Nonlinear liquid sloshing in square tanks subjected to horizontal random excitation
hing dynamics in a square tank are numerically investigated when the tank is subjected to horizontal, narrowband random ground excitation. The natural frequencies of the two predominant sloshing modes are identical and therefore 1:1 internal resonance may occur. Galerkin’s method is applied to deriv...
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Veröffentlicht in: | Nonlinear dynamics 2013-04, Vol.72 (1-2), p.439-453 |
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description | hing dynamics in a square tank are numerically investigated when the tank is subjected to horizontal, narrowband random ground excitation. The natural frequencies of the two predominant sloshing modes are identical and therefore 1:1 internal resonance may occur. Galerkin’s method is applied to derive the modal equations of motion for nonlinear sloshing including higher modes. The Monte Carlo simulation is used to calculate response statistics such as mean square values and probability density functions (PDFs). The two predominant modes exhibit complex phenomena including “autoparametric interaction” because they are nonlinearly coupled with each other. The mean square responses of these two modes and the liquid elevation are found to differ significantly from those of the corresponding linear model, depending on the characteristics of the random ground excitation such as bandwidth, center frequency and excitation direction. It is found that the direction of the excitation is a significant factor in predicting the mean square responses. The frequency response curves for the same system subjected to equivalent harmonic excitation are also calculated and compared with the mean square responses to further explain the phenomena. Changing the liquid level causes the peak of the mean square response to shift. Furthermore, the risk of the liquid overspill from the tank is discussed by showing the three-dimensional distribution charts of the mean square responses of liquid elevations. |
doi_str_mv | 10.1007/s11071-012-0726-2 |
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The natural frequencies of the two predominant sloshing modes are identical and therefore 1:1 internal resonance may occur. Galerkin’s method is applied to derive the modal equations of motion for nonlinear sloshing including higher modes. The Monte Carlo simulation is used to calculate response statistics such as mean square values and probability density functions (PDFs). The two predominant modes exhibit complex phenomena including “autoparametric interaction” because they are nonlinearly coupled with each other. The mean square responses of these two modes and the liquid elevation are found to differ significantly from those of the corresponding linear model, depending on the characteristics of the random ground excitation such as bandwidth, center frequency and excitation direction. It is found that the direction of the excitation is a significant factor in predicting the mean square responses. The frequency response curves for the same system subjected to equivalent harmonic excitation are also calculated and compared with the mean square responses to further explain the phenomena. Changing the liquid level causes the peak of the mean square response to shift. Furthermore, the risk of the liquid overspill from the tank is discussed by showing the three-dimensional distribution charts of the mean square responses of liquid elevations.</description><identifier>ISSN: 0924-090X</identifier><identifier>EISSN: 1573-269X</identifier><identifier>DOI: 10.1007/s11071-012-0726-2</identifier><language>eng</language><publisher>Dordrecht: Springer Netherlands</publisher><subject>Automotive Engineering ; Classical Mechanics ; Computer simulation ; Control ; Dynamical Systems ; Engineering ; Equations of motion ; Excitation ; Frequency response ; Galerkin method ; Harmonic excitation ; Horizontal ; Liquid sloshing ; Liquids ; Mathematical models ; Mean square values ; Mechanical Engineering ; Monte Carlo simulation ; Narrowband ; Nonlinear dynamics ; Nonlinear equations ; Original Paper ; Probability density functions ; Random excitation ; Resonant frequencies ; Tanks ; Vibration</subject><ispartof>Nonlinear dynamics, 2013-04, Vol.72 (1-2), p.439-453</ispartof><rights>Springer Science+Business Media Dordrecht 2013</rights><rights>Nonlinear Dynamics is a copyright of Springer, (2013). All Rights Reserved.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c448t-fed04cc2fe31390503e69a084a8e293dfb257dc0b6f000e6d0da427ebe55b9193</citedby><cites>FETCH-LOGICAL-c448t-fed04cc2fe31390503e69a084a8e293dfb257dc0b6f000e6d0da427ebe55b9193</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://link.springer.com/content/pdf/10.1007/s11071-012-0726-2$$EPDF$$P50$$Gspringer$$H</linktopdf><linktohtml>$$Uhttps://link.springer.com/10.1007/s11071-012-0726-2$$EHTML$$P50$$Gspringer$$H</linktohtml><link.rule.ids>314,780,784,27924,27925,41488,42557,51319</link.rule.ids></links><search><creatorcontrib>Ikeda, Takashi</creatorcontrib><creatorcontrib>Harata, Yuji</creatorcontrib><creatorcontrib>Ibrahim, Raouf A.</creatorcontrib><title>Nonlinear liquid sloshing in square tanks subjected to horizontal random excitation</title><title>Nonlinear dynamics</title><addtitle>Nonlinear Dyn</addtitle><description>hing dynamics in a square tank are numerically investigated when the tank is subjected to horizontal, narrowband random ground excitation. The natural frequencies of the two predominant sloshing modes are identical and therefore 1:1 internal resonance may occur. Galerkin’s method is applied to derive the modal equations of motion for nonlinear sloshing including higher modes. The Monte Carlo simulation is used to calculate response statistics such as mean square values and probability density functions (PDFs). The two predominant modes exhibit complex phenomena including “autoparametric interaction” because they are nonlinearly coupled with each other. The mean square responses of these two modes and the liquid elevation are found to differ significantly from those of the corresponding linear model, depending on the characteristics of the random ground excitation such as bandwidth, center frequency and excitation direction. It is found that the direction of the excitation is a significant factor in predicting the mean square responses. The frequency response curves for the same system subjected to equivalent harmonic excitation are also calculated and compared with the mean square responses to further explain the phenomena. Changing the liquid level causes the peak of the mean square response to shift. Furthermore, the risk of the liquid overspill from the tank is discussed by showing the three-dimensional distribution charts of the mean square responses of liquid elevations.</description><subject>Automotive Engineering</subject><subject>Classical Mechanics</subject><subject>Computer simulation</subject><subject>Control</subject><subject>Dynamical Systems</subject><subject>Engineering</subject><subject>Equations of motion</subject><subject>Excitation</subject><subject>Frequency response</subject><subject>Galerkin method</subject><subject>Harmonic excitation</subject><subject>Horizontal</subject><subject>Liquid sloshing</subject><subject>Liquids</subject><subject>Mathematical models</subject><subject>Mean square values</subject><subject>Mechanical Engineering</subject><subject>Monte Carlo simulation</subject><subject>Narrowband</subject><subject>Nonlinear dynamics</subject><subject>Nonlinear equations</subject><subject>Original Paper</subject><subject>Probability density functions</subject><subject>Random excitation</subject><subject>Resonant frequencies</subject><subject>Tanks</subject><subject>Vibration</subject><issn>0924-090X</issn><issn>1573-269X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2013</creationdate><recordtype>article</recordtype><sourceid>AFKRA</sourceid><sourceid>BENPR</sourceid><sourceid>CCPQU</sourceid><sourceid>DWQXO</sourceid><recordid>eNp1kM9LwzAYhoMoOKd_gLeAFy_VL2naNEcZ_oKhBxV2C2n7dcvski1pQf3r7aggCJ7ey_O-vDyEnDO4YgDyOjIGkiXAeAKS5wk_IBOWyTThuVockgkoLhJQsDgmJzGuASDlUEzIy5N3rXVoAm3trrc1ja2PK-uW1Doad70JSDvj3iONfbnGqsOadp6ufLBf3nWmpcG42m8oflS2M5317pQcNaaNePaTU_J2d_s6e0jmz_ePs5t5UglRdEmDNYiq4g2mLFWQQYq5MlAIUyBXad2UPJN1BWXeDHcxr6E2gkssMctKxVQ6JZfj7jb4XY-x0xsbK2xb49D3UTORKilFzrIBvfiDrn0f3PBOc54pwbks2ECxkaqCjzFgo7fBbkz41Az0XrMeNetBs95r1nzo8LETB9YtMfwu_1_6Bv7KgIg</recordid><startdate>20130401</startdate><enddate>20130401</enddate><creator>Ikeda, Takashi</creator><creator>Harata, Yuji</creator><creator>Ibrahim, Raouf A.</creator><general>Springer Netherlands</general><general>Springer Nature B.V</general><scope>AAYXX</scope><scope>CITATION</scope><scope>8FE</scope><scope>8FG</scope><scope>ABJCF</scope><scope>AFKRA</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>HCIFZ</scope><scope>L6V</scope><scope>M7S</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope><scope>PTHSS</scope><scope>7SC</scope><scope>7TB</scope><scope>8FD</scope><scope>FR3</scope><scope>JQ2</scope><scope>KR7</scope><scope>L7M</scope><scope>L~C</scope><scope>L~D</scope></search><sort><creationdate>20130401</creationdate><title>Nonlinear liquid sloshing in square tanks subjected to horizontal random excitation</title><author>Ikeda, Takashi ; Harata, Yuji ; Ibrahim, Raouf A.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c448t-fed04cc2fe31390503e69a084a8e293dfb257dc0b6f000e6d0da427ebe55b9193</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2013</creationdate><topic>Automotive Engineering</topic><topic>Classical Mechanics</topic><topic>Computer simulation</topic><topic>Control</topic><topic>Dynamical Systems</topic><topic>Engineering</topic><topic>Equations of motion</topic><topic>Excitation</topic><topic>Frequency response</topic><topic>Galerkin method</topic><topic>Harmonic excitation</topic><topic>Horizontal</topic><topic>Liquid sloshing</topic><topic>Liquids</topic><topic>Mathematical models</topic><topic>Mean square values</topic><topic>Mechanical Engineering</topic><topic>Monte Carlo simulation</topic><topic>Narrowband</topic><topic>Nonlinear dynamics</topic><topic>Nonlinear equations</topic><topic>Original Paper</topic><topic>Probability density functions</topic><topic>Random excitation</topic><topic>Resonant frequencies</topic><topic>Tanks</topic><topic>Vibration</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Ikeda, Takashi</creatorcontrib><creatorcontrib>Harata, Yuji</creatorcontrib><creatorcontrib>Ibrahim, Raouf A.</creatorcontrib><collection>CrossRef</collection><collection>ProQuest SciTech Collection</collection><collection>ProQuest Technology Collection</collection><collection>Materials Science & Engineering Collection</collection><collection>ProQuest Central UK/Ireland</collection><collection>ProQuest Central</collection><collection>Technology Collection</collection><collection>ProQuest One Community College</collection><collection>ProQuest Central Korea</collection><collection>SciTech Premium Collection</collection><collection>ProQuest Engineering Collection</collection><collection>Engineering 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>ProQuest Central China</collection><collection>Engineering Collection</collection><collection>Computer and Information Systems Abstracts</collection><collection>Mechanical & Transportation Engineering Abstracts</collection><collection>Technology Research Database</collection><collection>Engineering Research Database</collection><collection>ProQuest Computer Science Collection</collection><collection>Civil Engineering Abstracts</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>Computer and Information Systems Abstracts Academic</collection><collection>Computer and Information Systems Abstracts Professional</collection><jtitle>Nonlinear dynamics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Ikeda, Takashi</au><au>Harata, Yuji</au><au>Ibrahim, Raouf A.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Nonlinear liquid sloshing in square tanks subjected to horizontal random excitation</atitle><jtitle>Nonlinear dynamics</jtitle><stitle>Nonlinear Dyn</stitle><date>2013-04-01</date><risdate>2013</risdate><volume>72</volume><issue>1-2</issue><spage>439</spage><epage>453</epage><pages>439-453</pages><issn>0924-090X</issn><eissn>1573-269X</eissn><abstract>hing dynamics in a square tank are numerically investigated when the tank is subjected to horizontal, narrowband random ground excitation. The natural frequencies of the two predominant sloshing modes are identical and therefore 1:1 internal resonance may occur. Galerkin’s method is applied to derive the modal equations of motion for nonlinear sloshing including higher modes. The Monte Carlo simulation is used to calculate response statistics such as mean square values and probability density functions (PDFs). The two predominant modes exhibit complex phenomena including “autoparametric interaction” because they are nonlinearly coupled with each other. The mean square responses of these two modes and the liquid elevation are found to differ significantly from those of the corresponding linear model, depending on the characteristics of the random ground excitation such as bandwidth, center frequency and excitation direction. It is found that the direction of the excitation is a significant factor in predicting the mean square responses. The frequency response curves for the same system subjected to equivalent harmonic excitation are also calculated and compared with the mean square responses to further explain the phenomena. Changing the liquid level causes the peak of the mean square response to shift. Furthermore, the risk of the liquid overspill from the tank is discussed by showing the three-dimensional distribution charts of the mean square responses of liquid elevations.</abstract><cop>Dordrecht</cop><pub>Springer Netherlands</pub><doi>10.1007/s11071-012-0726-2</doi><tpages>15</tpages></addata></record> |
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subjects | Automotive Engineering Classical Mechanics Computer simulation Control Dynamical Systems Engineering Equations of motion Excitation Frequency response Galerkin method Harmonic excitation Horizontal Liquid sloshing Liquids Mathematical models Mean square values Mechanical Engineering Monte Carlo simulation Narrowband Nonlinear dynamics Nonlinear equations Original Paper Probability density functions Random excitation Resonant frequencies Tanks Vibration |
title | Nonlinear liquid sloshing in square tanks subjected to horizontal random excitation |
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