3.1. FTIR Analysis Before and After Immersion
Fig. (2) Illustrates the FTIR spectral curves of the undoped glass together with that for Mo2O3 – doped glass samples in the mid IR range of 400-1800 cm-1. Whereas the Infrared spectroscopy (IR) is used to attribute the observed absorption peaks to the suitable vibration of the atoms in geometric grouping for well understanding the structure and dynamics of glass matrix. The FTIR spectra show two broad bands cover the wavenumber ranges 400-700 and 700-1300 cm-1 besides the peaks at 1380, 1450, 1621 and 1722 cm-1 therefore the FTIR spectra have been deconvoluted to identify the overlapped or concealed IR peaks for the various glass network building units. Therefore, the resultant FTIR data can be assigned as follows:
(a) The FTIR absorption peaks located at 444 and 540 cm-1 are correlated to the bending oscillation of bridging phosphorus such as O꓿P–O and/or O–P–O [20, 21] in PO3, PO4, and P2O7 phosphate species [22].
(b) The peak around 719 cm-1 may be allocated to bending oscillation of B–O–B linkages and symmetric stretching of the P–O–P linkages vibration modes of bridging oxygen.
(c) The spectral peaks positioned at 893 is attributed to asymmetric stretching oscillations of P-O-P within boro-phosphate glass [23, 24], though frequency at 966 cm-1 can be due to the vibration way of the isolated (PO4)3- tetrahedral units [25], the asymmetric stretching oscillation of P–O–P bond [24] or the symmetric stretching vibration of (PO3) units of Q1 structural species [24, 25].
(d) The spectral bands identified around 1029 cm-1 reflects both the asymmetric stretching oscillation of PO32- in Q1 species besides stretching oscillation of B-O in BO4- [23-25], while the frequency at 1115 cm-1 plus 1161 cm-1 are assigned to symmetric stretching vibration of (PO2)- in Q2 phosphate units and B-O in BO4 species [25].
(e) The IR absorption bands occurred at 1386 and 1440 cm-1 could be attributed to
B–O stretching oscillations of (BO3)3− species in pyro-, meta- and ortho-borate linkages, as well as to the P=O asymmetric stretching vibration of meta-phosphate (PO2) species [26].
(f) The OH links, H-O-H of water molecule or P-OH bending vibration are assigned spectral bands at 1621 and 1716 cm-1 [27].
The impact of molybdenum oxide on the glass structure is obviously observed at the widely broad band covering the wavenumber in the range from 800 -1500 cm-1. This band is indeed splitting into three IR spectral ranges positioned at 800–1000 cm-1, 1000–1300 cm-1 and 1300- 1500 cm-1 with more pronounced absorption peaks than that detected in the base glass spectrum. Molybdenum ions could be Mo6+ and Mo5+ within the glass network, get in the matrix as former and modifier when associated with four or six oxygen creating tetrahedral MoO4 and octahedral MoO6 structural species. Molybdenum ions revealed infrared absorption with vibration bands at about 920–900, 850–830, 800 and 430–410 cm-1. as well as asymmetric and symmetric oscillations of Mo-O-Mo links can be observed at about 600 and 450 cm-1, respectively as confirmed through various studies on molybdate glasses [28-31]. Through these findings, the existence of the spectral infrared peak at about 840 cm-1 in 5-Mo and 10-Mo glasses and at about 912 cm-1 in 15-Mo glass elucidates the contribution of molybdenum ions within the glass lattice as an insulated MoO4 tetrahedron. In addition, the appearance of absorption peak around 622-614 cm-1 and 440-435 cm-1 with increase the molybdenum content is credited to asymmetric vibration of the Mo-O-Mo linkage. Besides the absorption peaks appeared around 1313 and 1253 cm-1 are ascribed to asymmetric stretching oscillations of nonbridging oxygen of P-O-P in phosphate chains [32] and to both asymmetric stretching vibration of PO2- in Q2 units and asymmetric stretching vibration of BØ3 and BØ2O-, respectively [25-26]. beside the bands at around 1102 and 889 cm-1 are reduced, demonstrating a raise in the pyro-phosphate as well as BO3 units. In addition, the intensity of the spectral band around 963 cm-1 increased and shifted to shorter wavenumber. From FTIR results it is well-known that, the intensities of altered vibration bands of phosphate structures improved by rise in the content of MoO3. Such oxide operated as an ionic cross-linker among non-bridging oxygens (NBOs), and consequently, intensify the ionic bond strength and reduce the P–O bonds. Therefore, Mo ions generate Mo–O–P and Mo–O–B bonds through its modifying action that depolymerize the phosphate chains [28].
The FTIR vibration spectra of the immersed parent glass together with the doped samples reveals more simplified IR features than that of the same glasses before immersion and the combined multi-vibrational bands was diminished (Fig. 3). The FT-IR spectral modes are related to P-O vibration that associated with the creation of the calcium-phosphate layer upon immersion in SBF [33] that declare the development of apatite layer. The more prominent bands in the far-IR range (440-735) cm-1 located at 549 and 665 cm-1 and shifted to 565 and 646 cm-1 with high content of MoO3 can be ascribed to the P-O bending vibrations [33]. The intensity of the spectral peak in the range (1033-1039) cm-1 growth with the increase of MoO3 content that may be assigned to PO43- vibrations, characteristic for calcium phosphate phase. The high intensity peak at around 1149 cm-1 is correlated to the corrosion process involving the development of P–OH instead of P–Na or parallel units [27]. Additionally, the band identified at about 1633 cm-1 is due to ν3–vibrations of CO32– units [34]. These bands all in all are representative for the calcium phosphate phase (Ca3(PO4)2·xH2O) [34].
3.2. XRD Spectroscopy
Figure (4) shows the XRD pattern of the studied glasses before immersion in SBF. It exhibits a broad band with no eminent sharp peaks. Such XRD features are certainly consistent with amorphous (un-structured) nature of the glass samples.
Fig. (5) Illustrates the XRD on the glass surface after immersion for 14 days in SBF. The X-ray diffraction spectra shows a main calcium phosphate phase of formula calcium pyrophosphate (Ca2P2O7, CPP) in the range of 2θ (25-35) o as one of the intermediate products in the biomineralization process corresponding to JCPDS card no. 17-0499 [35].
3.3. SEM spectroscopy
Fig. (6) Shows the SEM micrographs of the surface morphology of the as-prepared glasses and all post immersed glass samples in SBF for 14 days. By comparing the SEM image before and after 14 days immersion in SBF is easy to point out morphological changes. The development of the apatite layer goes through two stages. Starting with the foundation of the amorphous calcium phosphate (ACP) coating and then finally converting to crystalline apatite [33]. As depicted from Fig. (6), glass shows no identified crystalline phases before immersion. However, there are different morphological features on the surface of the immersed samples thus indicating the creation of calcium-phosphate biolayer. The characterized rounded or nodular shaped of the bioactive apatite micro-species can be clearly identified on the most surface of the immersed samples and it is more developed as MoO3 content increase. Therefore, it can be observed that the addition of MoO3 strengthens the growth of HA layer so enhancement the bioactivity of the studied glass samples. This result is in harmony with the FTIR results.
3.4. Glass Surveying as a Delivery System for Ciprofloxacin
3.4.1. Loading of Drug onto Glass
Ciprofloxacin (CIP) is one of the Biopharmaceutics Classification System (BCS) Class II/IV drugs, which is an antibiotic of broad-spectrum, second-generation fluoroquinolone [36]. Fig (7) displays the loaded amount of ciprofloxacin onto each glass sample which indicated that CIP was successfully loaded onto the glass and could be released [37]. It is proposed that CIP was positively loaded onto the glass samples. This was recognized because of the occurrence of the P2O5 oxides in the glass matrix. Upon hydrolysis, such oxide was identified to form POH groups which could form hydrogen bonding with the drug molecules and as a result improved the CIP loading onto the glass [38].
3.4.2. In vitro Drug Release Profile
Fig. (8) shows the ciprofloxacin (CIP in %) cumulative release profile from the glass samples as a function of time. The profile release of drug exhibited a preliminary fast release stage followed by slower successive release stage. The transition to the second stage occurred at 12 hours and continued throughout the end of the releasing period up to 28 days (i.e., 700 hours) which may be accredited to the slow diffusion of the CIP molecules held inside the glass structure. It can be observed that the higher the MoO3 content the faster the drug release rate, that can be related to the nonbridging oxygens development and negative charge potential with molybdenum content increase. It was revealed that Mo5+ ions depolymerize the glass matrix by forming further bonding defects and molybdenum ions Mo6+ can exist in fourth-fold coordination, resulting in loose and more opened glass network [39]. In addition, molybdenum has a smaller ionic field strength than some other elements such as vanadium, so the dipole effect is weaker and therefore the negative charge effectiveness is smaller on oxygen for hydrogen bonding. Therefore, the Mo-O bond forms a weak hydrogen bond upon contact with drug functional groups as confirmed by El-Meliegy et al [39]. Thus, a continuous drug release profile was attained by using glass samples doped with Mo2O3 as delivery vehicle for ciprofloxacin [40].
3.5. Textural Analysis:
Fig. (9) Elucidates the N2 adsorption isotherms of glass samples. They correspond to the type IV isotherm agreeing to the arrangement of the IUPAC. In the samples, the representative hysteresis loop of this isotherm could be detected [at relatively high P/P0 values, the desorption branch did not monitor the same route as that of the adsorption one]. This performance evidently designated the existence of mesopores according to the IUPAC classification [41].
The allocation of pore size attained from the desorption branch of the isotherm following the BJH method for all samples are shown in Fig. (10). Moreover, all samples showed monomodal pore size distribution. Table 1 summarizes all data of the textural analysis for all samples. It could be seen that the addition of MoO3 was in charge of the decrease in the surface area of the MoO3 modified samples as compared with the control. However, by increasing the MoO3 content, the surface area was increased, as the modifier molybdenum enters the glass system which make it more connected. Furthermore, the high surface area could enable the dispersion of drug solution into the glass interior structure through the loading period. Additionally, glass could congregate the drug molecules inside their pores and perform as reservoirs for the drug.
Table 1: The data of the textural analysis carried out for studied glass samples
Glass sample code
|
0-Mo
|
5-Mo
|
10-Mo
|
15-Mo
|
Surface area
|
0.89
|
0.15
|
0.29
|
0.45
|
Average pore diameter (nm)
|
5.94
|
4.51
|
5.88
|
4.91
|
Total pore volume (cm3 g-1)
|
1.33E-03
|
1.75E-03
|
4.32E-04
|
5.58E-04
|
3.6. The Kinetics of Cumulative Drug Released
To study the in vitro release kinetics, the drug released cumulative percent was plotted against time in hours. The in vitro release mechanism of ciprofloxacin was determined by fitting the dissolution data into two mathematical release models: Zero Order and Higuchi models of fitting [42, 43]. The kinetic equations, and regression coefficient, R2, were used as a suggestion of data fitting.
To investigate the kinetics of the released drug, we alienated curve in Fig (8) into two parts. First part was solved by zero order model and the second part by Higuchi model fitting. For zero-order release kinetics, the dissolution of a drug is merely a function of time. Such model is accurate in case of very slow drug release. The regression coefficient (R2) and kinetic equations are used as a clue of data fitting. In order to decide which model is appropriate for the drug release kinetics, the regression coefficients (R2) were considered by means of regression analysis. The diverse kinetic equations are zero order drug release model which deliberate the process of constant drug released from the drug delivery device and other delivery system suggested by equation (1):
Qt = Q0 + K0 t (1)
Where, Qt is the quantity of drug released in time t, Q0 the original amount of drug in sample solution and K0 is the zero-order constant.
On the other hand, the second model Higuchi is the relation between drug release concentration (%) and the square root of time (t0.5), to study the release of water soluble and poorly soluble drugs from variable matrices represented by Eq. 2:
Qt =KHt0.5 (2)
Where, KH is the Higuchi release rate constant. To clarify the mechanism of drug release, and to find a suitable model for drug release kinetics; the regression coefficient (R2) was calculated from the curve, in the present study; R2 was greater than 0.9 [i.e., it is significant to such model fitting]. Hence, it could be concluded that the regression coefficient (R2) of the in vitro release profile for ciprofloxacin drug could be best uttered by zero order and Higuchi models fitting (R2 > 0.9).