<?xml version="1.0" encoding="UTF-8"?><?xml-stylesheet type="text/xsl" href="static/style.xsl"?><OAI-PMH xmlns="http://www.openarchives.org/OAI/2.0/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/ http://www.openarchives.org/OAI/2.0/OAI-PMH.xsd"><responseDate>2026-06-02T21:42:41Z</responseDate><request verb="GetRecord" identifier="oai:riuma.uma.es:10630/40975" metadataPrefix="marc">https://riuma.uma.es/rest/oai/request</request><GetRecord><record><header><identifier>oai:riuma.uma.es:10630/40975</identifier><datestamp>2026-02-03T11:29:03Z</datestamp><setSpec>com_10630_2254</setSpec><setSpec>col_10630_37953</setSpec></header><metadata><record xmlns="http://www.loc.gov/MARC21/slim" xmlns:dcterms="http://purl.org/dc/terms/" xmlns:doc="http://www.lyncode.com/xoai" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.loc.gov/MARC21/slim http://www.loc.gov/standards/marcxml/schema/MARC21slim.xsd">
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      <subfield code="a">Fernández-Feria, Ramón</subfield>
      <subfield code="e">author</subfield>
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   <datafield ind2=" " ind1=" " tag="260">
      <subfield code="c">2016</subfield>
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      <subfield code="a">A vortical impulse theory is used to compute the thrust force of a plunging and&#xd;
pitching airfoil in forward flight at high Reynolds numbers within the framework of linear&#xd;
potential flow theory. The result is significantly different from the classical one of Garrick,&#xd;
which considered only two effects, the leading-edge suction and the projection in the&#xd;
flight direction of the pressure force on the airfoil. By taking into account the complete&#xd;
vorticity distribution on the airfoil and the wake the mean thrust coefficient contains, in&#xd;
addition to the pressure force projection term, a new term that generalizes the leading-edge&#xd;
suction term in Garrick’s theory. This term depends on Theodorsen function C(k) and&#xd;
on a new complex function C1(k) of the reduced frequency k. The main qualitative&#xd;
difference with Garrick’s theory is that the propulsive efficiency, or ratio of the mean&#xd;
thrust power and the mean input power required to drive the airfoil, tends to zero as&#xd;
the reduced frequency increases to infinity (as k−1), in contrast to Garrick’s propulsive&#xd;
efficiency that tends to a constant (1/2). Consequently, for pure pitching and combined&#xd;
pitching and plunging motions, the maximum of the propulsive efficiency is not reached&#xd;
as k → ∞ like in Garrick’s theory, but at a finite value of the reduced frequency that&#xd;
depends on the remaining nondimensional parameters. The present analytical results are&#xd;
in good agreement, for small amplitude oscillations, with numerical results from unsteady&#xd;
panel methods, and with experimental data and numerical results from the Navier-Stokes&#xd;
equations, except for small reduced frequencies where viscous effects are obviously&#xd;
important.</subfield>
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      <subfield code="a">Fernandez-Feria, R. (2016). Linearized propulsion theory of flapping airfoils revisited. Physical Review Fluids, 1(8). https://doi.org/10.1103/physrevfluids.1.084502</subfield>
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      <subfield code="a">https://hdl.handle.net/10630/40975</subfield>
   </datafield>
   <datafield ind1="8" ind2=" " tag="024">
      <subfield code="a">10.1103/PhysRevFluids.1.084502</subfield>
   </datafield>
   <datafield tag="653" ind2=" " ind1=" ">
      <subfield code="a">Aerodinámica</subfield>
   </datafield>
   <datafield tag="653" ind2=" " ind1=" ">
      <subfield code="a">Vuelo</subfield>
   </datafield>
   <datafield ind2="0" ind1="0" tag="245">
      <subfield code="a">Linearized propulsion theory of flapping airfoils revisited</subfield>
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