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a Department of Soil and Water, Connecticut Agricultural Experiment Station, 123 Huntington Street, P.O. Box 1106, New Haven, CT 06504-1106
b Department of Civil and Environmental Engineering, Vanderbilt University, 400 24th Avenue South, VU Station B 351831, Nashville, TN 37235
c Department of Environmental Sciences, Cook College, Rutgers University, New Brunswick, NJ 08901-8551
d State Key Laboratory of Organic Geochemistry, Guangzhou Institute of Geochemistry, Chinese Academy of Sciences, Guangzhou 510640, The People's Republic of China
e Department of Plant, Soil and Insect Sciences, University of Massachusetts, Amherst, MA 01003
* Corresponding author (joseph.pignatello{at}po.state.ct.us)
Received for publication September 20, 2005.
| ABSTRACT |
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Abbreviations: BC, black carbon DCB, dichlorobenzene HA, humic acid HOC, hydrophobic organic contaminant NAPH, naphthalene OC, organic carbon PHEN, phenanthrene SOM, soil and sediment organic matter TCB, trichlorobenzene TMDSC, temperature-modulated differential scanning calorimetry XYL, xylene
| INTRODUCTION |
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An early concept for HOC sorption to SOM that has achieved widespread acceptance attributes sorption to homogeneous dissolution (partition) into a gel-like SOM phase, similar to dissolution in an organic liquid (Chiou, 2002). In apparent agreement with data published at the time, this partition model predicted that sorption of nonpolar and weakly polar ("apolar") compounds would generate a linear isotherm and be noncompetitive when more than one sorbing chemical is present. Many studies have since demonstrated, however, that sorption of apolar HOCs to SOM in bulk soils or soil derivatives is nonideal, i.e., it displays nonlinear and competitive behavior. A rubberyglassy polymer model was proposed to explain the dual-sorbent nature of SOM, labeled "dual-mode" or "dual reactive domain" models (e.g., Pignatello and Xing, 1996; Chefetz et al., 2000; Huang et al., 1997). In these models, it was postulated that there are two SOM domains: one made up of loosely knit (flexible) macromolecules, where sorption is akin to "solid-phase dissolution" and is linear and noncompetitive, and the other made up of tightly knit (rigid) macromolecules, where sorption occurs by both dissolution and "adsorption" or "hole-filling" mechanisms with nonlinear and competitive behavior. Dual-mode sorption behavior is characteristic of glassy organic polymers (Xing and Pignatello, 1997; LeBoeuf and Weber, 2000a, 2000b, and references therein). Humic substances from several sources exhibit glass transition temperatures (discussed below) and dual domain flexibilities (Mao et al., 2002; Gunasekara et al., 2003). In addition, hysteresis and other irreversible phenomena may result from changing flexibility of the glassy humic matrix as a function of sorbate concentration (Lu and Pignatello, 2004b; Sander and Pignatello, 2005; Sander et al., 2006).
Around the same time that the dual models were being developed, findings began to appear of the potential importance of soot and charcoal particles (environmental BC) in sorption of contaminants to soils and sediments (Maruya et al., 1996; Gustafsson and Gschwend, 1997). It was suggested that, since BC materials have high surface areas and microporosities whichlike activated carbonsprovide adsorption sites, their presence could give rise to nonlinear and competitive behavior so often found in bulk soils (Chiou and Kile, 1998; Xia and Ball, 2000). Investigators have recently attempted to model sorption isotherms of polycyclic aromatic hydrocarbons (PAHs) and other large molecules in terms of two- or three-term equations. In these models, all of the observed nonlinearity is ascribed to the BC (Accardi-Dey and Gschwend, 2003; Lohmann et al., 2005), or BC and coal C (Cornelissen and Gustafsson, 2005) terms, and the term representing "ordinary" SOM is assumed linear. Ordinary SOM is usually taken to be "amorphous" humic and biological remnant substances. While these models can be made to work, the assumption on which they restthat of attributing all nonlinearity to BCis questionable.
The purpose of the this study was to document nonlinear and competitive sorption in macromolecular natural organic substances including humic acids and a wood lignin free of BC. We also present thermal analytical data consistent with the glassy character of these materials. Lignin is included because biopolymers derived from lignin are believed to be the main precursors of terrestrial and estuarine humic substances, as the lignin signature is abundantly clear in their structures.
| STRUCTURAL PROPERTIES OF SOIL ORGANIC MATTER |
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Lignin is an aromatic, high molecular weight, macromolecular solid second to cellulose in abundance among plant-derived "polymers" (Glasser and Kelley, 1987). Although the structure depends on whether the lignin is from nonwoody plants, softwoods, or hardwoods (Brunow, 2001), all lignins derive from the phenylpropane unit, which may be substituted with different functional groups.
Humic substances, which include humin, humic acid, and fulvic acid, are usually the most abundant components of SOM. Humic acids weigh hundreds to thousands of daltons, are rich in carboxyl and phenolic groups, and have O/C ratios of 1 or greater (Hedges, 1988). Structural models vary considerably, but in general feature a CC skeleton with COOH, ketone, and aliphatic and aromatic OH functional groups (Schulten and Schnitzer, 1997). Two-dimensional 1H nuclear Overhauser effect spectroscopy reveals pH-dependent conformational changes consistent with a chainlike primary structure for humic aliphatic structures, with humic aromatic regions exhibiting greater rigidity than aliphatic regions (Chien and Bleam, 1998). Recently, Mao et al. (2002) observed shifts in SOM domain mobility among a number of humic acid samples using solid-state NMR (nuclear magnetic resonance).
Kerogen is the dominant fraction of sedimentary organic matter that is insoluble in nonpolar or weakly polar organic solvents and is resistant to oxidizing acids. Coals, comprised primarily by Type III kerogen, are rich in condensed, crosslinked (usually by carboxyl and carbonyl groups) aromatic structures and, in more diagenetically advanced coals, show evidence of microcrystalline regions (Oberlin et al., 1980). A variable-temperature 1H NMR study of pyridine in Blind Canyon coal suggests a rigid macromolecular structure stabilized by interchain and intrachain crosslinks (Xiong and Maciel, 2002). Compared with humic acids, coal macromolecules generally have much higher molecular weights, often exceeding several hundred thousand daltons.
Glass-to-Rubber Transitions
Increasing temperature increases the motions of individual macromolecular chains, leading to expansion of free volume. If sufficient thermal energy is provided, individual chains may possess enough kinetic energy to break noncovalent interchain bonds, providing sufficient free volume to transcend from a more rigid, glass-like state to a more fluid, rubber-like state (McKenna, 1989). The transformation from glassy to rubbery states is complete at the glass transition temperature, Tg. While the Tg is often reported as a distinct temperature, in reality the heterogeneity of a macromolecule (e.g., molecular weight distribution, chemical composition) often provides a broadening of the glass transition over tens of degreesthe more heterogeneous the matrix, the larger the expected broadening (McKenna, 1989).
Evidence for glass transition behavior in a variety of SOMs is provided in the literature. The Tg of lignins varies from 66 to 190°C (Kadla et al., 2003), depending on their origin and isolation procedure. Glass transition behavior has been observed for a number of humic acids of terrestrial and aquatic origin, including two used in this study, AldHA (Aldrich humic acid; LeBoeuf and Weber, 1997) and PHA (peat humic acid; Young and LeBoeuf, 2000). Other humic materials exhibiting thermal transition behavior include Leonardite humic acid (LeBoeuf and Weber, 2001), Nordic aquatic humic acid (DeLapp and LeBoeuf, 2004), Georgetown aquatic humic acid, and Harpeth soil humic acid (DeLapp et al., 2005). Additional work by Schaumann and Antelmann (2000), DeLapp and LeBoeuf (2004), and Schaumann and LeBoeuf (2005) provide evidence that this behavior may also be prevalent in whole soils.
Glass transition behavior has been reported for numerous coals at temperatures ranging from 99 to 125°C (MacKinnon and Hall, 1995) for the lower temperature transitions, and to 307 to 359°C for higher temperature transitions (Lucht et al., 1987). Lucht et al. (1987) correlated the glass transition temperature with increasing degree of diagenetic alteration, or rank of the coal, observing that increased aromaticity of the coal corresponded with increased Tg values.
| MATERIALS AND METHODS |
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Properties of sorbents are given in Table 1. Organic C was determined in all cases by CO2 quantification on combustion of the sample. Humic acids were prepared following the standard procedures of the International Humic Substances Society (IHSS; Swift, 1996). Chelsea humic acid (CSHA) was extracted from a topsoil (Oxyaquic Hapludalf) collected from Chelsea, MI, following Swift (1996). Humic acids extracted from Florida peat soil (Lithic Medisaprist) (FlaHA), Amherst peat soil (Terric Haplosaprist; APHA), a mineral soil (Oxyaquic Dystrudept; MinHA), and a compost material (CompHA) were described earlier (Gunasekara et al., 2003; Wang and Xing, 2005; Yuan and Xing, 2001). A humic acid (H-HA) prepared from a different batch of Amherst peat soil is described in Lu and Pignatello (2004a); the alkaline soil extract was treated with a cation exchange resin to remove metal ions, precipitated, and de-ashed with HClHF solution. The final product H-HA contained a small amount of base-insoluble residue (see below).
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Two Al3+-exchanged humic acids were prepared. The MinHA(Al) was prepared by saturating solid particles of MinHA with 0.1 M AlCl3 solution (Yuan and Xing, 2001). The Al-HA was obtained by flocculating redissolved H-HA with Al3+ at pH 6 as described previously (Lu and Pignatello, 2004a); the batch prepared for this study had a slightly different elemental composition.
Acid Dichromate Treatment
The acid dichromate wet chemical oxidation method (Song et al., 2002) was used to detect the possible presence of BC by selectively oxidizing humic substances. In preparation, the samples were ground, demineralized at 60°C with a mixture of HCl (6 M) and HF (22 M) for 20 h, and finally rinsed three times with 6 M HCl followed by Milli-Q water (Millipore Corp., Billerica, MA). The OS-lig was presumed to be mineral free and was not demineralized. Additionally, for H-HA, a subsample was dissolved in a minimal amount of NaOH and centrifuged at 8000g; acid dichromate treatment was performed on the centrifugate, which, after rinsing with water and drying, corresponded to 0.05 kg/kg of H-HA, and the results were related back to the amount of the original H-HA.
Standard procedure involved suspending a 50- to 75-mg sample in 40 mL of a solution of 0.1 M K2Cr2O7 in 2 M H2SO4 at 55 ± 1°C for 60 h. After oxidation, the residual solid, if any, was collected by centrifugation, dried, weighed, and analyzed for total OC content by CO2 evolution on combustion. The acid dichromate treatment residual C content of each sorbent was then calculated from this weight and the total OC content of the original solid.
For comparison, a number of reference materials were also treated. These included a prepared wood char, paraffin flakes (Aldrich no. 411671), polyethylene microspheres (Aldrich, medium density, <149-µm diam.), n-hexadecanoic acid (palmitic acid, Sigma, 99%), n-octanoic acid (Acros, 99.5%), and decanedioc acid (sebacic acid, Aldrich, 99%). The char was prepared by muffling maple wood shavings at 400°C for 2 h in a watch-glass-covered crucible; it is characterized by Braida et al. (2003). Decomposition was monitored on replicate samples by the methods below, which were validated on controls without dichromate. Decomposition of paraffin wax and polyethylene was monitored by removing acid dichromate solution, rinsing the residual solid with water, and determining the weight of the solid after drying at 55°C. For decanedioic acid, the solution was refrigerated overnight to induce precipitation and the solid was collected and then dried in an ice bath with a stream of N2. The result was corrected for recovery (90 ± 2%) determined with controls. Decomposition of hexadecanoic and octanoic acids was monitored by extracting the solution with hexanes, passing the organic phase through a bed of Na2SO4 to remove water, evaporating the organic phase to dryness in a stream of N2, and weighing. Decomposition of char was monitored by its loss of C (Galbraith Laboratories, Knoxville, TN).
Thermal Analysis
Thermal analysis included the use of differential scanning calorimetry (DSC) and TMDSC (temperature-modulated DSC). Before analysis, each sample was heated to remove physisorbed water. Samples were subjected to multiple heatingcooling cycles to ensure repeatability of individual scans. Detailed instrumentation descriptions and experimental protocols are given in DeLapp and LeBoeuf (2004).
Sorption Methodologies
Customary shake-flask batch techniques were employed as described previously: AldHA, PHA, and OS-lig in LeBoeuf and Weber (2000b); H-HA and Al-HA in Lu and Pignatello (2004a, 2004b); MinHA, MinHA(Al), CompHA, and OS-lig in Xing and Pignatello (1997); and CSHA in Weber and Huang (1996). These techniques varied slightly among laboratories and can be summarized as follows. The solid was suspended in pH-adjusted aqueous solution containing appropriate electrolyte and bio-inhibitor (100200 mg/L NaN3 or HgCl2). The solid/liquid ratio was selected in each case to achieve 30 to 70% of uptake of the added solute. The solute was added either dissolved in water or methanol (<0.5% of solution volume). The vessel (which was filled to capacity) was then sealed and agitated gently for a time appropriate to reach apparent equilibrium (usually 714 d), as determined in preliminary experiments. Slight departure from complete equilibrium would have negligible effect on the degree of nonlinearity (Weber and Huang, 1996) and, we reasonably assume, of competitiveness. The liquid and solid phases were then separated (usually by centrifugation) and an aliquot of the liquid was withdrawn for analysis by gas chromatography, liquid chromatography, or liquid scintillation counting, as appropriate.
Sorption Model
Sorption equilibrium was modeled by the Freundlich equation:
![]() | [1] |
![]() | [2] |
For data reduction, we employed the linear regression of Eq. [2], rather than the nonlinear regression of Eq. [1]. The advantages of using Eq. [2] for modeling sorption data across a wide range in concentration have been discussed elsewhere (Huang et al., 1997). The underlying assumption of the linear regression is that Ce and qe are independently measured. When qe is not measured independently, this can be adequately satisfied if the mass left in solution at equilibrium is between 30 and 70% of the mass added, a condition for which a small variation of Ce has little effect on qe.
The concentration-dependent OC-normalized distribution coefficient KOC is calculated from the fractional OC content, fOC (kg/kg), and the Freundlich parameters by:
![]() | [3] |
| RESULTS AND DISCUSSION |
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Table 2 confirms previous reports (Masiello et al., 2002; Wolbach and Anders, 1989) that char is fairly stable to acid dichromate; only
17% of C of a prepared wood char (Braida et al., 2003) was oxidized during the standard 60-h treatment period, increasing to about 63% after an extended period of 23 d. Table 1 shows that OS-lig, APHA, and CSHA contained no C that survived the standard 60-h treatment, and that two additional humic acids, FlaHA and PHA, left only a trace of flocculant residual material after this time. These sorbents were, thus, essentially free of BC. Table 1 indicates that two other humic acids, MinHA and H-HA, left 4.7% and 1.0 to 3.3% unoxidized C, respectively, after standard treatment.
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1.3 x 106 L/kg OC) at the same concentration (Zhu and Pignatello, 2005). Acid dichromate treatment of the base-insoluble fraction of H-HA oxidized away about half the C within 60 h and the rest remained stable to the reagent during the next 100 h. The final residue had a C content of 17%, yet was pale gray in color, inconsistent with the color expected of a material having a char content of
25%. Rather, we believe that the residual C of H-HA (and possibly MinHA, as well) is made up of aliphatic hydrocarbon material present in the original sample. This is supported by the data in Table 2, which show that oxidation of aliphatic chainseither unfunctionalized (paraffin wax, polyethylene microspheres), monofunctionalized (n-octanoic acid, n-hexadecanoic acid), or difunctionalized (decanedioic acid)is extremely slow in acid dichromate. This is true even when the compound is melted (as was octanoic acid) or soluble (as was decanedioic acid) in the hot acid dichromate mixture. This should be taken as a cautionary note when applying the acid dichromate method to natural solids, since polymethylene chains originating from cutins, cutans, suberans, and related substances are common components of humic substances (Kang and Xing, 2005; Almendros et al., 1996). No attempt was made to remove aliphatic components from the original HA samples.
Figure 1 provides TMDSC scans for MinHA and CSHA that indicate thermal transitions. The MinHA exhibits transitions near 45 and 69°C that consolidate to a single transition near 52°C during a subsequent heating cycle. The CSHA exhibits a low-temperature transition between 3 and 6°C and a second transition between 63 and 67°C. Presence of multiple transition temperatures is not uncommon in macromolecules, and can be explained in terms of either (i) the presence of ß- and
-transitions, where the lower temperature ß-transitions are associated with side-chain mobility and the higher temperature
-transitions are attributed to mobilization of the main chain associated with the Tg; or (ii) the presence of regions having different chemical and physical properties, thus manifesting different mobilities and glass transition temperatures, as observed in inhomogeneous solids such as block copolymers. Also note that these transition behaviors apply to the dry solid. Water-wet glass transition behavior for AldHA was observed near 43°C (LeBoeuf and Weber, 1997). Transitions for PHA were observed at 62°C (Young and LeBoeuf, 2000). The TMDSC transitions were observed for H-HA at 56 or 61°C (duplicate measurements) and for Al-HA at 59 or 62°C (duplicates). The OS-lig exhibits glass transition behavior near 70°C (LeBoeuf and Weber, 2001), although a temperature near 115°C was reported by Glasser et al. (1998).
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Sorption affinity as log KOC calculated at Ce = 1 mg/L (Table 3) correlates with the hydrophobic character of the solute, expressed either as octanolwater partition coefficient, log KOW, (log KOC = 1.09 log KOW 0.89 [r2 = 0.904]) or inverse water solubility, log Sw (log KOC = 0.872 log SW 0.89 [r2 = 0.929]). This is generally consistent with many prior studies of HOC sorption to natural solids (e.g., Chiou, 2002); however, this correlation by itself says little about the mechanism, since KOCKOW or KOCSW linear free energy relationships can be expected for both absorption and adsorption processes that are driven predominantly by weak nonspecific interactions and water-exclusion effects. The effect of solute structure on the degree of linearity is unclear from the data presented in Table 3. While the isotherms of PHENthe largest and most hydrophobic compound among the HOCs testedappear to be the most nonlinear, the trend of increasing nonlinearity with molecular size (or KOW) is not evident when sorption of a series of HOCs to the same solid is compared: on CSHA, n = 0.845 for PHEN, 0.930 for NAPH, 0.986 for 1,3,5-TCB, and 0.867 for o-XYL. Evidently, the relationship between molecular size and n is complex.
The large variations in n and KOC for the same HOC indicate that HAs in different soils have different sorption properties, and thus they should not be regarded as a simple gel-like phase. It is known that the heterogeneous properties of HA are functions of source material, biogeochemical alteration history, and pedologic and geographic conditions. Furthermore, sorption capacities and nonlinearity are affected by the contents of aliphatic-C, aromatic-C, and O functional groups, the O/C atomic ratio, the size distribution of the macromolecules, glass transition temperature, and adsorbed minerals. For example, isotherm nonlinearity was reported to increase with aromaticity of several HAs extracted from different depths of a soil (Xing, 2001). Also, adsorption of HA by minerals can cause nonlinear and competitive sorption, particularly at low HA loadings (Murphy et al., 1994; Wang and Xing, 2005).
Influence on Sorption of Experimental Conditions that Alter Sorbent Properties
Temperature
Temperature affects sorption behavior as a result of increasing macromolecular mobility, even below the Tg. Thus, sorption typically becomes more linear with temperature approaching the Tg as the solid becomes more rubbery, and as solid-phase dissolution increases in importance compared with hole filling. Evidence for this trend has been reported for synthetic organic polymers (Vrentas and Vrentas, 1996; LeBoeuf and Weber, 2000a, and unpublished data, 2006), as well as SOM samples with known Tgs (LeBoeuf and Weber, 1997, 2000a). A trend of increasing linearity with temperature for 1,3-DCB and metolachlor sorption in the high-organic-matter (
93%) Pahokee soil was reported previously (Xing and Pignatello, 1997). On the other hand, sorption nonlinearity with respect to Illinois no. 6 and Wyoming coals was little influenced by temperature between 5 and 45°C due to the high Tg of the coals (LeBoeuf and Weber, unpublished data, 2006).
The thermal analysis summarized above indicate that, at and below room temperature, the HA and OS-lig sorbents probably exist in a glassy state, but they progress toward more a gel-like state with increasing temperature. Consistent with this, Fig. 5 shows a trend of increasing n with temperature for PHEN in CSHA, AldHA, PHA, and OS-lig and for NAPH in OS-lig. The results for the Pahokee soil (Xing and Pignatello, 1997) are also plotted for comparison. At temperatures well below the Tg, OS-lig gives clearly nonlinear behavior (n = 0.678 at 5°C for PHEN and 0.931 at 23°C for NAPH). For PHEN in OS-lig, the data support no significant change in sorption capacity and nonlinearity of the isotherm between 5 and 45°C; however, for NAPH in OS-lig, at temperatures closer to the Tg of 70°C, there is a trend toward increased linearity (n = 0.987 at 60°C and 0.991 at 85°C), suggesting increasing mobility of the lignin matrix near the Tg. Sorption of PHEN by CSHA and PHEN by PHA clearly show increasing linearity with temperature. For PHEN in AldHA, there is an increase in sorption linearity between 5 and 25, and 5 and 45°C, but a decrease between 25 and 45°C. Since the water-wet glass transition of AldHA was observed near 43°C, one would expect sorption of PHEN to be linear at 45°C, yet the value of n is 0.918 at that temperature. We suggest that additional, localized regions within the heterogeneous AldHA matrix that have yet to be fully mobilized may continue to influence sorption behavior (i.e., the glass transition may not be fully complete at 43°C).
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Organic Cosolvent Addition
Similar to energy input in the form of heat to a macromolecular solid, energy input in the form of sorbate chemical potential may induce matrix expansion, promote macromolecular flexibility, and reduce the energy required for glass-to-rubber conversion (McKenna, 1989). Consistent with this is the reduction in the Tg of AldHA from 70 to 43°C due to the swelling of the matrix by water (LeBoeuf and Weber, 1997). Plasticization was also observed for a peat soil at high water content (Schaumann and LeBoeuf, 2005). (Below 12% water, however, antiplasticization is observed due to H-bond cross-linking between water molecules and soil that is disrupted at higher water content.)
Sorption of NAPH to OS-lig from solutions containing methanol cosolvent represents another instance of the effects of solvent permeation (Table 2). The linearity of the NAPH isotherm at 23°C is clearly influenced by the volumetric fraction of cosolvent, changing from n = 0.931, to 0.959, to 1.000 at methanol contents of 0, 5, and 20% , respectively. The KOC of NAPH is simultaneously reduced. This suggests that methanol progressively lowers the Tg to a temperature near or below the temperature of the experiment. Similar results were reported in earlier work for sorption of HOCs by soils (Xing and Pignatello, 1997; Bouchard, 2002) and by a soil humin (Gunasekara and Xing, 2003).
Polyvalent Metal Ion Cross Linking
Isotherms were constructed in humic acids exchanged with Al3+ ion. Aluminum ions are known to be effective for coagulating humic substances. Coagulation occurs by bridging functional groups (particularly, carboxyl) located on the same or different macromolecules. The resulting cross-linked structure is expected to be less flexible at the strand scale, and therefore to generate isotherms with lower n values. The MinHA(Al) was prepared by saturating MinHA particles with AlCl3 solution (pH
3.5). The Al-HA was prepared by flocculating H-HA with Al3+ ion (Lu and Pignatello, 2004a), yielding a material in which Al ions preferentially coordinate to organic functional groups rather than incorporate in Al oxide polymers (Masion et al., 2000). Isotherms in both MinHA(Al) and Al-HA are more nonlinear than in the corresponding Ca2+- or H+-saturated form, respectively (Table 3). The link between glassiness of HA promoted by metal-ion cross-linking and enhanced nonlinearity is important because it supports the polymeric nature of HA and points away from BC as the source of nonlinearity in the original HA. By saturating HA with Al3+ ions, isotherm hysteresis is also increased (Yuan and Xing, 2001; Lu and Pignatello, 2004b), consistent with the more condensed form of Al-HA. True hysteresis is associated with matrix expansion in glassy, but not rubbery, solids (Sander and Pignatello, 2005; Sander et al., 2006). From the preceding discussion, it is evident that SOM properties (glassy character) can be altered and isotherm nonlinearity changes accordingly.
Cosolute Addition
If the solid contains a limited number of discreet sorption sites, then the addition of a cosolute can lead to a competitive effect in which there is mutual suppression of sorption. In fact, concave-down nonlinearity (n < 1) in the isotherm of a single solute can be regarded as a manifestation of self competition for sorption sites that increases in intensity with loading. Competitive sorption is expected, and observed, for sorption by glassy organic solids due to the presence of microporous holes in the solid phase (Xing and Pignatello, 1997). Competitive sorption has been observed in many soils (e.g., Lu and Pignatello, 2004a; Xing and Pignatello, 1997). Competition is not observed in partitioning behavior involving dissolution, such as partitioning between two liquids or between a fluid and a rubbery polymer (Xing et al., 1996; Sander et al., 2006).
Figure 6 shows the single-solute isotherms of TCB in H-HA and in Al-HA at pH 3 and pH 6, respectively. At specific points along the isotherm, we performed competitive sorption experiments by adding increasing amounts of the competing cosolute, 1,3-DCB, while keeping the mass of TCB constant. Increasing the concentration of 1,3-DCB resulted in decreasing sorption of TCB in both solids. Concurrently, the solution-phase concentration of TCB increased progressively with 1,3-DCB concentration, leading to the diagonal shift of the isotherm point illustrated in Fig. 6. Competitive sorption in H-HA and Al-HA by these nonspecifically interacting compounds is evidence that these two HA materials are not completely in a rubbery state.
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| CONCLUSIONS |
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| ACKNOWLEDGMENTS |
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