2.1. Effect of Sulfidization on the Surface Properties of Smithsonite
To avoid the interference of Na2S, 5 × 10−4 mol/L Na2S was added and agitated for 5 min, after settling for 30 s; then, solid–liquid separation was used to obtain sulfidized smithsonite. The effect of sulfidization on the surface properties was characterized by SEM-EDS, FTIR, and XPS.
SEM-EDS was used to observe the surface morphology and elemental changes of smithsonite and sulfidized smithsonite, and the apparent morphology and photoelectron spectral distribution of bare smithsonite and sulfidized smithsonite are shown in
Figure 1a and
Figure 1b, respectively.
As shown in
Figure 1a, the surface of smithsonite is relatively rough with fracture zones. A large number of fine-grained smithsonite particles adhere to the mineral surface, which may be due to the low hardness of smithsonite itself, which can be easily crushed. The micro-fine-grained minerals have strong specific surface energy, which can be adsorbed on the surface of the coarse-grained smithsonite. The distribution of elements on the surface of smithsonite was further analyzed by EDS, and only the characteristic absorption peaks of Zn, C, and O appeared in the surface scanning spectra, and these three elements were uniformly distributed on the surface of smithsonite with the content of Zn, C, and O atoms of 19.2%, 28.3%, and 52.5%.
Figure 1b shows the SEM-EDS of the sulfidized smithsonite; the apparent morphology of smithsonite after sulfidization is relatively complete and has not changed significantly, indicating that the sulfidization treatment has not had a significant impact on the bulk structure of smithsonite. The surface of smithsonite after sulfidization is relatively neat, and the amounts of fine particles attached are significantly reduced, which may be related to the strong dispersing effect of sodium sulfide. The surface of smithsonite after sulfidization was further analyzed using the EDS energy spectrum, and it was found that the characteristic peak of the S element appeared in the photoelectron energy spectrum of smithsonite after sulfidization, indicating that sulfide was generated on the surface of smithsonite after sulfidization. The sulfur content of smithsonite at different sites after sulfidization is quite different. The fine particles on the surface of the sample have the largest sulfur content, and the atomic content of S reaches 2.6%; the atomic content of S at the edge of the crack is second, which is 1.4%; and the sulfur content at the smooth and dense area is the lowest, which is only 0.6%, indicating that the sulfidization products generated on the surface of smithsonite are unevenly distributed, and the fracture zone on the surface and the surface of fine particles may be more prone to sulfidization reaction.
Figure 2 shows the FTIR spectrum of smithsonite before and after sulfidization. The absorption peaks on the surface of smithsonite are mainly distributed at 2916.37 cm
−1, 2848.86 cm
−1, 2488.17 cm
−1, 1815.02 cm
−1, 1442.75 cm
−1, 1045.42 cm
−1, 869.9 cm
−1 and 742.59 cm
−1. According to relevant literature [
18,
19], the absorption peaks at 1442.75 cm
−1, 869.9 cm
−1 and 742.59 cm
−1 are the characteristic peaks of CO
32− ions in smithsonite, among which the absorption peak at 1442.75 cm
−1 is the asymmetric stretching vibration absorption peak of CO
32− ions, and the absorption peaks at 869.9 cm
−1 and 742.59 cm
−1 are the out-of-plane and in-plane bending vibration absorption peaks of CO
32− ions, respectively. The absorption peak at 2488.17 cm
−1 is the combined frequency peak of the CO
32− ions asymmetric stretching vibration absorption peak and the out-of-plane bending vibration absorption peak, while the absorption characteristic peaks at 2916.37 cm
−1, 2848.86 cm
−1, and 1815.02 cm
−1 are also considered to be harmonic peaks or combined frequency peaks. The absorption peak at 1045.42 cm
−1 can be considered to be the vibration absorption peak of the zinc metal hydroxyl compound (Zn-OH) on the surface of smithsonite.
No new characteristic absorption peaks appear in the FTIR of smithsonite after sulfidization treatment, which may be because the generated sulfidization product is similar to the infrared spectrum of sphalerite, and the characteristic absorption peak appears below 400 cm−1. After sulfidization, the asymmetric stretching vibration absorption peak of CO32− ions in smithsonite decreased from 1442.75 to 1431.18 cm−1, and the harmonic peak or combined frequency peak at 2916.37 cm−1 disappeared, indicating that the sulfidization treatment had a certain effect on the surface structure of smithsonite. Further, taking the characteristic absorption peaks at 2488.17 cm−1 and 1815.02 cm−1 as reference peaks, the infrared spectrum of smithsonite before and after sulfidization was processed by the peak difference. It can be seen that after sulfidization, the relative peak intensity of the characteristic absorption peaks of CO32− ions at 1442.75 cm−1, 869.9 cm−1, and 742.59 cm−1 increased, while the relative peak intensity of the harmonic peak or combined frequency peak on the surface of smithsonite decreased, indicating that the sulfidization treatment changed the chemical environment of the zinc metal particles on the surface of smithsonite.
The XPS spectrum of the smithsonite before and after sulfidization and the surface element atomic abundance and binding energy changes are shown in
Figure 3 and
Table 1, respectively. Combining the results in
Figure 3 and
Table 1, it can be seen that in the XPS spectrum of the surface of sulfidized smithsonite, a characteristic peak with a binding energy of 161.86 eV attributed to S2p appears, and the surface sulfur atom abundance reaches 14.29%. It shows that sulfide ions are adsorbed on the surface of smithsonite and form sulfide products.
Compared with bare smithsonite, the Zn atomic abundance on the surface of smithsonite increased significantly after sulfide treatment, from 20.96% to 29.89%, and the Zn2p binding energy decreased from 1022.04 to 1021.59 eV, a decrease of 0.63 eV, further indicating that after sulfidization treatment, the chemical environment of zinc sites on the surface of smithsonite has changed significantly. Compared with the changes in zinc atoms, sulfidization has less influence on the changes in C and O binding energies on the surface of smithsonite. Sulfidization has a greater impact on the relative abundance of atoms. The atomic abundances of C1s and O2s decreased by 5.17% and 18.05%, respectively. This may be related to the generation of sulfide products on the surface of smithsonite. The sulfide products cover the surface of smithsonite, and the relative abundance of oxygen atoms decreases.
In order to deeply analyze the properties of sulfide products and deeply study the impact of sulfide on the chemical state of elemental elements on the surface of smithsonite, high-resolution scans of Zn2p on the surface of smithsonite before and after sulfide and S2p after sulfide were carried out, and the fine spectra obtained were carried out. The test results after peak fitting processing are shown in
Figure 4a and
Figure 4b, respectively.
Figure 4a shows high-resolution spectra of Zn2p of smithsonite before and after sulfidization, from which it can be seen that the binding energies of the Zn2p
3/2 and Zn2p
1/2 peaks on the surface of smithsonite are located at 1022.04 eV and 1045.02 eV, respectively, which should be attributed to the characteristic peaks of ZnCO
3. The Zn2p binding energy on the surface of smithsonite changed significantly after sulfidization, and the split-peak fitting process revealed that in addition to the characteristic peaks of Zn2p
3/2 and Zn2p
1/2 located at 1022.00 eV and 1045.14 eV attributed to smithsonite, a pair of Zn2p
3/2 and Zn2p
1/2 characteristic peaks located at 1021.51 eV and 1044.35 eV were newly appeared on the surface of the samples. As shown in the relevant literature, the peaks should be attributed to ZnS, indicating that the sulfide products generated on the surface of zincite after sulfidization are ZnS substances. The zinc atoms on the surface of smithsonite after sulfidization mainly exist in the form of ZnS and ZnCO
3, and according to the calculation of the peak area of the two, the proportion of ZnS and ZnCO
3 on the surface after sulfidization is 68.31% and 31.69%, respectively, which indicates that the sulfidization treatment can generate a large number of ZnS substances on the surface of zincite.
Figure 4b is the high-resolution spectra of S2p of sulfidized smithsonite. The S2p spectrum on the surface of sulfidized smithsonite can be separated into a pair of sub-peaks. The binding energies of S2p
3/2 and S2p
1/2 sub-peaks are located at 161.71 eV and 162.90 eV, respectively. According to the relevant literature, this peak position belongs to the characteristic peak of ZnS. Therefore, it is further concluded that the sulfidization product on the surface of sulfided smithsonite is ZnS.
2.2. Effect of Sulfidization on the Flotation Behavior of Smithsonite
In order to investigate the effect of sulfidization on the floatability of smithsonite in the presence of an octadecyl amine (ODA) collector, the flotation recovery of bare smithsonite and sulfidized smithsonite as a function of ODA concentration at pH 9.5 was tested, and the results are shown in
Figure 5.
It could be seen from
Figure 5 that by raising the concentration of ODA from 0.5 × 10
−5 to 3.5 × 10
−5 mol/L, the flotation recovery of bare smithsonite slightly increased from 30% to 45% in the presence of ODA alone, while the flotation recovery of smithsonite was only 41.6% at the ODA concentration of 2 × 10
−5 mol/L, indicating that the flotation behavior of smithsonite using ODA as the collectors was poor. However, sulfidization has changed this situation, and the floatability of sulfidized smithsonite with its recovery from 38% to 82% was significantly improved after the pretreatment of sulfidization before ODA. The flotation recovery can be increased to 64.3% with pretreatment of sulfidization at the same ODA concentration of 2 × 10
−5 mol/L.
Subsequently, the effect of pH on the flotation recovery of bare smithsonite and sulfidized smithsonite in the presence of 2.0 × 10
−5 mol/L ODA was tested, and the results are displayed in
Figure 5b. In the range of pulp pH from 7 to 13, the flotation recovery of smithsonite with and without sulfidization increased with the increase of pulp pH, which might be related to the present form of ODA in the different pH values (shown in
Figure 6). Meanwhile, it can be seen that the flotation recovery of smithsonite was more greatly affected by the pulp pH than sulfidized smithsonite, which may be related to the fact that the surface of smithsonite is more prone to hydrolysis at lower pH and, in contrast, the generation of sulfide products slowing down the hydrolysis behavior of smithsonite surface. The above results suggested that sulfidization treatment could significantly promote the ability of ODA to collect smithsonite.
2.3. Effect of Sulfidization on the Adsorption Capacity of ODA
To reveal the mechanism of sulfidization on strengthening the flotation recovery of smithsonite using ODA as a collector, the zeta potentials and contact angles of smithsonite under different reagent schemes were measured, and the results are presented in
Figure 7 and
Figure 8, respectively.
Figure 7 shows the changes in the surface electrical properties of smithsonite and sulfidized smithsonite with the pH value before and after the treatment of ODA. ODA could hydrolyze a variety of positively charged ammonium ions in aqueous solution, such as RNH
2(aq), RNH
3+, RNH
2·RNH
3+(aq), and (RNH
3+)
22+, which will lead to an increase in the zeta potential of the mineral. It can be seen that within the measured pH range, the zeta potential of smithsonite and sulfidized smithsonite shifted positively under the action of ODA, further indicating that ODA can be adsorbed on the mineral surface before and after sulfidization. In addition, under the same pH conditions, the positive shift of the surface potential of the sulfidized smithsonite sample after the action of ODA is greater than that of smithsonite, indicating that the adsorption of ODA on the surface of sulfidized smithsonite is greater.
Figure 8 demonstrates the contact angle of smithsonite under different treatment conditions. It can be seen that the sulfidization treatment of the smithsonite surface can increase the contact angle from 29.13° to 46.05°, indicating that the generation of sulfide products on the surface of smithsonite can increase the hydrophobicity of the mineral surface to a certain extent. After the treatment of ODA, the contact angle of the smithsonite surface increased from 29.13° to 50.96°, and that of the sulfidized smithsonite surface increased from 46.05° to 93.15°, indicating that the action of ODA can improve the hydrophobicity of the mineral surface, and the sulfidization treatment is conducive to promoting the effect of ODA on the hydrophobicity of smithsonite, which was the direct reason for a preferable floatability of smithsonite.
The inference was well verified by the adsorption results that the amount of ODA shown in
Figure 9 adsorbed on sulfidized smithsonite was greater than that on bare smithsonite, and it also agreed well with those of flotation and zeta potentials.
Figure 9a shows the effect of ODA on the quality change in the bare and sulfidized smithsonite sample. It can be seen that the mass of bare smithsonite did not increase after the addition of ODA, and it even decreased after 300 s. This may be due to the strong solubility of smithsonite itself. At this time, even if ODA is adsorbed on the surface of smithsonite, it might be dissolved into the liquid phase along with surface dissolution. For sulfidized smithsonite, the sample mass increased significantly with time after the addition of ODA and reached the maximum value at 450 s, which might be related to the rapid adsorption of ODA on the surface of sulfidized smithsonite. Since ODA has strong adsorption capacity, the quality of the sulfidized smithsonite sample decreases after 450 s, which may be due to the attenuation of the sulfide layer.
Figure 9b shows the adsorption amount of ODA on the surface of bare and sulfidized smithsonite detected by TOC. The test results show that the adsorption of ODA on the surface of bare and sulfidized smithsonite increases with the addition of ODA. Moreover, the adsorption of ODA on the surface of sulfidized smithsonite is greater than that on the surface of smithsonite, which is basically consistent with the above QCM test results, further indicating that sulfidization treatment can increase the adsorption of ODA on the surface of smithsonite, which might be beneficial to the flotation recovery of smithsonite using ODA as collectors.
2.4. FTIR Analysis Results
To study the mechanism of sulfidization of Na2S on the adsorption of ODA on the surface of smithsonite, FTIR spectra of ODA and smithsonite with and without sulfidization before and after the treatment of ODA were detected.
The spectrum of ODA is displayed in
Figure 10. In the ODA spectrum, the asymmetric and symmetric stretching vibration and symmetric bending vibration absorption peaks of R-NH
2 appeared at 3369.64 cm
−1, 3296.35 cm
−1, and 1644.57 cm
−1, respectively [
20]. The asymmetric (-CH
3), asymmetric and symmetric (-CH
2-) stretching vibration absorption peaks of C-H separately occurred at 2951.09 cm
−1, 2918.44 cm
−1, and 2848.86 cm
−1. The peaks that emerged at 1517.98 cm
−1~1543.05 cm
−1 were assigned to the antisymmetric bending vibration absorption band of RNH
3+, whereas the peaks belonging to the asymmetric bending vibration and symmetric bending vibration of -CH
3 were recorded at 1466.47 cm
−1 and 1406.98 cm
−1. In addition, the peak at 1174.65 cm
−1 was attributed to the stretching vibration of C-N. The FTIR spectra of bare and sulfidized smithsonite before and after the treatment of ODA are shown in
Figure 6.
As illustrated in
Figure 11, after ODA treatment, a new absorption peak at 2956.87 cm
−1 was detected on the smithsonite surface; meanwhile, the intensity of the characteristic peaks located at 2916.37 cm
−1 and 2848.86 cm
−1 was significantly enhanced. The three characteristic peaks were attributed to C-H stretching vibration in ODA, and the corresponding bands of them were also no obvious shift, indicating that ODA could be adsorbed on the surface of smithsonite. In addition, using the characteristic absorption peaks at 2488.17 cm
−1 and 1815.02 cm
−1 in the spectrum of bare smithsonite as reference peaks, peak difference processing was performed on the FTIR of smithsonite before and after the interaction with ODA. It could be seen that a symmetrical bending vibration absorption peak on the differential spectrum appeared at 1643.35 cm
−1, which was not apparent compared to 1644.57 cm
−1 belonging to -NH
2 in ODA. In addition, the relative peak intensity of the characteristic absorption peaks attributed to CO
32− ions at 1415.75 cm
−1, 866.04 cm
−1, and 744.52 cm
−1 was enhanced [
19]. The above results indicated that ODA might be physically adsorbed on the smithsonite surface and thus result in more CO
32− ions exposed on its surface.
It could also be seen from
Figure 11 that for the sulfidized smithsonite treated with ODA, its FTIR spectrum was similar to that of sulfidized smithsonite, except for the three new adsorption peaks at 3305.99 cm
−1, 3278.99 cm
−1 (both attributed to -NH
2) and 1591.27 cm
−1, indicating that the interaction mechanism of ODA with sulfidized smithsonite was relatively complex. Further, the absorption peaks at 2488.17 cm
−1 and 1815.02 cm
−1 were used as reference peaks to perform peak difference processing on the FTIR spectra of sulfidized smithsonite before and after interacting with ODA. This indicated that the new adsorption peaks at 3315.63 cm
−1, 3278.99 cm
−1, 1643.35 cm
−1, 1598.99 cm
−1, 1541.12 cm
−1, and 1143.79 cm
−1 appeared on the differential spectrum, and those at 3315.63 cm
−1 and 3278.99 cm
−1 were shifted from the -NH
2 (3369.64 cm
−1 and 3296.35 cm
−1) peaks contained in ODA. The peaks at 1598.99 cm
−1 and 1541.12 cm
−1 showed negative–positive deformation peaks, which might be caused by the peak shift of RNH
3+ in ODA. Therefore, it could be inferred that the ODA was chemically adsorbed on sulfidized smithsonite by the action of R-NH
2 and RNH
3+.
The above FTIR results have shown that ODA adsorbed on the bare (physically) and sulfidized (chemically) smithsonite in different forms of action, which might have led to the large differences in the adsorption of ODA and flotation behavior between bare smithsonite and sulfidized smithsonite.
2.5. XPS Analysis Results
To further reveal the reaction mechanism between ODA and bare/sulfidized smithsonite, XPS experiments were performed to analyze the composition and valence change in elements on the bare/sulfidized smithsonite surface before and after ODA treatment. The XPS survey spectra and various surface elements binding energy values of smithsonite under different reagent schemes are demonstrated in
Figure 12.
It could be seen from
Figure 12 that compared to bare/sulfidized smithsonite, after the interaction of them with ODA, the new peak of N1s appeared in their XPS survey spectra, and the peak intensity of the C1s peak was significantly enhanced, indicating that ODA was adsorbed on both bare and sulfidized smithsonite. Furthermore, it was also found from
Figure 8 that the peak intensity of N1s on sulfidized smithsonite was much stronger than that on bare smithsonite, indicating that the amount of ODA adsorbed on the sulfidized smithsonite surface, which was consistent with the results of zeta potential and adsorption.
Figure 13 shows the narrow spectra of N1s and Zn2p on bare/sulfidized smithsonite before and after the reaction with ODA. As shown in
Figure 13a, it can be seen that with the treatment of ODA, a new peak attributed to the N1s of ODA with the binding energy of 399.95 eV appeared on the smithsonite surface, while the N1s peak on the sulfidized smithsonite surface could be well fitted into two peaks of 399.98 eV and 398.61 eV. The results indicated that the chemical environment of part N1s of ODA adsorbed on sulfidized smithsonite had changed obviously with the binding energy of N1s shifting from 399.98 to 398.61 eV by 1.37 eV. In addition,
Figure 13b also indicated that the peak of Zn2p for smithsonite with the treatment of ODA could be fitted into double peaks at 1022.07 eV and 1045.02 eV separately belonging to Zn2p
3/2 and Zn2p
1/2 of smithsonite, while for Zn2p of sulfidized smithsonite treated with ODA, its binding energy shifted to a certain extent. It was found that the peak of Zn2p could be fitted into three pairs of characteristic peaks, among which the peaks at 1022.11 eV and 1045.26 eV were assigned to ZnCO
3, 1021.44 eV and 1044.31 eV were attributed to ZnS, and new peaks at 1020.30 eV and 1043.31 eV appeared. Based on the aforementioned analysis, it is reasonable to infer that the pretreatment of sulfidization could transform the interaction mechanism of ODA on the smithsonite surface from physical to chemical by providing a beneficial environment for complexing N of ODA with Zn active sites of smithsonite [
21,
22].