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Appl. Sci. 2018, 8(1), 81; https://doi.org/10.3390/app8010081
Supercritical Regeneration of an Activated Carbon Fiber Exhausted with Phenol
Dpto Química-Física, Facultad de Ciencias Química, Universidad de Salamanca, Plaza de la Merced s/n, 37008 Salamanca, Spain
Author to whom correspondence should be addressed.
Received: 27 November 2017 / Accepted: 13 December 2017 / Published: 9 January 2018
Authors are encouraged to provide a concise description of the specific application or a potential application of the work. This section is not mandatory.
The properties of supercritical CO2 (SCCO2) and supercritical water (SCW) turn them into fluids with a great ability to remove organic adsorbates retained on solids. These properties were used herein to regenerate an activated carbon fiber (ACF) saturated with a pollutant usually contained in wastewater and drinking water, phenol. Severe regeneration conditions, up to 225 bar and 400 °C, had to be employed in SCCO2 regeneration to break the strong interaction established between phenol and the ACF. Under suitable conditions (regeneration temperature, time, and pressure, and flow of SCCO2) the adsorption capacity of the exhausted ACF was completely recovered, and even slightly increased. Most of the retained phenol was removed by thermal desorption, but the extra percentage removed by extraction allowed SCCO2 regeneration to be significantly more efficient than the classical thermal regeneration methods. SCCO2 regeneration and SCW regeneration were also compared for the first time. The use of SCW slightly improved regeneration, although SCW pressure was thrice SCCO2 pressure. The pathways that controlled SCW regeneration were also investigated.
Keywords:supercritical carbon dioxide; supercritical water; extraction; thermal desorption
The critical point marks a borderline above which the physical properties of a fluid suffer severe changes. Supercritical fluids have a density similar to the density of liquids, but their high diffusivity, and low viscosity and surface tension are characteristics of gases. Furthermore, they efficiently dissolve gases and organic compounds thanks to their low dielectric constant. CO2 is the most used supercritical fluid because of its mild critical constants, Pc = 73 bar and Tc = 31 °C. Thanks to the previously described properties, supercritical CO2 (SCCO2) is used to extract organic compounds retained in liquids or on solid matrixes . The regeneration of activated carbons (ACs) is one of the applications in which SCCO2 is used as extracting fluid.
ACs have excellent adsorbent properties that turn them into a suitable material to purify polluted gaseous and liquid streams . During this process, the pollutants accumulate on the surface of the ACs and their adsorption capacity is progressively reduced until they are completely exhausted. The economical and environmental viabilities of this purification process strongly depend on the removal of the pollutants retained on the ACs and the recovery of their adsorption capacity, that is to say, on the regeneration of the ACs. Several methods to regenerate ACs exist [3,4], although the search for efficient, low-cost, and environmentally sustainable procedures continues because just a few methods gather all of these characteristics. As an example, thermal regeneration with inert gases at high temperatures is the most widespread method despite the damages that it causes in the structure of the ACs. Furthermore, temperatures about 700–900 °C are needed to remove strongly retained pollutants [5,6].
In this context, SCCO2 regeneration arises as an interesting alternative. SCCO2 is able to flow through the porous net of the ACs, reach the micropores where the pollutants are retained, and extract them. The temperatures used in this method so far are lower than 100 °C; consequently, the energy waste is restricted regarding thermal regeneration, and the porosity of the ACs is better preserved. Furthermore, the extracted adsorbate can be easily recovered to be reused or destroyed once the SCCO2 is cooled and depressurized to atmospheric pressure. SCCO2 is usually employed to regenerate ACs saturated with volatile organic compounds like benzene , toluene [8,9,10,11], m-xylene , cyclohexane , or ethyl acetate [14,15]. The regeneration of ACs saturated with inorganic compounds is less usual and co-solvents must be used to efficiently extract these adsorbates . The employment of SCCO2 has also been studied to regenerate ACs saturated with low-volatile organic compounds, e.g., phenol [17,18,19], pesticides , herbicides , or insecticides . Phenol is the most common model compound in the field of regeneration of ACs : it is a pollutant frequently found in wastewater and drinking water that remains strongly retained on the carbon surface of ACs. The limited number of works that have studied the SCCO2 regeneration of ACs exhausted with phenol state that, at regeneration pressures and temperatures below 200 bar and 60 °C, respectively, phenol is not properly extracted  and the ACs are not efficiently regenerated .
The exhausted activated carbon fibers (ACFs) can also be regenerated using other supercritical fluids as regeneration agents, namely, supercritical water (SCW). SCW is not used as commonly as SCCO2 because of its high critical constants, Pc = 221 bar and Tc = 374 °C. These constants make SCW regeneration be an energetically more demanding method than SCCO2 regeneration; despite this drawback, it has been probed that SCW and subcritical water (150 bar and 350 °C) are able to efficiently remove phenol  and some of its derivates  from traditional ACs. Under these conditions, SCW is not only able to remove the retained pollutants but also clean and open the microporosity of the solids, hence increasing the available surface area for subsequent adsorption stages.
This work reports the regeneration of an activated carbon fiber (ACF) exhausted with phenol using SCCO2 and SCW as regenerating fluids. The porous structure of ACFs is similar to that of ACs but their physical morphology provides them with better adsorbent properties than those of ACs. They have larger surface areas because their pores are more uniform and less branched than the pores of ACs, hence their adsorption capacity is greater [25,26]. However, it is an expensive material so an effective regeneration method is essential to guarantee the economical viability of the purification method based on the adsorption of pollutants on ACFs. In order to meet this requirement, the regeneration conditions were hardened in this investigation, thus reaching pressure and temperature up to 225 bar and 400 °C in SCCO2 regeneration and 300 bar and 425 °C in SCW regeneration. The influence of other parameters (regeneration time, flow of regenerating fluid and number of subsequent adsorption-desorption cycles) on the regeneration efficiency (RE) was also analyzed as well as the ability of the method to regenerate the material after several subsequent adsorption–regeneration cycles. Taking into account the scarce information regarding SCW regeneration, this work also reports the comparison between SCCO2 regeneration and SCW regeneration of an ACF exhausted with phenol for the first time.
2. Materials and Methods
A commercial ACF cloth supplied by Kynol Europe (Hamburg, Germany) was used as the adsorbent. This ACF was prepared from the textile fiber Novoloid. The original carbon fiber was activated in a one-step process combining carbonization and activation at 900–1000 °C. Phenol was purchased from Merck-Spain (Madrid, Spain) and used as received. Water was purified with a Milli-Q device (Wasserlab, Barbatáin, Navarra, Spain) before its use. CO2 (99.999% purity) and N2 (99.999% purity) gases were supplied by Air Liquide (Madrid, Spain).
2.2. Adsorption–Regeneration Cycles
The ACF was subjected to subsequent adsorption–regeneration cycles.
The adsorption step began by placing 0.18 g of the ACF into a home-made sample holder consisting of a cylindrical tube made of Hastelloy (5 cm in length, ¼″ OD), which was immersed in a thermostat at 27 °C. A HPLC (high performance liquid chromatography) pump model LC-10AS (Shimadzu, Kyoto, Japan) pumped a flow of 4.0 cm3·min−1 of a 5.35 × 10−4 M phenol solution through the ACF during 240 min. The effluent stream was monitored continuously with a spectrophotometer model UV-1603 supplied by Shimadzu, at a wavelength of 270 nm to obtain the phenol breakthrough curve. The amount of phenol adsorbed could be determined in two ways. On one hand, by integrating the breakthrough curve; on the other hand, by collecting all of the effluent stream and analyzing the amount of phenol contained in it. Both procedures led to the same result. The original ACF retained 162.7 ± 19.5 mgphenol·gACF−1 during this adsorption step.
Once the adsorption step had been completed, the regeneration step began. Figure 1 shows the schematic of the installation used for the SCCO2 regeneration experiments.
The sample holder was placed into the regeneration reactor, a cylindrical tube made of Hastelloy (50 cm in length, 2 cm OD), which was placed in the middle of a cylindrical induction coil. Then, the regenerating fluid was pumped through the exhausted ACF. Liquid cooled CO2 at 50 bar and −4 °C was pumped by a High Pressure P-Series Pump (Thar Technologies, Pittsburgh, PA, USA), a device designed to pump pressurized liquids. The effluent stream was discharged through an automatic pressure-regulating valve, which was used to control the regeneration pressure. Once the pressure had been attained, the reactor was heated by inductive heating. A generator of alternating current model Power Cube 90/180 (CEIA, Viciomaggio, Arezzo, Italy) circulated an electrical current through the coin. The magnetic field generated within the coin rapidly heated the reactor and allowed reaching the desired regeneration temperature in a few seconds. The hot effluent stream proceeding from the reactor went through a heat exchanger, where it was cooled to ambient temperature before reaching the pressure-regulating valve. This design allowed the ACF to remain into the sample holder at any time, thus avoiding any mass loss.
In SCCO2 regeneration, the temperature, time, pressure, and flow rate ranges investigated were 200–400 °C, 10–35 min, 100–225 bar, and 1–15 cm3·min−1, respectively. The SCCO2 flow rate was referred to the conditions at which the fluid was pumped (ρCO2 = 0.96 g·cm−3), so that the volumetric and mass flow rates essentially agreed.
The installation used for the SCW regeneration experiments was the same; in those experiments, CO2 was replaced by water and the fluid was pumped by a HPLC pump model K-501 (Knauer, Hamburg, Germany). The SCW regeneration experiments were carried out at 300 bar and 425 °C with a water flow of 3 cm3·min−1. The time range investigated was 5–15 min.
Once the ACF had been regenerated, it was exposed to a subsequent adsorption step. RE (regeneration efficiency) was calculated as follows, Equation (1):
2.3. Textural Characterization
The ACFs were texturally characterized by N2 adsorption–desorption isotherms at −196 °C and CO2 adsorption isotherms at 0 °C.
The N2 isotherms were obtained on a volumetric device ASAP 2010 from Micromeritics Spain (Madrid, Spain). The specific surface area (SBET) was calculated by applying the Brunauer-Emmet-Teller (BET) equation to the N2 isotherms. The micropore volume, V0(N2), was obtained by applying the Dubinin equation to the N2 isotherm. The mesopore volume (Vmeso) was calculated by subtracting the value of V0(N2) from the total pore volume determined from the N2 isotherm at a relative pressure of 0.95.
The CO2 isotherms were obtained on a volumetric device Tristar 3000 from Micromeritics Spain. The micropore volume, V0(CO2), was obtained by applying the Dubinin equation to the CO2 isotherms.
2.4. Temperature Programmed Desorption (TPD) with Pressurized Water
This technique was used to study the nature of the adsorption of phenol on the ACF. A detailed description of the procedure can be found elsewhere . In summary, a water stream pressurized at 250 bar was pumped through an exhausted ACF. The water stream was progressively heated at a 2.7 °C·min−1 heating rate from ambient temperature up to 580 °C. The experiment lasted 205 min. The phenol released from the ACF as the stream was heated was analyzed in a spectrophotometer at a wavelength of 270 nm.
3. Results and Discussion
3.1. Preliminary Studies: Effect of Supercritical Treatments on the Textural Properties of the ACF
Supercritical fluids can be used to prepare ACFs [28,29]. In this application, supercritical fluids react with a raw carbonized fiber at temperatures above 700 °C. The fiber is gasified and its porosity is increased, hence becoming an ACF. Consequently, when the regeneration procedure of an ACF is performed with supercritical fluids, the textural properties of the ACF may be changed, which would play an important role in the recovery of the adsorption capacity. Although the temperatures at which the gasification of similar fibers begins have been previously probed to be higher than the regeneration temperatures used herein [28,29], the mere exposure of the ACF to CO2 and water above their critical points may cause certain changes in its porosity.
A few experiments were made to assess the possible changes in the textural properties of the ACF when it was exposed to the supercritical fluids. The original ACF was exposed to a SCCO2 flow at 100 bar and two different temperatures, 250 °C (SCCO2.250) and 700 °C (SCCO2.700), during 180 min; and to a SCW flow at 650 °C and 300 bar during 180 min (SCW650). Table 1 shows the results obtained.
The original ACF was essentially microporous, as reflected by its high SBET and micropore volumes. Although SCCO2 at 250 °C did not gasify the raw material, it was able to unblock a few pore entrances. This unblocking led the surface area to slightly increase since some micropores become accessible. When SCCO2 was heated up to 700 °C, gasification began and some mass losses were registered. The textural parameters point that some narrow micropores detected by CO2 adsorption were being widened and turned into micropores with a larger diameter, as reflected by the increase in V0(N2) and SBET. A similar phenomenon was observed when the original ACF was exposed to SCW at 650 °C. SCW is a more reactive gasification agent than SCCO2 and because of that both the mass losses and the increases in V0(N2) and SBET were higher than in the previous case, although the temperature was lower.
The results of Table 1 may encourage regenerating the ACF at high temperatures: phenol would be removed more efficiently and the adsorption capacity of the regenerated material would be enlarged thanks to the increase in SBET. However, this approach is not advisable because of the induced mass losses. The regeneration method must be applicable in several consecutive cycles. If the ACF was regenerated several consecutive times, it would progressively lose a meaningful amount of mass, what may cause a collapse of the material .
3.2. SCCO2 Regeneration
3.2.1. Effect of Temperature
SCCO2 flows of 3 cm3·min−1 at 100 bar were circulated through exhausted samples of ACF during 15 min to study the effect of temperature on the regeneration. Four temperatures were assayed, 200, 250, 300, and 400 °C. The samples were exposed to two consecutive adsorption–regeneration cycles at each temperature. Figure 2 shows the phenol breakthrough curves for the original ACF and the sample regenerated at 250 °C after the first and the second cycle.
The curve for the sample regenerated once almost overlapped the curve for the original ACF, suggesting that, under these regeneration conditions, the original adsorption rate and capacity of the ACF were essentially preserved after one cycle. However, the curve for the sample regenerated twice was displaced towards the left side. This trend pointed that the ACF was able to adsorb a smaller amount of phenol after the second regeneration. This fact was confirmed when the REs were calculated, Figure 3.
The ACF recovered 97.8% of its original adsorption capacity when it was regenerated once at 250 °C. The recovery of the original adsorption capacity was reduced to 93.5% when the regenerated ACF was saturated again, and regenerated at this temperature.
Temperature has two opposite effects on SCCO2 regeneration, which are related to the mechanistic pathways involved in the process [11,19]. SCCO2 can remove a retained pollutant through two pathways: thermal desorption and extraction. Desorption phenomenon implies the supply of an amount of thermal energy (heating of the adsorbent) large enough to break the interactions established between the adsorbate and the adsorbent; in this way, regeneration is improved when high temperatures are used. On the other hand, the increase of the regeneration temperature diminishes the density of the supercritical fluid. A lower density means the reductions of the solubility of phenol in SCCO2 and the ability of the supercritical fluid to extract the pollutant. Considering this, regeneration is worsened when high temperatures are used.
Despite the meaningful reduction in the density of SCCO2 (ρ100bar, 200 °C = 0.122 g·cm−3; ρ100bar, 400 °C = 0.079 g·cm−3), Figure 3 shows that the thermal effect prevailed under the conditions studied herein. RE progressively increased when SCCO2 was heated from 200 to 300 °C; an overheating up to 400 °C did not lead to an increase in RE. Consequently, 400 °C was the highest temperature explored in SCCO2 regeneration since under these conditions regeneration was already complete and higher temperatures might cause structural damages in the ACF.
The RE at 200 °C hardly exceeded 80%. Studying how phenol was adsorbed on the ACF gave more information about why the regeneration was not complete. The nature of the adsorption of phenol on the ACF used herein was studied by TPD using pressurized water as the carrier fluid, Figure 4.
The thermogram showed two peaks. The first peak appeared at temperature between 100 and 250 °C, in the liquid water region. The second peak appeared above 350 °C, in the SCW region. Similar results have been obtained when the nature of the adsorption of phenol on other carbon materials was studied , even when the characterization was made with the classical TPD with inert gas as the carrier [6,31]. The two peaks were associated to different interactions between phenol and the ACF. The first peak was removed at low temperature because that fraction established a weak physical interaction with the adsorbent. This fraction is known as physisorbed phenol. The second peak was related to a fraction of phenol that needed more energy to be removed. In that case, a strong chemical interaction was established between the adsorbent and the adsorbate. This fraction is known as chemisorbed phenol. The removal of this fraction is the main challenge to achieve an efficient regeneration.
It seems probable that, under relatively mild conditions, 200 °C, the strongly retained chemisorbed phenol was not completely removed. The textural characterization of the regenerated ACFs allowed delving into this phenomenon. Figure 5 shows the N2 adsorption–desorption isotherms for the ACFs regenerated at the lowest and the highest temperatures investigated, as well as for the original ACF.
Due to the incomplete removal of phenol at 200 °C, the surface area available for the subsequent adsorption was reduced (recovery of SBET = 73%), which explained why the regenerated ACF did not fully recover its adsorption capacity. Further accumulation of phenol happened after a second adsorption step, thus leading the ACF regenerated twice at 200 °C to lose about 25% of its original adsorption capacity.
The ACFs treated at 300 and 400 °C adsorbed a greater amount of phenol after being regenerated than in their original form, as shown by the RE values over 100%. The high efficiency of the method under these conditions was preserved even when the ACF was exposed to two consecutive adsorption–regeneration cycles: the ACFs regenerated twice had the same adsorption capacity than the original ACF.
The slight increase in the adsorption capacity regarding the original ACF can be partially explained by the results of Table 1. Under these conditions, SCCO2 removed the retained phenol and unblocked the entrance of a few pores, but Figure 5 shows that the N2 isotherm for the ACF regenerated at 400 °C was below the isotherm for the original ACF. Namely, with the treatment at 400 °C only 90% of the original SBET was recovered. However, another phenomenon was occurring during the regeneration that may also be contributing to that increase. The surface chemistry of the adsorbent also plays a key role in the adsorption phenomenon. The adsorption of phenol and its derivates is hindered by the presence of oxygen-containing surface groups [32,33]. On the other hand, it has been probed that the surface chemistry of carbon materials is modified when they are exposed to supercritical fluids. The exposure of this ACF to a SCCO2 flow at 100 bar and 250 °C removes about 60% of the carboxylic acid surface groups of the material, and this percentage increases with temperature . Consequently, it is possible that the surface chemistry of the regenerated ACFs was more suitable for phenol adsorption than that of the original ACF. The combination of the probed notable recovery of the textural properties and a possible suitable modification of the surface chemistry may clarify why RE reached values above 100%.
There is not an unanimous conclusion about the effect of temperature on supercritical regeneration. Some authors affirm that density is the controlling parameter at pressures just above the critical pressure, and regeneration gets worse with increasing temperatures [7,14,15]. It is also stated that as the fluid is compressed, viscosity becomes progressively more influential and the negative effect of temperature is then mitigated [7,9,14,15].
It must be noted that, in all of these previous works, the influence of the extraction pathway was outstanding regarding the influence of the thermal desorption pathway because temperatures did not exceed 100 °C. In the current research the influence of the thermal desorption pathway is evidently more noticeable since temperatures above 200 °C are used. Thermal desorption is the main pathway when the exhausted adsorbents are regenerated with hot inert gases at temperatures lower than 300 °C . Regeneration with hot inert gases is an easier procedure than SCCO2 regeneration. Consequently, it is important to study the relative influence of each pathway in SCCO2 regeneration at high temperatures to assess if the use of the supercritical fluid is necessary, or the adsorbents would be efficiently regenerated with a simple flow of a hot inert gas. This point was studied by regenerating an exhausted ACF with a N2 flow of 300 cm3·min−1 during 15 min at 250 °C. The RE after two adsorption–regeneration cycles with the hot inert gas was 79.2%, in comparison to 93.5% with SCCO2 regeneration with the same conditions of temperature and time in both samples. The RE achieved by thermal desorption with hot inert gases was not low, but the concomitant extraction pathway related to the supercritical fluid provided a meaningful improvement that turned SCCO2 regeneration into a highly efficient regeneration method.
3.2.2. Mass Transfer Limitations: Effect of Time, Flow, and Pressure
Whereas the thermal desorption pathway is exclusively affected by the chosen regeneration temperature, the extraction pathway is affected by other parameters apart from temperature. Within the previous section the importance of the extraction pathway in SCCO2 regeneration has been probed, hence the search for those conditions which optimize this pathway is mandatory. An extraction step just becomes efficient when the limitations to the mass transfer are overcome. This overcoming is critical when the aimed compound is retained on highly microporous materials such as the ACF used herein. The majority of adsorption active sites are located on inner narrow micropores. This implies large mass transfer limitations, but the supercritical fluid must be able to reach those difficulty accessible zones to extract the phenol. Regeneration time, flow, and pressure can be properly modified to overcome these limitations.
Figure 6 shows the effect of time on RE for regeneration at 100 bar and 250 °C with a SCCO2 flow of 3 cm3·min−1.
RE increased with time when the regeneration step was prolonged from 10 to 15 min. It is commonly admitted that the penetration of SCCO2 in porous solids is easy and rapid. These results can be attributed to an external film resistance that slowed down the rate at which phenol could enter the bulk flowing fluid and be carried out of the adsorbent . As the regeneration experiments were lengthened from 10 to 15 min, phenol had more time to diffuse and reach the fluid. Greater amounts of phenol were removed from the micropores, hence improving the efficiency of the method. Further prolongation did not lead to changes in RE; this parameter described a plateau over 15 min.
From a technical point of view, the access of SCCO2 to the inner micropores does not mean a problem for the regeneration procedure, in contrast to other regeneration methods like solvent regeneration or NaOH regeneration. In these methods, a rinse step must be carried out between the regeneration and the adsorption steps because the presence of the regenerating agent within the structure of the adsorbent hinders the subsequent adsorption [35,36,37,38]. In a similar way to SCCO2 regeneration, the regenerating agents must reach all the micropores to efficiently regenerate the exhausted adsorbents, what makes the rinse step trickier. This rinse step is not necessary to the method reported in this work: once the adsorbent is depressurized and cooled, the remaining CO2 turns into gas and leaves the structure of the adsorbent on its own.
Figure 7 shows the effect of the SCCO2 flow on RE for regeneration at 100 bar and 200 °C during 15 min.
RE increased with the SCCO2 flow from 1 to 10 cm3·min−1 and remained unchanged when greater flows were used. The increase of RE with the regeneration flow is characteristic of solubility limited processes. Desorption at flow rates lower than 10 cm3·min−1 was primarily influenced by adsorption equilibrium constraints. The effluent concentration was fixed for each flow and it increased as greater amounts of SCCO2 were pumped. Above 10 cm3·min−1, such high flows were pumped that the equilibrium was not achieved, and the use of greater flows did not lead to the removal of greater amounts of phenol. Above that flow, the process was no longer limited by solubility but mass transfer limited. This effect of SCCO2 flow agreed with that reported by other authors [14,15,22].
Pressure is the last parameter that affects the mass transfers in an extraction step. Figure 8 shows the effect of pressure on regeneration at 200 °C during 15 min with a SCCO2 flow of 3 cm3·min−1.
As SCCO2 was more pressurized, the regenerated ACF recovered a greater percentage of its original adsorption capacity. The process was limited by solubility under the conditions used in this specific study. The solubility of phenol in SCCO2 increased as the fluid was pressurized and, as a consequence, the extraction pathway was also improved [10,13,17].
This last study reveals that pressure modification may be the most interesting way to optimize SCCO2 regeneration. At 200 °C and a pressure high enough the ACFs are effectively regenerated. Although it is still an energy-demanding temperature, it means a noticeable reduction of the energy requirements in comparison with the classical thermal regeneration carried out at temperatures above 700 °C. Furthermore, it neither requires an excessive waste of regenerating fluid. The necessity for devices made with special materials able to support high pressures and the energy waste needed to work at pressures are their major drawbacks. In this way, the compression of the fluid must be controlled: an optimal pressure will exist above which the increase in solubility will be negligible .
3.3. Comparison between SCCO2 Regeneration and SCW Regeneration
In order to make a strict comparison, SCW regeneration was first carried out at the only temperature within the SCCO2 regeneration studies that was over the critical point of water, 400 °C. However, the process was unstable because this temperature was too close to the critical temperature of water, and in this region the physical properties of the fluid suffer strong alterations. The SCW regeneration assays were finally carried out at 425 °C. Figure 9 shows the effect of time and the number of adsorption–regeneration cycles on SCW regeneration at 300 bar and 425 °C with a SCW flow of 3 cm3·min−1.
SCW regeneration also arose as a method able to completely recover, and even increase (RE values greater than 100%), the adsorption capacity of the original ACF. This increase was caused by the same phenomena than in the case of SCCO2. SCW also opened a few pore entrances and modified the surface chemistry in such a way  that the regenerated ACF adsorbed a greater amount of phenol than the original ACF. The high efficiency of the method allowed preserving the adsorption capacity after three cycles, although a slight decrease in RE was observed when the ACF was regenerated during 5 min. When the regeneration step was lengthened to 15 min, RE values were higher. The effects caused by the two phenomena previously described were more remarkable for longer regeneration times, hence leading to a 5% increase in the adsorption capacity of the original ACF. We did not explore temperatures above 425 °C in SCW regeneration since at this temperature the regeneration was already complete and higher temperatures might cause structural damages in the ACFs.
Consequently, SCW regeneration could be described as a method slightly more efficient than SCCO2 regeneration (RESCW,300 bar,425 °C,15 min = 104.6%; RESCCO2,100 bar,400 °C,15 min = 100.3%), although it must be noted that SCW pressure was thrice SCCO2 pressure.
SCW regeneration assays were also interesting from another point of view. Novel information about the regeneration mechanism could be obtained by analyzing the effluent aqueous stream proceeding from the regeneration reactor. The effluent was divided in three samples which were collected during different stages of the regeneration step: beginning stage, intermediate stage and final stage. Each sample was analyzed by UV-Vis spectrophotometry. Figure 10 shows the spectra for the three samples collected during a 7 min regeneration assay, as well as the spectrum for the original phenol solution. The samples were highly concentrated and they had to be diluted in order to fulfill the requirements of the Lambert-Beer law. The dilutions were as follows: 1:40 for the first sample, 1:20 for the second sample, and 1:4 for the third sample.
The spectra for the samples collected during the first 2 min of the treatment, and between minutes 2 to 4, had a similar shape to that for the phenol solution. This similarity meant that during the first 4 min the phenol was removed in its original form (without any degradation). This fact pointed to the same regeneration pathways that governed SCCO2 regeneration: thermal desorption and extraction. Taking into account the dilutions, the number of moles of phenol contained in these two samples was calculated. 93% of the adsorbed phenol was removed during the first 4 min.
On the other hand and regardless of the evident lower signal, the spectrum for the sample collected during the final 3 min showed a significantly different shape from that for the phenol solution. It also showed the typical peak at 270 nm and the shoulder at 275 nm, but its signal did not tend to zero as fast as the phenol spectrum at higher wavelengths. At wavelengths lower than 270 nm, it neither described the marked decrease of phenol spectrum and even a new peak appeared at about 250 nm. This dissimilarity meant that other species were present in the sample besides phenol. The ability of SCW to degrade and gasify phenol has been reported . At high temperatures, 700 °C, and reaction times long enough, the supercritical fluid turns a fraction of this pollutant into gases. Some of the formed by-products are polycyclic aromatic hydrocarbons like naphthalene and phenanthrene, products whose UV-Vis spectra are similar to that for the sample collected during the last minutes of the SCW regeneration treatment. Consequently and despite using low temperatures, the data in Figure 10 suggested that a fraction of the retained phenol was turned into these products. This implied a minor third regeneration pathway in the mechanism of SCW regeneration, a degradation pathway, through which the remaining phenol was removed.
Some authors who have studied the regeneration of carbon adsorbents exhausted with phenol using inert gases at high temperatures, 700–900 °C, state that due to the strength of the bond between the chemisorbed phenol and the adsorbent, the decomposition of that fraction is energetically less exigent than its desorption [6,31]. That is to say, chemisorbed phenol must be degraded to be removed when that method is used. The data reported herein also point that, although great amounts of phenol are removed without degradation thanks to the heating and extractive power of SCW, a fraction of phenol, probably related to the chemisorbed phenol, must also be degraded to be removed. This makes a question about SCCO2 regeneration mechanism arise. The obtained results probed that phenol was removed more efficiently at high temperatures. This trend could be favored by the degradation of a fraction of the chemisorbed phenol at high temperatures, which low-temperature SCCO2 was not able to degrade. However, the effluent gaseous streams from SCCO2 regeneration could not be analyzed and the possible participation of this third regeneration pathway could not be confirmed or denied for this method. Future work could provide a device to recover the extracted pollutants, which would allow studying the mechanism that governs SCCO2 regeneration more in depth; in that way, higher temperatures may also be explored to try to highlight this pathway.
The SCCO2 regeneration of an ACF exhausted with phenol was carried out under the most severe conditions assayed so far, 225 bar and 400 °C. The method efficiently recovered the adsorption capacity of the original ACF when regeneration temperatures were high enough, even after a few subsequent adsorption–regeneration cycles. Under certain conditions, SCCO2 modified both the textural properties and the surface chemistry of the regenerated ACF in such a way that it adsorbed greater amounts of phenol than the original ACF. Phenol was removed from the micropores through two pathways. Most of the phenol was removed because of the heating suffered by the ACF when it was exposed to the high-temperature SCCO2; however, a certain percentage of phenol was removed by extraction, a pathway that hot inert gases could not provide and which turned SCCO2 regeneration in a highly efficient method. The regeneration parameters time, flow of SCCO2, and pressure, were modified to study their influence on RE and improve it. The performances of SCCO2 and SCW as regenerating fluids were also compared. SCW regeneration was slightly more efficient than SCCO2 regeneration, although this method needs for a pressure three times greater. A third pathway, the degradation of a fraction of the chemisorbed phenol, was identified in the mechanism that governed SCW regeneration.
Financial support from the Spanish Ministerio de Economía y Competitividad (Project CTQ2015-64339-R) and Anticipos Fondos Feder is acknowledged.
M. Jesus Sanchez-Montero and Jennifer Pelaz conceived, designed, and performed the experiments; M. Jesus Sanchez-Montero and Nicolas Martin-Sanchez analyzed the data, and wrote the paper; Francisco Salvador and Carmen Izquierdo built the home-made facilities, and supervised the whole study.
Conflicts of Interest
The authors declare no conflict of interest.
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Figure 1. Schematic of the installation used for the supercritical CO2 (SCCO2) regeneration experiments.
Figure 2. Phenol breakthrough curves for the original activated carbon fiber (ACF) and the sample regenerated with SCCO2 at 250 °C after the first and the second adsorption–regeneration cycle.
Figure 3. Effect of temperature and the number of adsorption–regeneration cycles on RE (regeneration efficiency).
Figure 4. Desorption thermogram of phenol from the ACF using pressurized water as the carrier fluid.
Figure 5. N2 adsorption-desorption isotherms for the original ACF and the ACFs regenerated at 200 °C and 400 °C.
Figure 6. Effect of time on RE for regeneration at 100 bar and 250 °C with a SCCO2 flow of 3 cm3·min−1.
Figure 7. Effect of the SCCO2 flow on RE for SCCO2 regeneration at 100 bar and 200 °C during 15 min.
Figure 8. Effect of pressure on RE for SCCO2 regeneration at 200 °C with a SCCO2 flow of 3 cm3·min−1 during 15 min.
Figure 9. Effect of time and the number of adsorption–regeneration cycles on RE for supercritical water (SCW) regeneration at 300 bar and 425 °C with a SCW flow of 3 cm3·min−1.
Figure 10. Spectra for the original phenol solution and the three samples collected during a SCW regeneration assay.
Table 1. Changes in the textural properties of the original activated carbon fiber (ACF) when it is exposed to supercritical fluids.
|Sample||SBET (m2·g−1)||V0(N2) (cm3·g−1)||Vmeso (cm3·g−1)||V0(CO2) (cm3·g−1)||Mass Losses (%)|
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