2014
DOI: 10.1002/we.1800
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Cylindrical vortex wake model: right cylinder

Abstract: The vortex system consisting of a bound vortex disk, a root vortex and a vortex cylinder as introduced by Joukowski in 1912 is further studied in this paper. This system can be used for simple modeling of rotors (e.g. wind turbines) with infinite number of blades and finite tip-speed ratios. For each vortex element, the velocity components in all directions and in the entire domain are computed analytically in a novel approach. In particular, the velocity field from the vortex actuator disk is derived for the … Show more

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Cited by 50 publications
(62 citation statements)
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References 16 publications
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“…The newly shed wake is generated at the edge of the disc and convected downstream by the local velocity. By applying the equation of velocity induced by a finite vortex cylinder derived in Branlard and Gaunaa, the axial velocity at a position ( z p , r p ) induced by the wake vorticity system can be calculated by the following integral: normalΦfalse(zp,rp,tfalse)=true0γtfalse(z,tfalse)4πrpRfalse(z,tfalse)[]false(zzpfalse)m()Kfalse(m2false)+Rfalse(z,tfalse)rpRfalse(z,tfalse)+rpnormalΠfalse(m02,m2false)zz+dz, where < z p , r p > are the coordinates of point P where the velocity is to be calculated, γ t ( z , t ) is the tangential vorticity of the surface at location z at time t . K ( m 2 ), and normalΠfalse(m02,m2false) are the complete elliptic integrals of the first and third kind.…”
Section: Methodsmentioning
confidence: 99%
“…The newly shed wake is generated at the edge of the disc and convected downstream by the local velocity. By applying the equation of velocity induced by a finite vortex cylinder derived in Branlard and Gaunaa, the axial velocity at a position ( z p , r p ) induced by the wake vorticity system can be calculated by the following integral: normalΦfalse(zp,rp,tfalse)=true0γtfalse(z,tfalse)4πrpRfalse(z,tfalse)[]false(zzpfalse)m()Kfalse(m2false)+Rfalse(z,tfalse)rpRfalse(z,tfalse)+rpnormalΠfalse(m02,m2false)zz+dz, where < z p , r p > are the coordinates of point P where the velocity is to be calculated, γ t ( z , t ) is the tangential vorticity of the surface at location z at time t . K ( m 2 ), and normalΠfalse(m02,m2false) are the complete elliptic integrals of the first and third kind.…”
Section: Methodsmentioning
confidence: 99%
“…Some examples are Okulov and Sørensen and Branlard et al . . The effect of the number of blades is studied by Okulov and Sørensen using vortex theory, and by van Kuik describing the limit transitions from rotor to disc.…”
Section: Introductionmentioning
confidence: 99%
“…Some examples are Okulov and Sørensen 7,8 and Branlard et al. 9,10 The effect of the number of blades is studied by Okulov and Sørensen 8 using vortex theory, and by van Kuik 11 describing the limit transitions from rotor to disc. Textbooks like Schaffarczyk 12 and reviews like Wald 13 and Sørensen 14 present an overview of rotor aerodynamics and the role of the actuator disc herein.…”
Section: Introductionmentioning
confidence: 99%
“…The vortex cylinder model applied to the actuator disk concept yields a simple expression characterising the induction (Branlard and Gaunaa, 2015;Medici et al, 2011) that can be integrated into a WFR model. This simple induction model is one-dimensional.…”
Section: Combined Wind-induction Modelmentioning
confidence: 99%