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Print version ISSN 0104-6632
On-line version ISSN 1678-4383
Braz. J. Chem. Eng. vol.23 no.2 São Paulo Apr./June 2006
D. L. SilvaI, *; G. BrunnerII
IUniversidade Federal do Pará. Depto. de Engenharia Química e de Alimentos, Phone: +(55) (91) 3201-7297, Fax: +(55) (91) 3201-7293, Rua Augusto Corrêa 01, CEP 66075-900, Belém - PA, Brazil. E-mail: email@example.com
IITechnische Universitaet Hamburg-Harburg, Thermische Verfahrenstechnik Eissendorfer Strasse 38, 21073, Hamburg Germany
Adsorption and regeneration of ion exchange resins were studied using a subcritical solution of a CO2-H2O mixture and a fixed bed column. The commercial Amberlite IRC-50/IRC-86 cation exchange resins and Amberlite IRA-67 anion exchange resin were tested for heavy metals (Pb, Cu, Cd) adsorption from a solution with different initial metal concentrations at different temperatures. After adsorption, the loaded resins were regenerated with water and carbon dioxide at different temperatures and a pressure of 25 MPa. The efficiency of the IRC-50 resin was lower than that of the IRC-86 resin for the adsorption of metals like Cd, Cu and Pb. Results obtained for desorption of these metals indicated that the process could be used for Cd and in principle for Cu. Sorption of metal ions depended strongly on feed concentration. Mathematical modeling of the metal desorption process was carried out successfully as an extraction process. For this purpose, the VTII Model, which is applied to extraction from solids using supercritical solvents, was used in this work.
Keywords: Adsorption and regeneration; Ion exchange; Carbon dioxide.
Ion exchange resins are usually regenerated with highly concentrated electrolyte solutions so disposal of concentrated saline solutions is necessary. In order to increase the concentration of salt in aquifers as little as possible, the amount of disposed salt has to be small. This can be achieved either by a suitable regeneration process or by the use of especial regeneration chemicals (Höll, 1981). One of the more promising possibilities is to use carbonic acid as a regeneration agent by dissolving supercritical CO2 in water at a high pressure. The applications of this technology in different areas have been reviewed in detail by a number of researchers (Jessop, 1999; Marr & Gamse, 2000). One of these applications is to regenerate adsorbents (Picht et al., 1982; Tan & Liou, 1988). A study of the regeneration of the sodium form of some carboxylic cation exchange resins using pressurized CO2 aqueous solutions was carried out and demonstrates that the regeneration efficiency of carbonic acid depends upon the acidity of the resin. When a saturated CO2 solution is used as the regeneration agent, a solution of NaHCO3 is obtained as a product of the regeneration reaction. This solution, when degassed, can be used as a regeneration agent for the weak base anion exchange resin in a deionization system, further minimizing the cost of the deionization in the DESAL process (Kunin & Vassiliou, 1963). The CARIX process represents an example of the treatment of drinking water with ion exchange resins where the saturat resins are regenerated simultaneously by CO2 and water (Höll & Flemming, 1991). In this work, subcritical water and carbon dioxide were applied as an alternative method to study the possibility of recovering heavy metals, particularly Pb2+, Cd2+ and Cu2+, from ion exchange resins. Desorption experiments were carried out in a supercritical extraction pilot plant at 25 MPa and temperatures of 22, 38 and 35 °C.
MATERIAL AND METHODS
The Amberlite IRA-67 anion exchange resin and the Amberlite IRC-86/IRC-50 cation exchange resins, supplied by Aldrich, were tested in this study. The column experiments were performed on ion exchange resin with a particle size of 16-50 mesh. Analytical grade reagents Pb(NO3)2 , CuSO4.5H2O and Cd(NO3)2 [Merck], were used. Solutions of approximately 10 to 300 mg/L were prepared using demineralized water as the solvent. In order to improve the adsorption process, the Amberlite IRA-67 anion exchange resin was converted to its bicarbonate form by activation with the CO2-H2O mixture at 25 MPA and 22, 28 or 35 °C. After activation, the Amberlite IRA-67 anion exchange resin in the HCO3- form was used in the same stainless steel (SS) column (Autoclave Engineers, Pennsylvania, USA) with a 17.2 mm inner diameter and a length of 486 mm. The Amberlite IRC-86 or IRC-50 cation exchange resin was packed in an other SS column with an inner diameter of 14 mm and a length of 490 mm (Fig. 1).
Columns were operated in the down-flow mode at room pressure in the adsorption experiments. Metal concentration was measured using an atomic absorption spectrophotometer (Perkin-Elmer Optima 2000 DV OES/ICP, Boston, USA). After the adsorption experiment, the direction of the flux (H2O-CO2) through the columns containing cation and anion resins was inverted in order to do the desorption experiment in the same apparatus. In the columns, the heavy metal was extracted from the adsorbent particles with the mixture of H2O-CO2 under a given state condition (P and T). The H2O-CO2 + heavy metal solution was separated by reduction in pressure, and samples were collected to analyze the Pb2+, Cu2+ and Cd2+ concentrations.
RESULTS AND DISCUSSION
Kinetic Study on Amberlite IRC-50 Resin
The selectivity of the resin can be analyzed using the breakthrough results. Figure 2 shows the adsorption breakthrough curve for Pb2+, Cd2+ and Cu2+ at 22 °C using the IRC-50 cation exchange resin. In these breakthrough curves the normalized concentration, defined as the measured concentration divided by the inlet concentration, is plotted against bed volume, where one bed volume is defined as the empty volume of the column that is occupied by the packed-bed ion exchange resin. The order of adsorption capacity for the three metal ions tested was Pb2+>Cu2+>Cd2+ , i.e., of the metals ions studied the efficiency of removal was highest for the lead ions. The spreading observed in actual breakthrough curves could be due to the existence of flow nonidealities (channeling), mixing (axial dispersion and dead spaces) and finite mass transfer and sorption rates, as observed in the work of Sridhar (1996).
The elution of Pb, Cd and Cu separately from the IRC-50 resin after the breakthrough experiment was studied at the same temperature as that used in the adsorption experiment. As shown in Fig. 2, the concentration of Cd in the eluate decreased more rapidly for the resin than the concentration of Cu. This can be attributed to the lower capacity of the resin to bind with the Cd2+ ions, as shown previously in the breakthrough curve. It can also be observed that the elution profile for the Pb ions has a broad peak with a long tail. These observations support previous results, indicating that Pb binds strongly to the ion exchange resin.
Kinetic and Equilibrium Study on Amberlite IRC-86 Resin
The Effect of Feed
Figure 3 displays the effect of solute concentration (Cd ) on the breakthrough curve. The change in inlet metal concentration markedly affects the shape and position of the breakthrough curve. The higher the metal concentration, the faster the breakthrough is. Lean feed is found to be better for metal recovery. However, the quantity of solutions to be supplied is large when the metal concentration is low and an optimum value has to be obtained. The results of the breakthrough behavior experiment for a metal concentration of 21.8 mg/L show that about 1400 bed volumes of feed solution could be passed through the resin with less than 0.2 mg/L of Cd ion in the effluent.
The elution of Cd ions from the sample after using the breakthrough curve experiment was then studied. The H2O-CO2 mixture was passed through the bed at 250 bar and 35 °C. Figure 3 also depicts the effect of metal concentration on the elution curve. The higher metal concentration in the adsorption experiment, the slower Cd elution is. The elution of Cd ions is slow and requires a large number of bed volumes when the metal concentration is high; however given that the lean feed is found to be better for metal recovery, as illustrated by the breakthrough curve, the elution process will be also better, for the lean metal concentration.
The Effect of Temperature
The effect of temperature on the metal adsorption-desorption process was also verified.
Figure 4 shows these effects for the adsorption of Pb2+ at 22 °C, with a Pb2+ feed concentration about 100 mg/L. It is evident from the breakthrough curve that temperature has little effect on the efficiency of the adsorption process, corresponding to an efficiency of Pb removal of over approximately 96% after 1200 bed volumes. At 250 bar, the greatest desorption was obtained at the lowest temperature. The efficiency of regeneration decreased with increasing temperature.
The effect of temperature on the adsorption of Cd, with a feed concentration of 300 mg/L is shown in Fig. 4. The highest temperature of 35°C results in slightly more efficiency. It is evident that the effluent Cd concentration is below 1mg/L during the first 50 min (approximately 125 bed volumes) of adsorption operation, corresponding to an efficiency of removal nearly 100 %. However, in the desorption process efficiency was inverted. Here again, at a temperature of 28°C the desorption process is more efficient due to the higher acidity (lower pH value) of the carbonic acid at lower temperatures.
A series of column experiments was conducted for three different metals (Pb, Cd and Cu) in the adsorption-desorption processes using the Amberlite IRC-86 cation exchange resin in a single-metal system, where the affinity of the resin for the metals was examined. Figure 5 shows the breakthrough curves for Pb2+, Cd2+ and Cu2+ in a feed solution containing only one of the metals at temperature of 22°C. The order of adsorption capacity for the metal ions tested was Pb2+>Cd2+>Cu2+ , i.e., the efficiency of removal of Pb ions had the highest value of those obtained for the three metal ions studied. Approximately 1500 bed volumes of feed solution can be passed through, while maintaining the Pb concentration in the effluent below 1 ppm.
The elution of metal ions from the resin after the breakthrough experiment was also studied. The regeneration of the resin supports the selectivity sequence discussed above. Comparing the curves, it can be observed that the sequence of metal desorption is inverted. The rapid elution of Cu from the resin was expected and attributed to the lower capacity of the resin to bind with the Cu ions. In the sequence of the desorption process, Cd is seen first and then Pb.
Modeling of Heavy Metal Desorption - VTII Model
Metal desorption was modeled successfully as an extraction process. For this purpose, the VTII Model (Brunner, 1994) that is applied to extraction from solids using supercritical solvents, was chosen for this work. The experimental and calculated desorption curves are compared in Figures 6 and 7 for Amberlite IRC-86 cation exchange resin; the coincidence is sufficient.
Although the IRC-50 resin isn't as efficient as the IRC-86 resin in the adsorption of metals like Cd, Cu and Pb, the results obtained for desorption of these metals indicated that the process can be suitable for Cu and principally for Cd. Temperature does not have much effect on the efficiency of the adsorption process for the heavy metal, but exerts a strong effect on the efficiency of metal desorption, with the best results at the lowest temperature. The sorption of metal ions was strongly dependent on feed concentration and lean feed was found to be better for metal desorption from the resin. Metal desorption as an extraction process was successfully modeled. The fitting obtained for the experimental points with the kinetic VTII extraction model were shown to be appropriate for ion exchange.
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Received: October 20, 2004
Accepted: February 1, 2006
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