ORNL-5388 - the Molten Salt Energy Technologies Web Site
ORNL-5388 - the Molten Salt Energy Technologies Web Site
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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