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ORNL-5388 - the Molten Salt Energy Technologies Web Site

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7-16<br />

and overall fissile production (i.e., potential growth rate).<br />

Table 7.2-6. Equilibrium Cycle Net Fissile Production for<br />

Po ten ti a 1 LMFBR Transmuters*<br />

Net Fissile<br />

Production<br />

Reactor - (kg/GWe - yp)<br />

Core Axial Blanket Radial Blanket<br />

Material Material Materi a1 Pu 233U Fissile<br />

*Using values from Section 4.5-1 (~75% capacity factor). A more recent<br />

study [Proliferation Resistant Large Core Design Study (PRLCDS)] indicates<br />

that substantial improvements in <strong>the</strong> FBR performance is possible.<br />

In addition to <strong>the</strong> systems utilizing <strong>the</strong> classical homogeneous core configuration,<br />

systems utilizing a heterogeneous core configuration (i .e., interspersed fissile and<br />

fertile regions) were examined as a possible means of improving <strong>the</strong> performance of fast<br />

reactors operating on alternate fuel cycles. The substitution of different coolants<br />

and fuel forms (i.e., carbides and metals versus oxides) were also considered. The net<br />

effect of <strong>the</strong>se changes is to increase <strong>the</strong> fuel volume fraction in <strong>the</strong> reactor core,<br />

harden <strong>the</strong> spectrum, or, in some cases, both. The advanced fast reactor concepts show<br />

significant improvement regarding <strong>the</strong> breeding ratio (and doubling time) relative to <strong>the</strong><br />

classical design when operating on alternate fuel cycles; however, <strong>the</strong> performance of <strong>the</strong><br />

alternate fuel cycles is still degraded over that of <strong>the</strong> same reactor type operating on<br />

<strong>the</strong> Pu/~~*U cycle.<br />

7.2.3. Symbiotic Reactor Systems<br />

As has been stated throughout this report, in considering denatured 233U reactor<br />

systems it is assumed that <strong>the</strong> denatured reactors will operate as dispersed power systems<br />

supported by fuel cycle services and reactor transmuters located in secure energy centers.<br />

When <strong>the</strong> system is in full operation no external source of fissile material is supplied;<br />

that is, <strong>the</strong> system is self-contained. Initially <strong>the</strong> resource base (i.e., natural uranium)<br />

can be used to provide a source of 233U for implementing <strong>the</strong> denatured 233U fuel cycle [via<br />

<strong>the</strong> MEU(235)/Th cycle]; however, a shift to plutonium-fueled transmuters will eventually be<br />

required. During this transition period, <strong>the</strong> system can be characterized by <strong>the</strong> rate at<br />

which <strong>the</strong> resource base is consumed (see Chapter 6). In order to compare <strong>the</strong> long-term<br />

potential of various reactor systems under <strong>the</strong> restrictions imposed by <strong>the</strong> denatured fuel<br />

cycle, two system parameters have been developed: (1) <strong>the</strong> energy support ratio, defined<br />

as <strong>the</strong> ratio of dispersed reactor power relative to <strong>the</strong> energy center (or centralized) power,<br />

and (2) <strong>the</strong> inherent growth potential of <strong>the</strong> system. Since both <strong>the</strong> growth rate and <strong>the</strong><br />

energy support ratio involve fissile mass flows, <strong>the</strong>y are interrelated. In order to unambig-<br />

uously determine both parameters, <strong>the</strong> inherent system growth rate is determined at <strong>the</strong><br />

asymptotic value of <strong>the</strong> support ratio, a value which can be viewed as <strong>the</strong> "natural" operat-<br />

ing ratio of <strong>the</strong> system.<br />

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