Sondhauss and Rijke oscillations—thermodynamic analysis, possible applications and analogies
Identifieur interne : 000E56 ( Main/Corpus ); précédent : 000E55; suivant : 000E57Sondhauss and Rijke oscillations—thermodynamic analysis, possible applications and analogies
Auteurs : G. Bisio ; G. RubattoSource :
- Energy [ 0360-5442 ] ; 1998.
Abstract
The phenomena of acoustical pressure oscillations generated in a gas by a steady heat source may be separated into two distinct types: (i) Sondhauss oscillations which occur in a pipe having one end closed and one open; (ii) Rijke oscillations which occur in a pipe with both ends open. After reviewing representative literature, actual and possible applications are described. Analogies and differences among these and similar systems are considered from a thermodynamic point of view.
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DOI: 10.1016/S0360-5442(98)00090-5
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<record><TEI wicri:istexFullTextTei="biblStruct"><teiHeader><fileDesc><titleStmt><title>Sondhauss and Rijke oscillations—thermodynamic analysis, possible applications and analogies</title><author><name sortKey="Bisio, G" sort="Bisio, G" uniqKey="Bisio G" first="G" last="Bisio">G. Bisio</name><affiliation><mods:affiliation>Energy and Conditioning Department, University of Genoa, Via all'Opera Pia 15 A, 16145 Genoa, Italy</mods:affiliation></affiliation></author><author><name sortKey="Rubatto, G" sort="Rubatto, G" uniqKey="Rubatto G" first="G" last="Rubatto">G. Rubatto</name><affiliation><mods:affiliation>Energy and Conditioning Department, University of Genoa, Via all'Opera Pia 15 A, 16145 Genoa, Italy</mods:affiliation></affiliation></author></titleStmt><publicationStmt><idno type="wicri:source">ISTEX</idno><idno type="RBID">ISTEX:095EE539E8E912243B50C7F64FA0D360E5B3B33F</idno><date when="1999" year="1999">1999</date><idno type="doi">10.1016/S0360-5442(98)00090-5</idno><idno type="url">https://api.istex.fr/document/095EE539E8E912243B50C7F64FA0D360E5B3B33F/fulltext/pdf</idno><idno type="wicri:Area/Main/Corpus">000E56</idno></publicationStmt><sourceDesc><biblStruct><analytic><title level="a">Sondhauss and Rijke oscillations—thermodynamic analysis, possible applications and analogies</title><author><name sortKey="Bisio, G" sort="Bisio, G" uniqKey="Bisio G" first="G" last="Bisio">G. Bisio</name><affiliation><mods:affiliation>Energy and Conditioning Department, University of Genoa, Via all'Opera Pia 15 A, 16145 Genoa, Italy</mods:affiliation></affiliation></author><author><name sortKey="Rubatto, G" sort="Rubatto, G" uniqKey="Rubatto G" first="G" last="Rubatto">G. Rubatto</name><affiliation><mods:affiliation>Energy and Conditioning Department, University of Genoa, Via all'Opera Pia 15 A, 16145 Genoa, Italy</mods:affiliation></affiliation></author></analytic><monogr></monogr><series><title level="j">Energy</title><title level="j" type="abbrev">EGY</title><idno type="ISSN">0360-5442</idno><imprint><publisher>ELSEVIER</publisher><date type="published" when="1998">1998</date><biblScope unit="volume">24</biblScope><biblScope unit="issue">2</biblScope><biblScope unit="page" from="117">117</biblScope><biblScope unit="page" to="131">131</biblScope></imprint><idno type="ISSN">0360-5442</idno></series><idno type="istex">095EE539E8E912243B50C7F64FA0D360E5B3B33F</idno><idno type="DOI">10.1016/S0360-5442(98)00090-5</idno><idno type="PII">S0360-5442(98)00090-5</idno></biblStruct></sourceDesc><seriesStmt><idno type="ISSN">0360-5442</idno></seriesStmt></fileDesc><profileDesc><textClass></textClass><langUsage><language ident="en">en</language></langUsage></profileDesc></teiHeader><front><div type="abstract" xml:lang="en">The phenomena of acoustical pressure oscillations generated in a gas by a steady heat source may be separated into two distinct types: (i) Sondhauss oscillations which occur in a pipe having one end closed and one open; (ii) Rijke oscillations which occur in a pipe with both ends open. After reviewing representative literature, actual and possible applications are described. Analogies and differences among these and similar systems are considered from a thermodynamic point of view.</div></front></TEI><istex><corpusName>elsevier</corpusName><author><json:item><name>G Bisio</name><affiliations><json:string>Energy and Conditioning Department, University of Genoa, Via all'Opera Pia 15 A, 16145 Genoa, Italy</json:string></affiliations></json:item><json:item><name>G Rubatto</name><affiliations><json:string>Energy and Conditioning Department, University of Genoa, Via all'Opera Pia 15 A, 16145 Genoa, Italy</json:string></affiliations></json:item></author><language><json:string>eng</json:string></language><abstract>The phenomena of acoustical pressure oscillations generated in a gas by a steady heat source may be separated into two distinct types: (i) Sondhauss oscillations which occur in a pipe having one end closed and one open; (ii) Rijke oscillations which occur in a pipe with both ends open. After reviewing representative literature, actual and possible applications are described. Analogies and differences among these and similar systems are considered from a thermodynamic point of view.</abstract><qualityIndicators><score>5.9</score><pdfVersion>1.2</pdfVersion><pdfPageSize>547 x 746 pts</pdfPageSize><refBibsNative>true</refBibsNative><keywordCount>0</keywordCount><abstractCharCount>486</abstractCharCount><pdfWordCount>5786</pdfWordCount><pdfCharCount>33992</pdfCharCount><pdfPageCount>15</pdfPageCount><abstractWordCount>75</abstractWordCount></qualityIndicators><title>Sondhauss and Rijke oscillations—thermodynamic analysis, possible applications and analogies</title><pii><json:string>S0360-5442(98)00090-5</json:string></pii><genre><json:string>research-article</json:string></genre><host><volume>24</volume><pii><json:string>S0360-5442(00)X0047-3</json:string></pii><pages><last>131</last><first>117</first></pages><issn><json:string>0360-5442</json:string></issn><issue>2</issue><genre></genre><language><json:string>unknown</json:string></language><title>Energy</title><publicationDate>1999</publicationDate></host><categories><wos><json:string>ENERGY & FUELS</json:string><json:string>ENGINEERING, CHEMICAL</json:string><json:string>THERMODYNAMICS</json:string></wos></categories><publicationDate>1998</publicationDate><copyrightDate>1999</copyrightDate><doi><json:string>10.1016/S0360-5442(98)00090-5</json:string></doi><id>095EE539E8E912243B50C7F64FA0D360E5B3B33F</id><fulltext><json:item><original>true</original><mimetype>application/pdf</mimetype><extension>pdf</extension><uri>https://api.istex.fr/document/095EE539E8E912243B50C7F64FA0D360E5B3B33F/fulltext/pdf</uri></json:item><json:item><original>false</original><mimetype>application/zip</mimetype><extension>zip</extension><uri>https://api.istex.fr/document/095EE539E8E912243B50C7F64FA0D360E5B3B33F/fulltext/zip</uri></json:item><istex:fulltextTEI uri="https://api.istex.fr/document/095EE539E8E912243B50C7F64FA0D360E5B3B33F/fulltext/tei"><teiHeader><fileDesc><titleStmt><title level="a">Sondhauss and Rijke oscillations—thermodynamic analysis, possible applications and analogies</title></titleStmt><publicationStmt><authority>ISTEX</authority><publisher>ELSEVIER</publisher><availability><p>ELSEVIER</p></availability><date>1999</date></publicationStmt><notesStmt><note type="content">Fig. 1: A simple bulb-end Sondhauss pipe with external flame heating (Sondhauss, 1850; Rayleigh, 1878). A=heat addition; B=sound output.</note><note type="content">Fig. 2: A Rijke tube with open-ends (Rijke 1850). A=heater grid; B=convection flow; C=sound generated.</note><note type="content">Fig. 3: The Sondhauss pipe studied by Knipp. A=open end, which can be closed by a plug; B=closed end; C=junction end of the internal pipe; D=intermediate opening, which can be closed by a plug.</note><note type="content">Fig. 4: The bulb-end Sondhauss pipe with concentric tube insert studied by Carter in 1962. A=concentric tube; B=heat addition; C=sound emission.</note><note type="content">Fig. 5: A generalized Rijke oscillator. A=heater grid; B=convection flow; C=sound generated.</note><note type="content">Fig. 6: Schema of a Rijke tube with a feedback system A=heat source; B=microphone; C=phase-shifter; D=amplifier; E=loudspeaker.</note><note type="content">Fig. 7: Numerical results of overall pressure gain (from inlet plenum to exit plenum) vs operating frequency for a combustor with a resonant frequency of 180 Hz.</note><note type="content">Fig. 8: Neutral stability curve of a Bénard cell in the Ra (Rayleigh number) vs a (dimensionless wave number) plane. A=convection region; B=conduction region.</note><note type="content">Fig. 9: Neutral stability curve of a Sondhauss pipe with smooth but rapidly changing temperature profile in the central zone in the α (extreme temperature ratio) vs ω (wave number) plane. A=region with oscillations; B=region without oscillations.</note><note type="content">Fig. 10: Neutral stability curve of a Rijke pipe with experimental points (small rings ○) in the q (thermal power) vs GV (volumetric flow rate) plane. A=region with oscillations; B=region without oscillations.</note><note type="content">Table 1: Analogies and differences among some systems</note></notesStmt><sourceDesc><biblStruct type="inbook"><analytic><title level="a">Sondhauss and Rijke oscillations—thermodynamic analysis, possible applications and analogies</title><author><persName><forename type="first">G</forename><surname>Bisio</surname></persName><affiliation>Energy and Conditioning Department, University of Genoa, Via all'Opera Pia 15 A, 16145 Genoa, Italy</affiliation></author><author><persName><forename type="first">G</forename><surname>Rubatto</surname></persName><affiliation>Energy and Conditioning Department, University of Genoa, Via all'Opera Pia 15 A, 16145 Genoa, Italy</affiliation></author></analytic><monogr><title level="j">Energy</title><title level="j" type="abbrev">EGY</title><idno type="pISSN">0360-5442</idno><idno type="PII">S0360-5442(00)X0047-3</idno><imprint><publisher>ELSEVIER</publisher><date type="published" when="1998"></date><biblScope unit="volume">24</biblScope><biblScope unit="issue">2</biblScope><biblScope unit="page" from="117">117</biblScope><biblScope unit="page" to="131">131</biblScope></imprint></monogr><idno type="istex">095EE539E8E912243B50C7F64FA0D360E5B3B33F</idno><idno type="DOI">10.1016/S0360-5442(98)00090-5</idno><idno type="PII">S0360-5442(98)00090-5</idno></biblStruct></sourceDesc></fileDesc><profileDesc><creation><date>1999</date></creation><langUsage><language ident="en">en</language></langUsage><abstract xml:lang="en"><p>The phenomena of acoustical pressure oscillations generated in a gas by a steady heat source may be separated into two distinct types: (i) Sondhauss oscillations which occur in a pipe having one end closed and one open; (ii) Rijke oscillations which occur in a pipe with both ends open. After reviewing representative literature, actual and possible applications are described. Analogies and differences among these and similar systems are considered from a thermodynamic point of view.</p></abstract></profileDesc><revisionDesc><change when="1998-04-13">Received</change><change when="1998">Published</change></revisionDesc></teiHeader></istex:fulltextTEI><json:item><original>false</original><mimetype>text/plain</mimetype><extension>txt</extension><uri>https://api.istex.fr/document/095EE539E8E912243B50C7F64FA0D360E5B3B33F/fulltext/txt</uri></json:item></fulltext><metadata><istex:metadataXml wicri:clean="Elsevier, elements deleted: ce:floats; body; tail"><istex:xmlDeclaration>version="1.0" encoding="utf-8"</istex:xmlDeclaration><istex:docType PUBLIC="-//ES//DTD journal article DTD version 4.5.2//EN//XML" URI="art452.dtd" name="istex:docType"><istex:entity SYSTEM="gr1" NDATA="IMAGE" name="gr1"></istex:entity><istex:entity SYSTEM="gr2" NDATA="IMAGE" name="gr2"></istex:entity><istex:entity SYSTEM="gr3" NDATA="IMAGE" name="gr3"></istex:entity><istex:entity SYSTEM="gr4" NDATA="IMAGE" name="gr4"></istex:entity><istex:entity SYSTEM="gr5" NDATA="IMAGE" name="gr5"></istex:entity><istex:entity SYSTEM="gr6" NDATA="IMAGE" name="gr6"></istex:entity><istex:entity SYSTEM="gr7" NDATA="IMAGE" name="gr7"></istex:entity><istex:entity SYSTEM="gr8" NDATA="IMAGE" name="gr8"></istex:entity><istex:entity SYSTEM="gr9" NDATA="IMAGE" name="gr9"></istex:entity><istex:entity SYSTEM="gr10" NDATA="IMAGE" name="gr10"></istex:entity></istex:docType><istex:document><converted-article version="4.5.2" docsubtype="fla"><item-info><jid>EGY</jid><aid>666</aid><ce:pii>S0360-5442(98)00090-5</ce:pii><ce:doi>10.1016/S0360-5442(98)00090-5</ce:doi><ce:copyright year="1999" type="full-transfer">Elsevier Science Ltd</ce:copyright></item-info><head><ce:title>Sondhauss and Rijke oscillations—thermodynamic analysis, possible applications and analogies</ce:title><ce:author-group><ce:author><ce:given-name>G</ce:given-name><ce:surname>Bisio</ce:surname><ce:cross-ref refid="CORR1">*</ce:cross-ref></ce:author><ce:author><ce:given-name>G</ce:given-name><ce:surname>Rubatto</ce:surname></ce:author><ce:affiliation><ce:textfn>Energy and Conditioning Department, University of Genoa, Via all'Opera Pia 15 A, 16145 Genoa, Italy</ce:textfn></ce:affiliation><ce:correspondence id="CORR1"><ce:label>*</ce:label><ce:text>Corresponding author. Tel.: +39-10-353-2861; Fax: +39-10-311-870; E-mail: bisio@ditec.unige.it</ce:text></ce:correspondence></ce:author-group><ce:date-received day="13" month="4" year="1998"></ce:date-received><ce:abstract><ce:section-title>Abstract</ce:section-title><ce:abstract-sec><ce:simple-para>The phenomena of acoustical pressure oscillations generated in a gas by a steady heat source may be separated into two distinct types: (i) Sondhauss oscillations which occur in a pipe having one end closed and one open; (ii) Rijke oscillations which occur in a pipe with both ends open. After reviewing representative literature, actual and possible applications are described. Analogies and differences among these and similar systems are considered from a thermodynamic point of view.</ce:simple-para></ce:abstract-sec></ce:abstract></head></converted-article></istex:document></istex:metadataXml><mods version="3.6"><titleInfo><title>Sondhauss and Rijke oscillations—thermodynamic analysis, possible applications and analogies</title></titleInfo><titleInfo type="alternative" contentType="CDATA"><title>Sondhauss and Rijke oscillations—thermodynamic analysis, possible applications and analogies</title></titleInfo><name type="personal"><namePart type="given">G</namePart><namePart type="family">Bisio</namePart><affiliation>Energy and Conditioning Department, University of Genoa, Via all'Opera Pia 15 A, 16145 Genoa, Italy</affiliation><description>Corresponding author. Tel.: +39-10-353-2861; Fax: +39-10-311-870; E-mail: bisio@ditec.unige.it</description><role><roleTerm type="text">author</roleTerm></role></name><name type="personal"><namePart type="given">G</namePart><namePart type="family">Rubatto</namePart><affiliation>Energy and Conditioning Department, University of Genoa, Via all'Opera Pia 15 A, 16145 Genoa, Italy</affiliation><role><roleTerm type="text">author</roleTerm></role></name><typeOfResource>text</typeOfResource><genre type="research-article" displayLabel="Full-length article"></genre><originInfo><publisher>ELSEVIER</publisher><dateIssued encoding="w3cdtf">1998</dateIssued><dateCaptured encoding="w3cdtf">1998-04-13</dateCaptured><copyrightDate encoding="w3cdtf">1999</copyrightDate></originInfo><language><languageTerm type="code" authority="iso639-2b">eng</languageTerm><languageTerm type="code" authority="rfc3066">en</languageTerm></language><physicalDescription><internetMediaType>text/html</internetMediaType></physicalDescription><abstract lang="en">The phenomena of acoustical pressure oscillations generated in a gas by a steady heat source may be separated into two distinct types: (i) Sondhauss oscillations which occur in a pipe having one end closed and one open; (ii) Rijke oscillations which occur in a pipe with both ends open. After reviewing representative literature, actual and possible applications are described. Analogies and differences among these and similar systems are considered from a thermodynamic point of view.</abstract><note type="content">Fig. 1: A simple bulb-end Sondhauss pipe with external flame heating (Sondhauss, 1850; Rayleigh, 1878). A=heat addition; B=sound output.</note><note type="content">Fig. 2: A Rijke tube with open-ends (Rijke 1850). A=heater grid; B=convection flow; C=sound generated.</note><note type="content">Fig. 3: The Sondhauss pipe studied by Knipp. A=open end, which can be closed by a plug; B=closed end; C=junction end of the internal pipe; D=intermediate opening, which can be closed by a plug.</note><note type="content">Fig. 4: The bulb-end Sondhauss pipe with concentric tube insert studied by Carter in 1962. A=concentric tube; B=heat addition; C=sound emission.</note><note type="content">Fig. 5: A generalized Rijke oscillator. A=heater grid; B=convection flow; C=sound generated.</note><note type="content">Fig. 6: Schema of a Rijke tube with a feedback system A=heat source; B=microphone; C=phase-shifter; D=amplifier; E=loudspeaker.</note><note type="content">Fig. 7: Numerical results of overall pressure gain (from inlet plenum to exit plenum) vs operating frequency for a combustor with a resonant frequency of 180 Hz.</note><note type="content">Fig. 8: Neutral stability curve of a Bénard cell in the Ra (Rayleigh number) vs a (dimensionless wave number) plane. A=convection region; B=conduction region.</note><note type="content">Fig. 9: Neutral stability curve of a Sondhauss pipe with smooth but rapidly changing temperature profile in the central zone in the α (extreme temperature ratio) vs ω (wave number) plane. A=region with oscillations; B=region without oscillations.</note><note type="content">Fig. 10: Neutral stability curve of a Rijke pipe with experimental points (small rings ○) in the q (thermal power) vs GV (volumetric flow rate) plane. A=region with oscillations; B=region without oscillations.</note><note type="content">Table 1: Analogies and differences among some systems</note><relatedItem type="host"><titleInfo><title>Energy</title></titleInfo><titleInfo type="abbreviated"><title>EGY</title></titleInfo><genre type="Journal">journal</genre><originInfo><dateIssued encoding="w3cdtf">199902</dateIssued></originInfo><identifier type="ISSN">0360-5442</identifier><identifier type="PII">S0360-5442(00)X0047-3</identifier><part><date>199902</date><detail type="volume"><number>24</number><caption>vol.</caption></detail><detail type="issue"><number>2</number><caption>no.</caption></detail><extent unit="issue pages"><start>85</start><end>182</end></extent><extent unit="pages"><start>117</start><end>131</end></extent></part></relatedItem><identifier type="istex">095EE539E8E912243B50C7F64FA0D360E5B3B33F</identifier><identifier type="DOI">10.1016/S0360-5442(98)00090-5</identifier><identifier type="PII">S0360-5442(98)00090-5</identifier><accessCondition type="use and reproduction" contentType="">© 1999Elsevier Science Ltd</accessCondition><recordInfo><recordContentSource>ELSEVIER</recordContentSource><recordOrigin>Elsevier Science Ltd, ©1999</recordOrigin></recordInfo></mods></metadata><enrichments><istex:catWosTEI uri="https://api.istex.fr/document/095EE539E8E912243B50C7F64FA0D360E5B3B33F/enrichments/catWos"><teiHeader><profileDesc><textClass><classCode scheme="WOS">ENERGY & FUELS</classCode><classCode scheme="WOS">ENGINEERING, CHEMICAL</classCode><classCode scheme="WOS">THERMODYNAMICS</classCode></textClass></profileDesc></teiHeader></istex:catWosTEI></enrichments><serie></serie></istex></record>Pour manipuler ce document sous Unix (Dilib)
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