2014
DOI: 10.2514/1.c032719
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Far-Field Induced Drag Prediction Using Vorticity Confinement Technique

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Cited by 12 publications
(6 citation statements)
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“…However, separating out induced drag from profile drag, based on the type of measurements used here may not be feasible for flapping wings. Induced power is for fixed wings normally estimated from the in-plane velocity components in the Trefftz plane [49], but for flapping wings the magnitudes of these velocity components are influenced by the profile drag of the wings. Until a suitable method for separating profile and induced components is developed we can only speculate on how much the complexity of the wake influences the estimation of induced power from wakes in freely flying animals.…”
Section: Powermentioning
confidence: 99%
“…However, separating out induced drag from profile drag, based on the type of measurements used here may not be feasible for flapping wings. Induced power is for fixed wings normally estimated from the in-plane velocity components in the Trefftz plane [49], but for flapping wings the magnitudes of these velocity components are influenced by the profile drag of the wings. Until a suitable method for separating profile and induced components is developed we can only speculate on how much the complexity of the wake influences the estimation of induced power from wakes in freely flying animals.…”
Section: Powermentioning
confidence: 99%
“…The result not only confirms that, as a generic rule, the drag components expressed by wake integrals must depend on the choice of wake-plane streamwise location but also enables observing specific dynamic processes of flow structures responsible for the streamwise evolution of these force components. The innovative kinematic formula (18) for the x-derivative of induced drag, dD i /dx, reveals that it is exactly determined by a Wv-integral of the disturbance Lamb vector v × ω, while the kinetic formula (21) for dDi/dx = −dDP/dx reveals that assuming x-independence of Di implies neglecting the dissipation over the wake-plane. In the linear and viscous far wake, Di vanishes and DP becomes the total drag D. The numerical examples indicate that the concept of induced and profile drags as fixed numbers can at most be approximately true for attached flows, and these drags must strongly depend on x for more complex separated flows.…”
Section: Conclusion and Discussionmentioning
confidence: 99%
“…ex ⋅ (vπ × ωπ)dS, (18) of which the right-hand side can be easily calculated or measured. Its second expression comes from (A7).…”
Section: B Physical Root Of the X -Dependencymentioning
confidence: 99%
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