Solution for Nonlinear Three-Dimensional Intercept Problem with Minimum Energy
Classical orbit intercept applications are commonly formulated and solved as Lambert-type problems, where the time-of-flight (TOF) is prescribed. For general three-dimensional intercept problems, selecting a meaningful TOF is often a difficult and an iterative process. This work overcomes this limit...
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Series: | Mathematical Problems in Engineering |
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doaj-17453b2166b94befbb6f8dafc8a9dd3b2020-11-24T20:44:22ZengHindawi LimitedMathematical Problems in Engineering1024-123X1563-51472013-01-01201310.1155/2013/435725435725Solution for Nonlinear Three-Dimensional Intercept Problem with Minimum EnergyHenzeh Leeghim0Donghoon Kim1James Turner2Department of Aerospace Engineering, Chosun University, Gwangju 501-759, Republic of KoreaDepartment of Aerospace Engineering, Texas A&M University, College Station, TX 77843-3141, USADepartment of Aerospace Engineering, Texas A&M University, College Station, TX 77843-3141, USAClassical orbit intercept applications are commonly formulated and solved as Lambert-type problems, where the time-of-flight (TOF) is prescribed. For general three-dimensional intercept problems, selecting a meaningful TOF is often a difficult and an iterative process. This work overcomes this limitation of classical Lambert’s problem by reformulating the intercept problem in terms of a minimum-energy application, which then generates both the desired initial interceptor velocity and the TOF for the minimum-energy transfer. The optimization problem is formulated by using the classical Lagrangian f and g coefficients, which map initial position and velocity vectors to future times, and a universal time variable x. A Newton-Raphson iteration algorithm is introduced for iteratively solving the problem. A generalized problem formulation is introduced for minimizing the TOF as part of the optimization problem. Several examples are presented, and the results are compared with the Hohmann transfer solution approaches. The resulting minimum-energy intercept solution algorithm is expected to be broadly useful as a starting iterative for applications spanning: targeting, rendezvous, interplanetary trajectory design, and so on.http://dx.doi.org/10.1155/2013/435725 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Henzeh Leeghim Donghoon Kim James Turner |
spellingShingle |
Henzeh Leeghim Donghoon Kim James Turner Solution for Nonlinear Three-Dimensional Intercept Problem with Minimum Energy Mathematical Problems in Engineering |
author_facet |
Henzeh Leeghim Donghoon Kim James Turner |
author_sort |
Henzeh Leeghim |
title |
Solution for Nonlinear Three-Dimensional Intercept Problem with Minimum Energy |
title_short |
Solution for Nonlinear Three-Dimensional Intercept Problem with Minimum Energy |
title_full |
Solution for Nonlinear Three-Dimensional Intercept Problem with Minimum Energy |
title_fullStr |
Solution for Nonlinear Three-Dimensional Intercept Problem with Minimum Energy |
title_full_unstemmed |
Solution for Nonlinear Three-Dimensional Intercept Problem with Minimum Energy |
title_sort |
solution for nonlinear three-dimensional intercept problem with minimum energy |
publisher |
Hindawi Limited |
series |
Mathematical Problems in Engineering |
issn |
1024-123X 1563-5147 |
publishDate |
2013-01-01 |
description |
Classical orbit intercept applications are commonly formulated and solved as Lambert-type problems, where the time-of-flight (TOF) is prescribed. For general three-dimensional intercept problems,
selecting a meaningful TOF is often a difficult and an iterative process. This work overcomes this limitation of classical Lambert’s problem by reformulating the intercept problem in terms of
a minimum-energy application, which then generates both the desired initial interceptor velocity and the TOF for the minimum-energy transfer. The optimization problem is formulated by using the classical Lagrangian f and g coefficients, which map initial position and velocity vectors to future times, and a universal time variable x. A Newton-Raphson iteration algorithm is introduced for iteratively solving the problem. A generalized problem formulation is introduced for minimizing the TOF as part of the optimization problem. Several examples are presented, and the results are compared with the Hohmann transfer solution approaches. The resulting minimum-energy intercept solution algorithm is expected to be broadly useful as a starting iterative for applications spanning: targeting, rendezvous, interplanetary trajectory design, and so on. |
url |
http://dx.doi.org/10.1155/2013/435725 |
work_keys_str_mv |
AT henzehleeghim solutionfornonlinearthreedimensionalinterceptproblemwithminimumenergy AT donghoonkim solutionfornonlinearthreedimensionalinterceptproblemwithminimumenergy AT jamesturner solutionfornonlinearthreedimensionalinterceptproblemwithminimumenergy |
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