Synthesis and Adsorption Performance of a Hierarchical Micro-Mesoporous Carbon for Toluene Removal under Ambient Conditions

Ordered mesoporous carbons (OMCs) were synthesized in this study through a soft template method and then activated by employing different mass ratios of KOH/OMCs to obtain KOH-activated ordered mesoporous carbons (KOMCs) with hierarchical pore structures. To verify the adsorption capacity, the KOMCs have been subjected to toluene emission-reduction experiments. The KOMCs were characterized by TEM, XRD, N2 adsorption-desorption isotherms, and Raman spectroscopy. The pore structure of OMCs was found to be effectively optimized by the activation with KOH, with the BET-area and total pore volume values reaching as high as 2661 m2 g−1 and 2.14 cm3 g−1 respectively. Then, the dynamic adsorption capacity of toluene on KOMCs was investigated via breakthrough curves, which can be well described by the Yoon and Nelson (Y-N) model. The dynamic adsorption capacities of toluene exhibit the following order: OMC < KOMC-1 < KOMC-5 < KOMC-3. The sample activated by KOH/OMC with a mass ratio of 3:1 (KOMC-3) demonstrated the highest toluene adsorption capacity of 355.67 mg g−1, three times higher in comparison with the untreated carbon (104.61 mg g−1). The modified hierarchical porous carbons also exhibited good recyclability. The KOMCs with rich pore structure, high toluene adsorption capacity, and superior reusability thus display a huge potential for volatile organic compound (VOC) elimination.


Introduction
With the rapid development of industry air pollution has become a significant problem in the development of human society. Volatile organic compounds (VOCs), as the primary pollutants, have attracted wide attention from researchers in recent years. Acid rain, photochemical pollution, urban haze, and other pollution effects have a direct relationship with VOCs. Even under low concentrations, long-term exposure to VOCs can still seriously threaten human health. Therefore, eliminating VOCs is crucial to human health and the environment [1].
New technologies that contribute to emission reduction are continually being developed. Adsorption [2,3], catalytic combustion [4], condensation [5,6], photocatalytic oxidation [7], biodegradation methods [8,9], and others [10] are among the methods used to remove VOCs, of which adsorption is the most widely used method due to its better removal capacity and lower energy consumption with almost no toxicity [1,11]. Since adsorbents are a crucial part of adsorption

Synthesis of OMCs
OMCs were synthesized by a solvent evaporation-induced self-assembly method using the soft template method. First, 3.2 g F127 and 2.0 g 0.2 M HCl were dissolved in 6 g ethanol, before being mixed at 40 • C for 1 h. Next, 4.16 g TEOS and 10 g 20% phenolic resin solution were added to the above mixture and stirred continuously for 2 h. The phenolic resin was produced according to the method reported by the Cheng group [18]. The mixed solution was transferred into Petri dishes and kept at room temperature for 5-8 h to evaporate the ethanol. Subsequently, the product was heated at 100 • C for 24 h. The as-made polymer was carbonized at 800 • C for 2 h in a horizontal tubular furnace (Shanghai, China) under N 2 atmosphere, with the temperature gradient of 1 • C min −1 and N 2 flow rate of 100 mL min −1 . The obtained products were ground with a mortar and separated through mesh sizes of 40-60. The obtained carbon-silicon composite material was kept at 60 • C oven for 24 h in 4 M NaOH to remove silica. Then the OMC products were obtained through filtering, washing, and drying.

Synthesis of KOMCs
Initially, 0.5 g of OMC was mixed with KOH at different mass ratios (KOH/OMC = 1:1, 3:1, and 5:1) and the mixtures were immersed for 3 h in 10 mL of H 2 O/EtOH (1:1) solution at room temperature. The crucible was then placed in an oven at 80 • C to dry the mixture. The dried sample was calcined at 800 • C for 2 h in a horizontal tubular furnace under an N 2 atmosphere, with the temperature gradient of 5 • C min −1 and N 2 flow rate of 100 mL min −1 . The KOMCs products were obtained by filtration, washing to neutrality, and drying overnight at 105 • C. The sample was named as KOMC-x, where x implied the mass ratio of KOH/OMC.

Sample Characterization
A JEM-200CX transmission electron microscope (TEM, JEOL, Tokyo, Japan) was used to observe the microscopic morphology and structure of all samples. Before doing TEM, first, the sample was dispersed in an ethanol solution and sonicated for 30 min, and then a capillary tube was used to drop the solution uniformly on a copper mesh, and the test was start after the ethanol on the copper mesh had evaporated. The powder X-ray diffraction (XRD) data was analyzed on a D/MAX-2500 instrument (Rigaku, Tokyo, Japan) with Cu-Kα radiation (40 kV, 40 mA). The degree of graphitization and disorder in the carbon materials were measured employing Raman spectroscopy (JY-HR800, Horiba Jobin Yvon, Paris, France) using a laser with a wavelength of 532 nm and power of 5 mW. N 2 adsorption-desorption isotherms were recorded using a Nova 2200e instrument (Quantachrome, FL, USA) at −196 • C. Before testing, the samples were degassed under a vacuum of 200 • C to remove pre-adsorbed impurities. The surface areas were calculated by way of the Brunauer-Emmett-Teller (BET) method from the range of 0.05-0.2 relative pressure (P/P 0 ). The single point adsorption total pore volumes (V t ) were measured from the adsorption amount when the P/P 0 value was 0.99. The mesopore size distribution curves were from the desorption isotherms using the Barrett-Joyner-Halenda (BJH) method. The micropore volume (V mic ) and micropore surface area (S mic ) were calculated using the t-plot method, and micropore size distribution curves were determined through the Horvath-Kawazoe (HK) method.

Dynamic Adsorption Measurements
Dynamic adsorption was performed by methods previously reported by our research group [12]. To remove the physically adsorbed water molecules and small organic impurities in the sample, vacuum drying was carried out at 105 • C for 12 h before the adsorption test. Then 0.05 g of the sieved sample was placed in a fixed bed reactor with a length of 10 cm and a diameter of 0.6 cm (as shown in Figure 1). The catheters for the circulation of toluene gas was kept at a constant temperature of 25 • C with a thermal insulation belt and pressure was normal atmospheric pressure. High purity nitrogen was used as the diluent gas and toluene bubbling gas flows to adjust the flow rates to 50 mL min −1 and 10 mL min −1 , to maintain a total flow rate of 60 mL min −1 (with a toluene concentration of 2.2 mg L −1 ). Before each test, we did a blank experiment without adsorbent filling. Toluene gas concentration without adding an adsorbent was tested until the concentration reached the requirement for the experiment. It was stable for 2 h, and then adsorbent was filled for testing. To determine the adsorption capacity of the adsorbent, the concentration change before and after the adsorption measurement was performed using a GC equipped with a flame ionization detector (FID). In our experiments, different concentrations of toluene gas were injected into the GC detection port by manual injection, and the corresponding peak area was obtained by computer analysis. The same concentration of toluene gas was repeated five times, and the corresponding peak area was averaged. The above operation with different concentrations of toluene was repeated, and the peak area corresponding to the toluene gas with different concentrations was finally obtained. a standard curve was obtained by analyzing the correspondence between the peak area and the toluene concentration. The inlet concentration was thus obtained by substituting the stable peak area at the GC end into the standard curve formula. The equilibrium dynamic adsorption capacity (q, mg g −1 ; q', mmol g −1 ) of the OMCs were calculated according to the breakthrough curve, using the following calculation method: where Q (mL min −1 ) is the intake gas flow rate of toluene and high purity nitrogen, m (g) is the mass of the adsorbent, M (g mol −1 ) is the molar mass of toluene, C 0 (mg L −1 ) is the input concentration of toluene, and C t (mg L −1 ) is the output concentration of toluene at adsorption equilibrium time t (min).
adsorption measurement was performed using a GC equipped with a flame ionization detector (FID). In our experiments, different concentrations of toluene gas were injected into the GC detection port by manual injection, and the corresponding peak area was obtained by computer analysis. The same concentration of toluene gas was repeated five times, and the corresponding peak area was averaged. The above operation with different concentrations of toluene was repeated, and the peak area corresponding to the toluene gas with different concentrations was finally obtained. A standard curve was obtained by analyzing the correspondence between the peak area and the toluene concentration. The inlet concentration was thus obtained by substituting the stable peak area at the GC end into the standard curve formula. The equilibrium dynamic adsorption capacity (q, mg g −1 ; q', mmol g −1 ) of the OMCs were calculated according to the breakthrough curve, using the following calculation method: where Q (mL min −1 ) is the intake gas flow rate of toluene and high purity nitrogen, m (g) is the mass of the adsorbent, M (g mol −1 ) is the molar mass of toluene, C0 (mg L −1 ) is the input concentration of toluene, and Ct (mg L −1 ) is the output concentration of toluene at adsorption equilibrium time t (min).
Adsorption curves fits were performed using the Yoon and Nelson (Y-N) model: where t (min) is the adsorption equilibrium time, (min) is the time when Ct/C0 = 0.5 and k (min -1 ) is the rate constant that reflects diffusion and mass transfer.  Adsorption curves fits were performed using the Yoon and Nelson (Y-N) model:

Results and Discussion
where t (min) is the adsorption equilibrium time, τ (min) is the time when C t /C 0 = 0.5 and k (min −1 ) is the rate constant that reflects diffusion and mass transfer.

Characteristics of KOMCs
The ordered mesostructure of the prepared KOMC samples was observed by transmission electron microscopy (TEM) and low angle XRD patterns. Figure 2a,b display TEM images of OMC and KOMC-3. As shown in Figure 2a, OMC exhibits ordered wormhole-like pore structure [30], which may be the result of an inverse replica of the F127 soft template. After KOH activation, it remains as uniform mesopores with a wormhole-like pore structure, but the ordered pore arrangement of KOMC-3 decreases slightly. The low-angle XRD patterns of OMC and KOMC-3 are presented in Figure 3. a diffraction peak at around 0.9 was observed in OMC and KOMC-3 samples, confirming the ordered mesoporous structure. However, the peak intensity decreased after KOH activation, indicating a decline in the ordered mesoporous structure, consistent with the results of Mitome et al. [31].

Characteristics of KOMCs
The ordered mesostructure of the prepared KOMC samples was observed by transmission electron microscopy (TEM) and low angle XRD patterns. Figure 2a,b display TEM images of OMC and KOMC-3. As shown in Figure 2a, OMC exhibits ordered wormhole-like pore structure [30], which may be the result of an inverse replica of the F127 soft template. After KOH activation, it remains as uniform mesopores with a wormhole-like pore structure, but the ordered pore arrangement of KOMC-3 decreases slightly. The low-angle XRD patterns of OMC and KOMC-3 are presented in Figure 3. A diffraction peak at around 0.9 was observed in OMC and KOMC-3 samples, confirming the ordered mesoporous structure. However, the peak intensity decreased after KOH activation, indicating a decline in the ordered mesoporous structure, consistent with the results of Mitome et al. [31].    Figure 4 depicts the Raman spectra of OMC and KOMCs. All four samples displayed two prominent peaks at Raman shifts of ∼1340 and ∼1596 cm −1 , which corresponded to the D and G bands of the carbon structure. The D band manifests the disorder and defective graphitic structures of the carbon materials, while the G band indicates the feature of graphitic structures [32]. The extent of the disorder can be revealed by employing the intensity ratio of the D band and the G band (ID/IG) [33]. The higher the ID/IG ratio, the higher the degrees of disorder. The ID/IG ratio for OMC, KOMC-1, KOMC-3 and KOMC-5 were 1.20, 1.23, 1.46 and 1.48, respectively. These results indicate that the

Characteristics of KOMCs
The ordered mesostructure of the prepared KOMC samples was observed by transmission electron microscopy (TEM) and low angle XRD patterns. Figure 2a,b display TEM images of OMC and KOMC-3. As shown in Figure 2a, OMC exhibits ordered wormhole-like pore structure [30], which may be the result of an inverse replica of the F127 soft template. After KOH activation, it remains as uniform mesopores with a wormhole-like pore structure, but the ordered pore arrangement of KOMC-3 decreases slightly. The low-angle XRD patterns of OMC and KOMC-3 are presented in Figure 3. A diffraction peak at around 0.9 was observed in OMC and KOMC-3 samples, confirming the ordered mesoporous structure. However, the peak intensity decreased after KOH activation, indicating a decline in the ordered mesoporous structure, consistent with the results of Mitome et al. [31].   Figure 4 depicts the Raman spectra of OMC and KOMCs. All four samples displayed two prominent peaks at Raman shifts of ∼1340 and ∼1596 cm −1 , which corresponded to the D and G bands of the carbon structure. The D band manifests the disorder and defective graphitic structures of the carbon materials, while the G band indicates the feature of graphitic structures [32]. The extent of the disorder can be revealed by employing the intensity ratio of the D band and the G band (ID/IG) [33]. The higher the ID/IG ratio, the higher the degrees of disorder. The ID/IG ratio for OMC, KOMC-1, KOMC-3 and KOMC-5 were 1.20, 1.23, 1.46 and 1.48, respectively. These results indicate that the  Figure 4 depicts the Raman spectra of OMC and KOMCs. All four samples displayed two prominent peaks at Raman shifts of ∼1340 and ∼1596 cm −1 , which corresponded to the D and G bands of the carbon structure. The D band manifests the disorder and defective graphitic structures of the carbon materials, while the G band indicates the feature of graphitic structures [32]. The extent of the disorder can be revealed by employing the intensity ratio of the D band and the G band (I D /I G ) [33]. The higher the I D /I G ratio, the higher the degrees of disorder. The I D /I G ratio for OMC, KOMC-1, KOMC-3 and KOMC-5 were 1.20, 1.23, 1.46 and 1.48, respectively. These results indicate that the degree of defective graphitic structures of OMC improved with the increase of activation mass ratio, which is in agreement with the TEM and low-angle XRD results. Therefore, Raman spectroscopy shows that the amount of KOH has a certain effect on the degree of pore etch of carbon materials, which may affect the BET-area of carbon materials. degree of defective graphitic structures of OMC improved with the increase of activation mass ratio, which is in agreement with the TEM and low-angle XRD results. Therefore, Raman spectroscopy shows that the amount of KOH has a certain effect on the degree of pore etch of carbon materials, which may affect the BET-area of carbon materials. The OMC samples before and after activation with KOH were distinguished by wide-angle XRD, as shown in Figure 5. The wide-angle XRD pattern of OMC showed two typical peaks at 2-theta of 23.48 and 43.26, corresponding to (002) and (100) planes of graphitic carbon, respectively [22]. The weak (002) diffraction peak intensity implied the low degree of graphitization of the carbon material [34], signifying that the activated process had reduced the degree of graphitization. Nondistinct (002) diffraction peaks indicate the amorphous feature of sample KOMC-3 and KOMC-5. The disappearance of the (002) diffraction peaks of KOMC-3 and KOMC-5 may be due to the deep damage of the graphite layer arrangement during the activation process with the increase of the amount of KOH [35,36]. KOH activation improves the porosity on the premise of reducing the ordering of OMC, which enhances the adsorption performance to a certain extent. It can also be seen from Figure 5 that KOMC-1 and KOMC-3 have weaker peaks. This may be because the potassium compound or other Impurities were not completely washed during the washing process. Analysis results based on Raman spectra and wide-angle XRD patterns were consistent with the amorphous structure observed by TEM and low angle XRD patterns.   The OMC samples before and after activation with KOH were distinguished by wide-angle XRD, as shown in Figure 5. The wide-angle XRD pattern of OMC showed two typical peaks at 2-theta of 23.48 and 43.26, corresponding to (002) and (100) planes of graphitic carbon, respectively [22]. The weak (002) diffraction peak intensity implied the low degree of graphitization of the carbon material [34], signifying that the activated process had reduced the degree of graphitization. Nondistinct (002) diffraction peaks indicate the amorphous feature of sample KOMC-3 and KOMC-5. The disappearance of the (002) diffraction peaks of KOMC-3 and KOMC-5 may be due to the deep damage of the graphite layer arrangement during the activation process with the increase of the amount of KOH [35,36]. KOH activation improves the porosity on the premise of reducing the ordering of OMC, which enhances the adsorption performance to a certain extent. It can also be seen from Figure 5 that KOMC-1 and KOMC-3 have weaker peaks. This may be because the potassium compound or other Impurities were not completely washed during the washing process. Analysis results based on Raman spectra and wide-angle XRD patterns were consistent with the amorphous structure observed by TEM and low angle XRD patterns. degree of defective graphitic structures of OMC improved with the increase of activation mass ratio, which is in agreement with the TEM and low-angle XRD results. Therefore, Raman spectroscopy shows that the amount of KOH has a certain effect on the degree of pore etch of carbon materials, which may affect the BET-area of carbon materials. The OMC samples before and after activation with KOH were distinguished by wide-angle XRD, as shown in Figure 5. The wide-angle XRD pattern of OMC showed two typical peaks at 2-theta of 23.48 and 43.26, corresponding to (002) and (100) planes of graphitic carbon, respectively [22]. The weak (002) diffraction peak intensity implied the low degree of graphitization of the carbon material [34], signifying that the activated process had reduced the degree of graphitization. Nondistinct (002) diffraction peaks indicate the amorphous feature of sample KOMC-3 and KOMC-5. The disappearance of the (002) diffraction peaks of KOMC-3 and KOMC-5 may be due to the deep damage of the graphite layer arrangement during the activation process with the increase of the amount of KOH [35,36]. KOH activation improves the porosity on the premise of reducing the ordering of OMC, which enhances the adsorption performance to a certain extent. It can also be seen from Figure 5 that KOMC-1 and KOMC-3 have weaker peaks. This may be because the potassium compound or other Impurities were not completely washed during the washing process. Analysis results based on Raman spectra and wide-angle XRD patterns were consistent with the amorphous structure observed by TEM and low angle XRD patterns.     Table 1. The adsorption-desorption isotherms of all samples equal to the mixed type I and type IV definition in the IUPAC classification. There is an H1 type hysteresis loop in the P/P 0 range of 0.4-0.8, indicating that all samples have the micro-mesoporous structure [37,38]. The log scale isotherms show the micropore filling process between the different samples on the lowest relative pressure, indicating that micropores were present in the prepared samples. The BET-area and total pore volume increased with the increase of the KOH/OMC ratio (Table 1). For instance, the pure OMC BET-area was 1343 m 2 g −1 , while that of KOMC-1 and KOMC-5 was 1792 m 2 g −1 and 2661 m 2 g −1 , respectively. Moreover, total pore volume increased from the original 1.24 cm 3 g −1 OMC to 1.32 cm 3 g −1 in the KOMC-1 and 2.14 cm 3 g −1 in the KOMC-5. This means that well-developed pores were generated when the amount of KOH was appropriately increased.
C. The pore structural properties are listed in Table 1. The adsorption-desorption isotherms of ples equal to the mixed type I and type IV definition in the IUPAC classification. There is an pe hysteresis loop in the P/P0 range of 0.4-0.8, indicating that all samples have the -mesoporous structure [37,38]. The log scale isotherms show the micropore filling process en the different samples on the lowest relative pressure, indicating that micropores were nt in the prepared samples. The BET-area and total pore volume increased with the increase of OH/OMC ratio (Table 1). For instance, the pure OMC BET-area was 1343 m 2 g −1 , while that of C-1 and KOMC-5 was 1792 m 2 g −1 and 2661 m 2 g −1 , respectively. Moreover, total pore volume sed from the original 1.24 cm 3 g −1 OMC to 1.32 cm 3 g −1 in the KOMC-1 and 2.14 cm 3 g −1 in the C-5. This means that well-developed pores were generated when the amount of KOH was priately increased.  Micro-mesopore pore size distribution curves of OMC and KOMC-x, shown in Figur were analyzed using the HK and BJH methods, respectively. The BJH mesopore size distrib showed that the mesopores primarily lay within the rangee of 3.5-5 nm for the four prepared Still, the pore diameter of the mesopores was significantly reduced after activation. This may etching effect of the potassium, as mentioned earlier, metal on the carbon material. It can found from the HK micropore size distribution that the micropores were mainly distributed range of 0.6 and 0.9 nm, which were considered to be the optimum pore size for adsorbing t [39]. The increase of micropore volume and micropore surface area of the KOMCs indicate tha activation influenced the pore structures. The DFT method-determined pore size distribu  Micro-mesopore pore size distribution curves of OMC and KOMC-x, shown in Figure 6c,d, were analyzed using the HK and BJH methods, respectively. The BJH mesopore size distributions showed that the mesopores primarily lay within the rangee of 3.5-5 nm for the four prepared OMCs. Still, the pore diameter of the mesopores was significantly reduced after activation. This may be the etching effect of the potassium, as mentioned earlier, metal on the carbon material. It can also be found from the HK micropore size distribution that the micropores were mainly distributed in the range of 0.6 and 0.9 nm, which were considered to be the optimum pore size for adsorbing toluene [39]. The increase of micropore volume and micropore surface area of the KOMCs indicate that KOH activation influenced the pore structures. The DFT method-determined pore size distribution is provided in Figure S1 of Supplementary Materials.

Dynamic Adsorption Performance of Toluene
Breakthrough measurements are recognized as an effective means of evaluating adsorbents [40]. The breakthrough time is the most crucial parameter, reflecting the adsorption capacity of an adsorbent [41]. In this paper, the breakthrough and saturation mean the ratio of toluene outlet to inlet concentration is greater than 10% and 90%, respectively. Breakthrough mode generally consists of two processes [42]. The breakthrough curve was a horizontal line in the initial stage. The toluene concentration of the gas outlet gradually increased after breakthrough, and then entered the second stage. The breakthrough curves with an error bar of OMC, KOMC-1, KOMC-3, and KOMC-5 are displayed in Figure 7, and corresponding fitting lines deriving from the modified Y-N model are shown in Figure 8. It can be seen that KOMC-3 showed the longest toluene breakthrough time (129 min) in the first stage of dynamic adsorption, followed by KOMC-5 (108 min) and KOMC-1 (81 min). It is clear that OMC exhibit the minimum breakthrough time (33 min) for toluene. The adsorption capacities of toluene decreased in the order of KOMC-3 (355.67 mg g −1 ) > KOMC-5 (286.76 mg g −1 ) > KOMC-1 (242.89 mg g −1 ) > OMC (104.61 mg g −1 ) ( Table 2). However, compared with OMC, KOMC-x (1, 3, 5) gradually increased with time in the second stage of the toluene breakthrough curve, which indicates that the increase in microporous structure will increase the resistance to mass transfer slightly. In contrast, the toluene breakthrough curve of OMC increased sharply in the second stage, which means that the diffusion resistance in OMC is smaller, and the mass transfer rate is faster during the adsorption process. The dynamic adsorption results show that KOMC-3 has excellent adsorption performance, its dynamic adsorption capacity is higher than OMC, and its mass transfer resistance is less than KOMC-5. Hu et al. used cotton stalks as carbon source and zinc chloride as an activator for chemical activation. The AC-Z dynamic adsorption capacity of the prepared sample was 258 mg g −1 [43]. From the above experimental results and Table 1, it is known that the specific surface area and pore volume of OMC were increased after activation, following which the adsorption capacity is also enhanced. However, van der Waals force is the main attraction of physical adsorption, which increases with the increase of specific surface area, so the adsorption capacity increases after activation [44]. The adsorption capacity was generally expected to increase as the specific surface area and pore volume increased. As can be seen from Table 1, the specific surface area and pore volume of KOMC-3 were smaller than those of KOMC-5, but the breakthrough time of KOMC-3 was larger. This means that the factors affecting adsorption consisted of more than a specific surface area and pore volume.

Dynamic Adsorption Performance of Toluene
Breakthrough measurements are recognized as an effective means of evaluating adsorbents [40]. The breakthrough time is the most crucial parameter, reflecting the adsorption capacity of an adsorbent [41]. In this paper, the breakthrough and saturation mean the ratio of toluene outlet to inlet concentration is greater than 10% and 90%, respectively. Breakthrough mode generally consists of two processes [42]. The breakthrough curve was a horizontal line in the initial stage. The toluene concentration of the gas outlet gradually increased after breakthrough, and then entered the second stage. The breakthrough curves with an error bar of OMC, KOMC-1, KOMC-3, and KOMC-5 are displayed in Figure 7, and corresponding fitting lines deriving from the modified Y-N model are shown in Figure 8. It can be seen that KOMC-3 showed the longest toluene breakthrough time (129 min) in the first stage of dynamic adsorption, followed by KOMC-5 (108 min) and KOMC-1 (81 min). It is clear that OMC exhibit the minimum breakthrough time (33 min) for toluene. The adsorption capacities of toluene decreased in the order of KOMC-3 (355.67 mg g −1 ) > KOMC-5 (286.76 mg g −1 ) > KOMC-1 (242.89 mg g −1 ) > OMC (104.61 mg g −1 ) ( Table 2). However, compared with OMC, KOMC-x (1, 3, 5) gradually increased with time in the second stage of the toluene breakthrough curve, which indicates that the increase in microporous structure will increase the resistance to mass transfer slightly. In contrast, the toluene breakthrough curve of OMC increased sharply in the second stage, which means that the diffusion resistance in OMC is smaller, and the mass transfer rate is faster during the adsorption process. The dynamic adsorption results show that KOMC-3 has excellent adsorption performance, its dynamic adsorption capacity is higher than OMC, and its mass transfer resistance is less than KOMC-5. Hu et al. used cotton stalks as carbon source and zinc chloride as an activator for chemical activation. The AC-Z dynamic adsorption capacity of the prepared sample was 258 mg g −1 [43]. From the above experimental results and Table 1, it is known that the specific surface area and pore volume of OMC were increased after activation, following which the adsorption capacity is also enhanced. However, van der Waals force is the main attraction of physical adsorption, which increases with the increase of specific surface area, so the adsorption capacity increases after activation [44]. The adsorption capacity was generally expected to increase as the specific surface area and pore volume increased. As can be seen from Table 1, the specific surface area and pore volume of KOMC-3 were smaller than those of KOMC-5, but the breakthrough time of KOMC-3 was larger. This means that the factors affecting adsorption consisted of more than a specific surface area and pore volume.    The molecular diameter of the adsorbate and the pore size of the adsorbent determine the physical adsorption capacity [39]. When the pore size of the adsorbent is much larger than the diameter of the adsorbate, the adsorption potential is fragile extremely faint, and the adsorbate cannot enter a pore having a size smaller than the size of the adsorbate. The molecular diameter of toluene is 0.67 nm [45], corresponding with the HK pore diameter distribution of all samples. Although KOMC-5 had the highest pore volume and specific surface area, the micropore volume and micropore specific surface area of KOMC-3 were larger than those of KOMC-5, which means that KOMC-3 had a richer microporous structure. Thus the adsorption capacity of KOMC-3 was better. Chiang et al. [46] found that microporous surface structure is the main factor of adsorption capacity. Lillo et al. [47] studied the adsorption behavior of activated carbon on low concentrations of benzene and toluene, and pointed out that the adsorption of activated carbon is mostly controlled and dominated by micropores. The adsorption amount of toluene and benzene increased following the increase of micropore volume of activated carbon, indicating that the adsorption effect of activated carbon mainly depends on the microporous structure. Therefore, the enhanced ability of KOMC-3 to adsorb toluene can be attributed to the synergistic effect of large specific surface area, pore volume, and the abundant microporous structure after activation.

Recyclability Studies
The recyclability and stability of adsorbent are much important for practical applications. To evaluate its reusability, the KOMC-3 was regenerated through the heating of the materials at 200 • C in a nitrogen gas flow for 120 min. The regenerated samples were then subjected to three times adsorption-desorption cycles, and the change in equilibrium adsorption capacity was observed. Figure 9 shows the change in the adsorption capacity of KOMC-3 for 4 adsorption cycles.
The recyclability and stability of adsorbent are much important for practical applications. To evaluate its reusability, the KOMC-3 was regenerated through the heating of the materials at 200 °C in a nitrogen gas flow for 120 min. The regenerated samples were then subjected to three times adsorption-desorption cycles, and the change in equilibrium adsorption capacity was observed. Figure 9 shows the change in the adsorption capacity of KOMC-3 for 4 adsorption cycles.   The first adsorption capacity of KOMC-3 was 355.67 mg g −1 , and then it was decreased by 5% after a round of regeneration. The reason for the decrease in the adsorption capacity may be due to the toluene not being completely desorbed during the regeneration of the material, occupying a certain adsorption site. With the successive adsorption-regeneration process, the recycling efficiency of regenerated KOMC-3 remained at approximately 90%. The good desorption and reuse efficiency ability of KOMC-3 can be attributed to the presence of hierarchical pore structures. This means that KOMC-3 has good adsorption properties and stability. Therefore, KOMC-3 has certain practical potential in VOC adsorption.

Conclusions
The paper presents a newly prepared material for VOC removal built after a review of existing studies and by optimizing the performance of OMCs in current pollutant treatment practices. a series of KOH-activated ordered mesoporous carbons were synthesized by using KOH as an activating agent with a soft template method. KOH activation enhanced the BET-area and the pore volume of initial material up to 2661 m 2 g −1 and 2.139 cm 3 g −1 , respectively. The dynamic adsorption capacities of toluene are in the following order: OMC < KOMC-1 < KOMC-5 < KOMC-3. Toluene adsorption capacities of KOMC-x samples are largely enhanced, with the highest reaching 355.67 mg g −1 by KOMC-3, three times that of OMCs without activation. The results suggest that the increase of specific surface area and pore volume after activation, as well as the microporous structure, contribute to the enhancement of toluene adsorption capacity. Moreover, the adsorption capacity of the KOMC-3 remains around 90% after being used for four times, indicating good adsorption performance and stability of KOMC-3. The study is to explore the improvement and optimization of OMCs for VOC emission control with particular emphasis on KOMCs preparation and future applications in air pollution treatment.