Three-dimensional wave packet in a Mach 6 boundary layer on a flared cone
High-resolution direct numerical simulations (DNS) were carried out to investigate the nonlinear breakdown process of a three-dimensional wave packet initiated by a short-duration pulse in a flared cone boundary layer at Mach 6 and zero angle of attack. For these simulations the cone geometry of the...
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description | High-resolution direct numerical simulations (DNS) were carried out to investigate the nonlinear breakdown process of a three-dimensional wave packet initiated by a short-duration pulse in a flared cone boundary layer at Mach 6 and zero angle of attack. For these simulations the cone geometry of the flared cone experiments conducted in the Boeing/AFOSR Mach 6 Quiet Tunnel (BAM6QT) at Purdue University was considered. The computational domain covered a large extent of the cone in the azimuthal direction to allow for a wide range of azimuthal wavenumbers (
$k_{c}$
) and to include shallow instability waves with small azimuthal wavenumbers. The simulation results indicated that the wave packet development was dominated by axisymmetric and shallow (small
$k_{c}$
) second-mode waves for a large downstream extent. Towards the downstream end of the computational domain a rapid broadening of the disturbance amplitude spectra was observed, which is an indication that the wave packet reached the strongly nonlinear stages. The disturbance spectra of the nonlinear regime, and the downstream amplitude development of the dominant disturbance wave components, provided conclusive evidence that the so-called fundamental breakdown was the dominant nonlinear mechanism. Furthermore, contours of the time-averaged Stanton number exhibited ‘hot’ streaks within the wave packet on the surface of the cone. Hot streaks have also been observed in the Purdue flared cone experiments using temperature sensitive paint (TSP) and in numerical investigations using DNS. The azimuthal streak spacing obtained from the wave packet simulation agrees well with that observed in the Purdue quiet tunnel experiments. |
doi_str_mv | 10.1017/jfm.2019.1011 |
format | Article |
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$k_{c}$
) and to include shallow instability waves with small azimuthal wavenumbers. The simulation results indicated that the wave packet development was dominated by axisymmetric and shallow (small
$k_{c}$
) second-mode waves for a large downstream extent. Towards the downstream end of the computational domain a rapid broadening of the disturbance amplitude spectra was observed, which is an indication that the wave packet reached the strongly nonlinear stages. The disturbance spectra of the nonlinear regime, and the downstream amplitude development of the dominant disturbance wave components, provided conclusive evidence that the so-called fundamental breakdown was the dominant nonlinear mechanism. Furthermore, contours of the time-averaged Stanton number exhibited ‘hot’ streaks within the wave packet on the surface of the cone. Hot streaks have also been observed in the Purdue flared cone experiments using temperature sensitive paint (TSP) and in numerical investigations using DNS. The azimuthal streak spacing obtained from the wave packet simulation agrees well with that observed in the Purdue quiet tunnel experiments.</description><identifier>ISSN: 0022-1120</identifier><identifier>EISSN: 1469-7645</identifier><identifier>DOI: 10.1017/jfm.2019.1011</identifier><language>eng</language><publisher>Cambridge: Cambridge University Press</publisher><subject>Aircraft industry ; Amplitude ; Amplitudes ; Angle of attack ; Boundary layers ; Breakdown ; Computer applications ; Computer simulation ; Domain names ; Duration ; Experiments ; Geometry ; Instability waves (fluids) ; Reynolds number ; Simulation ; Spectra ; Stanton number ; Symmetry ; Temperature-sensitive paints ; Tunnels ; Zero angle of attack</subject><ispartof>Journal of fluid mechanics, 2020-02, Vol.885, Article R3</ispartof><rights>Copyright Cambridge University Press Feb 2020</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c265t-38f9b6d6d3ca0fc14e574ce9bdd5b775d2f18a4989c6cd796a7c5998f9a67d073</citedby><cites>FETCH-LOGICAL-c265t-38f9b6d6d3ca0fc14e574ce9bdd5b775d2f18a4989c6cd796a7c5998f9a67d073</cites><orcidid>0000-0002-0956-000X</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,778,782,27911,27912</link.rule.ids></links><search><creatorcontrib>Hader, Christoph</creatorcontrib><creatorcontrib>Fasel, Hermann F.</creatorcontrib><title>Three-dimensional wave packet in a Mach 6 boundary layer on a flared cone</title><title>Journal of fluid mechanics</title><description>High-resolution direct numerical simulations (DNS) were carried out to investigate the nonlinear breakdown process of a three-dimensional wave packet initiated by a short-duration pulse in a flared cone boundary layer at Mach 6 and zero angle of attack. For these simulations the cone geometry of the flared cone experiments conducted in the Boeing/AFOSR Mach 6 Quiet Tunnel (BAM6QT) at Purdue University was considered. The computational domain covered a large extent of the cone in the azimuthal direction to allow for a wide range of azimuthal wavenumbers (
$k_{c}$
) and to include shallow instability waves with small azimuthal wavenumbers. The simulation results indicated that the wave packet development was dominated by axisymmetric and shallow (small
$k_{c}$
) second-mode waves for a large downstream extent. Towards the downstream end of the computational domain a rapid broadening of the disturbance amplitude spectra was observed, which is an indication that the wave packet reached the strongly nonlinear stages. The disturbance spectra of the nonlinear regime, and the downstream amplitude development of the dominant disturbance wave components, provided conclusive evidence that the so-called fundamental breakdown was the dominant nonlinear mechanism. Furthermore, contours of the time-averaged Stanton number exhibited ‘hot’ streaks within the wave packet on the surface of the cone. Hot streaks have also been observed in the Purdue flared cone experiments using temperature sensitive paint (TSP) and in numerical investigations using DNS. The azimuthal streak spacing obtained from the wave packet simulation agrees well with that observed in the Purdue quiet tunnel experiments.</description><subject>Aircraft industry</subject><subject>Amplitude</subject><subject>Amplitudes</subject><subject>Angle of attack</subject><subject>Boundary layers</subject><subject>Breakdown</subject><subject>Computer applications</subject><subject>Computer simulation</subject><subject>Domain names</subject><subject>Duration</subject><subject>Experiments</subject><subject>Geometry</subject><subject>Instability waves (fluids)</subject><subject>Reynolds number</subject><subject>Simulation</subject><subject>Spectra</subject><subject>Stanton number</subject><subject>Symmetry</subject><subject>Temperature-sensitive paints</subject><subject>Tunnels</subject><subject>Zero angle of attack</subject><issn>0022-1120</issn><issn>1469-7645</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2020</creationdate><recordtype>article</recordtype><sourceid>8G5</sourceid><sourceid>ABUWG</sourceid><sourceid>AFKRA</sourceid><sourceid>AZQEC</sourceid><sourceid>BENPR</sourceid><sourceid>CCPQU</sourceid><sourceid>DWQXO</sourceid><sourceid>GNUQQ</sourceid><sourceid>GUQSH</sourceid><sourceid>M2O</sourceid><recordid>eNotkM1KAzEUhYMoWKtL9wHXqfmZJJOlFH-puKnrkElu6NTppCat0rfxWXwyZ6hw4XC491wOH0LXjM4YZfp2HTczTpkZHTtBE1YpQ7Sq5CmaUMo5YYzTc3RRyppSJqjRE_SyXGUAEtoN9KVNvevwt_sCvHX-A3a47bHDr86vfn8UbtK-Dy4fcOcOkHEad7FzGQL2qYdLdBZdV-DqX6fo_eF-OX8ii7fH5_ndgniu5I6IOppGBRWEdzR6VoHUlQfThCAbrWXgkdWuMrXxygdtlNNeGjOknNKBajFFN8e_25w-91B2dp32eWheLBeC1pKLYaaIHK98TqVkiHab283Q3jJqR1x2wGVHXKNj4g9pIF1s</recordid><startdate>20200225</startdate><enddate>20200225</enddate><creator>Hader, Christoph</creator><creator>Fasel, Hermann F.</creator><general>Cambridge University Press</general><scope>AAYXX</scope><scope>CITATION</scope><scope>3V.</scope><scope>7TB</scope><scope>7U5</scope><scope>7UA</scope><scope>7XB</scope><scope>88I</scope><scope>8FD</scope><scope>8FE</scope><scope>8FG</scope><scope>8FK</scope><scope>8G5</scope><scope>ABJCF</scope><scope>ABUWG</scope><scope>AEUYN</scope><scope>AFKRA</scope><scope>ARAPS</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>BHPHI</scope><scope>BKSAR</scope><scope>C1K</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>F1W</scope><scope>FR3</scope><scope>GNUQQ</scope><scope>GUQSH</scope><scope>H8D</scope><scope>H96</scope><scope>HCIFZ</scope><scope>KR7</scope><scope>L.G</scope><scope>L6V</scope><scope>L7M</scope><scope>M2O</scope><scope>M2P</scope><scope>M7S</scope><scope>MBDVC</scope><scope>P5Z</scope><scope>P62</scope><scope>PCBAR</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PTHSS</scope><scope>Q9U</scope><scope>S0W</scope><orcidid>https://orcid.org/0000-0002-0956-000X</orcidid></search><sort><creationdate>20200225</creationdate><title>Three-dimensional wave packet in a Mach 6 boundary layer on a flared cone</title><author>Hader, Christoph ; Fasel, Hermann F.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c265t-38f9b6d6d3ca0fc14e574ce9bdd5b775d2f18a4989c6cd796a7c5998f9a67d073</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2020</creationdate><topic>Aircraft industry</topic><topic>Amplitude</topic><topic>Amplitudes</topic><topic>Angle of attack</topic><topic>Boundary layers</topic><topic>Breakdown</topic><topic>Computer applications</topic><topic>Computer simulation</topic><topic>Domain names</topic><topic>Duration</topic><topic>Experiments</topic><topic>Geometry</topic><topic>Instability waves (fluids)</topic><topic>Reynolds number</topic><topic>Simulation</topic><topic>Spectra</topic><topic>Stanton number</topic><topic>Symmetry</topic><topic>Temperature-sensitive paints</topic><topic>Tunnels</topic><topic>Zero angle of attack</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Hader, Christoph</creatorcontrib><creatorcontrib>Fasel, Hermann F.</creatorcontrib><collection>CrossRef</collection><collection>ProQuest Central (Corporate)</collection><collection>Mechanical & Transportation Engineering Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Water Resources Abstracts</collection><collection>ProQuest Central (purchase pre-March 2016)</collection><collection>Science Database (Alumni Edition)</collection><collection>Technology Research Database</collection><collection>ProQuest SciTech Collection</collection><collection>ProQuest Technology Collection</collection><collection>ProQuest Central (Alumni) (purchase pre-March 2016)</collection><collection>Research Library (Alumni Edition)</collection><collection>Materials Science & Engineering Collection</collection><collection>ProQuest Central (Alumni Edition)</collection><collection>ProQuest One Sustainability</collection><collection>ProQuest Central UK/Ireland</collection><collection>Advanced Technologies & Aerospace Collection</collection><collection>ProQuest Central Essentials</collection><collection>ProQuest Central</collection><collection>Technology Collection</collection><collection>Natural Science Collection</collection><collection>Earth, Atmospheric & Aquatic Science Collection</collection><collection>Environmental Sciences and Pollution Management</collection><collection>ProQuest One Community College</collection><collection>ProQuest Central Korea</collection><collection>ASFA: Aquatic Sciences and Fisheries Abstracts</collection><collection>Engineering Research Database</collection><collection>ProQuest Central Student</collection><collection>Research Library Prep</collection><collection>Aerospace Database</collection><collection>Aquatic Science & Fisheries Abstracts (ASFA) 2: Ocean Technology, Policy & Non-Living Resources</collection><collection>SciTech Premium Collection</collection><collection>Civil Engineering Abstracts</collection><collection>Aquatic Science & Fisheries Abstracts (ASFA) Professional</collection><collection>ProQuest Engineering Collection</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>Research Library</collection><collection>Science Database</collection><collection>Engineering Database</collection><collection>Research Library (Corporate)</collection><collection>Advanced Technologies & Aerospace Database</collection><collection>ProQuest Advanced Technologies & Aerospace Collection</collection><collection>Earth, Atmospheric & Aquatic Science Database</collection><collection>ProQuest One Academic Eastern Edition (DO NOT USE)</collection><collection>ProQuest One Academic</collection><collection>ProQuest One Academic UKI Edition</collection><collection>Engineering Collection</collection><collection>ProQuest Central Basic</collection><collection>DELNET Engineering & Technology Collection</collection><jtitle>Journal of fluid mechanics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Hader, Christoph</au><au>Fasel, Hermann F.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Three-dimensional wave packet in a Mach 6 boundary layer on a flared cone</atitle><jtitle>Journal of fluid mechanics</jtitle><date>2020-02-25</date><risdate>2020</risdate><volume>885</volume><artnum>R3</artnum><issn>0022-1120</issn><eissn>1469-7645</eissn><abstract>High-resolution direct numerical simulations (DNS) were carried out to investigate the nonlinear breakdown process of a three-dimensional wave packet initiated by a short-duration pulse in a flared cone boundary layer at Mach 6 and zero angle of attack. For these simulations the cone geometry of the flared cone experiments conducted in the Boeing/AFOSR Mach 6 Quiet Tunnel (BAM6QT) at Purdue University was considered. The computational domain covered a large extent of the cone in the azimuthal direction to allow for a wide range of azimuthal wavenumbers (
$k_{c}$
) and to include shallow instability waves with small azimuthal wavenumbers. The simulation results indicated that the wave packet development was dominated by axisymmetric and shallow (small
$k_{c}$
) second-mode waves for a large downstream extent. Towards the downstream end of the computational domain a rapid broadening of the disturbance amplitude spectra was observed, which is an indication that the wave packet reached the strongly nonlinear stages. The disturbance spectra of the nonlinear regime, and the downstream amplitude development of the dominant disturbance wave components, provided conclusive evidence that the so-called fundamental breakdown was the dominant nonlinear mechanism. Furthermore, contours of the time-averaged Stanton number exhibited ‘hot’ streaks within the wave packet on the surface of the cone. Hot streaks have also been observed in the Purdue flared cone experiments using temperature sensitive paint (TSP) and in numerical investigations using DNS. The azimuthal streak spacing obtained from the wave packet simulation agrees well with that observed in the Purdue quiet tunnel experiments.</abstract><cop>Cambridge</cop><pub>Cambridge University Press</pub><doi>10.1017/jfm.2019.1011</doi><orcidid>https://orcid.org/0000-0002-0956-000X</orcidid></addata></record> |
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subjects | Aircraft industry Amplitude Amplitudes Angle of attack Boundary layers Breakdown Computer applications Computer simulation Domain names Duration Experiments Geometry Instability waves (fluids) Reynolds number Simulation Spectra Stanton number Symmetry Temperature-sensitive paints Tunnels Zero angle of attack |
title | Three-dimensional wave packet in a Mach 6 boundary layer on a flared cone |
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