8 results on '"nuclear fusion power"'
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2. Applicability Analysis of Energy Storage Techniques for CFETR Fusion Power Plant
- Author
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Zhanpeng LIANG, Kui XIANG, Hua LI, and Guangtao ZHU
- Subjects
nuclear fusion power ,energy storage ,cfetr ,research review ,power plant design ,Energy industries. Energy policy. Fuel trade ,HD9502-9502.5 - Abstract
[Introduction] The power output of China Fusion Engineering Test Reactor (CFETR) is periodic, which can not directly meet the stable and continuous input requirements of conventional power generation equipment. CFETR fusion power plant needs to integrate a specific process system between nuclear island and conventional island. [Method] By investigating the application of concentrating solar power plants and the literature research of fusion power plants, this paper presented a discussion based on the preliminary performance of CFETR about the comparison between energy storage and energy supplement, energy storage techniques, thermal storage mediums and thermal storage system schemes. [Result] For fusion reactors with water-cooled blanket and helium cooled blanket, it is proposed to integrate an indirect double-tanks sensible thermal storage system with hydrogenated triphenyl heat transfer oil and solar salt molten salt as thermal storage medium respectively, so as to ensure the stable and continuous operation of the power generation system. [Conclusion] The proposed energy storage scheme meets the conditions of large-scale commercial applications and supports the overall design of CFETR fusion power plant.
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- 2022
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3. CFETR聚变发电厂的储能技术适用性分析.
- Author
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梁展鹏, 向魁, 李华, and 朱光涛
- Abstract
Copyright of Southern Energy Construction is the property of Southern Energy Construction Editorial Office and its content may not be copied or emailed to multiple sites or posted to a listserv without the copyright holder's express written permission. However, users may print, download, or email articles for individual use. This abstract may be abridged. No warranty is given about the accuracy of the copy. Users should refer to the original published version of the material for the full abstract. (Copyright applies to all Abstracts.)
- Published
- 2022
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- View/download PDF
4. Fusion power predictions for β N ≈ 1.8 baseline scenario with 50–50 D–T fuel mix and NBI injection in preparation to D–T operations at JET
- Author
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V.K. Zotta, L. Garzotti, F.J. Casson, D. Frigione, F. Köchl, E. Lerche, P. Lomas, F. Rimini, M. Sertoli, D. Van Eester, R. Gatto, C. Mazzotta, G. Pucella, and null JET Contributors
- Subjects
modelling ,Nuclear and High Energy Physics ,JET ,magnetic confinement ,tokamak ,nuclear fusion power ,deuterium-tritium ,Condensed Matter Physics - Abstract
The fusion performance of ELMy H-mode 50–50 deuterium–tritium (DT) plasmas with 50–50 DT NBI injection and q 95 ≈ 3 and β N ≈ 1.8 (also referred to as medium-β N baseline scenario in the rest of this paper) are predicted with the JINTRAC suite of codes and the QuaLiKiZ transport model. The predictions are based on the analysis of plasmas from the first DT campaign on JET in 1997 (DTE1) and pure deuterium plasmas developed at JET in preparation for the DT experimental campaign in 2021 (DTE2), after the installation of a Be/W ITER-like wall in 2011. The sensitivity of the predictions to plasma parameters such as current, toroidal field, pedestal confinement and impurity content are analysed together with the sensitivity to the amount of auxiliary heating power available. The simulations indicate that a fusion power of 10 MW should be achievable under a fairly wide range of assumptions, provided that the auxiliary heating power is around or above 38 MW. Higher fusion power approaching 15 MW could be achievable for this value of β N only for particularly pure plasmas and with 40 MW of additional heating power.
- Published
- 2022
5. Helium Refrigerator Design for Pulsed Heat Load in Tokamaks.
- Author
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Kuendig, A. and Schoenfeld, H.
- Subjects
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TOKAMAKS , *REFRIGERATION & refrigerating machinery , *HELIUM at low temperatures , *NUCLEAR fusion , *LOW temperature engineering , *COOLING , *LOW temperatures - Abstract
Nuclear fusion reactors of the Tokamak type will be operated in a pulsed mode requiring the helium refrigerator to remove periodically large heat loads in time steps of approximately one hour. What are the necessary steps for a refrigerator to cope with such load variations? A series of numerical simulations has been performed indicating the possibility of an active refrigerator control with low exergetic losses. A basic comparison is made between the largest existing refrigerator sizes and the size required to service for example the ITER requirements. © 2006 American Institute of Physics [ABSTRACT FROM AUTHOR]
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- 2006
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6. Moderate beta baseline scenario in preparation to D-T operations at JET
- Author
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Zotta, V. K., Garzotti, L., Casson, F. J., Frigione, D., Gatto, R., Koechl, F., Lerche, E., Lomas, P., Mazzotta, C., Pucella, G., Rimini, F., and Van Eester, D.
- Subjects
modelling ,JET ,magnetic confinement ,tokamak ,nuclear fusion power ,deuterium-tritium - Published
- 2021
7. Scenario development for D-T operation at JET
- Author
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Garzotti, L., Challis, C., Dumont, R., Frigione, D., Graves, J., Lerche, E., Mailloux, J., Mantsinen, M., Rimini, F., Casson, F., Czarnecka, A., Eriksson, Jacob, Felton, R., Frassinetti, L., Gallart, D., Garcia, J., Giroud, C., Joffrin, E., Kim, Hyun-Tae, Krawczyk, N., Lennholm, M., Lomas, P., Lowry, C., Meneses, L., Nunes, I, Roach, C. M., Romanelli, M., Sharapov, S., Silburn, S., Sips, A., Stefániková, E., Tsalas, M., Valcarcel, D., Valovic, M., Garzotti, L., Challis, C., Dumont, R., Frigione, D., Graves, J., Lerche, E., Mailloux, J., Mantsinen, M., Rimini, F., Casson, F., Czarnecka, A., Eriksson, Jacob, Felton, R., Frassinetti, L., Gallart, D., Garcia, J., Giroud, C., Joffrin, E., Kim, Hyun-Tae, Krawczyk, N., Lennholm, M., Lomas, P., Lowry, C., Meneses, L., Nunes, I, Roach, C. M., Romanelli, M., Sharapov, S., Silburn, S., Sips, A., Stefániková, E., Tsalas, M., Valcarcel, D., and Valovic, M.
- Abstract
The JET exploitation plan foresees D-T operations in 2020 (DTE2). With respect to the first D-T campaign in 1997 (DTE1), when JET was equipped with a carbon wall, the experiments will be conducted in presence of a beryllium-tungsten ITER-like wall and will benefit from an extended and improved set of diagnostics and higher additional heating power (32 MW neutral beam injection + 8 MW ion cyclotron resonance heating). There are several challenges presented by operations with the new wall: a general deterioration of the pedestal confinement; the risk of heavy impurity accumulation in the core, which, if not controlled, can cause the radiative collapse of the discharge; the requirement to protect the divertor from excessive heat loads, which may damage it permanently. Therefore, an intense activity of scenario development has been undertaken at JET during the last three years to overcome these difficulties and prepare the plasmas needed to demonstrate stationary high fusion performance and clear alpha particle effects. The paper describes the status and main achievements of this scenario development activity, both from an operational and plasma physics point of view.
- Published
- 2019
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8. MO-A-217BCD-01: Internal Emitter Dose Estimation.
- Author
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Williams L
- Abstract
Tissue absorbed dose (D) is a computed result for internal emitters. For fixed geometries, D is calculated by a matrix (S) multiplication of the integrated activity vector (Ã). The last quantity is usually measured by nuclear imaging of activity in various source organs and performing a temporal integration. à is the same as the total number of source decays. Dose is computed for a number of target organs - some of which will be the same as the source organs. The D = S*à relationship is general in that the same formula may also be used for voxels within organs or even down to the cellular level. Finding the activity (A) in source tissues may be done by a number of methods of which 6 are described. The most common clinical technique is the geometric mean (GM) image of an organ. Uncertainties in the GM method are ≈ +/- 30%. If one can do quantitative SPECT, PET or CAMI imaging, the variation is reduced to around +/- 6%. These last three techniques, however, require fusion of anatomic (e.g. CT) and nuclear images. The S matrix is generated via Monte Carlo methods and may be used in two formats. The most common is a set of phantom-derived values for regulatory or scientific considerations. An example is the OLINDA program from Vanderbilt University. In this case, the corresponding animal or patient à value must be normalized using blood flow arguments. A second format is modification of a phantom's S values for a particular patient using the latter's geometry as found in CT or MRI scans. Corrections in such cases may be 2-fold or more because of patient organ size variability. These variations may be due to genetic reasons and/or disease. Two caveats to the use of the above dose formulation should be mentioned. One exception is that the geometry may vary during tissue irradiation; e.g., by tumor size decrease due to immediate radiation dose effects. In this case, the standard formula is replaced by its differential form: dD/dt = S(t)*A(t). Dose rate may also be an important biological factor in assessing tissue response. A second important biological consideration is that effects - such as tumor regression - may depend upon higher powers of D than the first. Thus, the tissue response may not be a linear function of D, but would exhibit a sigmoid shape. One would anticipate such responses due to saturation of a biological system., Learning Objectives: 1. Knowing the general formula for internal emitter absorbed dose estimation. 2. Understanding the various methods used to measure activity, at depth, in source organs in a living animal or patient. 3. Realizing that two types of dose may be computed: one for a phantom and a second type for an individual patient. S values must be modified accordingly for these two computations. 4. Estimating uncertainties - including those in both à and S - involved in the dose estimation process., (© 2012 American Association of Physicists in Medicine.)
- Published
- 2012
- Full Text
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