Trajectory optimisation of six degree of freedom aircraft using differential flatness
Citations
5 citations
2 citations
2 citations
2 citations
Cites background or methods from "Trajectory optimisation of six degr..."
...in [12] for trajectory optimization and the same model is adopted throughout this paper for all the simulations....
[...]
...More details on the modeling of forces, moments and parameters used can be found in [12]....
[...]
References
3,025 citations
"Trajectory optimisation of six degr..." refers background in this paper
...The set of 12 differential equations ((2), (3), (5) and (7)) for the 12 states – x, y, z, u, v, w, φ, θ, ψ, p, q, r constitute the aircraft’s six-degree-of-freedom (6DoF) equations of motion involving 6 control inputs – δf, δa, δe, δr, CTx, CTy....
[...]
...Flatness-based control was originally introduced by Fliess et al.(3), and its application to trajectory optimisation was explored by Nieuwstadt and Murray(4)....
[...]
..._ u _ v _ w 2 4 3 5 + S _ S uv w 2 4 3 5= f m + S 0 0 g 2 4 3 5 S Wxz _ z 0 0 2 4 3 5 ...(3)...
[...]
...introduced by Fliess et al.((3)), and its application to trajectory optimisation was explored by Nieuwstadt and Murray((4))....
[...]
...Rearrangement of the time derivative of (2) yields us (3) and (4), which concern the forces on the body and the rate of change of the components of the relative wind along the body axes:...
[...]
484 citations
451 citations
"Trajectory optimisation of six degr..." refers background or methods in this paper
...CL is determined by plugging this solution for CTx into (15) while Cm is known from (10)....
[...]
...The x and z components of the body axes force f in (9) can be rearranged to yield (15):...
[...]
...The aerodynamic forces and moments are estimated using a look-up table((15)) that spans across operating points....
[...]
...A quadratic equation (17) for CTx can be obtained from (15) and (16):...
[...]
270 citations
"Trajectory optimisation of six degr..." refers background in this paper
...Flatness-based control was originally introduced by Fliess et al.(3), and its application to trajectory optimisation was explored by Nieuwstadt and Murray(4)....
[...]
...These are then substituted into (4) and (7) to obtain f and m, respectively....
[...]
...f = Fx Fy Fz 2 4 3 5=m _ u_ v _ w 2 4 3 5 + wq vr ru pw pv qu 2 4 3 5 g Sθ CθSφ CθCφ 2 4 3 5 +Wxz _ z CψCθ CψSθSφ SψCφ CψSθCφ + SψSφ 2 4 3 5 0 @ 1 A ...(4)...
[...]
...Rearrangement of the time derivative of (2) yields us (3) and (4), which concern the forces on the body and the rate of change of the components of the relative wind along the body axes:...
[...]
..., and its application to trajectory optimisation was explored by Nieuwstadt and Murray((4))....
[...]
267 citations