<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">Health</journal-id><journal-title-group><journal-title>Health</journal-title></journal-title-group><issn pub-type="epub">1949-4998</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/health.2021.134035</article-id><article-id pub-id-type="publisher-id">Health-108761</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Biomedical&amp;Life Sciences</subject><subject> Medicine&amp;Healthcare</subject></subj-group></article-categories><title-group><article-title>
 
 
  Leakage versus Material Filtration in Barrier Facemask Efficiency
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Ali</surname><given-names>Bahloul</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Clothilde</surname><given-names>Brochot</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Barbara</surname><given-names>Layne</given-names></name><xref ref-type="aff" rid="aff3"><sup>3</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Chemical and Biological Hazard Prevention, Institut de recherche Robert-Sauvé en santé et en sécurité du travail, Montréal, Canada</addr-line></aff><aff id="aff2"><addr-line>Department of Building, Civil and Environmental Engineering, Concordia University, Montréal, Canada</addr-line></aff><aff id="aff3"><addr-line>Department of Studio Arts, The Milieux Institute for Art, Culture and Technology, Concordia University, Montréal, Canada</addr-line></aff><pub-date pub-type="epub"><day>09</day><month>04</month><year>2021</year></pub-date><volume>13</volume><issue>04</issue><fpage>439</fpage><lpage>453</lpage><history><date date-type="received"><day>6,</day>	<month>March</month>	<year>2021</year></date><date date-type="rev-recd"><day>24,</day>	<month>April</month>	<year>2021</year>	</date><date date-type="accepted"><day>27,</day>	<month>April</month>	<year>2021</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  The World Health Association and many governmental agencies recommend the wearing of facemasks by the general public to prevent the spread of COVID-19. It is believed that masks can significantly protect others and may offer some protection to the wearer. Although there are standards for FFRs, surgical masks, and recently for barrier face coverings, they all indicate the level of protection for the wearer. However, testing facial masks not at the point of inhalation, but at the source, the exhale, offers a new perspective on how to impede particle emissions. In this paper, the experimental results show that, although the barrier face covering is less effective than FFRs or surgical masks, it can reduce the concentration of aerosols downstream of the device. The results on barrier efficiency show a rapid decrease in effectiveness when the face covering is not sealed to the head. The barrier efficiency of two of the barrier face coverings tested is strongly dependent on leakage caused by the fit rather than the material. While some materials certainly are more effective than others in inhibiting particle penetration, an even more profound factor is the amount of leakage emitted from a mask. New approaches to fit and design in order to create a seal against leakage will become an important factor in combatting SARS-CoV-2.
 
</p></abstract><kwd-group><kwd>COVID-19</kwd><kwd> Facemask</kwd><kwd> Filtration</kwd><kwd> Leakage</kwd><kwd> Aerosol</kwd><kwd> Airborne Transmission</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Following numerous calls from the scientific community to outline evidence on the route of airborne transmission of SARS-CoV-2 [<xref ref-type="bibr" rid="scirp.108761-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.108761-ref2">2</xref>], the World Health Organization (WHO) [<xref ref-type="bibr" rid="scirp.108761-ref3">3</xref>] has updated its information on the routes of transmission of SARS-CoV-2 to integrate this new information into the two other transmission routes: contact and droplet transmission route. Facial masks are a key component of most reopening plans with some governments making masks obligatory in public spaces [<xref ref-type="bibr" rid="scirp.108761-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.108761-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.108761-ref6">6</xref>]. Recent findings [<xref ref-type="bibr" rid="scirp.108761-ref7">7</xref>] demonstrate that the mandating of face coverings for use in public spaces has been associated with a decline in the daily COVID-19 growth rate in selected locations in the USA. This suggests that hundreds of thousands of cases may have been averted by these directives.</p><p>In the light of this recommendation, one must first define the different “masks” that can be used during this pandemic period. It can be classified according to their use: some are designed to protect the wearer from environmental exposure (filtering facepieces respirators, FFRs), while other face coverings protect individuals from the wearer’s potential emissions. FFRs are disposable respiratory protection devices intended to protect the user against inhalation of harmful agents (such as aerosols). This type of mask is generally used in workplaces. In Canada [<xref ref-type="bibr" rid="scirp.108761-ref8">8</xref>], the wearing of medical masks is mainly recommended in healthcare establishments. On the other hand, face covering masks are designed to limit the spread of germs by the wearer in their environment, primarily by retaining respiratory droplets.</p><p>FFRs and surgical masks are devices widely used before the pandemics are subjected to standards testing before they are released to the market. For example, in North America, N95 FFRs are regulated by 42 CFR Part 84 [<xref ref-type="bibr" rid="scirp.108761-ref9">9</xref>]. This standard establishes performance via the filtration efficiency and the pressure drop measurements. In this study, the authors refer to the NIOSH certification as a reference. Also, fit tests are required to choose the best FFR considering the wearer’s face. However, no fit testing is mandated for medical masks.</p><p>Some papers are based on the classical efficiency measurement method (i.e. applied according to standards) in an attempt to estimate the effectiveness of these facemasks [<xref ref-type="bibr" rid="scirp.108761-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.108761-ref11">11</xref>] [<xref ref-type="bibr" rid="scirp.108761-ref12">12</xref>] [<xref ref-type="bibr" rid="scirp.108761-ref13">13</xref>]. They show that wearing a mask reduces the amount of aerosol generated downstream of the mask. However, the effectiveness is generally lower than the N95 FFRs or surgical mask efficiencies. Some researchers have proposed new methodologies to measure the material’s efficiency or the mask’s performance [<xref ref-type="bibr" rid="scirp.108761-ref14">14</xref>] [<xref ref-type="bibr" rid="scirp.108761-ref15">15</xref>] [<xref ref-type="bibr" rid="scirp.108761-ref16">16</xref>]. However, these methodologies either count particles larger than 0.5 micrometer or have been tested in a non-controlled environment.</p><p>Homemade facemasks or barrier face coverings are simple cloth face coverings that can be made at home and can help prevent the spread of COVID-19. A plethora of commercial and homemade facemasks appeared widely during the pandemic, and many tutorials for making facemasks could be found in different countries [<xref ref-type="bibr" rid="scirp.108761-ref17">17</xref>] [<xref ref-type="bibr" rid="scirp.108761-ref18">18</xref>]. It is still unknown which facemasks are most beneficial as there are countless variables in materials and designs.</p><p>The ASTM F3502-21 [<xref ref-type="bibr" rid="scirp.108761-ref19">19</xref>] standard, recently published in 2021, describes the specifications for barrier face coverings. This standard presents the methodology for testing filtering efficiency of the material. This method is generally applied to the assessment of inhalation efficiency and not exhalation efficiency. Indeed, the standard does not take into account the protection efficiency via the emitter wearing the barrier mask. Also, the fit factor is not considered in this standard.</p><p>The question here is whether a classical methodology is applicable to facemasks. In addition to efficiency and pressure drop, the fit of the mask to the head could be a predominant parameter for facemasks. Leaks from around the outer edges of the mask drastically decrease mask efficiency. Measurements on respiratory protection devices have shown that this decrease becomes greater in relation to increased amounts of leakage [<xref ref-type="bibr" rid="scirp.108761-ref20">20</xref>] [<xref ref-type="bibr" rid="scirp.108761-ref21">21</xref>] [<xref ref-type="bibr" rid="scirp.108761-ref22">22</xref>]. Van der Sande et al. [<xref ref-type="bibr" rid="scirp.108761-ref23">23</xref>] and Davies et al. [<xref ref-type="bibr" rid="scirp.108761-ref24">24</xref>] determined that facemasks provided about half the protection of standard surgical masks. Their results also demonstrate the importance of the fit. In the case of respiratory protective devices, respiratory protective device functions at negative pressure. In the case of facemasks, emission takes place under positive pressure that may increase the role of leaks in the wearer’s emission. Since it is generally considered that wearing a facemask is essentially to protect others, the scientific community should find a standard methodology to assess and qualify them. What is the relationship between the efficiency of materials used in masks and controlling particle leakage that may be expressed through the sides or other points of escape inherent to a mask’s design? Testing that measures the amount of particle escape in various mask scenarios leads to a clearer understanding of how the virus may enter the environment, providing new insights on how microorganism containment might best be achieved.</p><p>The goal is to determine the effects of the material filtration properties versus the effect of leakage related to facemask fit or holes in the design on the barrier efficiency. To determine how the environment may influence the results, tests are conducted in both a ventilated room and a controlled chamber. Different conditions are analyzed according to the environment, the filtration and air resistance properties of the facemask, the inhalation flowrate of the person to protect and the leakage due to the fitting of the mask. Two manikin heads are used, one head simulates the emitter (exhalation), the other acts as the receptor (inhalation). Barrier efficiency consists of an evaluation of the performance of the facemask in stopping projectiles from the wearer’s mouth simulating the droplets generated by coughing, sneezing, exhalation, and speaking. Particle sizes smaller than 1 mm are used, representing the worst-case scenario since they are likely to pass through the facemask material and also escape as leakage between the facemask and the manikin head.</p></sec><sec id="s2"><title>2. Materials and Methods</title><sec id="s2_1"><title>2.1. Facemasks</title><p>Three different facemasks are used during this study (<xref ref-type="fig" rid="fig1">Figure 1</xref>): two commercially available facemasks and one homemade mask made of one-layer of woven cotton and designed according to an online pattern. The facemasks are labelled as the “white facemask”, “blue facemask” and the “green facemask”. Each is tested inside a chamber under controlled conditions (<xref ref-type="fig" rid="fig2">Figure 2</xref>(b)).</p></sec><sec id="s2_2"><title>2.2. Facemasks’ Characteristics</title><p>The characteristics of the three facemasks used in this study are presented and compared in <xref ref-type="table" rid="table1">Table 1</xref>. The white facemask contains an electret medium, whose fibers are electrostatically charged. These charges allow the particles to be collected with an additional collection mechanism of electrostatic forces. The blue facemask contains a mechanical medium, collecting the particles through sedimentation, interception, inertial impaction and Brownian diffusion.</p></sec><sec id="s2_3"><title>2.3. Facemasks’ Filtration Efficiency and Pressure Drop</title><p>In this section, the filtration characteristics of the materials of the three facemasks are determined by using the classical methodology on an existing setup for measuring the performance of respiratory protection devices [<xref ref-type="bibr" rid="scirp.108761-ref24">24</xref>] [<xref ref-type="bibr" rid="scirp.108761-ref25">25</xref>] [<xref ref-type="bibr" rid="scirp.108761-ref26">26</xref>] [<xref ref-type="bibr" rid="scirp.108761-ref27">27</xref>] [<xref ref-type="bibr" rid="scirp.108761-ref28">28</xref>]. <xref ref-type="fig" rid="fig3">Figure 3</xref>(a) and <xref ref-type="fig" rid="fig3">Figure 3</xref>(b) respectively show the initial filtration efficiency and the pressure drop of the three facemasks at the receptor inhalation flowrate of 85 L/min. One can note that a certified N95 FFR must have a minimum</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Characteristics of facemasks</title></caption><table><tbody><thead><tr><th align="center" valign="middle" ></th><th align="center" valign="middle"  colspan="3"  >Facemasks</th></tr></thead><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" >White facemask</td><td align="center" valign="middle" >Blue facemask</td><td align="center" valign="middle" >Green facemask</td></tr><tr><td align="center" valign="middle" >Surface area (cm<sup>2</sup>)</td><td align="center" valign="middle" >305 cm<sup>2</sup></td><td align="center" valign="middle" >260 cm<sup>2</sup></td><td align="center" valign="middle" >285 cm<sup>2</sup></td></tr><tr><td align="center" valign="middle" >Number of layers and compositions</td><td align="center" valign="middle" >One layer of electret medium between two layers of polymers</td><td align="center" valign="middle" >One layer of mechanical medium between two layers of polymers</td><td align="center" valign="middle" >One layer of woven cotton fabric (thread count: 120)</td></tr><tr><td align="center" valign="middle" >Fiber diameters</td><td align="center" valign="middle" >External: 42 &#177; 4 &#181;m Medium: 10 &#177; 5 &#181;m Internal 42 &#177; 4 &#181;m</td><td align="center" valign="middle" >External: 60 &#177; 5 &#181;m Medium: 15 &#177; 6 &#181;m Internal 52 &#177; 5 &#181;m</td><td align="center" valign="middle" >25 &#177; 10 &#181;m</td></tr><tr><td align="center" valign="middle" >Images (1600&#215;)</td><td align="center" valign="middle" >External: <inline-formula><inline-graphic xlink:href="/html.scirp.org/file/10-8205256x4.png" xlink:type="simple"/></inline-formula> Medium: <inline-formula><inline-graphic xlink:href="/html.scirp.org/file/10-8205256x5.png" xlink:type="simple"/></inline-formula> Internal: <inline-formula><inline-graphic xlink:href="/html.scirp.org/file/10-8205256x6.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >External: <inline-formula><inline-graphic xlink:href="/html.scirp.org/file/10-8205256x7.png" xlink:type="simple"/></inline-formula> Medium: <inline-formula><inline-graphic xlink:href="/html.scirp.org/file/10-8205256x8.png" xlink:type="simple"/></inline-formula> Internal: <inline-formula><inline-graphic xlink:href="/html.scirp.org/file/10-8205256x9.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="/html.scirp.org/file/10-8205256x10.png" xlink:type="simple"/></inline-formula></td></tr></tbody></table></table-wrap><p>filtration efficiency of 95% and a maximum pressure drop of 3.43 mbar. One then plays between the two parameters to have a good efficiency while having an acceptable breathability for the wearer.</p><p>The white facemask material has a filtration efficiency of more than 90% and a low pressure drop of 0.3 mbar. The white facemask made of fiber is then very advantageous because it has good filtration efficiency and good breathing comfort.</p><p>The blue facemask material has a filtration efficiency of around 80% and a pressure drop of 0.6 mbar. The filtration efficiency and the breathing comfort associated with the blue facemask material are also acceptable.</p><p>Finally, the green facemask has a low filtration efficiency of less than 20% and pressure drop of 0.5 mbar. However, this resistance increases rapidly during the test. Clogging of the fabric material occurs on the surface and thus makes it uncomfortable with use.</p></sec><sec id="s2_4"><title>2.4. Aerosol Generation</title><p>A wet air jet containing NaCl particles is installed at the mouth of the exhalation head using an orifice with an air expiration speed of 6 m/s. According to previous studies, this can be considered as an extreme case. Respiration and speech generate jet speeds rarely exceeding 5 m/s [<xref ref-type="bibr" rid="scirp.108761-ref29">29</xref>] and mainly expel small droplets. Violent expiratory events such as coughing and sneezing generate turbulent jets with higher maximum speeds [<xref ref-type="bibr" rid="scirp.108761-ref29">29</xref>] [<xref ref-type="bibr" rid="scirp.108761-ref30">30</xref>] [<xref ref-type="bibr" rid="scirp.108761-ref31">31</xref>]. Experimental studies are still needed, in particular on the size distribution and velocities produced by sneezing. Humid NaCl particles are used to simulate droplets coming from head-exhalation. These particles are generated by a 6-jet collision (BGI) based on an NaCl solution using a flowrate of 15 L/min. The aerosol generation follows the NIOSH standard. The lognormal distribution has a mean count diameter around 70 nm and a geometric standard deviation lower than 1.86. Although particles of size around 100 nm cannot reflect the whole generated bioaerosol, it represents the “worst case scenario”.</p></sec><sec id="s2_5"><title>2.5. Measurement Method</title><p>A Scanning Mobility Particle Sizer (SMPS) is used to measure the concentration of NaCl particles inhaled by the receptor. The aerosol is collected by a probe inside the head. It is then selected according to its electric mobility diameter, by the electrostatic classifier used with a Long Differential Mobility Analyzer (Long-DMA TSI 3082) and the concentration is measured by a Condensation Particle Counter (CPC TSI 3752). Barrier efficiency is defined by the effectiveness of the facemask worn by the emitter head in stopping the transmission of the simulated virus to the receptor head. The measurement was carried out at the beginning of the experiment, before any possible clogging effect and facemasks were not conditioned before their use. As the authors use the 42 CFR Part 84 standard as a reference, the barrier efficiency measurements are performed at a constant flow rate of 85 L/min.</p><p>Barrier efficiency (E<sub>barrier</sub>) is then obtained via the ratio of average concentrations, expressed in number, with and without using facemasks using the following Equation (1). The results presented in this paper are the mean of three measurements.</p><p>E barrier = 1 − C with   mask C without   mask (1)</p><p>First, the barrier efficiency of one facemask is analyzed in a ventilated room with negative pressure (<xref ref-type="fig" rid="fig2">Figure 2</xref>(a)). and then in a controlled environment chamber (<xref ref-type="fig" rid="fig2">Figure 2</xref>(b)). Based on this comparison it was decided to perform the experiments in the controlled environment chamber to limit the variables to only the properties of the facemask with no environmental influences.</p></sec><sec id="s2_6"><title>2.6. Barrier Efficiency in a Ventilated Room</title><p>The ventilation room is a negative pressure chamber (controlled at −20 mbar) 5 meters long, 3 meters wide and approximately 2.5 meters high. An air supply plenum is installed in the center of the chamber ceiling and an outlet plenum is located at 0.2 meters from the floor. The two heads are installed on a table facing one another (<xref ref-type="fig" rid="fig2">Figure 2</xref>(a)).</p><p>These first tests were carried out on the homemade green facemask in a ventilated room with negative pressure. <xref ref-type="fig" rid="fig4">Figure 4</xref> presents the barrier efficiency according to the particle diameter. “One green face” facemask curve is calculated when the emitter head wear a facemask and the “two green facemasks” curve is calculated when the two heads wear a facemask. Wearing a facemask by both manikin heads thus increases the barrier efficiency. It can be noted that the ventilation</p><p>and the presence of structures in the room could influence the barrier efficiency of the facemask.</p></sec><sec id="s2_7"><title>2.7. Barrier Efficiency in the Controlled Environment Chamber</title><p>The controlled environment chamber consists of a vein with a section of 30.5 cm &#215; 30.5 cm (1 foot &#215; 1 foot), and approximately 50 cm in length, installed in the ventilated room. Considering the walls of the vein and its length, one can consider that this experiment represents an unrealistic situation, or at least a “worst case scenario”. This configuration was actually chosen to facilitate the measurement and characterize the barrier efficiency in the different configurations tested. Two configurations are then used:</p><p>1) The two heads are installed in the controlled environment chamber. A facemask is installed on the emitter head. This configuration permits to study the leakages related to the fit of the facemask (<xref ref-type="fig" rid="fig2">Figure 2</xref>(b)).</p><p>2) Instead of the emitter head, a 2.5 cm diameter tube is used to hold a circular piece of material (<xref ref-type="fig" rid="fig5">Figure 5</xref>). Assuring a complete seal around the perimeter of the fabric, this configuration provides a better control of the amount of leakage by creating 1.5 mm holes with an electric drill.</p><p>In the following test, two manikin heads were placed in the controlled environment chamber to isolate the heads (<xref ref-type="fig" rid="fig2">Figure 2</xref>(b)). Only the emitter head wears a facemask (the green homemade facemask).</p></sec><sec id="s2_8"><title>2.8. Calibration Tests in the Controlled Environment Chamber: Distance Test, Flow Rate Inhalation and Reproducibility Tests</title><p>The concentration of particles at 3 sizes (100, 300 and 600 nm) transmitted by the head source is measured as a function of the distance, separating the two manikin heads (<xref ref-type="fig" rid="fig6">Figure 6</xref>(a)). It is found that the concentration of the particles remains uniform in the distance range of 20 and 50 cm. In the controlled environment chamber, the transmission of particles released by the emitter is not influenced by the distance separating the two manikin heads. In the case of fine droplets in a poorly ventilated small space, distance alone seems to be insufficient in reducing coronavirus transmission.</p><p>The inhalation effect by the receptor head is analyzed at three different flowrates, 42.5, 60 and 85 L/min (<xref ref-type="fig" rid="fig6">Figure 6</xref>(b)). For particles of approximately</p><p>100 nm in size, the inhalation flowrate slightly increases the barrier efficiency in the test chamber. Small aerosols (around 100 nm) are carried more by the airflow. The greater the inhalation flowrate, the greater the intake of outside air into the chamber. Consequently, the dilution of the concentration of the particle transmission is great and subsequently the barrier efficiency increases. In contrast, the inhalation flowrate does not have a big influence for particle sizes greater than 200 nm.</p><p>The data reported in this paper were the result from a single measurement. However, tests have been conducted to estimate the reproducibility for one of the facemasks. Three barrier efficiency tests were performed with the green facemask. In <xref ref-type="fig" rid="fig6">Figure 6</xref>(c), one can note that the standard deviation is less than 10% of the whole curve. It can be assumed that the standard deviations measured in this situation can be applied to all configurations of facemasks presented in the “result and discussion” section. This statement is supported by the design similarities of the facemasks and by the use on the same manikin heads.</p></sec></sec><sec id="s3"><title>3. Results and Discussions</title><sec id="s3_1"><title>3.1. Barrier Efficiency of the 3 Facemasks</title><p><xref ref-type="fig" rid="fig7">Figure 7</xref> shows the barrier effectiveness of the three facemasks in the test chamber. The distance between the two heads is 20 cm. The efficiency barrier includes both the effect of facemask materials and leakage due to facemask fitting on the emitter head.</p><p>The white facemask offers a barrier efficiency between 70% and 50%.</p><p>The blue facemask offers a barrier efficiency between 80% and 50%. This barrier efficiency is lower than the one associated with the white facemask. This difference could be due to the material of the facemask or to the fitting of the facemask</p><p>on the manikin head.</p><p>Finally, the green facemask offers a barrier efficiency between 60% and 40%. This last result shows that the barrier efficiency in the test chamber is lower than that performed in the ventilated room (<xref ref-type="fig" rid="fig4">Figure 4</xref>). In the ventilated room, particles not blocked by the green facemask disperse in all directions in the chamber and are diluted by the ventilation airflow. Transmission is then less important in the ventilated, open-environment room than in the confined environment without ventilation.</p><p>In <xref ref-type="fig" rid="fig7">Figure 7</xref>, one can observe that the green facemask offers less barrier efficiency than the blue and the white ones. However, the difference between the results obtained by the three material facemasks is not significant.</p></sec><sec id="s3_2"><title>3.2. Leakage Related to Fitting of the 3 Facemasks</title><p>To study the intrinsic impact of facemask materials on barrier efficiency, the facemasks are sealed on the facemask wearer to eliminate leaks due to fitting. The results obtained are then compared to those without sealing (<xref ref-type="fig" rid="fig8">Figure 8</xref>).</p><p>The materials of the white and blue facemasks effectively block the particles emitted by the source. The barrier efficiency is in the order of 100% (<xref ref-type="fig" rid="fig8">Figure 8</xref>(a) and <xref ref-type="fig" rid="fig8">Figure 8</xref>(b)). This efficiency quickly drops when the facemasks are not sealed on the head wearer. Barrier efficiency is therefore influenced by leaks due to fitting and not by the material of the white and blue facemasks.</p><p>The same result is observed for the green material of the textile facemask for particles larger than 500 nm (<xref ref-type="fig" rid="fig8">Figure 8</xref>(c)). The effect of leakage decreases significantly for particle sizes below 500 nm. However, the barrier efficiency of the sealed green facemask is greater than that the unsealed one. It is greater than 70% for particles of size less than 500 nm and it reaches a barrier efficiency of 90% for particles of size greater than 500 nm.</p><p>The barrier efficiency appears to decrease when the particle size increases from 100 nm to 500 nm, and this trend is more pronounced for commercial facemasks than for homemade facemasks.</p><p>In conclusion, the barrier efficiency is more affected by fitting than the material of the facemask. These results show that the principle effect on the performance barrier of facemasks are breathability comfort (material pressure drop) and a design that provides the best fit for minimizing leakage. The impact of the filtration efficiency of the material is not a major factor for facemask qualifications.</p></sec><sec id="s3_3"><title>3.3. Leakage Related to Holes in the 3 Facemasks</title><p><xref ref-type="fig" rid="fig9">Figure 9</xref> presents the barrier efficiency according to the particle size measured using the material facemask holder (<xref ref-type="fig" rid="fig5">Figure 5</xref>) for the three different materials.</p><p><xref ref-type="fig" rid="fig9">Figure 9</xref>(a) shows the effect of the holes on the efficiency barrier of the white facemask material. Without holes, the material performs very well, and its</p><p>barrier efficiency is near 100%. With the presence of holes this efficiency continues to decrease as more holes are drilled. <xref ref-type="fig" rid="fig9">Figure 9</xref>(b) shows the effect of the holes on the efficiency barrier of the blue facemask material. Similar observations of the white facemask material were observed. <xref ref-type="fig" rid="fig9">Figure 9</xref>(c) shows the effect of the holes on the efficiency barrier of the green facemask of woven cotton material. The barrier efficiency increases with the size of the particles projected to reach a maximum plateau for particle sizes greater than 300 nm. The textile material offers a barrier efficiency greater than 80% and reaches the value of 100% without holes. These results agree with the studies of Chen and Willeke [<xref ref-type="bibr" rid="scirp.108761-ref21">21</xref>], Liu et al. [<xref ref-type="bibr" rid="scirp.108761-ref32">32</xref>] on FFRs and Mouret et al. [<xref ref-type="bibr" rid="scirp.108761-ref33">33</xref>] on filter media. These authors showed that above a specific hole size, the protection factor decreases very rapidly with increasing leakage size. In addition, Rengasamy and Eimer published two studies [<xref ref-type="bibr" rid="scirp.108761-ref34">34</xref>] [<xref ref-type="bibr" rid="scirp.108761-ref35">35</xref>] presenting the same conclusions for N95 FFRs. They also observed that FFRs with lower efficiency when sealed have higher protection factor that the other FFRs. Then the barrier efficiency is reduced in the presence of the holes or valves. These results confirm those obtained in the previous section that leaks have a major effect on the barrier effectiveness of the facemask. These results suggest that the facemask should be manufactured in such a way that leaks are minimized by emphasizing fit in the mask design and avoiding holes in its manufacture.</p></sec></sec><sec id="s4"><title>4. Conclusions</title><p>Since the transmission of SARS-CoV-2 by the aerosol route has been established and acknowledged by the WHO and many governments, the scientific community must work on the evaluation and qualification of facemasks. Unlike the masks conventionally used as respiratory protective devices and surgical masks, facemasks in use by the general population are still little studied, and do not currently have a standard stating their qualifications. Although it is possible to learn from the established standards for conventional masks, it is necessary to develop a new expertise and a methodology specific to these facemasks. This paper demonstrates the need for a different methodology for this type of facemask due to their specific use and design.</p><p>The results presented above have shown that a facemask, although less effective than an FFR or a surgical mask, can reduce the aerosol concentration downstream of the mask. The results also demonstrate that the effect of leaks on the face/mask interface drastically reduces the barrier efficiency of the facemasks studied here. In addition to the filtration efficiency and pressure drop, facial leakage plays a prominent role in the barrier performance of these masks in their ability to stop viral spread. The fit of the mask to the head must be optimal, and the design must limit the presence of side leakage, holes or valves. Each type of facemask has its own advantages, e.g. commercial facemasks are easier to wear for a long time because of breathability, but fabric facemasks have the advantage of being more environmentally friendly. Performance tests for facemask need to be deeply studied, defined more globally and classified according to their use (e.g. at work or for shopping).</p></sec><sec id="s5"><title>Acknowledgements</title><p>The authors would like to acknowledge the IRSST (Institut de recherch&#233; Robert Sauv&#233; en Sant&#233; et en s&#233;curit&#233; du Travail) for the financial support of this work.</p></sec><sec id="s6"><title>Conflicts of Interest</title><p>The authors declare no conflicts of interest regarding the publication of this paper.</p></sec><sec id="s7"><title>Cite this paper</title><p>Bahloul, A., Brochot, C. and Layne, B. (2021) Leakage versus Material Filtration in Barrier Facemask Efficiency. 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