Fibrous xonotlite was synthesized under the conditions of Na2SiO3 concentration of 0.05 mol·L−1, molar ratio of Si/Ca of 1:1, temperature of 220 °C and time of 9 h. It is worth pointing out that the Na2SiO3 solution as raw material was obtained from silicon residue through several procedures. The fibrous xonotlite exhibits excellent adsorption capacity for Congo red. 50 mL solution of Congo red with the concentrations of 100, 150 and 200 mg·L−1 can be almost completely adsorbed by 30 mg of fibrous xonotlite within 10 min, and the adsorption ratios are 94.05%, 95.50% and 94.14%. The Langmuir model describes the adsorption well, indicating the adsorption is monolayer. The adsorption kinetics follows the pseudo-second-order model. The calculated maximum adsorption capacity of fibrous xonotlite for Congo red is 574.71 mg·g−1 at room temperature. Fibrous xonotlite is a potential efficient adsorbent for Congo red owing to its rapid adsorption, high adsorption capacity and regeneration capacity.

  • It is a cleaner process of synthesizing fibrous xonotlite from waste silicon residue.

  • Waste for waste treatment is beneficial to environmental and resource sustainability.

  • Fibrous xonotlite exhibits excellent adsorption ability for Congo red.

  • Adsorption mechanism of xonotlite for Congo red was determined.

Graphical Abstract

Graphical Abstract
Graphical Abstract

The rapid development of industry has brought not only high economic benefits, but also environmental challenges. Waste aqueous effluent containing heavy metal ions (Chen & Wang 2006), phosphorus and fluorine (Kang et al. 2011) and organic dye (Ismail et al. 2019) causes serious environmental problems. The organic dye generated from the textiles and paper enterprises is considered extremely serious for their non-degradability and accumulation. Low concentration discharged may cause great pollution. Removing the organic dyes from industrial wastewater has become an urgent task (Feng et al. 2015). Many solutions have been developed, such as membrane separation (Yoon et al. 2014), ion co-precipitation (Liu et al. 2014), photocatalysis (Shen et al. 2020a, 2020b), adsorption (Xuan et al. 2014) and so on. Among them, adsorption is one of the promising and efficient methods owing to its simplicity and high efficiency (Wang et al. 2017).

The adsorbent plays an important role during the adsorption process. Up to now, micro-nano materials are promising adsorbents due to their unique physical and chemical properties and geometric structure (Shen et al. 2020a, 2020b). Generally, morphological structures of materials can significantly influence their performance, therefore, controllable synthesis of materials with special morphology has been given more attention. Many adsorbents with special shapes were reported, including rod-shaped (Yun et al. 2020), flower (Shen et al. 2020a, 2020b), hollow spherical (Qiao et al. 2012), fiber-shaped (Chen et al. 2018) etc. Meanwhile, some related synthesis methods, such as the sol-gel (Chen et al. 2019), hydrothermal (Wang et al. 2015), vapor deposition (Tofighy & Mohammadi 2011) and so on, also have been studied. The hydrothermal process is widely used in the preparation of micro-nano materials with the superiorities of simplicity, high yield, controllability and easy amplification. (Bao et al. 2016).

In recent years, silicate materials with special morphologies have attracted much attention in the field of wastewater treatment, and have been adopted to treat Pb2+ (Liu et al. 2021), PO43− (Guan et al. 2013) and Methylene blue (Maeda & Ishida 2011) etc. Notably, calcium silicate materials are non-toxic and environmentally friendly. Xonotlite, as a member of the calcium silicate family, has excellent adsorption properties. However, few reports are available on the synthesis of fibrous xonotlite from metallurgical residue. On the other hand, the metallurgical solid waste containing silicon causes great pressure to the environment due to huge quantity as well as the potential release of heavy metal ions and non-neutral wastewater. Therefore, the preparation of fibrous xonotlite from metallurgical residue is regarded as a feasible route towards environmental sustainability and resource utilization efficiency.

In this work, Na2SiO3 solution obtained from alkaline leaching waste residue was purified and used as raw material. Fibrous xonotlite was synthesized using the purified Na2SiO3 solution and self-made active Ca(OH)2 in the hydrothermal process. The adsorption performance of fibrous xonotlite for Congo red was discussed. The adsorption mechanism was determined, and the isotherm study was carried out using linear Langmuir and Freundlich models.

Materials

The main mineral phases in the silicon residue from nickel hydrometallurgy are quartz, lizardite, magnetite, amorphous SiO2, etc. Na2SiO3 solution was obtained through the reaction of residue and alkali. The obtained Na2SiO3 solution was purified. SiO32− solution concentration was adjusted to 0.05 mol·L−1. Active Ca(OH)2 emulsion with a concentration of 150 g·L−1 was prepared. The distilled water was homemade. Congo red purchased from Sinopharm Group was of analytical grade.

Preparation of fibrous xonotlite

120 mL of 0.05 mol·L−1 Na2SiO3 solution was added into a beaker fixed in a water bath with the pre-heated temperature of 40 °C. 3 mL Ca(OH)2 emulsion was slowly added according to Si/Ca molar ratio of 1:1 and held for 30 min under magnetic stirring. The slurry was transferred into a Teflon lining autoclave and aged for 1 h before 8 mL of 10 wt.% C12H25SO4Na (SDS) solution was added. The autoclave was placed in an oven preheated to 220 °C for 9 h. When the reaction was completed, the autoclave was naturally cooled down to room temperature. After filtration, the filter cake was washed four times using distilled water and three times using absolute ethanol. The fibrous xonotlite was obtained after being dried at 100 °C for 8 h. The filtrate was recycled to leach the residue for obtaining raw solution.

Adsorption experiments

In the kinetics adsorption, 50 mL Congo red solution with concentrations ranging from 100 to 200 mg·L−1 was employed. According to preset time intervals, the solutions were centrifuged and the concentrations of Congo red were measured before calculating the adsorption capacity.

In the thermodynamics adsorption, at the selected temperatures of 0, 20 and 40 °C, the experiments were implemented with the Congo red concentrations ranging from 100 to 300 mg·L−1.

Characterization

The morphology of the specimen was observed by a Hitachi 8010 scanning electron microscope. The structure of the specimen was identified by a Japan Rigakn UltimaIV X-ray diffraction, employing Cu radiation with a voltage of 40 kV, at a scanning rate of 8° min−1 with 2θ ranging from 5° to 90°. The FT-IR spectrum of the specimen was recorded on a Nicolet 380 infrared spectroscope. The concentrations of Congo red were measured using a TAS-990 atomic absorption spectrophotometer.

Characterization of fibrous xonotlite

Figure 1 shows the X-ray diffraction (XRD) pattern and scanning electron microscopy (SEM) image of fibrous xonotlite. XRD shows that all diffraction data are in good agreement with JCPDS file No. 230125, indicating that the obtained specimen is monoclinic xonotlite (Ca6Si6O17(OH)2). Fibrous xonotlite with high crystallinity exhibits good dispersibility and high aspect ratio.

Figure 1

XRD pattern (a) and SEM image (b) of fibrous xonotlite.

Figure 1

XRD pattern (a) and SEM image (b) of fibrous xonotlite.

Close modal

Adsorption of Congo red by fibrous xonotlite

The adsorption capacity of fibrous xonotlite for Congo red versus time using 30 mg xonotlite is presented in Figure 2(a). High adsorption capacities have been achieved in 1 min and adsorption capacities are 133.09, 213.60 and 278.15 mg·g−1. The adsorption almost reached the equilibrium in 10 min with the equilibrium adsorption capacities of 156.33, 237.72 and 316.77 mg·g−1 at the varied Congo red concentrations of 100–200 mg·L−1, respectively. Rapid and efficient adsorption makes fibrous xonotlite a potential adsorbent. The adsorption capacities of fibrous xonotlite for Congo red at varied initial concentrations ranging from 100 to 300 mg·L−1 and different temperatures within 10 min were studied, and the results were plotted in Figure 2(b). The adsorption capacities increase with increase of the temperature, implying that the adsorption is an endothermic process. Increasing temperature is favorable for adsorption. Furthermore, the adsorption capacities increase with the increase of Congo red concentration. This is because the increase of the Congo red molecules in solution improves the occupying opportunities of active sites of fibrous xonotlite. The equilibrium adsorption capacities at Congo red concentration of 300 mg·L−1 are 404.17, 445.86 and 454.16 mg·g−1 at temperatures of 0, 20 and 40 °C, respectively.

Figure 2

Relationships between adsorption capacities of Congo red and adsorption time (a), initial concentration (b).

Figure 2

Relationships between adsorption capacities of Congo red and adsorption time (a), initial concentration (b).

Close modal

Adsorption kinetics

The adsorption data of Congo red was fitted by the pseudo-first-order (Equation (1)) and pseudo-second-order (Equation (2)) models (Guo et al. 2018), which are given as below:
(1)
(2)
where t is time (min), qt and qe are the adsorbed capacities at time t and after reaching the adsorption equilibrium, respectively (mg·g−1), k1 (min−1) and k2 (g·(mg·min)−1) are the rate constants of the pseudo-first-order and the pseudo-second-order model, respectively.
Figure 3 shows the pseudo-first-order and the pseudo-second-order plots for adsorbing Congo red on fibrous xonotlite, and the corresponding parameters are listed in Table 1. It can be seen from Figure 3 that the pseudo-second-order kinetic model fits the adsorption data well, demonstrating that the adsorption process involves chemical adsorption. The rate constant k2 decreases with the increase of the initial Congo red concentration. As we know, the rate constant k2 can be expressed as a function of the absorption fraction F(F = qt/qe) and the time to reach F(tF), as shown in Equation (3) (Wang et al. 2007). Obviously, k2 is inversely proportional to tF, illustrating that as the initial Congo red concentration increases, k2 tends to decrease and adsorption requires more time.
(3)
Table 1

Kinetic parameters for the adsorption of Congo red

Pseudo-first-order model
Pseudo-second-order model
C0 (mg·L−1)qe (exp) (mg·g−1)qe (cal)k1R2qe (cal)k2R2
(mg·g−1)(min−1)(mg·g−1)(g·(mg·min)−1)
100 156.33 431.81 0.0021 0.3799 157.98 0.0345 0.9999 
150 237.71 352.56 0.0029 0.4463 239.81 0.0292 0.9999 
200 316.76 283.14 0.0060 0.4644 320.51 0.0174 0.9999 
Pseudo-first-order model
Pseudo-second-order model
C0 (mg·L−1)qe (exp) (mg·g−1)qe (cal)k1R2qe (cal)k2R2
(mg·g−1)(min−1)(mg·g−1)(g·(mg·min)−1)
100 156.33 431.81 0.0021 0.3799 157.98 0.0345 0.9999 
150 237.71 352.56 0.0029 0.4463 239.81 0.0292 0.9999 
200 316.76 283.14 0.0060 0.4644 320.51 0.0174 0.9999 
Figure 3

Pseudo-first-order (a) and pseudo-second-order (b) plots for the adsorption of Congo red.

Figure 3

Pseudo-first-order (a) and pseudo-second-order (b) plots for the adsorption of Congo red.

Close modal
The intra-particle diffusion model (Equation (4)) is employed to analyze the adsorption process (Yang & Al-Duri 2005).
(4)
where t is time (min), qt is the adsorbed capacity at time t (mg·g−1), k3 is the rate constant of the intra-particle diffusion model (mg·g−1·min−1/2), a is the intercept of the vertical axis (mg·g−1).

Figure 4(a) shows the fitting plots of the intra-particle diffusion model for the adsorption of Congo red on fibrous xonotlite. It can be clearly seen that the whole adsorption process can be divided into three stages. The external diffusion with the fastest adsorption rate occurred in the first stage of 1 min. In the second stage, the adsorption rate decreased obviously. The Congo red molecules might be transferred to the inner surface through intra-particle diffusion. In the last stage, the final adsorption equilibrium was reached. In the adsorption processes of macromolecular dyes, the rate of internal diffusion generally determines the adsorption rate of the whole process (Walker & Weatherley 2001). However, the fitting lines do not cross the ‘zero’, which reveals that internal diffusion is the main rate control step, but not the only one (Mohan et al. 2002). Other researchers also believed that if intra-particle diffusion was the only step, the internal diffusion rate kp would be linear with the square root of the initial solution concentration (Allen et al. 1992). To verify this conclusion, the experimental data are processed to obtain Figure 4(b). Clearly, there is no linear relationship between kp and the square root of the initial solution concentration. Therefore, the adsorption rate is controlled by the high-rate external diffusion and internal diffusion.

Figure 4

Intra-particle diffusion kinetics for the adsorption of Congo red (a) and relationships between kp and C00.5 (b).

Figure 4

Intra-particle diffusion kinetics for the adsorption of Congo red (a) and relationships between kp and C00.5 (b).

Close modal

Adsorption isotherms

To further investigate the effect of the temperature on Congo red adsorption, the experimental data were fitted by the Langmuir and Freundlich models. The results are shown in Figure 5, and the corresponding parameters are listed in Table 2.

Table 2

Langmuir and Freundlich model parameters for the adsorption of Congo red

Temperature/(°C)Langmuir
Freundlich
qmax (mg·g−1)KL(L·mg−1)R2KF (mg/g)(L/mg)1/nnR2
561.80 0.0325 0.9933 46.6316 1.9673 0.9762 
20 574.71 0.0618 0.9966 73.2531 2.1402 0.9607 
40 543.48 0.1007 0.9940 101.5549 2.4959 0.9821 
Temperature/(°C)Langmuir
Freundlich
qmax (mg·g−1)KL(L·mg−1)R2KF (mg/g)(L/mg)1/nnR2
561.80 0.0325 0.9933 46.6316 1.9673 0.9762 
20 574.71 0.0618 0.9966 73.2531 2.1402 0.9607 
40 543.48 0.1007 0.9940 101.5549 2.4959 0.9821 
Figure 5

Langmuir (a) and Freundlich (b) isotherm plots for the adsorption of Congo red.

Figure 5

Langmuir (a) and Freundlich (b) isotherm plots for the adsorption of Congo red.

Close modal
The Langmuir model is described as Equation (5):
(5)
where Ce is the equilibrium concentration of Congo red in the solution (mg·L−1), qe is the equilibrium adsorption capacity of Congo red on the adsorbent (mg·g−1), qmax is the theoretical maximum adsorption capacity (mg·g−1), and KL is the Langmuir adsorption equilibrium constant (L·mg−1), the value of which is related to the nature of the adsorbent and the temperature level; the higher the value of KL, the stronger the adsorption capacity.
The Freundlich model is described by Equation (6):
(6)
where KF is the adsorption capacity constant of the Freundlich model ((mg/g)(L/mg)1/n), and n is a constant related to adsorption strength, usually greater than 1.

It can be seen from Figure 5 that both of the isotherm models fitted well. By comparison, the R2 values of the Langmuir model are higher than those of the Freundlich model. In addition, the experimental maximum adsorption capacities (qmax) are basically consistent with those obtained from the Langmuir model, which indicates that the Langmuir model is more suitable to describe the adsorption. The adsorption of Congo red by fibrous xonotlite is monolayer, in agreement with the kinetic analysis. The maximum adsorption capacity reaches 574.71 mg·g−1 at 20 °C.

Adsorption thermodynamics

The plot of lnKL against 1/T according to the Langmuir model is shown in Figure 6. The free energy change (ΔGΘ), enthalpy change (ΔHΘ) and entropy change (ΔSΘ) were calculated using Equations (7) and (8) (Vimonses et al. 2009; Deng et al. 2016). The relevant parameters are displayed in Table 3. The values of ΔGΘ are negative, manifesting that the adsorption is spontaneous. It is more negative with the increase in temperature, indicating that high temperature increases the tendency to proceed spontaneously. A positive value of ΔHΘ reveals that the adsorption is endothermic. The positive value of ΔSΘ at the selected temperatures suggests that Congo red has a high affinity with fibrous anhydrite, and the randomness of the solid-liquid surface increases during the adsorption (Fu et al. 2018).
(7)
(8)
where KL is the adsorption capacity constant of the Langmuir model (L·mg−1), R is the gas constant of 8.314 (J·(mol·K)−1), T is the thermodynamic temperature (K).
Table 3

Thermodynamic parameters for the adsorption of Congo red

Temperature/KΔGΘ/(kJ·mol−1)ΔHΘ/(kJ·mol−1)ΔSΘ/(J·mol−1·K−1)
273 −7.918   
293 −9.973 20.137 102.765 
313 −12.028   
Temperature/KΔGΘ/(kJ·mol−1)ΔHΘ/(kJ·mol−1)ΔSΘ/(J·mol−1·K−1)
273 −7.918   
293 −9.973 20.137 102.765 
313 −12.028   
Figure 6

Plot of lnKL versus 1/ T for adsorption of Congo red on fibrous xonotlite.

Figure 6

Plot of lnKL versus 1/ T for adsorption of Congo red on fibrous xonotlite.

Close modal

Fourier transform infrared (FT-IR) spectra of fibrous xonotlite before and after adsorption

The FT-IR spectra of fibrous xonotlite before and after adsorption are displayed in Figure 7. The peak at 970 cm−1 is due to the antisymmetric tensile vibration of Si-OH. The broad bands at 1,204 and 1,074 cm−1 are attributed to the Si–O–Si asymmetric stretching vibration. The characteristic peak of the Si–O–Si bond is observed at 664 cm−1. The new adsorption band at 1,236 cm−1 is attributed to S = O stretching vibration and the bands appearing at 742 and 694 cm−1 can be assigned to the characteristic aromatic skeleton after Congo red adsorption (Hou et al. 2012). These results reveal that the Congo red molecules in solution have been effectively bound by fibrous xonotlite.

Figure 7

FT-IR spectra of fibrous xonotlite before and after adsorption.

Figure 7

FT-IR spectra of fibrous xonotlite before and after adsorption.

Close modal

Adsorption mechanism

The synthesized xonotlite has a fibrous structure with high aspect ratio, which not only provides a large specific surface area and a large number of active sites but also exhibits excellent hydroxyl releasing ability. According to the pHpzc of fibrous xonotlite, the surface of xonotlite is positively charged under pH less than 7, which can protonate the surface hydroxyl groups (Zhang et al. 2018). As a typical anionic organic, Congo red has a strong attraction to protonated hydroxyl groups (-OH2+) due to electrostatic attraction, which promotes the adsorption. Therefore, electrostatic attraction is considered to be the main mechanism of Congo red adsorption on fibrous xonotlite, as schematically presented in Figure 8.

Figure 8

Schematic diagram of Congo red adsorption on fibrous xonotlite.

Figure 8

Schematic diagram of Congo red adsorption on fibrous xonotlite.

Close modal
  • (1)

    Fibrous xonotlite with a high aspect ratio was successfully prepared at a Na2SiO3 concentration of 0.05 mol·L−1, Si/Ca molar ratio of 1:1, temperature of 220 °C and time of 9 h.

  • (2)

    Fibrous xonotlite shows excellent adsorption capacity for Congo red. The adsorption equilibrium can be reached in 10 min. The calculated maximum adsorption capacity is 574.71 mg·g−1 at 20 °C.

  • (3)

    The Langmuir model can describe the adsorption well. The adsorption kinetics follows the pseudo-second-order model. The adsorption rate is controlled by high-rate external diffusion and internal diffusion.

This work was supported by the National Natural Science Foundation of China (Nos. 51774070 and 52004165).

The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.

All relevant data are included in the paper or its Supplementary Information.

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