secondary spаcecraft reference plane primary spacecraft primary. orbit plane Once you fix the primary or target spacecraft (the selection of primary spacecraft is only a matter of context), the relative motion of the secondary spacecraft is governed by the following initial value problem: " - 2wy - 3w? a = fr ; (0) = xo, r' (0) = x, " + 2wa' = fyi y (0) = yo, y (0) = " + w? z = fz ; z (0) = 20; z (0) Where w stands for the mean angular velocity of the primary spacecraft within its orbit plane. () Also, fy represents the differential acceleration on the secondary spacecraft. fz (t) Assuming there is no external force acting on the secondary spacecraft, use Laplace Transform to determine its position y (t) in the space. Your |2(t), answer will be in terms of w and the set of intial conditions. Hint: The z part of the given IVP is a second order IVP by itself. Therefore it can be solved for z using Laplace Transform. For each of the first two differential equations (from the top), begin by taking Laplace Transform on both sides. This would eventually result in an algebraic system of equations in X (s) and (s).
secondary spаcecraft reference plane primary spacecraft primary. orbit plane Once you fix the primary or target spacecraft (the selection of primary spacecraft is only a matter of context), the relative motion of the secondary spacecraft is governed by the following initial value problem: " - 2wy - 3w? a = fr ; (0) = xo, r' (0) = x, " + 2wa' = fyi y (0) = yo, y (0) = " + w? z = fz ; z (0) = 20; z (0) Where w stands for the mean angular velocity of the primary spacecraft within its orbit plane. () Also, fy represents the differential acceleration on the secondary spacecraft. fz (t) Assuming there is no external force acting on the secondary spacecraft, use Laplace Transform to determine its position y (t) in the space. Your |2(t), answer will be in terms of w and the set of intial conditions. Hint: The z part of the given IVP is a second order IVP by itself. Therefore it can be solved for z using Laplace Transform. For each of the first two differential equations (from the top), begin by taking Laplace Transform on both sides. This would eventually result in an algebraic system of equations in X (s) and (s).
Elements Of Electromagnetics
7th Edition
ISBN:9780190698614
Author:Sadiku, Matthew N. O.
Publisher:Sadiku, Matthew N. O.
ChapterMA: Math Assessment
Section: Chapter Questions
Problem 1.1MA
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