Home Technology Activated carbon from sugarcane as an efficient adsorbent for phenol from petroleum refinery wastewater: Equilibrium, kinetic, and thermodynamic study
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Activated carbon from sugarcane as an efficient adsorbent for phenol from petroleum refinery wastewater: Equilibrium, kinetic, and thermodynamic study

  • Mustafa S. Abdulrahman , Alanood A. Alsarayreh , Suondos K. A. Barno , Mervat A. Abd Elkawi and Ammar S. Abbas EMAIL logo
Published/Copyright: June 28, 2023
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Abstract

The adsorption method may be one of the environmentally friendly, economical, and effective techniques to remove phenol from wastewater using low-cost adsorbent activated carbon (AC). The effects of the initial concentration of phenol, temperature, and time of the adsorption on the phenol removal percent were studied. The maximum removal percentage of phenol was 63.73% of the initial 150 mg/l concentration obtained at 25°C. Langmuir, Freundlich, Temkin, and Dubinin–Radushkevich isotherm models have been applied to study the adsorption equilibrium. The results show that both Langmuir and Freundlich isotherms fitted the equilibrium data better with a high correlation coefficient (R 2) and a maximum adsorption capacity of 108.70 mg/g. Thorough fitting of adsorption kinetics data followed the pseudo-second-order model. Thermodynamic parameters were calculated in the temperature range of 25–50°C. The results show that the adsorption process of phenol on AC is more favorable at low temperatures.

1 Introduction

Sugarcane is an important crop in tropical and subtropical regions. Agricultural research and practice on sugarcane are becoming increasingly data-intensive, with various modelling frameworks established to simulate processes such as adsorption [1,2,3]. The sugarcane industry in Brazil produces a substantial amount of sugarcane ashes, a waste product used in many industries [4].

Adsorption can be used to reduce the quantity of CO2 that is released into the air by industrial processes. For this purpose, activated carbons (ACs), zeolites, and mesoporous silica are used as sorbents. ACs can be made from a wide range of raw materials, including biomass wastes, which come from plants [5]. The biomass wastes are cheap, available materials, and can be converted into an adsorbent after making some modifications and chemical treatments [6]. Sugarcane ashes comprise cellulose fibers, lignin, and hemicellulose, making it a suitable raw material for carbon [7].

Phenol is considered a priority pollutant due to its high toxicity, as it is poisonous to organisms at low concentrations, and many of its constituents have been categorized as hazardous pollutants due to its potential to impact human health [8]. The removal of phenol from aqueous solutions can be done through the adsorption of biomass-derived AC [8,9].

On humans, excessive exposure to phenol may have adverse effects on the brain, digestive system, eye, heart, liver, lungs, and skin, among others [10]. Therefore, environmental specialists are overly concerned if phenol is found in drinking water or wastewater [11,12].

The primary sources of phenol contamination in the aquatic environment include wastewater from the paint, pesticide, coal conversion, polymeric resin, polymer synthesis, plastic, rubber, insecticides, pharmaceutical, gasoline, rubber proofing, steel, petroleum, and petrochemical industries [13,14].

Phenols have a negative influence on both human and animal health because these are highly toxic and carcinogenic. According to the World Health Organization, drinking water should contain no more than 1 µg/l of phenols [15,16]. Therefore, before disposing of sewage, industrial effluents must be treated with phenols [17].

As a result, a variety of techniques are available for treating phenol-containing wastewater prior to its discharge into natural streams. These techniques include electrochemical degradation and electrochemical oxidation [18]. Moreover, fouling-resistant nanofiltration membranes for the separation of oil–water emulsion and micropollutants from water, separation and purification technology, biological treatment, biodegradation of phenols from wastewater by microorganisms immobilized in bentonite and carboxymethyl cellulose gel, chemical coagulation, precipitation, ion exchange, photocatalytic degradation, reverse osmosis, and adsorption processes [19,20,21,22,23,24,25,26,27,28,29], in addition to solvent extraction, incineration, and nanofiltration, are used to treat wastewaters [30]. Each of these techniques has advantages and drawbacks. Compounds from wastewater are rarely used frequently or on a large scale due to their extremely high costs and disposal issues [31,32].

However, adsorption has emerged as one of the most effective techniques for resolving difficulties in purification and separation technology because it is the simplest, most successful, and least expensive way to eliminate phenol among these methods. ACs are the most prominent adsorbents due to their high surface area per mass, microporous nature, high adsorption capability for a variety of adsorbates, including phenolic compounds, high purity, and ease of availability [13,33,34,35].

AC can be produced using either the physical activation process or the chemical activation process. The type of precursor, the activation process, and the activation conditions affect the porosity properties of ACs, such as pore-size distribution, pore shape, and surface chemistry [36]. There are two steps in physical activation to create more porous structures [37]. First, the material is carbonized in an inert atmosphere and then activated at a high temperature using either steam or carbon dioxide as the activating reagent [38]. However, in chemical activation, raw materials are heated in an inert atmosphere after being impregnated with an activation reagent such as KOH, H3PO4, and ZnCl2. Chemical activation is preferred over physical activation due to its low energy and operating costs, high carbon yields, large surface areas, and porous structure, as well as its simplicity, speed, and need for lower activation temperatures [39,40].

Both the carbonization and activation processes occur simultaneously. The oxidation and dehydration reactions of chemicals result in the formation of pores. The created char is then cleaned to remove any remaining contaminants [41].

ACs are derived from carbonaceous substances. The selection of a precursor is heavily influenced by its availability, cost, and purity; however, the production processes and intended applications of the product are also significant factors [41]. Because biomass is renewable, accessible, economical, and environmentally friendly, it is receiving more and more attention worldwide [42]. Numerous biomass sources, including low-grade plants, agricultural waste, and municipal solid waste, can be used as AC precursors [41].

For the elimination of phenols and their derivatives, the agricultural waste materials like grain husk, apricot stone shell, peat, plum kernel, beet pulp corn grain, sugarcane bagasse, wood charcoal, babul sawdust, acacia glauca saw dust, modified clay, biological materials, chitin, and zeolite have been utilized directly or via producing ACs [43,44,45,46,47,48,49,50,51,52,53,54,55,56]. However, it has been found that sugarcane acts as an adsorbent for phenol adsorption.

Numerous adsorbents made from agricultural byproducts have already been utilized for phenol removal; however, according to the literature review, ACs made from sugarcane grown in Iraq as a phenol adsorbent or for treating oil refinery wastewater have not yet been reported widely. The objective of this study is to investigate the efficiency of sugarcane-AC in removing phenol from aqueous solutions. The purpose of this research is to prepare an inexpensive sugarcane waste to develop AC for the adsorption-based phenol removal from the synthesis effluent. Equilibrium data will be used to explore the phenol adsorption isotherms, followed by kinetics and thermodynamics of the adsorption process at various temperatures.

2 Experimental work

Sugarcane was used to prepare the AC. Sugarcane was first washed with water to remove impurities before being dried at 110°C for 24 h.

Sugarcane was prepared in a stainless-steel reactor with dimensions of 3 cm in diameter and 15 cm in length that was closed at one end and had a removable cover with a 1 mm hole in the middle to allow the burned gases to escape. The reactor was heated for 2 h at 360°C in an electrical furnace. After that, it was allowed to cool at room temperature. The produced carbon material was crushed by a disk mill and then sieved. Carbon material of a particle size less than 300 µm was activated by the addition of 10 ml of NaOH solution (1.5 M) per each 2 g of produced carbon material for 24 h. After that, samples that had been treated with NaOH solutions were dried completely overnight at 110°C in a dryer.

A quartz reactor with a diameter of 3 cm and a length of 13 cm was used in the microwave activation step. The reactor was filled with the dried sample, and the reactor was placed in a microwave oven with a radiation power of 540 W for 8 min. Then, the sample was allowed to cool and saturated with 10 ml of 0.1 M HCl solution using per gram of AC material for 24 h at room temperature and washed with water. Finally, dry AC samples were dried in a dryer at 110°C for 24 h, cooled in a desiccator, and then each sample was weighed to calculate the yield. The surface area and the pore volume of the yield AC were measured at the Petroleum Research & Development Center, Baghdad, Iraq.

Adsorption experiments were conducted by batch methods with 1 g of AC per liter of synthesis wastewater, which contains 10–150 ppm of phenol. To obtain the equilibrium state, The AC suspension and the aqueous solutions of phenol were placed on a shaker for 24 h at a constant speed of 200 rpm at 25°C. The adsorption kinetics was studied for solutions of the maximum phenol concentration (150 ppm) at different temperatures (25, 40, and 50°C).

At the required temperature and after a certain adsorption time (up to 90 min for kinetics experiments), the suspension sample was taken and filtered. The phenol concentrations of the filtrated solutions were determined by the GENESYS 10 S UV-VIS spectrophotometer at a wavelength of 268 nm, and then the total removal percentage was calculated.

The equilibrium experiments were completed for 24 h at 25°C. Equation (1) is used to figure out the amount of phenol adsorbed per weight of AC adsorbent at equilibrium:

(1) q e = ( C o C e ) × V m ,

where q e is the adsorption capacity of the adsorbent (mg/g), C o and C e in (mg/l) refer to initial and final equilibrium concentrations of phenol in the adsorption solution, V (L) is the volume of the adsorption solution, and m (g) is the weight of the AC adsorbent used.

3 Results and discussion

The surface area and pore volume of AC prepared from Iraqi sugarcane stalks were 1073.2 m2/g and 1.04 cm3/g, respectively.

The phenol equilibrium concentration can be represented to study the behavior of the adsorption equilibrium capacity progress process. Figure 1 shows that the relationship is directly proportional. As the initial phenol concentration increased from 10 to 150 ppm, the equilibrium concentrations increased from about 2 to 54 mg/l, and the equilibrium adsorption capacity increased from about 0.8 to 127.7 mg/g. These findings are in good agreement with the previously reported highest phenol removal percentage (75.29%) from aqueous solution by adsorption on the AC from banana peels at the same adsorbent dose (1 g/l) [15].

Figure 1 
               Equilibrium phenol adsorption capacity versus the initial concentration after 24 h of adsorption at 25°C.
Figure 1

Equilibrium phenol adsorption capacity versus the initial concentration after 24 h of adsorption at 25°C.

3.1 Adsorption isotherms models

Simulated wastewater containing 150 mg/l of phenol at 25°C was used to examine the adsorption isotherms. The most popular two-parameter isotherms were selected to describe the adsorption of phenol on AC [57,58]. These isotherm models include Langmuir, Freundlich, Temkin, and Dubinin–Radushkevich.

3.1.1 Langmuir adsorption isotherm model

The Langmuir isotherm model [59] is an empirical model that assumes that adsorption may only occur at a set number of defined confined sites without lateral interaction between the molecules being adsorbed. According to this model, the thickness of the adsorbed layer is one molecule or monolayer adsorption. According to the Langmuir isotherm, a homogeneous process occurs in which each molecule maintains a fixed enthalpy and sorption activation energy without transmigration of the adsorbate across the surface. Equation (2) depicts the linear formulation of the Langmuir adsorption isotherm

(2) 1 q e = 1 q m K L 1 C e + 1 q m ,

where q m and K L are the maximum adsorption capacity in (mg/g) and the Langmuir isotherm constant energy or net enthalpy of adsorption in (l/mg), respectively.

As shown in Figure 2, when [ 1 / q e ] is plotted against [ 1 / C e ] , a straight line with slope [ 1 / q m K L ] and intercept equal to [ 1 / q m ] is formed. The determined value of slope was 0.2384, and the intercept was 0.0092, with an R 2 value of 0.9751. Therefore, the highest adsorption capacity ( q m ) was 108.70 mg/g and K L was 0.0386 l/g.

Figure 2 
                     Langmuir isotherm model for phenol adsorption on AC.
Figure 2

Langmuir isotherm model for phenol adsorption on AC.

3.1.2 Freundlich adsorption isotherm model

The Freundlich isotherm model [60] is an empirical formula defining the non-ideal and reversible adsorption process for multilayer, heterogeneous adsorption states. The conventional form of the Freundlich equation is presented in the following equation:

(3) ln q e = ln K F + 1 n ln C e

where K F and n are a Freundlich constant indicative of the relative adsorption capacity of the adsorbent (mg/g) and the intensity or the heterogeneity factor, respectively.

As shown in Figure 3, when [ ln q e ] is plotted against [ ln C e ], a straight line with slope [ 1 / n ] and intercept [ ln K F ] is formed. The slope value determined to be 0.7994, so the relative adsorption capacity was 4.3606 mg/g. Since the intercept value was 1.4726, the intensity (n) was 1.2509. The model correlation coefficient (R 2) was 0.9888. When n = 1, the partition between phases is concentration independent. If the value of n is more than 1 (as determined by our research), this will be a sign of normal adsorption. In contrast, the fact that n is smaller than one indicates that cooperative adsorption occurs.

Figure 3 
                     Freundlich isotherm model for phenol adsorption on AC.
Figure 3

Freundlich isotherm model for phenol adsorption on AC.

Figure 4 
                     Temkin isotherm model for phenol adsorption on AC.
Figure 4

Temkin isotherm model for phenol adsorption on AC.

3.1.3 Temkin adsorption isotherm

The Temkin isotherm model is given as follows [61]:

(4) q e = B ln K T ± B ln C e ,

where B and K T are the Temkin energy constant (J/mol) and the constant describing the interaction between phenol molecules and BPAC surface (dimensionless), respectively. To determine the isotherm constants B and K T , a graph of q e vs ln C e was plotted (Figure 4).

Figure 5 
                     Dubinin–Radushkevich isotherm model for phenol adsorption on AC.
Figure 5

Dubinin–Radushkevich isotherm model for phenol adsorption on AC.

3.1.4 Dubinin–Radushkevich adsorption isotherm model

The Dubinin–Radushkevich isotherm model is an empirical model for expressing the adsorption process that occurs after a pore-filling mechanism has been obtained [62]. The Dubinin–Radushkevich isotherm describes the adsorption process on both homogeneous and heterogeneous surfaces. Equations (4) and (5) are the linear expression of the Dubinin–Radushkevich isotherm model

(4) ln q e = ln q s K DR ε 2 ,

(5) ε = RT ln 1 + 1 C e ,

where q s , K DR , R , and T are the theoretical monolayer saturation capacity constant in the Dubinin–Radushkevich isotherm model (mg/g), the constant correlated with the mean free energy of adsorption (mol2/kJ2), the gas constant (8.314 J/mol K), and the absolute temperature (K), respectively.

A straight line with a slope of [ K DR ] and an intercept equal to [ ln q s ] is obtained by plotting [ ln q e ] versus [ ε 2 ] (Figure 5). The slope and intercept of the Dubinin–Radushkevich isotherm model were calculated to be −0.0501 and 0.2571, respectively. Consequently, these values were equivalent to 1.2932 mg/g and 0.0501 mol2/kJ2. The Dubinin–Radushkevich isotherm’s R 2 was found to be 0.8501, which is less than those determined for other models.

Equation (6) can be used to estimate the apparent energy of adsorption from the Dubinin–Radushkevich isotherm, E, which was found to be +3.16 J/mol. The reported heat of physical adsorption in the liquid phase and the low positive value of E are in good agreement [63].

(6) E = 1 ( 2 K DR ) 1 2 .

Table 1 displays the constants determined for each of the equilibrium isotherm models described and the R 2 values. Based on the values of the established correlation coefficients, the tabulated data indicate that the R 2 constants of the Langmuir, Freundlich, and Temkin model's were 0.9751, 0.9888, and 0.9012, respectively, which accurately represent the equilibrium adsorption of phenol on AC. However, the Dubinin–Radushkevich isotherm model failed to adequately represent equilibrium data (R 2 = 0.6867). The higher value of the maximum adsorption capacity determined by the Langmuir isotherm model (108.70 mg/g) confirmed this model as the superior isotherm for describing phenol adsorption on AC.

Table 1

Constants for each of the equilibrium isotherm models and R 2

Isotherm model Model parameters Parameter value R 2
Langmuir q m (mg/g) 108.70 0.9751
K L (l/mg) 0.0386
Freundlich K F (mg1−n l n /g) 4.3606 0.9888
n (–) 1.2509
Temkin RT/b T, J/mol 0.0321 0.9012
b T is Temkin energy constant 79.53
ln K T, (K T in l/g) 33.6885
Dubinin–Radushkevich q s (mg/g) 55.9971 0.6867
K DR (mol2/kJ2) 2.0296
E (J/mol) 496.34

3.2 Kinetics of adsorption

In the first 25 min, the total elimination of phenol waste increased dramatically with time, but after 45 min, this trend tended to unchanged. As depicted in Figure 6, this behavior was found in all experiments performed at the analyzed temperatures (25, 40, and 50°C). In addition, Figure 7 shows that the adsorption capacity of phenol increased exceptionally rapidly from the beginning to 25 min and then remained unaffected by time after 45 min. The amount of phenol extracted decreased as temperatures increase. As indicated in Figure 6, the lowest total phenol removal value after 45 min at 50°C was 56.35%, while the highest total phenol removal value was 63.73% at 25°C. Figure 7 shows that the reduced adsorption capacity of the AC, which decreased from 156.7 to 147.0 mg/g as the temperature increased from 25 to 50°C, was the cause of the decrease in the phenol removal value.

Figure 6 
                  The effect of time on phenol removal at different temperatures.
Figure 6

The effect of time on phenol removal at different temperatures.

Figure 7 
                  The effect of time on the AC adsorption capacity at different temperatures.
Figure 7

The effect of time on the AC adsorption capacity at different temperatures.

The best adsorption models that captured the phenol adsorption data on AC were examined using the adsorption capacity versus time data. Pseudo-first order, pseudo-second order, and intra-particle kinetic model are the three kinetic models that were applied. In order to determine the adsorption rate constants for each model at the various temperatures, the linear form of these models (equations (7)–(9)) was solved by linear regression based on the least-squares criterion [64,65,66].

(7) Pseudo first order kinetic model : ln ( q e q t ) = ln q e k 1 t ,

(8) Pseudo second order kinetic model : t q t = 1 k 2 q e + t q e ,

(9)Intra-particle kinetic model: q t = k 3 t 1 2 + C ,

where q e , q t , k 1 , k 2 , k 3 , and C are the adsorption capacity of phenol at equilibrium (mg/g), the adsorption capacity of phenol at any time (t) (mg/g), adsorption rate constants for pseudo-first order (1/min), pseudo-second order (g/mg min), intra-particle kinetic model (mg g·min1/2), and an arbitrary constant (dimensionless), respectively.

Table 2 lists the rate constants that were calculated using the least square technique at various temperatures.

Table 2

Rate constant values for adsorption of phenol on AC

Adsorption kinetic model Model rate constant Model parameter value at temperature
25°C 40°C 50°C
Pseudo-first order k 1 (1/min) 0.0578 0.0678 0.0758
R² range 0.2318–0.5115
Pseudo-second order k 2 (g/mg min) 5.3457 6.3168 7.7247
R² 0.9981 0.9957 0.9931
Intra-particle k 3 (mg/g min1/2) 5.6494 5.4790 5.6976
C 51.627 47.298 41.022
R² range 0.5451 to 0.6248

The kinetic of phenol removal by adsorption on AC was follow a pseudo-second order model (high R 2 for all temperatures) but did not fit well to the pseudo-first order and intra-particle kinetic models, according to the values of the correlation coefficient calculated for the kinetic models with the obtained parameters. Regarding the environment, the pseudo-second-order kinetic model typically succeeded in describing the phenol substance adsorption data from the aqueous solution [67,68].

3.3 Thermodynamic of phenol adsorption on AC

The thermodynamic behavior of phenol adsorption on AC was examined. Based on equations (10) and (11), these parameters were the change in Gibbs free energy ( G ), enthalpy ( H ), and entropy ( S ) [69,70,71].

(10) G = RT ln ( K d ) ,

(11) G = H T S ,

where R, T, and K d are the gas constant (8.314 J/mol K), the absolute temperature of the adsorption process (K), and the distribution coefficient for the adsorption of adsorbate (phenol) at the adsorbent (AC) surface, respectively. The distribution coefficient can be calculated by the following equation:

(12) K d = q e C e m V ,

where q e, C e, V, and m are the adsorption capacity of the adsorbent (mg/g), the equilibrium concentrations of phenol in the adsorption solution (mg/l), the volume of the adsorption solution (l), and the weight of the AC adsorbent used (g), respectively.

The values of K d and the values of G were estimated by using equations (10) and (12), respectively. However, the plot of G versus T as depicted in Figure 8 can be utilized to obtain H , which represent the intercept of plot, and S , which represent the negative value of the slope. The obtained numerical values are summarized in Table 3.

Figure 8 
                  The change in Gibbs free energy versus adsorption temperature.
Figure 8

The change in Gibbs free energy versus adsorption temperature.

Table 3

Numerical values obtained of the distribution coefficient and thermodynamic parameters versus temperature (results of Figure 8)

Temperature (K) K d Thermodynamic parameters R 2
G (J/mol) H (J/mol) S (J/mol K)
298 4.769 −1548.2 −11132 −32.144 0.9994
313 3.286 −1082.6
323 2.659 −742.3

The negative value of H (exothermic process) and the increase in G with the temperature indicate that the adsorption process is more favorable at low temperatures. However, the negative value of S realized the decrease in the randomness at the solution/solid interface during the adsorption of phenol onto AC [72].

4 Conclusion

The adsorption method may be one of the best separation processes due to its high efficiency, low cost, and environment friendly to remove phenol pollutants from industrial wastewater using bio-adsorbents AC. The present results show that the AC removes phenol from wastewater effectively. The maximum phenol removal observed is 63.73% for 150 mg/l aqueous solution using 1 g/l dose AC. The equilibrium adsorption data can be well represented by the Langmuir isotherm with a maximum adsorption capacity of 108.7 mg/g. The calculated value of the apparent energy from the Dubinin–Radushkevich isotherm states that the adsorption of phenol on AC is a physical process. The adsorption of phenol on AC is a fast process during the first 15 min. The phenol adsorption process successfully follows the pseudo-second-order model. Thermodynamic results indicate that the adsorption of phenol on AC is a spontaneous exothermic process and satisfactory at low temperatures.

  1. Conflict of interest: The authors state no conflict of interest.

  2. Data availability statement: Most datasets generated and analyzed in this study are included in this submitted manuscript. The other datasets are available on reasonable request from the corresponding author with the attached information.

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Received: 2023-01-14
Revised: 2023-03-09
Accepted: 2023-04-13
Published Online: 2023-06-28

© 2023 the author(s), published by De Gruyter

This work is licensed under the Creative Commons Attribution 4.0 International License.

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