The Deposition of Calcium Oxalate and Amorphous Silica Scale under Dynamic Conditions which Simulate sugar mill Evaporators

2008 ◽  
Vol 12 (3-4) ◽  
pp. 309-322
Author(s):  
H. Yu ◽  
R. Sheikholeslami ◽  
W.O.S. Doherty
AIChE Journal ◽  
2005 ◽  
Vol 51 (4) ◽  
pp. 1214-1220 ◽  
Author(s):  
Hong Yu ◽  
Roya Sheikholeslami ◽  
William O. S. Doherty

1982 ◽  
Vol 22 (01) ◽  
pp. 9-16 ◽  
Author(s):  
Oleh Weres ◽  
Andrew Yee ◽  
Leon Tsao

Abstract The polymerization of dissolved silica in aqueous solutions up to 100 degrees C and containing up to 1 M NaCl has been studied experimentally, and theoretically. In this paper, the results of this work are presented in a form suitable for practical use in interpreting and predicting the chemistry of silica in geothermal brines. Empirical equations for calculating the rate of molecular deposition of silica on surfaces as a function of silica concentration. temperature, pH. and salinity are presented. Theoretically calculated type curves that depict the decrease of dissolved silica concentration by homogeneous nucleation and particle growth are presented, along with the procedures for using them to predict the course of this process under different conditions. Introduction Usually, silica precipitates from geothermal brines as colloidal amorphous silica (AS). The process of AS precipitation consists of the following steps. 1. Random growth of silica polymers past critical nucleus size. Above this size, the polymers become colloidal AS particles that are large enough to grow spontaneously and without interruption. This process is called homogeneous nucleation. 2. Growth of the supercritical AS particles by further chemical deposition of silicic acid on their surfaces. 3. Coagulation or flocculation of the colloidal particles to give a floc-like precipitate or gel. 4. Cementation of the coagulated particles by chemical bonding and further deposition of silica between them to form silica scale and other solid deposits. The preceding sequence of processes occurs when the concentration of dissolved silica is high enough for homogeneous nucleation to occur at a significant rate. Very roughly, this requires supersaturation by a factor of 2.5 or more. If this condition is met, rapid polymerization occurs, and massive precipitation or scale deposition may follow. This is the case with the brine at Niland (CA). Cerro Prieto (Mexico), and Wairakei (New Zealand). after it has been flashed down to atmospheric pressure. The voluminous floc-like silica deposits encountered in these areas consist of colloidal AS that has been flocculated by the salts in the brine. The crumbly gray and white scales associated with this material are cemented aggregates of colloidal silica. If the concentration of dissolved silica is too low for rapid homogeneous nucleation to occur, relatively slow heterogeneous nucleation and the deposition of dissolved silica directly on solid surfaces become the dominant ploymerization processes. The product of the latter process (essentially Step 2 of the preceding sequence alone) is a dense vitreous silica. At higher temperatures, this process may produce scale at a significant rate. This paper has two purposes: to summarize succinctly and quantitatively what we have learned in our kinetic studies of silica polymerization and to demonstrate by example how our results may be applied to studying practical problems in geothermal energy utilization. Because it is a summary, actual experimental data and most details of derivation have been omitted, they may be found elsewhere. Because some of the material in this paper is condensed from an earlier paper, it is partly of a review nature. It is an updated version of an earlier article. Studies of the actual formation of silica scale and the removal of colloidal silica from geothermal brines have been reported elsewhere. Molecular Deposition on Solid Surfaces By molecular deposition we mean the formation of compact, nonporous AS deposits by chemical bonding of dissolved silica directly onto solid surfaces. This is also the mechanism by which colloidal silica particles grow once nucleated. SPEJ P. 9^


2003 ◽  
Vol 42 (4) ◽  
pp. 904-910 ◽  
Author(s):  
Hong Yu ◽  
Roya Sheikholeslami ◽  
William O. S. Doherty

2016 ◽  
Vol 88 (10-11) ◽  
pp. 1037-1047 ◽  
Author(s):  
Argyro Spinthaki ◽  
Georgia Skordalou ◽  
Aggeliki Stathoulopoulou ◽  
Konstantinos D. Demadis

AbstractSilicic acid polycondensation leads to the formation of amorphous silica. This process is of great importance to the survival of certain living organisms, such as diatoms and sponges, but presents a significant problem in various production facilities that use water for heating or cooling. In the latter, amorphous silica can be a recalcitrant deposit that can hamper proper system operation. Hence, inhibition of silicic acid polycondensation by chemical inhibitors is an intensely sought strategy by water system operators. In this manuscript, we report the inhibitory effect of zwitterionic phosphonated analogs (PPEI’s) of the cationic polymeric chemical additive polyethyleneimine (PEI) in mildly supersaturated silica solutions (500 ppm/8.3 mM “Si”) at pH=7. The inhibition efficiency of PPEI’s depends on a variety of parameters, such as concentration and degree of phosphonomethylation of the parent PEI polymer.


Author(s):  
Vicki L. Baliga ◽  
Mary Ellen Counts

Calcium is an important element in the growth and development of plants and one form of calcium is calcium oxalate. Calcium oxalate has been found in leaf seed, stem material plant tissue culture, fungi and lichen using one or more of the following methods—polarized light microscopy (PLM), scanning electron microscopy (SEM), transmission electron microscopy (TEM) and x-ray diffraction.Two methods are presented here for qualitatively estimating calcium oxalate in dried or fixed tobacco (Nicotiana) leaf from different stalk positions using PLM. SEM, coupled with energy dispersive x-ray spectrometry (EDS), and powder x-ray diffraction were used to verify that the crystals observed in the dried leaf with PLM were calcium oxalate.


Author(s):  
H. J. Arnott ◽  
M. A. Webb ◽  
L. E. Lopez

Many papers have been published on the structure of calcium oxalate crystals in plants, however, few deal with the early development of crystals. Large numbers of idioblastic calcium oxalate crystal cells are found in the leaves of Vitis mustangensis, V. labrusca and V. vulpina. A crystal idioblast, or raphide cell, will produce 150-300 needle-like calcium oxalate crystals within a central vacuole. Each raphide crystal is autonomous, having been produced in a separate membrane-defined crystal chamber; the idioblast''s crystal complement is collectively embedded in a water soluble glycoprotein matrix which fills the vacuole. The crystals are twins, each having a pointed and a bidentate end (Fig 1); when mature they are about 0.5-1.2 μn in diameter and 30-70 μm in length. Crystal bundles, i.e., crystals and their matrix, can be isolated from leaves using 100% ETOH. If the bundles are treated with H2O the matrix surrounding the crystals rapidly disperses.


Author(s):  
J. W. Mellowes ◽  
C. M. Chun ◽  
I. A. Aksay

Mullite (3Al2O32SiO2) can be fabricated by transient viscous sintering using composite particles which consist of inner cores of a-alumina and outer coatings of amorphous silica. Powder compacts prepared with these particles are sintered to almost full density at relatively low temperatures (~1300°C) and converted to dense, fine-grained mullite at higher temperatures (>1500°C) by reaction between the alumina core and the silica coating. In order to achieve complete mullitization, optimal conditions for coating alumina particles with amorphous silica must be achieved. Formation of amorphous silica can occur in solution (homogeneous nucleation) or on the surface of alumina (heterogeneous nucleation) depending on the degree of supersaturation of the solvent in which the particles are immersed. Successful coating of silica on alumina occurs when heterogeneous nucleation is promoted and homogeneous nucleation is suppressed. Therefore, one key to successful coating is an understanding of the factors such as pH and concentration that control silica nucleation in aqueous solutions. In the current work, we use TEM to determine the optimal conditions of this processing.


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