Araştırma Makalesi
Yıl 2019,
Cilt: 6 Sayı: 1, 1 - 7, 26.12.2019
Öz
Kaynakça
- [1] J.H. Monkhorst, and N. Rostoker. Controlled fusion in a field reversed configuration and direct energy conversion. U.S. Patent No. 6,611:106 ( 2003)[2] T. A.Oliphant, F. L. Ribe and T. A. Coulta. "Direct conversion of thermonuclear plasma energy by high magnetic compression and expansion". Nuclear Fusion. 13 ,4 : 529 (1973) [3] R. W. Moir. Direct energy conversion in fusion reactors. Energy technology handbook, 5, 150-154 (1977) [4] A. B. Zylstra, J. A. Frenje, M. Gatu Johnson, G. M. Hale, C. R. Brune, A. Bacher, D. T. Casey,C. K. Li, D. McNabb, M. Paris,1 R. D. Petrasso, T. C. Sangster, D. B. Sayre, and F. H. S eguin. Proton Spectra from 3He + T and 3He + 3He Fusion at Low Center-of-Mass Energy, with Potential Implications for Solar Fusion Cross Sections, Physics Review Letter 119, 222701 (2017)[5] C.Baker, A. Bolon and R. Clemmer. Fusion reactor technology impact of alternate fusion fuels, No. ANL/FPP/TM—127( 1979)[6] A.Csótó, and K.Langanke. Large-space cluster model calculations for the 3He (3He, 2p) 4He and 3H (3H, 2n) 4He reactions, Nuclear Physics A 646.3, 387-396(1999) [7] G.H. Miley. 3He Sources for D3He fusion power, Nuclear Instruments and Methods in Physics Research A271 , 197-202(1988) [8] D.Petkow, G.Herdrich, R. Laufer, and H. P. Röse .Key technologies for fusion-based space propulsion: a case study, Proceedings of the 58th International Astronautical Congress (IAC-07-C3. 3.02) International Astronautical Federation, Hyderabad ( 2007)[9] S. V Ryzhkov. Thermal-physical analysis of low-radioactive thermonuclear plasma in the magnetic fusion device, Вопросы атомной науки и техники (2007) [10] R.feldbacher, the aep barnbok datlb IAEA international nuclear data commitee viema(1987)[11] M. Herman and A.Trkov. Data Formats and Procedures for the Evaluated Nuclear Data FIles ENDF/B-VI and ENDF/B-VII, National Nuclear Data Center Brookhaven National aboratory (2010)[12] W.M. Nevins. A Review of Confinement Requirements for Advanced Fuels , journal of Fusion Energy 17, 1(1998)[13] D.Gabuzda. Radiation Processes in the Universe: Synchrotron Radiation and Propagation Effects, 2nd MCCT-SKADS Training School. Radio Astronomy: fundamentals and the new instruments (2008) [14] J. Lin and A. A. van Ballegooijen. Equilbrium and evolution in multipolar magnetic configurations resulting from interactions among active regions. The Astrophysical Journal 591, 629:582 ( 2005)[15] K. D. Cole. Diamagnetism in a plasma , Physics of Plasmas 4,6 (1998). [16] J.Wesson. "Tokamaks", 3rd edition page 115, Oxford University Press( 2004)[17] L. Spitzer, Jr. The stability of isolated clusters, Monthly Notices of the. Royal Astronomical Society, Vol. 100, 396 – 413 (1940) [18] W. Fundamenski and O.E. Garcia. Comparison of Coulomb Collision Rates in the Plasma Physics and Magnetically Confined Fusion Literature , EFDA–JET–R(07)01 (2007)[19] M.Honda .Coulomb Logarithm Formulae for Collisions between Species with Different Temperatures,Japanese Journal of Applied Physics 52 ,108002(2013)
Yıl 2019,
Cilt: 6 Sayı: 1, 1 - 7, 26.12.2019
Öz
The possibilities of using advanced aneutronic fuels such as 3He3He for a clean and efficient fusion power generation are
regarded as the most important topics in nuclear engineering. This fuel is completely neutron-free thus, no material
activation inside the fusion reactor and no dangerous consequence of accidental radioactive release occurs but it requires
high demanding conditions for present-day technology. The investigations show that the radiation power losses are the
main problems in the use of this fuel in a fusion reactor. The losses have a principal role in determining the operating
temperature of this fuel. The results demonstrate that even under almost optimistic operating conditions, the bremsstrahlung
loss power is more than fusion power. To dominate the bremsstrahlung radiation, it would be desired to reduce the electron
temperature less than their normal equilibrium values. To improve the performance of 3He3He fusion reactor and to
minimize bremsstrahlung and synchrotron radiation, it is essential that the energy transmitted from ions to electrons is
minimized. When the electron temperature is low enough, the bremsstrahlung loss is manageable; however, the ionelectron energy transfer rate is very large. The studies indicate that the reduction in the bremsstrahlung power fraction is
more useful than the reduction in the ion-electron energy transfer fraction. To restrict he bremsstrahlung power to logical
theory level (less than half the fusion power), it is essential to reduce the ion-electron energy transfer rate to the possible
minimum in 3He3He fuel.
Kaynakça
- [1] J.H. Monkhorst, and N. Rostoker. Controlled fusion in a field reversed configuration and direct energy conversion. U.S. Patent No. 6,611:106 ( 2003)[2] T. A.Oliphant, F. L. Ribe and T. A. Coulta. "Direct conversion of thermonuclear plasma energy by high magnetic compression and expansion". Nuclear Fusion. 13 ,4 : 529 (1973) [3] R. W. Moir. Direct energy conversion in fusion reactors. Energy technology handbook, 5, 150-154 (1977) [4] A. B. Zylstra, J. A. Frenje, M. Gatu Johnson, G. M. Hale, C. R. Brune, A. Bacher, D. T. Casey,C. K. Li, D. McNabb, M. Paris,1 R. D. Petrasso, T. C. Sangster, D. B. Sayre, and F. H. S eguin. Proton Spectra from 3He + T and 3He + 3He Fusion at Low Center-of-Mass Energy, with Potential Implications for Solar Fusion Cross Sections, Physics Review Letter 119, 222701 (2017)[5] C.Baker, A. Bolon and R. Clemmer. Fusion reactor technology impact of alternate fusion fuels, No. ANL/FPP/TM—127( 1979)[6] A.Csótó, and K.Langanke. Large-space cluster model calculations for the 3He (3He, 2p) 4He and 3H (3H, 2n) 4He reactions, Nuclear Physics A 646.3, 387-396(1999) [7] G.H. Miley. 3He Sources for D3He fusion power, Nuclear Instruments and Methods in Physics Research A271 , 197-202(1988) [8] D.Petkow, G.Herdrich, R. Laufer, and H. P. Röse .Key technologies for fusion-based space propulsion: a case study, Proceedings of the 58th International Astronautical Congress (IAC-07-C3. 3.02) International Astronautical Federation, Hyderabad ( 2007)[9] S. V Ryzhkov. Thermal-physical analysis of low-radioactive thermonuclear plasma in the magnetic fusion device, Вопросы атомной науки и техники (2007) [10] R.feldbacher, the aep barnbok datlb IAEA international nuclear data commitee viema(1987)[11] M. Herman and A.Trkov. Data Formats and Procedures for the Evaluated Nuclear Data FIles ENDF/B-VI and ENDF/B-VII, National Nuclear Data Center Brookhaven National aboratory (2010)[12] W.M. Nevins. A Review of Confinement Requirements for Advanced Fuels , journal of Fusion Energy 17, 1(1998)[13] D.Gabuzda. Radiation Processes in the Universe: Synchrotron Radiation and Propagation Effects, 2nd MCCT-SKADS Training School. Radio Astronomy: fundamentals and the new instruments (2008) [14] J. Lin and A. A. van Ballegooijen. Equilbrium and evolution in multipolar magnetic configurations resulting from interactions among active regions. The Astrophysical Journal 591, 629:582 ( 2005)[15] K. D. Cole. Diamagnetism in a plasma , Physics of Plasmas 4,6 (1998). [16] J.Wesson. "Tokamaks", 3rd edition page 115, Oxford University Press( 2004)[17] L. Spitzer, Jr. The stability of isolated clusters, Monthly Notices of the. Royal Astronomical Society, Vol. 100, 396 – 413 (1940) [18] W. Fundamenski and O.E. Garcia. Comparison of Coulomb Collision Rates in the Plasma Physics and Magnetically Confined Fusion Literature , EFDA–JET–R(07)01 (2007)[19] M.Honda .Coulomb Logarithm Formulae for Collisions between Species with Different Temperatures,Japanese Journal of Applied Physics 52 ,108002(2013)
Toplam 1 adet kaynakça vardır.
Ayrıntılar
| Birincil Dil | İngilizce |
|---|---|
| Konular | Nükleer Fizik |
| Bölüm | Articles |
| Yazarlar | |
| Yayımlanma Tarihi | 26 Aralık 2019 |
| Gönderilme Tarihi | 3 Nisan 2019 |
| Yayımlandığı Sayı | Yıl 2019Cilt: 6 Sayı: 1 |