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Project Cyclops, A Design... - Department of Earth and Planetary ...

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where r = "Ym/'rs- If we let<br />

o-_--o----_<br />

+ --<br />

Nef f = n + (kr - l)P,_n (L7)<br />

c_<br />

c<br />

-------o--,_ ---3_ ----o_- _----o<br />

be the effective number <strong>of</strong> side tunnels <strong>of</strong> length s, then<br />

we have simply<br />

C = SNell7 s (L8)<br />

For the tunnel pattern shown in Figure L-la, k = I,<br />

<strong>and</strong> N m is twice the nearest inleger to as/S = x/)T/rr- i/2.<br />

Thus,<br />

Aim= ,.l_ntd7 ) (L9)<br />

Pattern<br />

2(a)<br />

where "int" means "the integer part <strong>of</strong>." Substituting in<br />

equation (L7) we find<br />

_, \ / /<br />

_, \ ,_ \, [ / / ,,<br />

Nla = n + 2(r- 1) int _ (LI0)<br />

For the tunnel pattern <strong>of</strong> Figure L-!b, k = VC2-<strong>and</strong><br />

N m is ]bur times the nearest integer to (as/SW_) - 1.<br />

Thus,<br />

.....<br />

Nlb = n + 4(Vr}-r - 1) int (LI 1)<br />

9<br />

For the tunnel pattern <strong>of</strong> Figure L-2a, k = _v/-ff/2 <strong>and</strong><br />

n m is twice tile nearest integer to 2ah/X/3s. Thus,<br />

/ / /), \ ,,<br />

Pattern<br />

2(b)<br />

3,'2a = ,<br />

(L12)<br />

Figure L-2. Tunnel patterns fi_r hexagonal lattice array.<br />

If we divide N by n to obtain the .:_l_ern factor<br />

f= N/n, we can express the tunneling cost simply as<br />

Finally, for the tunnel pattern <strong>of</strong> Figure L-2b,<br />

k = 2 anti N m is six times the nearesl integer to<br />

(% - s_3/2)/es.<br />

C = J'nSTs = fnC u (LI 4)<br />

N2b = n+6(2r-ltint-- i _J4 / F,/v n +l-v/-3 )<br />

Ll _)<br />

where Cu = cost <strong>of</strong> a unit side tunnel. Table L-3 !isis the<br />

pattern factors for the tunnel pattern <strong>of</strong> Figures l.-I <strong>and</strong><br />

L-2 for various sizes <strong>of</strong> array, <strong>and</strong> for r = l _<br />

217

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