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The FuTure oF nuclear Fuel cycle - MIT Energy Initiative

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(7A.3)<br />

and,<br />

(7A.4)<br />

<strong>The</strong>re is a unique p * such that these two LCOEs equal one another, and are equal to the<br />

LCOE for the <strong>cycle</strong> as a whole:<br />

This condition is what we use to determine the price of plutonium for the <strong>cycle</strong>. 4<br />

(7A.5)<br />

<strong>The</strong> Fast Reactor Re<strong>cycle</strong><br />

In recycling of spent fuel through fast reactors, the process of passing along a portion of the<br />

original fuel to the next reactor is repeated ad infinitum. A truly complete LCOE calculation<br />

requires a full accounting of the infinite chain of costs incurred as the packet of fuel<br />

moves from one reactor to the next. So the numerator of our formula will now show an infinite<br />

chain of profiles of costs, and the denominator will show an infinite chain of profiles of<br />

electricity production. Let subscript j index the passes through a reactor, with j=1 referring<br />

to the initial pass through the light water reactor with fresh UOX fuel, and j=2,3,4… referring<br />

to the subsequent passes through fast reactors using fast reactor fuel fabricated using<br />

re<strong>cycle</strong>d transuranics. <strong>The</strong> window of time [A j ,B j ] encompasses the electricity produced in<br />

the j th pass through a reactor, C jt denotes the full set of realized costs in pass j at date t, and<br />

Q jt denotes the time profile of electricity produced in pass j at date t. <strong>The</strong>n the LCOE for the<br />

Fast Reactor Re<strong>cycle</strong> is given by:<br />

(7A.6)<br />

appendix to chapter 7: economics 171

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