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Article

Development of Surface-Modified Polyacrylonitrile Fibers and Their Selective Sorption Behavior of Precious Metals

1
Department of Bioprocess Engineering, Chonbuk National University, Jeonju 561-756, Korea
2
School of Chemical Engineering, Chonbuk National University, Jeonju 561-756, Korea
*
Authors to whom correspondence should be addressed.
Appl. Sci. 2016, 6(12), 378; https://doi.org/10.3390/app6120378
Submission received: 6 November 2016 / Revised: 15 November 2016 / Accepted: 17 November 2016 / Published: 25 November 2016
(This article belongs to the Section Materials Science and Engineering)

Abstract

:
The purpose of this study was to design a powerful fibrous sorbent for recovering precious metals such as Pd(II) and Pt(IV), and moreover for identifying its selectivity toward Pd(II) or Pt(IV) from a binary metal solution. For the development of the sorbent, polyacrylonitrile (PAN) was selected as a model textile because its morphological property (i.e., thin fiber form) is suitable for fast adsorption processes, and a high amount of PAN has been discharged from industrial textile factories. The PAN fiber was prepared by spinning a PAN–dimethylsulfoxide mixture into distilled water, and then its surface was activated through amidoximation so that the fiber surface could possess binding sites for Pd(II) and Pt(IV). Afterwards, by Fourier-transform infrared (FT-IR) and scanning electron microscopy (SEM) analyses, it was confirmed that the amidoximation reaction successfully occurred. The surface-activated fiber, designated as PAN–oxime fiber, was used to adsorb and recover precious metals. In the experiment results, it was clearly observed that adsorption capacity of PAN–oxime fiber was significantly enhanced compared to the raw material form. Actually, the raw material does not have sorption capacity for the metals. In a comparison study with commercial sorbent (Amberjet™ 4200), it was found that adsorption capacity of PAN–oxime was rather lower than that of Amberjet™ 4200, however, in the aspects of sorption kinetics and metal selectivity, the new sorbent has much faster and better selectivity.

1. Introduction

Platinum group metals (such as Pd, Pt, Au, Ru, Ir, and Os) can be naturally found at very low quantities in the earth’s crust, and they are regarded as precious metals. In general, plenty of the precious metals have been used as catalytic elements by diverse industrial fields like automobile, petrochemical, and electronic components industries, although their availabilities are limited and they are expensive. After use, liquid or solid wastes, including a large amount of the precious metals, have been discharged from many industries. Such release of the metals without recovery is unprofitable for companies, and the released chemicals can play roles as toxicants in environments [1]. Therefore, recovery processes for precious metals from the industrial wastes should be an important practice.
If recovery processes for metals are methodologically established, the waste solution containing precious metals can be regarded as secondary sources. Indeed, many researchers reported that some precious metals could be recovered using various techniques such as solvent extraction [2,3], chemical precipitation [4,5], ion exchange system [6,7], and chelation [8]. However, there were several drawbacks to these techniques, such as poor selectivity, difficult stripping, low recovery efficiencies or high capital costs for establishing the processes, and disposal costs for chemical wastes used for recovery [9,10]. Therefore, the use of these techniques should be limited [11]. To overcome the drawbacks, adsorption-based recovery of precious metals from wastewater is a promising process, because the process is effective and economical for treating aqueous effluents, even at low concentrations of metal. However, the efficiency of the process is strongly dependent on the employed sorbent.
Among several sorbents’ types (e.g., bead, capsule, fiber, etc.), fibrous-type ones have been attractive because they have large surface areas, implying that plenty of functional groups can be potentially activated by chemical modifications. As a result, these characteristics can contribute to higher adsorption capacities and faster adsorption rates [12]. Until now, many types of fibrous agents—for example, activated carbon fiber [13], cotton fiber [14], glass fiber [15], and polymer fiber [16]—have been presented.
Currently, polyacrylonitrile (PAN), with a molecular formula of [C3H3N]n, as a raw material has been highlighted for designing a sorbent because it is abundant—a high amount (i.e., >64 million tons per year) has been discharged—and its stability in water is very advantages for the metal recovery process since metals or contaminants are mainly in aqueous phases. Other benefits of PAN fiber is its high strength, chemical resistivity, good mechanical properties, abrasion resistance, and electrostatic accumulation [17].
Because all fiber-form sorbents do not have good adsorption capacities, surface modification of fiber-formed sorbents are essential, as the case may be. In general, the technologies for functionalization of fiber can be divided into two categories: physical and chemical methods. The first case includes surface fibrillation and electric discharge, which can be used to change the structural and surface properties of the fiber and thus improve the mechanical bonding on the matrix. The latter can be conducted by hydrolysis, chemical coating, or activation [18].
In this study, we report the application of PAN fiber for a sorbent preparation for recovery of precious metals (i.e., Pd(II) or Pt(IV)) from aqueous phases. The PAN fiber has cyanide groups, but the groups are not effective binding sites for the negatively charged metal ions [19]. Therefore, the surface of PAN fiber was physically and chemically modified by firstly spinning PAN–dimethylsulfoxide mixture in distilled water and secondly amidoximation to generate the binding sites on the surface for anionic metals. The adsorption capacity of the prepared sorbent was tested using single and binary metal systems to check its metal selectivity. Moreover, the adsorption capacity and selectivity were compared with those of commercially available and predominantly used ion-exchange resin (Amberjet™ 4200).

2. Materials and Methods

2.1. Materials

Hydroxylamine hydrochloride (NH2OH·HCl), Amberjet™ 4200 ion-exchange resin, and polyacrylonitrile (PAN) with a molecular weight of 150,000 were all purchased from Sigma-Aldrich (Yongin, Korea). Sodium carbonate was obtained from Samchun Chemicals Co. (Seoul, Korea). Dimethylsulfoxide (DMSO) (99.5%) was supplied by Daejung Chemicals Co., Ltd. (Siheung, Korea). Palladium(II) chloride (PdCl2) and hydrogen hexachloroplatinate (IV) hydrate (H2PtCl6·5.5H2O) as adsorbates were purchased from Kojima Chemicals Co., Ltd. (Sayama, Japan).

2.2. Preparation of Polyacrylonitrile (PAN) Fiber

To prepare 10% (w/v) PAN solution, 10 g of PAN was dissolved in 100 mL of DMSO by stirring for 24 h at 40 ± 2 °C. The PAN solution was poured into a 50 mL barrel with a needle tip with 0.14 mm diameter and was spun into distilled water at 0.25 MPa. Then, the PAN fiber was formed by a phase transition process in aqueous phase. The collected fiber was washed several times with distilled water to remove residual DMSO. The final product was stored in distilled water.

2.3. Chemical Modification of PAN Fiber

To enhance the binding sites of the PAN fiber prepared in Section 2.2, it was chemically modified through the following processes. First, both 6 g of hydroxylamine hydrochloride and 4.5 g of sodium carbonate were mixed in 100 mL of distilled water at 70 ± 2 °C, and then, 3 g of wet PAN fiber was added to the mixture at 70 ± 2 °C for different durations (5–30 min). After the chemical reaction, the activated PAN (called PAN–oxime fiber) was washed several times with distilled water, and then freeze-dried for 24 h. The preparation methods are summarized in Scheme 1.

2.4. Characterization of PAN–Oxime Fiber

To identify if the functionalization of the fibers in Section 2.3 was successfully performed, their infrared spectrum was analyzed using a Fourier-transform infrared spectrometer (FT-IR; Spectrum GX, Perkin Elmer, Waltham, MA, USA). The FT-IR samples were prepared as KBr discs and examined within the range of 4000–400 cm−1. Also, scanning electron microscopy (SEM; JSM-5900, JEOL, Tokyo, Japan) was used to observe the surface of the prepared sorbent.

2.5. Batch Adsorption Experiments

In order to evaluate the effect of the amidoximation time on adsorption capacity of a sorbent, a single-point adsorption experiment was conducted on Pd(II). Here, a Pd(II) solution of 1000 mg/L was prepared by adding 0.1 M HCl solution; then, 0.03 g of the fibrous adsorbents was added to 30 mL of Pd(II) solution in a 50 mL polypropylene conical tube. The tubes were continuously shaken by an incubator at 160 rpm and 25 ± 2 °C and their samples were carefully taken.
Isotherm experiments for testing sorption capacity and metal selectivity of the prepared and commercial sorbents were conducted. Here, also 0.03 g of PAN–oxime fiber or Amberjet™ 4200 was added to 30 mL of metal solutions, which included Pd(II) and Pt(IV) single-metal systems or Pd(II)–Pt(IV) binary metal systems for 24 h at 25 ± 2 °C. The stock solutions of metals were prepared in 0.1 M HCl solution and diluted if necessary. In these experiments, the initial concentrations were changed from 0 to approximately 1200 mg/L.
The sorption kinetics of the adsorbents was performed to check equilibrium time. In this case, 0.1 g of the adsorbent was floated in 100 mL of 500 mg/L metal solution at 160 rpm and 25 ± 2 °C. The kinetic samples were collected at fixed time intervals. All taken samples from supernatant of batches were analyzed using an inductively coupled plasma spectrometer (ICP; ICP-7510, Shimadzu, Kyoto, Japan).
For isotherm and kinetic experiments, five replicates of independent separate sorption experiments were conducted and the standard errors were within 5%.

3. Results and Discussion

3.1. The Effect on Amidoximation on the Preparation of PAN–Oxime Fiber

The amine of amidoxime groups generated on the prepared sorbent (i.e., PAN–oxime fiber) by the chemical reaction can act as the binding sites for anionic metals via electrostatic interaction. Here, to check the effects of the reaction times, the morphological changes of the PAN fiber were examined at different reaction times, from 0 to 30 min. As shown in Figure 1, the PAN fiber became a rigid form as the reaction time increased. The PAN–oxime fibers prepared within reaction times of 20–25 min were easily broken, and when the reaction time was 30 min, the PAN–oxime fiber was agglomerated.
In order to identify if the amidoximation was successfully carried out, an FT-IR study of raw PAN and the prepared sorbents at different reaction times (i.e., 15 and 30 min) were performed. As shown in Figure 2, the FT-IR spectra of PAN and PAN–oxime fibers demonstrate several peaks of functional groups. The FT-IR spectrum of PAN fiber (Figure 2a) displays the most distinctive bonds of the nitrile groups (C≡N stretch; 2246 cm−1). After the chemical reaction of the matter, different spectral segments were observed (see Figure 2b,c). The FT-IR spectra of PAN–oxime fibers showed that the intensity of the nitrile peak (2246 cm−1) decreased as the reaction time increased, and instead the characteristic peaks of the functional groups appeared at around 1669, 1621, 1380, 923, and 3800–3000 cm−1. These peaks result from the C=N stretch, N–H bend, C–N stretch, N–H bond, and overlapping of the O–H and N–H stretch, respectively. Therefore, it was confirmed that the chemical reaction was appropriately performed to generate functional groups for anionic metals. However, the microscopic analysis did not show significant difference between PAN and PAN–oxime fiber, as shown in Figure 3. This indicates that the chemical modification was generated on the surface of the PAN fiber, while physical structure of the PAN fiber was not affected by the chemical reaction. Thus, the diameters of the adsorbents produced at different reaction times were similar (~100 µm). However, in the case of reaction for 30 min, the fiber could not maintain its shape, but aggregated likely due to the extensive extent of reaction.

3.2. Effect of Amidoximation Time on Adsorption Capacity

The effect of amidoximation time on the adsorption capacity of Pd(II) was studied. For that, the PAN–oxime fibers were prepared at different reaction times, from 0 to 30 min at 5 min intervals. Here, the PAN–oxime fiber reacted for 30 min was excluded because it was agglomerated and fiber no longer formed. After the adsorption experiments, the amount of adsorbed Pd(II) ions per unit mass of adsorbent (qt, mg/g) was calculated by a mass balance equation [20].
q t = ( V 0 C 0 V f C f ) / M
where V0 and Vf are the initial and final solution volumes (L), respectively, C0 and Cf are the initial and final solution concentrations of metal ions (mg/L), respectively, and M is the mass of adsorbent (g).
As shown in Figure 4, it was checked that the PAN–oxime fiber could be used for the recovery of precious metals, and the Pd(II) uptake increased as the reaction time increased. This means that the longer reaction time, the more binding sites that were generated. When the PAN–oxime fiber reacted for 25 min was used, the highest (412.6 mg/g) Pd(II) uptake was observed, while raw PAN fiber (reaction time = 0) has no metal adsorption, but shows a negative value due to water evaporation in this sample. However, for further studies (i.e., isotherm and kinetics), the PAN–oxime fiber reacted for 15 min was chosen because the fiber produced from 20 min reaction was too weak and brittle to be used.

3.3. Isotherms Study

The isotherm studies using the PAN–oxime fiber developed with a 15 min reaction time were conducted in single and binary metal systems of Pd(II) and Pt(IV). The adsorption capacities were compared with those of commercial ion-exchange resin (Amberjet™ 4200) which is predominantly used for metal adsorption. In order to evaluate the maximum adsorption capacity from the experimental data, the Langmuir isotherm model [21] was applied. The nonlinear Langmuir equation is shown below:
Langmuir model :   q e = q m b C e / ( 1 + b C e )
where qe is the uptake of metal at equilibrium (mg/g) and Ce is the concentration of the metal solution at equilibrium (mg/L). qm and b are related to the Langmuir constant, and they represent the adsorption capacity (mg/g) and affinity (L/mg), respectively.
As shown in Figure 5a, adsorption capacities for Pd(II) and Pt(IV) of both PAN–oxime fiber and Amberjet™ 4200 increase in the single-metal systems as the equilibrium concentrations of respective metals increase. The estimated parameters are given in Table 1. In single-metal systems, the maximum uptakes of Pd(II) and Pt(IV) by PAN–oxime fiber were estimated to be 244.06 ± 10.68 and 175.65 ± 6.62 mg/g, respectively. Those of Pd(II) and Pt(IV) by Amberjet™ 4200 were estimated to be 310.05 ± 13.25 and 422.65 ± 21.33 mg/g, respectively. In general, the sorption capacities of Amberjet™ 4200 for Pd(II) and Pt(IV) were higher than those of the PAN–oxime fiber.
In the binary metal system, the adsorption behaviors of the PAN–oxime fiber were quite interesting compared to those of Amberjet™ 4200. In case of Amberjet™ 4200, its metal uptakes in the binary metal mixture were lower than those in the single-metal systems, and it did not show any metal selectivity (Figure 5). However, in the same condition, Pd(II) uptakes of PAN–oxime fiber were similar in both cases of single (244.06 ± 10.68 mg/g) and binary metal systems (234.54 ± 11.53 mg/g). Note that the maximum Pd(II) uptake of PAN–oxime in the binary metal system may be higher than the calculated value, since the isotherm of Pt(IV) could not be fitted by the Langmuir model. Surprisingly, Pt(IV) uptake of PAN–oxime fiber, in the case of the multi-metal system, was significantly lowered (Figure 5b) from 62.99 mg/g in a single-metal system to 39.62 mg/L in a binary metal system. This indicates that PAN–oxime fiber has selective binding ability for Pd(II) in a mixture of Pd(II) and Pt(IV). For better comparison, the selectivity coefficients ( α P d ( I I ) / P t ( I V ) ) of PAN–oxime and Amberjet™ 4200 for Pd(II) in the mixture of Pd(II) and Pt(IV) were calculated using Equation (3).
α P d ( I I ) / P t ( I V ) = q t , P d ( I I ) / C f , P d ( I I ) q t , P t ( I V ) / C f , P t ( I V )
where q t , P d ( I I ) and q t , P t ( I V ) are the uptakes of Pd(II) and Pt(IV), respectively, and C f , P d ( I I ) and C f , P t ( I V ) are the final concentrations of Pd(II) and Pt(IV), respectively. Based on Equation (3), the selectivity coefficients of PAN–oxime and Amberjet™ 4200 at the initial metal concentrations (200~1000 mg/L) could be calculated. As can be seen in Figure 5c, the selectivity coefficients toward Pd(II) of PAN–oxime ranged from 15 to 33, which was approximately 19~89 times higher than those of Amberjet™ 4200. The selectivity of PAN–oxime decreased when initial metal concentration increased.

3.4. Kinetic Study

Figure 6a,b shows the kinetics of the developed PAN–oxime fiber in single and binary metal systems, respectively, and Figure 6c shows the kinetic results of the Amberjet™ 4200 resin in the binary metal system. As a result, more than 90% of the adsorptions by PAN–oxime fiber were completed within 10 min, while Amberjet™ 4200 was done within 120 min of contact with the metal solution. This indicates that PAN–oxime fiber has much better sorption kinetics than Amberjet™ 4200, because the former supports plenty of binding sites as a thin fiber form. In order to evaluate the kinetic results, the data points were fitted by pseudo-first- and pseudo-second-order models, which can be represented by their nonlinear kinetic equations as follows [22]:
Pseudo-first-order model :   q t = q 1 ( 1 exp ( k 1 t ) )
Pseudo-second-order model :   q t = q 2 2 k 2 t / ( 1 + q 2 k 2 t )
where both q1 and q2 are the amount of adsorbed metal ions at equilibrium (mg/g), qt is the amount of adsorbed metal ions at any time t (mg/g), k1 is the rate constant in the pseudo-first-order model (min−1), and k2 is the rate constant in the pseudo-second-order model (g/mg·min). The experimental and predicted equilibrium uptakes, rate constants, and correlation coefficients are exhibited in Table 2.
As shown in Figure 6a, high amounts of Pd(IV) and Pt(II) were rapidly adsorbed onto the PAN–oxime fiber in single-metal conditions, whose final uptakes were 235.52 and 162.16 mg/g, respectively. In the binary metal systems, the final uptake of Pd(II) by the PAN–oxime fiber was 221.00 mg/g, but the Pt(IV) uptake could not be estimated by the pseudo-second-order because an unusual phenomenon of Pt(IV) adsorption by PAN–oxime fiber was observed (Figure 6b). If it was visually checked, it was around 20~25 mg/g after 30 min. Again, in the beginning, Pt(IV) was adsorbed together with Pd(II) onto PAN–oxime fiber. However, as the Pd(II) uptake increased, the uptake of Pt(IV) sharply declined, which shows that initially adsorbed Pt(IV) was desorbed in a few minutes. This implies that Pd(II) has stronger binding affinity with the sorbent than Pt(IV). Although the commercial resin Amberjet™ 4200 has higher sorption capacities for both metal ions than PAN–oxime fiber in the single-metal system, it does not have the selective binding property in the binary system. However, the developed PAN–oxime fiber shows selectivity toward Pd(II) in the binary system. In addition, PAN–oxime fiber can bind metal ions much more quickly than the resin.

4. Conclusions

Polyacrylonitrile (PAN) fiber has been abundantly discharged from industrial textile factories, thus its recycling studies are essential. In this study, we applied PAN for preparing an excellent adsorbent for a fast and selective recovery process for precious metals (i.e., Pd(II) and Pt(IV)). For sorbent preparation with appropriate functional groups for metal binding (PAN–oxime fiber), spinning a PAN–dimethylsulfoxide mixture in water, followed by amidoxime chemical modification, was carried out. For the surface modification, it was found that as amidoximation time increased, the conversion from PAN to PAN–oxime increased. However, reaction greater than 20 min led to destruction of the fibrous structure. Isotherm and kinetic experiments in the single-metal systems showed that the uptakes of Pd(II) and Pt(IV) by Amberjet™ 4200 were approximately 1.3 and 2.4 times higher than those by the PAN–oxime fiber, respectively. However, in the binary solution, PAN–oxime fiber showed high selectivity for Pd(II), and moreover it had a much faster equilibrium time than Amberjet™ 4200.
This study showed that the PAN textile can be used to prepare an excellent adsorbent. As an example, it was clearly shown that the developed PAN–oxime fiber shows great potential for recovering anionic metals. Moreover, since it has fast binding ability and selectivity, it can be applied in column systems and other separation processes.

Acknowledgments

This work was supported by the Korean Government through KETEP (20115020100060) and KEITI (The Eco-Innovation project 20115020100060 ) grants and the Korean Government through NRF grant (2014R1A1A2008337 and 2014R1A2A1A09007378).

Author Contributions

Areum Lim and Myung-Hee Song contributed to sorbent development, batch experiments, and FTIR & microscopic analyses under supervision of Chul-Woong Cho and Yeoung-Sang Yun.

Conflict of Interest

The authors declare no conflict of interest.

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Scheme 1. Reaction for the synthesis of polyacrylonitrile (PAN)–oxime fiber.
Scheme 1. Reaction for the synthesis of polyacrylonitrile (PAN)–oxime fiber.
Applsci 06 00378 sch001
Figure 1. Photographs of the polyacrylonitrile (PAN)–oxime fibers prepared at different reaction times. (a) 0 min; (b) 5 min; (c) 10 min; (d) 15 min; (e) 20 min; (f) 25 min; and (g) 30 min.
Figure 1. Photographs of the polyacrylonitrile (PAN)–oxime fibers prepared at different reaction times. (a) 0 min; (b) 5 min; (c) 10 min; (d) 15 min; (e) 20 min; (f) 25 min; and (g) 30 min.
Applsci 06 00378 g001
Figure 2. Fourier-transform infrared (FT-IR) spectra of PAN fiber and PAN–oxime fiber at different reaction times: (a) 0 min; (b) 15 min; and (c) 30 min.
Figure 2. Fourier-transform infrared (FT-IR) spectra of PAN fiber and PAN–oxime fiber at different reaction times: (a) 0 min; (b) 15 min; and (c) 30 min.
Applsci 06 00378 g002
Figure 3. Scanning electron microscopy (SEM) images of (a) PAN fiber ×200 magnification; (b) PAN fiber ×2000 magnification; (c) PAN–oxime fiber ×200 magnification; and (d) PAN–oxime fiber ×1000 magnification. The PAN-oxime fiber was prepared with a reaction time of 15 min.
Figure 3. Scanning electron microscopy (SEM) images of (a) PAN fiber ×200 magnification; (b) PAN fiber ×2000 magnification; (c) PAN–oxime fiber ×200 magnification; and (d) PAN–oxime fiber ×1000 magnification. The PAN-oxime fiber was prepared with a reaction time of 15 min.
Applsci 06 00378 g003
Figure 4. Effect of amidoximation time on the Pd(II) uptake by PAN–oxime fiber.
Figure 4. Effect of amidoximation time on the Pd(II) uptake by PAN–oxime fiber.
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Figure 5. Adsorption isotherms of PAN–oxime fiber and Amberjet™ 4200. (a) Single-metal system; (b) binary metal system; and (c) selectivity. Standard errors are less than 5%.
Figure 5. Adsorption isotherms of PAN–oxime fiber and Amberjet™ 4200. (a) Single-metal system; (b) binary metal system; and (c) selectivity. Standard errors are less than 5%.
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Figure 6. Adsorption kinetics of PAN–oxime fiber in single-metal system (a) and binary metal system (b); and of Amberjet™ 4200 in binary metal system (c). Standard errors are less than 5%.
Figure 6. Adsorption kinetics of PAN–oxime fiber in single-metal system (a) and binary metal system (b); and of Amberjet™ 4200 in binary metal system (c). Standard errors are less than 5%.
Applsci 06 00378 g006aApplsci 06 00378 g006b
Table 1. Langmuir parameters in single and binary metal systems.
Table 1. Langmuir parameters in single and binary metal systems.
AdsorbentsConditionsMetalsParameters
qm (mg/g)b (L/mg)R2
PAN–oxime fiberSinglePd(II)244.06 ± 10.680.435 ± 0.1380.928
Pt(IV)175.64 ± 6.620.052 ± 0.0120.960
BinaryPd(II)234.54 ± 11.530.589 ± 0.2140.905
Pt(IV)---
Amberjet™ 4200SinglePd(II)310.05 ± 13.250.107 ± 0.0260.964
Pt(IV)422.65 ± 21.330.239 ± 0.0530.955
BinaryPd(II)163.35 ± 6.090.340 ± 0.0930.955
Pt(IV)198.61 ± 6.640.473 ± 0.1160.966
“-” represents that the data cannot be estimated using the Langmuir model.
Table 2. Kinetic parameters of the pseudo-first-order and pseudo-second-order models.
Table 2. Kinetic parameters of the pseudo-first-order and pseudo-second-order models.
AdsorbentsConditionsMetalsPseudo-First-OrderPseudo-Second-Order
q1 (mg/g)k1 (min−1)R2q2 (mg/g)k2 × 10−3 (g/mg·min)R2
PAN–oxime fiberSinglePd(II)229.26 ± 1.220.644 ± 0.0280.994235.52 ± 1.865.5 ± 0.50.990
Pt(IV)158.04 ± 1.931.008 ± 0.1170.973162.16 ± 1.7211.5 ± 1.70.983
BinaryPd(II)214.09 ± 2.740.757 ± 0.0840.972221.00 ± 1.056.0 ± 0.30.997
Pt(IV)------
Amberjet™ 4200BinaryPd(II)126.84 ± 3.100.053 ± 0.0060.933139.48 ± 2.110.5 ± 0.040.984
Pt(IV)149.40 ± 3.220.041 ± 0.0040.959166.82 ± 2.190.3 ± 0.020.991
“-” represents that the data cannot be estimated using the pseudo-first- and pseudo-second-order models.

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Lim, A.; Song, M.-H.; Cho, C.-W.; Yun, Y.-S. Development of Surface-Modified Polyacrylonitrile Fibers and Their Selective Sorption Behavior of Precious Metals. Appl. Sci. 2016, 6, 378. https://doi.org/10.3390/app6120378

AMA Style

Lim A, Song M-H, Cho C-W, Yun Y-S. Development of Surface-Modified Polyacrylonitrile Fibers and Their Selective Sorption Behavior of Precious Metals. Applied Sciences. 2016; 6(12):378. https://doi.org/10.3390/app6120378

Chicago/Turabian Style

Lim, Areum, Myung-Hee Song, Chul-Woong Cho, and Yeoung-Sang Yun. 2016. "Development of Surface-Modified Polyacrylonitrile Fibers and Their Selective Sorption Behavior of Precious Metals" Applied Sciences 6, no. 12: 378. https://doi.org/10.3390/app6120378

APA Style

Lim, A., Song, M. -H., Cho, C. -W., & Yun, Y. -S. (2016). Development of Surface-Modified Polyacrylonitrile Fibers and Their Selective Sorption Behavior of Precious Metals. Applied Sciences, 6(12), 378. https://doi.org/10.3390/app6120378

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