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A dealiasing method for use with ultrasonic pulsed Doppler in measuring velocity profiles and flow rates in pipes
The ultrasonic pulsed Doppler method (UDM) is a powerful tool for measuring velocity profiles in a pipe. However, the maximum detectable velocity is limited by the Nyquist sampling theorem. Furthermore, the maximum detectable velocity (also called Nyquist velocity), vmax, and the maximum measurable...
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Published in: | Measurement science & technology 2015-08, Vol.26 (8), p.85301-11 |
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description | The ultrasonic pulsed Doppler method (UDM) is a powerful tool for measuring velocity profiles in a pipe. However, the maximum detectable velocity is limited by the Nyquist sampling theorem. Furthermore, the maximum detectable velocity (also called Nyquist velocity), vmax, and the maximum measurable length are related and cannot be increased at the same time. If the velocity is greater than vmax, velocity aliasing occurs. Hence, the higher velocity that occurs with a larger pipe diameter, i.e. under higher flow rate conditions, cannot be measured with the conventional UDM. To overcome these limitations, dual-pulse repetition frequency (dual PRF) and feedback methods were employed in this study to measure velocity profiles in a pipe. The velocity distributions obtained with the feedback method were found to be more accurate than those obtained with the dual PRF method. However, misdetection of the Nyquist folding number using the feedback method was found to increase with the flow velocity. A feedback method with a moving average is proposed to improve the measurement accuracy. The method can accurately measure the velocity distributions at a velocity five times greater than the maximum velocity that can be measured with the conventional UDM. The measurement volume was found to be among the important parameters that must be considered in assessing the traceability of the reflector during the pulse emission interval. Hence, a larger measurement volume is required to measure higher velocities using the dual PRF method. Integrating velocity distributions measured using the feedback method with a moving average makes it possible to accurately determine flow rates six times greater than those that can be determined using the conventional pulsed Doppler method. |
doi_str_mv | 10.1088/0957-0233/26/8/085301 |
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However, the maximum detectable velocity is limited by the Nyquist sampling theorem. Furthermore, the maximum detectable velocity (also called Nyquist velocity), vmax, and the maximum measurable length are related and cannot be increased at the same time. If the velocity is greater than vmax, velocity aliasing occurs. Hence, the higher velocity that occurs with a larger pipe diameter, i.e. under higher flow rate conditions, cannot be measured with the conventional UDM. To overcome these limitations, dual-pulse repetition frequency (dual PRF) and feedback methods were employed in this study to measure velocity profiles in a pipe. The velocity distributions obtained with the feedback method were found to be more accurate than those obtained with the dual PRF method. However, misdetection of the Nyquist folding number using the feedback method was found to increase with the flow velocity. A feedback method with a moving average is proposed to improve the measurement accuracy. The method can accurately measure the velocity distributions at a velocity five times greater than the maximum velocity that can be measured with the conventional UDM. The measurement volume was found to be among the important parameters that must be considered in assessing the traceability of the reflector during the pulse emission interval. Hence, a larger measurement volume is required to measure higher velocities using the dual PRF method. Integrating velocity distributions measured using the feedback method with a moving average makes it possible to accurately determine flow rates six times greater than those that can be determined using the conventional pulsed Doppler method.</description><identifier>ISSN: 0957-0233</identifier><identifier>EISSN: 1361-6501</identifier><identifier>DOI: 10.1088/0957-0233/26/8/085301</identifier><identifier>CODEN: MSTCEP</identifier><language>eng</language><publisher>IOP Publishing</publisher><subject>dealiasing ; Doppler ; Doppler effect ; dual PRF ; Emission analysis ; Feedback ; feedback method ; Flow rate ; flow rate measurement ; Nyquist velocity ; Pipe ; Reflectors ; staggered PRF ; Velocity distribution</subject><ispartof>Measurement science & technology, 2015-08, Vol.26 (8), p.85301-11</ispartof><rights>2015 IOP Publishing Ltd</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c360t-5a3c7e5c9fe177b30c3cc8f13ef8e06f2bd3bfd54230d193adb5703001dc04cb3</citedby><cites>FETCH-LOGICAL-c360t-5a3c7e5c9fe177b30c3cc8f13ef8e06f2bd3bfd54230d193adb5703001dc04cb3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27924,27925</link.rule.ids></links><search><creatorcontrib>Murakawa, Hideki</creatorcontrib><creatorcontrib>Muramatsu, Ei</creatorcontrib><creatorcontrib>Sugimoto, Katsumi</creatorcontrib><creatorcontrib>Takenaka, Nobuyuki</creatorcontrib><creatorcontrib>Furuichi, Noriyuki</creatorcontrib><title>A dealiasing method for use with ultrasonic pulsed Doppler in measuring velocity profiles and flow rates in pipes</title><title>Measurement science & technology</title><addtitle>MST</addtitle><addtitle>Meas. Sci. Technol</addtitle><description>The ultrasonic pulsed Doppler method (UDM) is a powerful tool for measuring velocity profiles in a pipe. However, the maximum detectable velocity is limited by the Nyquist sampling theorem. Furthermore, the maximum detectable velocity (also called Nyquist velocity), vmax, and the maximum measurable length are related and cannot be increased at the same time. If the velocity is greater than vmax, velocity aliasing occurs. Hence, the higher velocity that occurs with a larger pipe diameter, i.e. under higher flow rate conditions, cannot be measured with the conventional UDM. To overcome these limitations, dual-pulse repetition frequency (dual PRF) and feedback methods were employed in this study to measure velocity profiles in a pipe. The velocity distributions obtained with the feedback method were found to be more accurate than those obtained with the dual PRF method. However, misdetection of the Nyquist folding number using the feedback method was found to increase with the flow velocity. A feedback method with a moving average is proposed to improve the measurement accuracy. The method can accurately measure the velocity distributions at a velocity five times greater than the maximum velocity that can be measured with the conventional UDM. The measurement volume was found to be among the important parameters that must be considered in assessing the traceability of the reflector during the pulse emission interval. Hence, a larger measurement volume is required to measure higher velocities using the dual PRF method. Integrating velocity distributions measured using the feedback method with a moving average makes it possible to accurately determine flow rates six times greater than those that can be determined using the conventional pulsed Doppler method.</description><subject>dealiasing</subject><subject>Doppler</subject><subject>Doppler effect</subject><subject>dual PRF</subject><subject>Emission analysis</subject><subject>Feedback</subject><subject>feedback method</subject><subject>Flow rate</subject><subject>flow rate measurement</subject><subject>Nyquist velocity</subject><subject>Pipe</subject><subject>Reflectors</subject><subject>staggered PRF</subject><subject>Velocity distribution</subject><issn>0957-0233</issn><issn>1361-6501</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2015</creationdate><recordtype>article</recordtype><recordid>eNp9kEtLAzEUhYMoWB8_QchON2NvJs08lsU3CG50HTJ52JR0kiYzlv57UyviQlxdDnzn3HsPQhcErgk0zRRaVhdQUjotq2mWDaNADtCE0IoUFQNyiCY_zDE6SWkJADW07QSt51hp4axItn_HKz0svMLGRzwmjTd2WODRDVEk31uJw-iSVvjWh-B0xLbPBpHGuLN-aOelHbY4RG-s0wmLPic5v8FRDFlmOtig0xk6MiLnnH_PU_R2f_d681g8vzw83cyfC0krGAomqKw1k63RpK47CpJK2RhCtWk0VKbsFO2MYrOSgiItFapjNVAAoiTMZEdP0dU-Nx-0HnUa-MomqZ0TvfZj4qSuSmiqsmQZZXtURp9S1IaHaFcibjkBvquY7-rju_p4WfEsvyrOvsu9z_rAl36MfX6Ir_KqXxQPymSS_EH-n_4JKOmM1Q</recordid><startdate>20150801</startdate><enddate>20150801</enddate><creator>Murakawa, Hideki</creator><creator>Muramatsu, Ei</creator><creator>Sugimoto, Katsumi</creator><creator>Takenaka, Nobuyuki</creator><creator>Furuichi, Noriyuki</creator><general>IOP Publishing</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7U5</scope><scope>8FD</scope><scope>F28</scope><scope>FR3</scope><scope>L7M</scope></search><sort><creationdate>20150801</creationdate><title>A dealiasing method for use with ultrasonic pulsed Doppler in measuring velocity profiles and flow rates in pipes</title><author>Murakawa, Hideki ; Muramatsu, Ei ; Sugimoto, Katsumi ; Takenaka, Nobuyuki ; Furuichi, Noriyuki</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c360t-5a3c7e5c9fe177b30c3cc8f13ef8e06f2bd3bfd54230d193adb5703001dc04cb3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2015</creationdate><topic>dealiasing</topic><topic>Doppler</topic><topic>Doppler effect</topic><topic>dual PRF</topic><topic>Emission analysis</topic><topic>Feedback</topic><topic>feedback method</topic><topic>Flow rate</topic><topic>flow rate measurement</topic><topic>Nyquist velocity</topic><topic>Pipe</topic><topic>Reflectors</topic><topic>staggered PRF</topic><topic>Velocity distribution</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Murakawa, Hideki</creatorcontrib><creatorcontrib>Muramatsu, Ei</creatorcontrib><creatorcontrib>Sugimoto, Katsumi</creatorcontrib><creatorcontrib>Takenaka, Nobuyuki</creatorcontrib><creatorcontrib>Furuichi, Noriyuki</creatorcontrib><collection>CrossRef</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>ANTE: Abstracts in New Technology & Engineering</collection><collection>Engineering Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Measurement science & technology</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Murakawa, Hideki</au><au>Muramatsu, Ei</au><au>Sugimoto, Katsumi</au><au>Takenaka, Nobuyuki</au><au>Furuichi, Noriyuki</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>A dealiasing method for use with ultrasonic pulsed Doppler in measuring velocity profiles and flow rates in pipes</atitle><jtitle>Measurement science & technology</jtitle><stitle>MST</stitle><addtitle>Meas. Sci. Technol</addtitle><date>2015-08-01</date><risdate>2015</risdate><volume>26</volume><issue>8</issue><spage>85301</spage><epage>11</epage><pages>85301-11</pages><issn>0957-0233</issn><eissn>1361-6501</eissn><coden>MSTCEP</coden><abstract>The ultrasonic pulsed Doppler method (UDM) is a powerful tool for measuring velocity profiles in a pipe. However, the maximum detectable velocity is limited by the Nyquist sampling theorem. Furthermore, the maximum detectable velocity (also called Nyquist velocity), vmax, and the maximum measurable length are related and cannot be increased at the same time. If the velocity is greater than vmax, velocity aliasing occurs. Hence, the higher velocity that occurs with a larger pipe diameter, i.e. under higher flow rate conditions, cannot be measured with the conventional UDM. To overcome these limitations, dual-pulse repetition frequency (dual PRF) and feedback methods were employed in this study to measure velocity profiles in a pipe. The velocity distributions obtained with the feedback method were found to be more accurate than those obtained with the dual PRF method. However, misdetection of the Nyquist folding number using the feedback method was found to increase with the flow velocity. A feedback method with a moving average is proposed to improve the measurement accuracy. The method can accurately measure the velocity distributions at a velocity five times greater than the maximum velocity that can be measured with the conventional UDM. The measurement volume was found to be among the important parameters that must be considered in assessing the traceability of the reflector during the pulse emission interval. Hence, a larger measurement volume is required to measure higher velocities using the dual PRF method. Integrating velocity distributions measured using the feedback method with a moving average makes it possible to accurately determine flow rates six times greater than those that can be determined using the conventional pulsed Doppler method.</abstract><pub>IOP Publishing</pub><doi>10.1088/0957-0233/26/8/085301</doi><tpages>11</tpages></addata></record> |
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source | Institute of Physics:Jisc Collections:IOP Publishing Read and Publish 2024-2025 (Reading List) |
subjects | dealiasing Doppler Doppler effect dual PRF Emission analysis Feedback feedback method Flow rate flow rate measurement Nyquist velocity Pipe Reflectors staggered PRF Velocity distribution |
title | A dealiasing method for use with ultrasonic pulsed Doppler in measuring velocity profiles and flow rates in pipes |
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