3.1. Characterization of reactive dyes
The XPS spectra collected from Novacron Ruby S-3B reactive dye in the spectral range of C
1s, Cl
2p, N
1s, Na
1s and S
2p orbitals are shown in
Figure 1. The C
1s spectral region may be fitted using three major peaks: (i) one attributed to C atoms participating in the benzene/naphthalene rings (284.5 eV), (ii) a second peak attributed to the C-S bond (285.2 eV) and (iii) a third one associated with C atoms attached to the quaternary nitrogen atom, the O atom or/and the Cl
o atom (286.2 eV) [
36,
37,
38]. The N
1s spectral region can be fitted with two peaks of non-quaternized nitrogen atoms. The main peak is attributed to either C-N-C or/and C=N-C and is found at 400 eV, while the weaker one attributed to either NH
2 or N=N is observed at ~398.9 eV [
37,
38].
The sodium counterions are observed in the Na
1s spectral region (1071.9 eV), while in both Cl
2p and S
2p regions, doublets are recorded. The first doublet at ~199.0 eV is assigned to Cl
0 attached to the triazine ring, while in the sulfur 2p spectral region a twin doublet is assigned to -SO
2-/SO
3- contribution at 168 eV and to SO
4- at 169.2 eV [
14,
15]; the intensity ratio of the two peaks is ~4/1, in close agreement with the chemical structure of the dye,
Figure 1(f).
XPS spectra of Remazol Brilliant Blue R reactive dye of C
1s, S
2p, N
1s, Na
1s, and O
1s orbitals’ characteristic spectral regions are shown in
Figure 2. For this dye, as for the previous one, the stoichiometry derived from peak intensity ratios is close to the corresponding structure at molecular level. Notice that there is no signal in the Cl
2p spectral region and for the S
2p doublets the intensity ratio of the -SO
2-/SO
3- to -SO
4- species is ~2/1, in agreement with the structure given in
Figure 2(f).
The characteristic ATR-FTIR vibrational bands of both reactive dyes in the solid phase can be identified in
Figure 3. The spectral contribution of major structural groups, such as benzene/naphthalene/anthraquinone rings, chloro-triazine and sulfone/sulfonate/sulfate are found in the 950-1650 cm
-1 region; the most characteristic of them are listed in Table 2.
The bands at 1040 cm-1 and 1183 cm-1 (1038 cm-1 and 1194 cm-1 for Remazol Brilliant Blue R) can be assigned as symmetric and antisymmetric stretching vibration of the sulfonate (SO3-) group, respectively. In the same manner, the symmetric stretching vibration of O=S=O group, which can be found separated or/and in the sulfate SO4- group, is found at 1110 cm-1, while the antisymmetric one at 1210 cm-1 (1118 cm-1 and 1215 cm-1 for Remazol Brilliant Blue R).
Table 1.
This is a table. Tables should be placed in the main text near to the first time they are cited.
Table 1.
This is a table. Tables should be placed in the main text near to the first time they are cited.
Ruby |
Blue |
Assignment |
975m |
~1000m |
ring bending [42] |
1040s |
1038s |
sym vSO3+ vCC [47,48] |
1110m-sh |
1118m-sh |
sym SO2 str (of SO4 gr) [42] |
1133m-s |
1138m-s |
Sym SO2 str of C-SO2-C νCS + νCC + νsSO3 [47,48,49,50,51] |
1183s |
1194sh |
SO3 asym str [47,48,49,50,51] |
1210sh |
1215s |
Asym SO2 str (of SO4 gr) [42] |
1280sh-m |
1265sh |
C-N str [42] |
1414w |
- |
C=N triazine ring str [42] |
1615m |
1615m |
Ring str [42] |
3.2. Interaction between the cationic modifiers and the reactive dyes
3.2.1. Investigation of dye-polymer aqueous solutions through UV-Vis and fluorescence spectroscopy
Intermolecular interactions may affect the electronic properties of the molecular moieties with an apparent alteration of their optical absorption as well as fluorescence spectra. Both reactive dyes used in the current study contain anionic SO3- and SO4- groups, able to interact electrostatically with the cationic VBCTEAM units of the polymers. The dye with the most available interactive sites with the VBCTEAM units of the polymers is Novacron Ruby S-3B; 5 sites versus 2 for the case of Remazol Brilliant Blue R. However, for all dye-polymer combinations homogeneous solutions were obtained for sufficiently low D-/P+ charge ratios. Therefore, we have chosen a fixed charge ratio for all binary systems, D-/P+ = 1/5, (the nominal dye negatively charged sites equal 20% of the cationic polymer sites). The absorbance and fluorescence spectra were recorded from these solutions and compared with the respective spectra of the solutions of the individual constituents.
Figure 4a depicts the UV-Vis spectra of aqueous solutions of PVBCTEAM, Novacron Ruby S-3B dye and the respective binary system with D
-/P
+ = 1/5. The polymer absorption bands at 224 and 261 nm are only hardly resolved in the binary system spectra. Concerning the absorption bands of the dye, these are shifted to higher wavelengths in the binary system; depending on the transition, this red-shift varies (2-15 nm), having a greater value for the n-π* type of transition(s) observed at ~500-550 nm. Alterations in the relative intensity of the bands can be resolved; however, they are not significant. Respective spectra were acquired for all dye-polymer combinations. Similar trends were noticed in all cases.
In agreement with the absorption spectra, the fluorescence spectra (
Figure 4b) of the corresponding systems exhibit spectral shifts as well. In this case, however, blue-shifts are observed along with considerable intensity increase. Hence, shifts in the range of 35-90 nm are observed in the binary system of Novacron Ruby S-3B and PVBCTEAM along with an intensity increase of the fluorescent peaks by ~65%. Similar observations were noticed for all dye-polymer combinations.
3.2.2. Investigation of dye-polymer precipitates through ATR-FTIR spectroscopy
From the previous discussion, it is evident that the electronic properties of the binary mixture deviate from those of the dye itself, which in turn suggests that any relevant experimental technique will in principle indicate the existence of the interaction between the reactive dye and the cationic polymer. Alterations in the respective vibrational modes may exist as well. To perform vibrational studies, such as ATR-FTIR spectroscopy, solid samples were obtained through setting the mixing dye/polymer charge ratio, D-/P+, equal to unity. Under these conditions, as mentioned, a colored solid precipitate is formed, readily recovered through filtration.
Figure 5(a) shows the ATR-FTIR spectra of the Novacron Ruby S-3B reactive dye, the cationic polymer P(VBC-co-VBCTEAM53) and their binary system, all in the solid state. The spectra are rather complicated; however, the bands in the 1400-1500 cm
-1 spectral range, are attributed to benzene/naphthalene and triazine ring deformations. Since these modes are expected to be less affected by the intermolecular interactions with the cationic polymer (at least comparing to the vibrational modes attributed to the anionic sites of the reactive dyes), these bands were considered as reference bands. After the normalization of the spectra, the most interesting changes are the relative intensity of the symmetric stretching vibrations of SO
3- (1040 cm
-1) and SO
4- (1110 cm
-1) with respect to the asymmetric ones (1183cm
-1 and 1205 cm
-1) observed in detail in
Figure 6(a). Similar results were obtained for the binary system of NR-homo,
Figure 5(b) and
Figure 6(b).
Identical spectral behavior can be observed referring to the P(VBC-co-VBCTEAM53) or PVBCTEAM and Remazol Brilliant Blue R precipitate (
Figure 7). Both intensities of the symmetric stretching vibrations of SO
3- and SO
4- groups have decreased (1038 cm
-1 and 1120 cm
-1, respectively), with respect to the intensity of the asymmetric vibrations at 1194 cm
-1 and 1215 cm
-1.
All these spectral differentiations may lead to the early conclusion that changes happen in the counterion of the sulfate/sulfonate anionic groups of the dye molecules. The Na+ counterions of the dyes probably have been replaced by the quaternary N+ groups of VBCTEAM units of the polymers; the latter induces changes in symmetry of these sulfate/sulfonate species affecting their vibrational behavior.
The work of Shishlov and Khursan [
52] focuses on the comparison between experimental and calculated vibrational spectra of benzenesulfonate salts, which are molecular units similar to some of the most characteristic ones of the reactive dyes in the current work; therefore, their findings may be applied on the study of pristine dyes and their binary system with cationic polymers. The authors stated that bidentate species introduce splitting of the asymmetric SO
3- vibrational band with the two generated modes well separated by >150 cm
-1. On the contrary, in more symmetric species, such as tridentate or dimers, the corresponding splitting is not so profound. The authors also described that for the organic sulfonic species, the coordination of sulfate/sulfonate ions with cationic counterparts is complex and depends on the environment. Considering the complexity of the dye molecules and their FTIR spectra it is ambiguous to explain the spectral alterations; Nevertheless, it is evident that the interaction of the reactive dyes with the cationic polymers involves exchange of the cationic counterpart Na
+ with the quaternary N
+ groups of VBCTEAM units, which in turn critically affects the symmetry of the sulfate/sulfonate species.
3.2.3. Investigation of dye-polymer precipitates through XPS spectroscopy
The estimation of the ratio between the species of dyes and the VBCTEAM units in the solid precipitates is of importance since it evaluates the number of dye molecules that each polymeric chain can uptake. This factor is not straightforward, and it is critical in terms of both scientific knowledge and applications since each dye possesses different active sites and may pose specific steric hindrances when interacting with the polymer chains.
The solid precipitates obtained at a mixing dye/polymer charge ratio fixed at D
-/P
+=1 were investigated through XPS spectroscopy.
Figure 8 depicts the N
1s spectral region of the XPS spectrum of the NR-copo precipitate. The accumulated spectrum consists of bands assigned to both quaternary and non-quaternary nitrogen atoms. The non-quaternary nitrogen contribution at 399.5 eV is attributed to the dye Novacron Ruby S-3B, a band that is well separated from the respective one of the quaternized nitrogen of VBCTEAM units located at a binding energy of 402 eV. This separation can be useful not only for qualitative but also for quantitative analysis in case of binary system study or/and the study of dyed cotton (see section 3.3). Regarding this particular binary system, an almost equal amount of nitrogen contribution can be detected (N
+/N~1.2/1). Considering that this dye contains 7 nitrogen atoms, whereas VBCTEAM unit contains only 1 nitrogen atom, this result indicates a ratio of 1 Novacron Ruby S-3B dye molecule for every ~5.8 VBCTEAM units, namely close to stoichiometric charge ratio, since the dye contains 5 negatively charged units. The same ratio value was estimated for the binary system of the same dye with PVBCTEAM (NR-homo) after calculation of the corresponding intensity ratio in the spectrum shown in
Figure 2S.
Sulfonates (SO
3-) and sulfate (SO
4-) of the Novacron Ruby S-3B molecule in
Figure 9(a) have some noticeable differences when compared to the corresponding spectrum of Remazol Brilliant Blue R binary system. These slight changes are attributed to the differentiation of the chemical environment of the anionic groups, after the electrostatic interaction. In this direction, 0.2-0.3eV increase at FWHM of the overall sulfur peak can be justified, while the peak position remains constant. These changes are mainly found in the Novacron Ruby S-3B system that contains four sulfonate groups, in which some of them may not interact due to steric hindrance.
The sodium 1s orbital peak at 1072 eV, in
Figure 9(b), is particularly strong in the Novacron Ruby S-3B spectrum indicating the counterions of the existing five anionic sites, while it is very weak in the case of the binary system.
In the chlorine 2p orbital peak at
Figure 10, there is a multiple contribution of chlorines Cl
0 of both the Novacron Ruby S-3B dye (199 eV) and VBC units for the case of the cationic copolymer (200 eV), while the chlorine counterions Cl
- of VBCTEAM units are observed at 197 eV. In the case of the binary system the Cl
- contribution is severely depressed.
This disappearance of both sodium (dye) and chlorine (polymer) counterions, indicate the strong tendency for the cationic polymer to interact with the reactive dye through electrostatic interactions. The replacement of Na+ ions with the cationic units of the polymer in the binary system is in agreement with the ATR-FTIR spectroscopic results that indicate alterations in the local environment of the sulfonate/sulfate groups.
The same arguments hold for all the different binary systems studied. It is interesting to note that for the case of Remazol Brilliant Blue R, from the respective spectra of
Figure 2S it is calculated that the ratio of VBCTEAM units per dye molecule is ~3.5 when binding with PVBCTEAM, and ~2 when binding with P(VBC-co-TEAM53). The lower ratio values for Remazol Brilliant Blue R, compared to the respective values for Novacron Ruby S-3B, can be explained by the different number of anions in their structure (2 for Remazol Brilliant Blue R and 5 for Novacron Ruby S-3B) as well as by the difference in size of the dye molecules.
3.3. Role of the cationic modifier in the dyeing process of cotton
The general reaction mechanism of reactive dyes with unmodified cellulose surface consists of two major steps. First, the physical contact of the molecules through the sorption of dyes from the dye bath on the cotton fiber and second, the chemical reaction with the cellulose. The reaction proceeds only in the presence of an alkaline bath which is used to activate the cellulose reactive site (fixation phase) [
33,
34]. Vinyl sulfone is the reactive group of both dyes used in the present study. In fact, during the dyeing process, the masking sulfate group is removed by a 1,2-trans elimination reaction, to form the free vinyl sulfone group, able to react with fiber nucleophiles by the Michael addition reaction [
33]. Vinyl sulfone dyes are applicable at the range of 40-60
oC [
35]. Novacron Ruby NRS-3B is bifunctional, since it contains also a chloro-triazine reactive site, able to react with cellulose through the classical SN
2 bimolecular substitution from nucleophilic attack of the electron-rich oxygen in the cellulosate anion on electron deficient carbon atoms in the triazine heterocycle (chlorine leaving group). The most important disadvantage of this dye category is the increased requirement of alkaline concentration (sodium carbonate) and temperature (80
oC) in the dye bath [
33,
34,
35].
When investigating the role of cationic modification of cotton, it is necessary to understand the effect on increasing the retention of dye. To demonstrate the capabilities of cotton modification with the present cationic modifiers, we applied the same dyeing protocols on modified and unmodified fabrics. The protocol involved high and low temperatures with and without salt (Section S2). Cationization resulted in fibers characterized by a thin modified layer. The thickness of the modified layer is so small that spectroscopic techniques such as FTIR and Raman scattering with a penetration depth of very few microns offer marginal information and extremely sensitive surface techniques, such as XPS, could identify and provide insight of the physical chemistry associated with the modification process. This argument is also supported by Scanning Electron Microscopy images (Image S1), where the morphology of untreated, dyed untreated and dyed treated fibers remains similar in the scale of hundred nm. This observation indicates that both modifier and dye are covering just a few nm of the fibers’ surface, which is similar to the order of XPS penetration depth.
The quantity of dye retained on the cellulose fibers’ surface can be qualitatively extracted by XPS and more clearly in the carbon 1s spectral region. XPS spectra obtained from the samples after the dyeing process (using Novacron Ruby S-3B) in this particular spectral region can be seen in
Figure 11. The most characteristic peak of cotton is the one at 286.6 eV; we use this peak as an internal standard in order to semi-quantify the degree of modification as well as of dyeing, taking into account that both modifier and dyes exhibit a characteristic band at ~285 eV. We thus observe a small intensity increase of the latter band after dyeing unmodified cotton at ambient temperatures. This small intensity increase agrees well with the macroscopic poor fabric color intensity (Image 1), while similar color intensity is observed in the modified fabrics with the copolymer. Modified fabrics exhibit strong contribution in the ~285 eV band indicating grafting of the cationic polymer to the cellulose fibers, while subsequent dyeing of the modified fabric resulted in further increase of the same band intensity. The ability of the XPS to semi-quantify the quantity of dye on fabrics may be furthermore demonstrated in the inset of
Figure 10 where small differentiation of the 285 eV intensity is resolved for fabrics dyed with and without salt at ambient temperatures, the first of which were characterized by slightly better retention of dye.
The ability of this surface technique further demonstrates the potential of the cationic modification process to retain large quantities of dye (more than an order of magnitude compared to the unmodified cotton) even at low temperatures. The higher degree of dyeability caused by the presence of the cationic modifier on the cotton surface is clearly resolved in Image 1
. Unmodified fabrics dyed using the typical procedure with and without salt exhibit low dyeability at low temperatures; the presence of salt results in a slightly higher dyeability. In comparison, modified fabrics exhibit high dyeability at low temperatures even without the presence of salt. Apart from being more vivid, the color on these fabrics is also particularly uniform. Extensive colorimetric studies performed on dyed fabrics modified by a series of cationic modifiers similar to the ones used in the current study can be found in [
53]. In the next paragraphs, the XPS study of the pair of dyed fabrics depicted in Image 1 will be given as a case study. The results of all other possibilities are comparable and lead to the same conclusions.
Image 1.
Dyed cotton fabric at low temperatures with: a) Novacron Ruby S-3B and b) Remazol Brilliant Blue R. Comparison of the color intensity for samples with and without modification is unambiguous. For the modified fabrics the dyeing protocol without salt (S2.1) was followed.
Image 1.
Dyed cotton fabric at low temperatures with: a) Novacron Ruby S-3B and b) Remazol Brilliant Blue R. Comparison of the color intensity for samples with and without modification is unambiguous. For the modified fabrics the dyeing protocol without salt (S2.1) was followed.
The N1s spectral region in the XPS spectra can be used to verify the coexistence of the components (quaternary VBCTEAM units and non-quaternary species of dyes), while the Cl2p one to reveal the interactions involved between cellulose, cationic polymer and dye.
The nitrogen existing in the dyed fabric is a combination of cotton residues and dye, as indicated by the peak at ~400 eV in the N
1s spectral region of the XPS spectra (
Figure 12a); the cotton residues contribution is considered much less than that of the dye. For the case of modified dyed fabrics two peaks are resolved, at ~400 eV assigned mainly to the dye and the ~402 eV assigned to the VBCTEAM units. From the signal to noise ratio, it is clear that the dye retention is significantly increased after treatment, in agreement with the respective findings from the carbon 1s spectral region.
The Cl
2p spectral region,
Figure 12(b), is indicative of the chloro-triazine sites when dyeing with the Novacron Ruby S-3B dye (at ~199 eV). This chemical unit is one of the two sites of potential direct interaction of this particular dye molecule with cotton. In the same spectral region, the Cl atoms of the polymers containing VBC units also contribute (~200 eV). However, as already shown [
32], their contribution in the modified fabrics cannot be observed in the XPS spectra; the latter was explained as an indication of polymer grafting on cellulose through this reactive site. Finally, the Cl
2p spectral region is characteristic of Cl
- at ~198 eV.
Our results reveal that no Cl2p bands are observed in the fabric, nor in the unmodified dyed fabric. The latter may be explained either by the low quantities of dye molecules retained at low temperature processes and/or by the direct grafting of the dye to cellulose. The weak band of chlorine ions observed (at ~197 eV) in the spectra of unmodified fabric are possibly attributed to small salt residues after the dyeing process performed in alkaline 1M NaCl solutions. The clearly resolved neutral chlorine band observed in the spectra of modified-dyed fabrics suggests a considerable fraction of unreacted dye sites. In the same spectra, the Cl- ion contribution is minimal and may explained either to salt residues or as a small number of counterions to the cationic VBCTEAM units that did not interact with dye molecules.
The question of whether the typical reactive dye process of grafting on cellulose i.e. through vinyl sulfone and chlorine sites is participating in the dyeing process of modified fabrics is difficult to be answered. As explained above, for Novacron Ruby S-3B dye it appears that its reaction with cellulose is not fully performed (Cl band intensity in
Figure 11b). As far as the masking sulfate groups are concerned, the XPS sulfur spectral region, which in principle offers the ability to extract the information, requires fitting of the respective band with two bands (namely SO
3- and SO
4- groups), a difficult task, especially for spectra of low signal to noise ratio. Observation of the width of the band for the untreated dyed fabric (
Figure 13) indicates that there exists a narrowing of the band-width (FWHM=2.3) if compared to the pristine dye band (FWHM=2.7). The XPS spectrum of pristine Novacron Ruby S-3B dye can be fitted with two doublets in the S
2p spectral region as shown in
Figure 1e. For the unmodified dyed cotton, a fitting is satisfactory by incorporating only the SO
3- pair of peaks (main peak at 168 eV) indicating a consumption of the SO
4- species during the dyeing process of cotton. The spectra of pristine Novacron Ruby S-2Band the modified-dyed cotton are compared in the Inset of
Figure 12. The similarity in the peak profiles and peak widths suggests that the SO
4- site are still present, suggesting that the dye has not been bonded to cellulose through the vinyl sulfone mechanism.