Response of hot-wire anemometry to transient flow induced by weak pressure waves
When a pressure wave propagates in a stationary fluid, the fluid flow is accelerated from zero to a certain value. Although hot-wire anemometry is among the most reliable measurement techniques for small-amplitude and high-frequency fluctuations of velocity or mass flow rate (mass flux), few reports...
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description | When a pressure wave propagates in a stationary fluid, the fluid flow is accelerated from zero to a certain value. Although hot-wire anemometry is among the most reliable measurement techniques for small-amplitude and high-frequency fluctuations of velocity or mass flow rate (mass flux), few reports on their response to step accelerations from zero velocity exist. In this study, the response of hot-wire anemometry operated in constant temperature mode (HW-CTA) to an accelerated flow with an initial flow velocity,
U
, to
U
+
Δ
u
, where
Δ
u
is the increase in flow velocity due to a pressure wave, was investigated. In the experiments, the opening valves generated a pressure wave in a pipe with a radius of 50 mm. The velocity signals measured by HW-CTA and flush-mounted pressure transducer were compared for several values of
U
and
Δ
u
. A non-negligible dead time and increased time constant were found in the signal measured by HW-CTA when compared with those measured by the pressure transducer for
U
=
0
, whereas a negligible delay was observed for
Re
U
>
0.2
U
>
0.5
m
/
s
.
Re
U
is the wire Reynolds number based on
U
and the hot-wire diameter. Finally, it was revealed that the sum of the dead time and time constant corresponded to the flow transitions from natural to forced convection.
Graphical abstract |
doi_str_mv | 10.1007/s00348-024-03779-z |
format | Article |
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U
, to
U
+
Δ
u
, where
Δ
u
is the increase in flow velocity due to a pressure wave, was investigated. In the experiments, the opening valves generated a pressure wave in a pipe with a radius of 50 mm. The velocity signals measured by HW-CTA and flush-mounted pressure transducer were compared for several values of
U
and
Δ
u
. A non-negligible dead time and increased time constant were found in the signal measured by HW-CTA when compared with those measured by the pressure transducer for
U
=
0
, whereas a negligible delay was observed for
Re
U
>
0.2
U
>
0.5
m
/
s
.
Re
U
is the wire Reynolds number based on
U
and the hot-wire diameter. Finally, it was revealed that the sum of the dead time and time constant corresponded to the flow transitions from natural to forced convection.
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U
, to
U
+
Δ
u
, where
Δ
u
is the increase in flow velocity due to a pressure wave, was investigated. In the experiments, the opening valves generated a pressure wave in a pipe with a radius of 50 mm. The velocity signals measured by HW-CTA and flush-mounted pressure transducer were compared for several values of
U
and
Δ
u
. A non-negligible dead time and increased time constant were found in the signal measured by HW-CTA when compared with those measured by the pressure transducer for
U
=
0
, whereas a negligible delay was observed for
Re
U
>
0.2
U
>
0.5
m
/
s
.
Re
U
is the wire Reynolds number based on
U
and the hot-wire diameter. Finally, it was revealed that the sum of the dead time and time constant corresponded to the flow transitions from natural to forced convection.
Graphical abstract</description><subject>Diameters</subject><subject>Elastic waves</subject><subject>Engineering</subject><subject>Engineering Fluid Dynamics</subject><subject>Engineering Thermodynamics</subject><subject>Flow velocity</subject><subject>Fluid flow</subject><subject>Fluid- and Aerodynamics</subject><subject>Forced convection</subject><subject>Heat and Mass Transfer</subject><subject>Mass flow rate</subject><subject>Measurement techniques</subject><subject>Pressure transducers</subject><subject>Research Article</subject><subject>Reynolds number</subject><subject>Time constant</subject><subject>Transducers</subject><subject>Unsteady flow</subject><subject>Velocity measurement</subject><subject>Wire</subject><issn>0723-4864</issn><issn>1432-1114</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2024</creationdate><recordtype>article</recordtype><recordid>eNp9kEtLxDAUhYMoOI7-AVcB19GbR5t0KeILBhTRdUjbW-0409SkdZj59UYruHN1z-J858JHyCmHcw6gLyKAVIaBUAyk1gXb7ZEZV1IwzrnaJzPQQjJlcnVIjmJcAvCsADMjj08Ye99FpL6hb35gmzYgdR2u_RqHsKWDp0NwXWyxG2iz8hvadvVYYU3LLd2ge6d9wBjHRG3cJ8ZjctC4VcST3zsnLzfXz1d3bPFwe391uWCV0DAwmXFRF2XmVNFkdVlhIyVIRCdAlsro0jSZVKUA4-pCaVMVIgWd5w6zCjnIOTmbdvvgP0aMg136MXTppRVFlieQG5NaYmpVwccYsLF9aNcubC0H-23OTuZsMmd_zNldguQExVTuXjH8Tf9DfQEY_nJk</recordid><startdate>20240401</startdate><enddate>20240401</enddate><creator>Miyachi, Tokuzo</creator><creator>Arai, Takakage</creator><creator>Sakaue, Shoji</creator><creator>Takashima, Koji</creator><general>Springer Berlin Heidelberg</general><general>Springer Nature B.V</general><scope>AAYXX</scope><scope>CITATION</scope><orcidid>https://orcid.org/0000-0002-6971-3549</orcidid><orcidid>https://orcid.org/0000-0003-3592-2366</orcidid><orcidid>https://orcid.org/0000-0002-5465-3838</orcidid></search><sort><creationdate>20240401</creationdate><title>Response of hot-wire anemometry to transient flow induced by weak pressure waves</title><author>Miyachi, Tokuzo ; Arai, Takakage ; Sakaue, Shoji ; Takashima, Koji</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c270t-3512d9b5a49f5dbcef3303eea203b487b8f534b208ad9478c92ad9766ae5ce103</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2024</creationdate><topic>Diameters</topic><topic>Elastic waves</topic><topic>Engineering</topic><topic>Engineering Fluid Dynamics</topic><topic>Engineering Thermodynamics</topic><topic>Flow velocity</topic><topic>Fluid flow</topic><topic>Fluid- and Aerodynamics</topic><topic>Forced convection</topic><topic>Heat and Mass Transfer</topic><topic>Mass flow rate</topic><topic>Measurement techniques</topic><topic>Pressure transducers</topic><topic>Research Article</topic><topic>Reynolds number</topic><topic>Time constant</topic><topic>Transducers</topic><topic>Unsteady flow</topic><topic>Velocity measurement</topic><topic>Wire</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Miyachi, Tokuzo</creatorcontrib><creatorcontrib>Arai, Takakage</creatorcontrib><creatorcontrib>Sakaue, Shoji</creatorcontrib><creatorcontrib>Takashima, Koji</creatorcontrib><collection>CrossRef</collection><jtitle>Experiments in fluids</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Miyachi, Tokuzo</au><au>Arai, Takakage</au><au>Sakaue, Shoji</au><au>Takashima, Koji</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Response of hot-wire anemometry to transient flow induced by weak pressure waves</atitle><jtitle>Experiments in fluids</jtitle><stitle>Exp Fluids</stitle><date>2024-04-01</date><risdate>2024</risdate><volume>65</volume><issue>4</issue><artnum>44</artnum><issn>0723-4864</issn><eissn>1432-1114</eissn><abstract>When a pressure wave propagates in a stationary fluid, the fluid flow is accelerated from zero to a certain value. Although hot-wire anemometry is among the most reliable measurement techniques for small-amplitude and high-frequency fluctuations of velocity or mass flow rate (mass flux), few reports on their response to step accelerations from zero velocity exist. In this study, the response of hot-wire anemometry operated in constant temperature mode (HW-CTA) to an accelerated flow with an initial flow velocity,
U
, to
U
+
Δ
u
, where
Δ
u
is the increase in flow velocity due to a pressure wave, was investigated. In the experiments, the opening valves generated a pressure wave in a pipe with a radius of 50 mm. The velocity signals measured by HW-CTA and flush-mounted pressure transducer were compared for several values of
U
and
Δ
u
. A non-negligible dead time and increased time constant were found in the signal measured by HW-CTA when compared with those measured by the pressure transducer for
U
=
0
, whereas a negligible delay was observed for
Re
U
>
0.2
U
>
0.5
m
/
s
.
Re
U
is the wire Reynolds number based on
U
and the hot-wire diameter. Finally, it was revealed that the sum of the dead time and time constant corresponded to the flow transitions from natural to forced convection.
Graphical abstract</abstract><cop>Berlin/Heidelberg</cop><pub>Springer Berlin Heidelberg</pub><doi>10.1007/s00348-024-03779-z</doi><orcidid>https://orcid.org/0000-0002-6971-3549</orcidid><orcidid>https://orcid.org/0000-0003-3592-2366</orcidid><orcidid>https://orcid.org/0000-0002-5465-3838</orcidid></addata></record> |
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source | Springer Nature - Complete Springer Journals |
subjects | Diameters Elastic waves Engineering Engineering Fluid Dynamics Engineering Thermodynamics Flow velocity Fluid flow Fluid- and Aerodynamics Forced convection Heat and Mass Transfer Mass flow rate Measurement techniques Pressure transducers Research Article Reynolds number Time constant Transducers Unsteady flow Velocity measurement Wire |
title | Response of hot-wire anemometry to transient flow induced by weak pressure waves |
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