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N<br />

∑<br />

i<br />

W i<br />

= 0.5⋅<br />

⎛<br />

max⎜<br />

⎝<br />

θ wedge,Legi<br />

N<br />

∑<br />

i<br />

θ wedge,Legi<br />

N<br />

∑<br />

i<br />

+ 0.5⋅<br />

⎞ ⎛<br />

⎟ max⎜<br />

⎠ ⎝<br />

∆V opt,Legi<br />

N<br />

∑<br />

i<br />

∆V opt,Legi<br />

⎞<br />

⎟<br />

⎠<br />

(17)<br />

Each <strong>pruning</strong> metric is summed over all of the legs in the sequence, where each leg<br />

represents each asteroid pair in the sequence, <strong>and</strong> then normalized to fall between zero<br />

<strong>and</strong> one. The two summed metrics are then combined with an equal weighting. By<br />

ranking all of the asteroid sequences using this single value, a user-defined percentage of<br />

sequences can be eliminated.<br />

Final Mass (kg)<br />

1000<br />

900<br />

800<br />

700<br />

600<br />

500<br />

400<br />

300<br />

200<br />

100<br />

0<br />

0 0.2 0.4 0.6 0.8 1 1.2<br />

Summed Pruning Metrics<br />

Figure 28: Final mass as a function of the summed <strong>pruning</strong> metric (Equation 17) <strong>for</strong> each asteroid<br />

sequence remaining in the small sample problem.<br />

Figure 28 plots W i from Equation 17 against the corresponding optimal low-thrust<br />

final mass <strong>for</strong> each asteroid sequence in the small sample problem. In order to keep all<br />

feasible solutions (all solutions with a final mass greater than 500 kg) in the <strong>design</strong> <strong>space</strong>,<br />

up to 55% of the asteroid sequences can be eliminated. In order to keep all of the top ten<br />

asteroid sequences in the <strong>design</strong> <strong>space</strong>, up to 85% of the sequences can be eliminated.<br />

Finally, to keep just the optimum solution in the <strong>design</strong> <strong>space</strong>, up to 99% of the<br />

sequences can be eliminated. The main drawback to this <strong>method</strong>, however, is that each<br />

67

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