Chemical structures and compositions of the bio-nanocomposite including MFe2O4 nanoparticles
ATR-FTIR was used to analyze the chemical structures of the HB, AHB and, containing metal ferrite, MFe2O4, bio-nanocomposites. The ATR-FTIR spectra of the HB and AHB are given in Fig. S1. In the spectrum of HB, characteristic bands, that is given in Table 1, of cellulose, hemicellulose, lignin and pectin main component of agricultural biomass are seen. The bands in cellulose and hemicellulose were seen between 3630 and 3000 cm− 1, which correspond to the O-H functional group, and between 2995 and 2795 cm− 1, which represent the aliphatic saturated C-H stretching. The C = O stretching in pectin is what causes the observed band at 1735 cm− 1. The bands at 1633, 1589, 1502, and 1453 cm− 1 are caused by C = C stretching vibration in lignin's aromatic or aliphatic molecules. The sharp band observed at 1020 cm− 1 is corresponding to the stretching vibration C-O-C of the cellulose and hemicellulose (Maaloul et al., 2017; Mihajlović et al., 2021; Mwaikambo and Ansell, 2002; Ouajai and Shanks, 2005; Zaman et al., 2012; Zhang et al., 2016).
Table 1
Functional groups observed in FTIR spectra of the HB
Wavenumber (cm− 1) | Vibration | Source |
3630 − 3000 | O-H stretching | Cellulose, hemicellulose |
2995 − 2795 | C-H symmetric stretching | Cellulose, hemicellulose |
1739 | C = O stretching | Pectin |
1633, 1589, 1502, 1453 | C = C aromatic and olefinic stretching | Lignin |
1423 | H-C-H and O-C-H in-plane bending | Cellulose |
1371 | CH plane bending | Cellulose, hemicellulose |
1320 | CH2 bending | Cellulose |
1231 | C-O-C symmetric stretching | Cellulose, hemicellulose |
1157 | C-O-C symmetric stretching | Cellulose, hemicellulose |
1026 | C-C, C-OH ring and side group bending | Cellulose, hemicellulose |
895 | C-O-C, C-C-O and C-C-H stretching | Cellulose |
After oxidation of the hemp biomass with HNO3/H2SO4 mixture, new bands are observed that not observed in the HB spectrum. The presence of new bands in the FTIR spectrum of AHB, including those associated with C-N (1318, 1357 cm− 1), O = S = O and S-OH (1030, 1057, 1105, 1157 cm− 1) (Manzoor et al., 2022; Santiago et al., 2018), as well as the bands associated with C-S and N-O stretching vibrations at 620 and 660 cm− 1, respectively, is evidence of the modification of the hemp biomass.
When the FTIR spectra of the bio-nanocomposites containing the metal ferrite nanoparticles shown in Fig. 1 are examined, the bands attributed to the Fe-O and M-O vibrations at 400–600 cm− 1 observed in the tetrahedral and octahedral crystal lattices in spinel ferrite compounds (Al Kiey et al., 2022; Bilal et al., 2022; Bodaghi et al., 2020; Jacob et al., 2011; Lawal Usman et al., 2022; Shabani et al., 2021), it clearly indicate that bio-nanocomposites including metal ferrite have been synthesized. Moreover, it is quite remarkable that the O-H stretching in the range of 3600 − 3050 cm− 1 and the stretching intensities attributed to the sulfonyl groups in the range of 1030–1157 cm− 1 decrease in the order of Mn, Cd, Co, Ni and Cu, respectively, in spinel ferrite-containing composites. In contrast to AHB-Cd and AHB-Mn, the spectra of AHB-Cu, AHB-Ni, and AHB-Co show intense and sharp bands at 1425 and 870 cm− 1, corresponding to the M(Cu, Ni, Co)-O-Fe vibration, indicating a stronger interaction between biomass and spinel ferrite compounds (Charradi et al., 2022). These clearly demonstrate that there are different interactions between the functional groups of the biomaterial and spinel compounds in the formation of bio-nanocomposites. Zeta potential values (for AHB-CuFe2O4:-25.7 mV, AHB-NiFe2O4:-55 mV, AHB-CdFe2O4:-42.4 mV, AHB-MnFe2O4:-38.8 mV and AHB-CoFe2O4:-31.9 mV) also support these interactions. AHB-CuFe2O4 has a smaller negative potential of -25.7 mV, which can be attributed to the presence of less electronegative - SO3− and -OH groups in its backbone (Li et al., 2022). This is also clearly seen in its FTIR spectrum because belonging to bands of -SO3− and -OH groups are not appearing.
EDX was utilized to analyses the element composition of the MFe2O4 bio-nanocomposites, and the results are presented with in Table 2. As seen in the table, Fe/M ratios in bio-nanocomposites are quite close to each other, except for AHB-CoFe2O4, indicating that AHB-CuFe2O4, AHB-NiFe2O4, AHB-CdFe2O4 and AHB-MnFe2O4 have similar spinal structures.
Table 2
Elemental composition of the AHB-MFe2O4
AHBMFe2O4 | M | Fe | C | O | N | S | Fe/M |
CuFe2O4 | 2.34 | 3.76 | 33.29 | 51.47 | 8.22 | 0.92 | 1.61 |
NiFe2O4 | 2.31 | 3.68 | 40.75 | 40.17 | 12.12 | 0.98 | 1.59 |
CdFe2O4 | 1.63 | 1.87 | 25.46 | 61.16 | 8.20 | 1.68 | 1.15 |
MnFe2O4 | 2.62 | 4.15 | 42.80 | 40.15 | 9.32 | 0.96 | 1.58 |
CoFe2O4 | 2.11 | 4.86 | 46.14 | 37.53 | 8.46 | 0.91 | 2.30 |
X-ray diffraction (XRD) and morphological analysis of the bio-nanocomposite including MFe2O4 nanoparticles
Typical XRD patterns that determine the lattice plane and orientation of synthesized CuFe2O4, NiFe2O4, CdFe2O4, MnFe2O4 and CoFe2O4 nanoparticles in the modified hemp biomass (AHB) with nitric acid /sulfuric acid mixture and SEM images of the relevant samples are given in Figs. 3(a-e), respectively.
It was determined that the XRD patterns of the nanoparticles produced in the modified hemp biomass were compatible with the characteristic diffraction peaks of the relevant pure nanoparticles in the literature. It was observed that the XRD patterns of the synthesized AHB-CuFe2O4, AHB-NiFe2O4 and AHB-CoFe2O4 samples had a more crystalline structure compared to the AHB-CdFe2O4 and AHB- MnFe2O4. The characteristics diffraction peaks for the AHB-CuFe2O4 were seen the lattice planes of (1 1 1), (2 2 0), (3 1 1), (2 2 2), (1 1 1), (4 0 0) and (3 3 3) at 2θ angle with 16.98, 30.28, 31.67, 35.35, 38.23, 45.67, 55.25 and 56.39 degrees in succession. The (1 1 1) and (1 1 3) crystal planes in the XRD patterns for AHB-CuFe2O4 are originated from the presence of CuO in the structure of the sample. On the other hand, spherical formations of nanoparticles were clearly seen from the SEM image of the relevant sample, while the formation of clumping that would adversely affect the mobility was observed (Rezaul Karim et al., 2020). The major diffraction peaks for the AHB-NiFe2O4 sample were observed by (3 1 1), (2 2 2), (4 0 0) and (4 2 2) lattice planes corresponding to the 2θ diffraction angles of 31.77, 37.93, 45.37 and 56.79 degrees, respectively. It was concluded that the presence of NiO in the structure of the sample had an effect on the formation of crystal planes corresponding to the diffraction angles of 37.93 and 45.37 for the AHB-NiFe2O4. When the SEM image of the relevant sample was analyzed, the formation of NiFe2O4 nanoparticles was detected, but it was observed that there were serious cracks in the sample. It was thought that these cracks would adversely affect the conductivity of the AHB-NiFe2O4 sample, which was synthesized by acid modification (Naidu and Narayana, 2019). When the XRD patterns of samples AHB-CdFe2O4 and AHB-MnFe2O4 were examined together, it was determined that the crystal formation of these samples was different from the others. Although it is much more obvious in AHB-CdFe2O4 sample, the effect of cellulose polymer together with the synthesized nanoparticles was recorded on the diffraction patterns of these two samples. It was determined that (2 2 0) and (3 1 1) lattice planes of AHB-CdFe2O4, corresponding to the diffraction angle of 31.61 and 45.67, were more compatible with the treated CdFe2O4, respectively (Nayak, 2008). It was observed that similar XRD patterns were formed in the AHB-MnFe2O4 sample. It was determined that the intensity values of these two samples, which determine the XRD patterns, were lower than the other samples. Moreover, among these two samples, the XRD intensity of AHB-MnFe2O4 was determined to be lower and therefore it is expected to perform better than all of them in terms of conductivity. On the other hand, it was observed that the surface morphologies were very similar to each other (Desai et al., 2020). Finally, it was determined that the patterns of the AHB-MnFe2O4 sample were similar to the previous AHB-CuFe2O4 and AHB-NiFe2O4 samples, although they were compatible with the literature. Moreover, it was observed that both the structural and morphological properties of this sample were very similar to AHB-NiFe2O4. The characteristics diffraction peaks for the AHB-CoFe2O4 were recorded the lattice planes of (2 2 0), (3 1 1) and (4 0 0) corresponding to the diffraction angle with 31.87, 38.13 and 45.57 degrees, respectively (Bodaghi et al., 2020). The XRD patterns of metal ferrite-containing bio-nanocomposites compared with the SEM images and XRD patterns of AHB given in Fig. S2, Fig. S3 and Fig. S4 clearly indicate that AHB-MFe2O4 bio-nanocomposites were synthesized.
Figure 4 displays STEM, and mapping images of the bio-nanocomposites (AHB-MFe2O4) containing metal ferrite (MFe2O4) nanoparticles. The STEM images obviously demonstrate that MFe2O4 particles were agglomerated and they were still nano-sized in the bio-nanocomposites (AHB). In addition, the presence of M/Fe (M: Cu, Ni, Cd, Mn and Co) in the mapping images and EDX results (in Table 2) are clearly evidence of the preparation of metal ferrite-containing bio-nanocomposites.
Thermogravimetric analysis (TGA/DTA) of the bio-nanocomposite including MFe2O4 nanoparticles to determine the thermal stability of the HB, AHB and its nanocomposites including MFe2O4 nanoparticles were analyzed under nitrogen atmosphere at a heating rate of 10°C/min and the TGA/DTG thermograms were illustrated in Fig. S5 and Fig. 5
The thermograms showed in Fig. S5 demonstrate that water loss within the structure is the cause of a minor mass loss up to 150 oC observed in both HB and AHB. Additionally, it is evident from the same thermograms that HB's activation reduced its initial breakdown temperature of 250 oC to 150 oC. When the thermogram of AHB is investigated, degradation due to the separation of SO2 from the structure as a result of desulfurization in the range can be used to explain it (Akköz et al., 2019). Also, the findings show that HB decomposes in a single step between 200 and 400 oC, leaving 20% char at 800oC. The thermograms of bio nanocomposites containing metal ferrite nanoparticles are presented in Fig. 5. in comparison with the thermogram of AHB. When the thermograms of bio-nanocomposites were examined, it was observed that it exhibited a behavior similar to the thermal behavior of AHB, but decomposed by multiple degradation steps and left approximately 45% char. This high char ratio and multiple degradation steps are thought to be a result of the strong interaction between biomass and metal ferrite compounds (Karanfil et al., 2022).
UV–visible spectroscopy of the bio-nanocomposite including MFe2O4 nanoparticles
Figure <link rid="fig6">6</link>-a and 6-b shows the wavelength evolution of the UV spectra of the bio-nanocomposites, non-including and including metal ferrites nanoparticles, and their optical band gaps ((αhν)2 versus hν plots), respectively.
As seen from Fig. 6-a, the maximum absorbance of bio-nanocomposites including metal ferrites nanoparticles derived from the hemp biomass occurs at about 400 nm not observed in AHB. UV spectra of the other samples excluding AHB are seen similar to each other in the wavelength range of 190 nm–800 nm in appearance. However, it was clearly seen that the absorbance value of each sample is different, which can be attributed to the particle size and shape of the nanoparticles. The sharp drop of the bio-nanocomposites including metal ferrites nanoparticles around 400 nm has been remarkable. The highest absorbance value has been for AHB-CoFe2O4 bio-nanocomposite in the low wavelength region. It is seen that the sample with the highest absorbance value is the AHB-CoFe2O4 sample. This situation is attributed to homogeneous distribution of the CoFe2O4 in the bio-nanocomposites, and dielectric medium effects. Among the bio-nanocomposites, the AHB-CuFe2O4 has the lowest absorption. This is due to the fact that the dipolar effect on the optical spectra is less than the others. Moreover, the absorbance values of the nanoparticles decrease together with the reduction in particle size (see Table 3). Similar results have also been reported in the literature by Goh et al. (Goh et al., 2014).
The band gaps or optical band gaps of all bio-nanocomposites were calculated using the equation given below.
$$\alpha hv=B{(hv-{E}_{g})}^{n}$$
2
In this equation, α, h, ν, B, Eg and B symbolizes the absorption coefficient, Planck constant, frequency of the incident photon, constant value, forbidden energy band gap and index related to the nature of the transition. The forbidden energy band gap for each bio-nanocomposite is shown in Fig. 6-b. The energy differences are due to doping different metal ferrite and the size of particle (Bilal et al., 2022). The reason for these different energies has been attributed to the interactions between metal ferrite nanoparticles and AHB, also the difference in interaction strength (Yoon et al., 2022). These differences showed that the oscillation times, which determine the energy band gap, change. The decrease in the band gap also showed that the conductivity increased.
Table 3
Particle size and zeta potential values of the bio-nanocomposites including MFe2O4 nanoparticles.
Sample | Particle size (nm) | Zeta potential (mV) |
AHB-CuFe2O4 | 190 | -25.7 |
AHB-NiFe2O4 | 219 | -55.0 |
AHB-CdFe2O4 | 315 | -42.4 |
AHB-MnFe2O4 | 508 | -38.8 |
AHB-CoFe2O4 | 690 | -31.9 |
Magnetization analysis of the bio-nanocomposite including MFe2O4 nanoparticles
Magnetic hysteresis loops for the bio-nanocomposites including metal ferrites nanoparticles derived from hemp biomass in the range of range of -50000Oe–50000Oe, are shown in Fig. 7 at room temperature. As can be clearly seen from the figure, the saturation magnetization values of bio-nanocomposites containing metal ferrite are different from each other; this difference can be attributed to their composition, crystal sizes and metal distributions between octahedral and tetrahedral sites. It was observed that the sample that reached the saturation magnetization value the fastest was AHB-CuFe2O4 while the slowest was AHB-NiFe2O4. This property is attributed to the fact that nickel is ferromagnetic at room temperature (Nasr et al., 2022). Moreover, the higher saturation magnetization values of AHB-MnFe2O4 and AHB-CoFe2O4 than those of AHB-CuFe2O4 and AHB-CdFe2O4, it can be attributed to the high amount of Fe3+ in their composition. As reported in the literature, magnetic properties in spinel structure are known to be highly sensitive to compositions, crystallite size, and cation distributions between octahedral and tetrahedral sites (Tian et al., 2015). Furthermore, the important characteristic observed in the magnetic hysteresis loops for AHB-CuFe2O4 and AHB-CdFe2O4 sample is, in fact, the appearance of crossover for as indicated figure. It was attributed to the conclusion that this crossover property could possibly be due to the high magneto crystalline anisotropy property at a positive external magnetic field at room temperature. Since the nanoparticles will make an additional contribution to the magneto crystal anisotropy due to the dipolar interaction, such a feature seems highly probable. In addition to the spin-orbit interaction, when the anisotropy effect from dipolar interactions is effective enough, ions contribute to conductivity by moving relative (like fast moving electrons).
Electrolytic conductivity of the bio-nanocomposite including MFe2O4 nanoparticles
Figure 8 shows the ionic conductivity of bio-nano composites including metal ferrite and no including at different concentrations. As can be seen from the Fig. 8, the ionic conductivity of the bio-nanocomposites, containing metal ferrite nanoparticles, increases with increasing concentration but that of the AHB unaffected. In other words, the aqueous dispersions of AHB-MFe2O4's exhibit electrolyte behavior. When compared with the conductivity of the 0.1 M KCl aqueous solution (12.8 mS/cm), it could also be concluded that the aqueous dispersions of bio-nanocomposites are also quite good electrolytes. This can be attributed to the increasing degree of ionization of metal ferrite compounds with increasing concentration. Similarly, the ionic conductivity of the bio-nanocomposites containing metal ferrite nanoparticles also increases with increasing temperature. This increase, it could be due to increase in the number of ions and increase in the transport of the ions to the electrodes with increasing temperature (see Fig. 9) (Kadir et al., 2010; Miyamoto and Shibayama, 1973).
This temperature-dependent ionic conductivity for all the bio-nanocomposites containing metal ferrite nanoparticles indicates an Arrhenius behavior given in Eq. 3 (Ma et al., 2007) (Rajendran et al., 2004).
$$\sigma ={\sigma }_{o}\text{e}\text{x}\text{p}\left(\frac{-{E}_{a}}{kT}\right)$$
3
where σ0 is the pre-exponential factor, Ea and k are the activation energy and Boltzmann constant, respectively. Figure 10 was derived with using the data of Fig. 9 and from the Arrhenius plot of lnσ versus 1/T. From the slopes of Fig. 9, the activation energies for AHB-CuFe2O4, AHB-NiFe2O4, AHB-CdFe2O4, AHB-MnFe2O4 and AHB-Fe2O4 were calculated as 0.171, 0.171 and 0.171, 0.180 and 0.176 eV respectively. Calculated activation energy values for bio-nanocomposites containing metal ferrite range from 0.171 to 0.180 eV. Considering the necessity of biopolymer electrolytes with low activation energy values for practical applications (Samsudin et al., 2012; Samsudin et al., 2011), the developed bio-nanocomposites are suitable for this purpose.
Photocatalytic activity of the bio-nanocomposite
The prepared bio-nanocomposites containing metal ferrite were utilized as a catalyst for the degradation of organic pollutants. Particularly, the degradation of dyes such as MB, CrV and MGO, which cause pollution of the aquatic environment, using catalysts is an important method to remove the pollution of the aquatic environment. The characteristic absorption peaks at the maximum wavelengths of the dyes (665, 590 and 620 nm for MB, CrV and MGO, respectively) were utilized for monitoring the catalytic degradation process. UV-Vis spectra showing the degradation of MB, CrV and MGO dyes over time are presented with in Fig. 11, Fig. 12 and Fig. 13, respectively. It was observed that the bio-nanocomposites containing metal ferrite nanoparticles, AHB-MFe2O4, exhibits a very high degradation activity for organic dyes, MB, CrV and MGO, with sun light, as seen figures.
The degradation percentages of dyes by bio-nanocomposites are presented with in Table 4. Bio- nanocomposites degrade both CrV and MGO by over 90% except for MB.
Table 4
Photocatalytic effect of the bio-nanocomposites onto different dyes
| Degradation (%) | |
| | MB | CrV | MGO | |
Samples | 2h | 4h | 2h | 4h | 2h | 4h |
AHB-CuFe2O4 | 84.5 | 95.6 | 92.1 | 93.5 | 98.7 | 98.9 |
AHB-NiFe2O4 | 82.7 | 96.0 | 95.6 | 96.2 | 98.6 | 99.1 |
AHB-CdFe2O4 | 85.7 | 96.7 | 95.4 | 97.4 | 98.8 | 99.1 |
AHB-MnFe2O4 | 86.7 | 91.6 | 89.9 | 91.0 | 95.7 | 98.3 |
AHB-CoFe2O4 | 70.9 | 77.7 | 90.1 | 90.8 | 98.0 | 98.3 |
The superior catalytic activities of the bio-nanocomposites, AHB-MFe2O4, can be probably associated with the weaker M-O bonds in metal ferrites (Ortiz-Quiñonez et al., 2022). The M-O bonds at the surface of the ferrite can be broken by solvents under sunlight, and they can easily break down the dye molecules. High degradation in daylight makes the metal ferrite-containing bio-nanocomposites exceptionally advantageous against the catalysts developed in the literature for this purpose (Dhiman et al., 2016; Liang et al., 2018; Ortiz-Quiñonez et al., 2022).