Gelation monitoring by quartz microbalance in pulse mode
Classical viscoelastic measurement setup with a quartz crystal microbalance uses a steady state input signal in order to measure the complex equivalent electrical parameters. Using a network analyzer, this method enables the measurement of the equivalent impedance around the first resonance peak of...
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creator | Caplain, E. Ehssein, C.O. Martinez, L. Serfaty, S. Griesmar, P. Gindre, M. |
description | Classical viscoelastic measurement setup with a quartz crystal microbalance uses a steady state input signal in order to measure the complex equivalent electrical parameters. Using a network analyzer, this method enables the measurement of the equivalent impedance around the first resonance peak of the quartz within a tiny frequency range (typically 10 kHz around a 6 MHz resonance frequency). However, due to the network analyzer acquisition time, such a setup cannot make two successive acquisitions in less than 15 s for one resonance peak. We excite the quartz by a short pulse and record its time impulse response. This kind of excitation allows us to record higher resonance peaks (up to the 11th order) and to reduce drastically the acquisition time, enabling up to 100 acquisitions per second. |
doi_str_mv | 10.1109/ULTSYM.2004.1417730 |
format | Conference Proceeding |
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Using a network analyzer, this method enables the measurement of the equivalent impedance around the first resonance peak of the quartz within a tiny frequency range (typically 10 kHz around a 6 MHz resonance frequency). However, due to the network analyzer acquisition time, such a setup cannot make two successive acquisitions in less than 15 s for one resonance peak. We excite the quartz by a short pulse and record its time impulse response. 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Using a network analyzer, this method enables the measurement of the equivalent impedance around the first resonance peak of the quartz within a tiny frequency range (typically 10 kHz around a 6 MHz resonance frequency). However, due to the network analyzer acquisition time, such a setup cannot make two successive acquisitions in less than 15 s for one resonance peak. We excite the quartz by a short pulse and record its time impulse response. This kind of excitation allows us to record higher resonance peaks (up to the 11th order) and to reduce drastically the acquisition time, enabling up to 100 acquisitions per second.</description><subject>Acoustics</subject><subject>Elasticity</subject><subject>Electric variables measurement</subject><subject>Electronics</subject><subject>Engineering Sciences</subject><subject>Frequency measurement</subject><subject>Impedance measurement</subject><subject>Monitoring</subject><subject>Resonance</subject><subject>Resonant frequency</subject><subject>Signal and Image processing</subject><subject>Steady-state</subject><subject>Time factors</subject><subject>Viscosity</subject><issn>1051-0117</issn><isbn>9780780384125</isbn><isbn>0780384121</isbn><fulltext>true</fulltext><rsrctype>conference_proceeding</rsrctype><creationdate>2004</creationdate><recordtype>conference_proceeding</recordtype><sourceid>6IE</sourceid><sourceid>RIE</sourceid><recordid>eNo9kE1Lw0AYhBdUsNb-gl5y9ZD4vvuRd_dYirZCxIPtwVPYbLZ2JR81TYX66xtpEQaGGR7mMIxNERJEMI_rbPX-8ZpwAJmgRCIBV2xiSMMgoSVydc1GCApjQKRbdrfffwFwUFyOmF74yvahbaK6bULfdqH5jIpj9H2wXf8b1cF1bWEr2zgfhSbaHaq9H9DS37ObjR3C5OJjtn5-Ws2Xcfa2eJnPsnjLwfRxIQiVo5TQSemc0d6QSnlpS6W1T73n3AiXlqi5VEZqLTepNNYQFIakLMSYPZx3t7bKd12obXfMWxvy5SzL_zpAAi0IfnBgp2c2eO__4csp4gRLf1QT</recordid><startdate>2004</startdate><enddate>2004</enddate><creator>Caplain, E.</creator><creator>Ehssein, C.O.</creator><creator>Martinez, L.</creator><creator>Serfaty, S.</creator><creator>Griesmar, P.</creator><creator>Gindre, M.</creator><general>IEEE</general><scope>6IE</scope><scope>6IH</scope><scope>CBEJK</scope><scope>RIE</scope><scope>RIO</scope><scope>1XC</scope><orcidid>https://orcid.org/0000-0002-8798-5361</orcidid><orcidid>https://orcid.org/0000-0002-3982-0853</orcidid><orcidid>https://orcid.org/0000-0003-4290-1336</orcidid><orcidid>https://orcid.org/0000-0002-0273-4986</orcidid></search><sort><creationdate>2004</creationdate><title>Gelation monitoring by quartz microbalance in pulse mode</title><author>Caplain, E. ; Ehssein, C.O. ; Martinez, L. ; Serfaty, S. ; Griesmar, P. ; Gindre, M.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-h209t-b3715c7671c44cc98e97562dad588e6ee2293c6d1824594884f649a970b9744b3</frbrgroupid><rsrctype>conference_proceedings</rsrctype><prefilter>conference_proceedings</prefilter><language>eng</language><creationdate>2004</creationdate><topic>Acoustics</topic><topic>Elasticity</topic><topic>Electric variables measurement</topic><topic>Electronics</topic><topic>Engineering Sciences</topic><topic>Frequency measurement</topic><topic>Impedance measurement</topic><topic>Monitoring</topic><topic>Resonance</topic><topic>Resonant frequency</topic><topic>Signal and Image processing</topic><topic>Steady-state</topic><topic>Time factors</topic><topic>Viscosity</topic><toplevel>online_resources</toplevel><creatorcontrib>Caplain, E.</creatorcontrib><creatorcontrib>Ehssein, C.O.</creatorcontrib><creatorcontrib>Martinez, L.</creatorcontrib><creatorcontrib>Serfaty, S.</creatorcontrib><creatorcontrib>Griesmar, P.</creatorcontrib><creatorcontrib>Gindre, M.</creatorcontrib><collection>IEEE Electronic Library (IEL) Conference Proceedings</collection><collection>IEEE Proceedings Order Plan (POP) 1998-present by volume</collection><collection>IEEE Xplore All Conference Proceedings</collection><collection>IEEE Electronic Library (IEL)</collection><collection>IEEE Proceedings Order Plans (POP) 1998-present</collection><collection>Hyper Article en Ligne (HAL)</collection></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext_linktorsrc</fulltext></delivery><addata><au>Caplain, E.</au><au>Ehssein, C.O.</au><au>Martinez, L.</au><au>Serfaty, S.</au><au>Griesmar, P.</au><au>Gindre, M.</au><format>book</format><genre>proceeding</genre><ristype>CONF</ristype><atitle>Gelation monitoring by quartz microbalance in pulse mode</atitle><btitle>IEEE Ultrasonics Symposium, 2004</btitle><stitle>ULTSYM</stitle><date>2004</date><risdate>2004</risdate><volume>1</volume><spage>323</spage><epage>324 Vol.1</epage><pages>323-324 Vol.1</pages><issn>1051-0117</issn><isbn>9780780384125</isbn><isbn>0780384121</isbn><abstract>Classical viscoelastic measurement setup with a quartz crystal microbalance uses a steady state input signal in order to measure the complex equivalent electrical parameters. Using a network analyzer, this method enables the measurement of the equivalent impedance around the first resonance peak of the quartz within a tiny frequency range (typically 10 kHz around a 6 MHz resonance frequency). However, due to the network analyzer acquisition time, such a setup cannot make two successive acquisitions in less than 15 s for one resonance peak. We excite the quartz by a short pulse and record its time impulse response. This kind of excitation allows us to record higher resonance peaks (up to the 11th order) and to reduce drastically the acquisition time, enabling up to 100 acquisitions per second.</abstract><pub>IEEE</pub><doi>10.1109/ULTSYM.2004.1417730</doi><orcidid>https://orcid.org/0000-0002-8798-5361</orcidid><orcidid>https://orcid.org/0000-0002-3982-0853</orcidid><orcidid>https://orcid.org/0000-0003-4290-1336</orcidid><orcidid>https://orcid.org/0000-0002-0273-4986</orcidid></addata></record> |
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source | IEEE Electronic Library (IEL) Conference Proceedings |
subjects | Acoustics Elasticity Electric variables measurement Electronics Engineering Sciences Frequency measurement Impedance measurement Monitoring Resonance Resonant frequency Signal and Image processing Steady-state Time factors Viscosity |
title | Gelation monitoring by quartz microbalance in pulse mode |
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