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R = v SNR V ¯ size 12{R= { {v rSub { size 8{ ital "SNR"} } } over { {overline {V}} } } } {}

This method allows us to obtain experimental values of dissolution rates just by precise measuring of average surface heights. Moreover, using this method we can measure local dissolution rates at etch pits by monitoring changes in the volume and density of etch pits across the surface over time. VSI technique is capable to perform these measurements because of large vertical range of scanning. In order to get precise values of rates which are not depend on observing place of crystal surface we need to measure enough large areas. VSI technique provides data from areas which are large enough to study surfaces with heterogeneous dissolution dynamics and obtain average dissolution rates. Therefore, VSI makes possible to measure rates of normal surface retreat during the dissolution and observe formation, growth and distribution of etch pits on the surface.

However, if the mechanism of dissolution is controlled by dynamics of atomic steps and kink sites within a smooth atomic surface area, the observation of the dissolution process need to use a more precise technique. AFM is capable to provide information about changes in step morphology in situ when the dissolution occurs. For example, immediate response of the dissolved surface to the changing of environmental conditions (concentrations of ions in the solution, pH etc.) can be studied by using AFM.

SEM is also used to examine micro and nanotexture of solid surfaces and study dissolution processes. This method allows us to observe large areas of crystal surface with high resolution which makes possible to measure a high variety of surfaces. The significant disadvantage of this method is the requirement to cover examine sample by conductive substance which limits the resolution of SEM. The other disadvantage of SEM is that the analysis is conducted in vacuum. Recent technique, environmental SEM or ESEM overcomes these requirements and makes possible even examine liquids and biological materials. The third disadvantage of this technique is that it produces only 2D images. This creates some difficulties to measure Δ h ¯ size 12{Δ {overline {h}} } {} within the dissolving area. One of advantages of this technique is that it is able to measure not only surface topography but also chemical composition and other surface characteristics of the surface. This fact is used to monitor changing in chemical composition during the dissolution.

Bibliography

  • A. C. Lasaga, Kinetic Theory in the Earth Sciences . Princeton Univ. Press, Princeton, NJ (1998).
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  • D. Kaczmarek, Vacuum , 2001, 62 , 303.
  • P. Hariharan. Optical interferometry , Second edition, Academic press (2003) ISBN 0-12-311630-9.
  • A. Luttge and P. G. Conrad, Appl. Environ. Microbiol. , 2004, 70 , 1627.
  • A. C. Lasaga and A. Luttge, American Mineralogist , 2004, 89 , 527.
  • K. J. Davis and A. Luttge, Am. J. Sci. , 2005, 305 , 727.
  • S. H. Wang and Tay, Meas. Sci. Technol. , 2006, 17 , 617.
  • A. Luttge and R. S. Arvidson, in Kinetics of water-rock interaction , Ed. S. Brantley, J. Kubicki, and A. White, Springer (2007).
  • L. Zhang and A. Luttge, American Mineralogist , 2007, 92 , 1316.
  • C. Fischer A. and Luttge, Am. J. Sci. , 2007, 307 , 955.
  • Y. Wyart, G. Georges, C. Deumie, C. Amra, and P. Moulina, J. Membrane Sci. , 2008, 315 , 82.
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Source:  OpenStax, Nanomaterials and nanotechnology. OpenStax CNX. May 07, 2014 Download for free at http://legacy.cnx.org/content/col10700/1.13
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