The fixed samples were treated with 5% AgNO3 solution for 5 min under ultraviolet radiation. After removing the AgNO3 solution, the samples were washed with PBS twice followed by the addition of 5% Na2S2O3 solution to the plate and allowing the plates to stand for 5 min. Finally, the samples were washed twice with distilled water and digital images of the Selleck Idasanutlin stained cells were obtained. Statistical analysis The results are displayed as the mean ± standard deviation. The statistical differences were determined using a student’s two-tailed

test. Scheffe’s method was used for the multiple comparison tests at a level of 95%. Results and discussion Preparation of nanofiber scaffolds Figure 2 illustrates the FESEM images of the electrospun PLGA/nHA-I, PLGA/nHA, and pristine PLGA nanofibers scaffolds. With optimized electrospinning click here parameters, no remarkable change was observed in the morphology of pristine PLGA, PLGA/nHA, or PLGA/nHA-I composite nanofiber scaffolds. The nanofibers were smooth and beadless in all the samples. However, the average diameters of PLGA/nHA (mean average diameter 500 nm) and PLGA/nHA-I (mean average diameter 520 nm) composite nanofibers increased slightly as compared to pristine PLGA

nanofiber having (mean average diameter 450 nm). This increase in the average diameter might be due to the incorporation of pristine nHA and nHA-I in the PLGA polymer matrix. A similar increase in the average diameter of the modified nanofibers has been also reported elsewhere [27]. Figure 2 FESEM images of (a) pristine PLGA, (b) PLGA/nHA, and (c) PLGA/nHA-I nanofiber scaffolds. Fourier learn more transform infrared spectroscopy Protirelin study Figure 3 illustrates the Fourier transform infrared (FTIR) spectra of the pristine nHA, nHA-I, pristine PLGA, and PLGA/nHA-I composite nanofiber scaffolds. The sharp band, which appeared in the regions of 1,000 to 1,100 cm-1 in the pristine

nHA spectrum is characteristic of a regular tetrahedral (PO4 -3) of nHA (Figure 3(a)) [28, 29]. The appearance of weak doublet bands in the region of 2,800 cm-1 to 3,200 cm-1 in nHA-I spectrum (Figure 3(b)) was attributed to hydrocarbons (CH, CH2) of succinic acid [30]. The two sharp bands at 1,648 and 1,540 cm-1 were attributed to the stretching vibration of the carbonyl group (C = O) within amide I (-CO-NH) and the coupling of N-H bending and C-N stretching of amide II (-CO-NH) [31]. The appearance of these bands at their characteristic positions confirmed the grafting insulin on the surface of succinic acid-modified nHA-s. The band at 3,500 cm-1 was attributed to the free carboxylic acid (COOH) moiety present in insulin [28]. A sharp peak at 1,742 cm-1 appeared in the PLGA polymer spectrum (Figure 3(c)), which was assigned to the C = O stretching of PLGA polymers.