ANS is committed to advancing, fostering, and promoting the development and application of nuclear sciences and technologies to benefit society.
Explore the many uses for nuclear science and its impact on energy, the environment, healthcare, food, and more.
Division Spotlight
Materials Science & Technology
The objectives of MSTD are: promote the advancement of materials science in Nuclear Science Technology; support the multidisciplines which constitute it; encourage research by providing a forum for the presentation, exchange, and documentation of relevant information; promote the interaction and communication among its members; and recognize and reward its members for significant contributions to the field of materials science in nuclear technology.
Meeting Spotlight
ANS Student Conference 2025
April 3–5, 2025
Albuquerque, NM|The University of New Mexico
Standards Program
The Standards Committee is responsible for the development and maintenance of voluntary consensus standards that address the design, analysis, and operation of components, systems, and facilities related to the application of nuclear science and technology. Find out What’s New, check out the Standards Store, or Get Involved today!
Latest Magazine Issues
Feb 2025
Jul 2024
Latest Journal Issues
Nuclear Science and Engineering
March 2025
Nuclear Technology
Fusion Science and Technology
February 2025
Latest News
Colin Judge: Testing structural materials in Idaho’s newest hot cell facility
Idaho National Laboratory’s newest facility—the Sample Preparation Laboratory (SPL)—sits across the road from the Hot Fuel Examination Facility (HFEF), which started operating in 1975. SPL will host the first new hot cells at INL’s Materials and Fuels Complex (MFC) in 50 years, giving INL researchers and partners new flexibility to test the structural properties of irradiated materials fresh from the Advanced Test Reactor (ATR) or from a partner’s facility.
Materials meant to withstand extreme conditions in fission or fusion power plants must be tested under similar conditions and pushed past their breaking points so performance and limitations can be understood and improved. Once irradiated, materials samples can be cut down to size in SPL and packaged for testing in other facilities at INL or other national laboratories, commercial labs, or universities. But they can also be subjected to extreme thermal or corrosive conditions and mechanical testing right in SPL, explains Colin Judge, who, as INL’s division director for nuclear materials performance, oversees SPL and other facilities at the MFC.
SPL won’t go “hot” until January 2026, but Judge spoke with NN staff writer Susan Gallier about its capabilities as his team was moving instruments into the new facility.
Kiyoshi Yatsu, Teruji Cho, Mafumi Hirata, Hitoshi Hojo, Makoto Ichimura, Kameo Ishii, Akiyoshi Itakura, Isao Katanuma, Junko Kohagura, Yousuke Nakashima, Teruo Saito, Teruo Tamano, Satoshi Tanaka, Yoshinori Tatematsu, Masayuki Yoshikawa
Fusion Science and Technology | Volume 39 | Number 1 | January 2001 | Pages 3-9
Invited Review Lectures | doi.org/10.13182/FST01-A11963408
Articles are hosted by Taylor and Francis Online.
After the last Novosibirsk Conference (1998), GAMMA 10 experiments have advanced in long sustainment of confining potential and higher density experiments. An experiment which attained doubling of density due to potential confinement with a 50 ms duration was reported before [1]. Experiments for long sustainment of potential confinement were carried out in order to study problems of steady state operation of a tandem mirror reactor. A confining potential was sustained for 150 ms by sequentially injecting two electron cyclotron resonance heating (ECRH) powers in the plug region. It was difficult before to increase the central cell density higher than about 2.5 × 1012cm−3 with and/or without potential confinement due to some density limiting mechanism. In order to overcome this problem, a new higher frequency ion cyclotron range of frequency (ICRF) system (RF3: 36–76 MHz, ω/ωci~6-10) has been installed. A higher density plasma has been produced with RF3. In addition to RF3, neutral beam injection (NBI) in the anchor cell became effective by reducing neutral gas from beam injectors. The plasma density in the anchor cell increased 70% by NBI for 20 ms, and the central cell density increased 20% with the density increase in the anchor cell. Potential confinement experiments at higher central cell densities up to 4 × 1012 cm−3 were carried out with RF3 and NBI and 15% density increase due to the potential confinement was obtained in the high density experiments. The ion temperature on the axis and particle confinement time during potential confinement were 3 keV and 10 ms, respectively. We expect a larger density increase at a higher initial density by optimization of heating scenario with respect to ECRH, ICRF heating and NBI.