Abhishek Nayak,
Shanon Viegas
,
Nithya Rajagopal
,
Adrian Marcel Rodrigues,
Harshini Dasari
and
Nethaji Sundarabal
*
Department of Chemical Engineering, Manipal Institute of Technology, Manipal Academy of Higher Education, Manipal, India. E-mail: nethaji.s@manipal.edu; Tel: +91 0820 2924316
First published on 16th June 2025
Asphaltenes, the most polar and complex class of compounds in petroleum crude oils, pose significant challenges in refining processes due to their tendency to precipitate, causing fouling, clogging, and corrosion in pipelines and reactors. These issues are further increased by their solubility behaviour, making their removal difficult. The present study investigates the synthesis of metal nanocomposites focused on a metal–organic framework (Cu-BTC), a spinel oxide (CoMn2O4) and an octahedral molecular sieve (K-OMS-2) for the adsorption and oxidation of asphaltenes from model solutions. The prepared nanocomposites were characterised using FE-SEM, EDX, HR-TEM, FT-IR, XRD, and BET surface area analysis. Furthermore, they were tested for their ability to adsorb asphaltenes using batch adsorption studies, and the equilibrium data obtained were interpreted using Langmuir, Freundlich, Temkin, Redlich–Peterson, and Hill isotherm models. Thermodynamic studies were performed, and changes in enthalpy (ΔH0), entropy (ΔS0) and free energy (ΔG0) were determined from the data. Kinetic studies were conducted, and the data were analysed using pseudo-first-order (PFO), pseudo-second-order (PSO), Elovich, intraparticle diffusion, and Boyd diffusion models. Adsorption studies revealed that asphaltenes’ adsorption onto Cu-BTC was best explained by the Freundlich adsorption isotherm, while CoMn2O4 followed the Langmuir model and K-OMS-2 was governed by the Hill isotherm. The monolayer adsorption capacities of the prepared nanocomposites varied in the order: K-OMS-2 (245 mg g−1) > CoMn2O4 (77 mg g−1) > Cu-BTC (50 mg g−1). Kinetic studies indicated that the adsorption process was rapid, and the Boyd diffusion model suggested that the rate-limiting step was the external mass transfer of asphaltenes onto the adsorbent. CoMn2O4 exhibited the highest catalytic activity among the prepared nanocomposites for asphaltene oxidation, achieving a 140 °C reduction in oxidation temperature. The findings indicated that K-OMS-2 is an effective material for adsorption, while CoMn2O4 is efficient in the catalytic oxidation of asphaltenes.
The interference of asphaltenes can be observed at every stage of petroleum production, transport and refining. Several removal strategies are employed to mitigate these adverse effects, including reservoir precipitation modelling, asphaltene precipitation simulations, chemical inhibition of asphaltenes, mechanical scraping, pigging, solvent extraction, coking, and adsorption.4 Modelling and simulation serve as preventive strategies for asphaltenes interference; however, they are inherently complex, well-specific, and demand expert knowledge. Chemical inhibition is an effective preventive measure that depends on the use of expensive chemical additives. Maintenance methods such as scraping, pigging, and solvent extraction are labour-intensive, costly, and lead to substantial operational downtime. Coking facilitates the conversion of asphaltenes into valuable products, which offers added value. Among these techniques, adsorption has shown considerable promise due to high removal efficiency and operational simplicity; nonetheless, it still requires optimisation for large-scale applications.5 As asphaltenes are a highly polar class of compounds, charged interactions strongly influence their adsorption. However, these stable charged interactions can lead to secondary pollution.6 To address this, the oxidation of asphaltenes is explored for the regeneration of the adsorbent, enabling reusability and reducing solid waste.
Various materials, such as carbon composites,7 metal composites,8 and metal oxide composites,9 have been explored for the adsorption and oxidation of asphaltenes. Among these, transition metal composites are particularly studied due to their ability to exhibit multiple oxidation states, provide diverse surface functionalities, and display various morphologies.10 The effects of metal oxide morphology are well established in applications such as oxidation catalysts for various processes. However, the influence of metal composite morphology on adsorption and oxidation has not been studied extensively. As a result, mixed-metal oxides, metal–organic frameworks (MOFs), and octahedral molecular sieves (OMS), which are known adsorbents and oxidation catalysts, remain to be investigated for asphaltene removal and oxidation.
MOFs are porous crystalline materials formed by linking metal ions with organic linkers. They are well known for their high surface area, porosity, and tunable properties.11 These materials have been studied extensively for applications involving gas storage and gas separation,12–17 as well as for adsorption, owing to their excellent surface properties. MOFs demonstrate significant potential in various adsorption applications, particularly in the adsorption of ionic compounds.18–20 Additionally, MOFs possess limited catalytic activity, often restricted to gas-phase reactions. Despite their proven adsorption and oxidation potential, MOFs have not been thoroughly explored for asphaltene adsorption. Therefore, this study investigates the use of MOFs for the adsorption and oxidation of asphaltenes.
Mixed metal oxides are compounds consisting of two metals in the form AxByOz.21 These oxides occur naturally in the form of mineral rocks and gemstones, while various phases of mixed metal oxides are synthesised and studied for diverse applications.22 Generally, mixed metal oxides with spinel, rutile, haematite, ilmenite and perovskite crystal structures are widely used in numerous applications.1,23–29 Among them, spinel oxides are exceptionally versatile and have applications in supercapacitors,30 photocatalysis,31 oxidation catalysis,32 battery electrode materials,33 electrocatalysis,34 and adsorption.35,36 Spinel oxides have a structure where large metal cations are bound to smaller cations and oxygen, represented by the formula AB2O4.37 The cations are coordinately bound by tetrahedrally bound A, octahedrally bound B and an oxygen atom. Spinels are often used as catalysts due to their multiple oxidation states.38 Despite their proven adsorption and catalytic properties, they are yet to be explored for the adsorption and oxidation of asphaltenes.
OMS are inorganic materials widely known for their octahedrally bound three-dimensional structure.39 OMS possess a porous surface with a tunnel-like three-dimensional framework, making them suitable for molecular separation and catalysis applications.40 They are generally used in ion exchange,40 separation processes,41 catalysis,42 and adsorption.43 OMS consist of metal oxide molecules octahedrally bound by coordinate bonds, with transition metal oxides such as manganese forming the core of the octahedra surrounded by oxygen atoms. These octahedral units link together to form a tunnel structure, characteristic of OMS. However, the OMS's size and shape depend on the arrangement of the metal–oxygen octahedra.44 Among the OMS, OMS-2 (cryptomelane) is well known for its 2 × 2 tunnel structure and has the general formula AxMn8O16, where A is potassium, sodium, hydrogen or transition metals.45 OMS-2 is widely used for adsorption, oxidation catalysis, and environmental remediation applications. Although OMS materials are well-known for their effective adsorption and catalytic abilities, their potential for asphaltene removal and oxidation has not been investigated.
Hence, in the present work, multifunctional materials, namely, Cu-BTC, CoMn2O4, and K-OMS-2, were investigated for the adsorption and oxidation of asphaltenes. The study evaluates structurally and functionally diverse materials for asphaltene treatment, a comparative approach that has not been previously reported. The distinct properties of each material are strategically explored: K-OMS-2 for its structural characteristics and redox catalytic activity,46,47 CoMn2O4 for its acid–base surface characteristics,48 and Cu-BTC for its highly porous and functionalised framework. This work aims to elucidate how these differing characteristics influence the adsorption and oxidation behaviour of asphaltenes.
The n-heptane was recovered from n-heptane-bitumen solution via distillation using a round-bottom flask connected to a condenser. The spent solution was boiled at 98 °C, and the resulting colourless n-heptane distillate fraction was collected and reused in subsequent extraction.
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Fig. 2 FE-SEM micrographs of (A) Cu-BTC at 10k×, (B) Cu-BTC at 75k×, (C) CoMn2O4 at 40k×, (D) CoMn2O4 at 180k×, (E) K-OMS-2 at 40k×, and (F) K-OMS-2 at 180k×. |
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Fig. 3 HR-TEM images of (A) Cu-BTC at 300k×, (B) Cu-BTC at 500k×, (C) CoMn2O4 at 80k×, (D) CoMn2O4 at 300k×, (E) K-OMS-2 at 80k×, and (F) K-OMS-2 at 300k×. |
The EDX analysis of the prepared metal nanocomposites was conducted before and after asphaltene adsorption to confirm the successful uptake of asphaltenes. The obtained spectrum is shown in Fig. S1 and S2 (ESI†). The EDX spectra confirmed the purity and elemental composition of the prepared metal nanocomposites. The spectrum in Fig. S1A (ESI†) confirmed the presence of Cu originating from the metal component, and C and O derived from the organic component in the prepared Cu-BTC. The EDX spectra of CoMn2O4 in Fig. S1B (ESI†) confirmed the presence of Co, Mn, and O. Similarly, the presence of K, Mn and O in K-OMS-2 was confirmed from the EDX spectra in Fig. S1C (ESI†) with no detectable impurities. Fig. S2 (ESI†) confirmed asphaltene uptake by indicating the presence of carbon in the EDX spectra of the spent nanocomposites.
FT-IR analysis of the prepared metal nanocomposites was performed to determine the surface functional moieties. The spectrum was obtained for the nanocomposites before and after asphaltene adsorption, as shown in Fig. 5. The surface functional groups of the adsorbent play a vital role in determining the mechanism of adsorption, particularly when the adsorbate contains charged functional groups. From the FT-IR spectrum shown in Fig. 5A, the transmittance peaks representing CO, C–O and Cu–O were observed at 1625 cm−1, 1400 cm−1 and 588 cm−1, which are characteristic peaks of Cu-BTC.62 In the FT-IR spectrum of Cu-BTC post-asphaltene adsorption, the Cu–O bond peak exhibited a significant shift alongside reduced intensity in the characteristic peaks, confirming asphaltene adsorption. The FT-IR spectrum of the prepared CoMn2O4 is represented by Fig. 5B. CoMn2O4 was confirmed by the absorption peak corresponding to the vibration of Co–O coordination and Mn–O coordination bond vibrations, which was observed at 640 cm−1 and 533 cm−1, respectively.63,64 A reduction in the intensity of the characteristic peaks was observed, in addition to a shift towards a lower wavenumber, which indicated asphaltenes’ accumulation on the surface. Similarly, the FT-IR spectrum for the prepared K-OMS-2 was obtained, as shown in Fig. 5C. The bands representing K-OMS-2 were observed at 467 cm−1, 532 cm−1, and 730 cm−1. The observed characteristic peak represents vibrations of the Mn–O units of the octahedral manganese oxide.65 Furthermore, O–H stretching of water was observed in the higher wavenumber region, which confirmed the moisture in the material. The presence of the moisture could be from the atmosphere or the hygroscopic nature of the prepared metal nanocomposites. After the asphaltene uptake, the peaks representing K-OMS-2 were observed to reduce in intensity. Furthermore, new peaks in the 1200–1600 cm−1 region were identified, indicating possible C
O/C
N stretching from asphaltene molecules.
![]() | ||
Fig. 5 FT-IR spectrum of (A) Cu-BTC, (B) CoMn2O4, and (C) K-OMS-2, before and after asphaltene adsorption. |
The prepared metal nanocomposites were further characterised for the surface area using BET analysis. A high surface area of 433 m2 g−1 and 400 m2 g−1 was observed for Cu-BTC and K-OMS-2, respectively. However, in the case of CoMn2O4, a lower surface area of 5 m2 g−1 was observed. The high surface area observed in Cu-BTC could be attributed to void spaces and the porous structures, while the fibre-like structure could have contributed towards high surface area in K-OMS-2. The low surface area of CoMn2O4 may be the result of particle agglomeration.
XRD spectra of the prepared metal nanocomposites are depicted in Fig. 6. From Fig. 6A, the XRD spectrum of Cu-BTC showed peaks representing (220), (400), (331), (422), (511), and (440) planes at 9.5°, 13.8°, 14.9°, 16.9°, 17.5°, and 19.1°, respectively. These peaks confirmed the face-centred cubic crystal lattice of Cu-BTC. The identified XRD peaks were consistent with the peaks in ICDD standard data, ICDD pdf number 00-062-1183.56
From Fig. 6B, peaks corresponding to the (202), (220), (113), (311), (004), (400), (332), (333), (511), (404), and (440) planes were identified at 29.4°, 31.2°, 33°, 36.5°, 39°, 45°, 52°, 54.5°, 59.2°, 60.8°, and 65.5°, respectively. The spectrum confirmed the body-centred tetragonal phase of CoMn2O4, matching JCPDS no. 18-0408.66,67
The XRD spectrum of K-OMS-2 shown in Fig. 6C exhibited peaks for planes (110), (200), (310), (211), (301), (411), (600), (521), and (002) at 12.5°, 17.5°, 28°, 37°, 42°, 50°, 56°, 60.5°, and 65.5°. The identified peaks confirmed the tetragonal crystalline structure of K-OMS-2, which was consistent with JCPDS: 29-1020 that represents cryptomelane.60
Further surface characteristics, such as acidic and basic functional groups, were determined by Boehm titration.68 The titration results revealed basic functional group contents of 0.60 mmol g−1, 0.96 mmol g−1, and 0.40 mmol g−1, and acidic functional group contents of 1.00 mmol g−1, 0.86 mmol g−1, and 1.14 mmol g−1, for Cu-BTC, CoMn2O4, and K-OMS-2, respectively.
The metal nanocomposites were used in the study of the effect of adsorbent dosage, which included varying the nanocomposite dosage from 2.5 g L−1 to 25 g L−1. The experiments were carried out at 30 °C, 150 rpm and 24 hours contact time, with an asphaltene concentration of 250 mg L−1 and the resulting relationship is depicted in Fig. S3 (ESI†). From Fig. S3A (ESI†), a 95% removal was achieved with the Cu-BTC dosage of 25 g L−1. However, a dosage of 12.5 g L−1 proved to be effective, since the asphaltene adsorption is observed to be 95%, and the removal appeared to saturate as the dosage was increased beyond 12.5 g L−1. Similar behaviour was observed for CoMn2O4, as depicted in Fig. S3B (ESI†). From Fig. S3C (ESI†), the removal of asphaltenes was found to increase with increasing dosage for dosages below 20 g L−1. However, the adsorption percentage remained constant for dosages above 20 g L−1, indicating saturation of the adsorbent's active sites.
Asphaltene adsorption using metal nanocomposites was evaluated for the effect of initial asphaltene concentration, and the adsorption behaviour is shown in Fig. S4 (ESI†). The studies were conducted by varying the initial asphaltene concentration from 100 mg L−1 to 1000 mg L−1, while keeping the adsorbent dosage constant (12.5 g L−1 for Cu-BTC and CoMn2O4, 20 g L−1 for K-OMS-2). The experiments were performed at 30 °C, with a stirring speed of 150 rpm, for 24 hours. From the figure, the adsorption percentage was found to decrease with increasing initial asphaltene concentration across all prepared materials. Maximum adsorption occurred at an asphaltene concentration of 100 mg L−1. The increase in asphaltene concentration led to a reduction in adsorption percentage, likely due to a decrease in available active sites.
The Langmuir isotherm model is given by:69
![]() | (1) |
The Freundlich isotherm model is given by:69
![]() | (2) |
The Temkin isotherm model is given by:70
![]() | (3) |
The Redlich–Peterson isotherm model is given by:71
![]() | (4) |
The Hill isotherm model is given by:72
![]() | (5) |
The isotherm model fitting for the asphaltene adsorption equilibrium data is depicted in Fig. 7, with model parameters tabulated in Table 1. Adsorption of asphaltenes onto Cu-BTC, CoMn2O4, and K-OMS-2 is shown in Fig. 7A, B and C, respectively. The model fitting was evaluated by using the χ2 value and r2 values, where the r2 value indicates the goodness of the fit, and χ2 quantifies the deviation of the experimental values from the model predictions. Since the r2 values were close, the goodness of fit was determined by χ2. The asphaltene adsorption using Cu-BTC was found to be governed by the Freundlich isotherm since the χ2 value is the least for this model. The Freundlich isotherm indicates a possible multilayer adsorption on heterogeneous adsorption sites of the adsorbent, and since nF ≫ 1, the adsorption is favourable. The CoMn2O4 system was found to follow the Langmuir isotherm model. The model describes adsorption processes in which adsorbate molecules form a monolayer on homogeneous adsorption sites. The χ2 for the Langmuir model fitting was found to be the lowest for the CoMn2O4 system; hence, the adsorption is likely to be monolayer in nature.73 Similarly, the adsorption of asphaltenes using K-OMS-2 was found to be explained by the Hill isotherm model. The Hill model describes cooperative adsorption in the system. According to the model parameters, asphaltenes’ adsorption promotes cooperative adsorption, thereby enhancing the uptake. The Langmuir isotherm parameters also provided the maximum monolayer adsorption capacity (qm) of the materials, and the qm was in the order K-OMS-2 (245.79 mg g−1) > CoMn2O4 (77.04 mg g−1) > Cu-BTC (50.59 mg g−1). The adsorption was strongly influenced by the surface acidity and basicity of the adsorbents. Among the materials, K-OMS-2 exhibited the highest acidity, leading to its maximum adsorption capacity.74 The qm for asphaltene adsorption onto K-OMS-2 was found to be one of the highest values reported in the literature.
Adsorption model | Parameter | Cu-BTC | CoMn2O4 | K-OMS-2 |
---|---|---|---|---|
Langmuir | qm (mg g−1) | 50.590 | 77.040 | 245.790 |
KL (L mg−1) | 0.006 | 0.006 | 0.007 | |
r2 | 0.980 | 0.968 | 0.986 | |
χ2 | 9.756 | 12.684 | 140.841 | |
Freundlich | KF (mg g−1) | 2.399 | 3.110 | 10.310 |
nF | 2.239 | 2.060 | 2.250 | |
r2 | 0.956 | 0.923 | 0.939 | |
χ2 | 6.593 | 21.674 | 479.178 | |
Temkin | KT (L mg−1) | 0.959 | 0.082 | 0.065 |
b (J mol−1) | 494.155 | 164.018 | 56.054 | |
r2 | 0.760 | 0.929 | 0.956 | |
χ2 | 52.022 | 22.442 | 198.896 | |
Redlich–Peterson | KRP (L g−1) | 9.352 | 0.436 | 0.838 |
αRP (L mg−1) | 3.573 | 0.002 | 1.45 × 10−4 | |
βRP | 0.566 | 1.138 | 1.489 | |
r2 | 0.964 | 0.951 | 0.982 | |
χ2 | 7.657 | 15.526 | 79.440 | |
Hill | qm (mg g−1) | 106.946 | 73.162 | 181.752 |
KD (mg L−1) | 65.335 | 197.275 | 1010.827 | |
nH | 0.579 | 1.071 | 1.447 | |
r2 | 0.968 | 0.950 | 0.982 | |
χ2 | 6.878 | 15.725 | 79.202 |
From Fig. S5A (ESI†), the adsorption of asphaltenes using Cu-BTC attained equilibrium in 0.6 h. Similarly, Fig. S5B (ESI†) shows that the equilibrium for asphaltene adsorption onto CoMn2O4 was observed at about 6 h of contact time, while equilibrium was attained in 2.5 h for K-OMS-2 (Fig. S5C, ESI†). The time-dependence experimental data were further interpreted using widely applied kinetic models: the PFO (eqn (6)), PSO (eqn (7)), and Elovich (eqn (8)) adsorption kinetic models.
The PFO model equation is given by,75
qt = qe·(1 − e−k1·t) | (6) |
The PSO kinetic model equation is given as,75
![]() | (7) |
The Elovich kinetic model equation is given as,76
![]() | (8) |
The kinetic model plots for asphaltene adsorption onto the prepared metal nanocomposite are shown in Fig. S6 (ESI†). The kinetic studies of asphaltene adsorption onto Cu-BTC, CoMn2O4, and K-OMS-2 are represented in Fig. S6A, B, and C (ESI†), respectively, and the model parameters are given in Table 2. The adsorption of asphaltenes by Cu-BTC was observed to follow the PFO model. The model suggests a possible physisorption, which could be due to the porous nature of Cu-BTC. The adsorption of asphaltenes onto CoMn2O4 was explained by the PSO model. The PSO model describes chemisorption-driven adsorption, and its fitting signifies a possible chemisorption mechanism.77 Similarly, asphaltene adsorption using K-OMS-2 was found to be governed by the Elovich model. The Elovich model is applicable for adsorption systems involving heterogeneous surfaces with chemisorption-driven interactions. The kinetic model parameters were analysed to determine the adsorption characteristics. The k1 and k2 values represent the rate of initial adsorption and driving force, respectively. These values were found to be higher for Cu-BTC, indicating rapid adsorption of asphaltenes onto Cu-BTC, a phenomenon which was also evident from the kinetic data. In addition, βE represents the extent of adsorption, which was found to be maximum for Cu-BTC. The observation could be attributed to the physisorption of asphaltenes onto Cu-BTC, as suggested by PFO models. The αE parameter denotes the chemisorption rate, which was found to be maximum for K-OMS-2.78 Asphaltenes are a highly polar class of compounds, with polarity arising from charged end functional groups. Therefore, chemisorption is expected. Both kinetic and adsorption isotherm studies support this mechanism.79 The predicted qe values from the fitted kinetic models were found to closely match the experimental qe values.
Adsorbent | PFO model | PSO model | Elovich model | |||||||||
---|---|---|---|---|---|---|---|---|---|---|---|---|
qe (mg g−1) | k1 (h−1) | r2 | χ2 | qe (mg g−1) | k2 (g mg−1 h−1) | r2 | χ2 | αE (mg g−1 min−1) | βE (g mg−1) | r2 | χ2 | |
Cu-BDC | 6.468 | 16.805 | 0.945 | 0.185 | 7.117 | 3.419 | 0.903 | 0.330 | 120.265 | 0.938 | 0.823 | 0.606 |
CoMn2O4 | 34.107 | 1.157 | 0.929 | 10.815 | 38.963 | 0.036 | 0.938 | 9.561 | 1024.742 | 0.127 | 0.936 | 9.734 |
K-OMS-2 | 141.620 | 15.701 | 0.758 | 335.897 | 150.846 | 0.157 | 0.894 | 147.238 | 36![]() |
0.053 | 0.995 | 5.890 |
The intraparticle diffusion model expression is given by,80
![]() | (9) |
The Boyd diffusion model equation is given as,81
Bt = −0.4977 − ln(1 − F) | (10) |
The transport mechanism of the adsorbate towards the adsorbent was analysed using the intraparticle diffusion model, providing insights into the adsorption mechanism. The model data are represented in Fig. S7 (ESI†). Fig. S7A, B, and C (ESI†) illustrate the intraparticle diffusion model for asphaltene adsorption onto Cu-BTC, CoMn2O4, and K-OMS-2, respectively.
From the figures, the adsorption mechanism can be described using three distinct zones, namely boundary layer diffusion, intraparticle diffusion, and equilibrium stage. Boundary layer diffusion is represented by the first linear segment of the curve, and this initial phase involves asphaltene molecules migrating towards the surface of the nanocomposite. Intraparticle diffusion is explained by the subsequent linear segment, which corresponds to asphaltenes penetrating the adsorbent's pores. The equilibrium stage is the final horizontal segment that indicates saturation, where adsorption ceases due to exhausted active sites. From Fig. S7A and B (ESI†), a rapid boundary layer diffusion of asphaltenes into Cu-BTC (within 6 min) and CoMn2O4 (within 10 min) was observed, followed by intraparticle diffusion that extended for 20 min for Cu-BTC and 4 h for CoMn2O4, respectively. However, in the case of asphaltene adsorption onto K-OMS-2, a slow film diffusion process was observed, extending up to 1 h, followed by an intraparticle diffusion process that continued for up to 3 h, as shown in Fig. S7C (ESI†).82
The mechanism of asphaltene adsorption can be further explained by identifying the rate-limiting step. Boyd's diffusion kinetics model was employed to determine the slowest step. Boyd's diffusion plot of Bt vs. t is shown in Fig. S8 (ESI†). A linear line passing through the origin suggests intraparticle diffusion as the slowest step. For plots that follow a linear trend without intersecting the origin or exhibit nonlinear trends, film diffusion governs the process. However, non-linear trends with a positive intercept were observed in Boyd's plots for the asphaltene adsorption systems. Therefore, the study suggests that the adsorption process is governed by film diffusion or external mass transfer.83 Typically, film diffusion dominates when the adsorbate has a high affinity for the adsorbent, a dilute system is used, the adsorbate particles are small, or mixing is poor.
ΔG0 = −R·T·ln(K) | (11) |
K (dimensionless) is calculated as follows:84
K = KL·Cs | (12) |
ΔG0 = ΔH0 − T·ΔS0 | (13) |
![]() | (14) |
The thermodynamic parameters were calculated using KL from isotherm plots (Fig. S9, ESI†), the van’t Hoff plot (shown in Fig. S10, ESI†), and eqn (11)–(14), which are tabulated in Table 3. The change in Gibbs free energy was found to be negative for the Cu-BTC and K-OMS-2 systems, but for CoMn2O4, negative values were observed at higher temperatures. The negative values suggest a spontaneous and favourable adsorption process, with the increasing negativity at higher temperatures indicating greater favourability. Similarly, positive entropy change values indicated an increase in randomness at the solid–liquid interface during adsorption.86 The negative enthalpy change reflects the exothermic nature of the adsorption. Values in the range of 40–800 kJ mol−1 represent a chemisorption-driven adsorption, while values below this range indicate physisorption.78 However, the results imply a chemisorption-driven adsorption mechanism for CoMn2O4 and K-OMS-2, whereas Cu-BTC exhibited characteristics of physisorption. The results were consistent with the observations from the kinetic studies. In the case of asphaltene adsorption onto Cu-BTC, the mechanism follows the PFO model, which indicates physisorption, while asphaltene adsorption onto CoMn2O4 and K-OMS-2 follows the PSO and Elovich models, respectively, which represent chemisorption. The pictorial representation of the adsorption mechanism is shown in Fig. S11 (ESI†).
Adsorbent | ΔH0 (kJ mol−1) | ΔS0 (J mol−1) | T (K) | ΔG0 (kJ mol−1) | KL (L mg−1) | r2 |
---|---|---|---|---|---|---|
Cu-BTC | −22.075 | 128.016 | 293 | −3.129 | 0.026 | 0.887 |
303 | −4.390 | 0.076 | 0.982 | |||
313 | −4.833 | 0.027 | 0.981 | |||
CoMn2O4 | −46.111 | 47.980 | 293 | 1.688 | 0.036 | 0.999 |
303 | 1.701 | 0.057 | 0.912 | |||
313 | −1.996 | 0.024 | 0.990 | |||
K-OMS-2 | −54.799 | 142.132 | 293 | −2.392 | 0.005 | 0.978 |
303 | −5.130 | 0.005 | 0.999 | |||
313 | −5.648 | 0.021 | 0.993 |
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Fig. 8 Thermal degradation profile of Cu-BTC, asphaltenes, and asphaltenes subjected to oxidation under Cu-BTC, CoMn2O4, and K-OMS-2. |
Fig. 8 illustrates the oxidation profiles of asphaltenes in the presence of the nanocomposites. From the figure, the Cu-BTC-catalysed asphaltene oxidation was observed at 540 °C, indicating a reduction in oxidation temperature, in comparison with non-catalysed oxidation. In addition, a 20% residual mass was observed which revealed the decomposition of the MOF, given that equal mass ratios were used in the analysis. To further investigate the oxidation phenomenon, the thermal degradation analysis of Cu-BTC was performed. The thermal degradation profile along with a previous study involving MOFs, confirmed the decomposition of Cu-BTC and the formation of metal oxides well before the asphaltene oxidation temperature.53 These observations demonstrate that Cu-BTC aids in asphaltene oxidation indirectly via its oxidation product, which acts as a catalyst. The metal oxide formed from Cu-BTC contributes to a 60 °C reduction in asphaltenes oxidation temperature.
Similarly, CoMn2O4 was studied for asphaltene oxidation. The thermal degradation profile showed a reduction in oxidation temperature from 600 °C to 440 °C. The stability of CoMn2O4 was also confirmed as the thermal profile remained unchanged above 440 °C, which was indicated by the horizontal trendline. Additionally, K-OMS-2 was studied for its capability in asphaltene oxidation, and the results indicated that K-OMS-2 reduced the oxidation temperature to 500 °C, showing its potential for regeneration. In both cases of asphaltene oxidation, the residual mass was observed to be about 50%, indicating complete oxidation of asphaltenes and the thermal stability of the nanocomposites. The thermal stability of the nanocomposites can be attributed to the high-temperature calcination step involved in the synthesis. However, K-OMS-2's high adsorption capacity, due to its tunnel-like pores and surface functional groups, did not significantly enhance oxidation, possibly due to the inefficiency of Mn phase formation during oxidation. These observations suggest that the catalytic oxidation capabilities of K-OMS-2 are limited, while it remains an efficient adsorbent.46,47 Meanwhile, the presence of basic sites enhances the catalytic activity of the materials; hence, CoMn2O4 outperformed Cu-BTC and K-OMS-2 in catalytic oxidation of asphaltenes.74
• Cu-BTC: precursors (copper nitrate, BTC, DMF, and ethanol) cost = INR 16300 kg−1. Total production cost = INR 16
500 kg−1.
• CoMn2O4: precursors (cobalt nitrate, manganese nitrate, ammonium hydroxide) cost = INR 3080 kg−1. Total production cost = INR 3150 kg−1.
• K-OMS-2: precursors (potassium permanganate, manganese sulphate, nitric acid) cost = INR 730 kg−1. Total production cost = INR 780 kg−1.
K-OMS-2 emerged as the most cost-effective material, offering the highest adsorption capacity (245.79 mg g−1) at the lowest expense.
Adsorption of asphaltenes significantly reduces energy consumption, resource use, and costs associated with asphaltene-related problems. Asphaltenes contribute to significant financial expenditure and pollution. This study provides a cost-effective, environmentally safe method for their removal. It also addresses the secondary environmental pollution that arises from disposal of spent adsorbents. The nanocomposites can generally be reused over multiple adsorption–desorption cycles as detailed in the reusability studies section. This approach also enables asphaltene recovery and utilisation. Furthermore, regeneration of the saturated adsorbents is also studied in the oxidation studies, which emphasises the reusability of the adsorbent. However, regeneration of the MOF is impractical due to framework decomposition at high temperatures, converting them into metal oxides. These oxides retain utility for alternative applications, enabling secondary material reuse.53,90
• Cu-BTC followed the Freundlich isotherm, indicating multilayer adsorption, with kinetic and thermodynamic studies suggesting physisorption dominance.
• CoMn2O4 adhered to the Langmuir isotherm (monolayer adsorption) and exhibited chemisorption behaviour.
• K-OMS-2 aligned with the Hill isotherm, reflecting cooperative adsorption, alongside chemisorption kinetics.
Intraparticle diffusion models revealed a multi-step adsorption process across all systems, with Boyd plots confirming film diffusion as the rate-limiting step. Regeneration studies revealed the decomposition of Cu-BTC below the asphaltene oxidation temperature rendering it unsuitable for reuse. CoMn2O4 and K-OMS-2 retained structural integrity, with CoMn2O4 showing particularly efficient regeneration due to thermal stability. These results highlight the exceptional adsorption performance of K-OMS-2 and superior catalytic capabilities of CoMn2O4, which makes them promising materials for industrial asphaltene management. However, studies using isolated asphaltenes may not yield the real behaviour of petroleum residues, since asphaltenes are specific to their source and crude oil contains a number of other polyaromatic species that can interfere in real-time samples. Hence, future work should investigate interactions with additional polyaromatic species under real-time conditions, and be expanded to include asphaltenes from diverse geological sources, given their composition-dependent behaviour.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d5ma00106d |
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