Lawrence Radiation Laboratory

H. Cheung, Critical Keview of Heat Pipe Theory and Applications, DCKT-50453, Lawrence Radiation Laboratory, University of California, Livermore, Calif., 1968. 

Lelevier, R. and Ragent, B., Lectures on Hydrodynamics and Shock Waves, Lawrence Radiation Laboratory, University of California Report No. UCRL-4333, Livermore, CA, 61 pp., April 1954. 

Wilkins, M. L. 1969. Calculation of elastic-plastic flow. Lawrence Radiation Laboratory report no. UCRL-7322 Rev. I. 

Ref A. vonEgidy et al, A New Liquid Explosive, NTN , UCRL-5861, Lawrence Radiation Laboratory, Univ of Calif, Livermore (1960)... 

Howe, P.W., T. C. Parsons and L. E. Miles The Water Shielded Cave Facility for Totally Enclosed Master-Slave Operations at Lawrence Radiation Laboratory. Report UCRL-9657 (9- Okt. 1961). 

Hiskes, J. R. Tarter, C. B. Report UCRL-7088 Lawrence Radiation Laboratory Livermore CA, 1964. 

Patricia W. Durbin Lawrence Radiation Laboratory University of California Berkeley, California... 

D. Omellas, J. Phys. Chem., 72, 2390 (1968). Strictly speaking, the code used in this paper was the RUBY code, H. B. Levine and R. E. Sharpies, Report UCRL-6185, Lawrence Radiation Laboratory, Livermore, CA, 1962 using the BKW equation of state from C. L. Mader, Report LA-2900, Los Alamos Scientific Laboratory (1963). (See also C. L. Mader, Numerical Modeling of Detonation, University of California Press, 1979)... 

Lawrence Radiation Laboratory, University of California, Livermore, Calif. 

Fujita, D. K., Ph.D. Thesis, University of California Doc. No. UCRL-19507, Lawrence Radiation Laboratory, U.S. Atomic Energy Commission, Berkeley, CA, 1969. 

Lawrencium was synthesized by Ghiorso, Sikkeland, Larsh and Latimer in 1961 in Lawrence Radiation Laboratory, Berkeley, California. The new element was named after Ernest 0. Lawrence. The element has no practical application. 

H. B. Levine and R. E. Sharpies, Operator s Manual for ruby, Lawrence Radiation Laboratory Rept., UCRL-6815, 1962. 

As used herein, the term RUBY includes the results of computations at tbe Los Alamos Scientific Laboratory by the STRETCH BKW computer code and at NOL by the Lawrence Radiation Laboratory s RUBY code. For the purposes of present discussions, these codes differ only in minor regards and, unless otherwise specified, RUBY computations shall he considered as based on Mader s most recent covolume factors and the more appropriate of his dual K-W parameter sets (Ref. 11 of Part I), with the heat of formation of solid carbon taken as zero. See Part I for other leading references. 

Dr. E. Lee, Lawrence Radiation Laboratory (private communication). The referee has pointed out to us that Mader experimented with a positive AH/ in the course of his BKW studies. While using a positive AHj for carbon was a help in calculating P and D, it caused troubles in calculations involving the isentropic expansion of the detonation products, perhaps because it was not allowed to change during this process. 

Dr. J. W. Kury, Lawrence Radiation Laboratory and B. G. Craig, Los Alamos Scientific Laboratory (private communications). Reference 19. 

Edwards, A. C., Holzman, R. L., Temperatures Induced in Plastic Samples by Irradiation in an Electron Beam, Internal Report of Chemical Engineering Section, Lawrence Radiation Laboratory, Livermore, Calif. 

Studies at Lawrence Radiation Laboratory (LRL) (Kury et al (Ref 7) quoting Wilkins) indicate that in 1-D systems a twofold volume expansion of the detonation products is sufficient to transfer the maximum amount of energy to a metal in contact with these detonation products, but for tangential incidence (2-D systems) a sevenfold volume expansion is required. They state that for explosively driven cylinders observations of the early stages of expansion are expected to provide information on 1-D systems, and measurements of the later stages of expansion are expected to characterize 2-D systems. We will consider their hypothesis in Section IV... 

Bedford, R. G., Jackson, D. D., Lawrence Radiation Laboratory, UCRL-... 

Samples of Sedan ejecta were collected around the crater lip and along several transects of the ejecta field. A 10-inch diameter hole is dug with a conventional posthole auger at each sampling station. Discrete samples are taken at depths of 6 inches, 1 foot and at 1-foot intervals below that to a depth of 5 or 6 feet. The sample is passed through a 2-mm. sieve and collected into 1-quart wide-mouthed Mason jars. Samples are shipped to the Lawrence Radiation Laboratory (Livermore, Calif.), where aliquots are taken from the jars and lyophilized on a large vacuum manifold. Individual glass traps are utilized on the manifold and extracted water from each ejecta sample is collected separately. The extracted water is assayed for tritium with a model 3375 Packard liquid... 

In Table IV, the atom ratio data obtained by radiochemical analysis of a series of aerial filter and fallout samples are presented. The analyses were performed by the Radiochemistry Division at Lawrence Radiation Laboratory, Livermore. The atom ratios, which we designate by rxA in... 

California, Lawrence Radiation Laboratory, UCRL-2057 (Title U, Report SRD) (1957). 

Lawrence Radiation Laboratory, Livermore. I would like to express my appreciation to them for their efforts, and especially to J. B. J. Read for his contribution to the mathematical analysis used. 

The relatively small spread of the numbers in Table I (about a factor of six from smallest to largest) is remarkable in view of the considerable differences in venting phenomenology among the three shots and the variety of sources for the radiochemical data used. Danny Boy data were supplied by the U.S. Air Force Sedan data by Tracerlab, Nuclear Science and Engineering Corp., and Hazleton Nuclear Science Corp. Palanquin data were supplied by Lawrence Radiation Laboratory. 

A study carried out at the Lawrence Radiation Laboratory of the University of California by Vanderveen (Vl) strongly suggests another type of interaction model see also Vermeulen (V5). Vanderveen measured the drop size at different distances from the impeller of a baffled, stirred tank reactor in which two immiscible liquid phases were contacted, and found that a very substantial increase in drop size occurs at remote distances. The increase, which was attributed to coalescence, appeared to be dependent on the physical properties of the phase system. 

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