1. Introduction
Carbon dioxide (CO2) capture and storage is a key strategy to mitigate greenhouse gas emissions and combat climate change. One of the major challenges in this area is to identify cost-effective and efficient materials for CO2 capture and storage.1,2 Porous organic materials (POMs) have emerged as one of the most promising materials for CO2 capture due to their high surface area, tunable functionality, and controllable pore size.3 POMs are organic compounds that have a highly porous structure and contain functional groups that can selectively adsorb CO2. The design and synthesis of POMs for CO2 capture is a rapidly growing research area, and various POMs, including porous aromatic frameworks (PAFs), porous organic polymers (POPs), and covalent organic frameworks (COFs), have been developed.4 PAFs are a subclass of POMs that have a rigid and stable framework with a high degree of conjugation, which allows for strong interactions with CO2 molecules.5 PAFs have shown promising results for CO2 capture due to their high CO2 adsorption capacity, selectivity, and excellent stability under a wide range of conditions. POPs are another class of POMs that have tunable properties, including pore size and surface area, which can be tailored for CO2 capture. COFs are a subclass of POMs that have a well-defined crystalline structure, and their properties can be precisely controlled by design.6 The development of POMs for CO2 capture has been driven by the need for highly efficient and cost-effective materials for industrial-scale CO2 capture.7 The conventional CO2 capture technologies, including amine-based absorption and adsorption technologies, have several limitations, including high energy consumption, corrosion issues, and low CO2 adsorption capacity.8 POMs offer several advantages over conventional CO2 capture technologies, including high CO2 adsorption capacity, high selectivity, and low energy consumption. Additionally, POMs can be regenerated by simple processes, making them ideal for large-scale industrial applications.9 The development of POMs for CO2 capture is a highly interdisciplinary research area that involves the synthesis of novel materials, fundamental studies of their properties and mechanisms, and optimization of their performance for real-world applications. In recent years, several studies have reported the synthesis and characterization of novel POMs for CO2 capture, including PAFs, POPs, and COFs. The properties of these materials have been investigated using various techniques, including X-ray diffraction (XRD), nitrogen adsorption-desorption isotherms, Fourier transform infrared spectroscopy (FTIR), and solid-state nuclear magnetic resonance (SSNMR) spectroscopy.10,11 Despite the significant progress made in the development of POMs for CO2 capture, several challenges remain. One of the key challenges is the optimization of the performance of POMs for real-world applications, including their stability under harsh operating conditions, their scalability, and their cost-effectiveness. Additionally, the development of POMs for CO2 capture requires a deep understanding of the fundamental mechanisms of CO2 adsorption and desorption, which is still an active area of research.12,13
Porous aromatic Schiff bases materials have gained significant attention as a promising class of materials for CO2 capture and storage applications due to their high surface area, porosity, and chemical stability.14,15 Porous aromatic Schiff base materials are a type of porous organic polymers that are synthesized by the condensation of aldehydes and amines under appropriate conditions.16 These materials possess a rigid and stable framework consisting of interconnected pores and channels, which offer high surface area and high porosity. The unique chemical structure of Porous aromatic Schiff base materials provides them with a large number of adsorption sites, which can selectively bind CO2 molecules over other gases.17-19 Recent studies have shown that Porous aromatic Schiff base materials exhibit exceptional CO2 sorption properties, making them a potential candidate for carbon capture applications.20,21 Porous aromatic Schiff base materials can capture CO2 through a range of mechanisms such as physisorption, chemisorption, and even reversible covalent bonding. Furthermore, porous aromatic Schiff base materials can be easily synthesized with tunable properties, making them highly versatile and suitable for a range of applications.22 In this context, this study aims to investigate the potential of porous aromatic Schiff base materials as a highly effective media for CO2 storage. The study will review the synthesis and characterization of porous aromatic Schiff base materials, their CO2 sorption properties, and the effect of various parameters such as temperature, pressure, and gas composition on their CO2 adsorption properties.23,24 Overall, this study is expected to provide valuable insights into the design of novel materials for CO2 capture and storage, which is a critical area of research for achieving a sustainable future.25 The use of porous aromatic Schiff base materials as an effective media for CO2 storage could contribute to reducing greenhouse gas emissions and mitigating climate change.26,27 The results of this study could be useful for developing new carbon capture technologies that are cost-effective and efficient. This study, we present the utilization of Schiff bases, which are highly aromatic and porous, as an effective CO2 capture media at 40 bars and 323 K.
2. Experimental
All chemicals utilized in this study were of the highest quality possible and were used directly from the metal chloride salts (CoCl2.6H2O, NiCl2.6H2O, CuCl2.2H2O, and ZnCl2) rather than undergoing any additional purification steps.
2.1. Instrumentation
Micrometric Surface Area and Porosity Analyzers, the nitrogen adsorption-desorption isotherms for gas storage samples (Co(II), Ni(II), Cu(II), and Zn(II)) complexes of synthesized Schiff base, in Tehran Iran, were analyzed using a Micro Active for TriStar II Plus Version 2.03 micrometric analyzer. Using Barrett-Joyner-hypothesis, Halenda's analyzer determined the pore volume, diameter, and pore size distribution of the sample under investigation (BJH). Field emission scanning electron microscopy (FESEM) and gas storage of Schiff base complexes (Co(II), Ni(II), Cu(II), and Zn(II) were performed using a ZEISS system model: Sigma VP from the USA at an accelerating voltage of 10Kv. When it comes to ligand's gas storage of Schiff base complexes (Co(II), Ni(II), Cu(II), and Zn(II)), tests for EDX and mapping were conducted by Oxford Instruments, UK.
2.2. Synthesis of malonic acid di hydrazide
The first step of the ligand synthesis process includes making malonic acid di hydrazide, as explained here. Malonic acid diethylester (10 g, 0.062 mol) was dissolved in 10 ml of ethanol and left to stir at room temperature. Aqueous hydrazine (10 g, 0.25 mol) was added dropwise while being constantly stirred, then the reaction was refluxed for 6 hours before being stopped and cooled down to ambient temperature. The formed residue was filtered and the precipitate was washed with dry ether and methanol. Absolute ethanol was used to recrystallize the product giving a white precipitate 80 % yield (7.1 g), m.p. 159 °C. Malonic acid di hydrazide preparation is shown in Scheme 1.
Scheme 1. Steps of preparation of malonic acid dihydrazide.
2.3. Synthesis of Schiff base ligand (L)
In mole ratio 1:2, 2-hydroxy-1-naphthaldehyde (2.6 g, 0.015 mol) in 10 mL of methanol was added slowly with stirring to prepared malonic acid dihydrazide solution (1.0 g, 0.004 mol), in 10 mL of methanol. Then 2-3 drops of glacial acetic acid were added to the reaction mixture. The mixture was left to react under reflux conditions for 5 hr, then yellow crystals glossy precipitate was formed which was collected by filtration, washed, and recrystallized by hot ethanol. The product was dried over anhydrous CaCl2 in a vacuum to give 80 % (2.88 g) yield, m.p 244 °C see Scheme 2 for the reaction Scheme.
Scheme 2. Steps of Preparation of Schiff base ligand.
2.4. Synthesis of Schiff base metal complexes
The copper complex was synthesized by dissolving 0.2 g, 0.001 mole of the Copper chloride dehydrate in 10 ml methanol and dissolving (0.5 g, 0.0001 mol) of the synthesized ligand in 10 ml of methanol with continuous stirring for about (10 min) and adding few drops of DMF to complete solubility, followed by adding the solution of the dissolved metal salt onto a solution of the dissolved ligand in the mole ratio (1:1) of (metal-ligand) and adding 1-2 drops of trimethylamine. The mixture was stirred under reflux for 5 hr until the precipitate was formed. The colored complexes were separated by filtration, washed with methanol, recrystallized, and left to dry at room temperature for 24 hours. All other complexes (CoCl2. 6H2O, NiCl2.6H2O, and ZnCl2) were prepared using the same procedure as shown in Scheme 3 with good to very good percentage yield see Table 1.
Scheme 3. Preparation of Schiff base Metal Complexes.
Table 1. The physical properties of the prepared compounds
3. Results and Discussion
The ligand was synthesized in two steps firstly malonyldihydrazide was synthesized from a reaction of malonic acid with two moles of hydrazine. The crude product was purified by recrystallization from absolute ethanol. The pure product was reacted with two moles of 2-hydroxy-1-naphthaldehyde to produce the target ligand which was purified as well by recrystallization. Finally, the prepared ligand was used to synthesized five new complexes by reacting it with corresponding metallic chloride. The percentage yields and physical features of prepared molecules were summarized in Table 1. Various techniques were used to characterize the chemical structure of synthesized materials as will be explained in the next sections.
3.1. Characterization of Schiff Bases ligand by 1H-NMR Spectroscopy
The synthesized ligand chemical structure was characterized using 1H NMR spectroscopy. Hence the 1H NMR spectrum shows all needed peaks at the corresponding environments, integrations, and multi-plicity to demonstrate the chemical structure of the ligand. The proton of the imine group (N = CH) gives a strong sharp singlet peak at 8.43 ppm with the integration two because the structure has two symmetrical imine groups. The exchange protons of (NH and OH) groups have shown singlet peaks at chemical shifts 10.88 and 8.11 ppm. It is suggested that 10.88 ppm belongs to the NH group because it is next to the carbonyl group which causes the de-shielding of protons. On the other hand, the protons of aromatic regions show peaks at regions between 7.15 to 7.69 ppm which is the aromatic region with required integration(12). Finally, the CH2 group showed a singlet peak at the aliphatic region 3.07 ppm, this is because it is next to two carbonyl groups as shown in Fig. 1. From all the above, it can be said that the ligand has been synthesized successfully with a high percentage of purity. The 1H NMR data of the syn-thesized ligand were summarized in Table 2.
Fig. 1. 1H NMR of synthesized ligand.
Table 2. 1H NMR data of synthesized ligand
3.2. Characterization of Schiff Bases ligand by 13C-NMR Spectroscopy
The synthesized ligand chemical structure was characterized using 13C NMR spectroscopy. Hence the 13C NMR spectrum shows all needed peaks at the corresponding environments to demonstrate the chemical structure of the synthesized ligand. The carbon atom of the imine group (N = CH) gives a peak at 148.10 ppm where Schiff base groups spouse to be. On the other hand, carbonyl groups show a peak at 167.11 ppm because oxygen has a higher electronegativity than nitrogen which causes more de-shielding. However, there is still a peak above the aromatic region (157.37 ppm) which could belong to aromatic carbon atoms next to the oxygen. Thus, the carbon atoms of aromatic regions show nine peaks at regions between 112.79 to 135.89 ppm which is the aromatic region. Finally, the CH2 group showed a peak at the aliphatic region 48.89 ppm, this is because it is next to two carbonyl groups as shown in Fig. 2. From all the above, it can be said that the ligand has been synthesized successfully with a high percentage of purity. The 13C NMR data of the synthesized ligand were summarized in Table 3.
Fig. 2. 13C NMR of synthesized ligand.
Table 3. 13C NMR data of synthesized ligand
3.3. Characterization of Schiff Bases ligand and its complexes by FTIR
Fourier Transform Infrared Spectroscopy is a valuable method to determine the functional groups and the creation of new bands in the manufactured compounds. Table 4 reports the FTIR spectroscopy results for the ligand and their produced complexes. Figs. 3-7 shows the FTIR spectrums of synthesized ligand and its complexes.
Table 4. FTIR Spectroscopy Measurements of ligand, and its Complexes
Fig. 3. FTIR-Spectrum of Schiff Base ligand.
Fig. 4. FTIR-Spectrum of Co(II) complex.
Fig. 5. FTIR-Spectrum of Ni(II) Complex.
Fig. 6. FTIR-Spectrum of Cu(II) Complex.
Fig. 7. FTIR-Spectrum of Zn(II) Complex
The tetradentate Schiff base ligand displays a sharp band at 3109 cm−1, and 1596 cm−1 assigned to ν(C-H)Ar, and ν(C = C) respectively.28 A strong band appeared at 1613 cm−1 assigned to the stretching band of the azomethine group. The coordination of the metal ions to the nitrogen azomethine leads to a shift-up in the frequency of ν(C = N) value due to the decreases in the electron density on the azomethine after donating electrons of nitrogen to the partially filled d-orbitals of the metal ions(II).29 The IR-spectra of the complexes, exhibit characteristic bands around (1613-1623) cm−1 showing that the metal ions coordinate to the ligand via the azomethine nitrogen atom.30 The stretching vibrations of the phenolic hydroxyl group cause a large band at 3409-3479 cm−1 in the IR spectra of the ligands. Intermolecular hydrogen bonding between the phenolic and azomethine groups accounts for the broadness. New stretching modes were observed in the far-infrared spectra of the complexes that didn't exist in the spectrum of ligand at (420-476) cm−1, (526-563), and (327-352) cm-1 which are attributed to υ (M-N), υ (M-O) and υ (M-Cl) as evidence on the formation bonds between the metal ions(II) and the nitrogen azomethine, hydroxyl group and chloride, respectively.
3.4. Energy dispersive X-ray (EDX) Analysis of Synthesized Schiff base Complexes
Energy dispersive X-ray (EDX) was used for synthetic Schiff base complexes to offer details on the elemental composition of solid surfaces.31 Field emission scanning electron microscopy (FESEM), a standard chemical microanalysis technique, and EDX are coupled to derive the chemical formula of produced compounds. The EDX mapping of the complexes, as seen in Fig. 8, reveals the elemental chemical compositions of the produced complexes.
Fig. 8. EDX graphs of (a) Cu(II), (b) Zn(II), (c) Ni(II), and (d) Co(II) complexes.
3.5. Inorganic complexes as gas storage materials
3.5.1. Surface area determination
Complexes were subjected to 77 K nitrogen gas adsorption and desorption experiments using a surface area measuring equipment. By using the Brunauer, Emmett, and Teller (BET) approach, specific surface areas of complexes were measured and gas volume-relative pressure isotherms were generated. The “nitrogen adsorption method”, which made it easier to analyze micro-, meso-, and macropore sizes and specific surface areas of the pores, yielded complicated pore diameters and sizes, which were presented in Table 5 and Fig. 9-12.
Table 5. Surface area and pore size distribution of metal complexes obtained by N2 Adsorption
Fig. 9. N2 Adsorbed isotherm of Co(II) complex.
Fig. 10. N2 Adsorbed isotherm of Ni(II) complex.
Fig. 11. N2 Adsorbed isotherm of Zn(II) complex
Fig. 12. N2 Adsorbed isotherm of Cu(II) Complex.
According to categorization in The International Union of Pure and Applied Chemistry (IUPAC), which correlates to meso pore size generally, results in Table 4 reveal the typical pore diameter is in the 2 to 50 nm range. According to Table 5, rather than the size of the particular pore volume, the size of a specific surface area is dependent on the size of the pores. Because the wall surface area increases with decreasing pore size of used materials. Additionally, it was shown that the specific surface area and pore volume were connected to the complexes' structure and adsorption capacity.32 There were no monolayers and only very weak interactions between the gas and adsorbents, as shown by the type III isotherms seen in (Fig. 2, Fig. 3, Fig. 4 and Fig. 5). The fact that the isotherms began at the origin indicates that the heat of adsorption and condensation were equivalent in intensity. Positive CO2 gas adsorption on the surface of metal complexes resulted in a significant rise in adsorption as the pressure rose.33,34 The potency and effectiveness of metal complexes in gas storage are enhanced by the strong stacking interactions, which also regulate the 2D solid-state packing and obstruct interpenetration, according to measurements of CO2 gas sorption at high pressures (up to 40 bar).
3.5.2. FESEM of metal complexes
The FESEM method was used to assess the morphology, porosity, and particle size of the produced Schiff base Co(II), Ni(II), Cu(II), and Zn(II) complexes. Images produced by the FESEM demonstrate superb resolution, clarity, and minimal distortion of the investigated particles.35,36 Schiff base complexes' homogeneous, amorphous, and rough surfaces are exposed in Fig. 13-16, and these characteristics make them an ideal surface for CO2 gas extraction. The complexes' images show minute particles creating various shapes and sizes through homogeneous agglomeration. According to the IUPAC pores classifications,37 the FESEM pictures indicate that the compounds have a mesoporous structure, supporting the findings of the BJH method. Macro-pores are those with a diameter more than 50 nm, Meso-pores have pores that range in size from 2 nm to 50 nm, and Micro-pores are those with a diameter of under 2 nm.
Fig. 13. Field emission scanning electron microscopy (FESEM) image of Cu(II) complex.
Fig. 14. Field emission scanning electron microscopy (FESEM) image of Ni(II) complex.
Fig. 15. Field emission scanning electron microscopy (FESEM) image of Zn(II) complex.
Fig. 16. Field emission scanning electron microscopy (FESEM) image of Co(II) complex.
The sorption of porous aromatic Schiff base complexes (Co(II), Ni(II), Zn(II), and Cu(II)) was studied at fixed pressure and temperature 50 bars and 323 K. Fig. 17 shows the adsorption isotherms of CO2 on metal complexes and the gases uptakes are recorded in Table 6.
Fig. 17. CO2 adsorption isotherms of metal complexes.
Table 6. CO2 capacity for metal complexes
Because they have a high capacity to create van der Waals and dipole-dipole interactions between the adsorbent and adsorbate, porous aromatic Schiff base complexes (Co(II), Ni(II), Zn(II), and Cu(II)) exhibited the effectiveness of CO2 adsorption. According to Fig. 17, the CO2 adsorption capacities for Co(II), Ni(II), Zn(II), and Cu(II) complexes, respectively, were 15.5, 18.3, 20.6, and 33.1 cm3/g. Evidently, when compared to the other investigated compounds, Cu(II)) complex showed the greatest efficiency of CO2 adsorption capacity. Other ways to boost adsorption effectiveness include strong dipole-dipole interactions and heteroatoms found inside molecules. Therefore, porous materials with oxygen and nitrogen atom units are efficient at trapping CO2 gas in a specific manner.
4. Conclusions
In conclusion, Carbon Dioxide (CO2) storage is a crucial challenge faced by the scientific community today, and extensive research is being carried out to find a viable solution to this issue. One of the promising approaches is the use of porous aromatic Schiff Bases as a highly effective media for CO2 storage and studied the influence of their morphologies. This technology has shown impressive results in CO2 adsorption and storage, and it is an excellent alternative to traditional methods of CO2 storage. All spectral data from this investigation showed that the produced Schiff base compound acted as a tetra dentate ligand, attaching to the metal ion via the phenolic oxygen and the azomethine nitrogen. The analytical results also showed that the M:L ratio is 1:1 in all the produced complexes, which is consistent with a mononuclear structure. porous aromatic Schiff Bases offer a high surface area and tunable chemical properties, which make them ideal for CO2 adsorption. Furthermore, their porous structure allows for the trapping and storage of CO2 molecules, leading to a reduction in greenhouse gas emissions. The application of this technology can potentially lead to the development of cost-effective, energy-efficient, and environmentally friendly solutions to tackle the issue of CO2 storage. In summary, the use of porous aromatic Schiff Bases as a highly effective media for CO2 storage is a promising area of research that holds significant potential for addressing the problem of climate change. Further research and development in this field is necessary to refine the technology and make it more practical for widespread use.
Conflict of Interest
The authors declare no conflict of interest.
References
- G. Zeng, Y. Zhang, L. Li, Y. Huang, M. Li, and C. Yan, Journal of Materials Chemistry A, 8(7), 3223-3244 (2020). DOI: 10.4324/9780429448935
- J. Wang, Y. Wang, H. Hu, Q. Yang, and J. Cai, Nanoscale, 12(7), 4238-4268 (2020). https://doi.org/10.1039/C9NR09697C
- J. Du, H. Ouyang, and B. Tan, Chemistry-An Asian Journal, 16(23), 3833-3850 (2021). https://doi.org/10.1002/asia.202100991
- G. Ji, Y. Zhao, and Z. Liu, Green Chemical Engineering, 3(2), 96-110 (2022). https://doi.org/10.1016/j.gce.2021.11.011
- F. Tang, J. Hou, K. Liang, J. Huang, and Y. N. Liu, European Journal of Inorganic Chemistry, 37, 4175-4180 (2018). https://doi.org/10.1002/ejic.201800764
- P. Bhanja, A. Modak, and A. Bhaumik, ChemCatChem, 11(1), 244-257 (2019). https://doi.org/10.1002/cctc.201801046
- X. Wu, R. Guan, W. T. Zheng, K. Huang, and F. Liu, Journal of Materials Science, 56, 9315-9329 (2021). https://doi.org/10.1007/s10853-021-05835-z
- L. Zou, Y. Sun, S. Che, X. Yang, X. Wang, M. Bosch, Q. Wang, H. Li, M. Smith, S. Yuan, and Z. Perry, Advanced Materials, 29(37), 1700229 (2017). https://doi.org/10.1002/adma.201700229
- N. Kundu and S. Sarkar, Journal of Environmental Chemical Engineering, 9(2), 105090 (2021). https://doi.org/10.1016/j.jece.2021.105090
- J. Chen, L. Jiang, W. Wang, Z. Shen, S. Liu, X. Li, and Y. Wang, Journal of Colloid and Interface Science, 609, 775-784 (2022). https://doi.org/10.1016/j.jcis.2021.11.091
- A. Chowdhury, S. Bhattacharjee, R. Chatterjee, and A. Bhaumik, Journal of CO2 Utilization, 65, 102236 (2022). https://doi.org/10.1016/j.jcou.2022.102236
- K. Huang, J.Y. Zhang, F. Liu, and S. Dai, Acs Catalysis, 8(10), 9079-9102 (2018). https://doi.org/10.1021/acscatal.8b02151
- D. Luo, T. Shi, Q. Li, Q. Xu, M. Stromme, Q. F. Zhang, and C. Xu, Angewandte Chemie International Edition, 62, e202305225 (2023). https://doi.org/10.1002/anie.202305225
- T. T. Liu, J. Liang, Y. B. Huang, and R. Cao, Chemical Communications, 52(90), 13288-13291 (2016). https://doi.org/10.1039/c6cc07662a
- Z. Yuan, M. R. Eden, and R. Gani, Industrial & Engineering Chemistry Research, 55(12), 3383-3419 (2016). https://doi.org/10.1021/acs.iecr.5b03277
- Y. Li, C. Zhang, X. Li, and H. Jiang, Journal of Materials Chemistry A, 7(24), 14309-14324 (2019). https://doi.org/10.1039/C9CP06925A
- A. A. Yaseen, E. T. Al-Tikrity, G. A. El-Hiti, D. S. Ahmed, M. A. Baashen, M. H. Al-Mashhadani, and E. Yousif, Processes, 9(4), 707 (2021). https://doi.org/10.3390/pr9040707
- Y. Wang, C. Kang, Z. Zhang, A. K. Usadi, D. C. Calabro, L. S. Baugh, Y. D. Yuan, and D. Zhao. ACS Sustainable Chemistry & Engineering, 10(1), 332-341 (2021). https://doi.org/10.1021/acssuschemeng.1c06318
- M. G. Rabbani, A. K. Sekizkardes, O. M. El-Kadri, B. R. Kaafarani, H. M. El-Kaderi. Journal of Materials Chemistry, 22(48), 25409-25417 (2012). https://doi.org/10.1039/C2JM34922A
- M. S. B. Reddy, D. Ponnamma, K. K. Sadasivuni, B. Kumar, and A. M. Abdullah,. RSC Advances, 11(21), 12658-12681 (2021). https://doi.org/10.1039/D0RA10902A
- A. Rehman and S. J. Park, Journal of CO2 Utilization, 21, 503-512 (2017). https://doi.org/10.1016/j.jcou.2017.08.016
- W. Xie, D. Cui, S. R. Zhang, Y. H . Xu, and D. L. Jiang, Materials Horizons, 6(8), 1571-1595 (2019). https://doi.org/10.1039/C8MH01656A
- R. M. Omer, E. T. B. Al-Tikrity, G. A. El-Hiti, M. F. Alotibi, D. S. Ahmed, and E. Yousif, Processes, 8, (2020). https://doi.org/10.3390/pr8010017
- B. Dziejarski, J. Serafin, K. Andersson, and R. Krzyzynska, Materials Today Sustainability, 24, 100483 (2023). https://doi.org/10.1016/j.mtsust.2023.100483
- M. N. Anwar, N. F. Fayyaz, M. F. Sohail, M. Khokhar, W. D. Baqar, K. Khan, K. Rasool, M. Rehan, and A. S. Nizami. Journal of Environmental Management 226, 131-144 (2018). https://doi.org/10.1016/j.jenvman.2018.08.009
- T. Saleh, E. Yousif, E. Al-Tikrity, D. Ahmed, M. Bufaroosha, M. Al-Mashhadani, and A. Yaseen, Materials Science for Energy Technologies, 5, 344-352 (2022). https://doi.org/10.1016/j.mset.2022.08.002
- D. S. Ahmed, G. A. El-Hiti, E. Yousif, A. A. Ali, and A. S. Hameed. Journal of Polymer Research, 25, 1-21, (2018). https://doi.org/10.1007/s10965-018-1474-x
- N. Emad, G.A . El-Hiti, E. Yousif, D. S. Ahmed, and B. M. Kariuki, Results in Chemistry, 6, 101137 (2023). https://doi.org/10.1016/j.rechem.2023.101137
- N. Emad, G. A. El-Hiti, E. Yousif, D. S. Ahmed, M. Fadhil, and B. M. Kariuki, Results in Chemistry, 6, 101099 (2023). https://doi.org/10.1016/j.rechem.2023.101099
- D. S. Ahmed, G. A. El-Hiti, E. Yousif, A. S. Hameed, and M. Abdalla. Polymers, 9, 336 (2017). https://doi.org/10.3390/polym9080336
- Z. N. Mahmood, M. Alias, E. Yousif, S. Baqer, M. Kadhom, D. Ahmed, A. Ahmed, A. Husain, M. Yusop, and A. Jawad, A. Pollution, 9(2), 693-701 (2023). https://doi.org/10.22059/poll.2022.348855.1632
- A. A. Yaseen, E. Yousif, E. T. Al-Tikrity, M. Kadhom, M. Yusop, and D. S. Ahmed. Pollution, 8(1), 239-248 (2022). doi: 10.22059/poll.2021.328835.1161
- O. G. Mousa, E. Yousif, A. A. Ahmed, G. A. El-Hiti, M. H. Alotaibi, and D. S. Ahmed. Applied Petrochemical Research, 10, 157-164 (2020). https://doi.org/10.1007/s13203-020-00255-7
- S. H. Mohamed, A. S. Hameed, E. Yousif, M. H. Alotaibi, D. S. Ahmed, and G. A. El-Hiti, Processes, 8, 1488 (2022). https://doi.org/10.3390/pr8111488
- O. Erdem and E. Yildiz, Inorganica Chimica Acta, 438, 1-4 (2015). https://doi.org/10.1016/j.ica.2015.08.015
- S. Sansul, E. Yousif, D. S. Ahmed, G. A. El-Hiti, B. M. Kariuki, H. Hashim, and A. Ahmed. Polymers 15(14), 2989 (2023). https://doi.org/10.3390/polym15142989
- S. A. Mahdi, A. A. Ahmed, E. Yousif, D. Ahmed, M. H. Al-Mashhadani, and M. Bufaroosha. Materials Science for Energy Technologies, 5, 197-207 (2022). https://doi.org/10.1016/j.mset.2022.02.002