| Literature DB >> 31963436 |
Xesús Feás1, M Pilar Vázquez-Tato2, Julio A Seijas2, Anna Pratima G Nikalje3, Francisco Fraga-López4.
Abstract
Fifteen years ago, at least one multimated female yellow-legged Asian hornet (Vespa velutina Lepeletier 1836) arrived in France, which gave rise to a pan-European invasion. In this study, the isolation and characterization of chitin (CHI) that was obtained from Vespa velutina (CHIVV) is described. In addition, an easy procedure is carried out to capture the raw insect, selectively and with high rates of success. The chitin contents of dry VV was observed to be 11.7%. Fourier transform infrared spectroscopy (FTIR), solid-state NMR (ssNMR), elemental analysis (EA), scanning electron microscopy (SEM), and thermogravimetric analysis (TG) characterized the physicochemical properties of CHIVV. The obtained CHIVV is close to pure (43.47% C, 6.94% H, and 6.85% N), and full acetylated with a value of 95.44%. Additionally, lifetime and kinetic parameters such as activation E and the frequency factor A using model-free and model-fitting methods, were determined. For CHIVV the solid state mechanism that follows the thermodegradation is of type F2 (random nucleation around two nuclei). The invasive Asian hornet is a promising alternative source of CHI, based on certain factors, such as the current and probable continued abundance of the quantity and quality of the product obtained.Entities:
Keywords: Asian hornet; Vespa velutina; chitin; insects; invasive species; polymer
Year: 2020 PMID: 31963436 PMCID: PMC7024375 DOI: 10.3390/molecules25020384
Source DB: PubMed Journal: Molecules ISSN: 1420-3049 Impact factor: 4.411
Figure 1Fourier-transform infrared spectroscopy (FT-IR) spectrum data of chitin extracted from Vespa velutina. 1652 and 1620 amide I (Am-I), 1552 amide II (Am-II) characteristic of α-chitin.
Figure 2Solid-state CP–MAS 13C NMR of chitin extracted from Vespa velutina. 13C NMR (126 MHz): δ 267.96, 173.17, 104.12, 82.74, 75.34, 60.34, 55.94, 22.79.
Elemental composition measurements and theoretical values for chitin from Vespa velutina.
| % C | % H | % N | % CHN | C/N | DA% | |
|---|---|---|---|---|---|---|
| 43.47 | 6.94 | 6.85 | 57.26 | 6.35 | 95.44 | |
| Theoretical value of chitin | 47.29 | 6.40 | 6.90 | 60.59 | 6.86 | 100 |
| Found-Theoretical | −3.82 | 0.54 | −0.05 | −3.33 | −0.51 | −4.56 |
Figure 3Scanning electron microscopy (SEM) pictures of chitin isolated from Vespa velutina. (a) magnification ×1500 (scale bar = 10 μm); (b) magnification ×5500 (scale bar = 2 μm); (c) magnification ×1500 (scale bar = 10 μm) and (d) magnification ×2500 (scale bar = 10 μm).
Figure 4Experimental thermogravimetric (TG) curves at different heating rates of chitin isolated from Vespa velutina.
Inflection point temperatures at different rates for chitin.
| B (°C/min) | T (°C) |
|---|---|
| 5 | 363 |
| 10 | 367.8 |
| 15 | 369.3 |
| 20 | 376.3 |
Degradation energies at different conversions for chitin obtained from Vespa velutina.
| α | Ea(kJ/mol) |
|---|---|
| 5 | 117.8 |
| 10 | 118.9 |
| 15 | 114.1 |
| 20 | 105.5 |
Degradation energies at different heating rates and different thermodegradation mechanisms for Vespa velutina chitin.
| Solid State Process | Mechanism | 5 °C/min | 10 °C/min | 15 °C/min |
|---|---|---|---|---|
| Nucleation and growth (Avrami Equation (1)) | A2 | 35.2 | 53.6 | 44.7 |
| Nucleation and growth (Avrami Equation (2)) | A3 | 16.9 | 33.8 | 11.3 |
| Nucleation and growth (Avrami Equation (3)) | A4 | 6.5 | 17.4 | 5.9 |
| Phase boundary controlled reaction (one-dimensional movement) | R1/F0 | 67.1 | 53.7 | 73.6 |
| Phase boundary controlled reaction (contracting area) | R2 | 77.2 | 62.8 | 82.7 |
| Phase boundary controlled reaction (contracting volume) | R3 | 80.8 | 66.07 | 85.9 |
| One-dimensional diffusion | D1 | 187.7 | 161.8 | 181.5 |
| Two-dimensional diffusion | D2 | 200.9 | 173.7 | 193.4 |
| Three-dimensional diffusion (Jander eq.) | D3 | 215 | 186.6 | 202.4 |
| Three-dimensional diffusion (Ginstling-Brounshtein eq.) | D4 | 205.6 | 177.9 | 197.6 |
| Random nucleation with one nucleus on the individual particle | F1 | 88 | 72.5 | 92.36 |
| Random nucleation with two nuclei on the individual particle |
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| Random nucleation with three nuclei on the individual particle |
| 137.1 |
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Half-life for chitin samples extracted from Vespa velutina at different temperatures.
| T (°C) | Time (years) |
|---|---|
| 20 | 285 |
| 30 | 61 |
| 40 | 14 |
| 50 | 4 |
| 60 | 1 |
| 70 | 0.3 (110 days) |
| 80 | 0.1 (37 days) |
| 90 | 0.03 (12 days) |
| 100 | 0.01 (5 days) |
Figure 5(a) The trap used to catch the Vespa velutina; (b) The (black dots) show the distribution of the traps in the apiary.