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Division Spotlight
Isotopes & Radiation
Members are devoted to applying nuclear science and engineering technologies involving isotopes, radiation applications, and associated equipment in scientific research, development, and industrial processes. Their interests lie primarily in education, industrial uses, biology, medicine, and health physics. Division committees include Analytical Applications of Isotopes and Radiation, Biology and Medicine, Radiation Applications, Radiation Sources and Detection, and Thermal Power Sources.
Meeting Spotlight
Conference on Nuclear Training and Education: A Biennial International Forum (CONTE 2025)
February 3–6, 2025
Amelia Island, FL|Omni Amelia Island Resort
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!
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Three nations, three ways to recycle plastic waste with nuclear technology
Plastic waste pollutes oceans, streams, and bloodstreams. Nations in Asia and the Pacific are working with the International Atomic Energy Agency through the Nuclear Technology for Controlling Plastic Pollution (NUTEC Plastics) initiative to tackle the problem. Launched in 2020, NUTEC Plastics is focused on using nuclear technology to both track the flow of microplastics and improve upstream plastic recycling before discarded plastic can enter the ecosystem. Irradiation could target hard-to-recycle plastics and the development of bio-based plastics, offering sustainable alternatives to conventional plastic products and building a “circular economy” for plastics, according to the IAEA.
R. Gwin, E. G. Silver, R. W. Ingle, H. Weaver
Nuclear Science and Engineering | Volume 59 | Number 2 | February 1976 | Pages 79-105
Technical Paper | doi.org/10.13182/NSE76-A15682
Articles are hosted by Taylor and Francis Online.
The neutron absorption and fission cross sections for 239Pu and 235U have been measured over the neutron energy range from 0.02 eV to 200 keV. In addition, the neutron capture cross section for 197Au was measured from 10 to 50 keV and the fission cross section of 233U was measured from 0.1 to 100 keV. Normalization of the 239Pu and 235U data was made over the energy region from 0.02 to 0.4 eV to the ENDF/B-III neutron cross sections for these isotopes, Mat 1159 and 1157, respectively. The capture cross section for 197Au was normalized using the saturated resonance method for the 4.9-eV resonance. For 233U fission, the normalization was made using the results of Weston et al. The neutron flux was measured using the 10B(n,α) reaction; the energy variation used for this reaction was that given in ENDF/B-III. The pulsed-neutron beam for these measurements was generated using the Oak Ridge Electron Linear Accelerator. A large liquid scintillator about 40 m from the neutron source was used to detect the prompt gamma-ray cascades resulting from neutron absorption in the sample. The time interval between the burst of neutrons and the detection of the absorption event was used to establish the neutron energy scale. The sample of the fissile isotopes was contained in multiplate (pulse) ionization chambers and those neutron absorption events detected in coincidence with a pulse from the ionization chamber were defined as fission events. In general for 239Pu and 235U, these experiments indicated lower neutron fission cross sections than contained in ENDF/B-III for energies above 10 keV. The measured values of the ratio α, neutron capture-to-neutron fission, for 239Pu agree within errors with those derived from ENDF/B-III, Mat 1159. For the present measurements, the uncertainty on α for 239Pu is ∼11% at 10 keV and increases to ∼30% at 100 keV. The experimental results for the neutron capture cross section for 197Au are ∼15% lower than the ENDF/B-III values. The measurements of the ratio of the neutron fission cross section for 233U to that for 235U are generally higher than the ENDF/B-III values by ∼5%.