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Remembering Joseph M. Hendrie
Joseph M. Hendrie
To those of us who knew Joe, even prior to his appointment as chair of the Nuclear Regulatory Commission, it is an understatement to say that he was a larger-than-life member of the nuclear science and technology enterprise. He was best known to the broader community for two major accomplishments: the design and construction of the High Flux Beam Reactor (HFBR) at Brookhaven National Laboratory and the creation of the standard review plan (SRP) for the U.S. Atomic Energy Commission.
In addition to the products of these endeavors becoming major fundaments to their respective communities, they were uniquely Joe. The safety analysis report for the HFBR was written essentially single-handedly by him. This was true of the SRP as well, which became the key safety review document for the NRC as it performed safety reviews for the growing number of power reactor applications in the United States. His deep technical knowledge of nuclear engineering and his extraordinary management skills made this possible.
Kaname Kizu, Keiji Miyazaki, Tetsuo Tanabe
Fusion Science and Technology | Volume 28 | Number 3 | October 1995 | Pages 1205-1210
Tritium Properties and Interaction with Material | Proceedings of the Fifth Topical Meeting on Tritium Technology In Fission, Fusion, and Isotopic Applications Belgirate, Italy May 28-June 3, 1995 | doi.org/10.13182/FST95-A30573
Articles are hosted by Taylor and Francis Online.
A precise hydrogen permeation experiment for beryllium was conducted at a temperature ranging from 735 to 1000 K under hydrogen gas pressure of 101 to 103 Pa. Diffusion coefficient and permeation coefficient were determined from the steady state penneation and time transient penneation independently. The steady state penneation rate was proportional to the square root of H2 pressure and the time sequence of penneation rate agreed well with theoretical one, indicating that the penneation controlled by bulk diffusion. The temperature dependencies of the penneation coefficients (Φ) and diffusion coefficients (D) were respectively,Φ=(1.0±0.1)×10−6exp[−73±20(kJ/mol)/RT] (mol·m−1·s−1·Pa1/2),D=(1.3±0.1)×10−7exp[59±20(kJ/mol)/RT] (m2·s−1).Solubility calculated from the relation Φ=DS wasS=7.1 exp[−14(kJ/mol)/RT] (mol·m−3·Pa−1/2).