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American Mineralogist; May 2003; v. 88; no. 5-6; p. 846-854
© 2003 Mineralogical Society of America
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Thermodynamics of Fe oxides: Part I. Entropy at standard temperature and pressure and heat capacity of goethite ({alpha}-FeOOH), lepidocrocite ({gamma}-FeOOH), and maghemite ({gamma}-Fe2O3)

Juraj Majzlan1,*, Brian E. Lang2, Rebecca Stevens2, Alexandra Navrotsky1, Brian F. Woodfield2 and Juliana Boerio-Goates2

1 Thermochemistry Facility, Department of Geology, University of California at Davis, Davis, California 95616, U.S.A.
2 Department of Chemistry and Biochemistry, Brigham Young University, Provo, Utah 84602, U.S.A.

The heat capacities (CP) of goethite (goe, {alpha}-FeOOH), lepidocrocite (lep, {gamma}-FeOOH), and maghemite (mag, {gamma}-Fe2O3) were measured from below liquid helium temperature up to their decomposition temperatures by a combination of adiabatic, semi-adiabatic, and differential scanning calorimetry. All three phases were synthetic, with <160 ppm of Al. Chlorine content in goe (32 ppm) and lep (202 ppm) is too low to affect the calorimetric results of this study. Phase purity was verified by Rietveld refinement of the powder X-ray diffraction (XRD) patterns; we determined lattice parameters, atomic positions, crystallite size, and microstrain for all three samples. The Brunauer-Emmet-Teller (BET) surface area is 21 (goe), 23 (lep), and 18 (mag) m2/g. No amorphous impurity was found in the goethite sample by extraction of the oxalate soluble fraction. The excess water, determined from weight loss after firing at 1200 K overnight, is 0.083 ± 0.010 (goe), 0.087 ± 0.005 (lep), 0.042 ± 0.003 (mag) moles of water per mole of FeOOH or Fe2O3.

The entropy at standard temperature and pressure (STP) was calculated from subambient CP data and corrected for the excess water content using a Debye-Einstein representation of the CP of hexagonal ice. The entropy at STP is 59.7 ± 0.2 (goe), 65.1 ± 0.2 (lep), and 93.0 ± 0.2 (mag) J/(K·mol). The XRD pattern of maghemite lacks superstructure peaks, and complete disorder of the vacancies leads to configurational entropy Sconf = 2.0 J/K·mol. Because very weak superstructure peaks can be overlooked, or the vacancies may be short-range ordered, this calculated Sconf represents only an upper limit. The heat capacity above 273 K was fitted to a Maier-Kelley polynomial CP [J/(K·mol), T in K] = a + bT + cT–2. The CP polynomial coefficients are a = 1.246, b = 0.2332, c = 313900 (goe, valid in temperature range 273–375 K), a = 59.76, b = 0.06052, c = –772900 (lep, 273–390 K), and a = 106.8, b = 0.06509, c = –1886000 (mag, 273–760 K).




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