Introduction

Metal–organic frameworks (MOFs) are a novel kind of crystalline porous materials self-assembled by metal ions or metal clusters and organic ligands. Due to their large specific surface areas, abundant and adjustable micro-/nanoporous structures, and functional responder loci, MOFs have become one of the most promising adsorption materials that have attracted considerable attention in recent times [1,2,3,4]. Zeolitic imidazolate framework (ZIF-8) is an important MOF fabricated with zinc ions coordinated by four imidazolate rings [5]. They contain small nanopores (0.34 nm) in their structures. Nanoporous structures with diameters of within 2.0 nm exhibit strong van der Waals forces that can effectively adsorb diverse small molecules of toxic or hazardous gases. ZIF-8 also contains larger molecular cages (11.6 nm in diameter) that can also improve adsorption. The specific surface area of ZIF-8 is quite large, and it has a pore volume of approximately 0.63 m3 g−1. ZIF-8 with stable structures can be obtained easily, cheaply, and quickly. Therefore, ZIF-8 is popularly used as an excellent adsorbent material for removing HCHO [6,7,8]. Long-term exposure to HCHO can cause different diseases such as eye, skin and throat irritation, headache, breathing problems, and even leukemia or cancer [9, 10]. Therefore, removing HCHO is very important to ensure good human health and environmental protection. However, ZIF-8 is typically a milli- to nanoscale crystalline material, which restricts its applications. The loading of nanoscale ZIF-8 on suitable substrates is necessary for practical applications [11, 12].

Nowadays, carbon-based materials, such as activated carbons, activated carbon fibers, and inorganic particles/carbon composite materials, are generally used as HCHO adsorbents [13,14,15,16]. The HCHO molecule is very small; hence, physical adsorption on activated carbon usually exhibits low efficiency for HCHO adsorption. Activated carbon fibers have become novel carbon materials with a large specific surface area, several micropores, fast adsorption rate, and nearly no impurity. However, the micropores are in the radial direction with small diffusion resistance; hence, it is easy to achieve HCHO desorption into the air. Functional particles, such as ZIF-8 nanocrystals, loaded on carbon fibers materials can improve the adsorption efficiency [17,18,19].

Atomic layer deposition (ALD) is a special chemical vapor deposition technique, which is a method of forming thin films by alternately passing a gas-phase precursor pulse through a reaction chamber and a chemical adsorption reaction on the surface of the deposition substrates. Depending on the desired film thickness, multiple repetitions of the growth cycle may be required. ALD technology has been applied in microelectronics, optoelectronics, energy, biology, nanotechnology, catalysis, corrosion resistance, and sealing coating. Some researchers have reported a method known as AIM (ALD in MOFs) that uses ALD to install atomic precision metals into metal–organic frames (MOFs) [20, 21]. They synthesized Zn-AIM-NU-1000 as a catalytical material using the AIM method. Based on this method, we can synthesize new composites that can catalyze HCHO by ALD (TiO2) and MOF (ZIF-8) on suitable substrates [22].

Since they combine the advantages of ACF felts and ZIF-8, they can be composited to achieve highly efficient removal of HCHO. Hydrothermal reaction is an efficient and simple method for the growth of ZIF-8 nanocrystals on fiber materials [23, 24]. To achieve higher growth of ZIF-8, the ACF felts can be modified in advance [25,26,27]. In this study, ACF felts were used as substrates and coated with TiO2 via ALD. ALD can be employed to make very thin and uniform films of TiO2, with the thickness controllable at the atomic level. The structures and properties of the substrates are not affected. In addition, it possesses excellent speed [28,29,30]. It is propitious for the growth of ZIF-8 nanocrystals; conversely, the HCHO can be photocatalyzed and decomposed into CO2 and H2O via TiO2 under UV light. The HCHO is first captured by the micro-/nanopores in ZIF-8@ALD-ACF felt composite materials and then photocatalyzed via TiO2 thin film under UV light, given enough contact and decomposition time. It is superior to the adsorption materials that do not compound the fixation and decomposition processes for HCHO. During the adsorption and photocatalysis process, 100% of the HCHO can be removed within 110 min at high concentration and within 6 min at low concentration. The composite material, ZIF-8@ALD-ACF felts, holds important practical applications for HCHO removal.

Experimental

Materials

2-Methylimidazole (2-MeIM) (98% purity) was purchased from MACKLIN. Zinc nitrate hexahydrate (Zn(NO3)2·6H2O, 99% purity) and HCHO solution were purchased from Sinopharm Chemical Reagent Co., Ltd of Shanghai (Shanghai, China). Titanium(IV) isopropoxide (TIP, 99.999% metals basis) was obtained from Aladdin Industrial Co., Ltd. Deionized water, purified using a Milli-Q Plus 185 water purification system (Millipore, Bedford, MA), was used throughout this study. The water had a resistivity of 10-16 MΩ cm. Activated carbon fiber felts were purchased from a local market in China. All materials and chemicals were of reagent grade and used without further purification.

Preparation of ZIF-8 nanocrystals

The ZIF-8 nanocrystals were synthesized in purely aqueous solution by integrating the methods reported by Yichang Pan et al. Typically, the molar ratio of Zn(NO3)2·6H2O/ 2-methylimidazole/ H2O in the synthesized solution was set at 1:70:1238 [31]. First, 1.17 g Zn(NO3)2·6H2O and 22.70 g 2-MeIM were dissolved in 8 and 80 ml deionized water, respectively. The two solutions were then mixed by mechanical stirring. Subsequently, the mixture was transferred to a Teflon-lined autoclave and hydrothermally reacted at 70 °C for 24 h. The final ZIF-8 nanocrystals were collected by centrifuging at 8000 r min−1 for 15 min, adequately washed with ethanol and deionized water, and then dried at 50 °C.

Preparation of ZIF-8-coated activated carbon fiber felts (ZIF-8@ACF felts)

The ZIF-8 @ ACF felts composite was prepared under the same conditions. The procedure for preparing ZIF-8-coated activated carbon fiber felts is presented in Fig. 1. First, 3 g activated carbon fiber felts were added to the solution of 22.70 g 2-MeIM 80 ml deionized water and moderately stirred for 5 min. Then, a solution of 1.17 g Zn(NO3)2·6H2O in 8 ml deionized water was added into the reaction system drop by drop. After stirring moderately for another 5 min, the mixture was transferred to a Teflon-lined autoclave and hydrothermally reacted at 70 °C for 24 h. The final ZIF-8 @ ACF felts samples were adequately washed with ethanol and deionized water and then dried naturally.

Figure 1
figure 1

Schematic showing the preparation procedure for ZIF-8-coated activated carbon fiber felts

Preparation of ZIF-8 nanocrystals growth on TiO2-coated activated carbon fiber felts via ALD (ZIF-8@ALD-ACF felts)

The process for preparing TiO2-coated activated carbon fiber felts via ALD was conducted using a Savannah S100 ALD reactor (Savannah System, Cambridge NanoTech. Inc., USA) equipped with a gas-flow system. Titanium(IV) isopropoxide and H2O were used as titanium and oxygen precursors, respectively, to deposit TiO2 at a temperature of 150 °C. High-purity nitrogen (N2, 99.999%) was used as both purge gas and carrier gas for both precursors. A steady flow of nitrogen at 50 sccm (standard cubic centimeters per minute) was used in the ALD process. Prior to the ALD processing, the activated carbon fiber felts were placed in the ALD reactor and dried in vacuum (∼ 0.5 Torr) at 150 °C for 5 min. To produce adequate vapor pressures, the TIP was heated to 80 °C and the water was maintained at the ambient temperature. In the first half cycle, water vapor was pulsed into the chamber for 0.05 s, the activated carbon fiber felts were exposed to water vapor for 8 s; the reactor was then purged with nitrogen for 20 s. In the second half cycle, TIP was pulsed into the chamber for 0.2 s, the activated carbon fiber felts were exposed to TIP for 8 s, and the reactor was purged with nitrogen for 20 s. Each complete ALD cycle lasted for a duration of 56.25 s [32].The TiO2-coated ACF felts used in this work were processed 1000 cycles. The hydrothermal method employed is the same as the above; however, the activated carbon fiber felts were replaced with TiO2-coated activated carbon fiber felts as substrate. The ZIF-8@ALD-ACF felts were obtained, and the entire process is shown in Fig. 2.

Figure 2
figure 2

Schematic diagram showing the process for TiO2-coated on ACF felts via ALD and ZIF-8 nanocrystals growth on ALD-ACF felts

Characterization

The magnetic suspension balance, RUBOTHERM, with a precision of 0.0001 g was supplied by Germany. Morphologies of the ACF felts, 1000 cycles of ALD-ACF felts, ZIF-8@ACF felts, and ZIF-8@ALD-ACF felts were examined on a scanning electron microscope (JSM-5610LV, JEOL Co. Ltd, Japan) at 15 kV after gold coating. X-ray diffraction (XRD) was performed at room temperature using an X’Pert PRO XRD spectrometer (PANalytical, Holland) with a Cu-Kα radiation source at a generator voltage of 40 kV and a generator current of 50 mA. The changes in the formaldehyde adsorbed by activated carbon fiber felt station was measured by Bruker Tensor 27 Fourier-transform infrared spectroscopy (FT-IR). The adsorbate for this study was HCHO solution purchased from Sinopharm Chemical Reagent Co., Ltd., with 99.0% purity. The HCHO standard solution was heated at a certain temperature before placing it inside the test chamber. The HCHO adsorption and catalysis tests are static at room temperature (25 °C), and the relative humidity was about 40%–60%. HCHO at high concentration (100 mg m−3) or low concentration (10 mg m−3) was used as an initial concentration in a test chamber having a volume of 0.5 m3. The mass of adsorbents (ACF, ALD-ACF, ZIF-8@ACF, and ZIF-8@ALD-ACF felts) was 3 g. At the beginning of the experiment, the corresponding HCHO concentration was recorded per minute.

Results and discussion

Structure and morphology of the ZIF-8 nanocrystals, ACF felts, ALD-ACF felts, ZIF-8@ACF felts, and ZIF-8@ALD-ACF felts

The morphology and microstructure of the pure ZIF-8 nanocrystals were examined using SEM and XRD. Figure 3a reveals that ZIF-8 particles exhibit hexagonal and cube-like shape ca. 100 nm in diameter. The XRD patterns of pure ZIF-8 nanocrystals are shown in Fig. 3b. ZIF-8 nanocrystal peaks at 2θ = 7.3°, 10.4°, 12.7°, 14.7°,16.4°, and 17.9° are associated with the crystal planes (011), (022), (112), (022), (013), and (222) of the ZIF-8 nanocrystals, respectively [33]. All observed peaks fairly matched the standard XRD pattern of ZIF-8 from the CCDC file (602542). The ZIF-8 nanocrystals were synthesized in a purely aqueous solution. The nanoparticles obtained can be suitably dispersed in deionized water to form a stable suspension and can be kept for several days without settling (the inset in Fig. 3a).

Figure 3
figure 3

a SEM images of pure ZIF-8 nanocrystals; the inset represents corresponding particle size distributions and a digital photograph of an opalescent stable suspension of the as-synthesized ZIF-8 nanocrystals dispersed in deionized water. b XRD patterns of pure ZIF-8 nanocrystals

The morphology and microstructure of the ACF felt, ALD-ACF felts, ZIF-8@ACF felts, and ZIF-8@ALD-ACF felts are shown in Fig. 4. ACF felts (Fig. 4a, b) and ALD-ACF felts (Fig. 4d, e) were clean with relatively smooth textures. The ALD process produces very thin and uniform films of TiO2 with smooth fibers surfaces. After the hydrothermal reaction, nanoscale ZIF-8 was coated on ACF felts or ALD-ACF felts. Some ZIF-8 crystalline particles could be observed to be coated on the ACF felts (Fig. 4g, h). However, it can be reached easily from relatively sparse ZIF-8 crystalline particles on ACF felts to dense ZIF-8 crystalline film on ALD-ACF felts (Fig. 4j, k). More active growth sites can be provided for ACF felts as substrates by TiO2 via ALD, which is beneficial to the coating of ZIF-8.

Figure 4
figure 4

SEM images and EDS spectra of the adsorbents: ac ACF felts, df ALD-ACF felts, gi ZIF-8@ACF felts, jl ZIF-8@ALD-ACF felts

Results of the EDS analyses conducted to determine the chemical composition of ACF felts, ALD-ACF felts, ZIF-8@ACF felts, and ZIF-8@ALD-ACF felts are illustrated in Fig. 4c, f, i, l. Only carbon, oxygen, and platinum were detected in the spectra of the ACF felts. The presence of platinum can be attributed to the coating layer used for the EDS measurement, while the presence of carbon and oxygen can be attributed to the ACF felts. After the ALD processing, elements such as carbon, oxygen, and platinum were found in the EDS spectra. No other elements, except titanium, were found in the EDS spectra, hence confirming that Ti is present on the surfaces of ALD-ACF felts and ZIF-8@ALD-ACF felts. Meanwhile, after the hydrothermal reaction, in the ZIF-8@ACF felts and ZIF-8@ALD-ACF felts samples, zinc element was found in the EDS spectra, indicating that ZIF-8 crystalline film was coated on the ACF felts and ALD-ACF felts.

Figure 5a shows the FT-IR spectra of the adsorbents, ZIF-8@ACF felts, and ZIF-8@ALD-ACF felts; nearly all the FT-IR bands are consistent with those of the previously reported ZIF-8. The bands at 2916–3170 cm−1 can be attributed to the aromatic and aliphatic C-H stretch of the imidazole. C=N stretching could be observed at 1590 cm−1. The imidazole ring out-of-plane bending vibrations result in absorption bands below 800 cm−1, such as peaks at 680, 745 cm−1, while bands due to in-plane bending vibrations can be observed in the range of 900–1350 cm−1, such as peaks at 1310 and 1110 cm−1. The bands at 1350–1500 cm−1 are associated with the entire imidazole stretching, such as a peak at 1432 cm−1 due to the effects of imidazole ring stretching or bending [14, 34, 35]. Figure 5b shows XRD patterns of the ACF felts, ALD-ACF felts, ZIF-8@ACF felts, ZIF-8@ALD-ACF felts, and ZIF-8 nanocrystals. As shown in Fig. 5b, the ACF felts exhibited characteristic peaks at 2θ = 24.5° and 2θ = 3.5°, indicating the coexistence of ACF felts I and ACF felts II structures. The peaks at 2θ = 24.5° and 2θ = 43.5° were also observed in the XRD patterns of ALD-ACF felts subjected to 1000 ALD cycles, but the intensity of the peaks was not as high as those for pure ACF felts, indicating that the amount of ACF felts I crystalline structure in the ALD-ACF felts was less than the amount in the ACF felts. It should be noted that there are no typical diffraction peaks for the rutile and/or anatase TiO2 structures on the ALD 1000 cycles-ACF felts. However, individual TiO2 replica exhibited an anatase structure with preferred (101) orientation, indicating that the ALD coating on the silk fabrics was TiO2 and that the crystal structure was an amorphous structure [33]. The ZIF-8@ACF felts and ZIF-8@ALD-ACF felts peaks at 2θ = 7.3°, 10.4°, 12.7°, 14.7°, 16.4°, and 17.9° were associated with characteristic peaks of ZIF-8 nanocrystals, indicating the abundant existence of ZIF-8 nanocrystals in the network of ZIF-8@ACF felts and ZIF-8@ALD-ACF felts.

Figure 5
figure 5

a FT-IR spectra of the adsorbents: ACF felts, ALD-ACF felts, ZIF-8@ACF felts, and ZIF-8@ALD-ACF felts. b XRD patterns of the ACF felts, ALD-ACF felts, ZIF-8@ACF felts, ZIF-8@ALD-ACF felts, and ZIF-8 nanocrystals. c Possible mechanisms (I) coordination interactions, (II) electrostatic interactions, for the growth of ZIF-8 nanocrystals on the surface of ACF felts or ALD-ACF felts

The content of ZIF-8 coated on the ACF or ALD-ACF felts was determined using the weighing method. The detailed data are shown in Table 1. The possible mechanisms for the growth of ZIF-8 nanocrystals on the surface of ACF felts and ALD-ACF felts are shown in Fig. 5c. The growth of ZIF-8 on the surface of fibers can be explained by two mechanisms: coordination interactions and electrostatic interactions. As shown in Fig. 5c I, after the addition of Zn2+ in the ACF felts or ALD-ACF felts, the Zn2+ ions interact with the -O or -OH groups existing on ACF felts or ALD-ACF felts surface by coordination. The bonded Zn2+ facilitates the nucleation of ZIF-8, thus leading to the immobilization of the generated ZIF-8 nanocrystals on the surface of the ACF felts or ALD-ACF felts [36,37,38]. In addition, as shown in Fig. 5c II, the surface of the ACF felts or ALD-ACF felts is electronegative in aqueous solutions. Once the Zn2+ sites for 2-methylimidazole molecules, finally resulting in the generated ZIF-8 nanocrystals were attached on the surface of ACF or ALD-ACF felts [33, 39]. Due to the TiO2 coated on the surface of the ACF felts, the coordination sites and charge numbers are greater than those of ACF felts. This is propitious to the growth of ZIF-8 nanocrystals.

Table 1 The mass of ZIF-8 coated on different samples

The porous features and Brunauer–Emmett–Teller (BET) analysis of the ZIF-8 nanocrystals, ZIF-8@ACF, and ZIF-8@ALD-ACF felts were investigated using nitrogen isothermal adsorption/desorption measurements. In Fig. 6, ZIF-8 shows a type-II isotherm, whereas the isotherms of ZIF-8@ACF and ZIF-8@ALD-ACF felts have the type-III shape with the H3 hysteresis loop (relative pressure ranging from 0.5 to 0.98; Fig. 6a), indicating both the micropore and mesopore structure of ZIF-8@ACF and ZIF-8@ALD-ACF felts. The corresponding specific surface areas of ZIF-8 nanocrystals, ZIF-8@ACF, and ZIF-8@ALD-ACF felts were determined to be 1278.75, 792.18, and 868.51 m2 g−1, respectively. The specific surface area of ZIF-8@ALD-ACF felts was found to be greater than that of the ZIF-8@ACF felts, which is favorable for the diffusion of HCHO molecules; this is also beneficial for the photocatalytic reaction by TiO2 thin film [30, 32, 40]. The pore width distribution in Fig. 6b also indicates that more micro-/mesopores exist in ZIF-8@ALD-ACF felts, which complies with both the total pore volume and surface area of pores as shown in Table 2.

Figure 6
figure 6

a Nitrogen adsorption–desorption isotherms and b pore size distributions of ZIF-8, ZIF-8@ACF, and ZIF-8@ALD-ACF felts. P the gas-phase pressure when adsorption equilibrium was achieved; P0 the saturated vapor pressure; V the volume; and W the width

Table 2 Porous structure of the samples evaluated by N2 adsorption

HCHO adsorption by the ACF felts, ALD-ACF felts, ZIF-8@ ACF felts, and ZIF-8@ ALD-ACF felts without UV light

The effect of initial HCHO concentration on the removal percentage was conducted with different initial concentrations (high HCHO concentration: 100 mg m−3 and low HCHO concentration: 10 mg m−3) in the test chamber. The amount of adsorbent was fixed and exposed to high HCHO concentration (100 mg m−3) in the test chamber for 2 h, with the data read at minute intervals. The removal efficiency of HCHO was calculated using Eq. 1. The adsorption capacity was evaluated using Eq. 2. The adsorption test for low HCHO concentration was performed in a similar manner. A given amount of adsorbent was exposed to a low concentration of HCHO until the amount of HCHO was adsorbed to zero; the adsorption time was then compared.

$$ {\text{Removal}}\;{\text{efficiency}}\; ( {\text{\% )}} = \frac{{C_{0} - C_{t} }}{{C_{0} }} \times 100\% $$
(1)
$$ {\text{Adsorption}}\;{\text{capacity}},\;q_{t} ({\text{mg}}\;{\text{g}}^{ - 1} ) = \frac{{C_{0} - C_{t} }}{M} \times V $$
(2)

where C0 represents the initial concentration of HCHO in the test chamber (mg/m3) at time, t = 0; Ct represents the concentration of HCHO at time = t (1, 2, 3 until 120 min); qt represents the HCHO adsorption capacity at time = t (1, 2, 3 until 120 min); M represents the weight of the adsorbent (g), and V represents the volume of the test chamber (m3).

The removal percentage of HCHO by different adsorbents (ACF felts, ALD-ACF felts, ZIF-8@ACF felts, ZIF-8@ALD-ACF felts) at high HCHO concentrations is shown in Fig. 7a. The removal rate is rapid within the first 20 min; it then rises gradually until it reaches the adsorption equilibrium at 120 min. The maximum HCHO removal efficiency is 78.02% for ACF felts, 79.51% for ALD-ACF felts, 95.36% for ZIF-8@ACF felts, and 99.01% for ZIF-8@ALD-ACF felts (Fig. 7b). The removal efficiencies for HCHO by ACF felts and ALD-ACF felts are about the same. The TiO2 forms a very thin film on the surface of the ACF via ALD, which does not have an obvious effect on the micropore structures of the ACF for HCHO adsorption. The growth of ZIF-8 nanocrystals on ACF felts significantly improves the removal efficiency. Using ALD-ACF felts as substrate provides more growth sites, and the amount of ZIF-8 nanocrystals is greater than those of the ACF felts substrate. The nanoporous and molecular cage structures in ZIF-8 are favorable for HCHO adsorption. Therefore, using ZIF-8@ALD-ACF felts as adsorbent offers the highest removal efficiency (above 99%). The curves of adsorption capacity vs. time for ZIF-8@ACF felts and ZIF-8@ALD-ACF felts are shown in Fig. 7c, d. The maximum HCHO adsorption capacity is 14.812 and 15.408 mg g−1 for ZIF-8@ACF felts and ZIF-8@ALD-ACF felts using 120 min. They both suitably fit the pseudo-second-order kinetic model. The pseudo-second-order kinetic model is evaluated using Eq. 3.

$$ {\text{Adsorption}}\;{\text{capacity}},\;q_{t} ({\text{mg}}\;{\text{g}}^{ - 1} ) = \frac{{k_{2} q_{e}^{2} t}}{{1k_{2} q_{e} t}} $$
(3)

where k2 represents the pseudo-secondary adsorption rate constant and qe represents the equilibrium adsorption capacity. In Fig. 7c, the fitting equation is given by \( q_{t} = \frac{{0.00804 \times 15.838^{2} \times t}}{1 + 0.00804 \times 15.838 \times t} \) (R2 = 0.999), and in Fig. 7d, \( q_{t} = \frac{{0.00829 \times 16.397^{2} \times t}}{1 + 0.00829 \times 16.397 \times t} \) (R2 = 0.999).

Figure 7
figure 7

a Percentage of HCHO removal at high concentration using different adsorbents, b column diagram of the adsorption efficiency, c adsorption capacity of ZIF-8@ACF felts and the pseudo-second-order kinetic model, d adsorption capacity of ZIF-8@ALD-ACF felts and the pseudo-second-order kinetic model

The percentage of HCHO removal using different adsorbents (ACF felts, ALD-ACF felts, ZIF-8@ACF felts, ZIF-8@ALD-ACF felts) at low HCHO concentration (10 mg/m3) is also studied. As shown in Fig. 8, the four adsorbents can all remove HCHO completely from the test chamber. ZIF-8@ALD-ACF felts have a rapid rate of HCHO removal at low concentration, leading to full adsorption of the HCHO in less than 8 min. ZIF-8@ACF felts come second, taking 13 min to ensure full adsorption of the HCHO. The slowest are untreated ACF felts and ALD-ACF felts, which take 16 min. The reason is the same as the above.

Figure 8
figure 8

HCHO removal at low concentration using different adsorbents a and column diagram of their adsorption time b

HCHO removal by the ACF felts, ALD-ACF felts, ZIF-8@ ACF felts, and ZIF-8@ ALD-ACF felts under UV light

The percentage of HCHO removal by adsorbents (ACF felts, ALD-ACF felts, ZIF-8@ACF felts, ZIF-8@ALD-ACF felts) at high HCHO concentrations under UV light is shown in Fig. 9a. Figure 9b shows a column diagram of their adsorption efficiencies. It can be observed from the figure that ZIF-8@ALD-ACF felts exhibit the highest removal efficiency at high HCHO concentration, achieving 100% removal at 110 min. ZIF-8@ACF felts come in second place (96.88%), while ALD-ACF felts come third (89.02%). The worst performance comes from untreated ACF felts that achieve only 78.01%.

Figure 9
figure 9

a Percentage of HCHO removal at high concentration using different adsorbents under UV light within 110 min, b column diagram of their adsorption efficiencies, c adsorption capacity of ZIF-8@ACF felts and the pseudo-second-order kinetic model under UV light, (d) adsorption capacity of ZIF-8@ALD-ACF felts and the pseudo-second-order kinetic model under UV light

The efficiencies of removal of ACF felts and ZIF-8@ACF felts are nearly no change with or without UV light. The efficiencies of removal of ALD-ACF felts and ZIF-8@ALD-ACF felts still clearly increase under the condition that the adsorption time is shortened by 10 min. This is mainly due to the photocatalysis of the TiO2. Adsorbents without TiO2 adsorb HCHO molecules due to their micro-/nanopores and large specific surface area. In contrast, adsorbents containing TiO2 capture first HCHO molecule, and then decompose it to CO2 and H2O using TiO2 under UV light. The process can also be observed from the curve of ZIF-8@ALD-ACF felts in Fig. 9a. A turning point can be clearly observed at 70 min. Before 70 min, the ZIF-8@ACF felts and ZIF-8@ALD-ACF felts exhibit similar adsorption behavior under UV light. From 70 min, photocatalysis of the TiO2 is dominant for HCHO decomposition. The amount of HCHO in the test chamber was completely removed.

The adsorption capacity of ZIF-8@ACF felts and ZIF-8@ALD-ACF felts under UV light is shown in Figs. 9c, d. The maximum HCHO adsorption capacity is 15.056 and 15.559 mg g−1 for ZIF-8@ACF felts and ZIF-8@ALD-ACF felts, respectively. In Fig. 9c, the curve of ZIF-8@ACF felts is consistent with the pseudo-second-order kinetic model. The fitting equation is given by \( q_{t} = \frac{{0.00475 \times 16.891^{2} \times t}}{1 + 0.00475 \times 16.891 \times t} \) (R2 = 0.999). In Fig. 9d, due to the turning point, the curve does not fit the pseudo-second-order kinetic model very well; hence, \( q_{t} = \frac{{0.00523 \times 16.584^{2} \times t}}{1 + 0.00523 \times 16.584 \times t} \) (R2 = 0.992).

The percentage of HCHO removal for adsorbents (ACF felts, ALD-ACF felts, ZIF-8@ACF felts, ZIF-8@ALD-ACF felts) at low HCHO concentrations under UV light is shown in Fig. 10. The figure shows that four different adsorbents can all remove HCHO completely from the test chamber. ZIF-8@ALD-ACF felts exhibit the fastest rate of removal of HCHO under UV light, achieving total removal in less than 6 min. ZIF-8@ACF felts as adsorbent come second, achieving total removal in 13 min. ALD-ACF felts come third at 14 min, while the slowest are untreated ACF felts that take 16 min. Compared to the adsorption conditions without UV light irradiation, there are also no influences on ACF felts and ZIF-8@ACF felts. Due to the photocatalysis of TiO2 under UV light, the adsorption times were shortened and the adsorption efficiencies of ZIF-8@ALD-ACF felts and ALD-ACF felts that both contain TiO2 thin films via ALD were significantly improved.

Figure 10
figure 10

Removal percentage at low HCHO concentration for different adsorbents under UV light (a) and column diagram of their adsorption time (b)

Figure 11 shows the mechanism of HCHO removal. The surface of the ACF is smooth and inert, making the growth of ZIF-8 nanocrystals on the fibers difficult. As can be seen from the SEM images and local magnification, the ACF surface became rough with sparse ZIF-8 nanocrystals. When the ACF was coated in advance with TiO2 thin film via ALD, a dense and uniform growth of nanocrystals on the ACF was observed. ALD makes the thickness of TiO2 thin film controllable at the atomic level. The speed of the reaction between ACF and TiO2 is excellent and does not affect the structures and properties of the ACF substrates. In addition, the TiO2 can provide more binding sites for the growth of ZIF-8. The nanopores and cage structures of ZIF-8 are propitious for adsorbing and fixing HCHO molecules. Due to the synergistic reaction of ZIF-8 and ACF felts, the ZIF-8@ACF felts and ZIF-8@ALD-ACF felts both achieve high HCHO adsorption efficiency (95.36% and 99.01%) without UV light. A large number of HCHO molecules are first captured by the composite materials on the surface of fibers and ZIF-8, in the nanopores and molecular cages, and in the micropores formed after compounding. In particular, the nanopores exhibit strong van der Waals forces that can effectively adsorb very small HCHO molecules and prevent desorption. When the adsorption equilibrium is reached, a very small amount of HCHO molecules are still left in the test chamber (the upper part of Fig. 11). Under UV light, the HCHO molecules are first captured by ZIF-8@ALD-ACF felts. Then, the HCHO molecules have sufficient time to contact the TiO2 thin film and decompose to CO2 and H2O [41,42,43,44,45]. They can be completely removed even within several minutes. The capture–sufficient contact–decomposition process employed in this study is very effective and practical for HCHO removal. The method can also effectively avoid secondary pollution and has wide application prospects.

Figure 11
figure 11

Mechanism of HCHO removal for ZIF-8@ACF felts and ZIF-8@ALD-ACF felts under UV light

Conclusion

In this study, we successfully prepared novel ZIF-8@ALD-ACF felts composite materials. These ZIF-8@ALD-ACF felts can be used as a highly efficient adsorbent for HCHO. Using TiO2-coated ACF felts via ALD as substrates can provide more growth sites for ZIF-8 nanocrystals and HCHO photocatalytic degradation. The adsorption and photocatalytic processes can be mainly described as the capture–sufficient contact–decomposition process. The felts achieve 100% removal of HCHO at high concentration within 110 min and 100% removal at low concentration within 6 min under UV light. Providing a sufficient contact time between HCHO and TiO2 thin film, HCHO captured and fixed in the micro-/nanopores of the ZIF-8@ALD-ACF felts is decomposed into CO2 and H2O. Hence, the process can effectively prevent secondary pollution. The ZIF-8@ALD-ACF felts composite materials hold important practical applications for HCHO removal.