In fast ignition (FI) mechanism, a pellet containing the thermonuclear fuel is first compressed by a nanosecond laser pulse, and then irradiated by an intense "ignition" beam, initiated by a high power picosecond laser pulse, is one of the promising approaches to the realization of the inertial confinement fusion (ICF). If the ignition beam is composed of deuterons, an additional energy is delivered to the target, in which coming from fusion reactions of the beam-target type, directly initiated by particles from the ignition beam .In this article, the D+T fuel is selected and at first step we compute new average reactivity using three parameter cross section formula in terms of temperature at second step we use the obtained results of step one and calculate the total deposited energy of deuteron beam inside the target fuel at available physical conditions, then in third step we write the nonlinear point kinetic balance equation of D+T mixture and solve numerically these nonlinear differential coupled equations versus time .In forth step ,we estimate the power density and energy gain under physical optimum conditions and finally we conclude that maximum energy deposited in the target from D+T and D+D reaction are equal to 19269.39061 keV and 39198.58043 keV, respectively
Published in | American Journal of Energy Engineering (Volume 2, Issue 2) |
DOI | 10.11648/j.ajee.20140202.13 |
Page(s) | 65-74 |
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This is an Open Access article, distributed under the terms of the Creative Commons Attribution 4.0 International License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution and reproduction in any medium or format, provided the original work is properly cited. |
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Copyright © The Author(s), 2014. Published by Science Publishing Group |
Deuteron Beam, Fast Ignition, Gain, Dynamics
[1] | A. W. Maschke, Proceedings of the (1975) Particle Accelerator Conference, page 1875, IEEE report NS-22, June (1975) |
[2] | M. Tabak, et al., Phys. Plasmas 1, 1626 (1994) |
[3] | M. Tabak, et. al. Int. HIF Symposium (Heidelberg) paper ( 1997) |
[4] | T. C. Magelssen, “Targets Driven by Dual-Energy Heavy Ions”, Nuclear Fusion24, 1527(1984). |
[5] | M. Sherlock et al., Phys. Rev. Lett. 99, 255003 (2007). |
[6] | S. Atzeni, M. Temporal, and J. Honrubia, Nucl. Fusion 42, L1 (2002). |
[7] | S. Atzeni et al., Nucl. Fusion 49, 055008 (2009). |
[8] | Xing Z. Li, Qing M. Wei and Bin Liu, Nucl. Fusion 48, 125003 ,5pp (2008). |
[9] | G. Velarde, Y. Ronen, and J. Martinez-Val. Nuclear fusion by Inertial Confinement: A comprehensive treatise. |
[10] | Logan, B. Grant Bangerter, Roger O.Callahan, Debra A.Tabak, Max Roth, Markus Perkins, L. John Caporaso, George ,Lawrence Berkeley National Laboratory (2005). |
[11] | V. Bychenkov, W. Rozmus, A. Maksimchuk, D. Umstadter, and C.Capjack, Plasma Phys. Rep. 27, 1017 (2001). |
[12] | N. Naumova, T. Schlegel, V. T. Tikhonchuk, C. Labaune, I. V. Sokolov,and G. Mourou, Phys. Rev. Lett. 102, 025002 (2009). |
[13] | V. T. Tikhonchuk, T. Schlegel, C. Regan, M. Temporal, J.-L. Feugeas, P.Nicolaï, and X. Ribeyre, Nucl. Fusion 50, 045003 (2010). |
[14] | M. L. Shmatov, J. Br. Interplanet. Soc. 60,180 (2007). |
[15] | M TEMPORAL J Honrubia, S Atzeni. Phys. Plas.9,3102(2002) |
[16] | A. Maksimchuk, S. Gu, K. Flippo, D. Umstadter, and V. Y. Bychenkov, Phys. Rev. Lett. 84, 4108 (2000). |
[17] | H. Schwoerer, S. Pfotenhauer, O. Jackel, K. U. Amthor, Ziegler, R. Sauerbrey, K. W. D. Ledingham, and T. Esirkepov ,Nature London439,445 (2006) |
[18] | C. Bathke, H. Towner, and G. H. Miley, Trans. Am. Nucl. Soc. 17, 41 (1973). |
[19] | M. L. Shmatov, J. Br. Interplanet. Soc. 57,362(2004). |
[20] | Xiaoling Yang, George H. Miley, Kirk A. Flippo, and Heinrich Hora, PHYSICS OF PLASMAS 18, 032703 (2011) |
[21] | D. J. Rose and M. Clark, Jr., Plasmas and Controlled Fusion MIT Press, Cambridge, MA(1965). |
[22] | G. H. Miley, Fusion Energy Conversion American Nuclear Society, Hinsdale, IL(1976). |
[23] | S .Pfalzner, “An Introduction to Inertial Confnement Fusion”, Published by CRC Press Taylor & Francis Group(2006). |
APA Style
S. N. Hosseinimotlagh, M. Jahedi. (2014). Time Dependent Studies on the Energy Gain of D-T Fuel Using Determination of Total Energy Deposited of Deuteron Beam in Hot Spot. American Journal of Energy Engineering, 2(2), 65-74. https://doi.org/10.11648/j.ajee.20140202.13
ACS Style
S. N. Hosseinimotlagh; M. Jahedi. Time Dependent Studies on the Energy Gain of D-T Fuel Using Determination of Total Energy Deposited of Deuteron Beam in Hot Spot. Am. J. Energy Eng. 2014, 2(2), 65-74. doi: 10.11648/j.ajee.20140202.13
AMA Style
S. N. Hosseinimotlagh, M. Jahedi. Time Dependent Studies on the Energy Gain of D-T Fuel Using Determination of Total Energy Deposited of Deuteron Beam in Hot Spot. Am J Energy Eng. 2014;2(2):65-74. doi: 10.11648/j.ajee.20140202.13
@article{10.11648/j.ajee.20140202.13, author = {S. N. Hosseinimotlagh and M. Jahedi}, title = {Time Dependent Studies on the Energy Gain of D-T Fuel Using Determination of Total Energy Deposited of Deuteron Beam in Hot Spot}, journal = {American Journal of Energy Engineering}, volume = {2}, number = {2}, pages = {65-74}, doi = {10.11648/j.ajee.20140202.13}, url = {https://doi.org/10.11648/j.ajee.20140202.13}, eprint = {https://article.sciencepublishinggroup.com/pdf/10.11648.j.ajee.20140202.13}, abstract = {In fast ignition (FI) mechanism, a pellet containing the thermonuclear fuel is first compressed by a nanosecond laser pulse, and then irradiated by an intense "ignition" beam, initiated by a high power picosecond laser pulse, is one of the promising approaches to the realization of the inertial confinement fusion (ICF). If the ignition beam is composed of deuterons, an additional energy is delivered to the target, in which coming from fusion reactions of the beam-target type, directly initiated by particles from the ignition beam .In this article, the D+T fuel is selected and at first step we compute new average reactivity using three parameter cross section formula in terms of temperature at second step we use the obtained results of step one and calculate the total deposited energy of deuteron beam inside the target fuel at available physical conditions, then in third step we write the nonlinear point kinetic balance equation of D+T mixture and solve numerically these nonlinear differential coupled equations versus time .In forth step ,we estimate the power density and energy gain under physical optimum conditions and finally we conclude that maximum energy deposited in the target from D+T and D+D reaction are equal to 19269.39061 keV and 39198.58043 keV, respectively}, year = {2014} }
TY - JOUR T1 - Time Dependent Studies on the Energy Gain of D-T Fuel Using Determination of Total Energy Deposited of Deuteron Beam in Hot Spot AU - S. N. Hosseinimotlagh AU - M. Jahedi Y1 - 2014/04/20 PY - 2014 N1 - https://doi.org/10.11648/j.ajee.20140202.13 DO - 10.11648/j.ajee.20140202.13 T2 - American Journal of Energy Engineering JF - American Journal of Energy Engineering JO - American Journal of Energy Engineering SP - 65 EP - 74 PB - Science Publishing Group SN - 2329-163X UR - https://doi.org/10.11648/j.ajee.20140202.13 AB - In fast ignition (FI) mechanism, a pellet containing the thermonuclear fuel is first compressed by a nanosecond laser pulse, and then irradiated by an intense "ignition" beam, initiated by a high power picosecond laser pulse, is one of the promising approaches to the realization of the inertial confinement fusion (ICF). If the ignition beam is composed of deuterons, an additional energy is delivered to the target, in which coming from fusion reactions of the beam-target type, directly initiated by particles from the ignition beam .In this article, the D+T fuel is selected and at first step we compute new average reactivity using three parameter cross section formula in terms of temperature at second step we use the obtained results of step one and calculate the total deposited energy of deuteron beam inside the target fuel at available physical conditions, then in third step we write the nonlinear point kinetic balance equation of D+T mixture and solve numerically these nonlinear differential coupled equations versus time .In forth step ,we estimate the power density and energy gain under physical optimum conditions and finally we conclude that maximum energy deposited in the target from D+T and D+D reaction are equal to 19269.39061 keV and 39198.58043 keV, respectively VL - 2 IS - 2 ER -