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Published online 2 December 2005
Published in Soil Sci Soc Am J 70:14-23 (2006)
DOI: 10.2136/sssaj2005.0044
© 2005 Soil Science Society of America
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Percolation Treatment of Charge Transfer in Humidified Smectite Clays

Allen G. Hunta,*, Sally D. Logsdonb and David A. Lairdb

a Dep. of Physics and Dep. of Geology, Wright State Univ., Dayton, OH 45435
b National Soil Tilth Lab., 2150 Pammel Dr., Ames, IA 50011



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Fig. 1. Diagram of possible pathways for proton transfer (a) along interlayer face through fill water away from interlayer cation, or (b) in two-dimensions passing close to cation.

 


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Fig. 2. Measured and predicted electrical conductivity spectra at the four humidity levels for Ca-hectorite showing the offset for the highest three humidity levels.

 


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Fig. 3. Relation between the exponent s and the activation energy.

 


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Fig. 4. The dc electrical conductivity as a function of the characteristic angular frequency, {omega}c.

 


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Fig. 5. The electrical conductivity at the phonon frequency minus the dc electrical conductivity as a function of the dc electrical conductivity minus the offset.

 


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Fig. 6. Predicted dc electrical conductivity as a function of measured: (a) predicted with no prefactor vs. measured minus offset (0.015 S m–1) forced through origin; (b) predicted percolation basal spacing with offset including samples with zero spacing (solid) or mean water content (dashed) as a function of measured; (c) predicted basal spacing not including samples with zero spacing.

 


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Fig. 7. Relation between 4{pi}{varepsilon}0{varepsilon}phlwvph/[qr0(4 + w)] and {sigma}ph as described in Eq. [20].

 





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