3.1. Confinement of naphthol green B in Zn-Al nanolayerd structures
Plate-like structure is the conventional structure for the synthetic LDHs and the natural materials of LDHs (pyroaurite) exhibiting plates with dimensions in the range of millimeters [
32]. In addition, hexagonal platy morphology was observed for the hydrotalcite crystals [
33]. The morphology of the sample ZA-1 agrees with the conventional structure of the synthetic and natural LDHs as shown in SEM and TEM images in
Figure 1.
Figure 1a revealed SEM image for ZA-1 indicating rounded plates. However, hexagonal nano-plates with few hundred nanometers in width were observed in the TEM image of ZA-1 as shown in
Figure 1b corresponding with the hydrotalcites structures because TEM images show the individual plates of LDHs and SEM images focus on aggregations or groups of plates.
These SEM and TEM images concluded that the sample ZA-1 is belonged to the LDH group. By intercalating different percentages of green dyes, strong aggregation of plates was observed as shown in
Figure 2. SEM image of NH-1 nanohybrid showed large cycles as seen in
Figure 2a. These cycles consist of large number of nanoplatelets that aggregated through self assembly behavior. This behavior was originated by generating hydrophobic character for the nanoplatelets of Zn-Al LDH. The hydrophobic character was produced by bonding the aromatic molecules of the green dyes (two benzene rings) with the nanoplatelets of Zn-Al LDHs through host-guest interaction. By increasing the percentage of green dyes,
Figure 2c indicated that the hydrophobic character enhanced as seen in SEM image of NH-3. The self assembly behavior of Zn-Al-dyes was clearly observed through magnifying the SEM image of NH-5 in
Figure 2b.
By thermal treatment of NH-5 at 450 °C, the green powder of the nanohybrid which based on the naphthol green B converted to yellow powder because of partial decomposition of the green dyes.
Figure 3 showed SEM images of the new nanohybrid NH-5-450.
SEM images indicated that the nanohybrid NH-5-450 has individual nanoplates as seen in
Figure 3a. It means that the yellow nanohyrid has lost part of the hydrophobic character. Also,
Figure 3b showed that the size of plate is 111 nm. By using X-ray diffraction, nanolayered structure of ZA-1 was observed as shown in
Figure 4a. The values of the basal peaks of planes hkl [003], [006] and [009] of ZA-1 showed an order arrangement of the packed stacks of brucite-like layers ordered along axis c; i.e., 0.76 nm = 2×0.38 nm = 3×0.26 nm.
According to the c dimension of the natural and synthetic hydrotalcite, which is assessed as three times the spacing for planes (003) and equals 2.31 nm [
31], it nearly agrees with the calculated value for the prepared material ZA-1, i.e., 2.28 nm. Depending on the spacing for plane (110), the average distance between Zn-cation and Al-cation within the brucite-like layer, which is related to the lattice parameter ‘a’ of the prepared material and can be determined as two times of d(110), could be calculated to be 2×0.153 nm = 0.306 nm agreeing with the reported data of LDHs [
31]. These parameters confirmed that the sample ZA-1 has LDH structure.
The main peak of ZA-1 which observed at 0.76 nm indicates the size and the orientation of the interlayered anions inside the layered structure of LDH. By comparing with the layered structure of the synthetic Zn–Al LDH (JCPDS file No. 48-1022) and the natural hydrotalcite (JCPDS file No. 37-629), the main interlayerd anions of the prepared material is carbonate anions as shown in
Figure 4a.
The XRD pattern of the ZA-1 after intercalation with 3% of green dyes exhibited new weak reflections at lower 2Ѳ in addition to the original basal spacing of LDH suggesting formation of two phases; LDH and nanohybrid material as shown in
Figure 4b.
The interlayer spacing of the LDH after intercalation reaction with green dyes increased to be 1.5 nm. In addition, there are two other weak peaks at 0.7 nm and 0.46 nm. The successive reflections by basal planes, i.e., 1.5 nm ≈ 2 × 0.7 nm ≈ 3 × 0.45 nm, indicated layered structure for the prepared nanohybrid. The reflection of (110) became unclear. In addition, the intercalation of organic species decreased the order arrangement of the layered structure. By increasing the percentage of green dyes through intercalation reactions, the layered structure of LDHs disappeared as shown in
Figure 4c-f. It means that the presence of aromatic molecules among the layers of nanohybrid led to distortion of the nanolayers because of the steric hindrance and repulsion of the benzene rings inside the interlayered space. It means that the absence of reflections corresponding to the nanolayered structure of LDH after organic modification is due to disappearance of coherent conditions in different directions (lack of repeated units).
The presence of organic molecules inside LDH structures and the formation of organic-inorganic nanohybrids were confirmed by the data of thermal analyses (TG and DTG). Thermal characteristics of the sample ZA-1 were measured by the diagrams of both TG and DTG as shown in
Figure 5a. The weight of ZA-1 was mainly lost through two stages. In the first stage, 9 wt.% was lost at 192 °C corresponding to the desorption of surface and intercalated water. The second stage was achieved at 323 °C to lose 18 wt.% agreeing with the removal of hydroxyl groups of LDHs and decomposition of anions. In the DTG diagram, three peaks were observed at 172 °C, 212 °C and 285 °C as shown in
Figure 5a. At first peak, removal of both surface and interlayered water happened at 172 °C agreeing with TG data. The other two peaks belonging to the removal of hydroxyl groups of LDHs and decomposition of anions occurred at 212 °C and 285 °C matching with the second stage of TG diagram.
Thermal characteristics of Zn–Al-dyes nanohybrids were observed in Figs.5b-f indicating three stages for weight losses. The first and second weight losses in all samples are due to the removal of water molecules and decomposition of carbonate anions; respectively. The third weight loss confirms the intercalation of aromatic rings of the green dyes inside LDH structures.
In case of the sample NH-1, the DTG diagram showed new peak at 517 °C agreeing with the third weight loss in the TG diagram as seen in
Figure 5b. By increasing the percentage of green dyes during the intercalation reactions of the samples from NH-1 to NH-5 , the third weight loss in TG curves increased from 5% to 13% ; respectively. In addition, the DTG diagrams showed that the intensity of the peak at 519 °C increased arriving to maximum at sample NH-5 as shown in Figs.5.
By comparing with the parent LDH (ZA-1), the content of the interlayered water of the nanohybrids decreased from 9% to 6%. Also, new peaks were observed in the TG diagram at the temperature range 262-266 °C and 517-557 °C for the prepared nanohybrids NH3-NH5 confirming the intercalation of organic species instead of carbonate anions.
3.2. Colored polymeric nanocomposites
According to the above results, the sample NH-5 considers the most suitable nanohybrid to be used a filler for building colored polymeric nanocomposites because it has organic–inorganic nanostructures and contains 13 wt% of green dyes.
Therefore, this nanohybrid has used as a filler for poly vinyl alcohol through two different ways. The first way depends on intercalation of the nanohybrid before calcination. In the other way, the nanohybrid has been used after calcination at 450 °C.
By using the first way, three polymeric nanocomposites were produced using different percentages of the nanohybrid. NCP-1, NCP-2 and NCP-3 were prepared by intercalating 2 wt.%, 10 wt.% and 20 wt.% of the nanohybrid inside PVA. The XRD pattern of the pure PVA was observed in
Figure 6a revealing a weak peak at 2θ = 19° (d-spacing = 0.45 nm) indicating the characteristic peak of the plane [101] of PVA. Also, This peak indicates the intermolecular hydrogen bonds that connect between the chains of PVA through hydroxyl groups [34, 35].Also,
Figure 6c-e showed the XRD patterns of the nanocomposites NCP-1, NCP-2 and NCP-3. For the nanocomposite NCP-1,
Figure 6c showed amorphous structure indicating that the low percentage of the nanohybrid (2 wt.%) is homogeneously dispersed inside the matrix of PVA. The disappearance of the diffraction maximum of the nanohybrids may be the result of the subsequent increase in interlayer periodicity and the shift of the maximum to the low-angle region beyond the range of the diffractometer used.
In case of the high percentages of the nanohybrid, new nanolayered structures were observed for the polymeric nanocomposite NCP-2 and NCP-3 as shown in
Figure 6d, e. X-ray diffraction patterns of NCP-2 and NCP-3 showed weak peak at 2.1 nm and clear peak at 0.75 nm in addition to the peak of PVA. It means that the polymer chains of PVA have intercalated among the nanolayers of the nanohybrids and expanded the inlayered spacing of the nanocomposites to become 2.1 nm. Comparing with the X-ray patterns of the nanohybrid and the parent PVA, the intercalation process increased the crystalline structure of PVA creating new phase of polymeric nanocomposite Zn-Al- dyes-PVA
In case of using the second way of intercalation process, another three samples of polymeric nanocomposites NCP-4, NCP-5 and NCP-6 were prepared through inserting 2 wt.%, 10 wt.% and 20 wt.% of the calcined nanohybrid inside PVA. The X-ray diffraction of the calcined nanohybrid showed that it has zinc oxide structure agreeing with
wurtzite crystals (JCPDS 36-1451) as shown in
Figure 7b.
It means that the calcined nanohybrid
has zinc oxide structure doping with aluminum and the products that produced from the decomposition of green dyes. By intercalating the low percentage of the calcined nanohybrid, the peaks of zinc oxide disappeared as shown in Figure 7c. X-ray diffraction pattern of NCP-4 showed only weak peak at 0.45 nm indicating that the nanohybrid layers are completely and uniformly dispersed in
the structure of PVA. By increasing the percentage of the calcined nanohybrid, new weak peaks were observed in the XRD patterns of both NCP-5 and NCP-6 as seen in Figs.7d, e. Figure 7d showed two peaks at low two theta with d-spacing at 2.0 nm and 1.1 nm. It means that the nanolayers of the nanohybrid were re-arranged to build the nanolayered structure again in presence of polymer chains depending on the phenomenon of memory effect of LDH structure. This phenomenon is familiar in the LDH structure. After heating the LDH at temperature 450 °C for a few hours, the nanolayered structures of LDHs are converted into mixed oxides, but still have memory for their own structure [36, 37]. These mixed oxides, after dispersion in an aqueous solution containing preferable anionic moieties followed by some degree of aging, revert to the original layered structures of LDHs.
3.3. Thermal Stability
The measurements of TGA and DTG have been used for studying the effect of green and yellow nanohybrids on the thermal stability of PVA through building nanocomposites as shown in
Figure 8,
Figure 9,
Figure 10 and
Figure 11.
Figure 8 indicates the different stages of thermal decay of pure PVA and the nanocomposite NCP-3.
Figure 8a showed that the main weight of the pure PVA (80%) lost at 372 °C through two stages. In case of the nanocomposite NCP-3, the TG curve showed that it has four stages for losing 80% of NCP-3 at 820 °C.
With noting that the temperature corresponding to the first loss 5% (T0.05) of the pure PVA is at 105 °C. This temperature was shifted to higher value at 175 °C for the nanocomposite NCP-3. The final residue of NCP-3 which obtained at 1000 °C was 2.6% while, there is no residue for the pure PVA. These data confirmed the positive effect of nanohybrids on the thermal stability of the PVA.
Similar results were observed for the nanocomposites NCP-1 and NCP-2.
Figure 9 showed that the temperature of the initial 5% weight loss of both NCP-1 and NCP-2 occurred at 250 °C and 210 °C. In the same trend, the nanocomposites NCP-1 and NCP-2 have lost 80% of its weight at higher temperature (457 °C and above 800 °C) comparing with the pure PVA.
In case of the second series of the nanocomposites NCP-6, NCP-5 and NCP-4, the thermal stability became higher than the pure PVA agreeing with the first series of the nanocomposites.
Figure 10 showed that 50% of the nanocomposite NCP-6 was lost at 414 °C while for the pure PVA was observed at 322 °C. For the weight loss 70%, figure 10 showed similar behavior because it achieved at 796 °C for NCP-6 while it was observed at lower degree for the pure PVA at 338 °C.
Figure 11 indicated that the nanocomposites NCP-4 and NCP-5 have higher thermal stability than the pure PVA.
The decomposition of the chains of polymer starts at their ends or the weak bonds through formation of free radicals. After that the degradation process continues by transferring to the adjacent chains via inter-chain reactions. In the prepared nanocomposites, the presence of the inorganic nanolayers slowed down the mobility of the chains of the polymer because of the hydrogen bonds which generated between the PVA chains and nanohybrid materials to improve the thermal stability of polymer [
38].
3.4. Optical Properties
It is known that poly (vinyl alcohol) has no clear optical behavior. In order to improve its optical properties, six samples of its nanocomposites were prepared and studied by the important details about their absorbance and band gaps that determined through the UV-Vis absorption spectra.
Figure 12 showed the UV-Vis absorbance and band gap of the pure PVA. Two weak absorption peaks are recorded at 200 nm and 300 nm indicating that it has wide band gap as shown in
Figure 12.
By plotting the incident photon energy (E) and the absorbance coefficient of the materials (Abs), the energy band gap (E
g) was assessed through the following procedure [
39]:
Where E = hc/λ; the values (h and c) are the Planck’s constant and speed of light. The value (Abs) means the absorption coefficient.
In order to determine the band gap energy, both (Abs.E)
2 and (E) were plotted. When the value (Abs.E)
2 equals zero, the energy matches with the optical band gap. It is achieved through extending the straight line to the (E) axis, as shown in
Figure 12.
Figure 12 indicated that the pure PVA has band gap energy at 5.5 eV.
In case of the nanocomposite NCP-1,
Figure 12b(inset) revealed that the optical properties of PVA improved through shifting the absorption edge of PVA to 800 nm. Also, the absorbance range become broader in the UV region to cover the range between 500 nm to 200 nm as shown in
Figure 12b(inset). It means that the low content of nanohybrid created new optical sites inside the PVA matrix to become active in the visible and UV regions after building the nanocomposite. These results were confirmed by calculating the band gap energy.
Figure 12b showed that the nanocomposite NCP-1 has band gap energy at 4.3 eV.
By increasing the content of the nanohybrid inside PVA, more improvement happened for the polymer as shown in the spectra of both NCP-2 and NCP-3.
Figure 13(inset) showed the absorption spectra and band gaps of both NCP-2 and NCP-3. Clear absorption was observed in the UV region in the range of 450 nm to 200 nm. Also, in the visible region, strong absorption was observed in the range of 600-800 nm. In addition, the band gap decreased to be 2.2 eV for both NCP-2 and NCP-3 as seen in
Figure 13.
In the second series of the nanocomposites, another trend for improving the optical behavior of PVA was observed for the samples NCP-4, NCP-5 and NCP-6. In the sample NCP-4, the absorption edge of PVA shifted to higher wavelength 400 nm as shown in
Figure 14a(inset). It means that the PVA became active in the UV region.
Figure 14a showed that the band gap of NCP-4 was observed at 3 eV. In the same trend, the sample NCP-5 showed more shifting for UV absorption to arrive at 500 nm indicating that it has band gap at 3 eV as seen in
Figure 14.
By increasing the content of the nanohybrid in the second series,
Figure 15 showed continuous shifting for the absorption edge of NCP-6 to be at 700 nm in the visible region. It means that NCP-6 became active in the visible region because its band gap decreased to become 2.5 eV.
This lowering of the band gap of PVA can be explained through formation of new optical sites inside the polymer structure because of the presence of the optical active dyes combined with optical inorganic nanolayers. The band gap energy of the pure PVA (5.5 eV) is very wide because the large gap between the HOMO and LUMO bands of PVA. For the prepared nanocomposites, the presence of the nanolayers of the Al-ZnO, which coated with dyes molecules, created trap levels between the HOMO and LUMO bands of PVA producing dangling orbitals. In the same time, it increased the band tails in the polymeric nanocomposites. Therefore, the band gap strongly decreased to become 2.5 eV. This explanation agrees with many previous studies [
40,
41,
42,
43,
44,
45].