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Conference Spotlight
Nuclear Energy Conference & Expo (NECX)
September 8–11, 2025
Atlanta, GA|Atlanta Marriott Marquis
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The Frisch-Peierls memorandum: A seminal document of nuclear history
The Manhattan Project is usually considered to have been initiated with Albert Einstein’s letter to President Franklin Roosevelt in October 1939. However, a lesser-known document that was just as impactful on wartime nuclear history was the so-called Frisch-Peierls memorandum. Prepared by two refugee physicists at the University of Birmingham in Britain in early 1940, this manuscript was the first technical description of nuclear weapons and their military, strategic, and ethical implications to reach high-level government officials on either side of the Atlantic. The memorandum triggered the initiation of the British wartime nuclear program, which later merged with the Manhattan Engineer District.
Helmut Jacobs
Nuclear Technology | Volume 71 | Number 1 | October 1985 | Pages 131-144
Technical Paper | Fusion | doi.org/10.13182/NT85-A33715
Articles are hosted by Taylor and Francis Online.
Modifications of Rayleigh-Taylor instability growth by a gradual density increase instead of a step increase, finite fluid thickness, convection (or ablation), three-dimensional disturbances, nearby stable stratification or fixed boundaries, and nonlinear saturation are quantitatively assessed in typical model cases. To account for gradual density transitions, novel approximate but conservative correlations are given that can replace a hitherto widely used incorrect relation. The stabilizing effects of stable stratification, a fixed boundary (below), and a free surface (above) close to the instability zone are discussed in detail for the first time. For the effect of convection a new and simple derivation of Bodner’s formula is presented, which reveals that the formula describes a fictitious effect due to observation of the disturbance at a moving location. A half-analytical procedure is proposed that allows an account at the same time for several effects resulting from the actual density profile and the possible variations of this profile and its acceleration with time, for example, during ablative acceleration of thin foils.