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image/svg+xml Jakob Voss, based on art designer at PLoS, modified by Wikipedia users Nina and Beao Closed Access logo, derived from PLoS Open Access logo. This version with transparent background. http://commons.wikimedia.org/wiki/File:Closed_Access_logo_transparent.svg Jakob Voss, based on art designer at PLoS, modified by Wikipedia users Nina and Beao zbMATH Openarrow_drop_down
image/svg+xml Jakob Voss, based on art designer at PLoS, modified by Wikipedia users Nina and Beao Closed Access logo, derived from PLoS Open Access logo. This version with transparent background. http://commons.wikimedia.org/wiki/File:Closed_Access_logo_transparent.svg Jakob Voss, based on art designer at PLoS, modified by Wikipedia users Nina and Beao
zbMATH Open
Article
Data sources: zbMATH Open
Journal of Guidance Control and Dynamics
Article . 1997 . Peer-reviewed
Data sources: Crossref
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Numerical Approach to Inverse Flight Dynamics

Numerical approach to inverse flight dynamics
Authors: BORRI, MARCO; BOTTASSO, CARLO LUIGI; F. Montelaghi;

Numerical Approach to Inverse Flight Dynamics

Abstract

We develop a general numerical approach to inverse problems of vehicle dynamics, suitable for both e xed- and rotating-wing aircrafts. The formulation is based on an energy-preserving e nite element in time for rigid body dynamics that ensures unconditional stability according to the energy method. The nonlinear inverse problem of motion is solved by assembling a suitable number of time elements over the time interval of interest and enforcing the appropriate boundary conditions. The capabilities and performance of the proposed procedure are illustrated by means of numerical examples. Nomenclature Di = ti, ti C 1; time element d ± (¢)/dt = corotational derivative I3, I6 = 3 £ 3 and 6 £ 6 identity matrices J = spatial inertia dyadic m = mass (O, ii) = e xed frame of origin O, i D 1, 2, 3 (P, ei) = embedded frame of origin P, i D 1, 2, 3 p = l, h; generalized momentum vector (linear, angular ) R(A) = rotation tensor associated with the rotation vector A r = f, m; generalized force vector (force, torque ) T = period of the maneuver t = time w = v, !; generalized velocity vector (linear, angular ) x = P i O; position vector of P in (O, ii) ® = direction cosine matrix D t = ti C1 i ti; time step ± = d a, d e, d r, d T; aileron, elevator, rudder, and thrust

Country
Italy
Related Organizations
Keywords

Application models in control theory, Computational methods in systems theory

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selected citations
These citations are derived from selected sources.
This is an alternative to the "Influence" indicator, which also reflects the overall/total impact of an article in the research community at large, based on the underlying citation network (diachronically).
BIP!Citations provided by BIP!
popularity
This indicator reflects the "current" impact/attention (the "hype") of an article in the research community at large, based on the underlying citation network.
BIP!Popularity provided by BIP!
influence
This indicator reflects the overall/total impact of an article in the research community at large, based on the underlying citation network (diachronically).
BIP!Influence provided by BIP!
impulse
This indicator reflects the initial momentum of an article directly after its publication, based on the underlying citation network.
BIP!Impulse provided by BIP!
17
Average
Top 10%
Average
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