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2023 | OriginalPaper | Buchkapitel

Second-order Sufficient Conditions of Strong Minimality with applications to Orbital Transfers

verfasst von : Leonardo Mazzini

Erschienen in: Modeling and Optimization in Space Engineering

Verlag: Springer International Publishing

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Abstract

We present second-order Extended Sufficiency Conditions applicable without Strict Legendre Conditions and without local controllability assumption also in the frame of saturated and bang–bang control. We provide a procedure to maximize the interval where the Sufficient Conditions can be applied using a Riccati Matrix Equation and compare this procedure with the classic conjugate point condition. Applications to Finite and Infinite Thrust Orbital Transfer cases are given at the end.

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Fußnoten
1
The symbol | | will be used to mean the Euclidean Norm.
 
2
Both hypotheses can be relaxed, and we introduce them in this form for simplicity.
 
3
We refer to the Clarke generalized gradient, see [10], which is a non-empty closed convex set; we use the same symbol to mean the generalized gradient set and the partial derivative, the ambiguity being resolved by the logical statement.
 
4
This representation structurally satisfies the Maximum Principle and is a general presentation of the H0/I Hamiltonians close to cross points. It is easy to verify that H(z) = H0(z) − k(S)S(z) does not agree with the Maximum Principle.
 
5
To clarify the notation used, σ,σg = ΣTx,xg Σ. xσ = ΣTx, so σ, π, ν, and μ are multi-indices that indicate the components of a matrix after a transformation by Σ,  Π, N, M; 01,π = 0ν,π = 01,dim(π), and Iσ,σ is the identity matrix of dimension dim(σ).
 
6
\(\partial _{\alpha ,\beta }\hat {H}_t\) are the second derivatives of the Hamiltonian on the candidate extremal arc.
 
7
Δ gives the jump of the variable in the time positive direction, i.e., \( \bar {x}|{ }_{t}=\bar {x}|{ }_{t+}-\bar {x}|{ }_{t-}\)
 
8
Calling as before in Eqs. (7) \(A_t=\partial _{xp}\hat {H}_t, B_t=\partial _{pp}\hat {H}_t,C_t=\partial _{xx}\hat {H}\).
 
9
At, Bt, and Ct are defined by Eqs. (7).
 
10
This is an extension of the classic ones which do not take into account the jumps at the cross points.
 
11
The solution at a given time t ∈ [t0, tf] − Θ can be seen as a finite chain of continuous functions. From the terminal point to the first crossing point, \((U^{\beta }_{t}, V^{\beta }_{t})\) are locally continuous with respect to β due to the classic ODE theorems and the continuity of At, Bt, and Ct, at the crossing point the left limit of the solution is continuous with respect to the right limit (see Eqs. (22)), and then we sequentially continue this process in a finite number of steps until we reach the point t.
 
12
The additional Normality condition requested in Ref.[12] is the Strong Normality of both terminals. The condition for the right terminal is obviously satisfied because Π = ⊘. The condition for the left terminal can be easily proved because \(p^T f(\hat {x},\hat {u})- p^T f(\hat {x},u)= p_3(\hat {p}_3/\chi -u_s)+p_4(\hat {p}_4/\chi -u_c) \geq 0, \forall (u_s,u_c) \in U\) admits as only solution p = 0 (it suffices to choose us = 2p3χ, uc = 2p4χ to make this expression strictly negative for any p ≠ 0).
 
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Metadaten
Titel
Second-order Sufficient Conditions of Strong Minimality with applications to Orbital Transfers
verfasst von
Leonardo Mazzini
Copyright-Jahr
2023
DOI
https://doi.org/10.1007/978-3-031-24812-2_8

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