Plutonium Denaturing by 238Pu

Abstract This paper analyzes whether reactor plutonium after denaturing by increasing its isotopic content of 238Pu to 6 to 8% can be regarded as proliferation resistant. In this case the utilization of such denatured reactor plutonium would become unsuitable for a nuclear explosive device (NED) because the high-explosive lenses surrounding the plutonium would melt or their elevated temperature would lead to self-ignition. Eight different plutonium isotopic mixtures with increasing 238Pu content are analyzed, and their critical masses if surrounded by a 5-cm-thick reflector of natural uranium are determined. This allows calculation of the alpha-particle heat power generated in the plutonium sphere by 238Pu and other plutonium isotopes. Then, three levels of technology with regard to the size of such hypothetical NEDs (HNEDs) and the technological level of high explosives are defined. On the basis of material data available in the open scientific literature, the radial temperature profiles in such HNEDs of an assumed configuration are calculated, and it is found that for low-technology HNEDs the limiting temperatures are exceeded for a 238Pu content of 1.6%. For high-technology HNEDs these limiting temperatures are exceeded for a 238Pu content above ˜6% or somewhat more. Such denatured plutonium can be considered as proliferation resistant, similarly as uranium with <20% 235U or <12% 233U.

[1]  G. Kessler,et al.  Fuel Cycle Options for the Production and Utilization of Denatured Plutonium , 2007 .

[2]  G. Kessler Requirements for nuclear energy in the 21st century , 2001 .

[3]  C. Mader,et al.  Thermal Initiation of Explosives , 1960 .

[4]  J. Serp,et al.  Promising Pyrochemical Actinide/Lanthanide Separation Processes Using Aluminum , 2006 .

[5]  G. Kesler,et al.  Moderne Strategien zur Beseitigung von Plutonium , 2001 .

[6]  B. M. Dobratz,et al.  Properties of chemical explosives and explosive simulants , 1972 .

[7]  C. Heising-Goodman An Evaluation of the Plutonium Denaturing Concept as an Effective Safeguards Method , 1980 .

[8]  Y. Ronen,et al.  A “Nonproliferating” Nuclear Fuel for Light Water Reactors , 1991 .

[9]  Steve Fetter,et al.  Detecting nuclear warheads , 1990 .

[10]  G. Karsten,et al.  Effects of Different Types of Void Volumes on the Radial Temperature Distribution of Fuel Pins , 1970 .

[11]  A. Schneider,et al.  The Role of Plutonium-238 in Nuclear Fuel Cycles , 1982 .

[12]  G. Kessler,et al.  Requirements for nuclear energy in the 21st century nuclear energy as a sustainable energy source , 2002 .

[13]  K. Rudolph,et al.  Vibrocompacted fuel for the liquid metal reactor BOR-60 , 1993 .

[14]  Harold A. Feiveson Proliferation Resistant Nuclear Fuel Cycles , 1978 .

[15]  Mujid S. Kazimi,et al.  Use of Thorium for Transmutation of Plutonium and Minor Actinides in PWRs , 2004 .

[16]  J. C. Mark,et al.  Explosive Properties of Reactor-Grade Plutonium , 2009 .

[17]  J. J. Laidler,et al.  Development of pyroprocessing technology , 1997 .

[18]  T. Yuge,et al.  Experiments on Heat Transfer From Spheres Including Combined Natural and Forced Convection , 1960 .