Mineral equilibria in silicate and ore systems


Kozerenko S.V.1, Fadeev V.V.1, Rusakov V.S.2, Kalinichenko A.M.3, Kolpakova N.N.1, Kopneva L.A.1 Reactions of iron hydroxides with sulfide sulfur.

key words [iron hydroxide sulfur pyrite]

The reactions under study are considered as main reactions of sulphide formation and to govern the oxygen and sulphate contents in the Word ocean at any geological epoch (1-3). Earlier, on the example of pyrite it was demonstrated that the most thermodynamically stable iron sulfides (final phases) cannot be precipitated directly from a solution at low temperatures because of high nucleation barrier. These sulfides more likely are the interactions products of metastable phase-precursors with the initial solutions (4). The aim of this study is to investigate the possible pathways of reactions proceeding namely in the interaction of iron hydroxides with sulphide sulphur at parameters of natural processes.

Solid products of these reactions obtained in laboratory were studied by use of chemical phase analysis (CA), x-ray diffractometry (XRD), M÷ssbauer spectroscopy (MS), electron spin resonance (ESR) and proton magnetic resonance (PMR) techniques.

In the interaction of Fe3+ hydroxides with sulphide sulphur the elemental sulphur is formed according to the reaction 2Fe3+ + S2- = 2Fe2+ + S0. As a result, the redox conditions of the case are determined by the buffer pairs F2S2-So. In this conditions at the first step of the reaction the x-ray amorphous iron sulphide is formed. According to CA data its content is close to monosulphide (Fe:S=1:1). On the base of PMR data this phase along with absorbed H2O was found to contain the structure protons presumably localised within OH- and HS- atomic groups. Thus, the primary sulphide phase was considered a compound of FeOHHS composition (phase precursors-hydrotroilite). We conclude that the following reaction takes place in this case 2Fe(OH)3 + 3H2S =2 FeHSOH +So. In the process of precipitate ageing the equilibrium pyrite formation was ascribed in terms of the following reaction: FeOHHS + So = FeS2 + H2O.

The synthesized phases, both the phase-precursor and final ones, were studied by MS on 57Fe nuclei and by ESR. Iron was found to exist predominantly in the form of Fe2+. Fe2+ ions in FeOHHS and FeS2 crystalline structures occurred in low spin state. The average values of isomer shift and quadrupole line shift for pyrite and hydrotroilite are in good agreement with corresponding values for the pyrite phase. As a result, we conclude that Fe2+ ions in the structure of the phase-precursor presumably as well as that of final phase should be ascribed as having the pyrite-like nearest surrounding, i.e. the cation sublattice of mineral phases in the process of x-ray amorphous to crystalline state transition is not sufficiently transformed. All the compositional changes of sulphide phases are related to changes in anion sublattice. PMR studies of synthesised phases lead to a conclusion that OH- and HS- atomic groups in sublattice are substituted for S22-.

In the interaction of Fe2+ with sulphide sulphur the redox parameters of corresponding reactions are determined by the series of sulphide-hydroxide sulphide buffer pairs being governed by pH and pS values of the initial solutions. In these conditions phase-precursor is more commonly presented by tochilinite [2 FeS1.5Fe(OH)2] subsequently transforming to mackinawite (FeS). According to structural studies performed by N.I.Organova the tochilinite structure is interpreted as mixed layered hydroxide-sulphide compound with regular interlayer brycite type layers of Fe(OH)2 composition with tetrahedral mackinawite like layers of FeS composition. Thus the interaction between Fe2+ with sulphide sulphur could be ascribed as follows:

1) 3.5 Fe(OH)2 + 1.5H2S = 2Fe(OH)21.5FeS + 3H2O

2) 2 Fe(OH)21.5FeS + 2H2S = 3.5FeS + 4H2O

The 57Fe Mossbauer spectra tochilinite (phase-precursor) and mackinawite (final-phase) have been taken at room temperature. The first showed no magnetic hyperfine structure whereas the second did. Chemical isomer shifts, quadruple interactions, and magnetic hyperfine fields have been determined from these spectra. The spectrum of tochilinite consists of some quadruple doublets which shows that the Fe2+ -ions states are the low-spin and high-spin states. For

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tochilinite superparamagnetic effect due to the rapid relaxation of atomic spins is observed. In fine particle synthetic tochilinite, magnetic reversals due to the thermal motion take place in a shorter time than the Mossbauer transition. The Fe2+-ions in this case are in the low-spin state.

Consequently our study is sufficient to allow the following conclusion: the reactions of iron hydroxide with sulphide sulphur have a steplike character. The first step is the hydroxide-sulphide formation, the latter being subsequently transformed to sulfides (pyrite or mackinawite). The phase-precursor is presented by hydrotroilite on the pyrite stability field whereas the tochilinite is formed in more reducing conditions.

References:

  1. Holland H.D. (1978) The Chemistry of the Atmosphere and Ocean. //Willey and Sons, 351p.
  2. Garrels R.M. and Lerman A. (1981) // Proc. Nat. Acad. V.78, p.4652.
  3. Berner R.A. (1984) // Geochim. et cosmochim. Acta, V.48, p.605.
  4. Shoonen M.A.A., Barnes H.L. (1991) // Geochim. et cosmochim. Acta, V.55, p.1495,1505,3491.
  5. Organova N.I. (1989) Crystallochemistry of incommensurated and modulated mixed-layer minerals. // Moscow, Nauka, 144p.

# Fed'kin M.V., Kotova A.A., and Osadchii E.G. A study of thermodynamic properties of pyrrhotite by EMF measurements.

key words [pyrrhotite thermodynamic properties]

A double electrochemical cell with Y2O3-stabilized ZrO2 as a solid electrolyte with O2--conductivity was used to measure the oxygen partial pressures in the equilibrium

3FeSpo + 6Ag + 2O2 = Fe3O4 + 3Ag2S (I)

Equilibrium (I) in turn results from the combination of the pyrrhotite-magnetite equilibrium

3FeS(po) + 5O2 = Fe3O4 + 3SO2

and the auxiliary equilibrium

2Ag + SO2 = Ag2S + O2

which fixes the SO2 partial pressure in the Fe-S-O system (figure). It is noteworthy that the components of the auxiliary system (Ag and Ag2S) do not yield any solid solutions with pyrrhotite and magnetite.

The oxygen partial pressures in Equilibrium (I) were measured relative to Ni-NiO buffer (pO2*) (Pejryd, 1984) in the cell

Pt, pO2, FeS(po), Fe3O4, Ag, Ag2S|YSZ|Ni, NiO, pO2*, Pt(A)

where YSZ denotes Y2O3-stabilized ZrO2.

Rezults and calculations

The emf (E) of an oxygen electrochemical cell relates to the difference in pO2 between the sample and reference system of the cell as:

E = RT(lnpO2* - lnpO2)/nF (1)

The least-squares treatment of the oxygen partial pressures in equilibrium (I) derived from the emf values of Cell (A) within the temperature range 980 - 1070 K gives the equation

lgO2 = 7.071 - 24257.6/T ( = +0.006) (2)

Fig. The stability diagram of the Fe-S-O system at 1000 K.

The calculation of K(I) and G(I) from the pO2 values obtained should take into account the variations of pyrrhotite composition with temperature according to the Ag-Ag2S buffer. From Barton and Toulmin's data (1964), pyrrhotite composition in equilibrium (I) varies from Fe0.949S at 980 K to Fe0.957S at 1070 K. As a result, equilibrium (I) can be rewritten in the general form as:

3Fe1-xSpo + 6Ag + 2(1-x)O2 = (1-x)Fe3O4 + 3Ag2S (II)


# This study was supported by the Russian Basic Research Foundation, project N 96-05-64872

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The equilibrium constant and Go values for equilibrium (II) are derived respectively as:

lgK(II) = -2(1-x)lgpO2 (3)

and Go = -RTlgK(II)ln10 (4)

The free energy of pyrrhotite formation can be determined as:

Gfo(po)= Gfo(Ag2S) + (1-x)/3 Gfo(Fe3O4) - 1/3*
*Go (II) (5)

The scatter of literature thermodynamic data on Ag2S and Fe3O4 is about 2.5 and 6.5 kJ, respectively, at 1000 K. For the calculation by equation (5), data on magnetite from Spencer and Kubaschewski (1978) were preferred which were also obtained by emf method and are in good agreement with other data (Bjorkman, 1985; O'Neill, 1987; Jacobson, 1985):

D Gfo(Fe3O4)/J/mol =
=-1089500 + 389.850(T/K) -12.548(T/K) ln(T/K).

As for Ag2S, data from Barin (1989) were chosen, which hold a mid-position among all published data on silver sulfide.

Within the T interval 980-1070 K, the temperature dependences of the Go(II) and Gfo(po) values obtained are described respectively by the equations:

Go (II) = -835181.4 + 209.494(T/K), = +250 J/mol

Gof(po) = -128679 + 35.83164(T/K), = +-80 J/mol

Discussion

The experimental Gof(po) values obtained are in satisfactory agreement with those calculated from data of Eriksson and Fredriksson (1983) for the same pyrrhotite compositions. Considering the existing uncertainties in Gof(Fe3O4) and Gof(Ag2S), the experimental Gof(po) values vary within 4.5 kJ and thus overlap the Eriksson and Fredriksson's data (1983).

References:

  1. Barin I. (1989) Thermodynamic Properties of Pure Substances. // VCH,. Bjorkman, B., CALPHAD, V.9, N.3, pp. 271-282.
  2. Eriksson G. and Fredriksson M. (1983) // Metallurgical Transactions, B, V.14B, pp. 459-464.
  3. Jacobson, E., Scandinavian (1985) // J. Metallurgy, V.14, pp. 252-256.
  4. O'Neill H.St.C. (1987) // Amer. Miner., V.72, N.1-2, pp. 67-75.
  5. Pejryd L. (1984) Acta Chemica Scandinavica, V.A38, pp. 241-246.
  6. Spencer L.S. and Kubaschewski O.A. (1978) // CALPHAD, V.2, pp. 147-167.
  7. Toulmin III P. and Barton P.B. (1964) // Geochim. Cosmochim. Acta, no. 5, pp. 641-671.

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