Preparation of Copper Ion Adsorbed Modified Montmorillonite/Cellulose Acetate Porous Composite Fiber Membrane by Centrifugal Spinning

The natural adsorption material montmorillonite (MMT) was selected, and cellulose acetate (CA) was used as the loading substrate to design and prepare a kind of green and environment-friendly recyclable porous composite fiber membrane with good heavy metal ion adsorption performance. Acetic acid modified montmorillonite (HCl-MMT), sodium dodecyl sulfonate modified montmorillonite (SDS-MMT), and chitosan modified montmorillonite (CTS-MMT) were prepared by inorganic modification and organic modification, and the porous MMT/CA composite fiber membrane was constructed by centrifugal spinning equipment. The morphological and structural changes of MMT before and after modification and their effects on porous composite fiber membranes were investigated. The morphology, structure, and adsorption properties of the composite fibers were characterized by scanning electron microscopy (SEM) and atomic absorption spectrometry (ASS). The experimental results showed that the maximum adsorption capacity of Cu2+ on the prepared 5 wt% CTS-MMT composite fiber membrane was 60.272 mg/g after 10 h static adsorption. The adsorption of Cu2+ by a porous composite fiber membrane conforms to the quasi-second-order kinetic model and Langmuir isothermal adsorption model. The main factor of the Cu2+ adsorption rate is chemical adsorption, and the adsorption mechanism is mainly monolayer adsorption.


Introduction
Heavy metal ions are one of the main sources of water pollution [1]. Most heavy metal ions are carcinogens, posing a threat to ecological balance and human health [2]. Cu 2+ is an essential trace element for the human body. However, too high a concentration of copper will lead to serious health problems such as brain and kidney issues and anemia [3]. The discharge of heavy-metal-polluted wastewater (e.g., brine) degrades water quality, and thus water cannot be directly used for potable water (via desalination) and industrial applications [4][5][6]. Therefore, it is necessary to remove residual copper ions in water. Many articles have reported various sewage treatment methods containing heavy metal ions, including adsorption, ion exchange, chemical precipitation, membrane filtration, electrochemical technology, and reverse osmosis [7][8][9][10]. As a water treatment technology with simple operation, obvious purification effects, large treatment capacity, and low cost, the adsorption method has been widely used in the treatment of heavy metal pollution in range of raw materials, and a controllable fluffy degree of fiber aggregate. It is a preparation method for micro/nanofiber with industrial application prospects [36,37].
To solve the above problems, three kinds of modified MMT were prepared by two modification methods and loaded on CA fiber to prepare an MMT/CA porous composite micro nanofiber membrane. The influence of MMT obtained by different modification methods on the composite fiber membrane was studied, and the influence of the amount of modified MMT on the morphology and properties of the porous composite fiber membrane was proved. The centrifugal spinning controllable preparation of a porous composite fiber membrane was realized, and it was applied to the adsorption of heavy metal ions in water.
The following equipment was used in the experiment: Pl203 electronic balance (Guangzhou Instrumental Laboratory Technology Co., Ltd.), IKA RET basic heating magnetic stirrer (Guangzhou Yike Laboratory Technology Co. Ltd.), vacuum over of-6020 vacuum drying oven (Shanghai Heheng Instrument Equipment Co. Ltd.), and pH-220 pen pH meter (Hangzhou Wenwei Instrument Co. Ltd.).

Preparation of Modified MMT
(a) HCl solution with a mass fraction of 36.5% was added to ultra-pure water and diluted to 150 mL HCl dilute solution with a mass fraction of 2%. An amount of 3.0 g montmorillonite was accurately weighed and added to the prepared HCl diluent. The constant temperature magnetic stirring water bath pot was used, the heating temperature was 50 • C, the rotation speed was set to 600 rpm, and the stirring was continued for 5 h under this condition. The mixed solution after stirring was centrifuged with a high-speed centrifuge (8000 rpm), the supernatant after centrifugation was discarded, the centrifuged precipitate was washed with purified water to remove HCl remaining in MMT, and the washing was repeated several times until the pH of MMT eluate reached 6. Centrifuging was performed again, and then the centrifuged products were dried in a vacuum drying oven with a constant temperature of 80 • C. Following this, the dried products were fully ground, and finally the acid-activated montmorillonite was prepared.
(b) The anionic surfactant SDS was accurately weighed and dissolved in ultra-pure water, and 150 mL of 0.1 mol/L SDS solution was prepared. Then, 3.0 g MMT was dispersed in the prepared SDS solution in the ratio of 1:60 (m/v), and the MMT/SDS mixed system was mixed and reacted at 80 • C and 600 rpm for 8 h by magnetic stirring. The reaction mixture was separated with a high-speed centrifuge (8000 rpm), and the precipitate was washed several times with 50% ethanol and centrifuged. Finally, the remaining solid was dried at 80 • C, and the dried product was fully ground to prepare SDS-MMT.
(c) A certain amount of glacial acetic acid (99%) was measured and added to ultra-pure water to prepare a 200 mL acetic acid aqueous solution with a mass fraction of 5%. It was stirred evenly and set aside. Then, 2 g CTS was accurately weighed and it was added to the prepared 5% acetic acid aqueous solution. It was stirred in a 60 • C water bath for 0.5 h to completely dissolve it to form a 10 g/L CTS solution. Then, 2 g MMT was accurately weighed, and it was added to the prepared CTS solution. The above mixture was placed on the collector-type constant temperature heating magnetic stirrer and stirred for 12 h at 35 • C and 600 rpm. The reaction mixture was separated with a high-speed centrifuge (8000 rpm) and the supernatant was discarded. The separated precipitated products were placed in a vacuum drying oven (80 • C) for drying, and then fully ground to finally prepare CTS-MMT.

Preparation of MMT/CA Porous Composite Fiber Membrane
Certain amounts of CA and MMT were weighed with an electronic balance, and they were then dissolved in the mixed solvent of DCM/DMSO (8:2 m/m) and placed in the sample bottle. The sample bottle was sealed with fresh-keeping film, raw material tape, and sealing film. After stirring for 12 h at 40 • C with a magnetic stirrer until it was completely dissolved, a centrifugal spinning solution with uniform MMT/CA dispersion was finally prepared. The centrifugal spinning machine was used with the following settings: the rotation speed of the centrifuge was set to 8000 r/min, the nozzle aperture to 0.4 mm, and the distance from the spinneret hole to the collecting rod to 12.0 cm. An amount of 5 mL of spinning solution and spinning head was taken, and it was stretched by the centrifugal force of the centrifuge and the solvent was volatilized rapidly. Finally, the porous composite fiber membrane was prepared.

Copper Ion Adsorption Experiment
An amount of 100 mg of prepared MMT/CA porous composite fiber membrane was immersed in a solution containing Cu 2+ (100 mg/L). The solution was placed in a shaking water bath for shaking, allowing the fiber membrane to fully contact the heavy metal ion solution. The fiber automatically adsorbed at a constant temperature of 25 • C, and the adsorption time was 24 h. After adsorption, the composite fiber membrane was taken out, soaked in ultra-pure water for 2 h, and dried for standby.
The adsorbed solution was diluted and the Cu 2+ concentration in the solution was detected by atomic absorption spectrometer. Then, the Cu 2+ adsorption capacity q e of the porous composite fiber membrane was calculated according to Formula (1).
In the formula, q e is the equilibrium adsorption amount of Cu 2+ after reaching the adsorption equilibrium of fiber membrane, mg/g; c 0 is the initial concentration of Cu 2+ in the solution prepared at the beginning of the experiment before adsorption, mg/L; c e is the concentration of Cu 2+ in the solution, mg/L, after reaching the adsorption equilibrium of the fiber membrane; m is the mass of the porous composite fiber membrane in the adsorption experiment, mg; and V is the volume of the Cu 2+ solution configured in the experiment, L.

Instruments and Characterization
The surface morphology of the composite fiber film was observed by scanning electron microscope (SEM, Germany, Carl Zeiss SMT Pte Ltd.), and the particle size distribution of the fiber was analyzed. Fourier transform infrared spectroscopy (FTIR, German Brooke spectrometer company, the number of scans was 32) was used to analyze the chemical structure of the samples by the potassium bromide mixed compression method. Analysis of the element composition of the composite fiber was conducted by X-ray photoelectron spectroscopy (K-Alpha, Thermo Scientific). The material composition and crystal structure of the composite fiber were analyzed by X-ray diffraction (XRD, ARL XTRA, Thermo ARL). The concentration change in Cu 2+ in the solution was detected by an AA-110 atomic absorption spectrometer (ASS, Beijing Purcell General Co., Ltd.).

Effect of Different Mass Fractions of MMT on Porous Composite Fiber Membrane
The porous composite fiber membranes with a different mass fraction of MMT (0~3%) and CA were prepared under the same spinning parameters. The influence of MMT mass fraction on the morphology of porous composite fibers was analyzed, and the relationship between MMT mass fraction and fiber diameter was investigated. Figure 1 shows SEM images and fiber diameter distribution of porous composite fiber membranes loaded with different mass fractions of MMT. According to the fiber diameter test results, the average fiber diameter corresponding to composite fiber membranes with MMT contents of 0%, 1%, 2%, and 3% is 11.74 µm, 12.04 µm, 13.49 µm, and 15.01 µm. With the increase in MMT content, the fiber surface still showed a porous structure, but the average diameter of the porous composite fiber increased gradually. This may be due to the higher mass fraction of MMT and the higher jet mass per unit spinning solution. Therefore, under the same centrifugal force, the spinning liquid jet is not easy to stretch, so the diameter of composite fibers increases with the increase in MMT content. When the addition of MMT is more than 3%, the porous CA fiber skeleton in the system cannot support too much MMT, which leads to difficulties in filamentation, and the fibers are mostly broken.

Effect of Different Mass Fractions of MMT on Porous Composite Fiber Membrane
The porous composite fiber membranes with a different mass fraction of MMT (0~3%) and CA were prepared under the same spinning parameters. The influence of MMT mass fraction on the morphology of porous composite fibers was analyzed, and the relationship between MMT mass fraction and fiber diameter was investigated. Figure 1 shows SEM images and fiber diameter distribution of porous composite fiber membranes loaded with different mass fractions of MMT. According to the fiber diameter test results, the average fiber diameter corresponding to composite fiber membranes with MMT contents of 0%, 1%, 2%, and 3% is 11.74 μm, 12.04 μm, 13.49 μm, and 15.01 μm. With the increase in MMT content, the fiber surface still showed a porous structure, but the average diameter of the porous composite fiber increased gradually. This may be due to the higher mass fraction of MMT and the higher jet mass per unit spinning solution. Therefore, under the same centrifugal force, the spinning liquid jet is not easy to stretch, so the diameter of composite fibers increases with the increase in MMT content. When the addition of MMT is more than 3%, the porous CA fiber skeleton in the system cannot support too much MMT, which leads to difficulties in filamentation, and the fibers are mostly broken.

SEM Analysis of Modified MMT
SEM images of various MMTs before and after modification are shown in Figure 2. Figure 2a shows that unmodified MMT mainly exists in the form of larger particles and has a layered structure. Figure 2b shows hydrochloric-acid-modified MMT (HCl-MMT). The modified MMT has a relatively small particle size, high dispersion, and large specific surface area. It is mainly because H + in a hydrochloric acid solution can dissolve some acid-soluble metal oxides and impurities in MMT, so that the lamellar structure of MMT becomes loose and the agglomerated particles are dispersed. The particle size of SDSmodified MMT (Figure 2c) decreases. As SDS enters the MMT lamellar structure, the agglomerated particles become dispersed, some particle multilayer structures are spread in

SEM Analysis of Modified MMT
SEM images of various MMTs before and after modification are shown in Figure 2. Figure 2a shows that unmodified MMT mainly exists in the form of larger particles and has a layered structure. Figure 2b shows hydrochloric-acid-modified MMT (HCl-MMT). The modified MMT has a relatively small particle size, high dispersion, and large specific surface area. It is mainly because H + in a hydrochloric acid solution can dissolve some acid-soluble metal oxides and impurities in MMT, so that the lamellar structure of MMT becomes loose and the agglomerated particles are dispersed. The particle size of SDSmodified MMT (Figure 2c) decreases. As SDS enters the MMT lamellar structure, the agglomerated particles become dispersed, some particle multilayer structures are spread in the form of single layers, and the specific surface area of MMT increases. Figure 2d shows chitosan-modified MMT (CTS-MMT). Compared with the morphology before modification, it can be seen that the surface of CTS-MMT is covered by a layer of flakes, and the specific surface area has increased. the form of single layers, and the specific surface area of MMT increases. Figure 2d shows chitosan-modified MMT (CTS-MMT). Compared with the morphology before modification, it can be seen that the surface of CTS-MMT is covered by a layer of flakes, and the specific surface area has increased.  Figure 3 shows the SEM images and corresponding fiber diameter distribution of composite fiber membranes prepared by three modified MMTs at different concentrations. It can be seen from Figure 3 that the modified MMT can prepare composite fiber membranes with porous surface structures. Under the same MMT addition (3 wt%), the average diameter of the prepared HCl-MMT/CA porous composite fiber membrane fiber is larger (average diameter is 15.48 μm), the spinning effect is relatively poor, and some fibers are twisted. However, SDS-MMT/CA and CTS-MMT/CA porous composite fiber membranes have better fiber morphology and smaller average fiber diameter (average diameters are 14.82 μm and 14.06 μm, respectively). This may be due to the existence of a long-chain molecular structure in SDS-MMT and CTS-MMT, which can be fully entangled with the CA molecular chain in the process of spinning solution preparation and stirring and can be more evenly distributed in the spinning solution system. The spinning effect of the prepared composite fiber is better. Due to the small particle size of HCl-MMT, it is easy to agglomerate in the spinning process, resulting in a poor spinning effect and composite fiber morphology. When the addition amount is 4 wt%, because the agglomeration phenomenon of HCl-MMT is intensified in the spinning process, the spinning solution cannot form a continuous jet, so the composite fiber membrane cannot be prepared. For SDS-MMT, due to the limited load of CA fibers, too much SDS-MMT will partially agglomerate. Although the composite fiber membrane is successfully prepared, its fiber morphology is poor, and the direct distribution of fibers is uneven (average diameter of 15.78 μm). CTS-MMT has a certain viscosity due to the existence of chitosan molecules on its surface, which can provide CA fibers with certain bonding properties during the spinning process so that its jet is not easily interrupted. Therefore, the morphology of the prepared composite fiber membrane is still good, and the surface roughness changes. However, when the addition of CTS-MMT reaches 5 wt%, the diameter of the composite fiber membrane fiber is relatively thick, the surface roughness of the fiber further increases, and the porous structure of the fiber surface begins to disappear gradually. When the addition  Figure 3 shows the SEM images and corresponding fiber diameter distribution of composite fiber membranes prepared by three modified MMTs at different concentrations. It can be seen from Figure 3 that the modified MMT can prepare composite fiber membranes with porous surface structures. Under the same MMT addition (3 wt%), the average diameter of the prepared HCl-MMT/CA porous composite fiber membrane fiber is larger (average diameter is 15.48 µm), the spinning effect is relatively poor, and some fibers are twisted. However, SDS-MMT/CA and CTS-MMT/CA porous composite fiber membranes have better fiber morphology and smaller average fiber diameter (average diameters are 14.82 µm and 14.06 µm, respectively). This may be due to the existence of a long-chain molecular structure in SDS-MMT and CTS-MMT, which can be fully entangled with the CA molecular chain in the process of spinning solution preparation and stirring and can be more evenly distributed in the spinning solution system. The spinning effect of the prepared composite fiber is better. Due to the small particle size of HCl-MMT, it is easy to agglomerate in the spinning process, resulting in a poor spinning effect and composite fiber morphology. When the addition amount is 4 wt%, because the agglomeration phenomenon of HCl-MMT is intensified in the spinning process, the spinning solution cannot form a continuous jet, so the composite fiber membrane cannot be prepared. For SDS-MMT, due to the limited load of CA fibers, too much SDS-MMT will partially agglomerate. Although the composite fiber membrane is successfully prepared, its fiber morphology is poor, and the direct distribution of fibers is uneven (average diameter of 15.78 µm). CTS-MMT has a certain viscosity due to the existence of chitosan molecules on its surface, which can provide CA fibers with certain bonding properties during the spinning process so that its jet is not easily interrupted. Therefore, the morphology of the prepared composite fiber membrane is still good, and the surface roughness changes. However, when the addition of CTS-MMT reaches 5 wt%, the diameter of the composite fiber membrane fiber is relatively thick, the surface roughness of the fiber further increases, and the porous structure of the fiber surface begins to disappear gradually. When the addition amount exceeds 5 wt%, the maximum load of CA fiber has been exceeded, and the porous composite fiber membrane with the corresponding addition amount cannot be successfully prepared. amount exceeds 5 wt%, the maximum load of CA fiber has been exceeded, and the po composite fiber membrane with the corresponding addition amount cannot be succ fully prepared. In order to further study the distribution of MMT on fibers, TEM images of sam were observed. As shown in Figure 4, compared with the pure CA fiber membrane, w the increase in the amount of modified MMT added, its distribution on the fiber sur also increases. The existence of MMT can be clearly observed on the porous fiber m brane prepared by the three modified MMTs. In order to further study the distribution of MMT on fibers, TEM images of samples were observed. As shown in Figure 4, compared with the pure CA fiber membrane, with the increase in the amount of modified MMT added, its distribution on the fiber surface also increases. The existence of MMT can be clearly observed on the porous fiber membrane prepared by the three modified MMTs.   Figure 5 shows the SEM diagram of the intercepted part of the high-load-modified MMT composite fiber membrane. It can be seen from the figure that when the addition amount of HCl-MMT is 4 wt%, the spun fiber is flat, and some fibers are melted and agglomerated together. When the addition amount of SDS-MMT is 5 wt%, the spun fiber is twisted and bonded and the amount is small. When the addition amount of CTS-MMT is 6 wt%, the spun fibers are different in thickness and twisted together. Therefore, the maximum spinnable addition amounts of each modified MMT are 3 wt% (HCl-MMT), 4 wt% (SDS-MMT), and 5 wt% (CTS-MMT), respectively.  Figure 6 shows the FTIR spectrum of MMT and modified MMT. It can be seen from Figure 6 that the peak at 3416 cm −1 in the four curves belongs to the -OH stretching vibration peak in MMT, indicating that the basic structure of the modified MMT is not damaged. New absorption peaks appear in the spectral curves c and d of SDS-MMT and CTS-MMT, while no new absorption peaks appear in the spectral curve b of HCl-MMT. The absorption peaks of curve c at wavelengths 2924 cm −1 and 2852 cm −1 correspond to the characteristic absorption peaks of -CH3 and -CH2 in SDS, respectively [38], which proves that SDS functional groups are successfully embedded in MMT. The new absorption peak at the wavelength of 1563 cm −1 in curve d belongs to the characteristic absorption peak of the amino group in CTS [32]. Due to the small concentration of CTS selected in the modification process, the characteristic absorption peak of the amino group at the wavelength of 1563 cm −1 in the measured data is small. Due to the dissolution of some impurities in the natural MMT, the measured infrared curve b of HCl-modified MMT is not significantly different from the natural MMT curve a. The feasibility of several modification methods was proved by FTIR analysis of MMT.    Figure 5 shows the SEM diagram of the intercepted part of the high-load-modified MMT composite fiber membrane. It can be seen from the figure that when the addition amount of HCl-MMT is 4 wt%, the spun fiber is flat, and some fibers are melted and agglomerated together. When the addition amount of SDS-MMT is 5 wt%, the spun fiber is twisted and bonded and the amount is small. When the addition amount of CTS-MMT is 6 wt%, the spun fibers are different in thickness and twisted together. Therefore, the maximum spinnable addition amounts of each modified MMT are 3 wt% (HCl-MMT), 4 wt% (SDS-MMT), and 5 wt% (CTS-MMT), respectively.  Figure 6 shows the FTIR spectrum of MMT and modified MMT. It can be seen from Figure 6 that the peak at 3416 cm −1 in the four curves belongs to the -OH stretching vibration peak in MMT, indicating that the basic structure of the modified MMT is not damaged. New absorption peaks appear in the spectral curves c and d of SDS-MMT and CTS-MMT, while no new absorption peaks appear in the spectral curve b of HCl-MMT. The absorption peaks of curve c at wavelengths 2924 cm −1 and 2852 cm −1 correspond to the characteristic absorption peaks of -CH3 and -CH2 in SDS, respectively [38], which proves that SDS functional groups are successfully embedded in MMT. The new absorption peak at the wavelength of 1563 cm −1 in curve d belongs to the characteristic absorption peak of the amino group in CTS [32]. Due to the small concentration of CTS selected in the modification process, the characteristic absorption peak of the amino group at the wavelength of 1563 cm −1 in the measured data is small. Due to the dissolution of some impurities in the natural MMT, the measured infrared curve b of HCl-modified MMT is not significantly different from the natural MMT curve a. The feasibility of several modification methods was proved by FTIR analysis of MMT.  Figure 6 shows the FTIR spectrum of MMT and modified MMT. It can be seen from Figure 6 that the peak at 3416 cm −1 in the four curves belongs to the -OH stretching vibration peak in MMT, indicating that the basic structure of the modified MMT is not damaged. New absorption peaks appear in the spectral curves c and d of SDS-MMT and CTS-MMT, while no new absorption peaks appear in the spectral curve b of HCl-MMT. The absorption peaks of curve c at wavelengths 2924 cm −1 and 2852 cm −1 correspond to the characteristic absorption peaks of -CH 3 and -CH 2 in SDS, respectively [38], which proves that SDS functional groups are successfully embedded in MMT. The new absorption peak at the wavelength of 1563 cm −1 in curve d belongs to the characteristic absorption peak of the amino group in CTS [32]. Due to the small concentration of CTS selected in the modification process, the characteristic absorption peak of the amino group at the wavelength of 1563 cm −1 in the measured data is small. Due to the dissolution of some impurities in the natural MMT, the measured infrared curve b of HCl-modified MMT is not significantly different from the natural MMT curve a. The feasibility of several modification methods was proved by FTIR analysis of MMT.  Figure 7 shows the EDS diagram of the composite fiber membrane and the EDS diagram of CTS prepared by the three modified MMTs at their respective maximum addition concentrations. According to the test results, the additional amount of MMT in the HCl-MMT composite fiber membrane is the same as that in the natural MMT composite fiber membrane (3 wt%). However, comparing Figure 7b with the EDS of the natural MMT composite fiber membrane (Figure 7a), it can be seen that the proportions of O, Al, and Si in the EDS diagram of HCl-MMT composite fiber membrane increased, which may be due to the more uniform dispersion of MMT modified by hydrochloric acid, which can obtain a larger load in spinning. SDS-MMT and CTS-MMT composite fiber films, due to their large amount of self-addition and easier preparation, account for a relatively large proportion of Al and Si elements in their EDS diagrams. According to Figure 7c, CTS molecules mainly contain C, N, and O elements, and the relative content of the N element is relatively small. A small amount of N-element peak can be observed in Figure 7d, indicating that CTS-MMT has a large content in the composite fiber membrane.   Figure 7 shows the EDS diagram of the composite fiber membrane and the EDS diagram of CTS prepared by the three modified MMTs at their respective maximum addition concentrations. According to the test results, the additional amount of MMT in the HCl-MMT composite fiber membrane is the same as that in the natural MMT composite fiber membrane (3 wt%). However, comparing Figure 7b with the EDS of the natural MMT composite fiber membrane (Figure 7a), it can be seen that the proportions of O, Al, and Si in the EDS diagram of HCl-MMT composite fiber membrane increased, which may be due to the more uniform dispersion of MMT modified by hydrochloric acid, which can obtain a larger load in spinning. SDS-MMT and CTS-MMT composite fiber films, due to their large amount of self-addition and easier preparation, account for a relatively large proportion of Al and Si elements in their EDS diagrams. According to Figure 7c, CTS molecules mainly contain C, N, and O elements, and the relative content of the N element is relatively small. A small amount of N-element peak can be observed in Figure 7d, indicating that CTS-MMT has a large content in the composite fiber membrane.

XRD Analysis of Porous Composite Fiber Membrane
To study the change in the layered structure of the modified MMT, X-ray diffraction (XRD) was used to characterize it. Figure 8 shows the XRD test results of MMT before and after modification. XRD test results combined with Bragg's law 2dsin θ = λ (Cu target, wavelength λ 0.15406 nm) can calculate the change in MMT layer spacing before and after modification. Compared with the natural MMT before modification, the diffraction angle of the characteristic crystal plane (001) of the three modified MMTs has shifted. It can be seen from the formula that the layer spacing does increase gradually when the diffraction angle shifts to a small angle. The characteristic diffraction peak of natural MMT is at 2θ = 9.18 • , corresponding layer spacing d = 0.96257 nm. The shift of the HCl-MMT characteristic diffraction peak is small at 2θ = 9.06 • , with a corresponding layer spacing d = 0.97530 nm. The characteristic diffraction peak of CTS-MMT is at 2θ = 8.62 • , with layer spacing d = 1.02498 nm. The maximum shift of the SDS-MMT characteristic diffraction peak is 2θ = 8.20 • , with a layer spacing d = 1.07738 nm. According to the calculation results, the interlayer spacing of HCl-modified MMT increased by 0.01273 nm due to the removal of interlayer impurities, while the interlayer spacing of CTS-modified MMT and SDS-modified MMT increased by 0.06241 nm and 0.11481 nm, respectively, due to CTS and SDS entering into the interlayer of MMT during the modification process. The shift of the MMT characteristic diffraction peak and the change in layer spacing before and after modification further illustrate the feasibility of the modification method.

XRD Analysis of Porous Composite Fiber Membrane
To study the change in the layered structure of the modified MMT, X-ray diffraction (XRD) was used to characterize it. Figure 8 shows the XRD test results of MMT before and after modification. XRD test results combined with Bragg's law 2dsin θ = λ (Cu target, wavelength λ 0.15406 nm) can calculate the change in MMT layer spacing before and after modification. Compared with the natural MMT before modification, the diffraction angle of the characteristic crystal plane (001) of the three modified MMTs has shifted. It can be seen from the formula that the layer spacing does increase gradually when the diffraction angle shifts to a small angle. The characteristic diffraction peak of natural MMT is at 2θ = 9.18°, corresponding layer spacing d = 0.96257 nm. The shift of the HCl-MMT characteristic diffraction peak is small at 2θ = 9.06°, with a corresponding layer spacing d = 0.97530 nm. The characteristic diffraction peak of CTS-MMT is at 2θ = 8.62°, with layer spacing d = 1.02498 nm. The maximum shift of the SDS-MMT characteristic diffraction peak is 2θ = 8.20°, with a layer spacing d = 1.07738 nm. According to the calculation results, the interlayer spacing of HCl-modified MMT increased by 0.01273 nm due to the removal of interlayer impurities, while the interlayer spacing of CTS-modified MMT and SDS-modified MMT increased by 0.06241 nm and 0.11481 nm, respectively, due to CTS and SDS entering into the interlayer of MMT during the modification process. The shift of the MMT characteristic diffraction peak and the change in layer spacing before and after modification further illustrate the feasibility of the modification method.

Kinetics of Adsorption of Cu 2+ on Porous Composite Fiber Membrane
Before the experiment, the influence of the pH value of the solution on the adsorption performance of the fiber membrane was tested. When the pH value is less than 5, the -NH2 in the CTS easily forms -NH3 + with the H + in the solution under acidic conditions, thus repelling Cu 2+ . When the pH value is greater than 5, with the decrease in the concentration of H + in the solution, Cu 2+ in the solution is easy to ionize in the water, forming hydrated ions, making it difficult to be adsorbed. When pH = 5, the porous composite fiber membrane had the best adsorption effect on Cu 2+ .The porous composite fiber

Kinetics of Adsorption of Cu 2+ on Porous Composite Fiber Membrane
Before the experiment, the influence of the pH value of the solution on the adsorption performance of the fiber membrane was tested. When the pH value is less than 5, the -NH 2 in the CTS easily forms -NH 3 + with the H + in the solution under acidic conditions, thus repelling Cu 2+ . When the pH value is greater than 5, with the decrease in the concentration of H + in the solution, Cu 2+ in the solution is easy to ionize in the water, forming hydrated ions, making it difficult to be adsorbed. When pH = 5, the porous composite fiber membrane had the best adsorption effect on Cu 2+ . The porous composite fiber membrane was added to the Cu 2+ adsorption solution (100 mg/L) with a pH value of 5 for the adsorption experiment. A certain amount of sample solution was extracted from the adsorption solution at 0.5, 1, 2, 4, 8, 12, and 24 h, respectively, for the atomic absorption spectrometry test. The relationship curve between adsorption time and adsorption capacity is shown in Figure 9. Due to a large number of binding points on the porous composite fiber and the high concentration of Cu 2+ in the solution, the adsorption capacity increases almost linearly [39], and the growth rate of the CTS-MMT porous composite fiber membrane is the largest. With the extension of adsorption time, due to the decrease in Cu 2+ concentration in the solution and the gradual reduction in binding points, the adsorption speed slows down. When the adsorption reaches a certain time, the adsorption capacity of the porous composite fiber membrane for Cu 2+ reaches saturation. The adsorption capacity of the 3% MMT composite fiber membrane reached the maximum value (44.243 mg/g) in 12 h, the 3% HCl-MMT composite fiber membrane reached the maximum adsorption capacity (46.155 mg/g) in 10 h, and the 4% SDS-MMT and 5% CTS-MMT composite fiber membranes reached the maximum adsorption capacity (52.381 mg/g and 60.272 mg/g) in 8 h. The reason is that the maximum spinning addition amount of CTS-MMT is 5 wt%. Compared with the other two modified MMTs, it can obtain a larger spinning addition amount, and the adsorption effect of heavy metal ions is more obvious.
membrane was added to the Cu 2+ adsorption solution (100 mg/L) with a pH value of 5 for the adsorption experiment. A certain amount of sample solution was extracted from the adsorption solution at 0.5, 1, 2, 4, 8, 12, and 24 h, respectively, for the atomic absorption spectrometry test. The relationship curve between adsorption time and adsorption capacity is shown in Figure 9. Due to a large number of binding points on the porous composite fiber and the high concentration of Cu 2+ in the solution, the adsorption capacity increases almost linearly [39], and the growth rate of the CTS-MMT porous composite fiber membrane is the largest. With the extension of adsorption time, due to the decrease in Cu 2+ concentration in the solution and the gradual reduction in binding points, the adsorption speed slows down. When the adsorption reaches a certain time, the adsorption capacity of the porous composite fiber membrane for Cu 2+ reaches saturation. The adsorption capacity of the 3% MMT composite fiber membrane reached the maximum value (44.243 mg/g) in 12 h, the 3% HCl-MMT composite fiber membrane reached the maximum adsorption capacity (46.155 mg/g) in 10 h, and the 4% SDS-MMT and 5% CTS-MMT composite fiber membranes reached the maximum adsorption capacity (52.381 mg/g and 60.272 mg/g) in 8 h. The reason is that the maximum spinning addition amount of CTS-MMT is 5 wt%. Compared with the other two modified MMTs, it can obtain a larger spinning addition amount, and the adsorption effect of heavy metal ions is more obvious. To further analyze the adsorption performance of porous composite fiber membranes, the test data were fitted with a kinetic model. The quasi-first-order dynamics and quasi-second-order dynamics models were used to fit and analyze them, respectively. The equation of the quasi-first-order dynamics model is shown in Formula (2): In the formula, qe is the adsorption amount when the adsorption reaches equilibrium, mg/g, qt is the Cu 2+ adsorption at time t, mg/g; t is the adsorption time, h; and K1 is the quasi-first-order adsorption rate constant, h −1 .
The equation of the quasi-second-order dynamics model is shown in formula (3): To further analyze the adsorption performance of porous composite fiber membranes, the test data were fitted with a kinetic model. The quasi-first-order dynamics and quasisecond-order dynamics models were used to fit and analyze them, respectively. The equation of the quasi-first-order dynamics model is shown in Formula (2): In the formula, q e is the adsorption amount when the adsorption reaches equilibrium, mg/g, q t is the Cu 2+ adsorption at time t, mg/g; t is the adsorption time, h; and K 1 is the quasi-first-order adsorption rate constant, h −1 .
The equation of the quasi-second-order dynamics model is shown in Formula (3): In the formula, q e , q t, and t are the same as in the quasi-first-order kinetic model, and K 2 represents the quasi-second-order adsorption rate constant, g/mg·h −1 .
According to the fitting results of Cu 2+ adsorption kinetics of the 5 wt% CTS-MMT composite fiber membrane ( Figure 10) and fitting parameters (Table 1), the correlation coefficient of the quasi-first-order kinetic model is 0.885, and the quasi-second-order correlation coefficient is 0.995. The saturated adsorption capacity obtained from the quasi-secondorder kinetic model is 65.92 mg/g, and the actual measured value is 60.272 mg/g. The equilibrium adsorption capacity fitted by the quasi-second-order kinetic model is closer to the actual adsorption capacity of a porous composite fiber membrane. Therefore, the adsorption process is more suitable to be explained by the quasi-second-order kinetic model; that is, the main factor affecting the adsorption rate of the porous composite fiber membrane is chemical adsorption, and the adsorption process is coordinated by a variety of kinetic mechanisms to achieve the maximum adsorption capacity.
In the formula, qe, qt, and t are the same as in the quasi-first-order kinetic model, and K2 represents the quasi-second-order adsorption rate constant, g/mg·h −1 .
According to the fitting results of Cu 2+ adsorption kinetics of the 5 wt% CTS-MMT composite fiber membrane ( Figure 10) and fitting parameters (Table 1), the correlation coefficient of the quasi-first-order kinetic model is 0.885, and the quasi-second-order correlation coefficient is 0.995. The saturated adsorption capacity obtained from the quasisecond-order kinetic model is 65.92 mg/g, and the actual measured value is 60.272 mg/g. The equilibrium adsorption capacity fitted by the quasi-second-order kinetic model is closer to the actual adsorption capacity of a porous composite fiber membrane. Therefore, the adsorption process is more suitable to be explained by the quasi-second-order kinetic model; that is, the main factor affecting the adsorption rate of the porous composite fiber membrane is chemical adsorption, and the adsorption process is coordinated by a variety of kinetic mechanisms to achieve the maximum adsorption capacity.   Figure 11 is the adsorption isotherm of Cu 2+ on a 5 wt% CTS-MMT composite fiber membrane. It can be seen from the test results in the figure that with the increase in the initial concentration of Cu 2+ in the adsorption solution, the adsorption capacity of the porous composite fiber also increases. When the concentration of Cu 2+ increases to 100 mg/L, its adsorption capacity will no longer continue to increase with the increase in Cu 2+ concentration, indicating that at this concentration, the adsorption of Cu 2+ by the porous composite fiber membrane has reached adsorption equilibrium, and the maximum adsorption capacity of Cu 2+ is 60.272 mg/g. The main reason for this is that when the quality of the composite fiber membrane is certain, with the continuous increase in Cu 2+ concentration in the adsorption solution, its mass transfer promotion ability also increases. Cu 2+ is easier to move to the surface of the porous composite fiber membrane, making the adsorption easier, and increasing the adsorption capacity. However, the number of active sites on the composite fiber membrane is certain. When it is filled with Cu 2+ , the maximum adsorption capacity of the composite fiber membrane will not change, which can be considered adsorption saturation.   Figure 11 is the adsorption isotherm of Cu 2+ on a 5 wt% CTS-MMT composite fiber membrane. It can be seen from the test results in the figure that with the increase in the initial concentration of Cu 2+ in the adsorption solution, the adsorption capacity of the porous composite fiber also increases. When the concentration of Cu 2+ increases to 100 mg/L, its adsorption capacity will no longer continue to increase with the increase in Cu 2+ concentration, indicating that at this concentration, the adsorption of Cu 2+ by the porous composite fiber membrane has reached adsorption equilibrium, and the maximum adsorption capacity of Cu 2+ is 60.272 mg/g. The main reason for this is that when the quality of the composite fiber membrane is certain, with the continuous increase in Cu 2+ concentration in the adsorption solution, its mass transfer promotion ability also increases. Cu 2+ is easier to move to the surface of the porous composite fiber membrane, making the adsorption easier, and increasing the adsorption capacity. However, the number of active sites on the composite fiber membrane is certain. When it is filled with Cu 2+ , the maximum adsorption capacity of the composite fiber membrane will not change, which can be considered adsorption saturation.

Study on Adsorption Isotherm of Cu 2+ on Porous Composite Fiber Membrane
The equilibrium adsorption mechanism was explored between the porous composite fiber membrane and Cu 2+ solution, and Langmuir and Freundlich adsorption isotherm models were used to linearly fit its adsorption isotherm. The linear equations of the two adsorption isotherm models can be described by Formulas (4) and (5): ln q e = ln K F + ln C e n In the formula, C e is the concentration of Cu 2+ in the solution at adsorption equilibrium, mg/L; q e is the adsorption amount of Cu 2+ when the adsorption reaches equilibrium, mg/g; q m is the maximum adsorption capacity of Cu 2+ when the adsorption reaches saturation, mg/g; b is the Langmuir constant, L/mg; K F is the Freundlich constant, L/mg; and n is the Freundlich constant. The equilibrium adsorption mechanism was explored between the porous composite fiber membrane and Cu 2+ solution, and Langmuir and Freundlich adsorption isotherm models were used to linearly fit its adsorption isotherm. The linear equations of the two adsorption isotherm models can be described by Formulas (4) and (5): In the formula, Ce is the concentration of Cu 2+ in the solution at adsorption equilibrium, mg/L; qe is the adsorption amount of Cu 2+ when the adsorption reaches equilibrium, mg/g; qm is the maximum adsorption capacity of Cu 2+ when the adsorption reaches saturation, mg/g; b is the Langmuir constant, L/mg; KF is the Freundlich constant, L/mg; and n is the Freundlich constant.
The fitting results of the isothermal adsorption model are shown in Figure 12 and Table 2. The fitting correlation coefficients R 2 of the two isothermal adsorption models are 0.993 (Langmuir model) and 0.889 (Freundlich model), respectively. The Langmuir adsorption isotherm is based on the assumption that the adsorbent surface is uniform, and the adsorption is regular when the adsorption reaches equilibrium in the case of the single molecular layer with the saturated adsorption capacity value. The Freundlich adsorption isotherm belongs to real adsorption, and there is no saturated adsorption capacity value. Therefore, the adsorption process of the 5 wt% CTS-MMT composite fiber membrane for Cu 2+ is more suitable to be described by the Langmuir adsorption isotherm model, that is, the adsorption process is mainly monolayer adsorption, and each of the adsorption sites on the composite fiber membrane have the same activity and do not affect each other [40]. The maximum equilibrium adsorption capacity fitted by this model is 64.023 mg/g, which The fitting results of the isothermal adsorption model are shown in Figure 12 and Table 2. The fitting correlation coefficients R 2 of the two isothermal adsorption models are 0.993 (Langmuir model) and 0.889 (Freundlich model), respectively. The Langmuir adsorption isotherm is based on the assumption that the adsorbent surface is uniform, and the adsorption is regular when the adsorption reaches equilibrium in the case of the single molecular layer with the saturated adsorption capacity value. The Freundlich adsorption isotherm belongs to real adsorption, and there is no saturated adsorption capacity value. Therefore, the adsorption process of the 5 wt% CTS-MMT composite fiber membrane for Cu 2+ is more suitable to be described by the Langmuir adsorption isotherm model, that is, the adsorption process is mainly monolayer adsorption, and each of the adsorption sites on the composite fiber membrane have the same activity and do not affect each other [40]. The maximum equilibrium adsorption capacity fitted by this model is 64.023 mg/g, which is larger than the actual maximum adsorption capacity of 60.272 mg/g, indicating that the prepared porous composite fiber membrane has great potential for Cu 2+ adsorption. According to the empirical parameter 1/n (0.298) in the Freundlich adsorption model, which is between 0-1, it shows that the porous composite fiber membrane maintains positive adsorption during the adsorption of Cu 2+ .

Study on the Recycling of Porous Composite Fiber Membrane
The porous composite fiber membrane of adsorbed Cu 2+ was desorbed with an EDTA-2Na solution (100 mg/L). It was soaked in the prepared desorption solution (25 °C, 2 h), then soaked in ultrapure water, rinsed several times, dried naturally after desorption, and the vacuum dried. After a period of time, the next adsorption desorption cycle was carried out for the Cu 2+ solution with the same concentration, and the concentration of Cu 2+ in the desorption solution was determined by atomic absorption spectrometer. The re-adsorption efficiency (Re) is calculated by Formula (6): In the formula: q1: The first Cu 2+ equilibrium adsorption capacity of the porous composite fiber membrane, mg/g; qd: Cu 2+ equilibrium adsorption capacity of the porous composite fiber membrane after desorption, mg/g. It can be seen from Figure 13 that after five desorption cycles, the 3 wt% natural MMT composite fiber membrane and the 5 wt% CTS-MMT composite fiber membrane have certain re-adsorption capacity. Among them, the chitosan-modified MMT composite fiber membrane has a relatively high re-adsorption effect (83%) after five desorption cycles. In this experiment, the regeneration of the CTS-MMT composite fiber membrane with strong adsorption capacity was also explored. The composite fiber membrane after the desorption cycle was dried, weighed, and prepared into a spinning solution for secondary spinning. As shown in Figure 14, by comparing the SEM images of the CTS-MMT composite fiber membrane prepared by two spinning processes, it can be seen that the surface of the composite fiber membrane prepared by re-dissolution and re-spinning still has a porous structure, and can maintain a good fiber morphology, which further illustrates that the selected load substrate CA has a certain renewable recycling usability.

Study on the Recycling of Porous Composite Fiber Membrane
The porous composite fiber membrane of adsorbed Cu 2+ was desorbed with an EDTA-2Na solution (100 mg/L). It was soaked in the prepared desorption solution (25 • C, 2 h), then soaked in ultrapure water, rinsed several times, dried naturally after desorption, and the vacuum dried. After a period of time, the next adsorption desorption cycle was carried out for the Cu 2+ solution with the same concentration, and the concentration of Cu 2+ in the desorption solution was determined by atomic absorption spectrometer. The re-adsorption efficiency (Re) is calculated by Formula (6): In the formula: q 1 : The first Cu 2+ equilibrium adsorption capacity of the porous composite fiber membrane, mg/g; q d : Cu 2+ equilibrium adsorption capacity of the porous composite fiber membrane after desorption, mg/g. It can be seen from Figure 13 that after five desorption cycles, the 3 wt% natural MMT composite fiber membrane and the 5 wt% CTS-MMT composite fiber membrane have certain re-adsorption capacity. Among them, the chitosan-modified MMT composite fiber membrane has a relatively high re-adsorption effect (83%) after five desorption cycles. In this experiment, the regeneration of the CTS-MMT composite fiber membrane with strong adsorption capacity was also explored. The composite fiber membrane after the desorption cycle was dried, weighed, and prepared into a spinning solution for secondary spinning. As shown in Figure 14, by comparing the SEM images of the CTS-MMT composite fiber membrane prepared by two spinning processes, it can be seen that the surface of the composite fiber membrane prepared by re-dissolution and re-spinning still has a porous structure, and can maintain a good fiber morphology, which further illustrates that the selected load substrate CA has a certain renewable recycling usability.

Conclusions
In this paper, MMT was modified by organic and inorganic methods. The porous MMT/CA composite fiber membrane with porous structure and good Cu 2+ adsorption properties was successfully prepared by mixing MMT and CA and adopting efficient spinning and centrifugal spinning technology. The prepared porous composite fiber membrane was applied to the adsorption of Cu 2+ . When pH = 5, the maximum adsorption capacity of the 5 wt% CTS-MMT composite fiber membrane for Cu 2+ could reach 60.272 mg/g after 10 h static adsorption. The fitting analysis of the data of Cu 2+ adsorption equilibrium shows that the adsorption process is more suitable to be described by the quasisecond-order kinetic model and Langmuir isothermal adsorption model. The prepared porous composite fiber membrane can still retain an 83% Cu 2+ adsorption effect after five desorption cycles. The composite fiber membrane with porous structure can be prepared again by dissolving and spinning the composite fiber membrane after desorption, which shows that the selected load base material, CA, has a certain recyclability.

Conflicts of Interest:
The authors declared no potential conflicts of interest concerning the research, authorship, and/or publication of this article.

Conclusions
In this paper, MMT was modified by organic and inorganic methods. The porous MMT/CA composite fiber membrane with porous structure and good Cu 2+ adsorption properties was successfully prepared by mixing MMT and CA and adopting efficient spinning and centrifugal spinning technology. The prepared porous composite fiber membrane was applied to the adsorption of Cu 2+ . When pH = 5, the maximum adsorption capacity of the 5 wt% CTS-MMT composite fiber membrane for Cu 2+ could reach 60.272 mg/g after 10 h static adsorption. The fitting analysis of the data of Cu 2+ adsorption equilibrium shows that the adsorption process is more suitable to be described by the quasisecond-order kinetic model and Langmuir isothermal adsorption model. The prepared porous composite fiber membrane can still retain an 83% Cu 2+ adsorption effect after five desorption cycles. The composite fiber membrane with porous structure can be prepared again by dissolving and spinning the composite fiber membrane after desorption, which shows that the selected load base material, CA, has a certain recyclability.

Conflicts of Interest:
The authors declared no potential conflicts of interest concerning the research, authorship, and/or publication of this article. Figure 14. SEM of the first spinning (a,b) and the second spinning (c,d) of CTS-MMT composite fiber membrane.

Conclusions
In this paper, MMT was modified by organic and inorganic methods. The porous MMT/CA composite fiber membrane with porous structure and good Cu 2+ adsorption properties was successfully prepared by mixing MMT and CA and adopting efficient spinning and centrifugal spinning technology. The prepared porous composite fiber membrane was applied to the adsorption of Cu 2+ . When pH = 5, the maximum adsorption capacity of the 5 wt% CTS-MMT composite fiber membrane for Cu 2+ could reach 60.272 mg/g after 10 h static adsorption. The fitting analysis of the data of Cu 2+ adsorption equilibrium shows that the adsorption process is more suitable to be described by the quasi-second-order kinetic model and Langmuir isothermal adsorption model. The prepared porous composite fiber membrane can still retain an 83% Cu 2+ adsorption effect after five desorption cycles. The composite fiber membrane with porous structure can be prepared again by dissolving and spinning the composite fiber membrane after desorption, which shows that the selected load base material, CA, has a certain recyclability.

Conflicts of Interest:
The authors declare no conflict of interest.