Experimental and finite element analysis of the generation mechanism of high impulse noise overpressure (caused by a recoilless weapon) at the bottom of the ear

•The finite element model of the impulsive noise-human-head model was established using the plane shock wave method. The simulation result were in good agreement with the experimental results.•The impulse noise formed a stagnation zone at the ear's bottom in the human head model. The overpressu...

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Veröffentlicht in:Computer methods and programs in biomedicine 2023-12, Vol.242, p.107786-107786, Article 107786
Hauptverfasser: Li, Zhiyu, Tao, Gang, Wen, Peng, Ren, Baoxiang
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Tao, Gang
Wen, Peng
Ren, Baoxiang
description •The finite element model of the impulsive noise-human-head model was established using the plane shock wave method. The simulation result were in good agreement with the experimental results.•The impulse noise formed a stagnation zone at the ear's bottom in the human head model. The overpressure at the ear's bottom was the total pressure of the impulse noise flowing into the ear canal. It was higher than the free field overpressure and related to the angle of incidence, λ. As λ increased, the overpressure at the entrance to the ear canal and the mach number decreased, causing the total pressure to decrease.•It found that the human head model caused a secondary entry of impulse noise into the ear canal. When λ was 0° and 30°, there were two overpressure peaks at the bottom of the ear. When λ was 60° and 90°, the two parts of the impulse noise were superimposed at the bottom of the ear, resulting in only one overpressure peak at the bottom of the ear. The intense impulse noise may damage the soldiers’ hearing organs during a weapon's firing. It is essential to find out the generation mechanism of the overpressure at the bottom of the ear. The experiments of measuring the overpressure at the bottom of the ear were conducted through a rotating human head model at a recoilless weapon firing platform. The results showed that the overpressure peak at the bottom of the ear decreases with the increasing incident angle. A simulation of the test condition was developed based on the plane shock wave method. The finite element model was verified reasonably compared to the test results. The Friedlander wave propagating to the ear canal was implemented at different incident angles. The generation of the overpressure at the bottom of the ear was analyzed. According to the pressure nephograms, the impulse noise stagnated at the bottom of the ear, so the overpressure was the total pressure of impulse noise. Two parts of impulse noise entered the canal successively due to the influence of the pinna. The overpressure and Mach number at the entrance of the ear canal both decreased with increasing incident angles, resulting in impulse noise superimposed at the bottom of the ear. Investigating the generation of overpressure at the bottom of the ear under varying incident angles may have important reference value for analyzing and preventing auditory organ damage caused by impulse noise.
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The simulation result were in good agreement with the experimental results.•The impulse noise formed a stagnation zone at the ear's bottom in the human head model. The overpressure at the ear's bottom was the total pressure of the impulse noise flowing into the ear canal. It was higher than the free field overpressure and related to the angle of incidence, λ. As λ increased, the overpressure at the entrance to the ear canal and the mach number decreased, causing the total pressure to decrease.•It found that the human head model caused a secondary entry of impulse noise into the ear canal. When λ was 0° and 30°, there were two overpressure peaks at the bottom of the ear. When λ was 60° and 90°, the two parts of the impulse noise were superimposed at the bottom of the ear, resulting in only one overpressure peak at the bottom of the ear. The intense impulse noise may damage the soldiers’ hearing organs during a weapon's firing. It is essential to find out the generation mechanism of the overpressure at the bottom of the ear. The experiments of measuring the overpressure at the bottom of the ear were conducted through a rotating human head model at a recoilless weapon firing platform. The results showed that the overpressure peak at the bottom of the ear decreases with the increasing incident angle. A simulation of the test condition was developed based on the plane shock wave method. The finite element model was verified reasonably compared to the test results. The Friedlander wave propagating to the ear canal was implemented at different incident angles. The generation of the overpressure at the bottom of the ear was analyzed. According to the pressure nephograms, the impulse noise stagnated at the bottom of the ear, so the overpressure was the total pressure of impulse noise. Two parts of impulse noise entered the canal successively due to the influence of the pinna. The overpressure and Mach number at the entrance of the ear canal both decreased with increasing incident angles, resulting in impulse noise superimposed at the bottom of the ear. Investigating the generation of overpressure at the bottom of the ear under varying incident angles may have important reference value for analyzing and preventing auditory organ damage caused by impulse noise.</description><identifier>ISSN: 0169-2607</identifier><identifier>EISSN: 1872-7565</identifier><identifier>DOI: 10.1016/j.cmpb.2023.107786</identifier><language>eng</language><publisher>Elsevier B.V</publisher><subject>Impulse noise ; The incident angle ; The overpressure at the bottom of the ear ; The plane shock wave method</subject><ispartof>Computer methods and programs in biomedicine, 2023-12, Vol.242, p.107786-107786, Article 107786</ispartof><rights>2023</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><cites>FETCH-LOGICAL-c284t-56f60964a1d1debe2cb81a27e9f9cf1c3a74ab4233c79fe2c04ed379bc042d163</cites><orcidid>0000-0002-2286-3945</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://www.sciencedirect.com/science/article/pii/S0169260723004522$$EHTML$$P50$$Gelsevier$$H</linktohtml><link.rule.ids>314,776,780,3537,27903,27904,65309</link.rule.ids></links><search><creatorcontrib>Li, Zhiyu</creatorcontrib><creatorcontrib>Tao, Gang</creatorcontrib><creatorcontrib>Wen, Peng</creatorcontrib><creatorcontrib>Ren, Baoxiang</creatorcontrib><title>Experimental and finite element analysis of the generation mechanism of high impulse noise overpressure (caused by a recoilless weapon) at the bottom of the ear</title><title>Computer methods and programs in biomedicine</title><description>•The finite element model of the impulsive noise-human-head model was established using the plane shock wave method. The simulation result were in good agreement with the experimental results.•The impulse noise formed a stagnation zone at the ear's bottom in the human head model. The overpressure at the ear's bottom was the total pressure of the impulse noise flowing into the ear canal. It was higher than the free field overpressure and related to the angle of incidence, λ. As λ increased, the overpressure at the entrance to the ear canal and the mach number decreased, causing the total pressure to decrease.•It found that the human head model caused a secondary entry of impulse noise into the ear canal. When λ was 0° and 30°, there were two overpressure peaks at the bottom of the ear. When λ was 60° and 90°, the two parts of the impulse noise were superimposed at the bottom of the ear, resulting in only one overpressure peak at the bottom of the ear. The intense impulse noise may damage the soldiers’ hearing organs during a weapon's firing. It is essential to find out the generation mechanism of the overpressure at the bottom of the ear. The experiments of measuring the overpressure at the bottom of the ear were conducted through a rotating human head model at a recoilless weapon firing platform. The results showed that the overpressure peak at the bottom of the ear decreases with the increasing incident angle. A simulation of the test condition was developed based on the plane shock wave method. The finite element model was verified reasonably compared to the test results. The Friedlander wave propagating to the ear canal was implemented at different incident angles. The generation of the overpressure at the bottom of the ear was analyzed. According to the pressure nephograms, the impulse noise stagnated at the bottom of the ear, so the overpressure was the total pressure of impulse noise. Two parts of impulse noise entered the canal successively due to the influence of the pinna. The overpressure and Mach number at the entrance of the ear canal both decreased with increasing incident angles, resulting in impulse noise superimposed at the bottom of the ear. 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The simulation result were in good agreement with the experimental results.•The impulse noise formed a stagnation zone at the ear's bottom in the human head model. The overpressure at the ear's bottom was the total pressure of the impulse noise flowing into the ear canal. It was higher than the free field overpressure and related to the angle of incidence, λ. As λ increased, the overpressure at the entrance to the ear canal and the mach number decreased, causing the total pressure to decrease.•It found that the human head model caused a secondary entry of impulse noise into the ear canal. When λ was 0° and 30°, there were two overpressure peaks at the bottom of the ear. When λ was 60° and 90°, the two parts of the impulse noise were superimposed at the bottom of the ear, resulting in only one overpressure peak at the bottom of the ear. The intense impulse noise may damage the soldiers’ hearing organs during a weapon's firing. It is essential to find out the generation mechanism of the overpressure at the bottom of the ear. The experiments of measuring the overpressure at the bottom of the ear were conducted through a rotating human head model at a recoilless weapon firing platform. The results showed that the overpressure peak at the bottom of the ear decreases with the increasing incident angle. A simulation of the test condition was developed based on the plane shock wave method. The finite element model was verified reasonably compared to the test results. The Friedlander wave propagating to the ear canal was implemented at different incident angles. The generation of the overpressure at the bottom of the ear was analyzed. According to the pressure nephograms, the impulse noise stagnated at the bottom of the ear, so the overpressure was the total pressure of impulse noise. Two parts of impulse noise entered the canal successively due to the influence of the pinna. The overpressure and Mach number at the entrance of the ear canal both decreased with increasing incident angles, resulting in impulse noise superimposed at the bottom of the ear. Investigating the generation of overpressure at the bottom of the ear under varying incident angles may have important reference value for analyzing and preventing auditory organ damage caused by impulse noise.</abstract><pub>Elsevier B.V</pub><doi>10.1016/j.cmpb.2023.107786</doi><tpages>1</tpages><orcidid>https://orcid.org/0000-0002-2286-3945</orcidid></addata></record>
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subjects Impulse noise
The incident angle
The overpressure at the bottom of the ear
The plane shock wave method
title Experimental and finite element analysis of the generation mechanism of high impulse noise overpressure (caused by a recoilless weapon) at the bottom of the ear
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