| Literature DB >> 35936028 |
Ashutosh Kumar1, Abhishek Raj1,2, Ankit Gupta2,3, Sneha Gautam4, Manish Kumar5, Hemant Bherwani1,2, Avneesh Anshul1,2.
Abstract
The high rate of transmission of the COVID-19 virus has brought various types of disinfection techniques, for instance, hydrogen peroxide vaporization, microwave generating steam, UV radiation, and dry heating, etc. to prevent the further transmission of the virus. The chemical-based techniques are predominantly used for sanitization of hands, buildings, hospitals, etc. However, these chemicals may affect the health of humans and the environment in unexplored aspects. Furthermore, the UV lamp-based radiation sanitization technique had been applied but has not gained larger acceptability owing to its limitation to penetrate different materials. Therefore, the optical properties of materials are especially important for the utilization of UV light on such disinfection applications. The germicidal or microorganism inactivation application of UV-C has only been in-use in a closed chamber, due to its harmful effect on human skin and the eye. However, it is essential to optimize UV for its use in an open environment for a larger benefit to mitigate the virus spread. In view of this, far UV-C (222nm) based technology has emerged as a potential option for the sanitization in open areas and degradation of microorganisms present in aerosol during the working conditions. Hence, in the present review article, efforts have been made to evaluate the technical aspects of UV (under the different spectrum and wavelength ranges) and the control of COVID 19 virus spread in the atmosphere including the possibilities of the human body sanitization in working condition.Entities:
Keywords: COVID-19; Disinfection; UV radiation; UV-C, Sanitization
Year: 2022 PMID: 35936028 PMCID: PMC9345658 DOI: 10.1016/j.gr.2022.07.010
Source DB: PubMed Journal: Gondwana Res ISSN: 1342-937X Impact factor: 6.151
Fig. 1Different types of UV on the basis of their wavelength as per ISO 21348.
Fig. 2(a) Various emission spectrum of UV LED. (b) Dose response characteristic of the HCoV-OC43 disinfected through UV-LEDs. N signifies the virus count after the designated irradiation and N0 represent the time zero (without irradiation). Panel (a-b) are reprinted with permission from (Gerchman et al., 2020), copyright Elsevier 2020.
Different form of UV in terms of disinfection with respective dose and time duration.
| 1. | UV-LED (267 & 279 nm) | – | 7 mJ/cm2 | 3-log inactivation of HCoV-OC43 | ( |
| 2. | UV-C (254) | 9 min | 1048 mJ/cm2 | High infectious titer of 5 | ( |
| 3. | UV-A (365 nm) | 15 min | 1048 mJ/cm2 | Weak effect was observed on infectious titer of 5 | ( |
| 4. | UV-chip | 3 min | 15 mJ/cm2 | The SARS-CoV-2 charge decline at 99.94% | ( |
| 10 min | 35 mJ/cm2 | Highest measurable attenuation of 5.7 Log (99.9998%) | ( | ||
| 5. | Far UV-C (222 nm) | 25 min | 3 mJ/cm2 | Aerosolized coronavirus 229E and OC43, respectively inactivated by almost 99.9%. | ( |
| 6. | UV-C (254) | 2.98 s | 6.556 mJ/cm2 | UV Clight was able to inactivate more than 99 % of SARS-CoV-2 viral particles | ( |
| 7. | UV-C(222 nm) | 30 s | 3 mJ/cm2 | The obtained result exhibited a 99.7% reduction of viable SARS-CoV-2 based on the TCID 50 assay | ( |
| 8. | UV-C (254 nm) | – | 1.5 J/cm2 | Efficiently deactivate the facepieces of 3 M 1860 and Moldex 1511 | ( |
| 9. | UV-C (222 nm) | 15 s | 81 mJ/cm2 | SARS-CoV-2 from forty-eight locations, become negative | ( |
| 10. | UV-C (253.7 nm) | 30 s | 500 μW/cm2 | Reduced SARS-CoV-2 by 10−4.9 fold | ( |
Fig. 3Inhibitory result of DUV-light on SARS-CoV-2. (a) Cytopathic variation in virus infected Vero cells under different irradiation conditions including (0 s) without DUV LED –light or with DUV LED –light for 1, 10, 20, 30, 60 s and each of them corresponds to 3.75, 37.5, 75, 112.5, or 225 mJ/cm2, respectively. (b) Formation of Plaque in Vero cell. (c) Disinfection of SARS-CoV-2 though DUV-LED irradiation under different time. Panel (a-c) are reprinted with permission from (Inagaki et al., 2020).
The emission maxima from halogens with rare gases in their respective combinations (Kogelschatz, 2004, Lebedev and Pryanichnikov, 1993, Pikulev et al., 2012).
| 172 nm | 146 nm | 126 nm | 84 nm | 74 nm | |||
|---|---|---|---|---|---|---|---|
| F | 157 nm | 354 nm | 248 nm | 193 nm | 108 nm | ||
| Cl | 259 nm | 308 nm | 175 nm | ||||
| Br | 289 nm | 282 nm | 207 nm | 165 nm | |||
| I | 342 nm | 253 nm | 190 nm | ||||
Fig. 4Oxygen absorption with different wavelength of UV. (b) The plot of the spectral power distribution of a typical KrCl lamp in semi logarithmic scale. Panel (a-b) are reprinted with permission from (Claus, 2021), copyright John Wiley and Sons 2021.