A Letter to Reconsider the Conditions for Testing Decontaminated N95 Respirators for Emergency Reuse to Address Shortage

Received: June 22, 2020
Revised: June 22, 2020
Accepted: June 29, 2020
Download Citation: RIS|BibTeX|https://doi.org/10.4209/aaqr.2020.06.0339  

Cite this article:

Vejerano, E.P. and Ahn, J. (2020). A Letter to Reconsider the Conditions for Testing Decontaminated N95 Respirators for Emergency Reuse to Address Shortage. Aerosol Air Qual. Res. 20: 1713–1715. https://doi.org/10.4209/aaqr.2020.0.0339

HIGHLIGHTS

• N95 respirators tested at 85 L min^–1 have predicted efficiencies of < 69%.
• Experimental efficiencies of respirators tested at 85 L min^–1 were < 55%.
• Test flow rate should be closer to normal breathing.
• Size of the test particle should reflect the size of respiratory aerosols.

MAIN TEXT

The shortage of N95 respirators was a critical issue during the early months of the COVID-19 pandemic. At that time, healthcare workers reused N95 respirators that are intended for single use. Some resorted to unproven methods of cleaning/sterilization that can severely compromise the ability of the respirator to capture airborne particles efficiently.

Recently, a guideline has been issued for testing decontaminated N95 respirators (NPPTL, 2020). In the guideline, the efficiency of used/decontaminated respirators will be tested against particles with a median diameter of 0.075 ± 0.020 µm at a flow rate of 85 L min^–1. For emergency reuse, the conditions in the guideline for testing used/decontaminated N95 respirators may be too stringent for two reasons. First, for most submicron particles, efficiency generally decreases at higher flow rates (note that efficiency will increase at extremely high flow rates). Second, existing lines of evidence suggest virus-laden respiratory aerosols are > 0.5 µm, which are efficiently captured by filters almost independent of flow rates.

To address the shortage of N95 respirators among healthcare workers, we describe the basis of our recommendation for testing N95 respirators for emergency reuse at the condition that mimics regular use of the respirators and the size of airborne respiratory aerosols. Based on our calculation and experimental measurement, heat/chemically treated N95 respirators will not pass under the condition prescribed in the guideline.

In our calculation, we assumed that heat/chemical treatments destroyed the electrostatic coating. Therefore, the single-fiber collection efficiency of the filter is entirely due to mechanisms of impaction, diffusion, and inertial impaction. Assuming a cross-sectional area of 81 cm², the normal breathing flow rate for an adult (5–7 L min^–1) (Warner and Patel, 2013) is equivalent to a face velocity (U) of ~1.02–1.43 cm s^–1. For a similar condition, the recommended flow rate in the guideline is equivalent ~12× the face velocity (U~17.5 cm s^–1) to that during normal breathing. In Table 1, we define low, medium, and high face velocities at values of 1.13, 7.20, 17.5 cm s^–1, respectively.

Table 1. Calculated efficiencies for different particle sizes and face velocities.

Fig. 1 depicts the calculated total efficiencies for a filter for different particle sizes as a function of face velocity. We chose particle sizes (d_p) of 0.020, 0.055, 0.075, 0.095, 0.118, 0.150, 0.180, 0.300, 0.500, and 1 µm, to assess the impact of small and large particles that include the range of the particle sizes in the guideline. At the low face velocity, all particle sizes had efficiencies > 95%. At the higher face velocityand for particle size 0.075 ± 0.020 µm, the efficiency was ≤ 95.8%. The efficiencies for particles ranging from 0.055–0.300 µm were 76.9% to 95%; the 0.180-µm particle exhibited the lowest efficiency. At medium face velocity, particles with sizes of 0.075 µm to 0.180 µm will have efficiencies < 90%, while the efficiency for particle size ranging from 0.055 µm to 0.3 µm was 82.5–99.7%. Extremely small particles (0.020 µm) are captured efficiently even at higher face velocity (> 95% at 100 cm s^–1) because of their high diffusivity. The measured experimental efficiency agrees well with the predicted efficiencies at the low face velocity (Table 1); for d_p~0.118 µm, the experimental efficiency was 99.5 ± 2.3%, whereas the calculated efficiency was 99.9%. At the high face velocity, the predicted efficiency was at most ~67.8%; the experimental efficiency was ~< 55%. If the SARS-CoV-2 viruses are naked particles floating in the air, ~90 nm in size (Kim et al., 2020), at the high face velocity, only ~83.7% of the particles will be collected.

Fig. 1. Dependence of the calculated efficiency for a filter as a function of face velocity (U) for different particle sizes.

We calculated efficiency (E) using , where  is the solidity or packing density, t is the filter thickness, d_f is the fiber diameter, and E_Σ is the sum of the single-fiber efficiencies due to diffusion, interception, and inertial impaction. We used the values of 0.05, 1 mm, and 2.0 µm for α, t, d_f, respectively. The vertical red line is the face velocity using the flow rate in the guideline, assuming a cross-sectional area of 81 cm². The vertical blue line is the face velocity we used in our test, whereas the vertical pink line is the face velocity at 35 L min^–1. The detail of the calculation is described in the Supplementary Appendix.

But when expelled from the respiratory tract by breathing, talking, coughing, or sneezing, viruses are encased in respiratory fluids, therefore, larger (Vejerano and Marr, 2018). Although the information on the size distribution of virus-laden aerosol is limited, existing lines of evidence suggest that viruses are contained in larger respiratory aerosols. Sick individuals expel larger respiratory droplets and aerosols than healthy individuals because of differences in the composition and properties of the secreted mucus (Edwards et al., 2004; Gralton et al., 2011). Also, the type of virus affects their emission. More human subjects (60%) infected with influenza A released the virus in their exhaled aerosols (d_p~0.300–< 5 µm) than those infected (14%) with influenza B (Fabian et al., 2008). But the study did not identify if the viruses were distributed in all size fractions, or only contained in the larger- or smaller-sized fraction. In a similar study, although human subjects infected with rhinovirus released smaller particles (d_p~0.300–0.449 µm) (Edwards et al., 2004), no pathogen has been detected in them (Fabian et al., 2011). In another study, while ferrets infected with the influenza virus expel mostly fine particle sizes within ~0.52–1.54 µm, only ferrets exposed to particles ≥ 1.5 µm became infected (Zhou et al., 2018). Sick ferrets that expelled virus-laden particles > 10 µm infected more healthy ferrets (Zhou et al., 2018).

While breathing may release smaller particles, including the most penetrating particle size (d_p~0.3 µm), findings in the literature suggest that virus-laden respiratory aerosols are > 0.5 µm (Fabian et al., 2011). These fine respiratory aerosols are captured efficiently by N95 respirators, even at higher face velocities. Therefore, we recommend adjusting the size of the test aerosols, or the face velocity should be close to that during breathing. Aerosol labs that can perform filter testing but at lower flow rates can relieve some of the burden experienced by certified testing labs during a pandemic

DISCLAIMER

 Reference to any companies or specific commercial products does not constitute an endorsement by the authors.