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order <strong>for</strong> the Node + Chebyshev <strong>for</strong>mulation to arrive at a solution. The Node +<br />

Chebyshev <strong>method</strong> appears to be the most beneficial <strong>for</strong> searching broad areas of the<br />

<strong>design</strong> <strong>space</strong>. On the other h<strong>and</strong>, the N-Vector <strong>for</strong>mulation is the most stable, although it<br />

was not always the fastest approach, <strong>and</strong> in some cases, it was significantly slower. The<br />

N-Vector <strong>for</strong>mulation is there<strong>for</strong>e a good st<strong>and</strong>ard <strong>method</strong> when only a small number of<br />

cases need to be per<strong>for</strong>med.<br />

1.1.3 Analytic, Shape-Based Methods<br />

Indirect <strong>and</strong> direct <strong>method</strong>s tend to be computationally intensive because the<br />

trajectory must be numerically integrated or propagated. An analytic <strong>method</strong>, on the<br />

other h<strong>and</strong>, has the potential to significantly reduce run times by eliminating the need <strong>for</strong><br />

numerical integration <strong>and</strong> instead solving <strong>for</strong> an analytic solution to the equations of<br />

motion.<br />

Petropoulos, at Purdue University, developed a shape-based <strong>method</strong> intended <strong>for</strong><br />

quickly searching a broad <strong>design</strong> <strong>space</strong> <strong>and</strong> generating initial guesses to then be used in a<br />

more accurate trajectory <strong>optimization</strong> program. 33,34,35<br />

This <strong>method</strong> assumes that the<br />

<strong>space</strong>craft trajectory follows a predetermined shape, from which the thrust profile can be<br />

determined. With the correct choice of shape, there exists an analytic solution to the<br />

equations of motion. The motion of the <strong>space</strong>craft between planets can either be purely<br />

conic (coasting) or involve thrusting. Each leg can be characterized as thrust, thrustcoast,<br />

or coast-thrust. For the thrusting segments, the in-plane motion of the <strong>space</strong>craft is<br />

assumed to follow an exponential sinusoid shape, given by Equation 11, where k 0 , k 1 , k 2 ,<br />

<strong>and</strong> φ are all constants that define the shape of the trajectory:<br />

r = k 0<br />

e k 1 sin( k 2 θ +φ)<br />

(11)<br />

13

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