > 7

Streaming potential measurements of calcite > Imposed water pressure difference p across

calcite/water interface, zeta potential displacement of the excess of charge in the

sample J C Anton Paar SurPASS electrokinetic analyzer > But, is it possible to neglect

8 Streaming potential measurements of calcite > Imposed water pressure difference p across coarse crystal powder: water flow U, streaming current J Str shear plane at the calcite/water interface, zeta potential displacement of the excess of charge in the diffuse layer macroscopic electric field, streaming potential conduction current in the sample J C Anton Paar SurPASS electrokinetic analyzer > But, is it possible to neglect conduction currents at the surface of calcite to infer zeta potential from streaming potential? jeudi 9 mars 2017 > 8

9 Theory of the streaming potential in steady-state conditions > Conduction and streaming current densities for viscous laminar flows: ε ζ J = J σ ψ w C + J = + p Revil et al. (1999) Journal of Geophysical Research Str ηwf > Streaming potential coupling coefficient C + sample electrical conductivity σ : Δψ εw C = = ζ Δp ηwfσ J= 0 ηwfσ Zeta potential ζ = C ε > Helmholtz-Smoluchowski equation: σw εwζ J = J C + JStr = ψ+ p F ηwf Δψ εw C = = ζa Δp η 0 wσ J= w ηwσ Apparent zeta potential ζ a = C ε > Sample conductivity: w σ F w σ = + σ s σ w : water electrical conductivity σ s : surface conductivity F: electrical formation factor w : water dielectric permittivity w : water viscosity jeudi 9 mars 2017 > 9 w w Can σ s be neglected to infer from C?

10 Apparent zeta potential vs corrected zeta potential of calcite powder HS equation High surface conductivity effects Corrected zeta potentials jeudi 9 mars 2017 > 10

Electrical double layer around calcite ((104) plane) > Surface charge of the calcite particle in water due to the: - calcium surface sites >Ca-OH -0.5 - carbonate surface sites >CO 3-0.

11 Electrical double layer around calcite ((104) plane) > Surface charge of the calcite particle in water due to the: - calcium surface sites >Ca-OH carbonate surface sites >CO > Surface charge compensated by: - adsorbed counter-ions at the Stern, - adsorbed counter-ions and co-ions in the diffuse layer. > Assumed shear plane at the beginning of the diffuse layer. Heberling et al. (2014) Applied geochemistry No water flow High viscosity φ d = ζ Water flow Low viscosity jeudi 9 mars 2017 > 11

12 Basic Stern model (BSM) of calcite (1) > Stoichiometric matrix of aqueous and surface reactions Li, Leroy et al. (2016), Influence of surface conductivity on the apparent zeta potential of calcite, Journal of Colloid and Interface Science jeudi 9 mars 2017 > 12

13 Basic Stern model of calcite (2) > Parameters - total surface site density, - equilibrium constants of adsorption, - capacitance C 1. > Measured data - electrophoresis, - streaming potential. Assumption: φ d = ζ > Output data - electrical potentials, zeta potential, - surface site densities of adsorbed ions, - surface charge densities of the Stern and diffuse layer. Computed excess of charge controlling the complex conductivity response. jeudi 9 mars 2017 > 13

14 Grain polarization model of Leroy et al. (2008) > Assumptions - continuous diffuse layer and discontinuous Stern layer. > Application of a sinusoidal electrical field - ions electromigration in the diffuse layer conduction of the diffuse layer. Leroy, Revil et al. (2008), Complex conductivity of watersaturated packs of glass beads, JCIS - ions electromigration and diffusion in the Stern layer polarization of the Stern layer. jeudi 9 mars 2017 > 14

15 Improvement of the grain polarization model of Leroy et al. (2008) > Multivalent and monovalent ions adsorbed in the Stern layer > Effects of the diffuse layer on Stern layer polarization Lyklema et al. (1983) JEC decrease of the relaxation time of the polarization of the Stern layer increase of the associated characteristic frequency f 2 τ = a / 2D M f =1/τ S Weak diffuse layer D S : diffusion coefficient of the counter-ions in the Stern layer M: effects of the diffuse layer on Stern layer polarization (M 1) w: angular frequency ω = 2 πf Strong diffuse layer jeudi 9 mars 2017 > 15

16 Grain polarization model theory (1) 1. BSM electrical potential at the onset of the diffuse layer surface charge density of the Stern layer ions surface site densities in the diffuse layer 2. Specific surface conductivities of the Stern and diffuse layer b s N d d d β = b bqb s = ez ibi Γi d i= 1 Σ β 3. Complex surface conductivity of the particle σ *(a,ω) = σ (a,ω) + iωε τ s 1 f 2 a 2 D 2 b = = = b bm s b b d σ s*(a, ω) = s s a + 1+ iωτb(a) + iωτ 2k a B 2 s (a) q Tβ b M jeudi 9 mars 2017 > 16 Q b d Γ i φ d : ions surface mobility in the Stern layer B i : ions effective mobility in the diffuse layer (electromigration+electroosmosis) ε s : dielectric permittivity of the particle (constant) iωαρ M = 1+ B s ε 0 qqb k TC C d : differential capacitance of the diffuse layer d 3 1 2

17 Grain polarization model theory (2) 4. Superposition principle: complex conductivity of particles of different sizes 5. Differential effective medium theory: porous medium complex conductivity F = m Q σs * = f(di)σs*(di, ω) i= 1 σw* 1 σs* /σw* σ* F 1 σs* / σ* = σ * = σ + iωε w w w m f(d i ): particle size distribution σ w ε w : water conductivity : water dielectric permittivity F: formation factor : porosity m: cementation exponent Self-similar model of rock (from Sen et al. (1981), A self-similar model for sedimentary rocks with application to the dielectric constant of fused glass beads, Geophysics) jeudi 9 mars 2017 > 17

18 Grain polarization model - comparison with experimental data (1) > Real and Imaginary conductivity response of calcite precipitation s f s f jeudi 9 mars 2017 > 18

19 Grain polarization model - comparison with experimental data (2) > Inverted particle size distribution Particle size (m) Particle size (m) Leroy et al., Modeling the evolution of spectral induced polarization during calcite precipitation on glass beads, under review in Geophysical Journal International jeudi 9 mars 2017 > 19

20 Grain polarization model - comparison with experimental data (3) > Adjusted cementation exponent for the shape of the calcite particles = 0.3 F = m (s ~ 0.06 S m -1 (day 2 - day 12)) jeudi 9 mars 2017 > 20

21 Grain polarization model - comparison with experimental data (4) > Modeled electrochemical properties of the calcite/water interface > Complex conductivity model parameters jeudi 9 mars 2017 > 21

22 Conclusions and perspectives > Complex conductivity model of the electrochemical polarization of the Stern layer surrounding calcite particles > Monovalent and multivalent counter-ions in the Stern layer > Effects of the diffuse layer on Stern layer polarization > Grain complex conductivity model combined with a basic Stern model of the electrochemical properties of the calcite/water interface > Zeta potentials of calcite corrected of surface conductivity effects > Measured complex conductivity spectra of calcite precipitation on glass beads successfuly reproduced by our models > Particle size distribution and particle shape deduced from our models > Application of our approach to non-intrusively estimate transport properties of porous media where calcite precipitation occurs jeudi 9 mars 2017 > 22

23 Thank you for your attention!

Modeling the evolution of spectral induced polarization during calcite precipitation on glass beads

Modeling the evolution of spectral induced polarization during calcite precipitation on glass eads Philippe Leroy Shuai Li Damien Jougnot André Revil Yuxin Wu Complex conductivity in frequency or spectral